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Volumn 74, Issue 19, 1995, Pages 3896-3899

Finite temperature transitions in 2D dipolar systems with uniaxial anisotropy

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0000745199 PISSN: 00319007 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevLett.74.3896 Document Type: Article

Times cited : (44)

References (33)

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26
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- The RG equation derived in Ref. [c20] is for a negative Δ, corresponding to x- y anisotropy. This result is correct. The RG equation derived in Ref. [c21] is claimed to be for the Ising anisotropy (positive Δ) and has the same form as that of Ref. [c19]. We think this is not completely correct. There is no direct anharmonic correction from the anisotropy term in that case. In the correct result, a factor of n ln(b)T/2π should be replaced by (n-1)ln(b)T/2π.

27
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- The self-consistent mean field equations can be easily obtained from Mi=∂βHilnZ′|H=0 where Z′ is the partition function given by Z′=∫exp(-βE). Making use of the identity exp( fcosφ)=Σn=-∞n=∞In( f)exp(-inφ) the φ integration can be carried out.

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