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Soviet Journal of Quantum Electronics

Laser detection of rare radioactive isotopes. Selective enrichment of the initial state

Alexander A. Makarov

Published Jun 30, 1983• 2 citations
Publisher

Abstract

An investigation is made of the enrichment of the initial state with atoms or ions of rare radioactive isotopes by using cw laser radiation. Estimates of the enrichment of metastable levels are obtained for 14C and 26Al atoms and 41Ca+ ions. The radioactive isotope 14C is used as an example to discuss the combination of enrichment of the initial state with multistage selective photoionization of atoms. It is shown that in this case, it is realistic to expect a selectivity higher than 1020.

DOI
10.1070/qe1983v013n06abeh004277

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An investigation is made of the enrichment of the initial state with atoms or ions of rare radioactive isotopes by using cw laser radiation. Estimates of the enrichment of metastable levels are obtained for 14C and 26Al atoms and 41Ca+ ions. The radioactive isotope 14C is used as an example to discuss the combination of enrichment of the initial state with multistage selective photoionization of atoms. It is shown that in this case, it is realistic to expect a selectivity higher than 1020.
We consider a gas of two-level atoms of two species (for example, natural Rb vapor consisting of two isotopes) in the field of laser radiation tuned close to resonance with the certain transition of a specific iostope. This radiation may turn to be rather close to a near lying transition of other isotope (within the linewidth of laser radiation), so it is necessary to take into account the possibility of excitation of other isotope in order to evaluate the enrichment degree if it is aimed at the isotope separation by means of selective excitation with subsequent chemcial reaction (in our example the rubidium hydride formation) of the excited isotope which is believed to take place at a rate much higher than that in the ground state of the atom.
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.
We present studies of resonance-enhanced photoionization for isotope-selective loading of Ca+{\mathrm{Ca}}^{+}Ca+ into a Paul trap. The ${4s}^{2}{}^{1}{S}_{0}\ensuremath{\leftrightarrow}4s4p{}^{1}{P}_{1}$ transition of neutral calcium is driven by a 423 nm laser and the atoms are photoionized by a second laser at 389 nm. Isotope selectivity is achieved by using crossed atomic and laser beams to reduce the Doppler width significantly below the isotope shifts in the 423 nm transition. The loading rate of ions into the trap is studied under a range of experimental parameters for the abundant isotope 40Ca+.{}^{40}{\mathrm{Ca}}^{+}.40Ca+. Using the fluorescence of the atomic beam at 423 nm as a measure of the Ca number density, we estimate a lower limit for the absolute photoionization cross section of 170(60) Mb. We achieve loading and laser cooling of all the naturally occurring isotopes, without the need for enriched sources. Laser heating/cooling is observed to enhance the isotope selectivity. In the case of the rare species 43Ca+{}^{43}{\mathrm{Ca}}^{+}43Ca+ and 46Ca+,{}^{46}{\mathrm{Ca}}^{+},46Ca+, which have not previously been laser cooled, the loading is not fully isotope selective, but we show that pure crystals of 43Ca+{}^{43}{\mathrm{Ca}}^{+}43Ca+ may nevertheless be obtained. We find that for loading 40Ca+{}^{40}{\mathrm{Ca}}^{+}40Ca+ the 389 nm laser may be replaced by an incoherent source.
We demonstrate an experimental technique that selects the nuclear spin I=0 isotope 138Ba^{138}\mathrm{Ba}138Ba for spectroscopic measurements from a beam of natural barium containing seven stable isotopes. A cw dye laser is used to optically pump the I=3/2 isotopes 135Ba^{135}\mathrm{Ba}135Ba and 137Ba^{137}\mathrm{Ba}137Ba into the metastable 6s5d 1^{1}1D2{\mathit{D}}_{2}D2​ and 3^{3}3D1,2{\mathit{D}}_{1,2}D1,2​ levels via the 6s6p 1^{1}1P1{\mathit{P}}_{1}P1​ excited state, leaving nearly pure 138Ba^{138}\mathrm{Ba}138Ba in the ground state. Photoionization spectra of the excited 5d6p 3^{3}3D1{\mathit{D}}_{1}D1​ even isotope state recorded with optical pumping of 135Ba^{135}\mathrm{Ba}135Ba and 137Ba^{137}\mathrm{Ba}137Ba to the metastable levels are essentially devoid of forbidden features associated with the hyperfine interaction in the odd isotopes.
Analytical solutions of the Schr?dinger equations for coherent excitation of an atom in the scheme of two- and three-stage photoionization are obtained as applied to the problem of laser isotope separation. A feature of the study is the introduction of laser excitation from an additional initial state to increase the fraction of the atoms involved in the separation process. The optimal from the points of view of photoion ratios of radiation intensities at individual photoionization stages are found. Key words: laser photoionization, laser isotope separation.