2019
DOI: 10.48550/arxiv.1903.06659
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Molecular ordering in lipid monolayers: an atomistic simulation

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“…4. As a reference, in each case the value of the temperature is chosen such that the density gap is close or of the same order as that observed in the atomistic simulations [9], which is approximately 27% with respect to the density of the LC phase. Therefore the temperatures are kT /ǫ GB = 0.13 in panel (a), 0.1825 in panel (b), 0.12 in panel (c) and 0.15 in panel (d), giving density gaps of 27%, 27%, 22% and 12%, respectively.…”
Section: Resultsmentioning
confidence: 99%
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“…4. As a reference, in each case the value of the temperature is chosen such that the density gap is close or of the same order as that observed in the atomistic simulations [9], which is approximately 27% with respect to the density of the LC phase. Therefore the temperatures are kT /ǫ GB = 0.13 in panel (a), 0.1825 in panel (b), 0.12 in panel (c) and 0.15 in panel (d), giving density gaps of 27%, 27%, 22% and 12%, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…Experimental values of λ for lipid monolayers, extracted from domain size distributions [15], are in the range 1 − 10 fN (although values measured using other techniques may be higher by even two orders of magnitude depending on the system [16][17][18]). Using σ 0 ∼ 0.4 nm (estimated from experimental values of area per lipid in LC domains of DPPC monolayers) and ǫ GB ∼ 50 kT (estimated from atomistic force-field simulations [9], and see also [19]), we obtain values of λ ∼ 2 − 15 fN, i. e. within the same order of magnitude as in [15]. Interestingly, line tensions exhibit well-defined minima which correspond to equilibrium oblique configurations at the boundary between LE and LC phases.…”
Section: Resultsmentioning
confidence: 99%
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