Argon I Standards for Emission Spectrometry

J. Brault
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引用次数: 1

Abstract

For over a decade, users of the FTS at the McMath Solar Telescope of the National Solar Observatory have had access to a simple but precise working wavenumber standard for absorption spectra in the form of a short sealed cell containing 10 or 20 Torr of N2O. Because of the high pressure, the observed wavenumbers are not those of the unperturbed molecule, but a direct calibration of the 0002 band at 4417 cm−1in this cell against the accurately known P(7) transition in CH4 yielded wavenumbers with a precision of the order of 0.000002 cm−1 and an accuracy thought to be at least 0.00001 cm−1 (Brault [1]). Some years later, this band was observed by Pollock, et al. [2] using laser heterodyne techniques, and when our cell values are corrected using the pressure shift which they observed, the absolute agreement is quite satisfactory: (NSO - Pollock, calculated) = 0.000035 ± .0000035 cm−1; note that the absolute uncertainty in Pollock, et al. is quoted as .000080 cm−1.
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氩发射光谱法标准
十多年来,美国国家太阳天文台麦克马斯太阳望远镜FTS的用户已经获得了一个简单但精确的吸收光谱工作波数标准,其形式是一个含有10或20 Torr N2O的短密封单元。由于高压,观察到的波数不是未受扰动分子的波数,而是直接校准该细胞中4417 cm−1处的0002波段与CH4中精确已知的P(7)跃迁产生的波数精度为0.000002 cm−1数量级,精度被认为至少为0.00001 cm−1 (Brault[1])。几年后,波洛克等人[2]使用激光外差技术观察到了这一波段,当我们的细胞值使用他们观察到的压力位移进行校正时,绝对一致是相当令人满意的:(NSO -波洛克,计算)= 0.000035±0.0000035 cm−1;请注意,Pollock等人引用的绝对不确定性为0.000080 cm−1。
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