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84890723225
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As a caveat we however note that in Fig. , the central region still shows some small magnetization gradient, and is thus not completely stationary.
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As a caveat we however note that in Fig., the central region still shows some small magnetization gradient, and is thus not completely stationary.
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59
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84890668798
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Since Siz=ci†ci-12
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Since S i z = c i † c i - 1 2, Eqs. and differ by an irrelevant global phase factor exp (i θ Σ r = - L / 2 L / 2 - 1 r / 2) = exp (- i L θ2)
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60
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84872952532
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PRBMDO 1098-0121 10.1103/PhysRevB.87.045112
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I. V. Protopopov, D. B. Gutman, P. Schmitteckert, and A. D. Mirlin, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.87.045112 87, 045112 (2013);
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(2013)
Phys. Rev. B
, vol.87
, pp. 045112
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Protopopov, I.V.1
Gutman, D.B.2
Schmitteckert, P.3
Mirlin, A.D.4
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84879137129
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PRLTAO 0031-9007 10.1103/PhysRevLett.110.257203
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J.-S. Caux and F. H. L. Essler, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.110.257203 110, 257203 (2013).
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(2013)
Phys. Rev. Lett.
, vol.110
, pp. 257203
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Caux, J.-S.1
Essler, F.H.L.2
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84890695494
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For simplicity we assume here that the anomalous terms
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For simplicity we assume here that the anomalous terms 〈 c p † c - p † ⌠vanish.
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84890742732
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Replacing q(u) by zero in Fp(q(u)) would describe the correlations in a different regime, namely that of times tâ‰L when the fronts have bounced a large number of times at the boundaries of the chain (see Sec. ).
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Replacing q (u) by zero in F p (q (u)) would describe the correlations in a different regime, namely that of times t ≠L when the fronts have bounced a large number of times at the boundaries of the chain (see Sec.)
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