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Physical Review B - Condensed Matter and Materials Physics

Volumn 78, Issue 2, 2008, Pages

Intrinsic properties of stoichiometric LaFePO

(9) McQueen, T M a Regulacio, M a Williams, A J a Huang, Q b Lynn, J W b Hor, Y S a West, D V a Green, M A b,c Cava, R J a

a PRINCETON UNIVERSITY (United States)

b NATIONAL INSTITUTE OF STANDARDS AND TECHNOLOGY (United States)

c UNIVERSITY OF MARYLAND (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 48749108743 PISSN: 10980121 EISSN: 1550235X Source Type: Journal
DOI: 10.1103/PhysRevB.78.024521 Document Type: Article

Times cited : (109)

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- g (εF) calc =6 states eVcell so γcalc =g (εF) calc /424.25=14.1 mJ mol K2.

43
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44
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- χmeas = χpauli + χlandau ≈ χpauli - 1 3 χpauli = 2 3 χpauli, where the relation χlandau =- 1 3 χpauli, assuming a free-electron gas, has been used.

45
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- For spin fluctuations, β= β3 -Aln Tsf and thus a plot of β versus A will be linear with intercept β3 and slope -ln Tsf.

46
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- For spin fluctuations, A= α γ0 T sf 2, where γ0 does not include any mass enhancement from the spin fluctuations and α= 6 π2 5 (S-1) 2 S. For a system with negligible mass enhancement, γ0 = γmeas.
- For spin fluctuations, A= α γ0 T sf 2, where γ0 does not include any mass enhancement from the spin fluctuations and α= 6 π2 5 (S-1) 2 S. For a system with negligible mass enhancement, γ0 = γmeas.

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