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Figure 8
Simulated distance distribution function, p(r), of LUV depending on the protein occlusion, obtained from Fig. 7[link]. The insert expands the p(r) functions in the short-distance region. The changes in the broad peak position at ∼500–700 Å and in the ripple profile below ∼55 Å can describe the experimental ones in Fig. 4[link].

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 20| Part 6| September 2013| Pages 869-874
doi:10.1107/S0909049513020827
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