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Journal of Applied Physics

The spectral characteristics of an atomic cesium resonance filter

Allen M. Flusberg

Published Oct 1, 1983• 6 citations
Publisher

Abstract

It is shown that the excitation spectrum of atomic Cs vapor around 455.5 nm (21947 cm−1), observed by Marling et al., contains 0.1 cm−1 structure which is not expected on the basis of hyperfine constants previously reported in the literature. If this structure is extraneous it follows that a Cs vapor resonance ‘‘filter’’ designed to fluoresce in the red when irradiated on its blue (455.5 nm) resonance can suppress background light better than has heretofore been thought. Additional experiments to determine the origin and relevance of this structure are therefore recommended.

DOI
10.1063/1.331784

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We have observed laser-induced fluorescence using 456 nm laser radiation, resonant with the 6S1/2-7P3/2 transition in Cs atoms. It includes red emission lines in the range of 580-730 nm and a prominent line at 852 nm corresponding to the 6P3/2-6S1/2 transition. A T-shaped all-sapphire cell with a length of 1 cm, containing Cs atomic vapor and capable of being heated up to 500 oC, was used. The laser-induced fluorescence (LIF) power at 852 nm was investigated as a function of the cell temperature. The maximum LIF power was achieved at 130 oC, while a significant decrease was observed around 300 oC. At 130 oC, the Doppler-broadened LIF spectrum at 852 nm exhibited self-conversion, resulting in the formation of two distinct peaks within the spectrum. The LIF power at 852 nm was also studied as a function of the 456 nm radiation power. The Cs cell demonstrated potential as an efficient optical filter and down-converter, effectively transforming 456 nm radiation into 852 nm radiation.

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Optics and Spectroscopy•Jan 1, 2018•0 citations
It is shown that the excitation spectrum of atomic Cs vapor around 455.5 nm (21947 cm−1), observed by Marling et al., contains 0.1 cm−1 structure which is not expected on the basis of hyperfine constants previously reported in the literature. If this structure is extraneous it follows that a Cs vapor resonance ‘‘filter’’ designed to fluoresce in the red when irradiated on its blue (455.5 nm) resonance can suppress background light better than has heretofore been thought. Additional experiments to determine the origin and relevance of this structure are therefore recommended.
We have observed laser-induced fluorescence using 456 nm laser radiation, resonant with the 6S1/2-7P3/2 transition in Cs atoms. It includes red emission lines in the range of 580-730 nm and a prominent line at 852 nm corresponding to the 6P3/2-6S1/2 transition. A T-shaped all-sapphire cell with a length of 1 cm, containing Cs atomic vapor and capable of being heated up to 500 oC, was used. The laser-induced fluorescence (LIF) power at 852 nm was investigated as a function of the cell temperature. The maximum LIF power was achieved at 130 oC, while a significant decrease was observed around 300 oC. At 130 oC, the Doppler-broadened LIF spectrum at 852 nm exhibited self-conversion, resulting in the formation of two distinct peaks within the spectrum. The LIF power at 852 nm was also studied as a function of the 456 nm radiation power. The Cs cell demonstrated potential as an efficient optical filter and down-converter, effectively transforming 456 nm radiation into 852 nm radiation.
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.
New experimental results and new phenomena related to the study of the retrofluorescence spectrum induced by a diode laser at the interface between glass and cesium vapor are presented. The Cs 62P3/2(Fe) hyperfine states are populated with a low-intensity tunable diode laser with a 10-MHz spectral bandwidth. We report an integrated atomic retrofluorescence spectrum in the 852.2-nm (62P3/2–62S1/2) resonance line and 917.2-nm (62D5/2–62P3/2) line generated by energy-pooling collisions. Emission spectra of the molecular fluorescence signal have been observed. At the resonance line a large proportion of the atoms excited by the laser are located in the vicinity of the surface. The interactions between the excited atomic 62P3/2 state and the surface appear as a spectral inhibition of the integrated retrofluorescence spectrum for both the atomic line and the molecular band. This spectral inhibition indicates that the nonradiative transformation process of changing atomically excited energy into thermal energy is preferred. We report the analysis of the dominant processes in the vicinity of the 852.2-nm resonance line, which can influence the retrofluorescence hyperfine spectrum at the boundary between the glass window and the saturated cesium vapor. Only the nonradiative transfer by evanescent waves toward the dissipative surface is retained. Using this mechanism, we formulate, for the first time to our knowledge, a simple model of a backscattered hyperfine fluorescence signal. The glass–vapor interface is considered as two distinct regions: a wavelength-thickness vapor layer joined to the surface and a more remote vapor region. The first region is analyzed as a spectral filter that annihilates the absorbed photons and the second one as a rich spectral light source. The experimental setup is described, and measured integrated retrofluorescence spectra are compared with predictions made by the model. The consistency between theory and experiment is remarkably good considering that the model depends only on two unknown parameters: the nonradiative transfer rate and the absorption shape line of the filtering region.
We have studied in detail the ionization and population of high-lying atomic states which occur in cesium vapor excited at the second resonance transition, 6S-7P. We have developed a simple model which qualitatively explains the laser-power dependences of level populations and electron densities which we observed. Measurements of spatial dependences of fluorescence point out the critical role of radiation trapping in these phenomena. Similar observations on rubidium demonstrate the same type of behavior when the first (5S-5P) or second (5S-6P) resonance is excited. At higher densities and temperatures we found that the fluorescence was dominated by diffuse molecular bands. Some of these bands probably consist of transitions to the repulsive $^{3}\mathrm{\ensuremath{\Sigma}}_{\mathrm{u}}^{+}$ state. Additionally four bands observed at 817.5, 826.6, 835.3, and 839.6 nm are tentatively identified as the cesium analog of the $^{3}\mathrm{\ensuremath{\Pi}}_{\mathrm{g}}$${\ensuremath{\rightarrow}}^{3}$${\mathrm{\ensuremath{\Sigma}}}_{\mathrm{u}}^{+}$ satellite bands which have previously been observed in the blue wing of the first resonance doublet of the lighter alkali metals.
Abstract Using laser radiation with a wavelength of 852 nm, which is in resonance with Cs atoms, the bright laser-induced fluorescence (LIF) on the blue lines of 456 and 459 nm (transitions 6S1/2 → 7P3/2 and 6S1/2 → 7 P1/2) was studied by the transition 6S1/2 → 6P3/2. A 1 cm long T-shaped sapphire cell containing Cs atomic vapors was used. The LIF power was investigated as a function of the cell temperature. A linear dependence of the LIF power on the pump radiation was observed. The LIF reached a maximum at 100°C. It is shown that the Cs cell can serve as an effective optical up-converter filter of radiation with a wavelength of 852 nm to radiation with a wavelength of 456 nm.
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.