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Optics and Spectroscopy

An Experimental Study of the Fluorescence Spectrum of Cesium Atoms in the Presence of a Buffer Gas

V. G. Davydov, V. N. Kulyasov

Published Jan 1, 2018• 0 citations
Publisher

Abstract

A direct experiment is performed to determine the quantum efficiency of a cesium fluorescence filter. The fluorescence spectra of cesium atoms are recorded under excitation of the upper states of the second resonance doublet with a Bell–Bloom cesium lamp. Introduction of different noble gases into the cell with cesium leads to the appearance of additional fluorescence photons. It is found that a fluorescence filter based on atomic cesium vapor with addition of helium in the working cell has the highest efficiency and response rate of all known fluorescence filters based on alkali-metal atomic vapors.

DOI
10.1134/s0030400x18010058

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A direct experiment is performed to determine the quantum efficiency of a cesium fluorescence filter. The fluorescence spectra of cesium atoms are recorded under excitation of the upper states of the second resonance doublet with a Bell–Bloom cesium lamp. Introduction of different noble gases into the cell with cesium leads to the appearance of additional fluorescence photons. It is found that a fluorescence filter based on atomic cesium vapor with addition of helium in the working cell has the highest efficiency and response rate of all known fluorescence filters based on alkali-metal atomic vapors.
The dependence of the quantum efficiency of fluorescence cesium vapor filters, which allow one to select with a high contrast the desired narrow-band signal against the background of broadband (solar) radiation, is studied. The most important characteristic of such filters, apart from the spectral band, is the quantum efficiency; i.e., the ratio of the number of florescent photons to the number of absorbed photons of excitation. It is experimentally shown that addition of a buffer gas to working cesium atoms can substantially increase the quantum efficiency as compared with that of working atoms in vacuum. The dependence of the quantum efficiency on the characteristic of transitions that are involved in population of atomic levels from which fluorescence occurs, and the processes resulting in an increase in the quantum efficiency of atomic fluorescence filters are considered.
A blue alkali laser operating by direct optical excitation of the 72P3/2 state of cesium is demonstrated. A mixture of cesium vapor and various buffer gases (4He, CH4, C2H6) were pumped with the output of a pulsed dye laser in a heated glass cell. The spin-orbit mixing and fluorescence quenching cross sections were calculated for each buffer gas using the time-dependent D1 (459 nm) side fluorescence. At certain temperatures and buffer gas pressures, a spatially coherent blue beam is produced in the forward direction. An analysis of the spectrum shows this beam contains both D1 amplified spontaneous emission (ASE) and Stimulated Raman Scattering (SRS).
Laser-induced fluorescence (LIF) was studied in the 400–1000 nm wavelength range using narrow-band 852 nm laser radiation resonant with Cs atomic 6S1/2 → 6P3/2 transition. T-shaped cells made entirely of technical sapphire with thicknesses of L = 1 cm, 40 μm, and ~400 nm, containing cesium atomic vapor, were used. It was shown that with the cell thickness decrease (from centimeters to nanometer thicknesses), many LIF signals are suppressed due to an increase in the number of atomic collisions with the walls, leading to quenching of excited states. By recording the LIF signal, it is also possible to estimate the amount of residual Rb atomic vapor (if any exists) in the Cs-containing cell. The Cs vapor cell can serve as an efficient optical frequency converter filter and has other applications.