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直接实时分析与电喷雾电离飞行时间质谱法的内禀能量沉积比较。

Comparison of the internal energy deposition of direct analysis in real time and electrospray ionization time-of-flight mass spectrometry.

机构信息

School of Chemistry and Biochemistry, Georgia Institute of Technology, Atlanta, Georgia 30317, USA.

出版信息

J Am Soc Mass Spectrom. 2010 May;21(5):855-63. doi: 10.1016/j.jasms.2010.01.019. Epub 2010 Jan 28.

DOI:10.1016/j.jasms.2010.01.019
PMID:20181493
Abstract

The internal energy (E(int)) distributions of a series of p-substituted benzylpyridinium ions generated by both direct analysis in real time (DART) and electrospray ionization (ESI) were compared using the "survival yield" method. DART mean E(int) values at gas flow rates of 2, 4, and 6 L min(-1), and at set temperatures of 175, 250, and 325 degrees C were in the 1.92-2.21 eV range. ESI mean E(int) at identical temperatures in aqueous and 50% methanol solutions ranged between 1.71 and 1.96 eV, and 1.53 and 1.63 eV, respectively. Although the results indicated that ESI is a "softer" ionization technique than DART, there was overlap between the two techniques for the particular time-of-flight mass spectrometer used. As a whole, there was an increase in E(int) with increasing reactive and drying gas temperatures for DART and ESI, respectively, indicating thermal ion activation. Three dimensional computational fluid dynamic simulations in combination with direct temperature measurements within the DART ionization region revealed complex inversely coupled fluid-thermal phenomena affecting ion E(int) values during atmospheric transport. Primarily, that DART gas temperature in the ionization region was appreciably less than the set gas temperature of DART due to the set gas flow rates. There was no evidence of E(int) deposition pathways from metastable-stimulated desorption, but fragmentation induced by high-energy helium metastables was observed at the highest gas flow rates and temperatures.

摘要

采用“存活产率”方法比较了由实时直接分析(DART)和电喷雾电离(ESI)产生的一系列取代的苄基吡啶鎓离子的内(E(int))能分布。在气体流速为 2、4 和 6 L min(-1)以及设定温度为 175、250 和 325°C 的情况下,DART 的平均 E(int)值在 1.92-2.21 eV 范围内。在相同温度下,在水溶液中和 50%甲醇溶液中 ESI 的平均 E(int)分别在 1.71-1.96 eV 和 1.53-1.63 eV 范围内。尽管结果表明 ESI 是比 DART 更“软”的电离技术,但对于所使用的特定飞行时间质谱仪,两种技术之间存在重叠。总的来说,随着反应性和干燥气体温度的升高,DART 和 ESI 的 E(int)分别增加,这表明热离子活化。DART 电离区的三维计算流体动力学模拟与直接温度测量相结合,揭示了在大气传输过程中影响离子 E(int)值的复杂反向耦合流-热现象。主要是,由于设定的气体流速,DART 气体在电离区的温度明显低于 DART 的设定气体温度。没有证据表明存在由亚稳态激发解吸引起的 E(int)沉积途径,但在最高气体流速和温度下观察到高能氦亚稳态引起的碎裂。

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