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中国物理学会期刊

由飞行时间质谱峰形获取光解碎片平动能分布

CSTR: 32037.14.aps.54.2418

An approach to obtain the photofragment translational energy distribution from time-of-flight profile

CSTR: 32037.14.aps.54.2418
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  • 由于在魔角条件下测量的飞行时间(TOF)质谱峰形与光解碎片的角分布无关,因而便于用含待定参数的平动能分布函数去拟合质谱峰形来获取光解碎片的平动能分布.与通常的拟合法不同,提出一种峰形参量法,只需通过测量TOF峰形的半高宽(t1/2)、四 分之一高宽(t1/4)和四分之三高宽(t3/4),便可借助文中提供 的曲线图或 解析式得出碎片平均平动能,平动能分布特征宽度以及描述实验装置本身的特征峰宽等.处 理过程中,平动能分布及实验装置峰形均采用相应的高斯分布函数描述.

     

    At the magic angle, the time_of_flight mass_spectrometer (TOF-MS) profile depends only on the translational energy distribution of photofragment, and is indep endent of the angle distribution of recoil momentum, therefore, the translationa l energy distribution is usually determined by fitting the measured TOF-MS profi le. Different from the above procedure, we take another approach in the present work. According to this method, by measuring three widths at half maximum (t 1/2), one-fourth maximum (t1/4) and three-fourth m aximum (t 3/4) of the TOF-MS profile, the averaged translational energy, th e width of translational energy distribution, as well as the width of instrumental func tion can be determined from numeric tables or mathematical expressions. In this method, both the translational energy distribution and the instrumental function are described by Gaussian functions.

     

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