• Acta Optica Sinica
  • Vol. 38, Issue 7, 0702002 (2018)
bin Zhu1, Guoli Wang1、*, Xiaoyong Li2, and Xiaoxin Zhou1
Author Affiliations
  • 1 College of Physics and Electronic Engineering, Northwest Normal University, Lanzhou, Gansu 730070, China
  • 2 Experimental Center, Northwest Minzu University, Lanzhou, Gansu 730030, China
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    DOI: 10.3788/AOS201838.0702002 Cite this Article Set citation alerts
    bin Zhu, Guoli Wang, Xiaoyong Li, Xiaoxin Zhou. Control and Preparation of Low Excited States of He Atoms Interacted with Strong Laser Field[J]. Acta Optica Sinica, 2018, 38(7): 0702002 Copy Citation Text show less
    Energy levels and preparation scheme of low excited states (n≤3) of He atoms
    Fig. 1. Energy levels and preparation scheme of low excited states (n≤3) of He atoms
    Population transfer from 1s ground state to 2p excited state of He atoms under different laser peak intensities. (a) 4.50×1013 W?cm-2; (b) 8.20×1013 W?cm-2; (c) 1.63×1014 W?cm-2; (d) 3.20×1014 W?cm-2
    Fig. 2. Population transfer from 1s ground state to 2p excited state of He atoms under different laser peak intensities. (a) 4.50×1013 W?cm-2; (b) 8.20×1013 W?cm-2; (c) 1.63×1014 W?cm-2; (d) 3.20×1014 W?cm-2
    Population transfer from 1s ground state to 3p excited state of He atoms under different laser peak intensities. (a) 9.96×1013 W?cm-2; (b) 3.80×1014 W?cm-2
    Fig. 3. Population transfer from 1s ground state to 3p excited state of He atoms under different laser peak intensities. (a) 9.96×1013 W?cm-2; (b) 3.80×1014 W?cm-2
    Population transfer from 2p state to 2s state of He atoms under different laser peak intensities. (a) 7.70×109 W?cm-2; (b) 3.10×1010 W?cm-2
    Fig. 4. Population transfer from 2p state to 2s state of He atoms under different laser peak intensities. (a) 7.70×109 W?cm-2; (b) 3.10×1010 W?cm-2
    Population transfers from 1s ground state to 3s and 3p excited states of He atoms under different laser peak intensities. (a) 2.10×1011 W?cm-2; (b) 4.00×1011 W?cm-2
    Fig. 5. Population transfers from 1s ground state to 3s and 3p excited states of He atoms under different laser peak intensities. (a) 2.10×1011 W?cm-2; (b) 4.00×1011 W?cm-2
    (a) Wavefunctions of 1s ground and 2p excited states of He atoms; (b) time evolution of electron wavepacket along z axis in a laser field; (c) adopted laser field
    Fig. 6. (a) Wavefunctions of 1s ground and 2p excited states of He atoms; (b) time evolution of electron wavepacket along z axis in a laser field; (c) adopted laser field
    Initial stateLaser intensity /(W∙cm-2)Laser wavelength/nmPulse duration/cycleFinal state(atomic population)
    1s4.50×101358.1401s (70%)+2p (30%)
    1s8.20×101358.1401s (50%)+2p (50%)
    1s1.63×101458.1401s (20%)+2p (80%)
    1s3.20×101458.1402p (100%)
    1s9.96×101353.5801s (50%)+3p (50%)
    1s3.80×101453.5803p (100%)
    2p7.70×1092064.082p (50%)+2s (50%)
    2p3.10×10102064.082s(100%)
    2p2.10×1011715.0243s (80%)+3d (4%)
    2p4.00×1011652.883s (7%)+3d (86%)
    Table 1. Laser pulse parameters for transferring atomic populations from ground state to specific excited states of He atoms
    bin Zhu, Guoli Wang, Xiaoyong Li, Xiaoxin Zhou. Control and Preparation of Low Excited States of He Atoms Interacted with Strong Laser Field[J]. Acta Optica Sinica, 2018, 38(7): 0702002
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