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Journal of Experimental and Theoretical Physics

Ionization detection of single atoms by laser radiation using Rydberg states

G. I. Bekov, Vladilen S Letokhov, Oleg I. Matveev, V.I. Mishin

Published Dec 1, 1978• 4 citations
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Time-dependent registration of ionization current for spectroscopy of rydberg atoms

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Spectroscopy of atoms in Rydberg states was an object of extensive investigation (see for example [1-5] and references therein). Usually necessary population of Rydberg states is achieved by means of multi-stage pulse laser pumping. That is why useful signal of ionization current from Single Channel Electron Multiplier (CEM or channeltron) is also pulse signal. Essential temporal instability of this signal is one of the main problems during its registration. More over in order to investigate Rydberg spectra of elements with high value of ionization potential (Al, Cu, Au etc.) it is necessary to apply high-temperature source of atoms (up to 2000 3000K). That is why there appears effect of redistribution of population by means of black body radiation. This effect makes additional difficulties to study ionization spectra. In order to overcome these obstacles we propose to apply time-dependent registration of ionization current from CEM. First of all such approach will allow us to store individual time-dependent realizations and to provide averaging of these realizations numerically excluding temporal instability. In addition after improvement of the receiving system it will be possible to detect ionization spectra resolving Rydberg states populated by means of black body radiation.

International Kharkiv Symposium on Physics and Engineering of Microwaves, Millimeter and Submillimeter Waves•Jun 1, 2010•0 citations
This review deals with the problem of selective detection of single atoms by laser radiaton. It begins with a classification of the detection methods (fluorescence, photoionization, deflection), discusses detection conditions (atomic vapor, atomic beam, buffer gas), and gives estimates of the parameters of laser radiation ensuring effective detection. Next, a detailed comparision is made of each of the detection methods. It is shown that in the fluorescence method the maximum efficiency of the detection process is achieved for cyclic interaction of atoms with laser radiation. In the photoionization method the most suitable technique is multistage photoionization of atoms by laser radiation. The highest ionization selectivity and a high efficiency are obtained by multistage excitation of an atom either to a Rydberg state followed by ionization with an electric field pulse or to a narrow autoionizing state with a large excitation cross section. Both these techniques are considered from the point of view of the sources of background and ways of discriminating against it, detection selectivity, and absolute sensitivity; the experimental results are analyzed. In discussing the deflection method consideration is given to deflection of an atom in a magnetic field after excitation with laser radiation and to deflection of atoms by resonant optical pressure. The review concludes with a brief discussion of the prospective applications of these detection methods in nuclear physics, atomic physics, and chemistry.
Spectroscopy of atoms in Rydberg states was an object of extensive investigation (see for example [1-5] and references therein). Usually necessary population of Rydberg states is achieved by means of multi-stage pulse laser pumping. That is why useful signal of ionization current from Single Channel Electron Multiplier (CEM or channeltron) is also pulse signal. Essential temporal instability of this signal is one of the main problems during its registration. More over in order to investigate Rydberg spectra of elements with high value of ionization potential (Al, Cu, Au etc.) it is necessary to apply high-temperature source of atoms (up to 2000 3000K). That is why there appears effect of redistribution of population by means of black body radiation. This effect makes additional difficulties to study ionization spectra. In order to overcome these obstacles we propose to apply time-dependent registration of ionization current from CEM. First of all such approach will allow us to store individual time-dependent realizations and to provide averaging of these realizations numerically excluding temporal instability. In addition after improvement of the receiving system it will be possible to detect ionization spectra resolving Rydberg states populated by means of black body radiation.