2023
DOI: 10.1021/acs.langmuir.3c02755
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Modulation of Phase Behavior and Microscopic Dynamics in Cationic Vesicles by 1-Decyl-3-methylimidazolium Bromide

Jyoti Gupta,
Veerendra Kumar Sharma,
Harish Srinivasan
et al.

Abstract: Synthetic cationic lipids have garnered significant attention as promising candidates for gene/DNA transfection in therapeutic applications. The phase behavior of the vesicles formed by these lipids is intriguing, revealing intricate connections to the structure and dynamics of the membrane. These phenomena emerge from the complex interplay between hydrophobic and electrostatic interactions of the lipids. In this study, we explore the impact of an ionic liquid-based surfactant, 1-decyl-3-methylimidazolium brom… Show more

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“…The DPPC membrane presents significant dynamical activity in the spatiotemporal range of the IRIS spectrometer, as revealed by the strong quasielastic broadening, with the incorporation of the IL accelerating the membrane dynamics. Within the spatiotemporal domain of the IRIS spectrometer, lipid molecules predominantly exhibit two distinct dynamical modes: (i) lateral motion within the leaflet and (ii) localized internal motions of lipid alkyl chains. ,, The observed scattering data can be described as a convolution of two scattering laws, each associated with one of the two motions, expressed as: S normalm normale normalm ( Q , E ) = A ( Q ) italicL normall normala normalt ( Γ l a t , E ) + false( 1 A ( Q ) L normalt normalo normalt ( Γ l a t + Γ int , E ) …”
mentioning
confidence: 99%
“…The DPPC membrane presents significant dynamical activity in the spatiotemporal range of the IRIS spectrometer, as revealed by the strong quasielastic broadening, with the incorporation of the IL accelerating the membrane dynamics. Within the spatiotemporal domain of the IRIS spectrometer, lipid molecules predominantly exhibit two distinct dynamical modes: (i) lateral motion within the leaflet and (ii) localized internal motions of lipid alkyl chains. ,, The observed scattering data can be described as a convolution of two scattering laws, each associated with one of the two motions, expressed as: S normalm normale normalm ( Q , E ) = A ( Q ) italicL normall normala normalt ( Γ l a t , E ) + false( 1 A ( Q ) L normalt normalo normalt ( Γ l a t + Γ int , E ) …”
mentioning
confidence: 99%