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19
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85033737550
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The incommensurate state which we use here includes a discommensurate state with magnetic solitons as well as an incommensurate state with a sinusoidal modulation
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The incommensurate state which we use here includes a discommensurate state with magnetic solitons as well as an incommensurate state with a sinusoidal modulation.
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24
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85033750654
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j
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submitted to
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M. Poirier, R. Beaudry, M. Castonguay, M. L. Plumer, G. Quirion, F. S. Razavi, A. Revcolevschi and G. Dhalenne; submitted to Phys. Rev. B.
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Preliminary results
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39
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85033750632
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note
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2; ref. 3] are almost the same.
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41
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0000635909
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G. A. Petrakovskii, K. A. Sablina, A. M. Vorotynov, A. I. Kruglik, A. G. Klimenko, A. D. Balayev and S. S. Aplesnin: Zh. Eksp. Teor. Fiz. 98 (1990) 1382. translation: Sov. Phys.-JETP 71 (1990) 772.
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Yamadaya, T.8
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47
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85033756292
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note
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3, since the main component of M(H, T, x) at 4.2 K is the orbital part, n(H ∼ 0, T, x) does not reflect density of S = 1/2 spins. Nonetheless the estimation of the density of the solitons is not affected by n(H ∼ 0, T, x), because n(H ∼ 0, T, x) is negligible.
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48
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85033755862
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In ref. 12, JaQ was obtained only at the phase boundary. We assume that JaQ is independent of T, because M(II, T, x) in high H mainly due to the solitons is almost independent of T
-
In ref. 12, JaQ was obtained only at the phase boundary. We assume that JaQ is independent of T, because M(II, T, x) in high H mainly due to the solitons is almost independent of T.
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49
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0011245132
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Y. Ajiro, T. Asano, F. Masui, M. Mekata, H. Aruga-Katori, T. Goto and H. Kikuchi: Phys. Rev. B 51 (1995) 9399.
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Goto, T.6
Kikuchi, H.7
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51
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85033745099
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private communication
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B. Keimer: private communication.
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Keimer, B.1
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