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(1 - 12 of 12)
- Title
- Anomalous Thermal Conductivity And Magnetic Torque Response In The Honeycomb Magnet Alpha-rucl3.
- Creator
- Leahy, Ian A., Pocs, Christopher A., Siegfried, Peter E., Graf, David, Do, S.-H., Choi, Kwang-Yong, Normand, B., Lee, Minhyea
- Abstract/Description
-
We report on the unusual behavior of the in-plane thermal conductivity. and torque tau response in the Kitaev-Heisenberg material alpha-RuCl3. kappa shows a striking enhancement with linear growth beyond H = 7 T, where magnetic order disappears, while t for both of the in-plane symmetry directions shows an anomaly at the same field. The temperature and field dependence of kappa are far more complex than conventional phonon and magnon contributions, and require us to invoke the presence of...
Show moreWe report on the unusual behavior of the in-plane thermal conductivity. and torque tau response in the Kitaev-Heisenberg material alpha-RuCl3. kappa shows a striking enhancement with linear growth beyond H = 7 T, where magnetic order disappears, while t for both of the in-plane symmetry directions shows an anomaly at the same field. The temperature and field dependence of kappa are far more complex than conventional phonon and magnon contributions, and require us to invoke the presence of unconventional spin excitations whose properties are characteristic of a field-induced spin-liquid phase related to the enigmatic physics of the Kitaev model in an applied magnetic field.
Show less - Date Issued
- 2017-05-05
- Identifier
- FSU_libsubv1_wos_000400673100007, 10.1103/PhysRevLett.118.187203
- Format
- Citation
- Title
- Thermodynamic Measurement Of Angular Anisotropy At The Hidden Order Transition Of Uru2si2.
- Creator
- Trinh, Jennifer, Bruck, Ekkes, Siegrist, Theo, Flint, Rebecca, Chandra, Premala, Coleman, Piers, Ramirez, Arthur P.
- Abstract/Description
-
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
- Magnetoelectric Coupling Through The Spin Flop Transition In Ni3teo6.
- Creator
- 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, Vanderbilt, David, Musfeldt, J. L.
- Abstract/Description
-
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
- Fate Of Spinons At The Mott Point.
- Creator
- Lee, Tsung-Han, Florens, Serge, Dobrosavljevic, Vladimir
- Abstract/Description
-
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
- Interaction-driven Spontaneous Quantum Hall Effect On A Kagome Lattice.
- Creator
- 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
- 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
-
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
- Evidence Of Topological Nodal-line Fermions In Zrsise And Zrsite.
- Creator
- 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
-
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
- Measurement of Long-Range Near-Side Two-Particle Angular Correlations in pp Collisions at root s=13 TeV.
- Creator
- Khachatryan, V., Sirunyan, A. M., Tumasyan, A., Adam, W., Asilar, E., Bergauer, T., Brandstetter, J., Brondolin, E., Dragicevic, M., Ero, J., Flechl, M., Friedl, M., Fruhwirth, R., Ghete, V. M., Hartl, C., Hormann, N., Hrubec, J., Jeitler, M., Knunz, V., Konig, A., Krammer, M., Kratschmer, I., Liko, D., Matsushita, T., Mikulec, I., Rabady, D., Rahbaran, B., Rohringer, H., Schieck, J., Schofbeck, 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., Fasanella, G., Favart, L., 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., Da Silveira, G. G., Delaere, C., Favart, D., Forthomme, L., Giammanco, A., Hollar, J., Jafari, A., Jez, P., Komm, M., Lemaitre, V., Mertens, A., Musich, M., 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, 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., 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., Sierra, L. F. Chaparro, 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., El-khateeb, E., Elkafrawy, T., Mohamed, A., Salama, E., 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., 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., 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., 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. 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., Guth, 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., 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., Campbell, A., 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. O., Saxena, P., Schoerner-Sadenius, T., 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., 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., Schettler, H., Schleper, P., Schlieckau, E., Schmidt, A., Schwandt, J., Sola, V., Stadie, H., Steinbrueck, G., Tholen, H., Troendle, D., Usai, E., Vanelderen, L., Vanhoefer, A., Vormwald, B., Barth, C., Baur, S., 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., Stober, F. M., 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., Jain, Sa, Majumdar, N., Modak, A., Mondal, K., 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., Sur, N., Sutar, B., Wickramage, N., Chauhan, S., Dube, S., Kapoor, A., Kothekar, K., 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., 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., 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., 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. 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F., Mucia, N., Odell, N., Pollack, B., Schmitt, M., Stoynev, S., Sung, K., Trovato, M., Velasco, M., Brinkerhoff, A., 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., 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., Saka, H., 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., Kumar, A., 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., Harel, A., Hindrichs, O., Khukhunaishvili, A., Petrillo, G., Tan, P., Verzetti, M., Arora, S., Chou, J. P., Contreras-Campana, C., Contreras-Campana, E., 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., 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., 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., Cox, B., Francis, B., Goodell, J., Hirosky, R., Ledovskoy, A., Li, H., Lin, C., 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., Cepeda, M., Dasu, S., Dodd, L., Duric, S., 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., Verwilligen, P., Woods, N.
- Abstract/Description
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Results on two-particle angular correlations for charged particles produced in pp collisions at a center-of- mass energy of 13 TeV are presented. The data were taken with the CMS detector at the LHC and correspond to an integrated luminosity of about 270 nb(-1). The correlations are studied over a broad range of pseudorapidity (vertical bar eta vertical bar < 2.4) and over the full azimuth (phi) as a function of charged particle multiplicity and transverse momentum (p(T)). In high...
Show moreResults on two-particle angular correlations for charged particles produced in pp collisions at a center-of- mass energy of 13 TeV are presented. The data were taken with the CMS detector at the LHC and correspond to an integrated luminosity of about 270 nb(-1). The correlations are studied over a broad range of pseudorapidity (vertical bar eta vertical bar < 2.4) and over the full azimuth (phi) as a function of charged particle multiplicity and transverse momentum (p(T)). In high-multiplicity events, a long-range (vertical bar Delta eta vertical bar > 2.0), near-side (Delta phi approximate to 0) structure emerges in the two-particle Delta eta-Delta phi correlation functions. The magnitude of the correlation exhibits a pronounced maximum in the range 1.0 < p(T) < 2.0 GeV/c and an approximately linear increase with the charged particle multiplicity, with an overall correlation strength similar to that found in earlier pp data at root s = 7 TeV. The present measurement extends the study of near-side long-range correlations up to charged particle multiplicities N-ch similar to 180, a region so far unexplored in pp collisions. The observed longrange correlations are compared to those seen in pp, pPb, and PbPb collisions at lower collision energies.
Show less - Date Issued
- 2016-04-27
- Identifier
- FSU_libsubv1_wos_000374964400005, 10.1103/PhysRevLett.116.172302
- Format
- Citation
- Title
- Fractional Quantum Hall States in a Ge Quantum Well.
- Creator
- Mironov, O. A., d'Ambrumenil, N., Dobbie, A., Leadley, D. R., Suslov, A. V., Green, E.
- Abstract/Description
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Measurements of the Hall and dissipative conductivity of a strained Ge quantum well on a SiGe/(001)Si substrate in the quantum Hall regime are reported. We analyze the results in terms of thermally activated quantum tunneling of carriers from one internal edge state to another across saddle points in the long-range impurity potential. This shows that the gaps for different filling fractions closely follow the dependence predicted by theory. We also find that the estimates of the separation of...
Show moreMeasurements of the Hall and dissipative conductivity of a strained Ge quantum well on a SiGe/(001)Si substrate in the quantum Hall regime are reported. We analyze the results in terms of thermally activated quantum tunneling of carriers from one internal edge state to another across saddle points in the long-range impurity potential. This shows that the gaps for different filling fractions closely follow the dependence predicted by theory. We also find that the estimates of the separation of the edge states at the saddle are in line with the expectations of an electrostatic model in the lowest spin-polarized Landau level (LL), but not in the spin-reversed LL where the density of quasiparticle states is not high enough to accommodate the carriers required.
Show less - Date Issued
- 2016-04-27
- Identifier
- FSU_libsubv1_wos_000374964400011, 10.1103/PhysRevLett.116.176802
- Format
- Citation
- Title
- Magnetic Ground States of the Rare-Earth Tripod Kagome Lattice Mg2RE3Sb3O14 (RE = Gd,Dy,Er).
- Creator
- Dun, Z. L., Trinh, J., Li, K., Lee, M., Chen, K. W., Baumbach, R., Hu, Y. F., Wang, Y. X., Choi, E. S., Shastry, B. S., Ramirez, A. P., Zhou, H. D.
- Abstract/Description
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We present the structural and magnetic properties of a new compound family, Mg2RE3Sb3O14 (RE = Gd, Dy, Er), with a hitherto unstudied frustrating lattice, the "tripod kagome" structure. Susceptibility (ac, dc) and specific heat exhibit features that are understood within a simple Luttinger-Tisza-type theory. For RE = Gd, we found long-ranged order (LRO) at 1.65 K, which is consistent with a 120 degrees structure, demonstrating the importance of diople interactions for this 2D Heisenberg...
Show moreWe present the structural and magnetic properties of a new compound family, Mg2RE3Sb3O14 (RE = Gd, Dy, Er), with a hitherto unstudied frustrating lattice, the "tripod kagome" structure. Susceptibility (ac, dc) and specific heat exhibit features that are understood within a simple Luttinger-Tisza-type theory. For RE = Gd, we found long-ranged order (LRO) at 1.65 K, which is consistent with a 120 degrees structure, demonstrating the importance of diople interactions for this 2D Heisenberg system. For RE = Dy, LRO at 0.37 K is related to the "kagome spin ice" physics for a 2D system. This result shows that the tripod kagome structure accelerates the transition to LRO predicted for the related pyrochlore systems. For RE = Er, two transitions, at 80 mK and 2.1 K are observed, suggesting the importance of quantum fluctuations for this putative XY system.
Show less - Date Issued
- 2016-04-12
- Identifier
- FSU_libsubv1_wos_000373773600014, 10.1103/PhysRevLett.116.157201
- Format
- Citation
- Title
- Static and Dynamical Properties of the Spin-1/2 Equilateral Triangular-Lattice Antiferromagnet Ba3CoSb2O9.
- Creator
- Ma, J., Kamiya, Y., Hong, Tao, Cao, H. B., Ehlers, G., Tian, W., Batista, C. D., Dun, Z. L., Zhou, H. D., Matsuda, M.
- Abstract/Description
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We present single-crystal neutron scattering measurements of the spin-1/2 equilateral triangular-lattice antiferromagnet Ba3CoSb2O9. Besides confirming that the Co2+ magnetic moments lie in the ab plane for zero magnetic field and then determining all the exchange parameters of the minimal quasi-2D spin Hamiltonian, we provide conclusive experimental evidence of magnon decay through observation of intrinsic line broadening. Through detailed comparisons with the linear and nonlinear spin-wave...
Show moreWe present single-crystal neutron scattering measurements of the spin-1/2 equilateral triangular-lattice antiferromagnet Ba3CoSb2O9. Besides confirming that the Co2+ magnetic moments lie in the ab plane for zero magnetic field and then determining all the exchange parameters of the minimal quasi-2D spin Hamiltonian, we provide conclusive experimental evidence of magnon decay through observation of intrinsic line broadening. Through detailed comparisons with the linear and nonlinear spin-wave theories, we also point out that the large-S approximation, which is conventionally employed to predict magnon decay in noncollinear magnets, is inadequate to explain our experimental observation. Thus, our results call for a new theoretical framework for describing excitation spectra in low-dimensional frustrated magnets under strong quantum effects.
Show less - Date Issued
- 2016-02-24
- Identifier
- FSU_libsubv1_wos_000370816600004, 10.1103/PhysRevLett.116.087201
- Format
- Citation
- Title
- Energy Gaps and Layer Polarization of Integer and Fractional Quantum Hall States in Bilayer Graphene.
- Creator
- Shi, Yanmeng, Lee, Yongjin, Che, Shi, Pi, Ziqi, Espiritu, Timothy, Stepanov, Petr, Smirnov, Dmitry, Lau, Chun Ning, Zhang, Fan
- Abstract/Description
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Owing to the spin, valley, and orbital symmetries, the lowest Landau level in bilayer graphene exhibits multicomponent quantum Hall ferromagnetism. Using transport spectroscopy, we investigate the energy gaps of integer and fractional quantum Hall (QH) states in bilayer graphene with controlled layer polarization. The state at filling factor nu = 1 has two distinct phases: a layer polarized state that has a larger energy gap and is stabilized by high electric field, and a hitherto unobserved...
Show moreOwing to the spin, valley, and orbital symmetries, the lowest Landau level in bilayer graphene exhibits multicomponent quantum Hall ferromagnetism. Using transport spectroscopy, we investigate the energy gaps of integer and fractional quantum Hall (QH) states in bilayer graphene with controlled layer polarization. The state at filling factor nu = 1 has two distinct phases: a layer polarized state that has a larger energy gap and is stabilized by high electric field, and a hitherto unobserved interlayer coherent state with a smaller gap that is stabilized by large magnetic field. In contrast, the nu = 2/3 quantum Hall state and a feature at nu = 1/2 are only resolved at finite electric field and large magnetic field. These results underscore the importance of controlling layer polarization in understanding the competing symmetries in the unusual QH system of BLG.
Show less - Date Issued
- 2016-02-05
- Identifier
- FSU_libsubv1_wos_000369495000015, 10.1103/PhysRevLett.116.056601
- Format
- Citation
