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Volumn 74, Issue 4, 2005, Pages 1214-1223

Quantum spin pump in S = 1/2 antiferromagnetic chains -holonomy of phase operators in sine-gordon theory-

Author keywords

Dirac monopole; Field induced spin gap systems; Landau Zener tunneling; Phase operator; Quantized spin transport; Sine Gordon theory; Topological stability

Indexed keywords


EID: 21744448915     PISSN: 00319015     EISSN: None     Source Type: Journal    
DOI: 10.1143/JPSJ.74.1214     Document Type: Article
Times cited : (58)

References (70)
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    • note
    • a] becomes a non-generic matrix in general.
  • 34
    • 4243468159 scopus 로고    scopus 로고
    • I. Affleck and M. Oshikawa: Phys. Rev. B 60 (1999) 1038. In these papers, not only the staggered component of g-tensor but also the alternating DM vector are found to be relevant to induce a finite spin gap.
    • (1999) Phys. Rev. B , vol.60 , pp. 1038
    • Affleck, I.1    Oshikawa, M.2
  • 36
    • 24644467581 scopus 로고    scopus 로고
    • note
    • If the system is invariant under the π-rotational symmetry which exchanges the nearest neighboring bonds, the direction of E must be deviated from this π-rotational axis.
  • 37
    • 24644477981 scopus 로고    scopus 로고
    • note
    • Here we also rotate by π around the z-direction in the spin space on odd sites: (equation presented) We take this sign convention only in §2.
  • 43
    • 0000609380 scopus 로고
    • For example, R. Shankar: Acta Phys. Pol. B 26 (1995) 1835. From this paper, we change its notations as follows; (equation presented)
    • (1995) Acta Phys. Pol. B , vol.26 , pp. 1835
    • Shankar, R.1
  • 45
    • 24644515733 scopus 로고    scopus 로고
    • note
    • z ≠ 0.
  • 48
    • 24644464965 scopus 로고    scopus 로고
    • note
    • 2.
  • 49
    • 24644432348 scopus 로고    scopus 로고
    • note
    • Here the wavefunction does not have the projected weight on the third excited state with n = 3 [thin line in Fig. 5(a)] during the cycle.
  • 50
    • 24644446804 scopus 로고    scopus 로고
    • note
    • + is quantized to be 1.
  • 67
    • 24644482540 scopus 로고    scopus 로고
    • note
    • In spin-gapped systems, the effects of the boundary range only within its magnetic correlation length from both ends.
  • 68
    • 24644523501 scopus 로고    scopus 로고
    • note
    • In the final line of eq. (A·7), we drop those terms which can be summarized into a form of the total derivative.
  • 70
    • 80052648759 scopus 로고    scopus 로고
    • +(0) denotes the phase operator at the midpoint of two contacts. This backscattering potential turns out to be relevant in the presence of repulsive electron-electron interactions and tunneling probability of spins between two contacts becomes vanishing. As a consequence of this vanishing tunneling probability of spins (TPS), number of spins transported between these two contacts is also quantized in their work. Even though our work treats a pumping in macro-scale systems and is different from their work which is about meso (nano)-scale systems, there is an interesting correspondence between these two works. Namely, in both stories, quantizations of spin transports result from the vanishing TPS between two "contacts". Two contacts in their configurations correspond to the two sample boundaries in this paper and TPS between these two "contacts", namely tunneling probability between the state of eq. (26) and that of eq. (27) decreases exponetially in thermodynamic limit, which is also a necessity of the quantized spin transfers in this paper (see §3).
    • (2003) Phys. Rev. B , vol.68 , pp. 035321
    • Sharma, P.1    Chamon, C.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.