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甘氨酸、N-甲基乙酰胺和苯甲酸根阴离子在重水溶液中的振动能量动力学

Vibrational energy dynamics of glycine, N-methylacetamide, and benzoate anion in aqueous (D2O) solution.

作者信息

Fang Ying, Shigeto Shinsuke, Seong Nak-Hyun, Dlott Dana D

机构信息

School of Chemical Sciences, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA.

出版信息

J Phys Chem A. 2009 Jan 8;113(1):75-84. doi: 10.1021/jp8062228.

Abstract

Ultrafast infrared-Raman spectroscopy is used to study vibrational energy dynamics of three molecules in aqueous solution (D(2)O) that serve as models for the building blocks of peptides. These are glycine-d(3) zwitterion (GLY), N-methylacetamide-d (NMA), and benzoate anion (BZ). GLY is the simplest amino acid, NMA a model compound with a peptide bond, and BZ a model for aromatic side chains. An ultrashort IR pulse pumps a parent CH-stretch on each solute. Anti-Stokes Raman monitors energy flow through the solutes' strongly Raman-active transitions. Stokes Raman of D(2)O stretching functions as a molecular thermometer to monitor energy dissipation from solute to solvent. A three-stage model is used to summarize the vibrational energy redistribution process and to provide a framework for discussing energy dynamics of different molecules. The initial CH-stretch excitation is found to be delocalized over some or all of the solute molecule in NMA and BZ but not in GLY. The overall time constants for energy dissipation are 7.2 ps for GLY, 4.9 ps for NMA, and 8.0 ps for BZ. CH-stretch energy in GLY is redistributed in a nearly statistical manner among observed GLY vibrations. In NMA the energy is distributed among about one-half of the observed vibrations, and in BZ much of the observed energy is channeled along a CH-stretch to the ring stretch pathway. The strongly Raman-active vibrations accurately represent the flow of vibrational energy through NMA but not through GLY or BZ.

摘要

超快红外拉曼光谱用于研究水溶液(重水)中三种分子的振动能量动力学,这三种分子作为肽构建单元的模型。它们分别是甘氨酸 -d₃两性离子(GLY)、N - 甲基乙酰胺 -d(NMA)和苯甲酸根阴离子(BZ)。GLY是最简单的氨基酸,NMA是具有肽键的模型化合物,BZ是芳香侧链的模型。一个超短红外脉冲泵浦每个溶质上的母体C - H伸缩振动。反斯托克斯拉曼光谱监测通过溶质强烈拉曼活性跃迁的能量流动。重水伸缩振动的斯托克斯拉曼光谱用作分子温度计,以监测从溶质到溶剂的能量耗散。使用一个三阶段模型来总结振动能量重新分布过程,并为讨论不同分子的能量动力学提供一个框架。发现初始C - H伸缩激发在NMA和BZ中的部分或全部溶质分子上是离域的,但在GLY中不是。能量耗散的总体时间常数对于GLY为7.2皮秒,对于NMA为4.9皮秒,对于BZ为8.0皮秒。GLY中的C - H伸缩能量在观察到的GLY振动之间以近乎统计的方式重新分布。在NMA中,能量分布在大约一半观察到的振动之间,而在BZ中,观察到的大部分能量沿着C - H伸缩到环伸缩途径传导。强烈的拉曼活性振动准确地代表了通过NMA的振动能量流动,但不代表通过GLY或BZ的振动能量流动。

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