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12
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17044427298
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4243487054
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T. M. Kelley, W. P. Beyermann, R. A. Robinson, H. Nakotte, P. C. Canfield and F. Trouw: Phys. Rev. B 61 (2000) 1831, and references therein.
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T. M. Kelley, W. P. Beyermann, R. A. Robinson, H. Nakotte, P. C. Canfield and F. Trouw: Phys. Rev. B 61 (2000) 1831, and references therein.
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15
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30344478240
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Goto, T.8
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16
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33847264500
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In this paper, we describe the compound as PrAg2In following the more general convention used in describing rare-earth- or actinide-based ternary compounds, and not as PrInAg2 as in most of the related literature on this compound
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2 as in most of the related literature on this compound.
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17
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33847281507
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1 (173 K).
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1 (173 K).
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18
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24644523713
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T. Kawae, C. Li, Y. Yoshida, K. Takeda, T. Asano and T. Kitai: J. Phys. Soc. Jpn. 74 (2005) 2332.
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Asano, T.5
Kitai, T.6
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20
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33847288361
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unpublished
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H. S. Suzuki et al.: unpublished.
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Suzuki, H.S.1
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22
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33847258369
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8 partial-wave states of the conduction electrons around the f -ions. With the Schrieffer-Wolff transformation, the model can be mapped onto the two-channel quadrupole Kondo model. This model is conventionally called the 3-7-8 model.
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8 partial-wave states of the conduction electrons around the f -ions. With the Schrieffer-Wolff transformation, the model can be mapped onto the two-channel quadrupole Kondo model. This model is conventionally called the "3-7-8" model.
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24
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0001541042
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D. Davidov, V. Zevin, R. Levin, D. Shaltiel and K. Baberschke: Phys. Rev. B 15 (1977) 2771.
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Davidov, D.1
Zevin, V.2
Levin, R.3
Shaltiel, D.4
Baberschke, K.5
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25
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33847308716
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zz(ω).
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zz(ω).
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27
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0019535042
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M. J. Besnus, J. P. Kappler, B. Lemius, M. Benakki and A. Meyer: J. Appl. Phys. 53 (1982) 2158.
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Besnus, M.J.1
Kappler, J.P.2
Lemius, B.3
Benakki, M.4
Meyer, A.5
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29
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33847257902
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3+ 4f moments with the conduction electrons.
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3+ 4f moments with the conduction electrons.
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31
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33847335606
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private communication
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H. Harima: private communication.
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Harima, H.1
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34
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33847262578
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z = ±1/2 states induced through the p (j = 3/2)-f hybridization between In 6p (j = 3/2) and Pr 4f states, which in turn produces the field gradient at the In nuclear site.
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z = ±1/2 states induced through the p (j = 3/2)-f hybridization between In 6p (j = 3/2) and Pr 4f states, which in turn produces the field gradient at the In nuclear site.
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