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Volumn 10, Issue 2, 1996, Pages 219-234

Chirality correlation of spin solitons: Bloch walls, spin-1/2 solitons and holes in a 2D antiferromagnetic background

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EID: 0000218454     PISSN: 02179792     EISSN: None     Source Type: Journal    
DOI: 10.1142/s021797929600009x     Document Type: Article
Times cited : (17)

References (31)
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    • x transform odd under C and P
    • x transform odd under C and P.
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    • Strictly speaking, periodic boundary conditions require either a Möbius-band topology or a pair of π-solitons. In the latter case, the solitons can be regarded as independent objects since we are interested in the dilute limit
    • Strictly speaking, periodic boundary conditions require either a Möbius-band topology or a pair of π-solitons. In the latter case, the solitons can be regarded as independent objects since we are interested in the dilute limit.
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    • H. B. Braun and D. Loss, J. Appl. Phys. 76, 6177 (1994); in Ref. 2; and Phys. Rev. B, in press.
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    • note
    • In (3) we have chosen A such that the Dirac-string runs through the south pole. An equivalent gauge choice would be As · dn. = -(1 + cos θ)dφ. Both, the nonzero value of the chirality and the correlation between adjacent band minima are gauge independent. However, the correlation between sgn k and sgn C is a gauge artifact.
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    • note
    • 3 term has now disappeared at the expense of a spin dependent potential of period 2α (which implies halving of the BZ).
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    • Since the soliton is a compact object, chiral symmetry is only broken in a, finite space region with vanishing weight in the thermodynamic limit. This symmetry breaking is thus not associated with a phase transition with broken symmetry every-where (Elitzur's theorem is thus of no relevance here). Note that this fact and our definition of chirality are fundamentally different from the "chiral phase" discussed by X.-G. Wen, F. Wilczek and A. Zee, Phys. Rev. B39, 1141 (1989).
    • (1989) Phys. Rev. , vol.B39 , pp. 1141
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.