The rapid measurement of spectral intensity with an oscillating Fabry-Perot spectrometer: isotope abundance in mercury

A high-resolution photoelectric spectrometer employing a mechanically scanned Fabry - Perot interferometer is described. The spectrometer produces high-finesse spectral profiles continuously and rapidly at repetitive frequencies of up to 1000 c/s corresponding to a time resolving limit of 4 u s for a scan of 5 orders. The display is on an oscilloscope or a pen-recorder function-plotter. The instrument has been tested with the high-frequency discharge spectrum of mercury. Single intensity measurements are reproducible to better than 0.5%. The wavelength scale is linear to 0.5% over an order and can be corrected to four times this accuracy. Hyperfine structures agree well with recent determinations which use both pressure scanned and photographic Fabry-Perot systems. The mercury isotope abundances have been obtained from the spectral intensity measurements agreeing well with mass-spectrometer values. The r.m.s. deviation for a single determination is less than 0.5% of the percentage abundance. Possible applications to rapidly varying phenomena in gas discharges and shock waves, the determination of refractive indices and extension to the ultra-violet region for spectroscopy from an earth satellite are briefly considered.

2010 ◽  
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D Hunger ◽  
T Steinmetz ◽  
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C Deutsch ◽  
T W Hänsch ◽  
...  
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2002 ◽  
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Yong Shim Yoo ◽  
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Hai-Woong Lee

2021 ◽  
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张天才 Zhang Tiancai ◽  
毋伟 Wu Wei ◽  
杨鹏飞 Yang Pengfei ◽  
李刚 Li Gang ◽  
张鹏飞 Zhang Pengfei

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R. Chiche ◽  
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2020 ◽  
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Yi Jiang ◽  
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Taojie Zhang ◽  
...  

1999 ◽  
Vol 162 (4-6) ◽  
pp. 267-279 ◽  
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A. Di Virgilio ◽  
M. Fiorentino ◽  
A. Porzio ◽  
S. Solimeno

2004 ◽  
Vol 82 (11) ◽  
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O Gagnon ◽  
...  

We determine the absolute density of a sample of laser-cooled atoms in a two-level system by recording the absorption spectrum of the 85Rb 5S1/2 (F = 3, mf = 3) → 5P3/2 (F′ = 4, m′f = 4) transition. Trapped atoms were prepared in the (F = 3, mf = 3) ground state through optical-pumping techniques. We compare our results with an independent measure of the density that relies on a direct measurement of the number of atoms and size of the atomic sample. We also study the contributions of power broadening, laser line width, and Doppler broadening to the measured absorption spectrum. Our studies suggest that the natural line width (~6 MHz) can be measured to a precision of less than ~50 kHz if the laser line width is measured in real-time with a high-finesse Fabry–Perot cavity. PACS Nos.: 32.70.Cs, 32.70.Jz, 32.80.Pj, 42.62.Fi, 32.70.–n, 32.30.–r


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