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- Title
- Revisiting The Ground State Of Coal2o4: Comparison To The Conventional Antiferromagnet Mnal2o4.
- Creator
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MacDougall, G. J., Aczel, A. A., Su, Yixi, Schweika, W., Faulhaber, E., Schneidewind, A., Christianson, A. D., Zarestky, J. L., Zhou, H. D., Mandrus, D., Nagler, S. E.
- Abstract/Description
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The A-site spinel material CoAl2O4 is a physical realization of the frustrated diamond-lattice antiferromagnet, a model in which unique incommensurate or "spin-spiral-liquid" ground states are predicted. Our previous single-crystal neutron scattering study instead classified it as a "kinetically inhibited" antiferromagnet, where the long-ranged correlations of a collinear Neel ground state are blocked by the freezing of domain-wall motion below a first-order phase transition at T* = 6.5 K....
Show moreThe A-site spinel material CoAl2O4 is a physical realization of the frustrated diamond-lattice antiferromagnet, a model in which unique incommensurate or "spin-spiral-liquid" ground states are predicted. Our previous single-crystal neutron scattering study instead classified it as a "kinetically inhibited" antiferromagnet, where the long-ranged correlations of a collinear Neel ground state are blocked by the freezing of domain-wall motion below a first-order phase transition at T* = 6.5 K. This paper provides new data sets from a number of experiments, which support and expand this work in several important ways. We show that the phenomenology leading to the kinetically inhibited order is unaffected by sample measured and instrument resolution, while new low-temperature measurements reveal spin correlations are unchanging between T = 2 K and 250 mK, consistent with a frozen state. Polarized diffuse neutron measurements show several interesting magnetic features, which can be entirely explained by the existence of short-ranged Neel order. Finally, and crucially, this paper presents some neutron scattering studies of single crystalline MnAl2O4, which acts as an unfrustrated analog to CoAl2O4 and shows all the hallmarks of a classical antiferromagnet with a continuous phase transition to Neel order at T-N = 39 K. Direct comparison between the two compounds indicates that CoAl2O4 is unique, not in the nature of high-temperature diffuse correlations, but rather in the nature of the frozen state below T*. The higher level of cation inversion in the MnAl2O4 sample indicates that this behavior is primarily an effect of greater next-nearest-neighbor exchange.
Show less - Date Issued
- 2016-11-17
- Identifier
- FSU_libsubv1_wos_000387887100005, 10.1103/PhysRevB.94.184422
- Format
- Citation
- Title
- Giant Suppression Of Phononic Heat Transport In A Quantum Magnet Bicu2po6.
- Creator
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Jeon, Byung-Gu, Koteswararao, B., Park, C. B., Shu, G. J., Riggs, S. C., Moon, E. G., Chung, S. B., Chou, F. C., Kim, Kee Hoon
- Abstract/Description
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Thermal transport of quantum magnets has elucidated the nature of low energy elementary excitations and complex interplay between those excited states via strong scattering of thermal carriers. BiCu2PO6 is a unique frustrated spin-ladder compound exhibiting highly anisotropic spin excitations that contain both itinerant and localized dispersion characters along the b- and a-axes respectively. Here, we investigate thermal conductivity. of BiCu2PO6 under high magnetic fields (H) of up to 30...
Show moreThermal transport of quantum magnets has elucidated the nature of low energy elementary excitations and complex interplay between those excited states via strong scattering of thermal carriers. BiCu2PO6 is a unique frustrated spin-ladder compound exhibiting highly anisotropic spin excitations that contain both itinerant and localized dispersion characters along the b- and a-axes respectively. Here, we investigate thermal conductivity. of BiCu2PO6 under high magnetic fields (H) of up to 30 tesla. A dip-feature in., located at similar to 15 K at zero-H along all crystallographic directions, moves gradually toward lower temperature (T) with increasing H, thus resulting in giant suppression by a factor of similar to 30 near the critical magnetic field of H-c congruent to 23.5 tesla. The giant H- and T-dependent suppression of kappa can be explained by the combined result of resonant scattering of phononic heat carriers with magnetic energy levels and increased phonon scattering due to enhanced spin fluctuation at Hc, unequivocally revealing the existence of strong spin-phonon coupling. Moreover, we find an experimental indication that the remaining magnetic heat transport along the b-axis becomes almost gapless at the magnetic quantum critical point realized at H-c.
Show less - Date Issued
- 2016-11-15
- Identifier
- FSU_libsubv1_wos_000387646400002, 10.1038/srep36970
- Format
- Citation
- Title
- Resolving Cypriniformes Relationships Using An Anchored Enrichment Approach.
- Creator
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Stout, Carla C., Tan, Milton, Lemmon, Alan R., Lemmon, Emily Moriarty, Armbruster, Jonathan W.
- Abstract/Description
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Background: Cypriniformes (minnows, carps, loaches, and suckers) is the largest group of freshwater fishes in the world (similar to 4300 described species). Despite much attention, previous attempts to elucidate relationships using molecular and morphological characters have been incongruent. In this study we present the first phylogenomic analysis using anchored hybrid enrichment for 172 taxa to represent the order (plus three out-group taxa), which is the largest dataset for the order to...
Show moreBackground: Cypriniformes (minnows, carps, loaches, and suckers) is the largest group of freshwater fishes in the world (similar to 4300 described species). Despite much attention, previous attempts to elucidate relationships using molecular and morphological characters have been incongruent. In this study we present the first phylogenomic analysis using anchored hybrid enrichment for 172 taxa to represent the order (plus three out-group taxa), which is the largest dataset for the order to date (219 loci, 315,288 bp, average locus length of 1011 bp). Results: Concatenation analysis establishes a robust tree with 97 % of nodes at 100 % bootstrap support. Species tree analysis was highly congruent with the concatenation analysis with only two major differences: monophyly of Cobitoidei and placement of Danionidae. Conclusions: Most major clades obtained in prior molecular studies were validated as monophyletic, and we provide robust resolution for the relationships among these clades for the first time. These relationships can be used as a framework for addressing a variety of evolutionary questions (e.g. phylogeography, polyploidization, diversification, trait evolution, comparative genomics) for which Cypriniformes is ideally suited.
Show less - Date Issued
- 2016-11-09
- Identifier
- FSU_libsubv1_wos_000387727200003, 10.1186/s12862-016-0819-5
- Format
- Citation
- Title
- Decomposing Transverse Momentum Balance Contributions For Quenched Jets In Pbpb Collisions At Root S(nn)=2.76 Tev.
- Creator
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Ruiz Vargas, J. C., Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Ero, J., Mossolov, V.,...
Show moreRuiz Vargas, J. C., Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Ero, J., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., De Wolf, E. A., Janssen, X., Lauwers, J., Van de Klundert, M., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Brun, H., Caillol, C., Clerbaux, B., De Lentdecker, G., Delannoy, H., Fasanella, G., Favart, L., Cimmino, A., Cornelis, T., Dobur, D., Fagot, A., Garcia, G., Gul, M., Poyraz, D., Salva, S., Bakhshiansohi, H., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Caudron, A., De Visscher, S., Beliy, N., Alda Junior, W. L., Alves, F. L., Alves, G. A., Brito, L., Hensel, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., Battilana, C., Pigazzini, S., De Nardo, G., Thyssen, F., Zanetti, M., Fedi, G., Giassi, A., Grippo, M. T., Ligabue, F., Lomtadze, T., Martini, L., Messineo, A., Palla, F., Rizzi, A., Savoy-Navarro, A., Spagnolo, P., Tenchini, R., Tonelli, G., Venturi, A., Verdini, P. G., Barone, L., Cavallari, F., Cipriani, M., D'imperio, G., Del Re, D., Diemoz, M., Gelli, S., Jorda, C., Longo, E., Margaroli, F., Meridiani, P., Organtini, G., Paramatti, R., Preiato, F., Rahatlou, S., Rovelli, C., Santanastasio, F., Amapane, N., Arcidiacono, R., Argiro, S., Arneodo, M., Bartosik, N., Bellan, R., Biino, C., Cartiglia, N., Cenna, F., Costa, M., Covarelli, R., Degano, A., Demaria, N., Finco, L., Kiani, B., Mariotti, C., Maselli, S., Migliore, E., Monaco, V., Monteil, E., Obertino, M. M., Pacher, L., Pastrone, N., Pelliccioni, M., Pinna Angioni, G. L., Ravera, F., Romero, A., Ruspa, M., Sacchi, R., Shchelina, K., Sola, V., Solano, A., Staiano, A., Traczyk, P., Belforte, S., Casarsa, M., Cossutti, F., Della Ricca, G., La Licata, C., Schizzi, A., Zanetti, A., Kim, D. H., Kim, G. N., Kim, M. S., Lee, S., Lee, S. W., Oh, Y. D., Sekmen, S., Son, D. C., Yang, Y. C., Lee, A., Brochero Cifuentes, J. A., Kim, T. J., Cho, S., Choi, S., Go, Y., Gyun, D., Ha, S., Hong, B., Jo, Y., Kim, Y., Lee, B., Lee, K., Lee, K. S., Lee, S., Lim, J., Park, S. K., Roh, Y., Almond, J., Kim, J., Oh, S. B., Seo, S. H., Yang, U. K., Yoo, H. D., Yu, G. B., Choi, M., Kim, H., Kim, H., Kim, J. H., Lee, J. S. H., Park, I. C., Ryu, G., Ryu, M. S., Choi, Y., Goh, J., Hwang, C., Lee, J., Yu, I., Dudenas, V., Juodagalvis, A., Vaitkus, J., Ahmed, I., Ibrahim, Z. A., Komaragiri, J. R., Md Ali, M. A. B., Mohamad Idris, F., Wan Abdullah, W. A. T., Yusli, M. N., Zolkapli, Z., Castilla-Valdez, H., De La Cruz-Burelo, E., Heredia-De La Cruz, I., Hernandez-Almada, A., Lopez-Fernandez, R., Magaa Villalba, R., Mejia Guisao, J., Sanchez-Hernandez, A., Carrillo Moreno, S., Oropeza Barrera, C., Vazquez Valencia, F., Carpinteyro, S., Pedraza, I., Salazar Ibarguen, H. A., Uribe Estrada, C., Morelos Pineda, A., Krofcheck, D., Butler, P. H., Ahmad, A., Ahmad, M., Hassan, Q., Hoorani, H. R., Khan, W. A., Shah, M. A., Shoaib, M., Waqas, M., Bialkowska, H., Bluj, M., Boimska, B., Frueboes, T., Groski, M., Kazana, M., Nawrocki, K., Romanowska-Rybinska, K., Szleper, M., Zalewski, P., Bunkowski, K., Byszuk, A., Doroba, K., Kalinowski, A., Konecki, M., Krolikowski, J., Misiura, M., Olszewski, M., Walczak, M., Bargassa, P., Beiro Da Cruz E Silva, C., Di Francesco, A., Faccioli, P., Ferreira Parracho, P. G., Gallinaro, M., Hollar, J., Leonardo, N., Lloret Iglesias, L., Nemallapudi, M. V., Rodrigues Antunes, J., Seixas, J., Toldaiev, O., Vadruccio, D., Varela, J., Vischia, P., Afanasiev, S., Bunin, P., Golutvin, I., Kamenev, A., Karjavin, V., Korenkov, V., Lanev, A., Malakhov, A., Matveev, V., Mitsyn, V. V., Moisenz, P., Palichik, V., Perelygin, V., Shmatov, S., Skatchkov, N., Smirnov, V., Tikhonenko, E., Yuldashev, B. S., Zarubin, A., Chtchipounov, L., Golovtsov, V., Ivanov, Y., Kim, V., Kuznetsova, E., Murzin, V., Oreshkin, V., Sulimov, V., Vorobyev, A., Andreev, Yu, Dermenev, A., Gninenko, S., Golubev, N., Karneyeu, A., Kirsanov, M., Krasnikov, N., Pashenkov, A., Tlisov, D., Toropin, A., Epshteyn, V., Gavrilov, V., Lychkovskaya, N., Popov, V., Pozdnyakov, I., Safronov, G., Spiridonov, A., Toms, M., Vlasov, E., Zhokin, A., Bylinkin, A., Chistov, R., Danilov, M., Rusinov, V., Andreev, V., Azarkin, M., Dremin, I., Kirakosyan, M., Leonidov, A., Rusakov, S. V., Terkulov, A., Baskakov, A., Belyaev, A., Boos, E., Demiyanov, A., Ershov, A., Gribushin, A., Kodolova, O., Korotkikh, V., Lokhtin, I., Miagkov, I., Obraztsov, S., Petrushanko, S., Savrin, V., Snigirev, A., Vardanyan, I., Blinov, V., Skovpen, Y., Azhgirey, I., Bayshev, I., Bitioukov, S., Elumakhov, D., Kachanov, V., Kalinin, A., Konstantinov, D., Krychkine, V., Petrov, V., Ryutin, R., Sobol, A., Troshin, S., Tyurin, N., Uzunian, A., Volkov, A., Adzic, P., Cirkovic, P., Devetak, D., Dordevic, M., Milosevic, J., Rekovic, V., Alcaraz Maestre, J., Barrio Luna, M., Calvo, E., Cerrada, M., Chamizo Llatas, M., Colino, N., De La Cruz, B., Delgado Peris, A., Escalante Del Valle, A., Fernandez Bedoya, C., Fernandez Ramos, J. P., Flix, J., Fouz, M. C., Garcia-Abia, P., Gonzalez Lopez, O., Goy Lopez, S., Hernandez, J. M., Josa, M. I., Navarro De Martino, E., Perez-Calero Yzquierdo, A., Puerta Pelayo, J., Quintario Olmeda, A., Redondo, I., Romero, L., Soares, M. S., de Trocniz, J. F., Missiroli, M., Moran, D., Cuevas, J., Fernandez Menendez, J., Gonzalez Caballero, I., Gonzalez Fernandez, J. R., Palencia Cortezon, E., Sanchez Cruz, S., Suarez Andres, I., Vizan Garcia, J. M., Cabrillo, I. J., Calderon, A., Castieiras De Saa, J. R., Curras, E., Fernandez, M., Garcia-Ferrero, J., Gomez, G., Lopez Virto, A., Marco, J., Martinez Rivero, C., Matorras, F., Piedra Gomez, J., Rodrigo, T., Ruiz-Jimeno, A., Scodellaro, L., Trevisani, N., Vila, I., Vilar Cortabitarte, R., Abbaneo, D., Auffray, E., Auzinger, G., Bachtis, M., Baillon, P., Ball, A. H., Barney, D., Bloch, P., Bocci, A., Bonato, A., Botta, C., Camporesi, T., Castello, R., Cepeda, M., Cerminara, G., D'Alfonso, M., d'Enterria, D., Dabrowski, A., Daponte, V., David, A., De Gruttola, M., De Guio, F., De Roeck, A., Di Marco, E., Dobson, M., Dorney, B., du Pree, T., Duggan, D., Dunser, M., Dupont, N., Elliott-Peisert, A., Fartoukh, S., Franzoni, G., Fulcher, J., Funk, W., Gigi, D., Gill, K., Girone, M., Glege, F., Gulhan, D., Gundacker, S., Guthoff, M., Hammer, J., Harris, P., Hegeman, J., Innocente, V., Janot, P., Kirschenmann, H., Knunz, V., Kornmayer, A., Kortelainen, M. J., Kousouris, K., Krammer, M., Lecoq, P., Lourenco, C., Lucchini, M. T., Malgeri, L., Mannelli, M., Martelli, A., Meijers, F., Mersi, S., Meschi, E., Moortgat, F., Morovic, S., Mulders, M., Neugebauer, H., Orfanelli, S., Orsini, L., Pape, L., Perez, E., Peruzzi, M., Petrilli, A., Petrucciani, G., Pfeiffer, A., Pierini, M., Racz, A., Reis, T., Rolandi, G., Rovere, M., Ruan, M., Sakulin, H., Sauvan, J. B., Schafer, C., Schwick, C., Seidel, M., Sharma, A., Silva, P., Simon, M., Sphicas, P., Steggemann, J., Stoye, M., Takahashi, Y., Tosi, M., Treille, D., Triossi, A., Tsirou, A., Veckalns, V., Veres, G. I., Wardle, N., Zagozdzinska, A., Zeuner, W. D., Bertl, W., Deiters, K., Erdmann, W., Horisberger, R., Ingram, Q., Kaestli, H. C., Kotlinski, D., Langenegger, U., Rohe, T., Bachmair, F., Bani, L., Bianchini, L., Casal, B., Dissertori, G., Dittmar, M., Donega, M., Eller, P., Grab, C., Heidegger, C., Hits, D., Hoss, J., Kasieczka, G., Lecomte, P., Lustermann, W., Mangano, B., Marionneau, M., Martinez Ruiz del Arbol, P., Masciovecchio, M., Meinhard, M. T., Meister, D., Micheli, F., Musella, P., Nessi-Tedaldi, F., Pandolfi, F., Pata, J., Pauss, F., Perrin, G., Perrozzi, L., Quittnat, M., Rossini, M., Schonenberger, M., Starodumov, A., Tavolaro, V. R., Theofilatos, K., Wallny, R., Aarrestad, T. K., Amsler, C., Caminada, L., Canelli, M. F., De Cosa, A., Galloni, C., Hinzmann, A., Hreus, T., Kilminster, B., Lange, C., Ngadiuba, J., Pinna, D., Rauco, G., Robmann, P., Salerno, D., Yang, Y., Candelise, V., Doan, T. H., Jain, Sh, Khurana, R., Konyushikhin, M., Kuo, C. M., Lin, W., Lu, Y. J., Pozdnyakov, A., Yu, S. S., Kumar, Arun, Chang, P., Chang, Y. H., Chang, Y. W., Chao, Y., Chen, K. F., Chen, P. H., Dietz, C., Fiori, F., Hou, W.-S., Hsiung, Y., Liu, Y. F., Lu, R.-S., Miano Moya, M., Paganis, E., Psallidas, A., Tsai, J. F., Tzeng, Y. M., Asavapibhop, B., Singh, G., Srimanobhas, N., Suwonjandee, N., Adiguzel, A., Cerci, S., Damarseckin, S., Demiroglu, Z. S., Dozen, C., Dumanoglu, I., Girgis, S., Gokbulut, G., Guler, Y., Gurpinar, E., Hos, I., Kangal, E. E., Kara, O., Kayis Topaksu, A., Kiminsu, U., Oglakci, M., Onengut, G., Ozdemir, K., Sunar Cerci, D., Topakli, H., Turkcapar, S., Zorbakir, I. S., Zorbilmez, C., Bilin, B., Bilmis, S., Isildak, B., Karapinar, G., Yalvac, M., Zeyrek, M., Gulmez, E., Kaya, M., Kaya, O., Yetkin, E. A., Yetkin, T., Cakir, A., Cankocak, K., Sen, S., Grynyov, B., Levchuk, L., Sorokin, P., Aggleton, R., Ball, F., Beck, L., Brooke, J. J., Burns, D., Clement, E., Cussans, D., Flacher, H., Goldstein, J., Grimes, M., Heath, G. P., Heath, H. F., Jacob, J., Kreczko, L., Lucas, C., Newbold, D. M., Paramesvaran, S., Poll, A., Sakuma, T., Seif El Nasr-storey, S., Smith, D., Smith, V. J., Barducci, D., Belyaev, A., Brew, C., Brown, R. M., Calligaris, L., Cieri, D., Cockerill, D. J. A., Coughlan, J. A., Harder, K., Harper, S., Olaiya, E., Petyt, D., Shepherd-Themistocleous, C. H., Thea, A., Tomalin, I. R., Williams, T., Baber, M., Bainbridge, R., Buchmuller, O., Bundock, A., Burton, D., Casasso, S., Citron, M., Colling, D., Corpe, L., Dauncey, P., Davies, G., De Wit, A., Della Negra, M., Di Maria, R., Dunne, P., Elwood, A., Futyan, D., Haddad, Y., Hall, G., Iles, G., James, T., Lane, R., Laner, C., Lucas, R., Lyons, L., Magnan, A.-M., Malik, S., Mastrolorenzo, L., Nash, J., Nikitenko, A., Pela, J., Penning, B., Pesaresi, M., Raymond, D. M., Richards, A., Rose, A., Seez, C., Summers, S., Tapper, A., Uchida, K., Vazquez Acosta, M., Virdee, T., Wright, J., Zenz, S. C., Cole, J. E., Hobson, P. R., Khan, A., Kyberd, P., Leslie, D., Reid, I. D., Symonds, P., Teodorescu, L., Turner, M., Borzou, A., Call, K., Dittmann, J., Hatakeyama, K., Liu, H., Pastika, N., Charaf, O., Cooper, S. I., Henderson, C., Rumerio, P., Arcaro, D., Avetisyan, A., Bose, T., Gastler, D., Rankin, D., Richardson, C., Rohlf, J., Sulak, L., Zou, D., Benelli, G., Berry, E., Cutts, D., Garabedian, A., Hakala, J., Heintz, U., Hogan, J. M., Jesus, O., Laird, E., Landsberg, G., Mao, Z., Narain, M., Piperov, S., Sagir, S., Spencer, E., Syarif, R., Breedon, R., Breto, G., Burns, D., Calderon De La Barca Sanchez, M., Chauhan, S., Chertok, M., Conway, J., Conway, R., Cox, P. T., Erbacher, R., Flores, C., Funk, G., Gardner, M., Ko, W., Lander, R., Mclean, C., Mulhearn, M., Pellett, D., Pilot, J., Ricci-Tam, F., Shalhout, S., Smith, J., Squires, M., Stolp, D., Tripathi, M., Wilbur, S., Yohay, R., Cousins, R., Everaerts, P., Florent, A., Hauser, J., Ignatenko, M., Saltzberg, D., Takasugi, E., Valuev, V., Weber, M., Burt, K., Clare, R., Ellison, J., Gary, J. W., Hanson, G., Heilman, J., Jandir, P., Kennedy, E., Lacroix, F., Long, O. R., Malberti, M., Olmedo Negrete, M., Paneva, M. I., Shrinivas, A., Wei, H., Wimpenny, S., Yates, B. R., Branson, J. G., Cerati, G. B., Cittolin, S., Derdzinski, M., Gerosa, R., Holzner, A., Klein, D., Krutelyov, V., Letts, J., Macneill, I., Olivito, D., Padhi, S., Pieri, M., Sani, M., Sharma, V., Simon, S., Tadel, M., Vartak, A., Wasserbaech, S., Welke, C., Wood, J., Wurthwein, F., Yagil, A., Zevi Della Porta, G., Bhandari, R., Bradmiller-Feld, J., Campagnari, C., Dishaw, A., Dutta, V., Flowers, K., Franco Sevilla, M., Geffert, P., George, C., Golf, F., Gouskos, L., Gran, J., Heller, R., Incandela, J., Mccoll, N., Mullin, S. D., Ovcharova, A., Richman, J., Stuart, D., Suarez, I., West, C., Yoo, J., Anderson, D., Apresyan, A., Bendavid, J., Bornheim, A., Bunn, J., Chen, Y., Duarte, J., Lawhorn, J. M., Mott, A., Newman, H. B., Pena, C., Spiropulu, M., Vlimant, J. R., Xie, S., Zhu, R. Y., Andrews, M. B., Azzolini, V., Ferguson, T., Paulini, M., Russ, J., Sun, M., Vogel, H., Vorobiev, I., Cumalat, J. P., Ford, W. T., Jensen, F., Johnson, A., Krohn, M., Mulholland, T., Stenson, K., Wagner, S. R., Alexander, J., Chaves, J., Chu, J., Dittmer, S., Mcdermott, K., Mirman, N., Nicolas Kaufman, G., Patterson, J. R., Rinkevicius, A., Ryd, A., Skinnari, L., Soffi, L., Tan, S. M., Tao, Z., Thom, J., Tucker, J., Wittich, P., Zientek, M., Winn, D., Abdullin, S., Albrow, M., Apollinari, G., Banerjee, S., Bauerdick, L. A. T., Beretvas, A., Berryhill, J., Bhat, P. C., Bolla, G., Burkett, K., Butler, J. N., Cheung, H. W. K., Chlebana, F., Cihangir, S., Cremonesi, M., Elvira, V. D., Fisk, I., Freeman, J., Gottschalk, E., Gray, L., Green, D., Grunendahl, S., Gutsche, O., Hare, D., Harris, R. M., Hasegawa, S., Hirschauer, J., Hu, Z., Jayatilaka, B., Jindariani, S., Johnson, M., Joshi, U., Klima, B., Kreis, B., Lammel, S., Linacre, J., Lincoln, D., Lipton, R., Liu, T., Lopes De Sa, R., Lykken, J., Maeshima, K., Magini, N., Marraffino, J. M., Maruyama, S., Mason, D., McBride, P., Merkel, P., Mrenna, S., Nahn, S., Newman-Holmes, C., O'Dell, V., Pedro, K., Prokofyev, O., Rakness, G., Ristori, L., Sexton-Kennedy, E., Soha, A., Spalding, W. J., Spiegel, L., Stoynev, S., Strobbe, N., Taylor, L., Tkaczyk, S., Tran, N. V., Uplegger, L., Vaandering, E. W., Vernieri, C., Verzocchi, M., Vidal, R., Wang, M., Weber, H. A., Whitbeck, A., Acosta, D., Avery, P., Bortignon, P., Bourilkov, D., Brinkerhoff, A., Carnes, A., Carver, M., Curry, D., Das, S., Field, R. D., Furic, I. K., Konigsberg, J., Korytov, A., Ma, P., Matchev, K., Mei, H., Milenovic, P., Mitselmakher, G., Rank, D., Shchutska, L., Sperka, D., Thomas, L., Wang, J., Wang, S., Yelton, J., Linn, S., Markowitz, P., Martinez, G., Rodriguez, J. L., Ackert, A., Adams, J. R., Adams, T., Askew, A., Bein, S., Diamond, B., Hagopian, S., Hagopian, V., Johnson, K. F., Khatiwada, A., Prosper, H., Santra, A., Weinberg, M., Baarmand, M. M., Bhopatkar, V., Colafranceschi, S., Hohlmann, M., Noonan, D., Roy, T., Yumiceva, F., Adams, M. R., Apanasevich, L., Berry, D., Betts, R. R., Bucinskaite, I., Cavanaugh, R., Evdokimov, O., Gauthier, L., Gerber, C. E., Hofman, D. J., Kurt, P., O'Brien, C., Sandoval Gonzalez, I. D., Trauger, H., Turner, P., Varelas, N., Wang, H., Wu, Z., Zakaria, M., Zhang, J., Bilki, B., Clarida, W., Dilsiz, K., Durgut, S., Gandrajula, R. P., Haytmyradov, M., Khristenko, V., Merlo, J.-P., Mermerkaya, H., Mestvirishvili, A., Moeller, A., Nachtman, J., Ogul, H., Onel, Y., Ozok, F., Penzo, A., Snyder, C., Tiras, E., Wetzel, J., Yi, K., Anderson, I., Blumenfeld, B., Cocoros, A., Eminizer, N., Fehling, D., Feng, L., Gritsan, A. V., Maksimovic, P., Osherson, M., Roskes, J., Sarica, U., Swartz, M., Xiao, M., Xin, Y., You, C., Al-bataineh, A., Baringer, P., Bean, A., Bowen, J., Bruner, C., Castle, J., Kenny, R. P., Kropivnitskaya, A., Majumder, D., Mcbrayer, W., Murray, M., Sanders, S., Stringer, R., Tapia Takaki, J. D., Wang, Q., Ivanov, A., Kaadze, K., Khalil, S., Makouski, M., Maravin, Y., Mohammadi, A., Saini, L. K., Skhirtladze, N., Toda, S., Rebassoo, F., Wright, D., Anelli, C., Baden, A., Baron, O., Belloni, A., Calvert, B., Eno, S. C., Ferraioli, C., Gomez, J. A., Hadley, N. J., Jabeen, S., Kellogg, R. G., Kolberg, T., Kunkle, J., Lu, Y., Mignerey, A. C., Shin, Y. H., Skuja, A., Tonjes, M. B., Tonwar, S. C., Abercrombie, D., Allen, B., Apyan, A., Barbieri, R., Baty, A., Bi, R., Bierwagen, K., Brandt, S., Busza, W., Cali, I. A., Demiragli, Z., Di Matteo, L., Gomez Ceballos, G., Goncharov, M., Hsu, D., Iiyama, Y., Innocenti, G. M., Klute, M., Kovalskyi, D., Krajczar, K., Lai, Y. S., Lee, Y.-J., Levin, A., Luckey, P. D., Marini, A. C., Mcginn, C., Mironov, C., Narayanan, S., Niu, X., Paus, C., Roland, C., Roland, G., Salfeld-Nebgen, J., Stephans, G. S. F., Sumorok, K., Tatar, K., Varma, M., Velicanu, D., Veverka, J., Wang, J., Wang, T. W., Wyslouch, B., Yang, M., Zhukova, V., Benvenuti, A. C., Chatterjee, R. M., Evans, A., Finkel, A., Gude, A., Hansen, P., Kalafut, S., Kao, S. C., Kubota, Y., Lesko, Z., Mans, J., Nourbakhsh, S., Ruckstuhl, N., Rusack, R., Tambe, N., Turkewitz, J., Acosta, J. G., Oliveros, S., Avdeeva, E., Bartek, R., Bloom, K., Claes, D. R., Dominguez, A., Fangmeier, C., Gonzalez Suarez, R., Kamalieddin, R., Kravchenko, I., Malta Rodrigues, A., Meier, F., Monroy, J., Siado, J. E., Snow, G. R., Stieger, B., Alyari, M., Dolen, J., George, J., Godshalk, A., Harrington, C., Iashvili, I., Kaisen, J., Kharchilava, A., Kumar, A., Parker, A., Rappoccio, S., Roozbahani, B., Alverson, G., Barberis, E., Baumgartel, D., Hortiangtham, A., Knapp, B., Massironi, A., Morse, D. M., Nash, D., Orimoto, T., Teixeira De Lima, R., Trocino, D., Wang, R.-J., Wood, D., Bhattacharya, S., Hahn, K. A., Kubik, A., Kumar, A., Low, J. F., Mucia, N., Odell, N., Pollack, B., Schmitt, M. H., Sung, K., Trovato, M., Velasco, M., Dev, N., Hildreth, M., Hurtado Anampa, K., Jessop, C., Karmgard, D. J., Kellams, N., Lannon, K., Marinelli, N., Meng, F., Mueller, C., Musienko, Y., Planer, M., Reinsvold, A., Ruchti, R., Smith, G., Taroni, S., Valls, N., Wayne, M., Wolf, M., Woodard, A., Alimena, J., Antonelli, L., Brinson, J., Bylsma, B., Durkin, L. S., Flowers, S., Francis, B., Hart, A., Hill, C., Hughes, R., Ji, W., Liu, B., Luo, W., Puigh, D., Winer, B. L., Wulsin, H. W., Cooperstein, S., Driga, O., Elmer, P., Hardenbrook, J., Hebda, P., Lange, D., Luo, J., Marlow, D., Medvedeva, T., Mei, K., Mooney, M., Olsen, J., Palmer, C., Piroue, P., Stickland, D., Tully, C., Zuranski, A., Malik, S., Barker, A., Barnes, V. E., Folgueras, S., Gutay, L., Jha, M. K., Jones, M., Jung, A. W., Jung, K., Miller, D. H., Neumeister, N., Radburn-Smith, B. C., Shi, X., Sun, J., Svyatkovskiy, A., Wang, F., Xie, W., Xu, L., Parashar, N., Stupak, J., Adair, A., Akgun, B., Chen, Z., Ecklund, K. M., Geurts, F. J. M., Guilbaud, M., Li, W., Michlin, B., Northup, M., Padley, B. P., Redjimi, R., Roberts, J., Rorie, J., Tu, Z., Zabel, J., Betchart, B., Bodek, A., de Barbaro, P., Demina, R., Duh, Y. T., Ferbel, T., Galanti, M., Garcia-Bellido, A., Han, J., Hindrichs, O., Khukhunaishvili, A., Lo, K. H., Tan, P., Verzetti, M., Chou, J. P., Contreras-Campana, E., Gershtein, Y., Gmez Espinosa, T. A., Halkiadakis, E., Heindl, M., Hidas, D., Hughes, E., Kaplan, S., Kunnawalkam Elayavalli, R., Kyriacou, S., Lath, A., Nash, K., Saka, H., Salur, S., Schnetzer, S., Sheffield, D., Somalwar, S., Stone, R., Thomas, S., Thomassen, P., Walker, M., Foerster, M., Heideman, J., Riley, G., Rose, K., Spanier, S., Thapa, K., Bouhali, O., Celik, A., Dalchenko, M., De Mattia, M., Delgado, A., Dildick, S., Eusebi, R., Gilmore, J., Huang, T., Juska, E., Kamon, T., Mueller, R., Pakhotin, Y., Patel, R., Perloff, A., Pernis, L., Rathjens, D., Rose, A., Safonov, A., Tatarinov, A., Ulmer, K. A., Akchurin, N., Cowden, C., Damgov, J., Dragoiu, C., Dudero, P. R., Faulkner, J., Kunori, S., Lamichhane, K., Lee, S. W., Libeiro, T., Undleeb, S., Volobouev, I., Wang, Z., Delannoy, A. G., Greene, S., Gurrola, A., Janjam, R., Johns, W., Maguire, C., Melo, A., Ni, H., Sheldon, P., Tuo, S., Velkovska, J., Xu, Q., Arenton, M. W., Barria, P., Cox, B., Goodell, J., Hirosky, R., Ledovskoy, A., Li, H., Neu, C., Sinthuprasith, T., Sun, X., Wang, Y., Wolfe, E., Xia, F., Clarke, C., Harr, R., Karchin, P. E., Lamichhane, P., Sturdy, J., Belknap, D. A., Dasu, S., Dodd, L., Duric, S., Gomber, B., Grothe, M., Herndon, M., Herve, A., Klabbers, P., Lanaro, A., Levine, A., Long, K., Loveless, R., Ojalvo, I., Perry, T., Pierro, G. A., Polese, G., Ruggles, T., Savin, A., Sharma, A., Smith, N., Smith, W. H., Taylor, D., Woods, N.
Show less - Abstract/Description
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Interactions between jets and the quark-gluon plasma produced in heavy ion collisions are studied via the angular distributions of summed charged-particle transverse momenta (p(T)) with respect to both the leading and subleading jet axes in high-p(T) dijet events. The contributions of charged particles in different momentum ranges to the overall event p(T) balance are decomposed into short-range jet peaks and a long-range azimuthal asymmetry in charged-particle p(T). The results for PbPb...
Show moreInteractions between jets and the quark-gluon plasma produced in heavy ion collisions are studied via the angular distributions of summed charged-particle transverse momenta (p(T)) with respect to both the leading and subleading jet axes in high-p(T) dijet events. The contributions of charged particles in different momentum ranges to the overall event p(T) balance are decomposed into short-range jet peaks and a long-range azimuthal asymmetry in charged-particle p(T). The results for PbPb collisions are compared to those in pp collisions using data collected in 2011 and 2013, at collision energy root s(NN) = 2.76 TeV with integrated luminosities of 166 mu b(-1) and 5.3 pb(-1), respectively, by the CMS experiment at the LHC. Measurements are presented as functions of PbPb collision centrality, charged-particle p(T), relative azimuth, and radial distance from the jet axis for balanced and unbalanced dijets.
Show less - Date Issued
- 2016-11-09
- Identifier
- FSU_libsubv1_wos_000387813900001, 10.1007/JHEP11(2016)055
- Format
- Citation
- Title
- The Effects Of A High Magnetic Field On The Annealing Of [(fe0.5co0.5)(0.75)b0.2si0.05](96)nb-4 Bulk Metallic Glass.
- Creator
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Jia, Peng, Wang, En-gang, Han, Ke
- Abstract/Description
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In contrast with amorphous alloys, nanocrystalline soft magnetic materials show improved thermal stability and higher soft magnetic properties. The nanocrystalline soft magnetic composites are usually fabricated by partially crystallizing from parent amorphous alloys. This paper reports our experimental observation on the sequence of crystallization in metallic glass under a high magnetic field (HMF). An application of a HMF to bulk metallic glass (BMG) of [(Fe0.5Co0.5)(0.75)B0.2Si0.05](96)Nb...
Show moreIn contrast with amorphous alloys, nanocrystalline soft magnetic materials show improved thermal stability and higher soft magnetic properties. The nanocrystalline soft magnetic composites are usually fabricated by partially crystallizing from parent amorphous alloys. This paper reports our experimental observation on the sequence of crystallization in metallic glass under a high magnetic field (HMF). An application of a HMF to bulk metallic glass (BMG) of [(Fe0.5Co0.5)(0.75)B0.2Si0.05](96)Nb-4 prioritizes the precipitation of alpha-(Fe,Co) phase separated from the subsequent precipitation of borides, (Fe,Co)(23)B-6, upon isothermal annealing at a glass transition temperature. Furthermore, it was observed that, through the annealing treatment under a HMF, a soft magnetic nanocomposite, in which only alpha-(Fe,Co) phase uniformly distributes in amorphous matrix, was achieved for boron-bearing BMG. The promotion of the alpha-Fe or (Fe,Co) phase and the prevention of the boride phases during the isothermal annealing process help to produce high-quality soft magnetic nanocomposite materials. The mechanism by which a HMF influences the crystallization sequence was interpreted via certain changes in Gibbs free energies for two ferromagnetic phases. This finding evidences that the annealing treatment under a HMF is suitable for enhancing the soft magnetic properties of high B content (Fe,Co)-based bulk amorphous and nanocrystalline materials.
Show less - Date Issued
- 2016-11
- Identifier
- FSU_libsubv1_wos_000387254000040, 10.3390/ma9110899
- Format
- Citation
- Title
- Intrinsic And Extrinsic Pinning In Ndfeas(o,f): Vortex Trapping And Lock-in By The Layered Structure.
- Creator
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Tarantini, C., Iida, K., Haenisch, J., Kurth, F., Jaroszynski, J., Sumiya, N., Chihara, M., Hatano, T., Ikuta, H., Schmidt, S., Seidel, P., Holzapfel, B., Larbalestier, D. C.
- Abstract/Description
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Fe-based superconductors (FBS) present a large variety of compounds whose properties are affected to different extents by their crystal structures. Amongst them, the REFeAs(O,F) (RE1111, RE being a rare-earth element) is the family with the highest critical temperature T-c but also with a large anisotropy and Josephson vortices as demonstrated in the flux-flow regime in Sm1111 (T-c similar to 55 K). Here we focus on the pinning properties of the lower-T-c Nd1111 in the flux-creep regime. We...
Show moreFe-based superconductors (FBS) present a large variety of compounds whose properties are affected to different extents by their crystal structures. Amongst them, the REFeAs(O,F) (RE1111, RE being a rare-earth element) is the family with the highest critical temperature T-c but also with a large anisotropy and Josephson vortices as demonstrated in the flux-flow regime in Sm1111 (T-c similar to 55 K). Here we focus on the pinning properties of the lower-T-c Nd1111 in the flux-creep regime. We demonstrate that for H//c critical current density J(c) at high temperatures is dominated by point-defect pinning centres, whereas at low temperatures surface pinning by planar defects parallel to the c-axis and vortex shearing prevail. When the field approaches the ab-planes, two different regimes are observed at low temperatures as a consequence of the transition between 3D Abrikosov and 2D Josephson vortices: one is determined by the formation of a vortex-staircase structure and one by lock-in of vortices parallel to the layers. This is the first study on FBS showing this behaviour in the full temperature, field, and angular range and demonstrating that, despite the lower T-c and anisotropy of Nd1111 with respect to Sm1111, this compound is substantially affected by intrinsic pinning generating a strong ab-peak in J(c).
Show less - Date Issued
- 2016-10-26
- Identifier
- FSU_libsubv1_wos_000386470100001, 10.1038/srep36047
- Format
- Citation
- Title
- Phenomenological Mssm Interpretation Of Cms Searches In Pp Collisions At Root S=7 And 8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Koenig, A., Krammer, M., Kraetschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rad, N., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Van de Klundert, M., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moortgat, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Brun, H., Caillol, C., Clerbaux, B., De Lentdecker, G., Fasanella, G., Favart, L., Goldouzian, R., Grebenyuk, A., Karapostoli, G., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-Conde, A., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Dobur, D., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Rios, A. A. Ocampo, Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Caudron, A., Ceard, L., De Visscher, S., Delaere, C., Delcourt, M., Favart, D., Forthomme, L., Giammanco, A., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Musich, M., Nuttens, C., Perrini, L., Piotrzkowski, K., Quertenmont, L., Selvaggi, M., Marono, M. Vidal, Beliy, N., Hammad, G. H., Alda Junior, W. L., Alves, F. L., Alves, G. A., Brito, L., Correa Martins Junior, M., Hamer, M., Hensel, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., Jesus Damiao, D. De, De Oliveira Martins, C., Fonseca De Souza, S., Huertas Guativa, L. M., Malbouisson, H., Matos Figueiredo, D., Mora Herrera, C., Mundim, L., Nogima, H., Prado Da Silva, W. L., Santoro, A., Sznajder, A., Tonelli Manganote, E. J., Vilela Pereira, A., Ahuja, S., Bernardes, C. A., De Souza Santos, A., Dogra, S., Fernandez Perez Tomei, T. R., Gregores, E. M., Mercadante, P. G., Moon, C. S., Novaes, S. F., Padula, Sandra S., Romero Abad, D., Ruiz Vargas, J. C., Aleksandrov, A., Hadjiiska, R., Iaydjiev, P., Rodozov, M., Stoykova, S., Sultanov, G., Vutova, M., Dimitrov, A., Glushkov, I., Litov, L., Pavlov, B., Petkov, P., Fang, W., Ahmad, M., Bian, J. G., Chen, G. M., Chen, H. S., Chen, M., Cheng, T., Du, R., Jiang, C. H., Leggat, D., Plestina, R., Romeo, F., Shaheen, S. M., Spiezia, A., Tao, J., Wang, C., Wang, Z., Zhang, H., Asawatangtrakuldee, C., Ban, Y., Li, Q., Liu, S., Mao, Y., Qian, S. J., Wang, D., Xu, Z., Avila, C., Cabrera, A., Chaparro Sierra, L. F., Florez, C., Gomez, J. P., Gomez Moreno, B., Sanabria, J. C., Godinovic, N., Lelas, D., Puljak, I., Cipriano, P. M. Ribeiro, Antunovic, Z., Kovac, M., Brigljevic, V., Kadija, K., Luetic, J., Micanovic, S., Sudic, L., Attikis, A., Mavromanolakis, G., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. A., Rykaczewski, H., Finger, M., Finger, M., Elkafrawy, T., Mahmoud, M. A., Mohammed, Y., Calpas, B., Kadastik, M., Murumaa, M., Raidal, M., Tiko, A., Veelken, C., Eerola, P., Pekkanen, J., Voutilainen, M., Harkonen, J., Karimaki, V., Kinnunen, R., Lampen, T., Lassila-Perini, K., Lehti, S., Linden, T., Luukka, P., Peltola, T., Tuominiemi, J., Tuovinen, E., Wendland, L., Talvitie, J., Tuuva, T., Besancon, M., Couderc, F., Dejardin, M., Denegri, D., Fabbro, B., Faure, J. L., Favaro, C., Ferri, F., Ganjour, S., Givernaud, A., Gras, P., de Monchenault, G. Hamel, Jarry, P., Locci, E., Machet, M., Malcles, J., Rander, J., Rosowsky, A., Titov, M., Zghiche, A., Abdulsalam, A., Antropov, I., Oni, S. Ba Ffi, Beaudette, F., Busson, P., Cadamuro, L., Chapon, E., Charlot, C., Davignon, O., Filipovic, N., de Cassagnac, R. Granier, Jo, M., Kraml, S., Lisniak, S., Mine, P., Naranjo, I. N., Nguyen, M., Ochando, C., Ortona, G., Paganini, P., Pigard, P., Regnard, S., Salerno, R., Sirois, Y., Strebler, T., Yilmaz, Y., Zabi, A., Agram, J.-L., Andrea, J., Aubin, A., Bloch, D., Brom, J.-M., Buttignol, M., Chabert, E. C., Chanon, N., Conte, C. Collard E., Coubez, X., Fontaine, J.-C., Gele, D., Goerlach, U., Goetzmann, C., Le Bihan, A.-C., Merlin, J. A., Skovpen, K., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Bouvier, E., Montoya, C. A. Carrillo, Chierici, R., Contardo, D., Courbon, B., Depasse, P., El Mamouni, H., Fan, J., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Lagarde, F., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Popov, A., Alvarez, J. D. Ruiz, Sabes, D., Sordini, V., Vander Donckt, M., Verdier, P., Viret, S., Toriashvili, T., Tsamalaidze, Z., Autermann, C., Beranek, S., Feld, L., Heister, A., Kiesel, M. K., Klein, K., Lipinski, M., Ostapchuk, A., Preuten, M., Raupach, F., Schael, S., Schulte, J. 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I., Henderson, C., Rumerio, P., Arcaro, D., Avetisyan, A., Bose, T., Gastler, D., Rankin, D., Richardson, C., Rohlf, J., Sulak, L., Zou, D., Alimena, J., Benelli, G., Berry, E., Cutts, D., Ferapontov, A., Garabedian, A., Hakala, J., Heintz, U., Jesus, O., Laird, E., Landsberg, G., Mao, Z., Narain, M., Piperov, S., Sagir, S., Syarif, R., Breedon, R., Breto, G., Sanchez, M. Calderon De la Barca, Chauhan, S., Chertok, M., Conway, J., Conway, R., Cox, P. T., Erbacher, R., Funk, G., Gardner, M., Gunion, J., Ko, W., Lander, R., Mclean, C., Mulhearn, M., Pellett, D., Pilot, J., Ricci-Tam, F., Shalhout, S., Smith, J., Squires, M., Stolp, D., Tripathi, M., Wilbur, S., Yohay, R., Cousins, R., Everaerts, P., Florent, A., Hauser, J., Ignatenko, M., Saltzberg, D., Takasugi, E., Valuev, V., Weber, M., Burt, K., Clare, R., Ellison, J., Gary, J. W., Hanson, G., Heilman, J., Paneva, M. Ivova, Jandir, P., Kennedy, E., Lacroix, F., Long, O. R., Malberti, M., Negrete, M. Olmedo, Shrinivas, A., Wei, H., Wimpenny, S., Yates, B. R., Branson, J. G., Cerati, G. B., Cittolin, S., D'Agnolo, R. T., Derdzinski, M., Holzner, A., Kelley, R., Klein, D., Letts, J., Macneill, I., Olivito, D., Padhi, S., Pieri, M., Sani, M., Sharma, V., Simon, S., Tadel, M., Vartak, A., Wasserbaech, S., Welke, C., Wurthwein, F., Yagil, A., Della Porta, G. Zevi, Bradmiller-Feld, J., Campagnari, C., Dishaw, A., Dutta, V., Flowers, K., Sevilla, M. Franco, Geffert, P., George, C., Golf, F., Gouskos, L., Gran, J., Incandela, J., Mccoll, N., Mullin, S. D., Richman, J., Stuart, D., Suarez, I., West, C., Yoo, J., Anderson, D., Apresyan, A., Bendavid, J., Bornheim, A., Bunn, J., Chen, Y., Duarte, J., Mott, A., Newman, H. B., Pena, C., Spiropulu, M., Vlimant, J. R., Xie, S., Zhu, R. Y., Andrews, M. B., Azzolini, V., Calamba, A., Carlson, B., Ferguson, T., Paulini, M., Russ, J., Sun, M., Vogel, H., Vorobiev, I., Cumalat, J. P., Ford, W. T., Gaz, A., Jensen, F., Johnson, A., Krohn, M., Mulholland, T., Nauenberg, U., Stenson, K., Wagner, S. R., Alexander, J., Chatterjee, A., Chaves, J., Chu, J., Dittmer, S., Eggert, N., Mirman, N., Kaufman, G. Nicolas, Patterson, J. R., Rinkevicius, A., Ryd, A., Skinnari, L., Soffi, L., Sun, W., Tan, S. M., Teo, W. D., Thom, J., Thompson, J., Tucker, J., Weng, Y., Wittich, P., Abdullin, S., Albrow, M., Apollinari, G., Banerjee, S., Bauerdick, L. A. T., Beretvas, A., Berryhill, J., Bhat, P. C., Bolla, G., Burkett, K., Butler, J. N., Cheung, H. W. K., Chlebana, F., Cihangir, S., Elvira, V. D., Fisk, I., Freeman, J., Gottschalk, E., Gray, L., Green, D., Grunendahl, S., Gutsche, O., Hanlon, J., Hare, D., Harris, R. M., Hasegawa, S., Hirschauer, J., Hu, Z., Jayatilaka, B., Jindariani, S., Johnson, M., Joshi, U., Klima, B., Kreis, B., Lammel, S., Lewis, J., Linacre, J., Lincoln, D., Lipton, R., Liu, T., De Sa, R. Lopes, Lykken, J., Maeshima, K., Marraffino, J. M., Maruyama, S., Mason, D., McBride, P., Merkel, P., Mrenna, S., Nahn, S., Newman-Holmes, C., O'Dell, V., Pedro, K., Prokofyev, O., Rakness, G., Sexton-Kennedy, E., Soha, A., Spalding, W. J., Spiegel, L., Stoynev, S., Strobbe, N., Taylor, L., Tkaczyk, S., Tran, N. V., Uplegger, L., Vaandering, E. W., Vernieri, C., Verzocchi, M., Vidal, R., Wang, M., Weber, H. A., Whitbeck, A., Acosta, D., Avery, P., Bortignon, P., Bourilkov, D., Brinkerhoff, A., Carnes, A., Carver, M., Curry, D., Das, S., Field, R. D., Furic, I. K., Konigsberg, J., Korytov, A., Kotov, K., Ma, P., Matchev, K., Mei, H., Milenovic, P., Mitselmakher, G., Rank, D., Rossin, R., Shchutska, L., Snowball, M., Sperka, D., Terentyev, N., Thomas, L., Wang, J., Wang, S., Yelton, J., Linn, S., Markowitz, P., Martinez, G., Rodriguez, J. L., Ackert, A., Adams, J. R., Adams, T., Askew, A., Bein, S., Bochenek, J., Diamond, B., Haas, J., Hagopian, S., Hagopian, V., Johnson, K. F., Khatiwada, A., Prosper, H., Weinberg, M., Baarmand, M. M., Bhopatkar, V., Colafranceschi, S., Hohlmann, M., Kalakhety, H., Noonan, D., Roy, T., Yumiceva, F., Adams, M. R., Apanasevich, L., Berry, D., Betts, R. R., Bucinskaite, I., Cavanaugh, R., Evdokimov, O., Gauthier, L., Gerber, C. E., Hofman, D. J., Kurt, P., O'Brien, C., Gonzalez, I. D. Sandoval, Turner, P., Varelas, N., Wu, Z., Zakaria, M., Zhang, J., Bilki, B., Clarida, W., Dilsiz, K., Durgut, S., Gandrajula, R. P., Haytmyradov, M., Khristenko, V., Merlo, J.-P., Mermerkaya, H., Mestvirishvili, A., Moeller, A., Nachtman, J., Ogul, H., Onel, Y., Ozok, F., Penzo, A., Snyder, C., Tiras, E., Wetzel, J., Yi, K., Anderson, I., Barnett, B. A., Blumenfeld, B., Cocoros, A., Eminizer, N., Fehling, D., Feng, L., Gritsan, A. V., Maksimovic, P., Osherson, M., Roskes, J., Sarica, U., Swartz, M., Xiao, M., Xin, Y., You, C., Baringer, P., Bean, A., Bruner, C., Kenny, R. P., Majumder, D., Malek, M., Mcbrayer, W., Murray, M., Sanders, S., Stringer, R., Wang, Q., Ivanov, A., Kaadze, K., Khalil, S., Makouski, M., Maravin, Y., Mohammadi, A., Saini, L. K., Skhirtladze, N., Toda, S., Lange, D., Rebassoo, F., Wright, D., Anelli, C., Baden, A., Baron, O., Belloni, A., Calvert, B., Eno, S. C., Ferraioli, C., Gomez, J. A., Hadley, N. J., Jabeen, S., Kellogg, R. G., Kolberg, T., Kunkle, J., Lu, Y., Mignerey, A. C., Shin, Y. H., Skuja, A., Tonjes, M. B., Tonwar, S. C., Apyan, A., Barbieri, R., Baty, A., Bi, R., Bierwagen, K., Brandt, S., Busza, W., Cali, I. A., Demiragli, Z., Di Matteo, L., Ceballos, G. Gomez, Goncharov, M., Gulhan, D., Iiyama, Y., Innocenti, G. M., Klute, M., Kovalskyi, D., Krajczar, K., Lai, Y. S., Lee, Y.-J., Levin, A., Luckey, P. D., Marini, A. C., Mcginn, C., Mironov, C., Narayanan, S., Niu, X., Paus, C., Roland, C., Roland, G., Salfeld-Nebgen, J., Stephans, G. S. F., Sumorok, K., Tatar, K., Varma, M., Velicanu, D., Veverka, J., Wang, J., Wang, T. W., Wyslouch, B., Yang, M., Zhukova, V., Benvenuti, A. C., Dahmes, B., Evans, A., Finkel, A., Gude, A., Hansen, P., Kalafut, S., Kao, S. C., Klapoetke, K., Kubota, Y., Lesko, Z., Mans, J., Nourbakhsh, S., Ruckstuhl, N., Rusack, R., Tambe, N., Turkewitz, J., Acosta, J. G., Oliveros, S., Avdeeva, E., Bartek, R., Bloom, K., Bose, S., Claes, D. R., Dominguez, A., Fangmeier, C., Suarez, R. Gonzalez, Kamalieddin, R., Knowlton, D., Kravchenko, I., Meier, F., Monroy, J., Ratnikov, F., Siado, J. E., Snow, G. R., Stieger, B., Alyari, M., Dolen, J., George, J., Godshalk, A., Harrington, C., Iashvili, I., Kaisen, J., Kharchilava, A., Kumar, A., Rappoccio, S., Roozbahani, B., Alverson, G., Barberis, E., Baumgartel, D., Chasco, M., Hortiangtham, A., Massironi, A., Morse, D. M., Nash, D., Orimoto, T., De Lima, R. Teixeira, Trocino, D., Wang, R.-J., Wood, D., Zhang, J., Bhattacharya, S., Hahn, K. A., Kubik, A., Low, J. F., Mucia, N., Odell, N., Pollack, B., Schmitt, M. H., Sung, K., Trovato, M., Velasco, M., Dev, N., Hildreth, M., Jessop, C., Karmgard, D. J., Kellams, N., Lannon, K., Marinelli, N., Meng, F., Mueller, C., Musienko, Y., Planer, M., Reinsvold, A., Ruchti, R., Rupprecht, N., Smith, G., Taroni, S., Valls, N., Wayne, M., Wolf, M., Woodard, A., Antonelli, L., Brinson, J., Bylsma, B., Durkin, L. S., Flowers, S., Hart, A., Hill, C., Hughes, R., Ji, W., Ling, T. Y., Liu, B., Luo, W., Puigh, D., Rodenburg, M., Winer, B. L., Wulsin, H. W., Driga, O., Elmer, P., Hardenbrook, J., Hebda, P., Koay, S. A., Lujan, P., Marlow, D., Medvedeva, T., Mooney, M., Olsen, J., Palmer, C., Piroue, P., Stickland, D., Tully, C., Zuranski, A., Malik, S., Barker, A., Barnes, V. E., Benedetti, D., Bortoletto, D., Gutay, L., Jha, M. K., Jones, M., Jung, A. W., Jung, K., Miller, D. H., Neumeister, N., Radburn-Smith, B. C., Shi, X., Shipsey, I., Silvers, D., Sun, J., Svyatkovskiy, A., Wang, F., Xie, W., Xu, L., Parashar, N., Stupak, J., Adair, A., Akgun, B., Chen, Z., Ecklund, K. M., Geurts, F. J. M., Guilbaud, M., Li, W., Michlin, B., Northup, M., Padley, B. P., Redjimi, R., Roberts, J., Rorie, J., Tu, Z., Zabel, J., Betchart, B., Bodek, A., de Barbaro, P., Demina, R., Eshaq, Y., Ferbel, T., Galanti, M., Garcia-Bellido, A., Han, J., Hindrichs, O., Khukhunaishvili, A., Lo, K. H., Tan, P., Verzetti, M., Chou, J. P., Contreras-Campana, E., Ferencek, D., Gershtein, Y., Halkiadakis, E., Heindl, M., Hidas, D., Hughes, E., Kaplan, S., Elayavalli, R. Kunnawalkam, Lath, A., Nash, K., Saka, H., Salur, S., Schnetzer, S., Sheffield, D., Somalwar, S., Stone, R., Thomas, S., Thomassen, P., Walker, M., Foerster, M., Riley, G., Rose, K., Spanier, S., Thapa, K., Bouhali, O., Hernandez, A. Castaneda, Celik, A., Dalchenko, M., De Mattia, M., Delgado, A., Dildick, S., Eusebi, R., Gilmore, J., Huang, T., Kamon, T., Krutelyov, V., Mueller, R., Osipenkov, I., Pakhotin, Y., Patel, R., Perloff, A., Rathjens, D., Rose, A., Safonov, A., Tatarinov, A., Ulmer, K. A., Akchurin, N., Cowden, C., Damgov, J., Dragoiu, C., Dudero, P. R., Faulkner, J., Kunori, S., Lamichhane, K., Lee, S. W., Libeiro, T., Undleeb, S., Volobouev, I., Appelt, E., Delannoy, A. G., Greene, S., Gurrola, A., Janjam, R., Johns, W., Maguire, C., Mao, Y., Melo, A., Ni, H., Sheldon, P., Tuo, S., Velkovska, J., Xu, Q., Arenton, M. W., Barria, P., Cox, B., Francis, B., Goodell, J., Hirosky, R., Ledovskoy, A., Li, H., Neu, C., Sinthuprasith, T., Sun, X., Wang, Y., Wolfe, E., Wood, J., Xia, F., Clarke, C., Harr, R., Karchin, P. E., Don, C. Kottachchi Kankanamge, Lamichhane, P., Sturdy, J., Belknap, D. A., Carlsmith, D., Dasu, S., Dodd, L., Duric, S., Gomber, B., Grothe, M., Herndon, M., Herve, A., Klabbers, P., Lanaro, A., Levine, A., Long, K., Loveless, R., Mohapatra, A., Ojalvo, I., Perry, T., Pierro, G. A., Polese, G., Ruggles, T., Sarangi, T., Savin, A., Sharma, A., Smith, N., Smith, W. H., Taylor, D., Verwilligen, P., Woods, N.
Show less - Abstract/Description
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Searches for new physics by the CMS collaboration are interpreted in the framework of the phenomenological minimal supersymmetric standard model (pMSSM). The data samples used in this study were collected at root s = 7 and 8 TeV and have integrated luminosities of 5.0 fb(-1) and 19.5 fb(-1), respectively. A global Bayesian analysis is performed, incorporating results from a broad range of CMS supersymmetry searches, as well as constraints from other experiments. Because the pMSSM incorporates...
Show moreSearches for new physics by the CMS collaboration are interpreted in the framework of the phenomenological minimal supersymmetric standard model (pMSSM). The data samples used in this study were collected at root s = 7 and 8 TeV and have integrated luminosities of 5.0 fb(-1) and 19.5 fb(-1), respectively. A global Bayesian analysis is performed, incorporating results from a broad range of CMS supersymmetry searches, as well as constraints from other experiments. Because the pMSSM incorporates several well-motivated assumptions that reduce the 120 parameters of the MSSM to just 19 parameters defined at the electroweak scale, it is possible to assess the results of the study in a relatively straightforward way. Approximately half of the model points in a potentially accessible subspace of the pMSSM are excluded, including all pMSSM model points with a gluino mass below 500 GeV, as well as models with a squark mass less than 300 GeV. Models with chargino and neutralino masses below 200 GeV are disfavored, but no mass range of model points can be ruled out based on the analyses considered. The nonexcluded regions in the pMSSM parameter space are characterized in terms of physical processes and key observables, and implications for future searches are discussed.
Show less - Date Issued
- 2016-10-24
- Identifier
- FSU_libsubv1_wos_000387226700001, 10.1007/JHEP10(2016)129
- Format
- Citation
- Title
- Evidence For Impact Ionization In Vanadium Dioxide.
- Creator
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Holleman, Joshua, Bishop, Michael M., Garcia, Carlos, Winfred, J. S. R. Vellore, Lee, Shinbuhm, Lee, Ho Nyung, Beekman, Christianne, Manousakis, Efstratios, McGill, Stephen A.
- Abstract/Description
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Pump-probe optical spectroscopy was used to investigate proposed charge-carrier multiplication via impact ionization in the M-1 insulating phase of VO2. By comparing the transient reflectivities of the film when pumped at less than and then more than twice the band-gap energy, we observed a larger ultrafast response with the higher energy pump color while the film was still transiently in the insulating phase. We additionally identified multiple time scales within the charge dynamics and...
Show morePump-probe optical spectroscopy was used to investigate proposed charge-carrier multiplication via impact ionization in the M-1 insulating phase of VO2. By comparing the transient reflectivities of the film when pumped at less than and then more than twice the band-gap energy, we observed a larger ultrafast response with the higher energy pump color while the film was still transiently in the insulating phase. We additionally identified multiple time scales within the charge dynamics and analyzed how these changed when the pump and probe wavelengths were varied. This experiment provided evidence that a fast carrier multiplication process, i.e., impact ionization, acts efficiently in this prototypical strongly correlated insulator, as was recently predicted by theoretical calculations.
Show less - Date Issued
- 2016-10-17
- Identifier
- FSU_libsubv1_wos_000386097100004, 10.1103/PhysRevB.94.155129
- Format
- Citation
- Title
- A route for a strong increase of critical current in nanostrained iron-based superconductors.
- Creator
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Ozaki, Toshinori, Wu, Lijun, Zhang, Cheng, Jaroszynski, Jan, Si, Weidong, Zhou, Juan, Zhu, Yimei, Li, Qiang
- Abstract/Description
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The critical temperature T-c and the critical current density J(c) determine the limits to large-scale superconductor applications. Superconductivity emerges at T-c. The practical current-carrying capability, measured by J(c), is the ability of defects in superconductors to pin the magnetic vortices, and that may reduce T-c. Simultaneous increase of T-c and J(c) in superconductors is desirable but very difficult to realize. Here we demonstrate a route to raise both T-c and J(c) together in...
Show moreThe critical temperature T-c and the critical current density J(c) determine the limits to large-scale superconductor applications. Superconductivity emerges at T-c. The practical current-carrying capability, measured by J(c), is the ability of defects in superconductors to pin the magnetic vortices, and that may reduce T-c. Simultaneous increase of T-c and J(c) in superconductors is desirable but very difficult to realize. Here we demonstrate a route to raise both T-c and J(c) together in iron-based superconductors. By using low-energy proton irradiation, we create cascade defects in FeSe0.5Te0.5 films. T-c is enhanced due to the nanoscale compressive strain and proximity effect, whereas J(c) is doubled under zero field at 4.2 K through strong vortex pinning by the cascade defects and surrounding nanoscale strain. At 12 K and above 15 T, one order of magnitude of J(c) enhancement is achieved in both parallel and perpendicular magnetic fields to the film surface.
Show less - Date Issued
- 2016-10-06
- Identifier
- FSU_libsubv1_wos_000385556300001, 10.1038/ncomms13036
- Format
- Citation
- Title
- Thermodynamic Measurement Of Angular Anisotropy At The Hidden Order Transition Of Uru2si2.
- Creator
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Trinh, Jennifer, Bruck, Ekkes, Siegrist, Theo, Flint, Rebecca, Chandra, Premala, Coleman, Piers, Ramirez, Arthur P.
- Abstract/Description
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The heavy fermion compound URu2Si2 continues to attract great interest due to the unidentified hidden order it develops below 17.5 K. The unique Ising character of the spin fluctuations and low-temperature quasiparticles is well established. We present detailed measurements of the angular anisotropy of the nonlinear magnetization that reveal a cos(4)theta Ising anisotropy both at and above the ordering transition. With Landau theory, we show this implies a strongly Ising character of the...
Show moreThe heavy fermion compound URu2Si2 continues to attract great interest due to the unidentified hidden order it develops below 17.5 K. The unique Ising character of the spin fluctuations and low-temperature quasiparticles is well established. We present detailed measurements of the angular anisotropy of the nonlinear magnetization that reveal a cos(4)theta Ising anisotropy both at and above the ordering transition. With Landau theory, we show this implies a strongly Ising character of the itinerant hidden order parameter.
Show less - Date Issued
- 2016-10-05
- Identifier
- FSU_libsubv1_wos_000385341600008, 10.1103/PhysRevLett.117.157201
- Format
- Citation
- Title
- Evidence For Correlated Dynamics Near The Berezinskii-kosterlitz-thouless-like Transition In Highly Underdoped La2-xsrxcuo4.
- Creator
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Shi, Zhenzhong, Shi, Xiaoyan, Popovic, Dragana
- Abstract/Description
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A low-frequency resistance noise study in highly underdoped thick films of La2-xSrxCuO4 (x = 0.07 and 0.08) reveals slow, correlated dynamics and breaking of ergodicity near the superconducting transition of the Berezinskii-Kosterlitz-Thouless type. The observed correlated behavior is strongly suppressed by disorder.
- Date Issued
- 2016-10-05
- Identifier
- FSU_libsubv1_wos_000385239900002, 10.1103/PhysRevB.94.134503
- Format
- Citation
- Title
- Magnetoelectric Coupling Through The Spin Flop Transition In Ni3teo6.
- Creator
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Yokosuk, M. O., al-Wahish, Amal, Artyukhin, Sergey, O'Neal, K. R., Mazumdar, D., Chen, P., Yang, Junjie, Oh, Yoon Seok, McGill, Stephen A., Haule, K., Cheong, Sang-Wook,...
Show moreYokosuk, M. O., al-Wahish, Amal, Artyukhin, Sergey, O'Neal, K. R., Mazumdar, D., Chen, P., Yang, Junjie, Oh, Yoon Seok, McGill, Stephen A., Haule, K., Cheong, Sang-Wook, Vanderbilt, David, Musfeldt, J. L.
Show less - Abstract/Description
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We combined high field optical spectroscopy and first principles calculations to analyze the electronic structure of Ni3TeO6 across the 53 K and 9 T magnetic transitions, both of which are accompanied by large changes in electric polarization. The color properties are sensitive to magnetic order due to field-induced changes in the crystal field environment, with those around Ni1 and Ni2 most affected. These findings advance the understanding of magnetoelectric coupling in materials in which...
Show moreWe combined high field optical spectroscopy and first principles calculations to analyze the electronic structure of Ni3TeO6 across the 53 K and 9 T magnetic transitions, both of which are accompanied by large changes in electric polarization. The color properties are sensitive to magnetic order due to field-induced changes in the crystal field environment, with those around Ni1 and Ni2 most affected. These findings advance the understanding of magnetoelectric coupling in materials in which magnetic 3d centers coexist with nonmagnetic heavy chalcogenide cations.
Show less - Date Issued
- 2016-09-30
- Identifier
- FSU_libsubv1_wos_000385971800013, 10.1103/PhysRevLett.117.147402
- Format
- Citation
- Title
- Electrical Transport Properties Of Single-crystal Cab6, Srb6, And Bab6.
- Creator
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Stankiewicz, Jolanta, Rosa, Priscila F. S., Schlottmann, Pedro, Fisk, Zachary
- Abstract/Description
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The electrical resistivity and Hall effect of alkaline-earth-metal hexaboride single crystals are measured as a function of temperature, hydrostatic pressure, and magnetic field. The transport properties vary weakly with the external parameters and are modeled in terms of intrinsic variable-valence defects. These defects can stay either in (1) delocalized shallow levels or in (2) localized levels resonant with the conduction band, which can be neutral or negatively charged. Satisfactory...
Show moreThe electrical resistivity and Hall effect of alkaline-earth-metal hexaboride single crystals are measured as a function of temperature, hydrostatic pressure, and magnetic field. The transport properties vary weakly with the external parameters and are modeled in terms of intrinsic variable-valence defects. These defects can stay either in (1) delocalized shallow levels or in (2) localized levels resonant with the conduction band, which can be neutral or negatively charged. Satisfactory agreement is obtained for electronic transport properties in a broad temperature and pressure range, although fitting the magnetoresistance is less straightforward and a combination of various mechanisms is needed to explain the field and temperature dependences.
Show less - Date Issued
- 2016-09-22
- Identifier
- FSU_libsubv1_wos_000383865700005, 10.1103/PhysRevB.94.125141
- Format
- Citation
- Title
- Fate Of Spinons At The Mott Point.
- Creator
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Lee, Tsung-Han, Florens, Serge, Dobrosavljevic, Vladimir
- Abstract/Description
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Gapless spin liquids have recently been observed in several frustrated Mott insulators, with elementary spin excitations-"spinons"-reminiscent of degenerate Fermi systems. However, their precise role at the Mott point, where charge fluctuations begin to proliferate, remains controversial and ill understood. Here we present the simplest theoretical framework that treats the dynamics of emergent spin and charge excitations on the same footing, providing a new physical picture of the Mott metal...
Show moreGapless spin liquids have recently been observed in several frustrated Mott insulators, with elementary spin excitations-"spinons"-reminiscent of degenerate Fermi systems. However, their precise role at the Mott point, where charge fluctuations begin to proliferate, remains controversial and ill understood. Here we present the simplest theoretical framework that treats the dynamics of emergent spin and charge excitations on the same footing, providing a new physical picture of the Mott metal-to-insulator transition at half filing. We identify a generic orthogonality mechanism leading to strong damping of spinons, arising as soon as the Mott gap closes. Our results indicate that spinons should not play a significant role within the high-temperature quantum critical regime above the Mott point-in striking agreement with all available experiments.
Show less - Date Issued
- 2016-09-20
- Identifier
- FSU_libsubv1_wos_000383849400011, 10.1103/PhysRevLett.117.136601
- Format
- Citation
- Title
- Magnetic Phases Of The Quasi-two-dimensional Antiferromagnet Cucro2 On A Triangular Lattice.
- Creator
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Sakhratov, Yu A., Svistov, L. E., Kuhns, P. L., Zhou, H. D., Reyes, A. P.
- Abstract/Description
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We have carried out Cu-63,Cu-65 NMR spectra measurements in a magnetic field up to about 45 T on a single crystal of a multiferroic triangular antiferromagnet CuCrO2. The measurements were performed for magnetic fields aligned along the crystal c axis. Field and temperature evolution of the spectral shape demonstrates a number of phase transitions. It was found that the 3D magnetic ordering takes place in the low field range (H less than or similar to 15 T). At higher fields magnetic...
Show moreWe have carried out Cu-63,Cu-65 NMR spectra measurements in a magnetic field up to about 45 T on a single crystal of a multiferroic triangular antiferromagnet CuCrO2. The measurements were performed for magnetic fields aligned along the crystal c axis. Field and temperature evolution of the spectral shape demonstrates a number of phase transitions. It was found that the 3D magnetic ordering takes place in the low field range (H less than or similar to 15 T). At higher fields magnetic structures form within individual triangular planes whereas the spin directions of the magnetic ions from neighboring planes are not correlated. It is established that the 2D-3D transition is hysteretic in field and temperature. Line-shape analysis reveals several possible magnetic structures existing within individual planes for different phases of CuCrO2. Within certain regions on the magnetic H-T phase diagram of CuCrO2 a 3D magnetic ordering with tensor order parameter is expected.
Show less - Date Issued
- 2016-09-12
- Identifier
- FSU_libsubv1_wos_000383138700003, 10.1103/PhysRevB.94.094410
- Format
- Citation
- Title
- Interlayer Electronic Transport In Camnbi2 Antiferromagnet.
- Creator
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Wang, Aifeng, Graf, D., Wu, Lijun, Wang, Kefeng, Bozin, E., Zhu, Yimei, Petrovic, C.
- Abstract/Description
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We report interlayer electronic transport in CaMnBi2 single crystals. Quantum oscillations and angular magnetoresistance suggest coherent electronic conduction and valley polarized conduction of Dirac states. The small cyclotron mass, high mobility of carriers, and nontrivial Berry's phase are consistent with the presence of Dirac fermions on the side wall of the warped cylindrical Fermi surface. Similarly to SrMnBi2, which features an anisotropic Dirac cone, our results suggest that magnetic...
Show moreWe report interlayer electronic transport in CaMnBi2 single crystals. Quantum oscillations and angular magnetoresistance suggest coherent electronic conduction and valley polarized conduction of Dirac states. The small cyclotron mass, high mobility of carriers, and nontrivial Berry's phase are consistent with the presence of Dirac fermions on the side wall of the warped cylindrical Fermi surface. Similarly to SrMnBi2, which features an anisotropic Dirac cone, our results suggest that magnetic-field-induced changes in interlayer conduction are also present in layered bismuth-based materials with a zero-energy line in momentum space created by the staggered alkaline earth atoms.
Show less - Date Issued
- 2016-09-12
- Identifier
- FSU_libsubv1_wos_000383145300004, 10.1103/PhysRevB.94.125118
- Format
- Citation
- Title
- Non-ising-like Two-dimensional Superconductivity In A Bulk Single Crystal.
- Creator
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Zhang, Q. R., Rhodes, D., Zeng, B., Johannes, M. D., Balicas, L.
- Abstract/Description
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Both Nb3PdxSe7 and Ta4Pd3Te16 crystallize in a monoclinic point group while exhibiting superconducting transition temperatures as high as T-c similar to 3.5 and similar to 4.7K, respectively. Disorder was claimed to lead to the extremely large upper critical fields (H-c2) observed in related compounds. Despite the presence of disorder and heavier elements, H-c2s in Ta4Pd3Te16 are found to be considerably smaller than those of Nb3PdxSe7 while displaying an anomalous, nonsaturating linear...
Show moreBoth Nb3PdxSe7 and Ta4Pd3Te16 crystallize in a monoclinic point group while exhibiting superconducting transition temperatures as high as T-c similar to 3.5 and similar to 4.7K, respectively. Disorder was claimed to lead to the extremely large upper critical fields (H-c2) observed in related compounds. Despite the presence of disorder and heavier elements, H-c2s in Ta4Pd3Te16 are found to be considerably smaller than those of Nb3PdxSe7 while displaying an anomalous, nonsaturating linear dependence on temperature T for fields along all three crystallographic axes. In contrast, crystals of the latter compound displaying the highest T(c)s display H-c2 alpha (1-T/T-c)(1/2), which in monolayers of transition metal dichalcogenides is claimed to be evidence for an Ising paired superconducting state resulting from strong spin-orbit coupling. This anomalous T dependence indicates that the superconducting state of Nb3PdxSe7 is quasi-two-dimensional in nature. This is further supported by a nearly divergent anisotropy in upper-critical fields, i.e., gamma= H-c2(b)/H-c2(a)', upon approaching T-c. Hence, in Nb3PdxSe7 the increase of T-c correlates with a marked reduction in electronic dimensionality as observed, for example, in intercalated FeSe. For the Nb compound, Density functional theory (DFT) calculations indicate that an increase in the external field produces an anisotropic orbital response, with especially strong polarization at the Pd sites when the field is perpendicular to their square planar environment. The field also produces an anisotropic spin moment at both Pd sites. Therefore, DFT suggests the field-induced pinning of the spin to the lattice as a possible mechanism for decoupling the superconducting planes.
Show less - Date Issued
- 2016-09-12
- Identifier
- FSU_libsubv1_wos_000383138700005, 10.1103/PhysRevB.94.094511
- Format
- Citation
- Title
- Spatially Inhomogeneous Electron State Deep In The Extreme Quantum Limit Of Strontium Titanate.
- Creator
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Bhattacharya, Anand, Skinner, Brian, Khalsa, Guru, Suslov, Alexey V.
- Abstract/Description
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When an electronic system is subjected to a sufficiently strong magnetic field that the cyclotron energy is much larger than the Fermi energy, the system enters the extreme quantum limit (EQL) and becomes susceptible to a number of instabilities. Bringing a three-dimensional electronic system deeply into the EQL can be difficult however, since it requires a small Fermi energy, large magnetic field, and low disorder. Here we present an experimental study of the EQL in lightly-doped single...
Show moreWhen an electronic system is subjected to a sufficiently strong magnetic field that the cyclotron energy is much larger than the Fermi energy, the system enters the extreme quantum limit (EQL) and becomes susceptible to a number of instabilities. Bringing a three-dimensional electronic system deeply into the EQL can be difficult however, since it requires a small Fermi energy, large magnetic field, and low disorder. Here we present an experimental study of the EQL in lightly-doped single crystals of strontium titanate. Our experiments probe deeply into the regime where theory has long predicted an interaction-driven charge density wave or Wigner crystal state. A number of interesting features arise in the transport in this regime, including a striking re-entrant nonlinearity in the current-voltage characteristics. We discuss these features in the context of possible correlated electron states, and present an alternative picture based on magnetic-field induced puddling of electrons.
Show less - Date Issued
- 2016-09
- Identifier
- FSU_libsubv1_wos_000385388600001, 10.1038/ncomms12974
- Format
- Citation
- Title
- Determination Of The Effective Kinematic Viscosity For The Decay Of Quasiclassical Turbulence In Superfluid He-4.
- Creator
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Gao, J., Guo, W., Vinen, W. F.
- Abstract/Description
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The energy dissipation of quasiclassical homogeneous turbulence in superfluid He-4 (He II) is controlled by an effective kinematic viscosity nu', which relates the energy decay rate dE / dt to the density of quantized vortex lines L as dE / dt = -nu'(kappa L)(2). The precise value of nu' is of fundamental importance in developing our understanding of the dissipation mechanism in He II, and it is also needed in many high-Reynolds-number turbulence experiments and model testing that use He II...
Show moreThe energy dissipation of quasiclassical homogeneous turbulence in superfluid He-4 (He II) is controlled by an effective kinematic viscosity nu', which relates the energy decay rate dE / dt to the density of quantized vortex lines L as dE / dt = -nu'(kappa L)(2). The precise value of nu' is of fundamental importance in developing our understanding of the dissipation mechanism in He II, and it is also needed in many high-Reynolds-number turbulence experiments and model testing that use He II as the working fluid. However, a reliable determination of nu' requires the measurements of both E(t) and L(t), which was never achieved. Here we discuss our study of the quasiclassical turbulence that emerges in the decay of thermal counterflow in He II above 1 K. We were able to measure E(t) by using a recently developed flow-visualization technique and L(t) via second-sound attenuation. We report the nu' values in a wide temperature range determined from a comparison of the time evolution of E(t) and L(t).
Show less - Date Issued
- 2016-09-01
- Identifier
- FSU_libsubv1_wos_000383033500004, 10.1103/PhysRevB.94.094502
- Format
- Citation
- Title
- Hall Effect Within The Colossal Magnetoresistive Semimetallic State Of Mote2.
- Creator
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Zhou, Qiong, Rhodes, D., Zhang, Q. R., Tang, S., Schoenemann, R., Balicas, L.
- Abstract/Description
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Here, we report a systematic study on the Hall effect of the semimetallic state of bulk MoTe2, which was recently claimed to be a candidate for a novel type of Weyl semimetallic state. The temperature (T) dependence of the carrier densities and of their mobilities, as estimated from a numerical analysis based on the isotropic two-carrier model, indicates that its exceedingly large and nonsaturating magnetoresistance may be attributed to a near perfect compensation between the densities of...
Show moreHere, we report a systematic study on the Hall effect of the semimetallic state of bulk MoTe2, which was recently claimed to be a candidate for a novel type of Weyl semimetallic state. The temperature (T) dependence of the carrier densities and of their mobilities, as estimated from a numerical analysis based on the isotropic two-carrier model, indicates that its exceedingly large and nonsaturating magnetoresistance may be attributed to a near perfect compensation between the densities of electrons and holes at low temperatures. A sudden increase in hole density, with a concomitant rapid increase in the electron mobility below T similar to 40 K, leads to comparable densities of electrons and holes at low temperatures suggesting a possible electronic phase transition around this temperature.
Show less - Date Issued
- 2016-09-01
- Identifier
- FSU_libsubv1_wos_000383035100001, 10.1103/PhysRevB.94.121101
- Format
- Citation
- Title
- Weathering Of Oil Spilled In The Marine Environment.
- Creator
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Tarr, Matthew A., Zito, Phoebe, Overton, Edward B., Olson, Gregory M., Adhikari, Puspa L., Reddy, Christopher M.
- Abstract/Description
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Crude oil is a complex mixture of many thousands of mostly hydrocarbon and nitrogen-, sulfur-, and oxygen-containing compounds with molecular weights ranging from below 70 Da to well over 2,000 Da. When this complex mixture enters the environment from spills, ruptures, blowouts, or seeps, it undergoes a continuous series of compositional changes that result from a process known as weathering. Spills of petroleum involving human activity generally result in more rapid input of crude oil or...
Show moreCrude oil is a complex mixture of many thousands of mostly hydrocarbon and nitrogen-, sulfur-, and oxygen-containing compounds with molecular weights ranging from below 70 Da to well over 2,000 Da. When this complex mixture enters the environment from spills, ruptures, blowouts, or seeps, it undergoes a continuous series of compositional changes that result from a process known as weathering. Spills of petroleum involving human activity generally result in more rapid input of crude oil or refined products (diesel, gasoline, heavy fuel oil, and diluted bitumens) to the marine system than do natural processes and urban runoffs. The primary physicochemical processes involved in weathering include evaporation, dissolution, emulsification, dispersion, sedimentation/flocculation, microbial degradation, and photooxidation.
Show less - Date Issued
- 2016-09
- Identifier
- FSU_libsubv1_wos_000382334500019, 10.5670/oceanog.2016.77
- Format
- Citation
- Title
- Seafood And Beach Safety In The Aftermath Of The Deepwater Horizon Oil Spill.
- Creator
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Dickey, Robert, Huettel, Markus
- Abstract/Description
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The 2010 explosion and sinking of the Deepwater Horizon oil platform in the Gulf of Mexico resulted in the largest oil spill the United States has ever endured. The oil spill raised many public health and environmental concerns, including those about the safety of Gulf seafood and public beaches. Analysis of seafood and coastal beaches in the aftermath of the oil spill indicated that public health risks from exposure to harmful crude oil residues returned to pre-spill levels soon after the...
Show moreThe 2010 explosion and sinking of the Deepwater Horizon oil platform in the Gulf of Mexico resulted in the largest oil spill the United States has ever endured. The oil spill raised many public health and environmental concerns, including those about the safety of Gulf seafood and public beaches. Analysis of seafood and coastal beaches in the aftermath of the oil spill indicated that public health risks from exposure to harmful crude oil residues returned to pre-spill levels soon after the oil spill had dissipated. However, the official seafood risk assessment elicited concerns about the inclusion of vulnerable populations, and gaps in toxicological knowledge and related risk information about many of the harmful components in crude oil. Residual crude oil may persist in water-saturated sediments and submerged oil mats that can act as sources for remobilization and future exposures. The response to the Deepwater Horizon event revealed a lack of adequate demographic and human health baseline data, benchmark environmental contaminant data, effective risk communication strategies, and integrated surveillance systems linking human and environmental health status and trends. The development of such knowledge would help improve responses and outcomes to future large-scale catastrophic events.
Show less - Date Issued
- 2016-09
- Identifier
- FSU_libsubv1_wos_000382334500025, 10.5670/oceanog.2016.83
- Format
- Citation
- Title
- Structure And Ferromagnetic Instability Of The Oxygen-deficient Srtio3 Surface.
- Creator
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Ghosh, Soham S., Manousakis, Efstratios
- Abstract/Description
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SrTiO3 (STO) is the substrate of choice to grow oxide thin films and oxide heterojunctions, which can form quasi-two-dimensional electronic phases that exhibit a wealth of phenomena, and thus a workhorse in the emerging field of metal-oxide electronics. Hence, it is of great importance to know the exact character of the STO surface itself under various oxygen environments. Using density functional theory within the spin generalized gradient approximation we have investigated the structural,...
Show moreSrTiO3 (STO) is the substrate of choice to grow oxide thin films and oxide heterojunctions, which can form quasi-two-dimensional electronic phases that exhibit a wealth of phenomena, and thus a workhorse in the emerging field of metal-oxide electronics. Hence, it is of great importance to know the exact character of the STO surface itself under various oxygen environments. Using density functional theory within the spin generalized gradient approximation we have investigated the structural, electronic, and magnetic properties of the oxygen-deficient STO surface. We find that the surface oxygen vacancies order in periodic arrays giving rise to surface magnetic moments and a quasi-two-dimensional electron gas in the occupied Ti 3d orbitals. The surface confinement, the oxygen-vacancy ordering, and the octahedra distortions give rise to spin-polarized t(2g) dispersive subbands; their energy split near the Brillouin zone center acts as an effective Zeeman term, which, when we turn on a Rashba interaction, produces bands with momentum-spin correlations similar to those recently discovered on oxygen-deficient STO surface.
Show less - Date Issued
- 2016-08-24
- Identifier
- FSU_libsubv1_wos_000381890100001, 10.1103/PhysRevB.94.085141
- Format
- Citation
- Title
- Interaction-driven Spontaneous Quantum Hall Effect On A Kagome Lattice.
- Creator
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Zhu, W., Gong, Shou-Shu, Zeng, Tian-Sheng, Fu, Liang, Sheng, D. N.
- Abstract/Description
-
Topological states of matter have been widely studied as being driven by an external magnetic field, intrinsic spin-orbital coupling, or magnetic doping. Here, we unveil an interaction-driven spontaneous quantum Hall effect (a Chern insulator) emerging in an extended fermion-Hubbard model on a kagome lattice, based on a state-of-the-art density-matrix renormalization group on cylinder geometry and an exact diagonalization in torus geometry. We first demonstrate that the proposed model...
Show moreTopological states of matter have been widely studied as being driven by an external magnetic field, intrinsic spin-orbital coupling, or magnetic doping. Here, we unveil an interaction-driven spontaneous quantum Hall effect (a Chern insulator) emerging in an extended fermion-Hubbard model on a kagome lattice, based on a state-of-the-art density-matrix renormalization group on cylinder geometry and an exact diagonalization in torus geometry. We first demonstrate that the proposed model exhibits an incompressible liquid phase with doublet degenerate ground states as time-reversal partners. The explicit spontaneous time-reversal symmetry breaking is determined by emergent uniform circulating loop currents between nearest neighbors. Importantly, the fingerprint topological nature of the ground state is characterized by quantized Hall conductance. Thus, we identify the liquid phase as a quantum Hall phase, which provides a "proof-of-principle" demonstration of the interaction-driven topological phase in a topologically trivial noninteracting band.
Show less - Date Issued
- 2016-08-23
- Identifier
- FSU_libsubv1_wos_000382007600009, 10.1103/PhysRevLett.117.096402
- Format
- Citation
- Title
- Melting Of Wigner Crystal In High-mobility N-gaas/algaas Heterostructures At Filling Factors 0.18 > Nu > 0.125: Acoustic Studies.
- Creator
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Drichko, I. L., Smirnov, I. Yu, Suslov, A. V., Galperin, Y. M., Pfeiffer, L. N., West, K. W.
- Abstract/Description
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By using acoustic methods the complex high-frequency conductance of high-mobility n-GaAs/AlGaAs heterostructures was determined in magnetic fields 12-18 T. Based on the observed frequency and temperature dependences, we conclude that in the investigated magnetic field range and at sufficiently low temperatures, T less than or similar to 200 mK, the electron system forms a Wigner crystal deformed due to pinning by disorder. At some temperature, which depends on the electron filling factor, the...
Show moreBy using acoustic methods the complex high-frequency conductance of high-mobility n-GaAs/AlGaAs heterostructures was determined in magnetic fields 12-18 T. Based on the observed frequency and temperature dependences, we conclude that in the investigated magnetic field range and at sufficiently low temperatures, T less than or similar to 200 mK, the electron system forms a Wigner crystal deformed due to pinning by disorder. At some temperature, which depends on the electron filling factor, the temperature dependences of both components of the complex conductance get substantially changed. We have ascribed this rapid change of the conduction mechanism to melting of the Wigner crystal and study the dependence of the so-defined melting temperature on the electron filling factor.
Show less - Date Issued
- 2016-08-15
- Identifier
- FSU_libsubv1_wos_000381482600007, 10.1103/PhysRevB.94.075420
- Format
- Citation
- Title
- Variational Monte Carlo Study Of Chiral Spin Liquid In Quantum Antiferromagnet On The Triangular Lattice.
- Creator
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Hu, Wen-Jun, Gong, Shou-Shu, Sheng, D. N.
- Abstract/Description
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By using Gutzwiller projected fermionic wave functions and variational Monte Carlo technique, we study the spin-1/2 Heisenberg model with the first-neighbor (J(1)), second-neighbor (J(2)), and additional scalar chiral interaction J(chi)S(i) . (S-j x S-k) on the triangular lattice. In the nonmagnetic phase of the J(1)-J(2) triangular model with 0.08 less than or similar to J(2)/J(1) less than or similar to 0.16, recent density-matrix renormalization group (DMRG) studies [Zhu and White, Phys....
Show moreBy using Gutzwiller projected fermionic wave functions and variational Monte Carlo technique, we study the spin-1/2 Heisenberg model with the first-neighbor (J(1)), second-neighbor (J(2)), and additional scalar chiral interaction J(chi)S(i) . (S-j x S-k) on the triangular lattice. In the nonmagnetic phase of the J(1)-J(2) triangular model with 0.08 less than or similar to J(2)/J(1) less than or similar to 0.16, recent density-matrix renormalization group (DMRG) studies [Zhu and White, Phys. Rev. B 92, 041105(R) (2015) and Hu, Gong, Zhu, and Sheng, Phys. Rev. B 92, 140403(R) (2015)] find a possible gapped spin liquid with the signal of a competition between a chiral and a Z(2) spin liquid. Motivated by the DMRG results, we consider the chiral interaction J(chi)S(i) . (S-j x S-k) as a perturbation for this nonmagnetic phase. We find that with growing J(chi), the gapless U(1) Dirac spin liquid, which has the best variational energy for J(chi) = 0, exhibits the energy instability towards a gapped spin liquid with nontrivial magnetic fluxes and nonzero chiral order. We calculate topological Chern number and ground-state degeneracy, both of which identify this flux state as the chiral spin liquid with fractionalized Chern number C = 1/2 and twofold topological degeneracy. Our results indicate a positive direction to stabilize a chiral spin liquid near the nonmagnetic phase of the J(1)-J(2) triangular model.
Show less - Date Issued
- 2016-08-15
- Identifier
- FSU_libsubv1_wos_000381482600002, 10.1103/PhysRevB.94.075131
- Format
- Citation
- Title
- Tunable Symmetries of Integer and Fractional Quantum Hall Phases in Heterostructures with Multiple Dirac Bands.
- Creator
-
Stepanov, Petr, Barlas, Yafis, Espiritu, Tim, Che, Shi, Watanabe, Kenji, Taniguchi, Takashi, Smirnov, Dmitry, Lau, Chun Ning
- Abstract/Description
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The copresence of multiple Dirac bands in few-layer graphene leads to a rich phase diagram in the quantum Hall regime. Using transport measurements, we map the phase diagram of BN-encapsulated ABA-stacked trilayer graphene as a function charge density n, magnetic field B, and interlayer displacement field D, and observe transitions among states with different spin, valley, orbital, and parity polarizations. Such a rich pattern arises from crossings between Landau levels from different...
Show moreThe copresence of multiple Dirac bands in few-layer graphene leads to a rich phase diagram in the quantum Hall regime. Using transport measurements, we map the phase diagram of BN-encapsulated ABA-stacked trilayer graphene as a function charge density n, magnetic field B, and interlayer displacement field D, and observe transitions among states with different spin, valley, orbital, and parity polarizations. Such a rich pattern arises from crossings between Landau levels from different subbands, which reflect the evolving symmetries that are tunable in situ. At D = 0, we observe fractional quantum Hall (FQH) states at filling factors 2/3 and -11/3. Unlike those in bilayer graphene, these FQH states are destabilized by a small interlayer potential that hybridizes the different Dirac bands.
Show less - Date Issued
- 2016-08-12
- Identifier
- FSU_libsubv1_wos_000381478800009, 10.1103/PhysRevLett.117.076807
- Format
- Citation
- Title
- Influence of grain boundary characteristics on thermal stability in nanotwinned copper.
- Creator
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Niu, Rongmei, Han, Ke, Su, Yi-feng, Besara, Tiglet, Siegrist, Theo M., Zuo, Xiaowei
- Abstract/Description
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High density grain boundaries provide high strength, but may introduce undesirable features, such as high Fermi levels and instability. We investigated the kinetics of recovery and recrystallization of Cu that was manufactured to include both nanotwins (NT) and high-angle columnar boundaries. We used the isothermal Johnson-Mehl-Avrami-Kolmogorov (JMAK) model to estimate activation energy values for recovery and recrystallization and compared those to values derived using the non-isothermal...
Show moreHigh density grain boundaries provide high strength, but may introduce undesirable features, such as high Fermi levels and instability. We investigated the kinetics of recovery and recrystallization of Cu that was manufactured to include both nanotwins (NT) and high-angle columnar boundaries. We used the isothermal Johnson-Mehl-Avrami-Kolmogorov (JMAK) model to estimate activation energy values for recovery and recrystallization and compared those to values derived using the non-isothermal Kissinger equation. The JMAK model hinges on an exponent that expresses the growth mechanism of a material. The exponent for this Cu was close to 0.5, indicating low-dimensional microstructure evolution, which is associated with anisotropic twin coarsening, heterogeneous recrystallization, and high stability. Since this Cu was of high purity, there was a negligible impurity-drag-effect on boundaries. The twin coarsening and heterogeneous recrystallization resulted from migration of high-angle columnar boundaries with their triple junctions in one direction, assisted by the presence of high concentration vacancies at boundaries. Analyses performed by electron energy loss spectroscopy of atomic columns at twin boundaries (TBs) and in the interior showed similar plasma peak shapes and L3 edge positions. This implies that values for conductivity and Fermi level are equal for atoms at TBs and in the interior.
Show less - Date Issued
- 2016-08-12
- Identifier
- FSU_libsubv1_wos_000381292600001, 10.1038/srep31410
- Format
- Citation
- Title
- Temperature-driven Massless Kane Fermions In Hgcdte Crystals.
- Creator
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Teppe, F., Marcinkiewicz, M., Krishtopenko, S. S., Ruffenach, S., Consejo, C., Kadykov, A. M., Desrat, W., But, D., Knap, W., Ludwig, J., Moon, S., Smirnov, D., Orlita, M.,...
Show moreTeppe, F., Marcinkiewicz, M., Krishtopenko, S. S., Ruffenach, S., Consejo, C., Kadykov, A. M., Desrat, W., But, D., Knap, W., Ludwig, J., Moon, S., Smirnov, D., Orlita, M., Jiang, Z., Morozov, S. V., Gavrilenko, V. I., Mikhailov, N. N., Dvoretskii, S. A.
Show less - Abstract/Description
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It has recently been shown that electronic states in bulk gapless HgCdTe offer another realization of pseudo-relativistic three-dimensional particles in condensed matter systems. These single valley relativistic states, massless Kane fermions, cannot be described by any other relativistic particles. Furthermore, the HgCdTe band structure can be continuously tailored by modifying cadmium content or temperature. At critical concentration or temperature, the bandgap collapses as the system...
Show moreIt has recently been shown that electronic states in bulk gapless HgCdTe offer another realization of pseudo-relativistic three-dimensional particles in condensed matter systems. These single valley relativistic states, massless Kane fermions, cannot be described by any other relativistic particles. Furthermore, the HgCdTe band structure can be continuously tailored by modifying cadmium content or temperature. At critical concentration or temperature, the bandgap collapses as the system undergoes a semimetal-to-semiconductor topological phase transition between the inverted and normal alignments. Here, using far-infrared magneto-spectroscopy we explore the continuous evolution of band structure of bulk HgCdTe as temperature is tuned across the topological phase transition. We demonstrate that the rest mass of Kane fermions changes sign at critical temperature, whereas their velocity remains constant. The velocity universal value of (1.07 +/- 0.05) x 10(6) m s(-1) remains valid in a broad range of temperatures and Cd concentrations, indicating a striking universality of the pseudo-relativistic description of the Kane fermions in HgCdTe.
Show less - Date Issued
- 2016-08
- Identifier
- FSU_libsubv1_wos_000384683700001, 10.1038/ncomms12576
- Format
- Citation
- Title
- Magnetic Torque Anomaly In The Quantum Limit Of Weyl Semimetals.
- Creator
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Moll, Philip J. W., Potter, Andrew C., Nair, Nityan L., Ramshaw, B. J., Modic, K. A., Riggs, Scott, Zeng, Bin, Ghimire, Nirmal J., Bauer, Eric D., Kealhofer, Robert, Ronning,...
Show moreMoll, Philip J. W., Potter, Andrew C., Nair, Nityan L., Ramshaw, B. J., Modic, K. A., Riggs, Scott, Zeng, Bin, Ghimire, Nirmal J., Bauer, Eric D., Kealhofer, Robert, Ronning, Filip, Analytis, James G.
Show less - Abstract/Description
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Electrons in materials with linear dispersion behave as massless Weyl-or Dirac-quasi-particles, and continue to intrigue due to their close resemblance to elusive ultra-relativistic particles as well as their potential for future electronics. Yet the experimental signatures of Weyl-fermions are often subtle and indirect, in particular if they coexist with conventional, massive quasiparticles. Here we show a pronounced anomaly in the magnetic torque of the Weyl semimetal NbAs upon entering the...
Show moreElectrons in materials with linear dispersion behave as massless Weyl-or Dirac-quasi-particles, and continue to intrigue due to their close resemblance to elusive ultra-relativistic particles as well as their potential for future electronics. Yet the experimental signatures of Weyl-fermions are often subtle and indirect, in particular if they coexist with conventional, massive quasiparticles. Here we show a pronounced anomaly in the magnetic torque of the Weyl semimetal NbAs upon entering the quantum limit state in high magnetic fields. The torque changes sign in the quantum limit, signalling a reversal of the magnetic anisotropy that can be directly attributed to the topological nature of the Weyl electrons. Our results establish that anomalous quantum limit torque measurements provide a direct experimental method to identify and distinguish Weyl and Dirac systems.
Show less - Date Issued
- 2016-08
- Identifier
- FSU_libsubv1_wos_000381905000001, 10.1038/ncomms12492
- Format
- Citation
- Title
- Nearly Massless Dirac Fermions Hosted By Sb Square Net In Bamnsb2.
- Creator
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Liu, Jinyu, Hu, Jin, Cao, Huibo, Zhu, Yanglin, Chuang, Alyssa, Graf, D., Adams, D. J., Radmanesh, S. M. A., Spinu, L., Chiorescu, I., Mao, Zhiqiang
- Abstract/Description
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Layered compounds AMnBi(2) (A = Ca, Sr, Ba, or rare earth element) have been established as Dirac materials. Dirac electrons generated by the two-dimensional (2D) Bi square net in these materials are normally massive due to the presence of a spin-orbital coupling (SOC) induced gap at Dirac nodes. Here we report that the Sb square net in an isostructural compound BaMnSb2 can host nearly massless Dirac fermions. We observed strong Shubnikov-de Haas (SdH) oscillations in this material. From the...
Show moreLayered compounds AMnBi(2) (A = Ca, Sr, Ba, or rare earth element) have been established as Dirac materials. Dirac electrons generated by the two-dimensional (2D) Bi square net in these materials are normally massive due to the presence of a spin-orbital coupling (SOC) induced gap at Dirac nodes. Here we report that the Sb square net in an isostructural compound BaMnSb2 can host nearly massless Dirac fermions. We observed strong Shubnikov-de Haas (SdH) oscillations in this material. From the analyses of the SdH oscillations, we find key signatures of Dirac fermions, including light effective mass (similar to 0.052m(0); m(0), mass of free electron), high quantum mobility (1280 cm(2)V(-1)S(-1)) and a pi Berry phase accumulated along cyclotron orbit. Compared with AMnBi(2), BaMnSb2 also exhibits much more significant quasi two-dimensional (2D) electronic structure, with the out-of-plane transport showing nonmetallic conduction below 120 K and the ratio of the out-of-plane and in-plane resistivity reaching similar to 670. Additionally, BaMnSb2 also exhibits a G-type antiferromagnetic order below 283 K. The combination of nearly massless Dirac fermions on quasi-2D planes with a magnetic order makes BaMnSb2 an intriguing platform for seeking novel exotic phenomena of massless Dirac electrons.
Show less - Date Issued
- 2016-07-28
- Identifier
- FSU_libsubv1_wos_000380964100001, 10.1038/srep30525
- Format
- Citation
- Title
- Emergent Quasi-one-dimensionality In A Kagome Magnet: A Simple Route To Complexity.
- Creator
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Gong, Shou-Shu, Zhu, Wei, Yang, Kun, Starykh, Oleg A., Sheng, D. N., Balents, Leon
- Abstract/Description
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We study the ground-state phase diagram of the quantum spin-1/2 Heisenberg model on the kagome lattice with first-(J(1) 0) by means of analytical low-energy field theory and numerical density-matrix renormalization group (DMRG) studies. The results offer a consistent picture of the J(d)-dominant regime in terms of three sets of spin chains weakly coupled by the ferromagnetic interchain interactions J(1,2). When either J(1) or J(2) is much stronger than the other one, the model is found to...
Show moreWe study the ground-state phase diagram of the quantum spin-1/2 Heisenberg model on the kagome lattice with first-(J(1) < 0), second-(J(2) < 0), and third-neighbor interactions (J(d) > 0) by means of analytical low-energy field theory and numerical density-matrix renormalization group (DMRG) studies. The results offer a consistent picture of the J(d)-dominant regime in terms of three sets of spin chains weakly coupled by the ferromagnetic interchain interactions J(1,2). When either J(1) or J(2) is much stronger than the other one, the model is found to support one of two cuboctohedral phases, cuboc1, and cuboc2. These cuboc states host noncoplanar long-ranged magnetic order and possess finite scalar spin chirality. However, in the compensated regime J(1) similar or equal to J(2), a valence bond crystal phase emerges between the two cuboc phases. We find excellent agreement between an analytical theory based on coupled spin chains and unbiased DMRG calculations, including at a very detailed level of comparison of the structure of the valence bond crystal state. To our knowledge, this is the first such comprehensive understanding of a highly frustrated two-dimensional quantum antiferromagnet. We find no evidence of either the one-dimensional gapless spin liquid or the chiral spin liquids, which were previously suggested by parton mean-field theories.
Show less - Date Issued
- 2016-07-27
- Identifier
- FSU_libsubv1_wos_000381482700001, 10.1103/PhysRevB.94.035154
- Format
- Citation
- Title
- Spin correlations and topological entanglement entropy in a non-Abelian spin-one spin liquid.
- Creator
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Wildeboer, Julia, Bonesteel, N. E.
- Abstract/Description
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We analyze the properties of a non-Abelian spin-one chiral spin liquid state proposed by Greiter and Thomale [Phys. Rev. Lett. 102, 207203 (2009)] using Monte Carlo. In this state the bosonic nu = 1 Moore-Read Pfaffian wave function is used to describe a gas of bosonic spin flips on a square lattice with one flux quantum per plaquette. For toroidal geometries there is a three-dimensional space of these states corresponding to the topological degeneracy of the bosonic Moore-Read state on the...
Show moreWe analyze the properties of a non-Abelian spin-one chiral spin liquid state proposed by Greiter and Thomale [Phys. Rev. Lett. 102, 207203 (2009)] using Monte Carlo. In this state the bosonic nu = 1 Moore-Read Pfaffian wave function is used to describe a gas of bosonic spin flips on a square lattice with one flux quantum per plaquette. For toroidal geometries there is a three-dimensional space of these states corresponding to the topological degeneracy of the bosonic Moore-Read state on the torus. We show that spin correlations for different states in this space become indistinguishable for large system size. We also calculate the Renyi entanglement entropy for different system partitions to extract the topological entanglement entropy and provide evidence that the topological order of the lattice spin-liquid state is the same as that of the continuum Moore-Read state from which it is constructed.
Show less - Date Issued
- 2016-07-18
- Identifier
- FSU_libsubv1_wos_000380104300008, 10.1103/PhysRevB.94.045125
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- Citation
- Title
- Probing 5 f -state configurations in URu2Si2 with U L-III-edge resonant x-ray emission spectroscopy.
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Booth, C. H., Medling, S. A., Tobin, J. G., Baumbach, R. E., Bauer, E. D., Sokaras, D., Nordlund, D., Weng, T.-C.
- Abstract/Description
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Resonant x-ray emission spectroscopy (RXES) was employed at the U L-III absorption edge and the L-alpha 1 emission line to explore the 5f occupancy, n(f), and the degree of 5f -orbital delocalization in the hidden-order compound URu2Si2. By comparing to suitable reference materials such as UF4, UCd11, and alpha-U, we conclude that the 5f orbital in URu2Si2 is at least partially delocalized with n(f) = 2.87 +/- 0.08, and does not change with temperature down to 10 K within the estimated error....
Show moreResonant x-ray emission spectroscopy (RXES) was employed at the U L-III absorption edge and the L-alpha 1 emission line to explore the 5f occupancy, n(f), and the degree of 5f -orbital delocalization in the hidden-order compound URu2Si2. By comparing to suitable reference materials such as UF4, UCd11, and alpha-U, we conclude that the 5f orbital in URu2Si2 is at least partially delocalized with n(f) = 2.87 +/- 0.08, and does not change with temperature down to 10 K within the estimated error. These results place further constraints on theoretical explanations of the hidden order, especially those requiring a localized f(2) ground state.
Show less - Date Issued
- 2016-07-15
- Identifier
- FSU_libsubv1_wos_000379651600007, 10.1103/PhysRevB.94.045121
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- Citation
- Title
- Interaction-driven Fractional Quantum Hall State Of Hard-core Bosons On Kagome Lattice At One-third Filling.
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Zhu, W., Gong, S. S., Sheng, D. N.
- Abstract/Description
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There has been a growing interest in realizing topologically nontrivial states of matter in band insulators, where a quantum Hall effect can appear as an intrinsic property of the band structure. While ongoing progress is under way with a number of directions, the possibility of realizing novel interaction-generated topological phases, without the requirement of a nontrivial invariant encoded in single-particle wave function or band structure, can significantly extend the class of topological...
Show moreThere has been a growing interest in realizing topologically nontrivial states of matter in band insulators, where a quantum Hall effect can appear as an intrinsic property of the band structure. While ongoing progress is under way with a number of directions, the possibility of realizing novel interaction-generated topological phases, without the requirement of a nontrivial invariant encoded in single-particle wave function or band structure, can significantly extend the class of topological materials and is thus of great importance. Here, we show an interaction-driven topological phase emerging in an extended Bose-Hubbard model on a kagome lattice, where the noninteracting band structure is topological trivial with zero Berry curvature in the Brillouin zone. By means of an unbiased state-of-the-art density-matrix renormalization group technique, we identify that the ground state in a broad parameter region is equivalent to a bosonic fractional quantum Hall Laughlin state, based on the characterization of universal properties including ground-state degeneracy, edge excitations, and anyonic quasiparticle statistics. Our work paves a way to finding an interaction-induced topological phase at the phase boundary of conventionally ordered solid phases.
Show less - Date Issued
- 2016-07-13
- Identifier
- FSU_libsubv1_wos_000379502800001, 10.1103/PhysRevB.94.035129
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- Citation
- Title
- Crystal Structure And Partial Ising-like Magnetic Ordering Of Orthorhombic Dy2tio5.
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Shamblin, Jacob, Calder, Stuart, Dun, Zhiling, Lee, Minseong, Choi, Eun Sang, Neuefeind, Joerg, Zhou, Haidong, Lang, Maik
- Abstract/Description
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The structure andmagnetic properties of orthorhombic Dy2TiO5 have been investigated using x-ray diffraction, neutron diffraction, and alternating current (ac)/direct current (dc) magnetic susceptibility measurements. We report a continuous structural distortion below 100 K characterized by negative thermal expansion in the [0 1 0] direction. Neutron diffraction and magnetic susceptibility measurements revealed that two-dimensional (2D) magnetic ordering begins at 3.1 K, which is followed by a...
Show moreThe structure andmagnetic properties of orthorhombic Dy2TiO5 have been investigated using x-ray diffraction, neutron diffraction, and alternating current (ac)/direct current (dc) magnetic susceptibility measurements. We report a continuous structural distortion below 100 K characterized by negative thermal expansion in the [0 1 0] direction. Neutron diffraction and magnetic susceptibility measurements revealed that two-dimensional (2D) magnetic ordering begins at 3.1 K, which is followed by a three-dimensional magnetic transition at 1.7 K. The magnetic structure has been solved through a representational analysis approach and can be indexed with the propagation vector k = [0 1/2 0]. The spin structure corresponds to a coplanar model of interwoven 2D "sheets" extending in the [0 1 0] direction. The local crystal field is different for each Dy3+ ion (Dy1 and Dy2), one of which possesses strong uniaxial symmetry indicative of Ising-like magnetic ordering. Consequently, two succeeding transitions under magnetic field are observed in the ac susceptibility, which are associated with flipping each Dy3+ spin independently.
Show less - Date Issued
- 2016-07-12
- Identifier
- FSU_libsubv1_wos_000379500900004, 10.1103/PhysRevB.94.024413
- Format
- Citation
- Title
- Search For A Low-mass Pseudoscalar Higgs Boson Produced In Association With A B(b)over-bar Pair In Pp Collisions At Root S=8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Knunz, V., Koenig, A., Kraemmer, M., Kratschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Rougny, R., De Klundert, M. Van, Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Barria, P., Brun, H., Caillol, C., Clerbaux, B., De Lentdecker, G., Fasanella, G., Favart, L., Grebenyuk, A., Karapostoli, G., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-conde, A., Reis, T., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Dobur, D., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Ocampo Rios, A. A., Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Strobbe, N., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Caudron, A., Ceard, L., Da Silveira, G. G., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Hollar, J., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Nuttens, C., Perrini, L., Pin, A., Piotrzkowski, K., Popov, A., Quertenmont, L., Selvaggi, M., Vidal Marono, M., Beliy, N., Hammad, G. H., Alda Junior, W. L., Alves, G. A., Brito, L., Correa Martins Junior, M., Hamer, M., Hensel, C., Mora Herrera, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., De Jesus Damiao, D., De Oliveira Martins, C., Fonseca De Souza, S., Huertas Guativa, L. M., Malbouisson, H., Matos Figueiredo, D., Mundim, L., Nogima, H., Prado Da Silva, W. L., Santoro, A., Sznajder, A., Tonelli Manganote, E. J., Vilela Pereira, A., Ahuja, S., Bernardes, C. A., De Souza Santos, A., Dogra, S., Fernandez Perez Tomei, T. R., Gregores, E. M., Mercadante, P. G., Moon, C. S., Novaes, S. F., Padula, Sandra S., Romero Abad, D., Ruiz Vargas, J. C., Aleksandrov, A., Hadjiiska, R., Iaydjiev, P., Rodozov, M., Stoykova, S., Sultanov, G., Vutova, M., Dimitrov, A., Glushkov, I., Litov, L., Pavlov, B., Petkov, P., Ahmad, M., Bian, J. G., Chen, G. M., Chen, H. S., Chen, M., Cheng, T., Du, R., Jiang, C. H., Plestina, R., Romeo, F., Shaheen, S. M., Tao, J., Wang, C., Wang, Z., Zhang, H., Asawatangtrakuldee, C., Ban, Y., Li, Q., Liu, S., Mao, Y., Qian, S. J., Wang, D., Xu, Z., Zou, W., Avila, C., Cabrera, A., Chaparro Sierra, L. F., Florez, C., Gomez, J. P., Gomez Moreno, B., Sanabria, J. C., Godinovic, N., Lelas, D., Puljak, I., Cipriano, P. M. Ribeiro, Antunovic, Z., Kovac, M., Brigljevic, V., Kadija, K., Luetic, J., Micanovic, S., Sudic, L., Attikis, A., Mavromanolakis, G., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. A., Rykaczewski, H., Bodlak, M., Finger, M., Finger, M., Abdelalim, A. A., Awad, A., Mahrous, A., Radi, A., Calpas, B., Kadastik, M., Murumaa, M., Raidal, M., Tiko, A., Veelken, C., Eerola, P., Pekkanen, J., Voutilainen, M., Harkonen, J., Karimaki, V., Kinnunen, R., Lampen, T., Lassila-Perini, K., Lehti, S., Linden, T., Luukka, P., Maenpaa, T., Peltola, T., Tuominen, E., Tuominiemi, J., Tuovinen, E., Wendland, L., Talvitie, J., Tuuva, T., Besancon, M., Couderc, F., Dejardin, M., Denegri, D., Fabbro, B., Faure, J. L., Favaro, C., Ferri, F., Ganjour, S., Givernaud, A., Gras, P., de Monchenault, G. Hamel, Jarry, P., Locci, E., Machet, M., Malcles, J., Rander, J., Rosowsky, A., Titov, M., Zghiche, A., Antropov, I., Baffioni, S., Beaudette, F., Busson, P., Cadamuro, L., Chapon, E., Charlot, C., Dahms, T., Davignon, O., Filipovic, N., Florent, A., de Cassagnac, R. Granier, Lisniak, S., Mastrolorenzo, L., Mine, P., Naranjo, I. N., Nguyen, M., Ochando, C., Ortona, G., Paganini, P., Pigard, P., Regnard, S., Salerno, R., Sauvan, J. B., Sirois, Y., Strebler, T., Yilmaz, Y., Zabi, A., Agram, J.-L., Andrea, J., Aubin, A., Bloch, D., Brom, J.-M., Buttignol, M., Chabert, E. C., Chanon, N., Collard, C., Conte, E., Coubez, X., Fontaine, J.-C., Gele, D., Goerlach, U., Goetzmann, C., Le Bihan, A.-C., Merlin, J. A., Skovpen, K., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Bouvier, E., Montoya, C. A. Carrillo, Chierici, R., Contardo, D., Courbon, B., Depasse, P., El Mamouni, H., Fan, J., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Lagarde, F., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Alvarez, J. D. Ruiz, Sabes, D., Sgandurra, L., Sordini, V., Vander Donckt, M., Verdier, P., Viret, S., Toriashvili, T., Tsamalaidze, Z., Autermann, C., Beranek, S., Edelhoff, M., Feld, L., Heister, A., Kiesel, M. K., Klein, K., Lipinski, M., Ostapchuk, A., Preuten, M., Raupach, F., Schael, S., Schulte, J. F., Verlage, T., Weber, H., Wittmer, B., Zhukov, V., Ata, M., Brodski, M., Dietz-Laursonn, E., Duchardt, D., Endres, M., Erdmann, M., Erdweg, S., Esch, T., Fischer, R., Gueth, A., Hebbeker, T., Heidemann, C., Hoepfner, K., Klingebiel, D., Knutzen, S., Kreuzer, P., Merschmeyer, M., Meyer, A., Millet, P., Olschewski, M., Padeken, K., Papacz, P., Pook, T., Radziej, M., Reithler, H., Rieger, M., Scheuch, F., Sonnenschein, L., Teyssier, D., Thueer, S., Cherepanov, V., Erdogan, Y., Fluegge, G., Geenen, H., Geisler, M., Hoehle, F., Kargoll, B., Kress, T., Kuessel, Y., Kuensken, A., Lingemann, J., Nehrkorn, A., Nowack, A., Nugent, I. M., Pistone, C., Pooth, O., Stahl, A., Martin, M. Aldaya, Asin, I., Bartosik, N., Behnke, O., Behrens, U., Bell, A. J., Borras, K., Burgmeier, A., Cakir, A., Calligaris, L., Campbell, A., Choudhury, S., Costanza, F., Pardos, C. Diez, Dolinska, G., Dooling, S., Dorland, T., Eckerlin, G., Eckstein, D., Eichhorn, T., Flucke, G., Gallo, E., Garcia, J. Garay, Geiser, A., Gizhko, A., Gunnellini, P., Hauk, J., Hempel, M., Jung, H., Kalogeropoulos, A., Karacheban, O., Kasemann, M., Katsas, P., Kieseler, J., Kleinwort, C., Korol, I., Lange, W., Leonard, J., Lipka, K., Lobanov, A., Lohmann, W., Mankel, R., Marfin, I., Melzer-Pellmann, I.-A., Meyer, A. B., Mittag, G., Mnich, J., Mussgiller, A., Naumann-Emme, S., Nayak, A., Ntomari, E., Perrey, H., Pitzl, D., Placakyte, R., Raspereza, A., Roland, B., Sahin, M. Oe, Saxena, P., Schoerner-Sadenius, T., Schroeder, M., Seitz, C., Spannagel, S., Trippkewitz, K. D., Walsh, R., Wissing, C., Blobel, V., Vignali, M. Centis, Draeger, A. R., Erfle, J., Garutti, E., Goebel, K., Gonzalez, D., Goerner, M., Haller, J., Hoffmann, M., Hoeing, R. S., Junkes, A., Klanner, R., Kogler, R., Lapsien, T., Lenz, T., Marchesini, I., Marconi, D., Meyer, M., Nowatschin, D., Ott, J., Pantaleo, F., Peiffer, T., Perieanu, A., Pietsch, N., Poehlsen, J., Rathjens, D., Sander, C., Schettler, H., Schleper, P., Schlieckau, E., Schmidt, A., Schwandt, J., Seidel, M., Sola, V., Stadie, H., Steinbruck, G., Tholen, H., Troendle, D., Usai, E., Vanelderen, L., Vanhoefer, A., Vormwald, B., Akbiyik, M., Barth, C., Baus, C., Berger, J., Boeser, C., Butz, E., Chwalek, T., Colombo, F., De Boer, W., Descroix, A., Dierlamm, A., Fink, S., Frensch, F., Giffels, M., Gilbert, A., Hartmann, F., Heindl, S. M., Husemann, U., Katkov, I., Kornmayer, A., Pardo, P. Lobelle, Maier, B., Mildner, H., Mozer, M. U., Mueller, T., Mueller, Th, Plagge, M., Quast, G., Rabbertz, K., Roecker, S., Roscher, F., Simonis, H. J., Stober, F. M., Ulrich, R., Wagner-Kuhr, J., Wayand, S., Weber, M., Weiler, T., Woehrmann, C., Wolf, R., Anagnostou, G., Daskalakis, G., Geralis, T., Giakoumopoulou, V. A., Kyriakis, A., Loukas, D., Psallidas, A., Topsis-Giotis, I., Agapitos, A., Kesisoglou, S., Panagiotou, A., Saoulidou, N., Tziaferi, E., Evangelou, I., Flouris, G., Foudas, C., Kokkas, P., Loukas, N., Manthos, N., Papadopoulos, I., Paradas, E., Strologas, J., Bencze, G., Hajdu, C., Hazi, A., Hidas, P., Horvath, D., Sikler, F., Veszpremi, V., Vesztergombi, G., Zsigmond, A. J., Beni, N., Czellar, S., Karancsi, J., Molnar, J., Szillasi, Z., Bartok, M., Makovec, A., Raics, P., Trocsanyi, Z. L., Ujvari, B., Mal, P., Mandal, K., Sahoo, D. K., Sahoo, N., Swain, S. K., Bansal, S., Beri, S. B., Bhatnagar, V., Chawla, R., Gupta, R., Bhawandeep, U., Kalsi, A. K., Kaur, A., Kaur, M., Kumar, R., Mehta, A., Mittal, M., Singh, J. B., Walia, G., Kumar, Ashok, Bhardwaj, A., Choudhary, B. C., Garg, R. B., Kumar, A., Malhotra, S., Naimuddin, M., Nishu, N., Ranjan, K., Sharma, R., Sharma, V., Bhattacharya, S., Chatterjee, K., Dey, S., Dutta, S., Jain, Sa, Majumdar, N., Modak, A., Mondal, K., Mukherjee, S., Mukhopadhyay, S., Roy, A., Roy, D., Chowdhury, S. Roy, Sarkar, S., Sharan, M., Abdulsalam, A., Chudasama, R., Dutta, D., Jha, V., Kumar, V., Mohanty, A. K., Pant, L. M., Shukla, P., Topkar, A., Aziz, T., Banerjee, S., Bhowmik, S., Chatterjee, R. M., Dewanjee, R. K., Dugad, S., Ganguly, S., Ghosh, S., Guchait, M., Gurtu, A., Kole, G., Kumar, S., Mahakud, B., Maity, M., Majumder, G., Mazumdar, K., Mitra, S., Mohanty, G. B., Parida, B., Sarkar, T., Sudhakar, K., Sur, N., Sutar, B., Wickramage, N., Chauhan, S., Dube, S., Sharma, S., Bakhshiansohi, H., Behnamian, H., Etesami, S. M., Fahim, A., Goldouzian, R., Khakzad, M., Najafabadi, M. Mohammadi, Naseri, M., Mehdiabadi, S. Paktinat, Hosseinabadi, F. Rezaei, Safarzadeh, B., Zeinali, M., Felcini, M., Grunewald, M., Abbrescia, M., Calabria, C., Caputo, C., Colaleo, A., Creanza, D., Cristella, L., De Filippis, N., De Palma, M., Fiore, L., Iasellia, G., Maggi, G., Maggi, M., Miniello, G., My, S., Nuzzo, S., Pompili, A., Puglies, G., Radogna, R., Ranieri, A., Selvaggi, G., Silvestris, L., Venditti, R., Verwilligen, P., Abbiendi, G., Battilana, C., Benvenuti, A. C., Bonacorsi, D., Braibant-Giacomelli, S., Brigliadori, L., Campanini, R., Capiluppi, P., Castro, A., Cavallo, F. R., Chhibra, S. S., Codispoti, G., Cuffiani, M., Dallavalle, G. M., Fabbri, F., Fanfani, A., Fasanella, D., Giacomelli, P., Grandi, C., Guiducci, L., Marcellini, S., Masetti, G., Montanari, A., Navarria, F. L., Perrotta, A., Rossi, A. M., Rovelli, T., Siroli, G. P., Tosi, N., Travaglini, R., Cappello, G., Chiorboli, M., Costa, S., Giordano, F., Potenza, R., Tricomi, A., Tuve, C., Barbagli, G., Ciulli, V., Civinini, C., D'Alessandro, R., Focardi, E., Gonzi, S., Gori, V., Lenzi, P., Meschini, M., Paoletti, S., Sguazzoni, G., Tropiano, A., Viliani, L., Benussi, L., Bianco, S., Fabbri, F., Piccolo, D., Primavera, F., Calvelli, V., Ferro, F., Lo Vetere, M., Monge, M. R., Robutti, E., Tosi, S., Brianz, L., Dinardo, M. E., Fiorendi, S., Gennai, S., Gerosa, R., Ghezzi, A., Govoni, P., Malvezzi, S., Manzoni, R. A., Marzocchi, B., Menasce, D., Moroni, L., Paganoni, M., Pedrini, D., Ragazzi, S., Redaelli, N., de Fatis, T. Tabarelli, Buontempo, S., Cavallo, N., Di Guida, S., Esposito, M., Fabozzi, F., Iorio, A. O. M., Lanza, G., Lista, L., Meola, S., Merola, M., Paolucci, P., Sciacca, C., Thyssen, F., Azzi, P., Bacchetta, N., Bellato, M., Benato, L., Bisello, D., Boletti, A., Branca, A., Carlin, R., Checchi, P., Dall'Osso, M., Dorigo, T., Dosselli, U., Gasparini, F., Gasparini, U., Gozzelino, A., Lacaprara, S., Margoni, M., Meneguzzo, A. T., Pazzini, J., Pozzobon, N., Ronchese, P., Simonetto, F., Torassa, E., Tosi, M., Ventura, S., Zanetti, M., Zotto, P., Zucchetta, A., Zumerle, G., Braghieri, A., Magnani, A., Montagna, P., Ratti, S. P., Re, V., Riccardi, C., Salvini, P., Vai, I., Vitulo, P., Solestizi, L. Alunni, Biasini, M., Bilei, G. M., Ciangottini, D., Fano, L., Lariccia, P., Mantovani, G., Menichelli, M., Saha, A., Santocchia, A., Spiezia, A., Androsov, K., Azzurri, P., Bagliesi, G., Bernardini, J., Boccali, T., Broccolo, G., Castaldi, R., Ciocci, M. A., Dell'Orso, R., Donato, S., Fedi, G., Foa, L., Giassi, A., Grippo, M. T., Ligabue, F., Lomtadze, T., Martini, L., Messineo, A., Palla, F., Rizzi, A., Savoy-Navarro, A., Serban, A. T., Spagnolo, P., Squillacioti, P., Tenchini, R., Tonelli, G., Venturi, A., Verdini, P. G., Barone, L., Cavallari, F., D'imperio, G., Del Re, D., Diemoz, M., Gelli, S., Jorda, C., Longo, E., Margaroli, F., Meridiani, P., Organtini, G., Paramatti, R., Preiato, F., Rahatlou, S., Rovelli, C., Santanastasio, F., Traczyk, P., Amapane, N., Arcidiacono, R., Argiro, S., Arneodo, M., Bellan, R., Biino, C., Cartiglia, N., Costa, M., Covarelli, R., Degano, A., Demaria, N., Finco, L., Kiani, B., Mariotti, C., Maselli, S., Migliore, E., Monaco, V., Monteil, E., Musich, M., Obertino, M. M., Pacher, L., Pastrone, N., Pelliccioni, M., Angioni, G. L. Pinna, Ravera, F., Romero, A., Ruspa, M., Sacchi, R., Solano, A., Staiano, A., Tamponi, U., Belforte, S., Candelise, V., Casarsa, M., Cossutti, F., Della Ricca, G., Gobbo, B., La Licata, C., Marone, M., Schizzi, A., Zanetti, A., Kropivnitskaya, A., Nam, S. K., Kim, D. H., Kim, G. N., Kim, M. S., Kong, D. J., Lee, S., Oh, Y. D., Sakharov, A., Son, D. C., Cifuentes, J. A. Brochero, Kim, H., Kim, T. J., Ryu, M. S., Song, S., Choi, S., Go, Y., Gyun, D., Hong, B., Jo, M., Kim, H., Kim, Y., Lee, B., Lee, K., Lee, K. S., Lee, S., Park, S. K., Roh, Y., Yoo, H. D., Choi, M., Kim, H., Kim, J. H., Lee, J. S. H., Park, I. C., Ryu, G., Choi, Y., Goh, J., Kim, D., Kwon, E., Lee, J., Yu, I., Juodagalvis, A., Vaitkus, J., Ahmed, I., Ibrahim, Z. A., Komaragiri, J. R., Ali, M. A. B. Md, Idris, F. Mohamad, Abdullah, W. A. T. Wan, Yusli, M. N., Linares, E. 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A., Carlsmith, D., Cepeda, M., Christian, A., Dasu, S., Dodd, L., Duric, S., Friis, E., Gomber, B., Grothe, M., Hall-Wilton, R., Herndon, M., Herve, A., Klabbers, P., Lanaro, A., Levine, A., Long, K., Loveless, R., Mohapatra, A., Ojalvo, I., Perry, T., Pierro, G. A., Polese, G., Ruggles, T., Sarangi, T., Savin, A., Sharma, A., Smith, N., Smith, W. H., Taylor, D., Woods, N.
Show less - Abstract/Description
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A search is reported for a light pseudoscalar Higgs boson decaying to a pair of tau leptons, produced in association with a b (b) over bar pair, in the context of two-Higgs-doublet models. The results are based on pp collision data at a centre-of-mass energy of 8 TeV collected by the CMS experiment at the LHC and corresponding to an integrated luminosity of 19.7 fb(-1). Pseudoscalar boson masses between 25 and 80 GeV are probed. No evidence for a pseudoscalar boson is found and upper limits...
Show moreA search is reported for a light pseudoscalar Higgs boson decaying to a pair of tau leptons, produced in association with a b (b) over bar pair, in the context of two-Higgs-doublet models. The results are based on pp collision data at a centre-of-mass energy of 8 TeV collected by the CMS experiment at the LHC and corresponding to an integrated luminosity of 19.7 fb(-1). Pseudoscalar boson masses between 25 and 80 GeV are probed. No evidence for a pseudoscalar boson is found and upper limits are set on the product of cross section and branching fraction to tau pairs between 7 and 39 pb at the 95% confidence level. This excludes pseudoscalar A bosons with masses between 25 and 80 GeV, with SM-like Higgs boson negative couplings to down-type fermions, produced in association with bb pairs, in Type II, two-Higgs-doublet models. (C) 2016 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommonnorg/licensesiby/4.01).
Show less - Date Issued
- 2016-07-10
- Identifier
- FSU_libsubv1_wos_000377330500044, 10.1016/j.physletb.2016.05.003
- Format
- Citation
- Title
- Measurement Of Spin Correlations In Tf Production Using The Matrix Element Method In The Muon Plus Jets Final State In Pp Collisions At Root S=8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
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Show less - Abstract/Description
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The consistency of the spin correlation strength in top quark pair production with the standard model (SM) prediction is tested in the muon+jets final state. The events are selected from pp collisions, collected by the CMS detector, at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The data are compared with the expectation for the spin correlation predicted by the SM and with the expectation of no correlation. Using a template fit method, the...
Show moreThe consistency of the spin correlation strength in top quark pair production with the standard model (SM) prediction is tested in the muon+jets final state. The events are selected from pp collisions, collected by the CMS detector, at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The data are compared with the expectation for the spin correlation predicted by the SM and with the expectation of no correlation. Using a template fit method, the fraction of events that show SM spin correlations is measured to be 0.72 0.08 (stat)(-013)(+015) (syst), representing the most precise measurement of this quantity in the muon+jets final state to date. (C) 2016 The Author. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.orglicenses/by/4.01).
Show less - Date Issued
- 2016-07-10
- Identifier
- FSU_libsubv1_wos_000377330500045, 10.1016/j.physletb.2016.05.005
- Format
- Citation
- Title
- High hardness in the biocompatible intermetallic compound beta-Ti3Au.
- Creator
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Svanidze, Eteri, Besara, Tiglet, Ozaydin, M. Fevsi, Tiwary, Chandra Sekhar, Wang, Jiakui K., Radhakrishnan, Sruthi, Mani, Sendurai, Xin, Yan, Han, Ke, Liang, Hong, Siegrist,...
Show moreSvanidze, Eteri, Besara, Tiglet, Ozaydin, M. Fevsi, Tiwary, Chandra Sekhar, Wang, Jiakui K., Radhakrishnan, Sruthi, Mani, Sendurai, Xin, Yan, Han, Ke, Liang, Hong, Siegrist, Theo, Ajayan, Pulickel M., Morosan, E.
Show less - Abstract/Description
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The search for new hard materials is often challenging, but strongly motivated by the vast application potential such materials hold. Ti3Au exhibits high hardness values (about four times those of pure Ti and most steel alloys), reduced coefficient of friction and wear rates, and biocompatibility, all of which are optimal traits for orthopedic, dental, and prosthetic applications. In addition, the ability of this compound to adhere to ceramic parts can reduce both the weight and the cost of...
Show moreThe search for new hard materials is often challenging, but strongly motivated by the vast application potential such materials hold. Ti3Au exhibits high hardness values (about four times those of pure Ti and most steel alloys), reduced coefficient of friction and wear rates, and biocompatibility, all of which are optimal traits for orthopedic, dental, and prosthetic applications. In addition, the ability of this compound to adhere to ceramic parts can reduce both the weight and the cost of medical components. The fourfold increase in the hardness of Ti3Au compared to other Ti-Au alloys and compounds can be attributed to the elevated valence electron density, the reduced bond length, and the pseudogap formation. Understanding the origin of hardness in this intermetallic compound provides an avenue toward designing superior biocompatible, hard materials.
Show less - Date Issued
- 2016-07
- Identifier
- FSU_libsubv1_wos_000381805300026, 10.1126/sciadv.1600319
- Format
- Citation
- Title
- Evidence Of Topological Nodal-line Fermions In Zrsise And Zrsite.
- Creator
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Hu, Jin, Tang, Zhijie, Liu, Jinyu, Liu, Xue, Zhu, Yanglin, Graf, David, Myhro, Kevin, Tran, Son, Lau, Chun Ning, Wei, Jiang, Mao, Zhiqiang
- Abstract/Description
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A Dirac nodal-line semimetal phase, which represents a new quantum state of topological materials, has been experimentally realized only in a few systems, including PbTaSe2, PtSn4, and ZrSiS. In this Letter, we report evidence of nodal-line fermions in ZrSiSe and ZrSiTe probed in de Haas-van Alphen quantum oscillations. Although ZrSiSe and ZrSiTe share a similar layered structure with ZrSiS, our studies show the Fermi surface (FS) enclosing a Dirac nodal line has a 2D character in ZrSiTe, in...
Show moreA Dirac nodal-line semimetal phase, which represents a new quantum state of topological materials, has been experimentally realized only in a few systems, including PbTaSe2, PtSn4, and ZrSiS. In this Letter, we report evidence of nodal-line fermions in ZrSiSe and ZrSiTe probed in de Haas-van Alphen quantum oscillations. Although ZrSiSe and ZrSiTe share a similar layered structure with ZrSiS, our studies show the Fermi surface (FS) enclosing a Dirac nodal line has a 2D character in ZrSiTe, in contrast with 3D-like FS in ZrSiSe and ZrSiS. Another important property revealed in our experiment is that the nodal-line fermion density in this family of materials (similar to 10(20) cm(-3)) is much higher than the Dirac fermion density of other topological materials with discrete nodes. In addition, we have demonstrated ZrSiSe and ZrSiTe single crystals can be thinned down to 2D atomic thin layers through microexfoliation, which offers the first platform to explore exotic properties of topological nodal-line fermions in low dimensions.
Show less - Date Issued
- 2016-06-30
- Identifier
- FSU_libsubv1_wos_000378881300009, 10.1103/PhysRevLett.117.016602
- Format
- Citation
- Title
- Coexistence of Weyl physics and planar defects in the semimetals TaP and TaAs.
- Creator
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Besara, T., Rhodes, D. A., Chen, K.-W., Das, S., Zhang, Q. R., Sun, J., Zeng, B., Xin, Y., Balicas, L., Baumbach, R. E., Manousakis, E., Singh, D. J., Siegrist, T.
- Abstract/Description
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We report a structural study of the Weyl semimetals TaAs and TaP, utilizing diffraction and imaging techniques, where we show that they contain a high density of defects, leading to nonstoichiometric single crystals of both semimetals. Despite the observed defects and nonstoichiometry on samples grown using techniques already reported in the literature, de Haas-van Alphen measurements on TaP reveal quantum oscillations and a high carrier mobility, an indication that the crystals are of...
Show moreWe report a structural study of the Weyl semimetals TaAs and TaP, utilizing diffraction and imaging techniques, where we show that they contain a high density of defects, leading to nonstoichiometric single crystals of both semimetals. Despite the observed defects and nonstoichiometry on samples grown using techniques already reported in the literature, de Haas-van Alphen measurements on TaP reveal quantum oscillations and a high carrier mobility, an indication that the crystals are of quality comparable to those reported elsewhere. Electronic structure calculations on TaAs reveal that the position of the Weyl points relative to the Fermi level shift with the introduction of vacancies and stacking faults. In the case of vacancies the Fermi surface becomes considerably altered, while the effect of stacking faults on the electronic structure is to allow the Weyl pockets to remain close to the Fermi surface. The observation of quantum oscillations in a nonstoichiometric crystal and the persistence of Weyl fermion pockets near the Fermi surface in a crystal with stacking faults point to the robustness of these quantum phenomena in these materials.
Show less - Date Issued
- 2016-06-27
- Identifier
- FSU_libsubv1_wos_000378816000007, 10.1103/PhysRevB.93.245152
- Format
- Citation
- Title
- Persistence Of Slow Fluctuations In The Overdoped Regime Of Ba(fe1-xrhx)(2)as-2 Superconductors.
- Creator
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Bossoni, L., Moroni, M., Julien, M. H., Mayaffre, H., Canfield, P. C., Reyes, A., Halperin, W. P., Carretta, P.
- Abstract/Description
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We present nuclear magnetic resonance evidence that very slow (
Show moreWe present nuclear magnetic resonance evidence that very slow (<= 1 MHz) spin fluctuations persist into the overdoped regime of Ba(Fe1-xRhx)(2)As-2 superconductors. Measurements of the As-75 spin echo decay rate, obtained both with Hahn Echo and Carr Purcell Meiboom Gill pulse sequences, show that the slowing down of spin fluctuations can be described by short-range diffusive dynamics, likely involving domain walls motions separating (pi/a, 0) from (0, pi/a) correlated regions. This slowing down of the fluctuations is weakly sensitive to the external magnetic field and, although fading away with doping, it extends deeply into the overdoped regime.
Show less - Date Issued
- 2016-06-23
- Identifier
- FSU_libsubv1_wos_000378305600003, 10.1103/PhysRevB.93.224517
- Format
- Citation
- Title
- Search for lepton flavour violating decays of heavy resonances and quantum black holes to an e mu pair in proton-proton collisions at root s=8 TeV.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Knuenz, V., Koenig, A., Krammer, M., Kraetschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rad, N., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Van de Klundert, M., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Barria, P., Brun, H., Caillol, C., Clerbaux, B., De Lentdecker, G., Fang, W., Fasanella, G., Favart, L., Goldouzian, R., Grebenyuk, A., Karapostoli, G., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-conde, A., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Dobur, D., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Rios, A. A. Ocampo, Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Caudron, A., Ceard, L., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Musich, M., Nuttens, C., Perrini, L., Piotrzkowski, K., Popov, A., Quertenmont, L., Selvaggi, M., Marono, M. Vidal, Beliy, N., Hammad, G. H., Alda Junior, W. L., Alves, F. L., Alves, G. A., Brito, L., Correa Martins Junior, M., Hamer, M., Hensel, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., De Jesus Damiao, D., De Oliveira Martins, C., Fonseca De Souza, S., Huertas Guativa, L. M., Malbouisson, H., Matos Figueiredo, D., Mora Herrera, C., Mundim, L., Nogima, H., Prado Da Silva, W. L., Santoro, A., Sznajder, A., Tonelli Manganote, E. J., Vilela Pereira, A., Ahuja, S., Bernardes, C. A., De Souza Santos, A., Dogra, S., Fernandez Perez Tomei, T. R., Gregores, E. M., Mercadante, P. G., Moon, C. S., Novaes, S. F., Padula, Sandra S., Romero Abad, D., Ruiz Vargas, J. C., Aleksandrov, A., Hadjiiska, R., Iaydjiev, P., Rodozov, M., Stoykova, S., Sultanov, G., Vutova, M., Dimitrov, A., Glushkov, I., Litov, L., Pavlov, B., Petkov, P., Ahmad, M., Bian, J. G., Chen, G. M., Chen, H. S., Chen, M., Cheng, T., Du, R., Jiang, C. H., Leggat, D., Plestina, R., Romeo, F., Shaheen, S. M., Spiezia, A., Tao, J., Wang, C., Wang, Z., Zhang, H., Asawatangtrakuldee, C., Ban, Y., Li, Q., Liu, S., Mao, Y., Qian, S. J., Wang, D., Xu, Z., Avila, C., Cabrera, A., Chaparro Sierra, L. F., Florez, C., Gomez, J. P., Gomez Moreno, B., Sanabria, J. C., Godinovic, N., Lelas, D., Puljak, I., Cipriano, P. M. Ribeiro, Antunovic, Z., Kovac, M., Brigljevic, V., Kadija, K., Luetic, J., Micanovic, S., Sudic, L., Attikis, A., Mavromanolakis, G., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. A., Rykaczewski, H., Bodlak, M., Finger, M., Finger, M., Assran, Y., Elgammal, S., Kamel, A. Ellithi, Mahmoud, M. A., Calpas, B., Kadastik, M., Murumaa, M., Raidal, M., Tiko, A., Veelken, C., Eerola, P., Pekkanen, J., Voutilainen, M., Harkonen, J., Karimaki, V., Kinnunen, R., Lampen, T., Lassila-Perini, K., Lehti, S., Linden, T., Luukka, P., Peltola, T., Tuominiemi, J., Tuovinen, E., Wendland, L., Talvitie, J., Tuuva, T., Besancon, M., Couderc, F., Dejardin, M., Denegri, D., Fabbro, B., Faure, J. L., Favaro, C., Ferri, F., Ganjour, S., Givernaud, A., Gras, P., de Monchenault, G. Hamel, Jarry, P., Locci, E., Machet, M., Malcles, J., Rander, J., Rosowsky, A., Titov, M., Zghiche, A., Abdulsalam, A., Antropov, I., Baffioni, S., Beaudette, F., Busson, P., Cadamuro, L., Chapon, E., Charlot, C., Davignon, O., Filipovic, N., de Cassagnac, R. Granier, Jo, M., Lisniak, S., Mastrolorenzo, L., Mine, P., Naranjo, I. N., Nguyen, M., Ochando, C., Ortona, G., Paganini, P., Pigard, P., Regnard, S., Salerno, R., Sauvan, J. B., Sirois, Y., Strebler, T., Yilmaz, Y., Zabi, A., Agram, J.-L., Andrea, J., Aubin, A., Bloch, D., Brom, J.-M., Buttignol, M., Chabert, E. C., Chanon, N., Collard, C., Conte, E., Coubez, X., Fontaine, J.-C., Gele, D., Goerlach, U., Goetzmann, C., Le Bihan, A.-C., Merlin, J. A., Skovpen, K., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Bouvier, E., Montoya, C. A. Carrillo, Chierici, R., Contardo, D., Courbon, B., Depasse, P., El Mamouni, H., Fan, J., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Lagarde, F., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Alvarez, J. D. Ruiz, Sabes, D., Sgandurra, L., Sordini, V., Vander Donckt, M., Verdier, P., Viret, S., Toriashvili, T., Rurua, L., Autermann, C., Beranek, S., Feld, L., Heister, A., Kiesel, M. K., Klein, K., Lipinski, M., Ostapchuk, A., Preuten, M., Raupach, F., Schael, S., Schulte, J. F., Verlage, T., Weber, H., Zhukov, V., Ata, M., Brodski, M., Dietz-Laursonn, E., Duchardt, D., Endres, M., Erdmann, M., Erdweg, S., Esch, T., Fischer, R., Gueth, A., Hebbeker, T., Heidemann, C., Hoepfner, K., Knutzen, S., Kreuzer, P., Merschmeyer, M., Meyer, A., Millet, P., Mukherjee, S., Olschewski, M., Padeken, K., Papacz, P., Pook, T., Radziej, M., Reithler, H., Rieger, M., Scheuch, F., Sonnenschein, L., Teyssier, D., Thueer, S., Cherepanov, V., Erdogan, Y., Fluegge, G., Geenen, H., Geisler, M., Hoehle, F., Kargoll, B., Kress, T., Kuensken, A., Lingemann, J., Nehrkorn, A., Nowack, A., Nugent, I. M., Pistone, C., Pooth, O., Stahl, A., Martin, M. Aldaya, Asin, I., Bartosik, N., Behnke, O., Behrens, U., Borras, K., Burgmeier, A., Campbell, A., Contreras-Campana, C., Costanza, F., Pardos, C. Diez, Dolinska, G., Dooling, S., Dorland, T., Eckerlin, G., Eckstein, D., Eichhorn, T., Flucke, G., Gallo, E., Garcia, J. Garay, Geiser, A., Gizhko, A., Gunnellini, P., Hauk, J., Hempel, M., Jung, H., Kalogeropoulos, A., Karacheban, O., Kasemann, M., Katsas, P., Kieseler, J., Kleinwort, C., Korol, I., Lange, W., Leonard, J., Lipka, K., Lobanov, A., Lohmann, W., Mankel, R., Melzer-Pellmann, I.-A., Meyer, A. B., Mittag, G., Mnich, J., Mussgiller, A., Naumann-Emme, S., Nayak, A., Ntomari, E., Perrey, H., Pitzl, D., Placakyte, R., Raspereza, A., Roland, B., Sahin, M. Oe, Saxena, P., Schoerner-Sadenius, T., Seitz, C., Spannagel, S., Stefaniuk, N., Trippkewitz, K. D., Walsh, R., Wissing, C., Blobel, V., Vignali, M. Centis, Draeger, R., Erfle, J., Garutti, E., Goebel, K., Gonzalez, D., Goerner, M., Haller, J., Hoffmann, M., Hoeing, R. S., Junkes, A., Klanner, R., Kogler, R., Kovalchuk, N., Lapsien, T., Lenz, T., Marchesini, I., Marconi, D., Meyer, M., Nowatschin, D., Ott, J., Pantaleo, F., Peiffer, T., Perieanu, A., Pietsch, N., Poehlsen, J., Rathjens, D., Sander, C., Scharf, C., Schleper, P., Schlieckau, E., Schmidt, A., Schumann, S., Schwandt, J., Sola, V., Stadie, H., Steinbrueck, G., Stober, F. M., Tholen, H., Troendle, D., Usai, E., Vanelderen, L., Vanhoefer, A., Vormwald, B., Barth, C., Baus, C., Berger, J., Boeser, C., Butz, E., Chwalek, T., Colombo, F., De Boer, W., Descroix, A., Dierlamm, A., Fink, S., Frensch, F., Friese, R., Giffels, M., Gilbert, A., Haitz, D., Hartmann, F., Heindl, S. M., Husemann, U., Katkov, I., Kornmayer, A., Pardo, P. Lobelle, Maier, B., Mildner, H., Mozer, M. U., Mueller, T., Mueller, Th, Plagge, M., Quast, G., Rabbertz, K., Roecker, S., Roscher, F., Schroeder, M., Sieber, G., Simonis, H. J., Ulrich, R., Wagner-Kuhr, J., Wayand, S., Weber, M., Weiler, T., Williamson, S., Woehrmann, C., Wolf, R., Anagnostou, G., Daskalakis, G., Geralis, T., Giakoumopoulou, V. A., Kyriakis, A., Loukas, D., Psallidas, A., Topsis-Giotis, I., Agapitos, A., Kesisoglou, S., Panagiotou, A., Saoulidou, N., Tziaferi, E., Evangelou, I., Flouris, G., Foudas, C., Kokkas, P., Loukas, N., Manthos, N., Papadopoulos, I., Paradas, E., Strologas, J., Bencze, G., Hajdu, C., Hazi, A., Hidas, P., Horvath, D., Sikler, F., Veszpremi, V., Vesztergombi, G., Zsigmond, A. J., Beni, N., Czellar, S., Karancsi, J., Molnar, J., Szillasi, Z., Bartok, M., Makovec, A., Raics, P., Trocsanyi, Z. L., Ujvari, B., Choudhury, S., Mal, P., Mandal, K., Sahoo, D. K., Sahoo, N., Swain, S. K., Bansal, S., Beri, S. B., Bhatnagar, V., Chawla, R., Gupta, R., Bhawandeep, U., Kalsi, A. K., Kaur, A., Kaur, M., Kumar, R., Mehta, A., Mittal, M., Singh, J. B., Walia, G., Kumar, Ashok, Bhardwaj, A., Choudhary, B. C., Garg, R. B., Malhotra, S., Naimuddin, M., Nishu, N., Ranjan, K., Sharma, R., Sharma, V., Bhattacharya, S., Chatterjee, K., Dey, S., Dutta, S., Majumdar, N., Modak, A., Mondal, K., Mukhopadhyay, S., Roy, A., Roy, D., Chowdhury, S. Roy, Sarkar, S., Sharan, M., Chudasama, R., Dutta, D., Jha, V., Kumar, V., Mohanty, A. K., Pant, L. M., Shukla, P., Topkar, A., Aziz, T., Banerjee, S., Bhowmik, S., Chatterjee, R. M., Dewanjee, R. K., Dugad, S., Ganguly, S., Ghosh, S., Guchait, M., Gurtu, A., Jain, Sa, Kole, G., Kumar, S., Mahakud, B., Maity, M., Majumder, G., Mazumdar, K., Mitra, S., Mohanty, G. B., Parida, B., Sarkar, T., Sur, N., Sutar, B., Wickramage, N., Chauhan, S., Dube, S., Kapoor, A., Kothekar, K., Sharma, S., Bakhshiansohi, H., Behnamian, H., Etesam, S. M., Fahim, A., Khakzad, M., Najafabadi, M. Mohammadi, Naseri, M., Mehdiabadi, S. Paktinat, Hosseinabadi, F. Rezaei, Safarzadeh, B., Zeinali, M., Felcini, M., Grunewald, M., Abbrescia, M., Calabria, C., Caputo, C., Colaleo, A., Creanza, D., Cristella, L., De Filippis, N., De Palma, M., Fiore, L., Iaselli, G., Maggi, G., Maggi, M., Miniello, G., My, S., Nuzzo, S., Pompili, A., Pugliese, G., Radogna, R., Ranieri, A., Selvaggi, G., Silvestris, L., Venditti, R., Abbiendi, G., Battilana, C., Bonacorsi, D., Braibant-Giacomelli, S., Brigliadori, L., Campanini, R., Capiluppi, P., Castro, A., Cavallo, F. R., Chhibra, S. S., Codispoti, G., Cuffiani, M., Dallavalle, G. M., Fabbri, F., Fanfani, A., Fasanella, D., Giacomelli, P., Grandi, C., Guiducci, L., Marcellini, S., Masetti, G., Montanari, A., Navarria, F. L., Perrotta, A., Rossi, A. M., Rovelli, T., Siroli, G. P., Tosi, N., Cappello, G., Chiorboli, M., Costa, S., Di Mattia, A., Giordano, F., Potenza, R., Tricomi, A., Tuve, C., Barbagli, G., Ciulli, V., Civinini, C., D'Alessandro, R., Focardi, E., Gori, V., Lenzi, P., Meschini, M., Paoletti, S., Sguazzoni, G., Viliani, L., Benussi, L., Bianco, S., Fabbri, F., Piccolo, D., Primavera, F., Calvelli, V., Ferro, F., Lo Vetere, M., Monge, M. R., Robutti, E., Tosi, S., Brianza, L., Dinardo, M. E., Fiorendi, S., Gennai, S., Gerosa, R., Ghezzi, A., Govoni, P., Malvezzi, S., Manzoni, R. A., Marzocchi, B., Menasce, D., Moroni, L., Paganoni, M., Pedrini, D., Ragazzi, S., Redaelli, N., de Fatis, T. Tabarelli, Buontempo, S., Cavallo, N., Di Guida, S., Esposito, M., Fabozzi, F., Iorio, A. O. M., Lanza, G., Lista, L., Meola, S., Merola, M., Paolucci, P., Sciacca, C., Thyssen, F., Azzi, P., Bacchetta, N., Benato, L., Bisello, D., Boletti, A., Branca, A., Carlin, R., Checchia, P., Dall'Osso, M., Dorigo, T., Dosselli, U., Gasparini, F., Gasparini, U., Gozzelino, A., Kanishchev, K., Lacaprara, S., Margoni, M., Meneguzzo, A. T., Montecassiano, F., Pazzini, J., Pozzobon, N., Ronchese, P., Simonetto, F., Torassa, E., Tosi, M., Zanetti, M., Zotto, P., Zucchetta, A., Zumerle, G., Braghieri, A., Magnani, A., Montagna, P., Ratti, S. P., Re, V., Riccardi, C., Salvini, P., Vai, I., Vitulo, P., Solestizi, L. Alunni, Bilei, G. M., Ciangottini, D., Fano, L., Lariccia, P., Mantovani, G., Menichelli, M., Saha, A., Santocchia, A., Androsov, K., Azzurri, P., Bagliesi, G., Bernardini, J., Boccali, T., Castaldi, R., Ciocci, M. A., Dell'Orso, R., Donato, S., Fedi, G., Foa, L., Giassi, A., Grippo, M. 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C., Shi, X., Shipsey, I., Silvers, D., Sun, J., Svyatkovskiy, A., Wang, F., Xie, W., Xu, L., Parashar, N., Stupak, J., Adair, A., Akgun, B., Chen, Z., Ecklund, K. M., Geurts, F. J. M., Guilbaud, M., Li, W., Michlin, B., Northup, M., Padley, B. P., Redjimi, R., Roberts, J., Rorie, J., Tu, Z., Zabel, J., Betchart, B., Bodek, A., De Barbaro, P., Demina, R., Eshaq, Y., Ferbel, T., Galanti, M., Garcia-Bellido, A., Han, J., Hindrichs, O., Khukhunaishvili, A., Lo, K. H., Tan, P., Verzetti, M., Chou, J. P., Contreras-Campana, E., Ferencek, D., Gershtein, Y., Halkiadakis, E., Heindl, M., Hidas, D., Hughes, E., Kaplan, S., Elayavalli, R. Kunnawalkam, Lath, A., Nash, K., Saka, H., Salur, S., Schnetzer, S., Sheffield, D., Somalwar, S., Stone, R., Thomas, S., Thomassen, P., Walker, M., Foerster, M., Riley, G., Rose, K., Spanier, S., Thapa, K., Bouhali, O., Hernandez, A. 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Show less - Abstract/Description
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A search for narrow resonances decaying to an electron and a muon is presented. The e mu mass spectrum is also investigated for non-resonant contributions from the production of quantum black holes (QBHs). The analysis is performed using data corresponding to an integrated luminosity of 19.7 fb(-1) collected in proton-proton collisions at a centre-of-mass energy of 8 TeV with the CMS detector at the LHC. With no evidence for physics beyond the standard model in the invariant mass spectrum of...
Show moreA search for narrow resonances decaying to an electron and a muon is presented. The e mu mass spectrum is also investigated for non-resonant contributions from the production of quantum black holes (QBHs). The analysis is performed using data corresponding to an integrated luminosity of 19.7 fb(-1) collected in proton-proton collisions at a centre-of-mass energy of 8 TeV with the CMS detector at the LHC. With no evidence for physics beyond the standard model in the invariant mass spectrum of selected e mu pairs, upper limits are set at 95 % confidence level on the product of cross section and branching fraction for signals arising in theories with charged lepton flavour violation. In the search for narrow resonances, the resonant production of a tau sneutrino in R-parity violating supersymmetry is considered. The t sneutrino is excluded for masses below 1.28 TeV for couplings lambda(132) = lambda(231) = lambda(')(311) = 0.01, and below 2.30 TeV for lambda(132) = lambda(231) = 0.07 and lambda(')(311) = 0.11. These are the most stringent limits to date from direct searches at high-energy colliders. In addition, the resonance searches are interpreted in terms of a model with heavy partners of the Z boson and the photon. In a framework of TeV-scale quantum gravity based on a renormalization of Newton's constant, the search for non-resonant contributions to the e mu mass spectrum excludes QBH production below a threshold mass M-th of 1.99 TeV. In models that invoke extra dimensions, the bounds range from 2.36 TeV for one extra dimension to 3.63 TeV for six extra dimensions. This is the first search for QBHs decaying into the e mu final state.
Show less - Date Issued
- 2016-06-10
- Identifier
- FSU_libsubv1_wos_000386035500001, 10.1140/epjc/s10052-016-4149-y
- Format
- Citation
- Title
- Search For Supersymmetry In Events With A Photon, A Lepton, And Missing Transverse Momentum In Pp Collisions At Root S=8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Knuenz, V., Koenig, A., Krammer, M., Kraetschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Ochesanu, S., Rougny, R., Van De Klundert, M., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Barria, P., Caillol, C., Clerbaux, B., De Lentdecker, G., Delannoy, H., Dobur, D., Fasanella, G., Favart, L., Gay, A. P. R., Grebenyuk, A., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-conde, A., Reis, T., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Rios, A. A. Ocampo, Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Strobbe, N., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Castello, R., Caudron, A., Ceard, L., Da Silveira, G. G., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Hollar, J., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Nuttens, C., Perrini, L., Pin, A., Piotrzkowski, K., Popov, A., Quertenmont, L., Selvaggi, M., Marono, M. Vidal, Beliy, N., Hammad, G. H., Alda Junior, W. L., Alves, G. A., Brito, L., Correa Martins Junior, M., Dos Reis Martins, T., Hensel, C., Mora Herrera, C., Moraes, A., Pol, M. E., Rebello Teles, P., Belchior Batista Das Chagas, E., Carvalho, W., Chinellato, J., Custodio, A., Da Costa, E. M., De Jesus Damiao, D., De Oliveira Martins, C., Fonseca De Souza, S., Huertas Guativa, L. M., Malbouisson, H., Matos Figueiredo, D., Mundim, L., Nogima, H., Prado Da Silva, W. L., Santoro, A., Sznajder, A., Tonelli Manganote, E. J., Vilela Pereira, A., Ahuja, S., Bernardes, C. A., De Souza Santos, A., Dogra, S., Fernandez Perez Tomei, T. R., Gregores, E. M., Mercadante, P. G., Moon, C. S., Novaes, S. F., Padula, Sandra S., Romero Abad, D., Ruiz Vargas, J. C., Aleksandrov, A., Genchev, V., Hadjiiska, R., Iaydjiev, P., Piperov, S., Rodozov, M., Stoykova, S., Sultanov, G., Vutova, M., Dimitrov, A., Glushkov, I., Litov, L., Pavlov, B., Petkov, P., Ahmad, M., Bian, J. G., Chen, G. M., Chen, H. S., Chen, M., Cheng, T., Du, R., Jiang, C. 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N., Nguyen, M., Ochando, C., Ortona, G., Paganini, P., Regnard, S., Salerno, R., Sauvan, J. B., Sirois, Y., Strebler, T., Yilmaz, Y., Zabi, A., Agram, J.-L., Andrea, J., Aubin, A., Bloch, D., Brom, J.-M., Buttignol, M., Chabert, E. C., Chanon, N., Collard, C., Conte, E., Coubez, X., Fontaine, J.-C., Gele, D., Goerlach, U., Goetzmann, C., Le Bihan, A.-C., Merlin, J. A., Skovpen, K., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Bouvier, E., Montoya, C. A. Carrillo, Chasserat, J., Chierici, R., Contardo, D., Courbon, B., Depasse, P., El Mamouni, H., Fan, J., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Alvarez, J. D. Ruiz, Sabes, D., Sgandurra, L., Sordini, V., Donckt, M. Vander, Verdier, P., Viret, S., Xiao, H., Toriashvili, T., Tsamalaidze, Z., Autermann, C., Beranek, S., Edelhoff, M., Feld, L., Heister, A., Kiesel, M. 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A., Carlsmith, D., Cepeda, M., Christian, A., Dasu, S., Dodd, L., Duric, S., Friis, E., Gomber, B., Hall-Wilton, R., Herndon, M., Herve, A., Klabbers, P., Lanaro, A., Levine, A., Long, K., Loveless, R., Mohapatra, A., Ojalvo, I., Perry, T., Pierro, G. A., Polese, G., Ross, I., Ruggles, T., Sarangi, T., Savin, A., Sharma, A., Smith, N., Smith, W. H., Taylor, D., Woods, N.
Show less - Abstract/Description
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A search for supersymmetry involving events with at least one photon, one electron or muon, and large missing transverse momentum has been performed by the CMS experiment. The data sample corresponds to an integrated luminosity of 19.7 fb(-1) of pp collisions at root s = 8 TeV, produced at the CERN LHC. No excess of events is observed beyond expectations from standard model processes. The result of the search is interpreted in the context of a general model of gauge-mediated supersymmetry...
Show moreA search for supersymmetry involving events with at least one photon, one electron or muon, and large missing transverse momentum has been performed by the CMS experiment. The data sample corresponds to an integrated luminosity of 19.7 fb(-1) of pp collisions at root s = 8 TeV, produced at the CERN LHC. No excess of events is observed beyond expectations from standard model processes. The result of the search is interpreted in the context of a general model of gauge-mediated supersymmetry breaking, where the charged and neutral winos are the next-to-lightest supersymmetric particles. Within this model, winos with a mass up to 360 GeV are excluded at the 95% confidence level. Two simplified models inspired by gauge-mediated supersymmetry breaking are also examined, and used to derive upper limits on the production cross sections of specific supersymmetric processes. (C) 2016 CERN for the benefit of the CMS Collaboration. Published by Elsevier B.V.
Show less - Date Issued
- 2016-06-10
- Identifier
- FSU_libsubv1_wos_000376800300002, 10.1016/j.physletb.2016.03.039
- Format
- Citation
- Title
- Measurement Of The Cp-violating Weak Phase Phi(s) And The Decay Width Difference Delta Gamma(s) Using The B-s(0) -> J/psi Phi (1020) Decay Channel In Pp Collisions At Root S=8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Knuenz, V., Koenig, A., Krammer, M., Kraetschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Ochesanu, S., Rougny, R., De Klundert, M. Van, Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Barria, P., Brun, H., Caillol, C., Clerbaux, B., De Lentdecker, G., Delannoy, H., Fasanella, G., Favart, L., Gay, A. P. R., Grebenyuk, A., Karapostoli, G., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-Conde, A., Reis, T., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Dobur, D., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Rios, A. A. Ocampo, Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Strobbe, N., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Castello, R., Caudron, A., Ceard, L., Da Silveira, G. G., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Hollar, J., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Nuttens, C., Perrini, L., Pin, A., Piotrzkowski, K., Popov, A., Quertenmont, L., Selvaggi, M., Marono, M. Vidal, Beliy, N., Hammad, G. H., Alda Junior, W. 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M., Tao, J., Wang, C., Wang, Z., Zhang, H., Asawatangtrakuldee, C., Ban, Y., Li, Q., Liu, S., Mao, Y., Qian, S. J., Wang, D., Xu, Z., Zou, W., Avila, C., Cabrera, A., Chaparro Sierra, L. F., Florez, C., Gomez, J. P., Gomez Moreno, B., Sanabria, J. C., Godinovic, N., Lelas, D., Puljak, I., Cipriano, P. M. Ribeiro, Antunovic, Z., Kovac, M., Brigljevic, V., Kadija, K., Luetic, J., Micanovic, S., Sudic, L., Attikis, A., Mavromanolakis, G., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. 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N., Nguyen, M., Ochando, C., Ortona, G., Paganini, P., Pigard, P., Regnard, S., Salerno, R., Sauvan, J. B., Sirois, Y., Strebler, T., Yilmaz, Y., Zabi, A., Agram, J.-L., Andrea, J., Aubin, A., Bloch, D., Brom, J.-M., Buttignol, M., Chabert, E. C., Chanon, N., Collard, C., Conte, E., Coubez, X., Fontaine, J.-C., Gele, D., Goerlach, U., Goetzmann, C., Le Bihan, A.-C., Merlin, J. A., Skovpen, K., Van Hove, P., Gadrat, S., Beauceron, S., Bernet, C., Boudoul, G., Bouvier, E., Montoya, C. A. Carrillo, Chierici, R., Contardo, D., Courbon, B., Depasse, P., El Mamouni, H., Fan, J., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Lagarde, F., Laktineh, I. B., Lethuillier, M., Mirabito, L., Pequegnot, A. L., Perries, S., Alvarez, J. D. Ruiz, Sabes, D., Sgandurra, L., Sordini, V., Vander Donckt, M., Verdier, P., Viret, S., Xiao, H., Toriashvili, T., Tsamalaidze, Z., Autermann, C., Beranek, S., Edelhoff, M., Feld, L., Heister, A., Kiesel, M. 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Diez, Dolinska, G., Dooling, S., Dorland, T., Eckerlin, G., Eckstein, D., Eichhorn, T., Flucke, G., Gallo, E., Garcia, J. Garay, Geiser, A., Gizhko, A., Gunnellini, P., Hauk, J., Hempel, M., Jung, H., Kalogeropoulos, A., Karacheban, O., Kasemann, M., Katsas, P., Kieseler, J., Kleinwort, C., Korol, I., Lange, W., Leonard, J., Lipka, K., Lobanov, A., Lohmann, W., Mankel, R., Marfin, I., Melzer-Pellmann, I.-A., Meyer, A. B., Mittag, G., Mnich, J., Mussgiller, A., Naumann-Emme, S., Nayak, A., Ntomari, E., Perrey, H., Pitzl, D., Placakyte, R., Raspereza, A., Roland, B., Sahin, M. Oe, Saxena, P., Schoerner-Sadenius, T., Schroeder, M., Seitz, C., Spannagel, S., Trippkewitz, K. D., Walsh, R., Wissing, C., Blobel, V., Vignali, M. Centis, Draeger, A. R., Erfle, J., Garutti, E., Goebel, K., Gonzalez, D., Goerner, M., Haller, J., Hoffmann, M., Hoeing, R. 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Show less - Abstract/Description
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The CP-violating weak phase phi(s) of the B-s(0) meson and the decay width difference Delta Gamma(s) of the B-s(0) light and heavy mass eigenstates are measured with the CMS detector at the LHC using a data sample of B-s(0)-> J/psi phi(1020) -> mu(+)mu-K+K- decays. The analysed data set corresponds to an integrated luminosity of 19.7 fb(-1) collected in pp collisions at a centre-of-mass energy of 8 TeV. A total of 49200 reconstructed B-s(0) decays are used to extract the values of phi(s) and...
Show moreThe CP-violating weak phase phi(s) of the B-s(0) meson and the decay width difference Delta Gamma(s) of the B-s(0) light and heavy mass eigenstates are measured with the CMS detector at the LHC using a data sample of B-s(0)-> J/psi phi(1020) -> mu(+)mu-K+K- decays. The analysed data set corresponds to an integrated luminosity of 19.7 fb(-1) collected in pp collisions at a centre-of-mass energy of 8 TeV. A total of 49200 reconstructed B-s(0) decays are used to extract the values of phi(s) and Delta Gamma(s) by performing a time dependent and flavour-tagged angular analysis of the mu(+)mu-K+K- final state. The weak phase is measured to be phi(s) =-0.075 +/- 0.097 (stat) +/- 0.031 (syst) rad, and the decay width difference is Delta Gamma(s) = 0.095 +/- 0.013 (stat) +/- 0.007 (syst) ps(-1). (C) 2016 CERN for the benefit of the CMS Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP(3).
Show less - Date Issued
- 2016-06-10
- Identifier
- FSU_libsubv1_wos_000376800300014, 10.1016/j.physletb.2016.03.046
- Format
- Citation
- Title
- Inclusive And Differential Measurements Of The T(t)over-bar Charge Asymmetry In Pp Collisions At Root S=8 Tev.
- Creator
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Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth...
Show moreKhachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Eroe, J., Flechl, M., Friedl, M., Fruehwirth, R., Ghete, V. M., Hartl, C., Hoermann, N., Hrubec, J., Jeitler, M., Knuenz, V., Koenig, A., Krammer, M., Kraetschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rahbaran, B., Rohringer, H., Schieck, J., Schoefbeck, R., Strauss, J., Treberer-Treberspurg, W., Waltenberger, W., Wulz, C.-E., Mossolov, V., Shumeiko, N., Gonzalez, J. Suarez, Alderweireldt, S., Cornelis, T., De Wolf, E. A., Janssen, X., Knutsson, A., Lauwers, J., Luyckx, S., Ochesanu, S., Rougny, R., Van De Klundert, M., Van Haevermaet, H., Van Mechelen, P., Van Remortel, N., Van Spilbeeck, A., Abu Zeid, S., Blekman, F., D'Hondt, J., Daci, N., De Bruyn, I., Deroover, K., Heracleous, N., Keaveney, J., Lowette, S., Moreels, L., Olbrechts, A., Python, Q., Strom, D., Tavernier, S., Van Doninck, W., Van Mulders, P., Van Onsem, G. P., Van Parijs, I., Barria, P., Caillol, C., Clerbaux, B., De Lentdecker, G., Delannoy, H., Fasanella, G., Favart, L., Gay, A. P. R., Grebenyuk, A., Lenzi, T., Leonard, A., Maerschalk, T., Marinov, A., Pernie, L., Randle-Conde, A., Reis, T., Seva, T., Vander Velde, C., Vanlaer, P., Yonamine, R., Zenoni, F., Zhang, F., Beernaert, K., Benucci, L., Cimmino, A., Crucy, S., Dobur, D., Fagot, A., Garcia, G., Gul, M., Mccartin, J., Rios, A. A. Ocampo, Poyraz, D., Ryckbosch, D., Salva, S., Sigamani, M., Strobbe, N., Tytgat, M., Van Driessche, W., Yazgan, E., Zaganidis, N., Basegmez, S., Beluffi, C., Bondu, O., Brochet, S., Bruno, G., Castello, R., Caudron, A., Ceard, L., Da Silveira, G. G., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Hollar, J., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Nuttens, C., Perrini, L., Pin, A., Piotrzkowski, K., Popov, A., Quertenmont, L., Selvaggi, M., Marono, M. Vidal, Beliy, N., Hammad, G. H., Alda Junior, W. L., Alves, G. 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A., Kubik, A., Mucia, N., Odell, N., Pollack, B., Pozdnyakov, A., Schmitt, M., Stoynev, S., Sung, K., Trovato, M., Velasco, M., Won, S., Brinkerhoff, A., Dev, N., Hildreth, M., Jessop, C., Karmgard, D. J., Kellams, N., Lannon, K., Lynch, S., Marinelli, N., Meng, F., Mueller, C., Musienko, Y., Pearson, T., Planer, M., Reinsvold, A., Ruchti, R., Smith, G., Taroni, S., Valls, N., Wayne, M., Wolf, M., Woodard, A., Antonelli, L., Brinson, J., Bylsma, B., Durkin, L. S., Flowers, S., Hart, A., Hill, C., Hughes, R., Kotov, K., Ling, T. Y., Liu, B., Luo, W., Puigh, D., Rodenburg, M., Winer, B. L., Wulsin, H. W., Driga, O., Elmer, P., Hardenbrook, J., Hebda, P., Koay, S. A., Lujan, P., Marlow, D., Medvedeva, T., Mooney, M., Olsen, J., Palmer, C., Piroue, R., Quan, X., Saka, H., Stickland, D., Tully, C., Werner, J. S., Zuranski, A., Barnes, V. E., Benedetti, D., Bortoletto, D., Gutay, L., Jha, M. K., Jones, M., Jung, K., Kress, M., Miller, D. H., Neumeister, N., Primavera, F., Radburn-Smith, B. C., Shi, X., Shipsey, I., Silvers, D., Sun, J., Svyatkovskiy, A., Wang, F., Xie, W., Xu, L., Zablocki, J., Parashar, N., Stupak, J., Adair, A., Akgun, B., Chen, Z., Ecklund, K. M., Geurts, F. J. M., Guilbaud, M., Li, W., Michlin, B., Northup, M., Padley, B. P., Redjimi, R., Roberts, J., Rorie, J., Tu, Z., Zabel, J., Betchart, B., Bodek, A., de Barbaro, P., Demina, R., Eshaq, Y., Ferbel, T., Galanti, M., Garcia-Bellido, A., Goldenzweig, P., Han, J., Harel, A., Hindrichs, O., Khukhunaishvili, A., Petrillo, G., Verzetti, M., Demortier, L., Arora, S., Barker, A., Chou, J. P., Contreras-Campana, C., Contreras-Campana, E., Duggan, D., Ferencek, D., Gershtein, Y., Gray, R., Halkiadakis, E., Hidas, D., Hughes, E., Kaplan, S., Elayavalli, R. Kunnawalkam, Lath, A., Nash, K., Panwalkar, S., Park, M., Salur, S., Schnetzer, S., Sheffield, D., Somalwar, S., Stone, R., Thomas, S., Thomassen, P., Walker, M., Foerster, M., Riley, G., Rose, K., Spanier, S., York, A., Bouhali, O., Hernandez, A. Castaneda, Dalchenko, M., De Mattia, M., Delgado, A., Dildick, S., Eusebi, R., Flanagan, W., Gilmore, J., Kamon, T., Krutelyov, V., Montalvo, R., Mueller, R., Osipenkov, I., Pakhotin, Y., Patel, R., Perloff, A., Roe, J., Rose, A., Safonov, A., Tatarinov, A., Ulmer, K. A., Akchurin, N., Cowden, C., Damgov, J., Dragoiu, C., Dudero, P. R., Faulkner, J., Kunori, S., Lamichhane, K., Lee, S. W., Libeiro, T., Undleeb, S., Volobouev, I., Appelt, E., Delannoy, A. G., Greene, S., Gurrola, A., Janjam, R., Johns, W., Maguire, C., Mao, Y., Melo, A., Sheldon, P., Snook, B., Tuo, S., Velkovska, J., Xu, Q., Arenton, M. W., Boutle, S., Cox, B., Francis, B., Goodell, J., Hirosky, R., Ledovskoy, A., Li, H., Lin, C., Neu, C., Wolfe, E., Wood, J., Xia, F., Clarke, C., Harr, R., Karchin, P. E., Don, C. Kottachchi Kankanamge, Lamichhane, P., Sturdy, J., Belknap, D. A., Carlsmith, D., Cepeda, M., Christian, A., Dasu, S., Dodd, L., Duric, S., Friis, E., Gomber, B., Hall-Wilton, R., Herndon, M., Herve, A., Klabbers, R., Lanaro, A., Levine, A., Long, K., Loveless, R., Mohapatra, A., Ojalvo, I., Perry, T., Pierro, G. A., Polese, G., Ross, I., Ruggles, T., Sarangi, T., Savin, A., Sharma, A., Smith, N., Smith, W. H., Taylor, D., Woods, N.
Show less - Abstract/Description
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The t (t) over bar charge asymmetry is measured in proton-proton collisions at a centre-of-mass energy of 8 TeV. The data, collected with the CMS experiment at the LHC, correspond to an integrated luminosity of 19.7 fb(-1). Selected events contain an electron or a muon and four or more jets, where at least one jet is identified as originating from b-quark hadronization. The inclusive charge asymmetry is found to be 0.0010 +/- 0.0068 (stat)+/- 0.0037 (syst). In addition, differential charge...
Show moreThe t (t) over bar charge asymmetry is measured in proton-proton collisions at a centre-of-mass energy of 8 TeV. The data, collected with the CMS experiment at the LHC, correspond to an integrated luminosity of 19.7 fb(-1). Selected events contain an electron or a muon and four or more jets, where at least one jet is identified as originating from b-quark hadronization. The inclusive charge asymmetry is found to be 0.0010 +/- 0.0068 (stat)+/- 0.0037 (syst). In addition, differential charge asymmetries as a function of rapidity, transverse momentum, and invariant mass of the If system are studied. For the first time at the LHC, the measurements are also performed in a reduced fiducial phase space of top quark pair production, with an integrated result of -0.0035 +/- 0.0072 (stat) +/- 0.0031 (syst). All measurements are consistent within two standard deviations with zero asymmetry as well as with the predictions of the standard model. (C) 2016 CERN for the benefit of the CMS Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP(3).
Show less - Date Issued
- 2016-06-10
- Identifier
- FSU_libsubv1_wos_000376800300021, 10.1016/j.physletb.2016.03.060
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- Citation
- Title
- Chronic Methamphetamine Effects on Brain Structure and Function in Rats.
- Creator
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Thanos, Panayotis K., Kim, Ronald, Delis, Foteini, Ananth, Mala, Chachati, George, Rocco, Mark J., Masad, Ihssan, Muniz, Jose A., Grant, Samuel C., Gold, Mark S., Cadet, Jean...
Show moreThanos, Panayotis K., Kim, Ronald, Delis, Foteini, Ananth, Mala, Chachati, George, Rocco, Mark J., Masad, Ihssan, Muniz, Jose A., Grant, Samuel C., Gold, Mark S., Cadet, Jean Lud, Volkow, Nora D.
Show less - Abstract/Description
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Methamphetamine (MA) addiction is a growing epidemic worldwide. Chronic MA use has been shown to lead to neurotoxicity in rodents and humans. Magnetic resonance imaging (MRI) studies in MA users have shown enlarged striatal volumes and positron emission tomography (PET) studies have shown decreased brain glucose metabolism (BGluM) in the striatum of detoxified MA users. The present study examines structural changes of the brain, observes microglial activation, and assesses changes in brain...
Show moreMethamphetamine (MA) addiction is a growing epidemic worldwide. Chronic MA use has been shown to lead to neurotoxicity in rodents and humans. Magnetic resonance imaging (MRI) studies in MA users have shown enlarged striatal volumes and positron emission tomography (PET) studies have shown decreased brain glucose metabolism (BGluM) in the striatum of detoxified MA users. The present study examines structural changes of the brain, observes microglial activation, and assesses changes in brain function, in response to chronic MA treatment. Rats were randomly split into three distinct treatment groups and treated daily for four months, via i.p. injection, with saline (controls), or low dose (LD) MA (4 mg/kg), or high dose (HD) MA (8 mg/kg). Sixteen weeks into the treatment period, rats were injected with a glucose analog, [F-18] fluorodeoxyglucose (FDG), and their brains were scanned with micro-PET to assess regional BGluM. At the end of MA treatment, magnetic resonance imaging at 21T was performed on perfused rats to determine regional brain volume and in vitro [H-3]PK 11195 autoradiography was performed on fresh-frozen brain tissue to measure microglia activation. When compared with controls, chronic HD MA-treated rats had enlarged striatal volumes and increases in [H-3]PK 11195 binding in striatum, the nucleus accumbens, frontal cortical areas, the rhinal cortices, and the cerebellar nuclei. FDG microPET imaging showed that LD MA-treated rats had higher BGluM in insular and somatosensory cortices, face sensory nucleus of the thalamus, and brainstem reticular formation, while HD MA-treated rats had higher BGluM in primary and higher order somatosensory and the retrosplenial cortices, compared with controls. HD and LD MA-treated rats had lower BGluM in the tail of the striatum, rhinal cortex, and subiculum and HD MA also had lower BGluM in hippocampus than controls. These results corroborate clinical findings and help further examine the mechanisms behind MA-induced neurotoxicity.
Show less - Date Issued
- 2016-06-08
- Identifier
- FSU_libsubv1_wos_000377561700005, 10.1371/journal.pone.0155457
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- Citation
- Title
- Crystallization of spin superlattices with pressure and field in the layered magnet SrCu2(BO3)(2).
- Creator
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Haravifard, S., Graf, D., Feiguin, A. E., Batista, C. D., Lang, J. C., Silevitch, D. M., Srajer, G., Gaulin, B. D., Dabkowska, H. A., Rosenbaum, T. F.
- Abstract/Description
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An exact mapping between quantum spins and boson gases provides fresh approaches to the creation of quantum condensates and crystals. Here we report on magnetization measurements on the dimerized quantum magnet SrCu2(BO3)(2) at cryogenic temperatures and through a quantum-phase transition that demonstrate the emergence of fractionally filled bosonic crystals in mesoscopic patterns, specified by a sequence of magnetization plateaus. We apply tens of Teslas of magnetic field to tune the density...
Show moreAn exact mapping between quantum spins and boson gases provides fresh approaches to the creation of quantum condensates and crystals. Here we report on magnetization measurements on the dimerized quantum magnet SrCu2(BO3)(2) at cryogenic temperatures and through a quantum-phase transition that demonstrate the emergence of fractionally filled bosonic crystals in mesoscopic patterns, specified by a sequence of magnetization plateaus. We apply tens of Teslas of magnetic field to tune the density of bosons and gigapascals of hydrostatic pressure to regulate the underlying interactions. Simulations help parse the balance between energy and geometry in the emergent spin superlattices. The magnetic crystallites are the end result of a progression from a direct product of singlet states in each short dimer at zero field to preferred filling fractions of spin-triplet bosons in each dimer at large magnetic field, enriching the known possibilities for collective states in both quantum spin and atomic systems.
Show less - Date Issued
- 2016-06
- Identifier
- FSU_libsubv1_wos_000379086000001, 10.1038/ncomms11956
- Format
- Citation
- Title
- Superconducting Subphase In The Layered Perovskite Ruthenate Sr2ruo4 In A Parallel Magnetic Field.
- Creator
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Kikugawa, Naoki, Terashima, Taichi, Uji, Shinya, Sugii, Kaori, Maeno, Yoshiteru, Graf, David, Baumbach, Ryan, Brooks, James
- Abstract/Description
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Magnetic torque measurements using a microcantilever have been performed to investigate the superconducting phase of Sr2RuO4 down to 40 mK. For high-quality single crystals with the transition temperature (T-c) of 1.48-1.49 K, an abrupt jump of the torque signal is found near 1.5 T in field parallel to the conducting RuO2 planes below similar to 0.8K. The jump corresponds to the first order transition recently revealed by magnetocaloric and magnetization measurements [Yonezawa et al., Phys....
Show moreMagnetic torque measurements using a microcantilever have been performed to investigate the superconducting phase of Sr2RuO4 down to 40 mK. For high-quality single crystals with the transition temperature (T-c) of 1.48-1.49 K, an abrupt jump of the torque signal is found near 1.5 T in field parallel to the conducting RuO2 planes below similar to 0.8K. The jump corresponds to the first order transition recently revealed by magnetocaloric and magnetization measurements [Yonezawa et al., Phys. Rev. Lett. 110, 077003 (2013); Kittaka et al., Phys. Rev. B 90, 220502(R) (2014)]. Furthermore, weak diamagnetic and irreversible signals are found to persist above the first order transition up to 1.85 T. The result indicates the presence of a subphase boundary separating low-and high-field phases in the superconducting phase. The high-field subphase disappears when the field is tilted from the conducting planes only by a few degrees. Quantum oscillation measurements are also reported to clarify the strong sample-quality dependence of the high-field subphase.
Show less - Date Issued
- 2016-05-31
- Identifier
- FSU_libsubv1_wos_000376908700006, 10.1103/PhysRevB.93.184513
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- Citation
- Title
- Striped Quantum Hall State In A Half-filled Landau Level.
- Creator
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Wan, Xin, Yang, Kun
- Abstract/Description
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The nature of the fractional quantum Hall state at Landau level filling factor 5/2 remains elusive despite intensive experimental and theoretical work. While the leading theoretical candidates are Moore-Read Pfaffian (Pf) and its particle-hole conjugate anti-Pfaffian (APf), neither received unambiguous experimental support. We show that a state that is intermediate between them, made of alternating stripes of Pf and APf in the bulk, is a viable candidate. Such a state is shown to be...
Show moreThe nature of the fractional quantum Hall state at Landau level filling factor 5/2 remains elusive despite intensive experimental and theoretical work. While the leading theoretical candidates are Moore-Read Pfaffian (Pf) and its particle-hole conjugate anti-Pfaffian (APf), neither received unambiguous experimental support. We show that a state that is intermediate between them, made of alternating stripes of Pf and APf in the bulk, is a viable candidate. Such a state is shown to be incompressible and thus a charge insulator in the bulk, but a heat conductor due to the presence of gapless neutral bulk modes. We argue that the properties of such a state are consistent with existing numerical and experimental work, and discuss possible experimental probes of its presence.
Show less - Date Issued
- 2016-05-23
- Identifier
- FSU_libsubv1_wos_000376638200001, 10.1103/PhysRevB.93.201303
- Format
- Citation