Sato Hideo, Bottle Steven E, Blinco James P, Micallef Aaron S, Eaton Gareth R, Eaton Sandra S
Department of Chemistry and Biochemistry, University of Denver, Denver, CO 80208, USA.
J Magn Reson. 2008 Mar;191(1):66-77. doi: 10.1016/j.jmr.2007.12.003. Epub 2007 Dec 14.
Electron spin-lattice relaxation rates, 1/T1, at X-band of nitroxyl radicals (4-hydroxy-2,2,6,6-tetramethylpiperidin-1-oxyl, 4-oxo-2,2,6,6-tetramethylpiperidin-1-oxyl, 3-carbamoyl-2,2,5,5-tetramethylpyrrolidin-1-oxyl and 3-carbamoyl-2,2,5,5-tetramethylpyrrolin-1-oxyl) in glass-forming solvents (decalin, glycerol, 3-methylpentane, o-terphenyl, 1-propanol, sorbitol, sucrose octaacetate, and 1:1 water:glycerol) at temperatures between 100 and 300K were measured by long-pulse saturation recovery to investigate the relaxation processes in slow-to-fast tumbling regimes. A subset of samples was also studied at lower temperatures or at Q-band. Tumbling correlation times were calculated from continuous wave lineshapes. Temperature dependence and isotope substitution (2H and 15N) were used to distinguish the contributions of various processes. Below about 100K relaxation is dominated by the Raman process. At higher temperatures, but below the glass transition temperature, a local mode process makes significant contributions. Above the glass transition temperature, increased rates of molecular tumbling modulate nuclear hyperfine and g anisotropy. The contribution from spin rotation is very small. Relaxation rates at X-band and Q-band are similar. The dependence of 1/T1 on tumbling correlation times fits better with the Cole-Davidson spectral density function than with the Bloembergen-Purcell-Pound model.
通过长脉冲饱和恢复法测量了在100至300K温度范围内,玻璃形成溶剂(十氢化萘、甘油、3 - 甲基戊烷、邻三联苯、1 - 丙醇、山梨醇、蔗糖八乙酸酯以及1:1的水:甘油)中硝酰自由基(4 - 羟基 - 2,2,6,6 - 四甲基哌啶 - 1 - 氧基、4 - 氧代 - 2,2,6,6 - 四甲基哌啶 - 1 - 氧基、3 - 氨基甲酰基 - 2,2,5,5 - 四甲基吡咯烷 - 1 - 氧基和3 - 氨基甲酰基 - 2,2,5,5 - 四甲基吡咯啉 - 1 - 氧基)在X波段的电子自旋 - 晶格弛豫速率1/T1,以研究慢到快翻滚区域的弛豫过程。还在较低温度或Q波段对一部分样品进行了研究。通过连续波线形计算翻滚相关时间。利用温度依赖性和同位素取代(2H和15N)来区分各种过程的贡献。在约100K以下,弛豫主要由拉曼过程主导。在较高温度但低于玻璃化转变温度时,局部模式过程起重要作用。在玻璃化转变温度以上,分子翻滚速率的增加调制了核超精细和g各向异性。自旋旋转的贡献非常小。X波段和Q波段的弛豫速率相似。1/T1对翻滚相关时间的依赖性与科尔 - 戴维森光谱密度函数的拟合优于与布洛姆伯根 - 珀塞尔 - 庞德模型的拟合。