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Volumn 86, Issue 9, 2001, Pages 1785-1788

Renormalization of pinned elastic systems: How does it work beyond one loop?

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; ELASTICITY; EQUATIONS OF MOTION; PHASE EQUILIBRIA; SURFACE ROUGHNESS;

EID: 0035243002     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.86.1785     Document Type: Article
Times cited : (241)

References (35)
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    • note
    • At equilibrium, time persistent, i.e., ∝ δ(ω) quantities identify (to all orders in perturbation) to distinct replica averages and equal time to same replica averages.
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    • note
    • Noting [21] that graphs can be grouped in subsets (e.g., pairs ac, bd, ef in Fig. 2) which vanish by shifting the endpoint of an internal line within a splitted vertex.
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    • note
    • 2 (we thank E. Brézin for this remark).
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    • note
    • Anomalous contributions (e.g., ∝ ln2/∈) are found to cancel.
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    • note
    • */(+∞) ≠ 0, as it should for RF.
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    • note
    • The FP is however unstable in one direction.
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    • note
    • Fractional powers of disorder then appear in equilibrium expectation values.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.