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85034541404
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note
-
c2 = 50 mK the physical quantities become exponentially small by opening the remaining down-spin gap. It is also true that above T ∼ 50 mK the specific heat behaves as if half the density of states at the Fermi level remains ungapped. These T-dependences are not seen experimentally. Thus we do not consider it any further.
-
-
-
-
29
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85034543921
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note
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y which has no line node on the equator in general both for the bipolar or planar states. Thus it is not appropriate for the present case.
-
-
-
-
30
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85034530678
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note
-
The gap topology of the planar state is the same as in Sauls state. We note, however, that the spin structure is completely different.
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31
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0022751991
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85034562105
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-
note
-
Inelastic scattering is anisotropic, thus b could depend on the direction. However we ignore it for simplicity. We thank A. Huxley for pointing out this fact.
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-
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42
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85034531549
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-
note
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3 < 0 is required.
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43
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21144480880
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K. Machida, T. Fujita and T. Ohmi: J. Phys. Soc. 62 (1993) 680; T. Fujita, W. Aoyama, K. Machida and T. Ohmi: J. Phys. Soc. 63 (1994) 247; Y. Hirano, T. Fujita, K. Machida and T. Ohmi: J. Phys. Soc. 64 (1995) 210.
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21344482337
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K. Machida, T. Fujita and T. Ohmi: J. Phys. Soc. 62 (1993) 680; T. Fujita, W. Aoyama, K. Machida and T. Ohmi: J. Phys. Soc. 63 (1994) 247; Y. Hirano, T. Fujita, K. Machida and T. Ohmi: J. Phys. Soc. 64 (1995) 210.
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Fujita, T.1
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21844491961
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K. Machida, T. Fujita and T. Ohmi: J. Phys. Soc. 62 (1993) 680; T. Fujita, W. Aoyama, K. Machida and T. Ohmi: J. Phys. Soc. 63 (1994) 247; Y. Hirano, T. Fujita, K. Machida and T. Ohmi: J. Phys. Soc. 64 (1995) 210.
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P. A. Midgley, S. M. Hayden, L. Taillefer, B. Bogenberger and H. v. Löhneysen: Phys. Rev. Lett. 70 (1993) 678; also see, K. Elboussiri: Appl. Phys. A 59 (1994) 223; B. Ellman, A. Zaluska and L. Taillefer: Physica B 205 (1995) 346; B. Ellman, M. Sutton, B. Lussier, R. Bruning, L. Taillefer, S. M. Hayden and G. Shea-McCarthy: preprint (cond-mat/9704125).
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Ellman, B.1
Zaluska, A.2
Taillefer, L.3
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0027541839
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preprint (cond-mat/9704125)
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P. A. Midgley, S. M. Hayden, L. Taillefer, B. Bogenberger and H. v. Löhneysen: Phys. Rev. Lett. 70 (1993) 678; also see, K. Elboussiri: Appl. Phys. A 59 (1994) 223; B. Ellman, A. Zaluska and L. Taillefer: Physica B 205 (1995) 346; B. Ellman, M. Sutton, B. Lussier, R. Bruning, L. Taillefer, S. M. Hayden and G. Shea-McCarthy: preprint (cond-mat/9704125).
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Ellman, B.1
Sutton, M.2
Lussier, B.3
Bruning, R.4
Taillefer, L.5
Hayden, S.M.6
Shea-McCarthy, G.7
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50
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85034552264
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private communication. They have done the Knight shift experiments on two samples. The nominally same b-axis experiments on them give rise to a different Knight shift result, indicating that the hexagonal symmetry of the basal plane is broken
-
H. Tou and Y. Kitaoka: private communication. They have done the Knight shift experiments on two samples. The nominally same b-axis experiments on them give rise to a different Knight shift result, indicating that the hexagonal symmetry of the basal plane is broken.
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Tou, H.1
Kitaoka, Y.2
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51
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85034558634
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cond-mat/9904349
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Keizer, R.J.1
De Visser, A.2
Menovsky, A.A.3
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Amato, A.5
Gygax, F.N.6
Pinkpank, M.7
Schenck, A.8
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cond-mat/9903333
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Preliminary experiment by A. Sawada (private communication), who measures the length changes under H, detects some anomalies
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Preliminary experiment by A. Sawada (private communication), who measures the length changes under H, detects some anomalies.
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