|
|
|
|
LEADER |
01000caa a22002652 4500 |
001 |
NLM110035747 |
003 |
DE-627 |
005 |
20250202085546.0 |
007 |
tu |
008 |
231222s2000 xx ||||| 00| ||eng c |
028 |
5 |
2 |
|a pubmed25n0367.xml
|
035 |
|
|
|a (DE-627)NLM110035747
|
035 |
|
|
|a (NLM)11088111
|
040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
041 |
|
|
|a eng
|
100 |
1 |
|
|a Lippiello
|e verfasserin
|4 aut
|
245 |
1 |
0 |
|a Fluctuation dissipation ratio in the one-dimensional kinetic ising model
|
264 |
|
1 |
|c 2000
|
336 |
|
|
|a Text
|b txt
|2 rdacontent
|
337 |
|
|
|a ohne Hilfsmittel zu benutzen
|b n
|2 rdamedia
|
338 |
|
|
|a Band
|b nc
|2 rdacarrier
|
500 |
|
|
|a Date Revised 20.11.2019
|
500 |
|
|
|a published: Print
|
500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
520 |
|
|
|a The exact relation between the response function R(t,t(')) and the two time correlation function C(t,t(')) is derived analytically in the one-dimensional kinetic Ising model subjected to a temperature quench. The fluctuation dissipation ratio X(t,t(')) is found to depend on time through C(t,t(')) in the time region where scaling C(t,t('))=f(t/t(')) holds. The crossover from the nontrivial form X[C(t,t('))] to X(t,t(')) identical with1 takes place as the waiting time t(w) is increased from below to above the equilibration time t(eq)
|
650 |
|
4 |
|a Journal Article
|
700 |
1 |
|
|a Zannetti
|e verfasserin
|4 aut
|
773 |
0 |
8 |
|i Enthalten in
|t Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics
|d 1993
|g 61(2000), 4 Pt A vom: 27. Apr., Seite 3369-74
|w (DE-627)NLM098226002
|x 1063-651X
|7 nnns
|
773 |
1 |
8 |
|g volume:61
|g year:2000
|g number:4 Pt A
|g day:27
|g month:04
|g pages:3369-74
|
912 |
|
|
|a GBV_USEFLAG_A
|
912 |
|
|
|a SYSFLAG_A
|
912 |
|
|
|a GBV_NLM
|
912 |
|
|
|a GBV_ILN_350
|
951 |
|
|
|a AR
|
952 |
|
|
|d 61
|j 2000
|e 4 Pt A
|b 27
|c 04
|h 3369-74
|