Unveiling the phase diagram of a bond-alternating spin-1/2 K-Γ chain

被引:27
作者
Luo, Qiang [1 ]
Zhao, Jize [2 ,3 ,4 ]
Wang, Xiaoqun [5 ,6 ]
Kee, Hae-Young [1 ,7 ]
机构
[1] Univ Toronto, Dept Phys, Toronto, ON M5S 1A7, Canada
[2] Lanzhou Univ, Sch Phys Sci & Technol, Lanzhou 730000, Peoples R China
[3] Lanzhou Univ, Key Lab Magnetism & Magnet Mat MoE, Lanzhou 730000, Peoples R China
[4] Lanzhou Univ, Lanzhou Ctr Theoret Phys, Lanzhou 730000, Peoples R China
[5] Shanghai Jiao Tong Univ, Sch Phys & Astron, Tsung Dao Lee Inst, Key Lab Artificial Struct & Quantum Control,Minis, Shanghai 200240, Peoples R China
[6] Beijing Computat Sci Res Ctr, Beijing 100084, Peoples R China
[7] Canadian Inst Adv Res, Toronto, ON M5G 1Z8, Canada
基金
加拿大自然科学与工程研究理事会; 加拿大创新基金会; 中国国家自然科学基金;
关键词
QUANTUM; GAP; TRANSITIONS;
D O I
10.1103/PhysRevB.103.144423
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The key to unraveling intriguing phenomena observed in various Kitaev materials lies in understanding the interplay of Kitaev (K) interaction and a symmetric off-diagonal Gamma interaction. To provide insight into the challenging problems, we study the quantum phase diagram of a bond-alternating spin-1/2 g(x)-g(y) K-Gamma chain by density-matrix renormalization-group method where g(x) and g(y) are the bond strengths of the odd and even bonds, respectively. The phase diagram is dominated by even-Haldane (g(x) > g(y)) and odd-Haldane (g(x) < g(y)) phases where the former is topologically trivial while the latter is a symmetry-protected topological phase. Near the antiferromagnetic Kitaev limit, there are two gapped A(x) and A(y) phases characterized by distinct nonlocal string correlators. In contrast, the isotropic ferromagnetic (FM) Kitaev point serves as a multicritical point where two topological phase transitions meet. The remaining part of the phase diagram contains three symmetry-breaking magnetic phases. One is a sixfold degenerate FMU6 phase where all the spins are parallel to one of the +/-<(x)over cap>, +/-(y) over cap, and +/-(z) over cap axes in a six-site spin-rotated basis, while the other two have more complex spin structures with all the three spin components being finite. Existence of a rank-two spin-nematic ordering in the latter is also discussed.
引用
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页数:12
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共 68 条
[1]   UNIVERSAL TERM IN THE FREE-ENERGY AT A CRITICAL-POINT AND THE CONFORMAL ANOMALY [J].
AFFLECK, I .
PHYSICAL REVIEW LETTERS, 1986, 56 (07) :746-748
[2]   RESONATING VALENCE BONDS - NEW KIND OF INSULATOR [J].
ANDERSON, PW .
MATERIALS RESEARCH BULLETIN, 1973, 8 (02) :153-160
[3]   S=1/2 alternating chain using multiprecision methods [J].
Barnes, T ;
Riera, J ;
Tennant, DA .
PHYSICAL REVIEW B, 1999, 59 (17) :11384-11397
[4]   CONFORMAL-INVARIANCE, THE CENTRAL CHARGE, AND UNIVERSAL FINITE-SIZE AMPLITUDES AT CRITICALITY [J].
BLOTE, HWJ ;
CARDY, JL ;
NIGHTINGALE, MP .
PHYSICAL REVIEW LETTERS, 1986, 56 (07) :742-745
[5]   String correlation functions of the spin-1/2 Heisenberg XXZ chain [J].
Bortz, Michael ;
Sato, Jun ;
Shiroishi, Masahiro .
JOURNAL OF PHYSICS A-MATHEMATICAL AND THEORETICAL, 2007, 40 (16) :4253-4271
[6]   Quantum phase transition in the one-dimensional compass model [J].
Brzezicki, Wojciech ;
Dziarmaga, Jacek ;
Oles, Andrzej M. .
PHYSICAL REVIEW B, 2007, 75 (13)
[7]   Nonlocal string order parameter in the S=1/2 Kitaev-Heisenberg ladder [J].
Catuneanu, Andrei ;
Sorensen, Erik S. ;
Kee, Hae-Young .
PHYSICAL REVIEW B, 2019, 99 (19)
[8]   Path to stable quantum spin liquids in spin-orbit coupled correlated materials [J].
Catuneanu, Andrei ;
Yamaji, Youhei ;
Wachtel, Gideon ;
Kim, Yong Baek ;
Kee, Hae-Young .
NPJ QUANTUM MATERIALS, 2018, 3
[9]   Zigzag Magnetic Order in the Iridium Oxide Na2IrO3 [J].
Chaloupka, Jiri ;
Jackeli, George ;
Khaliullin, Giniyat .
PHYSICAL REVIEW LETTERS, 2013, 110 (09)
[10]   Entanglement entropy scaling of the XXZ chain [J].
Chen, Pochung ;
Xue, Zhi-long ;
McCulloch, I. P. ;
Chung, Ming-Chiang ;
Cazalilla, Miguel ;
Yip, S-K .
JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT, 2013,