ionization yield
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Author(s):  
A. Selva ◽  
D. Bolst ◽  
S. Guatelli ◽  
V. Conte
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2021 ◽  
Vol 16 (07) ◽  
pp. P07053
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S.X. Wu ◽  
B.G. Lenardo ◽  
G. Gratta
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2020 ◽  
Vol 124 (1) ◽  
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R. M. Schwartz ◽  
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H. M. Milchberg

2019 ◽  
Vol 28 (8) ◽  
pp. 083201
Author(s):  
Hristina Delibašić ◽  
Violeta Petrović
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2017 ◽  
Vol 12 (05) ◽  
pp. C05010-C05010 ◽  
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A. Bondar ◽  
A. Buzulutskov ◽  
A. Dolgov ◽  
E. Grishnyaev ◽  
V. Nosov ◽  
...  

2016 ◽  
Vol 94 (12) ◽  
pp. 989-997 ◽  
Author(s):  
Qing Liao ◽  
Wen Li ◽  
H. Bernhard Schlegel

The angle dependence of strong field ionization has been studied for a set of molecules containing triple bonds: HCCH, HCN, HCC–CN, H2N–CCH, H2N–CN, and H2N–CC–CN. Time-dependent configuration interaction (TDCI) with a complex absorbing potential was used to model strong field ionization by a linearly polarized seven-cycle 800 nm cosine squared pulse. The ionization yields have been calculated as a function of the laser intensity and polarization direction and plotted as three-dimensional surfaces. At low field strengths, the angular dependence can be understood in terms of ionization from the highest occupied orbitals. At higher laser intensities, ionization occurs from lower lying orbitals as well as from the highest occupied orbitals, as indicated by changes in the angular dependence of the ionization yield and by variations in the population analysis of the TDCI wavefunction with the intensity of the laser field. The ionization yield for directions parallel to the molecular axis increases more rapidly than perpendicular to the axis as the conjugation length is increased. NH2 substitution substantially increases the ionization yield along the molecular axis but has only a small effect for perpendicular directions.


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