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12
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85037178517
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L.Ts. Adzhemyan, A.N. Vasiljev, and A.V. Serdukov, in Proceedings of the RG96-Conference, Dubna, August 1996 (World Scientific, Singapore, in press)
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L.Ts. Adzhemyan, A.N. Vasiljev, and A.V. Serdukov, in Proceedings of the RG96-Conference, Dubna, August 1996 (World Scientific, Singapore, in press).
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19
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85037254348
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If in the background the correlation length reaches its constant value [Formula Presented] the matching condition leads to a flow parameter depending only on frequency. A simple approximation for not too large frequencies would be [Formula Presented], [Formula Presented]
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If in the background the correlation length reaches its constant value ξb the matching condition leads to a flow parameter depending only on frequency. A simple approximation for not too large frequencies would be (formula presented).
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23
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0001258298
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the second reference a fit with [Formula Presented] and correction terms is performed. PRBMDO
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C. Pittman, T. Dorion, and H. Meyer, Phys. Rev. B 20, 3678 (1979). In the second reference a fit with γ=1.24 and correction terms is performed
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(1979)
Phys. Rev. B
, vol.20
, pp. 3678
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Pittman, C.1
Dorion, T.2
Meyer, H.3
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25
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85037248153
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Note that we use the effective exponent [Formula Presented] instead of [Formula Presented] as in c20, which leads to a different value of [Formula Presented]
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Note that we use the effective exponent γ=1.19 instead of γ=1.16 as in 20, which leads to a different value of ΓT.
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39
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0023344781
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C.C. Agosta, S. Wang, L.H. Cohen, and H. Meyer, J. Low Temp. Phys. 67, 237 (1987)
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(1987)
J. Low Temp. Phys.
, vol.67
, pp. 237
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Agosta, C.C.1
Wang, S.2
Cohen, L.H.3
Meyer, H.4
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44
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85037235972
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(private communication)
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H. Meyer (private communication).
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Meyer, H.1
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47
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85037237105
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c31 [see Fig. 1(c) there] the attenuation has been normalized at each frequency separately. Therefore the agreement at higher frequencies in Fig. 99 is “less perfect” than in the earlier presentation
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In 31 [see Fig. 1(c) there] the attenuation has been normalized at each frequency separately. Therefore the agreement at higher frequencies in Fig. 99 is “less perfect” than in the earlier presentation.
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50
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85037214512
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fact one should replot the sound data with the correct nonasymptotic frequency scale. We do not expect substantial changes compared with those presented in Fig. 1515
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In fact one should replot the sound data with the correct nonasymptotic frequency scale. We do not expect substantial changes compared with those presented in Fig. 1515.
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