001     31343
005     20240610121328.0
017 _ _ |a This version is available at the following Publisher URL: http://pre.aps.org
024 7 _ |a 10.1103/PhysRevE.68.061905
|2 DOI
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024 7 _ |a 2128/1485
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037 _ _ |a PreJuSER-31343
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Fluids & Plasmas
084 _ _ |2 WoS
|a Physics, Mathematical
100 1 _ |a Kohyama, T.
|b 0
|u FZJ
|0 P:(DE-Juel1)VDB24716
245 _ _ |a Budding of crystalline domains in fluid membranes
260 _ _ |a College Park, Md.
|b APS
|c 2003
264 _ 1 |3 online
|2 Crossref
|b American Physical Society (APS)
|c 2003-12-17
264 _ 1 |3 print
|2 Crossref
|b American Physical Society (APS)
|c 2003-12-01
300 _ _ |a 061905
336 7 _ |a Journal Article
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336 7 _ |a article
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440 _ 0 |a Physical Review E
|x 1539-3755
|0 4924
|v 68
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a Crystalline domains embedded in fluid membrane vesicles are studied by Monte Carlo simulations of dynamically triangulated surfaces and by scaling arguments. A budding transition from a caplike state to a budded shape is observed for increasing spontaneous curvature C-0 of the crystalline domain as well as increasing line tension lambda. The location of the budding transition is determined as a function of C-0, lambda, and the radius R-A of the crystalline domain. In contrast to previous theoretical predictions, it is found that budding occurs at a value of the spontaneous curvature C-0, that is always a decreasing function of the domain size R-A. Several characteristic scaling regimes are predicted. The distribution of five- and sevenfold disclinations as the budding transition is approached is determined, and the dynamics of the generation of defects is studied.
536 _ _ |a Kondensierte Materie
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700 1 _ |a Kroll, D. M.
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700 1 _ |a Gompper, G.
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773 1 8 |a 10.1103/physreve.68.061905
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|t Physical Review E
|v 68
|y 2003
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773 _ _ |a 10.1103/PhysRevE.68.061905
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856 7 _ |u http://dx.doi.org/10.1103/PhysRevE.68.061905
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856 4 _ |u https://juser.fz-juelich.de/record/31343/files/31905.pdf
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