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J.O. Indekeu and J.M.J. van Leeuwen, Phys. Rev. Lett 75 (1995) 1618; Physica C 251 (1995) 290; Further, see R. Blossey and J.O. Indekeu, Phys. Rev. B 53 (1996) 8599.
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Indekeu, J.O.1
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4243644524
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J.O. Indekeu and J.M.J. van Leeuwen, Phys. Rev. Lett 75 (1995) 1618; Physica C 251 (1995) 290; Further, see R. Blossey and J.O. Indekeu, Phys. Rev. B 53 (1996) 8599.
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Physica C
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J.O. Indekeu and J.M.J. van Leeuwen, Phys. Rev. Lett 75 (1995) 1618; Physica C 251 (1995) 290; Further, see R. Blossey and J.O. Indekeu, Phys. Rev. B 53 (1996) 8599.
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Phys. Rev. B
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Blossey, R.1
Indekeu, J.O.2
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Meunier, J.2
Broseta, D.3
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Bonn, D.5
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8
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0011386917
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For ordinary fluids, see, e.g., H. Kellay, D. Bonn and J. Meunier, Phys. Rev. Lett. 71 (1993) 2607; 73 (1994) 3560; For quantum fluids, see, e.g., K.S. Ketola, S. Wang and R.B. Hallock, Phys. Rev. Lett. 68 (1992) 201; J.E. Rutledge and P. Taborek, Phys. Rev. Lett. 69 (1992) 937.
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Kellay, H.1
Bonn, D.2
Meunier, J.3
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9
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0001348147
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For ordinary fluids, see, e.g., H. Kellay, D. Bonn and J. Meunier, Phys. Rev. Lett. 71 (1993) 2607; 73 (1994) 3560; For quantum fluids, see, e.g., K.S. Ketola, S. Wang and R.B. Hallock, Phys. Rev. Lett. 68 (1992) 201; J.E. Rutledge and P. Taborek, Phys. Rev. Lett. 69 (1992) 937.
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Phys. Rev. Lett.
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, pp. 3560
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10
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0000641368
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For ordinary fluids, see, e.g., H. Kellay, D. Bonn and J. Meunier, Phys. Rev. Lett. 71 (1993) 2607; 73 (1994) 3560; For quantum fluids, see, e.g., K.S. Ketola, S. Wang and R.B. Hallock, Phys. Rev. Lett. 68 (1992) 201; J.E. Rutledge and P. Taborek, Phys. Rev. Lett. 69 (1992) 937.
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Phys. Rev. Lett.
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, pp. 201
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Ketola, K.S.1
Wang, S.2
Hallock, R.B.3
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11
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0000484845
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For ordinary fluids, see, e.g., H. Kellay, D. Bonn and J. Meunier, Phys. Rev. Lett. 71 (1993) 2607; 73 (1994) 3560; For quantum fluids, see, e.g., K.S. Ketola, S. Wang and R.B. Hallock, Phys. Rev. Lett. 68 (1992) 201; J.E. Rutledge and P. Taborek, Phys. Rev. Lett. 69 (1992) 937.
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Phys. Rev. Lett.
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Rutledge, J.E.1
Taborek, P.2
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16
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0043263598
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note
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1, ≈ (1 - coth C). In the region relevant to our phase boundary analysis the breakdown only occurs for κ ≫ 1. Thus we find κ* (τ = -0.6) ≈ 7.16, κ*(τ = -0.4) ≈ 3.31 and κ* (τ = -0.2) ≈ 1.15. However as |T| → 0 the coth-like solutions are not valid across the wide range 0 < κ < I but rather a much reduced range, for example κ* (τ = - 0.1) = 0.48 and κ* (τ = - 0.05) ≈ 0.22.
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