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Volumn 84, Issue 13, 2011, Pages

Ferromagnetic-glassy transitions in three-dimensional Ising spin glasses

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EID: 80155211545     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.84.134202     Document Type: Article
Times cited : (23)

References (39)
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    • In the case of the random-field Ising model, where hyperscaling is violated, the space dimension d in Eq. is replaced by (Ref.) d-θ, thus, β=ν(d-θ-2+η)/2, where θ is the hyperscaling violation exponent.
    • In the case of the random-field Ising model, where hyperscaling is violated, the space dimension d in Eq. is replaced by (Ref.) d - θ, thus, β = ν (d - θ - 2 + η) / 2, where θ is the hyperscaling violation exponent.
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    • )φ for p≥0.7 and a straight line for 0.5≤p≤0.7.
    • ) φ for p ≥ 0.7 and a straight line for 0.5 ≤ p ≤ 0.7.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.