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85086288229
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x transform odd under C and P
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x transform odd under C and P.
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18
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2842557918
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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
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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.
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20
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in press
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Phys. Rev. B
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2842521161
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note
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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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22
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85086288134
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note
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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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23
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24444455824
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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).
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