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Spatial extent of a single lipid's influence on bilayer mechanics.
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Membrane hydrophobicity determines the activation free energy of passive lipid transport.
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Measurement of the membrane curvature preference of phospholipids reveals only weak coupling between lipid shape and leaflet curvature.
Proc Natl Acad Sci U S A. 2009 Dec 29;106(52):22245-50. doi: 10.1073/pnas.0907354106. Epub 2009 Dec 23.
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A unifying Tm diagram for phosphatidylethanolamines with sn-1 C20 saturated and sn-2 C18 unsaturated acyl chains.
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Many-body effect of antimicrobial peptides: on the correlation between lipid's spontaneous curvature and pore formation.
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Pressure-induced ordering in mixed-lipid bilayers.
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9
Influence of cholesterol on the bilayer properties of monounsaturated phosphatidylcholine unilamellar vesicles.
Eur Phys J E Soft Matter. 2007 Jul;23(3):247-54. doi: 10.1140/epje/i2007-10202-8. Epub 2007 Jul 5.
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Structure and Dynamics of the Acyl Chains in the Membrane Trafficking and Enzymatic Processing of Lipids.
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2Danalysis: A toolbox for analysis of lipid membranes and biopolymers in two-dimensional space.
bioRxiv. 2025 Mar 2:2025.02.27.640563. doi: 10.1101/2025.02.27.640563.
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Softening in Two-Component Lipid Mixtures by Spontaneous Curvature Variance.
J Phys Chem B. 2024 Jul 4;128(26):6317-6326. doi: 10.1021/acs.jpcb.3c08117. Epub 2024 Jun 18.
3
Softening in two-component lipid mixtures by spontaneous curvature variance.
bioRxiv. 2023 Dec 13:2023.12.12.571323. doi: 10.1101/2023.12.12.571323.
4
Kinetic relaxation of giant vesicles validates diffusional softening in a binary lipid mixture.
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5
Simulated dynamic cholesterol redistribution favors membrane fusion pore constriction.
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Physiological changes in bilayer thickness induced by cholesterol control GPCR rhodopsin function.
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Lipid redistribution in the highly curved footprint of Piezo1.
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8
Molecular mechanisms of spontaneous curvature and softening in complex lipid bilayer mixtures.
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Curvature-based sorting of eight lipid types in asymmetric buckled plasma membrane models.
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2
Model Plasma Membrane Exhibits a Microemulsion in Both Leaves Providing a Foundation for "Rafts".
Biophys J. 2020 Mar 10;118(5):1019-1031. doi: 10.1016/j.bpj.2020.01.004. Epub 2020 Jan 16.
4
Mechanical properties of lipid bilayers: a note on the Poisson ratio.
Soft Matter. 2019 Nov 28;15(44):9085-9092. doi: 10.1039/c9sm01290g. Epub 2019 Oct 28.
5
6
Nonadditive Compositional Curvature Energetics of Lipid Bilayers.
Phys Rev Lett. 2016 Sep 23;117(13):138104. doi: 10.1103/PhysRevLett.117.138104.
7
The Continuing Mystery of Lipid Rafts.
J Mol Biol. 2016 Dec 4;428(24 Pt A):4749-4764. doi: 10.1016/j.jmb.2016.08.022. Epub 2016 Aug 26.
8
CHARMM-GUI Input Generator for NAMD, GROMACS, AMBER, OpenMM, and CHARMM/OpenMM Simulations Using the CHARMM36 Additive Force Field.
J Chem Theory Comput. 2016 Jan 12;12(1):405-13. doi: 10.1021/acs.jctc.5b00935. Epub 2015 Dec 3.
9
Routine Microsecond Molecular Dynamics Simulations with AMBER on GPUs. 2. Explicit Solvent Particle Mesh Ewald.
J Chem Theory Comput. 2013 Sep 10;9(9):3878-88. doi: 10.1021/ct400314y. Epub 2013 Aug 20.
10
Growth Conditions and Cell Cycle Phase Modulate Phase Transition Temperatures in RBL-2H3 Derived Plasma Membrane Vesicles.
PLoS One. 2015 Sep 14;10(9):e0137741. doi: 10.1371/journal.pone.0137741. eCollection 2015.

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