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Chin. Phys.; (United States)

Separation of Li isotopes by laser defection of atomic beams

L. Li, Y. Wang, Minghui Li

Published Jan 1, 1983• 0 citations
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Abstract

Separation of Li isotopes by laser deflection of atomic beams has been carried out. An atomic beam apparatus with a collimating ratio of 450/1 generates are Li atomic beam of 10/sup 9/ atoms/cm/sup 3/ at the oven temperature of 600 /sup 0/C. The CW tunable dye laser crossing the atomic beam at a right angle has a linewidth of 6 MHz and its intensity as the I-cm interaction area is about 70 mW/cm/sup 2/. When the laser frequency is tuned to coincide with /sup 7/Li2/sup 2/P/sub 3/2/F = 3-2/sup 2/S/sub 1/2/ F = 2 transition, /sup 7/Li atoms are deflected from the beam. The deflected atoms are very pure /sup 7/Li and almost do not contain /sup 8/Li. When the laser frequency coincides with any other transition of 2/sup 2/P-2/sup 5/S of both /sup 5/Li and /sup 7/Li, no apparent deflection is observed because of the optical pumping of the hyperfine levels of the 2/sup 2/S/sub 1/2/ ground state.

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Bulletin of the American Physical Society•May 1, 1993•0 citations
Separation of Li isotopes by laser deflection of atomic beams has been carried out. An atomic beam apparatus with a collimating ratio of 450/1 generates are Li atomic beam of 10/sup 9/ atoms/cm/sup 3/ at the oven temperature of 600 /sup 0/C. The CW tunable dye laser crossing the atomic beam at a right angle has a linewidth of 6 MHz and its intensity as the I-cm interaction area is about 70 mW/cm/sup 2/. When the laser frequency is tuned to coincide with /sup 7/Li2/sup 2/P/sub 3/2/F = 3-2/sup 2/S/sub 1/2/ F = 2 transition, /sup 7/Li atoms are deflected from the beam. The deflected atoms are very pure /sup 7/Li and almost do not contain /sup 8/Li. When the laser frequency coincides with any other transition of 2/sup 2/P-2/sup 5/S of both /sup 5/Li and /sup 7/Li, no apparent deflection is observed because of the optical pumping of the hyperfine levels of the 2/sup 2/S/sub 1/2/ ground state.
The authors have succeeded in demonstrating laser isotope enrichment via magnetic deflection of a polarized atomic beam. By using a single dye laser with the frequency tuned to the two accidentally close transitions of the natural lithium (2 2 S 1/2 (F=1/2) to 2 2 P 3/2 for 6 Li and 2 2 S 1/2 (F=2) to 2 2 P 1 2/(F=1) for 7 Li), 6 Li and 7 Li atoms in a beam were positively and negatively polarized respectively. The 6 Li enrichment was achieved via magnetic deflection of the polarized beam through a hexapole magnet which focuses the positively polarized 6 Li atoms and defocuses the negatively polarized 7 Li atoms. The dependence of 7 Li polarization on laser intensity was experimentally examined, and the result was in good agreement with that calculated by rate equations. The abundance ratio of 6 Li to 7 Li was enhanced from 1 : 12.5 to about 1 : 3.1.
We deflected a well-collimated beam of krypton atoms in the metastable ls5 state by radiation pressure from a single-frequency dye laser. To produce the radiation pressure, we resonantly excited the krypton atoms, using the 1s5–2p9 transition. The natural width of this transition is much smaller than its isotope shift, which allowed us to deflect one isotope at a time. This created a new isotopically enriched atomic beam of Kr(1s5). We achieved a maximum enrichment factor of 1.2 × 104 at a deflection angle of 19 mrad. This enrichment is limited mainly by scattering of the parent atomic beam by residual gas. This degree of enrichment may make it possible to perform sensitive measurements of the concentrations of rare krypton isotopes in environmental samples.
Isotope separation by laser deflecting an atomic beam is analyzed theoretically. Interacting with a tilted one-dimensional optical molasses, an ytterbium atomic beam is split into multi-beams with different isotopes like 172 Yb, 173 Yb, and 174 Yb. By using the numerical calculation, the dependences of the splitting angle on the molasses laser intensity and detuning are studied, and the optimal parameters for the isotope separation are also investigated. Furthermore, the isotope separation efficiency and purity are estimated. Finally a new scheme for the efficient isotope separation is proposed. These findings will give a guideline for simply obtaining pure isotopes of various elements.
Isotopes of barium are selectively excited to a metastable state using a single ring dye laser. The excited atoms are then deflected out of an atomic beam by an inhomogeneous magnetic field. The deflection of the beam is studied using a hot wire detector and a quadrupole mass spectrometer. Measurements are presented showing that nearly all atoms of a particle isotope can be excited from the 6s{sup 2} ground still to the 6s5d state and subsequently spatially separated. This method of isotope separation requires metastable states having lifetimes greater than about 100 {mu}sec. These states can be readily excited from the ground state in atoms such as the Group II elements.
In studying ionization reactions in a single dense effusive beam of laser-excited Na(3p) atoms, we observe production of both Na{sub 2}{sup +} and Na{sup +} ions. The Na{sup +} results from the familiar associative ionization reaction of two Na(3p) atoms and the Na{sup +} ions under our conditions result mostly from the collisional dissociation of the Na{sub 2}{sup +} by reaction with a third excited Na(3p) atom, rather than from photo- dissociation or photoionization. A CW, single-frequency dye laser tuned to 589 nm resonantly excites the Na(3s) atoms to the 3p state. The atomic beam Na(3s) density is determined from low-intensity 589 absorption measurements. Na{sup +} ion yield depends on the cube of the Na beam density, suggesting successive collisions of three Na(3p) atoms: we believe the Na{sub 2}{sup +} ions polarize the third Na(3p) atom, resulting in a R{sup -4} orbiting collision interaction. A large collisional dissociation cross-section of approximately (4{plus_minus}2)x10{sup -13} cm{sup 2} results, for oven temperatures in the 500-600K range.