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77956922672
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edited by F. Seitz and D. Turnbull (Academic, New York)
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Solid State Physics
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Kohn, W.1
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2
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0019056783
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T. F. Rosenbaum, K. Andres, and G. A. Thomas, Solid State Commun. 35, 663 (1980); T. F. Rosenbaum et al., Phys. Rev. B 27, 7509 (1983).
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Rosenbaum, T.F.1
Andres, K.2
Thomas, G.A.3
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3
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0001547961
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T. F. Rosenbaum, K. Andres, and G. A. Thomas, Solid State Commun. 35, 663 (1980); T. F. Rosenbaum et al., Phys. Rev. B 27, 7509 (1983).
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Phys. Rev. B
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Rosenbaum, T.F.1
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7
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33646619331
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J. D. Quirt and J. R. Marko, Phys. Rev. Lett. 26, 318 (1971); Phys. Rev. B 7, 3842 (1973).
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Phys. Rev. B
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11
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0018020795
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S. Kobayashi, Y. Fukagawa, S. Kiehata, and W. Sasaki, J. Phys. Soc. Jpn. 45, 1276 (1978).
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Kobayashi, S.1
Fukagawa, Y.2
Kiehata, S.3
Sasaki, W.4
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13
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0000420798
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France
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H. Alloul and P. Dellouve, Phys. Rev. Lett. 59, 578 (1987); J. Phys. (France) 49, 1185 (1988).
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4243640611
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M. J. Hirsch, D. F. Holcomb, R. N. Bhatt, and M. A. Paalanen, Phys. Rev. Lett. 68, 1418 (1992).
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Hirsch, M.J.1
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18
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0000832297
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S. E. Fuller, E. M. Meintjes, and W. W. Warren, Jr., Phys. Rev. Lett. 76, 2806 (1996).
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Fuller, S.E.1
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Warren Jr., W.W.3
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20
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15444372128
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note
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The Hall effect measurements form the basis of a Senior Thesis in Physics at Oregon State University by Jeremy Danielson.
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21
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15444364060
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note
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1/2. The fit was found to be inferior to the power law fits. We emphasize, nevertheless, that the power law fits are merely empirical representations of the observed temperature dependence. We have proposed no physical mechanism for this behavior.
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24
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15444375578
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note
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31P NMR results does not include the possible influence of exchange effects on the susceptibilities responsible for the shifts and relaxation. We cannot exclude a role for such effects. However, as we show below, the observations can be explained in the context of a model based on noninteracting electrons.
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25
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0000079740
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Amsterdam
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J. Korringa, Physica (Amsterdam) 16, 601 (1950).
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(1950)
Physica
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Korringa, J.1
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28
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0000264024
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R. C. Fletcher, W. A. Yager, G. L. Pearson, and F. R. Merritt, Phys. Rev. 95, 844 (1954).
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Phys. Rev.
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Fletcher, R.C.1
Yager, W.A.2
Pearson, G.L.3
Merritt, F.R.4
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30
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5244381613
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private communication
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2/V s, respectively, for A=1. In the context of the simple models being used for this analysis, we do not consider these differences to be significant.
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Holcomb, D.F.1
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33
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15444367083
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note
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Electron spin resonance characterization of our samples was carried out by A. Hofstaetter in the laboratory of B. K. Meyer at the Universität Gießen, Germany.
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34
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15444377285
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private communication
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D. F. Holcomb (private communication).
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Holcomb, D.F.1
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