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. 2019 Nov 28;48(2):924–933. doi: 10.1093/nar/gkz1096

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© The Author(s) 2019. Published by Oxford University Press on behalf of Nucleic Acids Research.

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.

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Figure 6. — Comparison of PELDOR signals calculated from MD (red) to experiments (black) for RNA(1,10). (A) PELDOR time traces measured at X-band with different offsets ν_n between probe and pump pulse frequency from 40 MHz (lower time trace) to 90 MHz (upper time trace). (B) PELDOR time traces measured at G-band at different field positions with a constant offset of 60 MHz. The field position correspond to B∥g_xx − B∥g_zz (C) Distance distribution from PELDOR measurements obtained by Tikhonov regularization (black), and from MD simulation (red), including the individual conformational states of the molecules.

Inline graphic — Comparison of PELDOR signals calculated from MD (red) to experiments (black) for RNA(1,10). (A) PELDOR time traces measured at X-band with different offsets ν_n between probe and pump pulse frequency from 40 MHz (lower time trace) to 90 MHz (upper time trace). (B) PELDOR time traces measured at G-band at different field positions with a constant offset of 60 MHz. The field position correspond to B∥g_xx − B∥g_zz (C) Distance distribution from PELDOR measurements obtained by Tikhonov regularization (black), and from MD simulation (red), including the individual conformational states of the molecules.