Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions

doi:10.1088/1674-1056/ab90ef

中国物理B ›› 2020, Vol. 29 ›› Issue (7): 73202-073202.doi: 10.1088/1674-1056/ab90ef

• ATOMIC AND MOLECULAR PHYSICS • 上一篇下一篇

Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions

Fengzheng Zhu(朱风筝), Genliang Li(黎根亮), Aihua Liu(刘爱华)

1 Institute of Atomic and Molecular Physics, Jilin University, Changchun 130012, China;
2 School of Mathematics and Physics, Hubei Polytechnic University, Huangshi 435003, China

收稿日期:2020-03-21 修回日期:2020-04-28 出版日期:2020-07-05 发布日期:2020-07-05
通讯作者: Aihua Liu E-mail:aihualiu@jlu.edu.cn
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 11774131 and 91850114).

Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions

Fengzheng Zhu(朱风筝)^1,2, Genliang Li(黎根亮)¹, Aihua Liu(刘爱华)¹

1 Institute of Atomic and Molecular Physics, Jilin University, Changchun 130012, China;
2 School of Mathematics and Physics, Hubei Polytechnic University, Huangshi 435003, China

Received:2020-03-21 Revised:2020-04-28 Online:2020-07-05 Published:2020-07-05
Contact: Aihua Liu E-mail:aihualiu@jlu.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 11774131 and 91850114).

摘要/Abstract

摘要： We investigate the intensity effect of ultrashort assisting infrared laser pulse on the single-XUV-photon double ionization of helium atoms by solving full six-dimensional time-dependent Schrödinger equation with implement of finite element discrete variable representation. The studies of joint energy distributions and joint angular distributions of the two photoelectrons reveal the competition for ionized probabilities between the photoelectrons with odd parity and photoelectrons with even parity in single-XUV-photon double ionization process in the presence of weak infrared laser field, and such a competition can be modulated by changing the intensity of the weak assisting-IR laser pulses. The emission angles of the two photoelectrons can be adjusted by changing the laser parameters as well. We depict how the assisting-IR laser field enhances and/or enables the back-to-back and side-by-side emission of photoelectrons created in double ionization process.

关键词: laser-assisted, double photoionization, helium atom, angular distribution

Abstract: We investigate the intensity effect of ultrashort assisting infrared laser pulse on the single-XUV-photon double ionization of helium atoms by solving full six-dimensional time-dependent Schrödinger equation with implement of finite element discrete variable representation. The studies of joint energy distributions and joint angular distributions of the two photoelectrons reveal the competition for ionized probabilities between the photoelectrons with odd parity and photoelectrons with even parity in single-XUV-photon double ionization process in the presence of weak infrared laser field, and such a competition can be modulated by changing the intensity of the weak assisting-IR laser pulses. The emission angles of the two photoelectrons can be adjusted by changing the laser parameters as well. We depict how the assisting-IR laser field enhances and/or enables the back-to-back and side-by-side emission of photoelectrons created in double ionization process.

Key words: laser-assisted, double photoionization, helium atom, angular distribution

中图分类号: (Photoionization and excitation)

32.80.-t

42.65.Re (Ultrafast processes; optical pulse generation and pulse compression) 87.64.mn (Multiphoton)

朱风筝, 黎根亮, 刘爱华. Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions[J]. 中国物理B, 2020, 29(7): 73202-073202.

Fengzheng Zhu(朱风筝), Genliang Li(黎根亮), Aihua Liu(刘爱华). Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions[J]. Chin. Phys. B, 2020, 29(7): 73202-073202.

参考文献 41

[1]	Bengtsson S and Mauritsson J 2019 J. Phys. B: At. Mol. Opt. Phys. 52 063002 doi: 10.1088/1361-6455/ab01c2
[2]	l'Huillier A, Lompre L, Mainfray G and Manus C 1982 Phys. Rev. Lett. 48 1814 doi: 10.1103/PhysRevLett.48.1814
[3]	Schwarzkopf O, Krässig B, Elmiger J and Schmidt V 1993 Phys. Rev. Lett. 70 3008 doi: 10.1103/PhysRevLett.70.3008
[4]	Feuerstein B, Moshammer R, Fischer D, Dorn A, Schröter C D, Deipenwisch J, Lopez-Urrutia J C, Höhr C, Neumayer P, Ullrich J et al. 2001 Phys. Rev. Lett. 87 043003 doi: 10.1103/PhysRevLett.87.043003
[5]	Maulbetsch F and Briggs J S 1993 J. Phys. B: At. Mol. Opt. Phys. 26 1679 doi: 10.1088/0953-4075/26/11/005
[6]	McCurdy C W, Baertschy M and Rescigno T N 2004 J. Phys. B: At. Mol. Opt. Phys. 37 R137
[7]	Avaldi L and Huetz A 2005 J. Phys. B: At. Mol. Opt. Phys. 38 S861
[8]	Emma P, Akre R, Arthur J, Bionta R, Bostedt C, Bozek J, Brachmann A, Bucksbaum P, Coffee R, Decker F J et al. 2010 Nat. Photon. 4 641 doi: 10.1038/nphoton.2010.176
[9]	Rosenblum S, Bechler O, Shomroni I, Lovsky Y, Guendelman G and Dayan B 2016 Nat. Photon. 10 19 doi: 10.1038/nphoton.2015.227
[10]	Shintake T, Tanaka H, Hara T et al. 2008 Nat. Photon. 2 555 doi: 10.1038/nphoton.2008.134
[11]	Lewenstein M, Balcou P, Ivanov M Y, L'Huillier A and Corkum P B 1994 Phys. Rev. A 49 2117 doi: 10.1103/PhysRevA.49.2117
[12]	Briggs J S and Schmidt V 2000 J. Phys. B: At. Mol. Opt. Phys. 33 R1
[13]	McPherson A, Gibson G, Jara H, Johann U, Luk T S, McIntyre I A, Boyer K and Rhodes C K 1987 J. Opt. Soc. Am. B 4 595 doi: 10.1364/JOSAB.4.000595
[14]	Hasegawa H, Takahashi E J, Nabekawa Y, Ishikawa K L and Midorikawa K 2005 Phys. Rev. A 71 023407 doi: 10.1103/PhysRevA.71.023407
[15]	Huetz A, Selles P, Waymel D and Mazeau J 1991 J. Phys. B At. Mol. Opt. Phys. 24 1917 doi: 10.1088/0953-4075/24/8/010
[16]	Wannier G H 1953 Phys. Rev. 90 817 doi: 10.1103/PhysRev.90.817
[17]	Palacios A, Rescigno T N and McCurdy C W 2008 Phys. Rev. A 77 032716 doi: 10.1103/PhysRevA.77.032716
[18]	Bräuning H, Dörner R, Cocke C L, Prior M H et al. 1998 J. Phys. B: At. Mol. Opt. Phys. 31 5149 doi: 10.1088/0953-4075/31/23/012
[19]	Ye D F, Liu X and Liu J 2008 Phys. Rev. Lett. 101 233003 doi: 10.1103/PhysRevLett.101.233003
[20]	Ho P J, Panfili R, Haan S L and Eberly J H 2005 Phys. Rev. Lett. 94 093002 doi: 10.1103/PhysRevLett.94.093002
[21]	Li Y, Xu J, Yu B and Wang X 2020 Opt. Express 28 7341 doi: 10.1364/OE.384819
[22]	Meyer M, Cubaynes D, Glijer D et al. 2008 Phys. Rev. Lett. 101 193002 doi: 10.1103/PhysRevLett.101.193002
[23]	Becker W, Grasbon F, Kopold R, Milošević D, Paulus G G and Walther H 2002 Adv. Atom. Mol. Opt. Phys. 48 35 doi: 10.1016/S1049-250X(02)80006-4
[24]	Pi L W and Starace A F 2014 Phys. Rev. A 90 023403 doi: 10.1103/PhysRevA.90.023403
[25]	Li J, Saydanzad E and Thumm U 2018 Phys. Rev. Lett. 120 223903 doi: 10.1103/PhysRevLett.120.223903
[26]	Kim I J, Kim C M, Kim H T, Lee G H, Lee Y S, Park J Y, Cho D J and Nam C H 2005 Phys. Rev. Lett. 94 243901 doi: 10.1103/PhysRevLett.94.243901
[27]	Wang J, Liu A and Yuan K J 2020 Opt. Commun. 460 125216 doi: 10.1016/j.optcom.2019.125216
[28]	Liao Q, Zhou Y, Huang C and Lu P 2012 New J. Phys. 14 013001 doi: 10.1088/1367-2630/14/1/013001
[29]	Zhang L, Xie X H, Roither S, Zhou Y M, Lu P X, Kartashov D, Schöffler M, Shafir D, Corkum P B, Baltuška A, Staudte A and Kitzler M 2014 Phys. Rev. Lett. 112 193002 doi: 10.1103/PhysRevLett.112.193002
[30]	Hu S X 2013 Phys. Rev. Lett. 111 123003 doi: 10.1103/PhysRevLett.111.123003
[31]	Rescigno T N and McCurdy C W 2000 Phys. Rev. A 62 032706 doi: 10.1103/PhysRevA.62.032706
[32]	Feist J, Nagele S, Pazourek R, Persson E, Schneider B, Collins L and Burgdörfer J 2008 Phys. Rev. A 77 043420 doi: 10.1103/PhysRevA.77.043420
[33]	Pazourek R, Feist J, Nagele S, Persson E, Schneider B, Collins L and Burgdörfer J 2011 Phys. Rev. A 83 053418 doi: 10.1103/PhysRevA.83.053418
[34]	Maulbetsch F and Briggs J S 1994 J. Phys. B: At. Mol. Opt. Phys. 27 4095 doi: 10.1088/0953-4075/27/18/009
[35]	Zhang Z, Peng L Y, Xu M H, Starace A F, Morishita T and Gong Q 2011 Phys. Rev. A 84 043409 doi: 10.1103/PhysRevA.84.043409
[36]	Liu A and Thumm U 2014 Phys. Rev. A 89 063423 doi: 10.1103/PhysRevA.89.063423
[37]	Jin F C, Li F, Yang Y J, Chen J, Liu X J and Wang B B 2018 J. Phys. B: At. Mol. Opt. Phys. 51 245601 doi: 10.1088/1361-6455/aaecdc
[38]	Jin F C, Tian Y Y, Chen J, Yang Y J, Liu X J, Yan Z C and Wang B B 2016 Phys. Rev. A 93 043417 doi: 10.1103/PhysRevA.93.043417
[39]	Hu S X 2010 Phys. Rev. E 81 056705 doi: 10.1103/PhysRevE.81.056705
[40]	Liu A and Thumm U 2015 Phys. Rev. A 91 043416 doi: 10.1103/PhysRevA.91.043416
[41]	Zhou S, Liu A, Liu F, Wang C and Ding D J 2019 Chin. Phys. B 28 083101 doi: 10.1088/1674-1056/28/8/083101

Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions

Laser-assisted XUV double ionization of helium atoms: Intensity dependence of joint angular distributions

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