2019
DOI: 10.1101/782631
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Two-dimensional NMR lineshape analysis of single, multiple, zero and double quantum correlation experiments

Abstract: NMR spectroscopy provides a powerful approach for the characterisation of chemical exchange and molecular interactions by analysis of series of experiments acquired over the course of a titration measurement. The appearance of NMR resonances undergoing chemical exchange depends on the frequency difference relative to the rate of exchange, and in the case of one-dimensional experiments chemical exchange regimes are well established and well known. However, two-dimensional experiments present additional complexi… Show more

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Cited by 3 publications
(10 citation statements)
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“…Despite the small 15 N dispersions, the V111 and S155 resonances both become broadened during the peptide titration (Fig 3A, Appendix Figs S5 and S8A), indicative of slow‐to‐intermediate exchange. In a 2D 1 H‐ 15 N HSQC spectrum, chemical exchange‐induced broadening can arise from chemical shift changes to either the 15 N or 1 H nucleus or both (Waudby et al, 2020). Therefore, the broadening of V111 and S155 presumably arises from large 1 H chemical shift changes upon peptide binding, with Δω H V111 = 0.3 ppm and Δω H S155 = 0.5 ppm, respectively, corresponding to 1,131 rad/s and 1,885 rad/s at 14.1 T. By contrast, peptide binding does not significantly affect the 15 N chemical shifts of V111 and S155 (Δω N V111 = 0.2 ppm, Δω N S155 = 0.1 ppm; 90 rad/s and 45 rad/s at 14.1 T).…”
Section: Methodsmentioning
confidence: 99%
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“…Despite the small 15 N dispersions, the V111 and S155 resonances both become broadened during the peptide titration (Fig 3A, Appendix Figs S5 and S8A), indicative of slow‐to‐intermediate exchange. In a 2D 1 H‐ 15 N HSQC spectrum, chemical exchange‐induced broadening can arise from chemical shift changes to either the 15 N or 1 H nucleus or both (Waudby et al, 2020). Therefore, the broadening of V111 and S155 presumably arises from large 1 H chemical shift changes upon peptide binding, with Δω H V111 = 0.3 ppm and Δω H S155 = 0.5 ppm, respectively, corresponding to 1,131 rad/s and 1,885 rad/s at 14.1 T. By contrast, peptide binding does not significantly affect the 15 N chemical shifts of V111 and S155 (Δω N V111 = 0.2 ppm, Δω N S155 = 0.1 ppm; 90 rad/s and 45 rad/s at 14.1 T).…”
Section: Methodsmentioning
confidence: 99%
“…Despite the small 15 N dispersions, the V111 and S155 resonances both become broadened during the peptide titration (Fig 3A, Appendix Figs S5 and S8A), indicative of slow-to-intermediate exchange. In a 2D 1 H-15 N HSQC spectrum, chemical exchangeinduced broadening can arise from chemical shift changes to either the 15 N or 1 H nucleus or both(Waudby et al, 2020). Therefore, the broadening of V111 and S155 presumably arises from large 1 H chemical shift changes upon peptide binding, with Δω…”
mentioning
confidence: 99%
“…2A). This approach, in which individual phase cycle steps are stored during acquisition and re-combined during processing, was also recently applied to the simultaneous measurement of HZQC and HDQC correlation spectra 11 . In both instances, the total time required to acquire the pair of experiments is halved without any compromise to the quality of the individual measurements.…”
Section: Discussionmentioning
confidence: 99%
“…2A). As demonstrated for the simultaneous acquisition of HZQC and HDQC correlation experiments 11 , by storing individual increments of the phase program and applying receiver phase cycling postacquisition it is possible to acquire P-and N-type pathways for both DQ' and QQ relaxation measurements within a single super-experiment 46 , without loss of sensitivity. Shaded grey pulses represent consecutive 5 kHz 2 ms Hx and 3 ms Hy purge pulses before the recycle delay, B!9 (with low power presaturation applied, if required).…”
Section: A Hahn Echo Super-experiments For the Measurement Of Relaxation Rates Of Four Spin Coherencesmentioning
confidence: 99%
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