TY - JOUR
T1 - Electron dynamics in CaB6 induced by one- and two-color femtosecond laser
AU - Jiao, Y. L.
AU - Wang, F.
AU - Hong, X. H.
AU - Su, W. Y.
AU - Chen, Q. H.
AU - Zhang, F. S.
PY - 2013/5/3
Y1 - 2013/5/3
N2 - We simulate nonlinear electron dynamics in CaB6 crystal within the framework of time-dependent density functional theory (TDDFT) under one-color femtosecond laser fields (400 nm, 800 nm) and two-color cases (400 nm+800 nm) with different relative phases of φ=0, φ=π/4, φ=π/2. The time-dependent Kohn-Sham equation (TDKS) is solved in real-time and real-space evolution scheme. We investigate the energy absorption and the electron excitation of CaB6 crystal in detail. Besides, the electron density distributions and occupations are shown after each external field ends. Computational results indicate that for one-color case, the excitation behaviors are distinct due to the different frequencies; for two-color laser, we adjust the phase and obtain the asymmetric field, which causes the change of the dynamics response comparing with the symmetric field. At the end of laser, the electron occupation is broadly distributed in the energy range of 2.4-42.4 eV, which means a high excitation rate in the narrow-gap semiconductor under intense laser field. The occurrence of the breakdown is also checked for each case in the Letter.
AB - We simulate nonlinear electron dynamics in CaB6 crystal within the framework of time-dependent density functional theory (TDDFT) under one-color femtosecond laser fields (400 nm, 800 nm) and two-color cases (400 nm+800 nm) with different relative phases of φ=0, φ=π/4, φ=π/2. The time-dependent Kohn-Sham equation (TDKS) is solved in real-time and real-space evolution scheme. We investigate the energy absorption and the electron excitation of CaB6 crystal in detail. Besides, the electron density distributions and occupations are shown after each external field ends. Computational results indicate that for one-color case, the excitation behaviors are distinct due to the different frequencies; for two-color laser, we adjust the phase and obtain the asymmetric field, which causes the change of the dynamics response comparing with the symmetric field. At the end of laser, the electron occupation is broadly distributed in the energy range of 2.4-42.4 eV, which means a high excitation rate in the narrow-gap semiconductor under intense laser field. The occurrence of the breakdown is also checked for each case in the Letter.
UR - http://www.scopus.com/inward/record.url?scp=84874313746&partnerID=8YFLogxK
U2 - 10.1016/j.physleta.2013.02.002
DO - 10.1016/j.physleta.2013.02.002
M3 - Article
AN - SCOPUS:84874313746
SN - 0375-9601
VL - 377
SP - 823
EP - 827
JO - Physics Letters, Section A: General, Atomic and Solid State Physics
JF - Physics Letters, Section A: General, Atomic and Solid State Physics
IS - 12
ER -