2022
DOI: 10.1021/acs.chemrev.2c00442
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Rotating Frame Relaxation in Magic Angle Spinning Solid State NMR, a Promising Tool for Characterizing Biopolymer Motion

Abstract: Magic angle spinning NMR rotating frame relaxation measurements provide a unique experimental window into biomolecules dynamics, as is illustrated by numerous recent applications. We discuss experimental strategies for this class of experiments, with a particular focus on systems where motion-driven modulation of the chemical shift interaction is the main mechanism for relaxation. We also explore and describe common strategies for interpreting the data sets to extract motion time scale, activation energy, and … Show more

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Cited by 7 publications
(8 citation statements)
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“…Under MAS, 15 N R 1ρ rates depend on the spectral densities J (ω) at the sum and difference frequencies of the spin-lock field strengths ω 1 and MAS frequency ω r . ,,,, For ω 1 /2π values of 2–12.5 kHz and ω r /2π of 55 kHz, motions with rates of 55–132 × 10 3 s –1 modulate the 15 N- 1 H dipolar coupling and 15 N chemical shift anisotropy (CSA) to cause R 1ρ relaxation. Therefore, the 15 N R 1ρ rates measured under our experimental conditions are sensitive to motions on the timescale of 8–18 μs.…”
Section: Resultssupporting
confidence: 59%
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“…Under MAS, 15 N R 1ρ rates depend on the spectral densities J (ω) at the sum and difference frequencies of the spin-lock field strengths ω 1 and MAS frequency ω r . ,,,, For ω 1 /2π values of 2–12.5 kHz and ω r /2π of 55 kHz, motions with rates of 55–132 × 10 3 s –1 modulate the 15 N- 1 H dipolar coupling and 15 N chemical shift anisotropy (CSA) to cause R 1ρ relaxation. Therefore, the 15 N R 1ρ rates measured under our experimental conditions are sensitive to motions on the timescale of 8–18 μs.…”
Section: Resultssupporting
confidence: 59%
“…Under MAS, 15 N R 1ρ rates depend on the spectral densities J (ω) at the sum and difference frequencies of the spin-lock field strengths ω 1 and MAS frequency ω r . ,,,, R 1 ρ , NH = 1 20 true[ μ 0 4 π γ normalH γ normalN r NH 3 0.25em true] 2 true[ 2 3 ( J false( ω 1 + 2 ω r false) + J false( ω 1 2 ω r false) ) + 4 3 0.25em ( J false( ω 1 + ω r false) + J false( ω 1 ω r false) ) + 0.25em 3 J ( ω N ) + J ( …”
Section: Resultsmentioning
confidence: 99%
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“…Longitudinal relaxation (R 1 ) is sensitive mostly to amplitudes and time scales of motions occurring on ps-ns time scales. Relaxation of 15 N coherence in the presence of a spin-lock pulse (R 1ρ ) is mostly sensitive to motions on time scales of tens of nanoseconds to hundreds of µs (26)(27)(28)(29)(30)(31)(32). Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Longitudinal relaxation ( R 1 ) is sensitive mostly to amplitudes and time scales of motions occurring on ps-ns time scales. Relaxation of 15 N coherence in the presence of a spin-lock pulse ( R 1ρ ) is mostly sensitive to motions on time scales of tens of nanoseconds to hundreds of μs. Figure A, B shows calculated relaxation rate constants for motion occurring on different time scales. R 1ρ experiments can be applied at multiple radiofrequency (RF) spin-lock field strengths, and the dependence on the RF field strength reveals specifically μs–ms motion (Figure A, insert), an effect sometimes referred to as NEar Rotary-resonance Relaxation Dispersion (NERRD; see below). ,, Thus, these different relaxation measurements allow the identification and quantitative interpretation of motional time scales and amplitudes in different time windows.…”
Section: Results and Discussionmentioning
confidence: 99%