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M. E. Zhitomirsky and I. A. Luk'yanchuk: -JETP Lett. 58 (1993) 131; M. E. Zhitomirsky and K. Ueda: Phys. Rev. B 53 (1996) 6591: A. Garg and D. -C. Chen: Phys. Rev. B 49 (1994) 479.
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M. E. Zhitomirsky and I. A. Luk'yanchuk: -JETP Lett. 58 (1993) 131; M. E. Zhitomirsky and K. Ueda: Phys. Rev. B 53 (1996) 6591: A. Garg and D. -C. Chen: Phys. Rev. B 49 (1994) 479.
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19
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85033745530
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private communication
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Y. Kitaoka et al.: private communication.
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Kitaoka, Y.1
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20
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85033770193
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-
note
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2) the weak coupling calculation using the band structure data still gives a nonvanishing result of ∼10% of the main term, which is large enough to remove the desired tetra-critical point. Note that in the spin degenerate scenario, this dangerous term identically vanishes.
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21
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0343958526
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Norman has already investigated the relative stability of various pairing states within the same framework and failed to stabilize the following desired state. We use the newly found ferromagnetic fluctuation mode and we do not assume the strong SO coupling, thus the resulting pairing state is quite different. See M. R. Norman: Phys. Rev. B 37 (1988) 4987; ibid. 41 (1990) 170.
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Phys. Rev. B
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Norman, M.R.1
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22
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25944454916
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Norman has already investigated the relative stability of various pairing states within the same framework and failed to stabilize the following desired state. We use the newly found ferromagnetic fluctuation mode and we do not assume the strong SO coupling, thus the resulting pairing state is quite different. See M. R. Norman: Phys. Rev. B 37 (1988) 4987; ibid. 41 (1990) 170.
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(1990)
Phys. Rev. B
, vol.41
, pp. 170
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23
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0000080776
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For an early attempt, see P. W. Anderson: Phys. Rev. B 30 (1984) 1549.
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Phys. Rev. B
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Anderson, P.W.1
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G. Aeppli et al.: Phys. Rev. Lett. 60 (1988) 615; J. Magn. Magn. Mater. 76-77 (1988) 385.
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Aeppli, G.1
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G. Aeppli et al.: Phys. Rev. Lett. 60 (1988) 615; J. Magn. Magn. Mater. 76-77 (1988) 385.
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G. R. Stewart et al.: Phys. Rev. Lett. 52 (1984) 679; G. E. Brodale et al.: Phys. Rev. Lett. 57 (1986) 234.
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Brodale, G.E.1
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31
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85033755933
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report no static AF in the recent μSR experiment contrary to the old one
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P. Dalmas de Réotier et al.: Phys. Lett. 205 (1995) 101, report no static AF in the recent μSR experiment contrary to the old one; R. H. Heffner et al.: Phys. Rev. B 39 (1989) 11345.
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Dalmas de Réotier, P.1
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32
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0001420341
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P. Dalmas de Réotier et al.: Phys. Lett. 205 (1995) 101, report no static AF in the recent μSR experiment contrary to the old one; R. H. Heffner et al.: Phys. Rev. B 39 (1989) 11345.
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Phys. Rev. B
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Heffner, R.H.1
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0027905244
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and preprint. This implies that the field may help to stabilize the static AF by some unknown reason
-
Except for the clastic measurement under H by G. Bruls et al.: Physica B 186-188 (1993) 258 and preprint. This implies that the field may help to stabilize the static AF by some unknown reason.
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(1993)
Physica B
, vol.186-188
, pp. 258
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Bruls, G.1
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34
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85033751935
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note
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2 with a similar tiny spontaneous moment ∼0.02 μB/U should be noted; yet various measurements clearly detect the AF.
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-
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35
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85033764689
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We thank G. Aeppli for pointing this out
-
We thank G. Aeppli for pointing this out.
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36
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85033761500
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note
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K) term in the specific heat, as mentioned before.
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38
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85033752168
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-
note
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K whose energy range is not covered by the above calculations.
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39
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85033738885
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14 failed to stabilize the triplet state over the singlet state using this mode
-
14) failed to stabilize the triplet state over the singlet state using this mode.
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46
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21844500766
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For a microscopic calculation for stabilizing a nonunitary state, see T. Sugiyama and T. Ohmi: J. Phys. Soc. Jpn. 64 (1995) 2746.
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, vol.64
, pp. 2746
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Sugiyama, T.1
Ohmi, T.2
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