Bose-Einstein condensation of the triplet states in the magnetic insulator TlCuCl3
Bose-Einstein condensation of the triplet states in the magnetic insulator TlCuCl3
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DOI:
10.1038/nature01617
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发表时间:
2003-05-01
期刊:
影响因子:
64.8
通讯作者:
Wildes, A
中科院分区:
文献类型:
--
作者:
Rüegg, C;Cavadini, N;Wildes, A
Bose-Einstein condensation denotes the formation of a collective quantum ground state of identical particles with integer spin or intrinsic angular momentum. In magnetic insulators, the magnetic properties are due to the unpaired shell electrons that have half-integer spin. However, in some such compounds (KCuCl3 and TlCuCl3), two Cu2+ ions are antiferromagnetically coupled(1) to form a dimer in a crystalline network: the dimer ground state is a spin singlet (total spin zero), separated by an energy gap from the excited triplet state (total spin one). In these dimer compounds, Bose-Einstein condensation becomes theoretically possible(2). At a critical external magnetic field, the energy of one of the Zeeman split triplet components (a type of boson) intersects the ground-state singlet, resulting in long-range magnetic order; this transition represents a quantum critical point at which Bose-Einstein condensation occurs. Here we report an experimental investigation of the excitation spectrum in such a field-induced magnetically ordered state, using inelastic neutron scattering measurements of TlCuCl3 single crystals. We verify unambiguously the theoretically predicted(3) gapless Goldstone mode characteristic of the Bose-Einstein condensation of the triplet states.