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Volumn 78, Issue 22, 2008, Pages

Superuniversality in phase-ordering disordered ferromagnets

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EID: 58149271051     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.224419     Document Type: Article
Times cited : (42)

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    • Indeed, if we take ε=2, then for T≳0.6 notable finite-time corrections to simple aging are seen, which may be accounted for by including a finite-time correction term (Refs.). C (t,s) = FC (t/s) - s- b′ GC (t/s) and a new correction exponent b′ >0.
    • Indeed, if we take ε=2, then for T≳0.6 notable finite-time corrections to simple aging are seen, which may be accounted for by including a finite-time correction term (Refs.). C (t,s) = FC (t/s) - s- b′ GC (t/s) and a new correction exponent b′ >0.
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    • The consideration of the spatiotemporal response allows for a much more demanding test of dynamical scaling than is possible by merely considering the autoresponse alone. Our results hence strengthen the conclusions of a simple power-law scaling in the disordered Ising model reached earlier (Refs.).
    • The consideration of the spatiotemporal response allows for a much more demanding test of dynamical scaling than is possible by merely considering the autoresponse alone. Our results hence strengthen the conclusions of a simple power-law scaling in the disordered Ising model reached earlier (Refs.).
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    • It is conceivable that our finding of a distinct behavior for ε=2 might be a sort of borderline behavior when going from ferromagnets to frustrated magnet.
    • It is conceivable that our finding of a distinct behavior for ε=2 might be a sort of borderline behavior when going from ferromagnets to frustrated magnet.


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