High order harmonic spectra of CO under external electrostatic field

被引:1
|
作者
Lan Wan [1 ]
Chi Chen-Yang [1 ]
Guo Ying-Chun [1 ]
Yang Yu-Jun [2 ]
Wang Bing-Bing [3 ,4 ]
机构
[1] East China Normal Univ, Sch Phys & Elect Sci, Shanghai 200241, Peoples R China
[2] Jilin Univ, Inst Atom & Mol Phys, Changchun 130012, Peoples R China
[3] Chinese Acad Sci, Beijing Natl Lab Condensed Matter Phys, Inst Phys, Key Lab Opt Phys, Beijing 100190, Peoples R China
[4] Univ Chinese Acad Sci, Beijing 100049, Peoples R China
基金
中国国家自然科学基金;
关键词
high order harmonic spectra of CO; external static electric field; molecular orientation; double plateau structure; ATTOSECOND PULSE GENERATION; INTERFERENCE;
D O I
10.7498/aps.72.20230560
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
In this work, we use Lewenstein's theory to calculate the high order harmonic spectra of CO molecule in a linearly polarized laser field combined with an external electrostatic field. The results show that the characteristics of the high order harmonic spectra of CO molecule depend strongly on the direction of the external static electric field relative to the orientation of CO. Especially, when the direction of the external static electric field points from O to C, the plateau of the harmonic spectrum becomes wider and the cutoff frequency reaches a larger value than the scenario without external static electric field. When the direction of the external static electric field points from C to O, the harmonic spectrum shows a double-plateau structure. Using Lewenstein theory, these phenomena can be understood from the viewpoint that the harmonic generation comes from a coherent superposition of the contributions of two kinds of channels characterized by C-end ionization and O-end ionization. The C(O)-end ionization channel means that the electron is ionized from C(O) end, then accelerated by the driving electric field, finally recombines with its parent molecular ion at either C or O end, emitting the harmonics. For the same harmonic order, the contribution of the C-end ionization channel is greater than that of the the O-end ionization channel. The two kinds of channels emit harmonics in adjacent half period of laser, where the external static electric field causes the cutoff frequency of the harmonic spectrum to increase and decrease in the adjacent half period of the laser field. Especially, when the direction of external static electric field is from the C to O, the cutoff frequency of the harmonic spectrum of the C-end ionization channel decreases, resulting in a higher first plateau in the spectrum. While, the increase of cut-off frequency of the O-end ionization channel will result in a lower second plateau. When the direction of external static electric field is reversed, the cutoff frequency of the harmonics of the C-end channel increases, leading the plateau of CO harmonic spectrum to become wider than that without the external static electric field. The cut-off frequency of the O-end ionization channel decreases. Because the contribution of the O-end ionization channel can be ignored compared with that of C-end ionization channel, the C-end channel dominates the contribution to harmonic generation and hence there is only one plateau in the harmonic spectrum. This work provides a clear physical picture for the formation of a double-plateau structure of CO harmonic spectra under the action of an external static electric field.
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页数:8
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共 24 条
  • [1] Multielectron corrections in molecular high-order harmonic generation for different formulations of the strong-field approximation
    Augstein, B. B.
    Faria, C. Figueira de Morisson
    [J]. JOURNAL OF MODERN OPTICS, 2011, 58 (13) : 1173 - 1187
  • [2] Effect of the dynamic core-electron polarization of CO molecules on high-order harmonic generation
    Cam-Tu Le
    Van-Hung Hoang
    Lan-Phuong Tran
    Van-Hoang Le
    [J]. PHYSICAL REVIEW A, 2018, 97 (04)
  • [3] Effect of the carrier phase of ultra-short laser pulses on high-order harmonic generation spectra
    Chen Ji-Gen
    Chen Gao
    Zeng Si-Liang
    Yang Yu-Jun
    Zhu Qi-Ren
    [J]. ACTA PHYSICA SINICA, 2008, 57 (07) : 4104 - 4109
  • [4] Asymmetric Molecular Imaging through Decoding Odd-Even High-Order Harmonics
    Chen, Y. J.
    Fu, L. B.
    Liu, J.
    [J]. PHYSICAL REVIEW LETTERS, 2013, 111 (07)
  • [5] Control of quantum paths of high-order harmonics and attosecond pulse generation in the presence of a static electric field
    Hong, Weiyi
    Lu, Peixiang
    Cao, Wei
    Lan, Pengfei
    Wang, Xinlin
    [J]. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 2007, 40 (12) : 2321 - 2331
  • [6] Pure Even Harmonic Generation from Oriented CO in Linearly Polarized Laser Fields
    Hu, Hongtao
    Li, Na
    Liu, Peng
    Li, Ruxin
    Xu, Zhizhan
    [J]. PHYSICAL REVIEW LETTERS, 2017, 119 (17)
  • [7] High-order harmonic generation of CO and N2 molecules under linearly- and bi circularly-polarized laser pulses by TD-DFT
    Koushki, A. M.
    Sadighi-Bonabi, R.
    Mohsen-Nia, M.
    Irani, E.
    [J]. LASER PHYSICS, 2018, 28 (07)
  • [8] THEORY OF HIGH-HARMONIC GENERATION BY LOW-FREQUENCY LASER FIELDS
    LEWENSTEIN, M
    BALCOU, P
    IVANOV, MY
    LHUILLIER, A
    CORKUM, PB
    [J]. PHYSICAL REVIEW A, 1994, 49 (03): : 2117 - 2132
  • [9] Static field ionization rates for multi-electron atoms and small molecules
    Majety, Vinay Pramod
    Scrinzi, Armin
    [J]. JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 2015, 48 (24)
  • [10] Quantum Path Selection and Isolated-Attosecond-Pulse Generation of H2+ with an Intense Laser Pulse and a Static Field
    Miao Xiang-Yang
    Liu Sha-Sha
    [J]. CHINESE PHYSICS LETTERS, 2015, 32 (01)