Department of Chemistry and Biochemistry, University of Denver, Denver, CO 80208, USA.
J Magn Reson. 2012 Dec;225:52-7. doi: 10.1016/j.jmr.2012.10.002. Epub 2012 Oct 17.
Electron spin relaxation times of perdeuterated tempone (PDT) 1 and of a nitronyl nitroxide (2-(4-carboxy-phenyl)-4,4,5,5-tetramethylimidazoline-3-oxide-1-oxyl) 2 in aqueous solution at room temperature were measured by 2-pulse electron spin echo (T(2)) or 3-pulse inversion recovery (T(1)) in the frequency range of 250 MHz to 34 GHz. At 9 GHz values of T(1) measured by long-pulse saturation recovery were in good agreement with values determined by inversion recovery. Below 9 GHz for 1 and below 1.5 GHz for 2,T(1)~T(2), as expected in the fast tumbling regime. At higher frequencies T(2) was shorter than T(1) due to incomplete motional averaging of g and A anisotropy. The frequency dependence of 1/T(1) is modeled as the sum of spin rotation, modulation of g and A-anisotropy, and a thermally-activated process that has maximum contribution at about 1.5 GHz. The spin lattice relaxation times for the nitronyl nitroxide were longer than for PDT by a factor of about 2 at 34 GHz, decreasing to about a factor of 1.5 at 250 MHz. The rotational correlation times, τ(R) are calculated to be 9 ps for 1 and about 25 ps for 2. The longer spin lattice relaxation times for 2 than for 1 at 9 and 34 GHz are due predominantly to smaller contributions from spin rotation that arise from slower tumbling. The smaller nitrogen hyperfine couplings for the nitronyl 2 than for 1 decrease the contribution to relaxation due to modulation of A anisotropy. However, at lower frequencies the slower tumbling of 2 results in a larger value of ωτ(R) (ω is the resonance frequency) and larger values of the spectral density function, which enhances the contribution from modulation of anisotropic interactions for 2 to a greater extent than for 1.
室温下,通过在 250MHz 至 34GHz 的频率范围内使用双脉冲电子自旋回波(T(2))或三脉冲反转恢复(T(1)),测量了全氘代 tempone(PDT)1 和硝酰基氮氧化物(2-(4-羧基-苯基)-4,4,5,5-四甲基咪唑啉-3-氧化物-1-氧自由基)2 在水溶液中的电子自旋弛豫时间。在 9GHz 时,通过长脉冲饱和恢复测量的 T(1)值与通过反转恢复确定的值非常吻合。对于 1,在低于 9GHz,对于 2,在低于 1.5GHz 时,T(1)~T(2),这在快速翻滚状态下是预期的。在较高频率下,由于 g 和 A 各向异性的不完全运动平均,T(2)短于 T(1)。1/T(1)的频率依赖性被建模为自旋旋转、g 和 A 各向异性调制以及在约 1.5GHz 处具有最大贡献的热激活过程的总和。硝酰基氮氧化物的自旋晶格弛豫时间比 PDT 长约 2 倍,在 34GHz 时为 250MHz。旋转相关时间τ(R)计算为 9ps 对于 1 和大约 25ps 对于 2.在 9GHz 和 34GHz 时,2 比 1 的自旋晶格弛豫时间更长,主要是由于自旋旋转的贡献较小,这是由于翻滚速度较慢引起的。对于 2 比 1,较小的氮超精细耦合降低了由于 A 各向异性调制而导致的弛豫贡献。然而,在较低频率下,2 的较慢翻滚导致更大的 ωτ(R)(ω 是共振频率)值和更大的谱密度函数值,这使得对于 2 比 1 更大程度地增强了各向异性相互作用调制的贡献。