Inhomogeneous spin excitations in weakly coupled spin-1/2 chains

被引:3
|
作者
Shen, L. [1 ]
Campillo, E. [1 ]
Zaharko, O. [2 ]
Steffens, P. [3 ]
Boehm, M. [3 ]
Beauvois, K. [3 ]
Ouladdiaf, B. [3 ]
He, Z. [4 ]
Prabhakaran, D. [5 ]
Boothroyd, A. T. [5 ]
Blackburn, E. [1 ]
机构
[1] Lund Univ, Div Synchrotron Radiat Res, SE-22100 Lund, Sweden
[2] Paul Scherrer Inst, Lab Neutron Scattering & Imaging, CH-5232 Villigen, Switzerland
[3] Inst Laue Langevin, 71 Ave Martyrs, F-38042 Grenoble 9, France
[4] Chinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Matter, Fuzhou 350002, Fujian, Peoples R China
[5] Univ Oxford, Dept Phys, Clarendon Lab, Oxford OX1 3PU, England
来源
PHYSICAL REVIEW RESEARCH | 2022年 / 4卷 / 01期
基金
瑞典研究理事会; 英国工程与自然科学研究理事会;
关键词
BOSE-EINSTEIN CONDENSATION; QUANTUM; CRITICALITY; EXPONENTS; DYNAMICS; BENEATH; PHASE;
D O I
10.1103/PhysRevResearch.4.013111
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We present a systematic inelastic neutron scattering and neutron diffraction study on the magnetic structure of the quasi-one-dimensional spin-1/2 magnet SrCo2V2O8, where the interchain coupling in the Neel-type antiferromagnetic ground state breaks the static spin lattice into two independent domains. At zero magnetic field, we have observed two new spin excitations with small spectral weights inside the gapped region defined by the spinon bound states. In an external magnetic field along the chain axis, the Neel order gets partially destabilized at mu H-0*=2.0T and completely suppressed at mu(0)Hp=3.9T, above which a quantum disordered Tomonaga-Luttinger liquid (TLL) prevails. The low-energy spin excitations between mu H-0* and mu H-0(p) are not homogeneous, containing the dispersionless (or weakly dispersive) spinon bound states excited in the Neel phase and the highly dispersive psinon-antipsinon mode characteristic of a TLL. We propose that the two new modes at zero field are spinon excitations inside the domain walls. Since they have a smaller gap than those excited in the Neel domains, the underlying spin chains enter the TLL state via a local quantum phase transition at mu H-0*, making the Neel/TLL coexistence a stable configuration until the excitation gap in the Neel domains closes at mu H-0(p).
引用
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页数:10
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