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2·mol) is assumed after J. M. Lawrence, P. S. Riseborough, C. H. Booth, J. L. Sarrao, J. D. Thompson, and R. Osborn: Phys. Rev. B 63 (2001) 054427.
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e/T above 10K down to T = 0.
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34
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private communication
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H. S. Jeevan: private communication.
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33847391503
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γ0 of YPd3 is used here, C. L. Seaman and M. B. Maple: Physica B 199-200 (1994) 396; LaPd3 has anomalously small γ0 of 0.28 mJ/(K2·mol),35) and does not serve as reference to CePd3. This is supported by the large difference of the lattice constant between CePd3 and LaPd 3 (Δa, 0.11 Å) compared with that between CePd3 and YPd3 Δa, 0.05Å
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3 (Δa = 0.05Å).
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N. Takeda and M. Ishikawa: J. Phys. Soc. Jpn. 69 (2000) 868; This work reports a large Ce/T of 190- 380 mJ/(mol 2·K) below 2K due to NFL formation. We have estimated a Kondo contribution of 50-85 mJ/(mol2·K) by extrapolating the C/T vs T2 plot above 4K down to 0 K
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2 plot above 4K down to 0 K.
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G. Czycholl and H. J. Leder: Z. Phys. B 44 (1981) 59; When a k-independent Ṽ is assumed, as in many PAM-based theories on HF compounds, only the c component of the total dos can contribute to σ(ω).
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