Abstract Selective photoionization of ytterbium isotope is studied numerically based on a three-step photoionization scheme, 46S (0 cm) 466pP (17992.008 cm) (466p) (7/2, 3/2) (35196.98 cm) auto-ionization state (52353 cm) Yb, by the density matrix theory with the consideration of atomic hyperfine structures and magnetic sublevels. To examine the physical model, the numerical isotopic abundance of ytterbium is compared with that from mass spectroscopy experiment, showing that they are in good agreement with each other. The excitation process and ionization process of ytterbium, especially for odd isotopes, are discussed and analyzed in detail on this basis. The effects of frequency detuning, power densities, spectral bandwidths, polarization of two excitation lasers, and atomic Doppler broadening on the total ionization yield and isotopic abundance are investigated numerically and the optimal excitation conditions for Yb enrichment are identified semi-quantitatively.
(Strong-field excitation of optical transitions in quantum systems; multiphoton processes; dynamic Stark shift)
Corresponding Authors:
Xiao-Yong Lu
E-mail: lu-xy15@tsinghua.org.cn
Cite this article:
Xiao-Yong Lu(卢肖勇) and Li-De Wang(王立德) Numerical studies of isotopic selective photoionization of ytterbium in a three-step ionization scheme 2023 Chin. Phys. B 32 053204
[1] Chellan P and Sadler P J 2015 Phil. Trans. R. Soc. A373 20140182 [2] Yakovlenko S I 1999 Russ. Phys. J.42 732 [3] Babichev A P, Grigoriev I S and Grigoriev A I 2005 Quantum Electron35 879 [4] Yamabayashi H 1994 Radioisotopes43 296 [5] D'yachkov A B, Gorkunov A A and Labozin A V 2018 Opt. Spectrosc124 13 [6] Cutler C S, Smith C J and Ehrhardt G J 2000 Cancer Biother. Radio.15 531 [7] Fricker S P 2006 Chem. Soc. Rev.35 524 [8] Kostelnik T I and Orvig C 2019 Chem. Rev.119 902 [9] Dash A, Raghavan M and Pillai A 2015 Nucl. Med. Mol. Imaging49 85 [10] Banerjee S, Pillai M R A and Knapp F F 2015 Chem. Rev.115 2934 [11] Suryanarayana M V and Sankari M 2021 J. Opt. Soc. Am. B38 3331 [12] Suryanarayana M V 2021 J. Opt. Soc. Am. B38 353 [13] Vogel W V, Marck S C and Versleijen M W J 2021 Eur. J. Nucl. Med. Mol. Imaging.48 2329 [14] Borisov S K, Kuz'mina M A and Mishin V A 1996 Russ. Laser Res.17 332 [15] Yakovlenko S I 1998 Quantum Electron28 945 [16] Andreev O I, Derzhiev V I and Dyakin V M 2006 Quantum Electron36 84 [17] Park H, Kwon D H and Cha Y H 2008 J. Nucl. Sci. Technol. Supplement6 111 [18] Park H, Kwon D H and Cha Y H 2006 J. Korean Phys. Soc.49 382 [19] Rabi I I 1937 Phys. Rev.51 652 [20] Demtröder W 2008 Laser Spectroscopy Vol. 1 Basic Principles, 4th edn. (Berlin, Heidelberg: Springer-Verlag) [21] Greenland P T 1990 Contemp. Phys.31 405 [22] Sankari M, Kumar P and Suryanarayana M 2008 J. Opt. Soc. Am. B25 1820 [23] Krynetskii B B, Mishin V A and Prokhorov A M 1991 J. Appl. Spectrosc.54 338 [24] Park H, Kostritsa S and Kwon D 2002 J. Korean Phys. Soc.41 322 [25] Lu X Y, Wang L D and Li Y F 2022 Chin. Phys. B31 063203 [26] Sahoo A C, Mandal P K and Shah M L 2017 J. Phys. Commun.1 055010
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.