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Figure 6
Scattering intensity I as a function of the dimensionless wavevector qR0 obtained (a) from the symmetric three-Gaussian EDP with ρ1 = ρ3 [cf. equation (4)[link] and Table 3[link]] and (b) with the curvature-dependent EDP, equation (2)[link], parameterized from the MARTINI model simulation (cf. Fig. 3[link]).

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 54| Part 2| April 2021| Pages 557-568
https://doi.org/10.1107/S1600576721001461
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