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In PrAg2In, previous μ-SR studies in ref. 31 have yielded an estimate of 1/141T1, 2:2 ×- 10 6 s-1 at T, 0.7 K. The enhanced 1/ 141T1 as a nonmagnetic GS system seems to correspond to the anomalously enhanced 1/T1 of both 109Ag and 115In in our recent NMR studies in ref. 18, which have been discussed in terms of the multipole, particularly octupole, fluctuations of the GS Γ3. Since a similarly short 141T1 can be expected for PrMg3, CP(T) measured by the thermal relaxation method is considered to appropriately include the nuclear Schottky contribution CN(T, Due to its poor natural abundance (10.13, and small gyromagnetic ratio (2.6054 MHz/T, the contribution from 25Mg to CN(T) can safely be neglect
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N(T) can safely be neglected.
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31
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17044427298
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33
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33847345499
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It has been known from ref. 28 that the resonant-level model (with ΔEΓ3, 0 K) yields a slightly higher C 4f (T) peak by ∼0.07 J/(mol K) than the 1-ch. Kondo model (J, 1/2, Within the resonant-level model, ΔEΓ 3, 1.0 K enhances the peak by ∼0:12 J/(mol K, which is comparable to the observed value ∼0:09 J/mol K
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3 = 1.0 K enhances the peak by ∼0:12 J/(mol K), which is comparable to the observed value ∼0:09 J/(mol K).
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