|
|
|
|
| LEADER |
01000caa a22002652 4500 |
| 001 |
NLM118490044 |
| 003 |
DE-627 |
| 005 |
20250203055156.0 |
| 007 |
tu |
| 008 |
231222s1999 xx ||||| 00| ||eng c |
| 028 |
5 |
2 |
|a pubmed25n0395.xml
|
| 035 |
|
|
|a (DE-627)NLM118490044
|
| 035 |
|
|
|a (NLM)11969866
|
| 040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
| 041 |
|
|
|a eng
|
| 100 |
1 |
|
|a Reimann, P
|e verfasserin
|4 aut
|
| 245 |
1 |
0 |
|a Universal equivalence of mean first-passage time and Kramers rate
|
| 264 |
|
1 |
|c 1999
|
| 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 Completed 27.08.2002
|
| 500 |
|
|
|a Date Revised 28.07.2019
|
| 500 |
|
|
|a published: Print
|
| 500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
| 520 |
|
|
|a We prove that for an arbitrary time-homogeneous stochastic process, Kramers's flux-over-population rate is identical to the inverse of the associated mean first-passage time. In this way the mean first-passage time problem can be treated without making use of the adjoint equation in conjunction with cumbersome boundary conditions
|
| 650 |
|
4 |
|a Journal Article
|
| 700 |
1 |
|
|a Schmid, G J
|e verfasserin
|4 aut
|
| 700 |
1 |
|
|a Hänggi, P
|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 60(1999), 1 vom: 30. Juli, Seite R1-4
|w (DE-627)NLM098226002
|x 1063-651X
|7 nnns
|
| 773 |
1 |
8 |
|g volume:60
|g year:1999
|g number:1
|g day:30
|g month:07
|g pages:R1-4
|
| 912 |
|
|
|a GBV_USEFLAG_A
|
| 912 |
|
|
|a SYSFLAG_A
|
| 912 |
|
|
|a GBV_NLM
|
| 912 |
|
|
|a GBV_ILN_350
|
| 951 |
|
|
|a AR
|
| 952 |
|
|
|d 60
|j 1999
|e 1
|b 30
|c 07
|h R1-4
|