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Baumgart, T.; Hess, S. T.; Webb, W. W. Nature 2003, 425, 821-824.
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Nature
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Baumgart, T.1
Hess, S.T.2
Webb, W.W.3
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(a) Drouffe, J. M.; Maggs, A. C.; Leibler, S. Science 1991, 254, 1353-1356.
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(c) Yamamoto, S.; Maruyma, Y.; Hyodo, S. J. Chem. Phys. 2002, 116, 5842-5849.
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Yamamoto, S.1
Maruyma, Y.2
Hyodo, S.3
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9
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4143138518
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Simulations were performed using isotropic pressure (P = 1 bar) conditions at T = 323 K with the force field as described for system F in: Anézo, C.; de Vries, A. H.; Höltje, H.-D.; Tieleman, D. P.; Marrink, S. J. J. Phys. Chem. B 2003, 107, 9424-9433, with a long-range cutoff of 1.5 nm, using a reaction-field correction and periodic boundary conditions. All simulations were performed with the GROMACS code (Lindahl, E.; Hess, B.; van der Spoel, D. J. Mol. Model. 2001, 7, 306-317) on a cluster of 1.7 GHz Intel Pentium IV processors. The code was run in parallel on four or eight processors under MPI. The rate of simulation was 1 ps per processor CPU hour.
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(2003)
J. Phys. Chem. B
, vol.107
, pp. 9424-9433
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Anézo, C.1
De Vries, A.H.2
Höltje, H.-D.3
Tieleman, D.P.4
Marrink, S.J.5
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10
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0035789518
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Simulations were performed using isotropic pressure (P = 1 bar) conditions at T = 323 K with the force field as described for system F in: Anézo, C.; de Vries, A. H.; Höltje, H.-D.; Tieleman, D. P.; Marrink, S. J. J. Phys. Chem. B 2003, 107, 9424-9433, with a long-range cutoff of 1.5 nm, using a reaction-field correction and periodic boundary conditions. All simulations were performed with the GROMACS code (Lindahl, E.; Hess, B.; van der Spoel, D. J. Mol. Model. 2001, 7, 306-317) on a cluster of 1.7 GHz Intel Pentium IV processors. The code was run in parallel on four or eight processors under MPI. The rate of simulation was 1 ps per processor CPU hour.
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(2001)
J. Mol. Model.
, vol.7
, pp. 306-317
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Lindahl, E.1
Hess, B.2
Van Der Spoel, D.3
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11
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0035812426
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Marrink, S. J.; Lindahl, E.; Edholm, O.; Mark, A. E. J. Am. Chem. Soc. 2001, 123, 8638-8639.
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J. Am. Chem. Soc.
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Marrink, S.J.1
Lindahl, E.2
Edholm, O.3
Mark, A.E.4
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12
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1842703812
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note
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Note, the formation of a (multi)lamellar system is not prohibited.
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13
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0038514127
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(a) Tieleman, D. P.; Leontiadou, H.; Mark, A. E.; Marrink, S. J. J. Am. Chem. Soc. 2003, 125, 6382-6383.
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(2003)
J. Am. Chem. Soc.
, vol.125
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Tieleman, D.P.1
Leontiadou, H.2
Mark, A.E.3
Marrink, S.J.4
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15
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0141794070
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Kakorin, S.; Liese, T.; Neumann, E. J. Phys. Chem. B 2003, 107, 10243-10251.
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J. Phys. Chem. B
, vol.107
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Kakorin, S.1
Liese, T.2
Neumann, E.3
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16
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0020468317
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(a) Cornell, B. A.; Fletcher, G. C.; Middlehurst, J.; Separovic, F. Biochim. Biophys. Acta 1982, 690, 15-19.
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(1982)
Biochim. Biophys. Acta
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Cornell, B.A.1
Fletcher, G.C.2
Middlehurst, J.3
Separovic, F.4
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17
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0037144033
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(b) Vesicles with a diameter of 13 nm have been observed for other amphiphiles: Buwalda, R. T.; Stuart, M. C. A.; Engberts, J. B. F. N. Langmuir 2002, 18, 6507-6512.
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(2002)
Langmuir
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Buwalda, R.T.1
Stuart, M.C.A.2
Engberts, J.B.F.N.3
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18
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1842804673
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note
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A simulation using the CG model of ref 3d with the same setup as used for the atomistic model resulted in a sealed vesicle containing 1012 lipids after 30 ns with intermediates similar to those shown here for the atomistic model.
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19
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1842703813
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note
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The vesicular state at the end of the simulation is formed by 1002 DPPC lipids. The remaining 15 lipids formed a micelle during the simulation. The assignment of lipids to inner and outer leaflets is somewhat arbitrary because a number of headgroups are lining water pores and therefore do not clearly belong to either the inner or the outer leaflet.
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20
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1842703808
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note
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First neighbor headgroups strongly favor antiparallel orientations, minimizing dipole-dipole repulsion. Second neighbors show a weak preference for parallel orientation. After the second shell of neighbors, the correlation disappears quickly.
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