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Physica Scripta

Numerical study of multi-step photoionization of gadolinium-160 based on a polarization ionization path developed for odd gadolinium isotopes

Lide Wang, Junyao Zhang, X. X. Lu

Published Jun 16, 2026• 0 citations
Publisher

Abstract

Abstract The enriched 160 Gd isotope is an important target nucleus for the production of the next-generation β -emitting therapeutic nuclide 161 Tb. To address the limitation that the J = 2 → 2 → 1 → 0 polarization ionization path, although suitable for separating odd Gd isotopes with parallel linearly polarized lasers, cannot be used to enrich even Gd isotopes, we propose an efficient and highly selective ionization scheme for 160 Gd. Based on the density matrix theory, a general four-color, three-step ionization model was established by taking into account magnetic sublevel degeneracy and hyperfine structure. Numerical calculations of photoionization dynamics were performed to optimize laser parameters such as polarization, power density, and frequency detuning, with the aim of enhancing the ionization yield and isotopic abundance of 160 Gd. The results show that, in the absence of Doppler broadening, the ionization yield obtained with orthogonal linear polarization is higher than that obtained with parallel linear polarization in both three-color, three-step and four-color, three-step schemes. To maximize ionization yield, resonant excitation is required in the three-color, three-step scheme, whereas detuned excitation is needed in the four-color, three-step schemes to mitigate the population trapping effect. When Doppler broadening is taken into account, the selective photoionization performance depends on the residual Doppler broadening and on the number of laser beams passing through the atomic vapor. The calculations indicate that the optimal ionization scheme, namely the four-color, three-step scheme with parallel linear polarization, detuned excitation, saturation power density, and a bandwidth of 0.5 GHz, can achieve a 160 Gd abundance exceeding 98% at a residual Doppler broadening of 0.45 GHz, thereby meeting the application requirements.

DOI
10.1088/1402-4896/ae7e5e

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Abstract The enriched 160 Gd isotope is an important target nucleus for the production of the next-generation β -emitting therapeutic nuclide 161 Tb. To address the limitation that the J = 2 → 2 → 1 → 0 polarization ionization path, although suitable for separating odd Gd isotopes with parallel linearly polarized lasers, cannot be used to enrich even Gd isotopes, we propose an efficient and highly selective ionization scheme for 160 Gd. Based on the density matrix theory, a general four-color, three-step ionization model was established by taking into account magnetic sublevel degeneracy and hyperfine structure. Numerical calculations of photoionization dynamics were performed to optimize laser parameters such as polarization, power density, and frequency detuning, with the aim of enhancing the ionization yield and isotopic abundance of 160 Gd. The results show that, in the absence of Doppler broadening, the ionization yield obtained with orthogonal linear polarization is higher than that obtained with parallel linear polarization in both three-color, three-step and four-color, three-step schemes. To maximize ionization yield, resonant excitation is required in the three-color, three-step scheme, whereas detuned excitation is needed in the four-color, three-step schemes to mitigate the population trapping effect. When Doppler broadening is taken into account, the selective photoionization performance depends on the residual Doppler broadening and on the number of laser beams passing through the atomic vapor. The calculations indicate that the optimal ionization scheme, namely the four-color, three-step scheme with parallel linear polarization, detuned excitation, saturation power density, and a bandwidth of 0.5 GHz, can achieve a 160 Gd abundance exceeding 98% at a residual Doppler broadening of 0.45 GHz, thereby meeting the application requirements.
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Photoexcitation and photoionization of atoms, the central part of atom vapor laser isotope separation (AVLIS), relate to the ionization yield and isotope selectivity directly. Doppler broadening of absorption lines is one of the parameters that influence the photoexcitation and photoionization process of atoms. When evaporation temperature is high or beam equipment is absent, Doppler broadening has obvious influence on the ionization yield because most of atoms are non-resonantly excited. In this paper, we study the influences of Doppler broadening of absorption lines on a multi-step photoexcitation and photoionization process of atoms according to the facts of AVLIS. A Doppler-broadened three-level atom system with two resonant lasers is investigated. The interaction between laser field and atoms is described by a density matrix, which is calculated by fourth-order Runge-Kutta numerical method with variable steps. The results show that the ionization yield of atoms decreases with the increase of Doppler broadening of absorption lines under the same laser parameters. At a constant laser power, the ionization yield reaches its maximum value at the best laser bandwidths, which is different from that obtained without Doppler broadening, as reported in published papers. Meanwhile, the best laser bandwidth increases with the increase of Rabi frequency and Doppler broadening when other parameters are constant. Moreover, the best bandwidth of the second laser is smaller than that of the first laser in a multi-step photoionization process of atoms. Therefore, lasers should work at the best bandwidths in AVLIS for highest ionization yield. It is advantageous to make laser bandwidths slightly bigger than the best bandwidths technically for smaller fluctuation of ionization yield, owing to incoercible stochastic volatility in laser bandwidths. The ionization yield increases with the decrease of Doppler broadening, especially at the best laser bandwidths. Therefore, it is necessary to reduce Doppler broadening of atom vapor in laser ionization zone.
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