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¹ØÓÚ²£É«²£Á§ÏàµÄ˼¿¼ ·¢±íÈÕÆÚ£º2012Äê9ÔÂ20ÈÕ ²£É«-°®Òò˹̹Äý¾Û(BEC)ºÍ³¬Á÷¶¯ÐÔÊÇÒѾ±»Ñо¿ºÜ¶àµÄ¡°²£É«×Óϵ×Û¡±ÔÚµÍÎÂÏ¿ÉÒÔ±íÏÖ³öÀ´µÄÒì³£ºê¹ÛÁ¿×ÓÁ¦Ñ§×´Ì¬µÄÀý×Ó¡£ÎÒÃÇËù²»Ì«ÊìϤµÄÊÇ¡°²£Á§¡±Ì¬£¬ÕâÖÖ״̬¾ÝÔ¤²âÔÚÎÞÐò´æÔÚʱ»á¶ÔÏ໥×÷ÓõIJ£É«×Ó³öÏÖ£¬µ«Æù½ñΪֹÔÚʵÑéÖÐȴûÓй۲⵽¡£ÏÖÔÚ£¬Rong YuµÈÈË·¢ÏÖ£¬Ò»ÖÖ²ôÔÓµÄÁ¿×Ó´ÅÌåÖеĴż¤·¢·Ç³£ÊʺÏʵÏÖºÍÑо¿ÕâÖÖÐÐΪ¡££¨Link to Article p. 379£© doi: 10.1038/nature11406 Bose glass and Mott glass of quasiparticles in a doped quantum magnet Rong Yu1 Liang Yin2 Neil S. Sullivan2 J. S. Xia2 Chao Huan2 Armando Paduan-Filho3 Nei F. Oliveira Jr3 Stephan Haas4 Alexander Steppke5 Corneliu F. Miclea6, 7 Franziska Weickert6 Roman Movshovich6 Eun-Deok Mun6 Brian L. Scott6 Vivien S. Zapf6 Tommaso Roscilde8 Affiliations Contributions Corresponding author Journal name: Nature Volume: 489, Pages: 379¨C384 Date published: (20 September 2012) DOI: doi:10.1038/nature11406 Received 14 May 2012 Accepted 11 July 2012 Published online 19 September 2012 The low-temperature states of bosonic fluids exhibit fundamental quantum effects at the macroscopic scale: the best-known examples are Bose¨CEinstein condensation and superfluidity, which have been tested experimentally in a variety of different systems. When bosons interact, disorder can destroy condensation, leading to a ¡®Bose glass¡¯. This phase has been very elusive in experiments owing to the absence of any broken symmetry and to the simultaneous absence of a finite energy gap in the spectrum. Here we report the observation of a Bose glass of field-induced magnetic quasiparticles in a doped quantum magnet (bromine-doped dichloro-tetrakis-thiourea-nickel, DTN). The physics of DTN in a magnetic field is equivalent to that of a lattice gas of bosons in the grand canonical ensemble; bromine doping introduces disorder into the hopping and interaction strength of the bosons, leading to their localization into a Bose glass down to zero field, where it becomes an incompressible Mott glass. The transition from the Bose glass (corresponding to a gapless spin liquid) to the Bose¨CEinstein condensate (corresponding to a magnetically ordered phase) is marked by a universal exponent that governs the scaling of the critical temperature with the applied field, in excellent agreement with theoretical predictions. Our study represents a quantitative experimental account of the universal features of disordered bosons in the grand canonical ensemble. http://www.nature.com/nature/jou ... pdf/nature11406.pdf [ Last edited by yexuqing on 2012-9-21 at 13:06 ] |
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