[1] |
Goulielmakis E, Schultze M, Hofstetter M, et al. Single-cycle nonlinear optics [J]. Science, 2008, 320 (5883): 1614-1617.
|
[2] |
Feng L Q. Characteristics of high-order harmonic emission from He+ in bowtie-shaped metal nanostructure [J]. Chinese Journal of Quantum Electronics(量子电子学报), 2018, 35 (4): 479-485 (in Chinese).
|
[3] |
Liu H, Feng L Q. Theoretical investigation on harmonic emission and attosecond pulse generation from H2+ molecule under spatial inhomogeneous field [J]. Chinese Journal of Quantum Electronics(量子电子学报), 2017, 34 (2): 162-169 (in Chinese).
|
[4] |
Yang Y T, Qiao H X. Single short pulse generated by hydrogen atom exposed to the combined field of two laser pulses with similar frequency [J]. Chinese Journal of Quantum Electronics(量子电子学报), 2013, 30 (4): 405-410 (in Chinese).
|
[5] |
Corkum P B. Plasma perspective on strong field multiphoton ionization [J]. Physical Review Letters, 1993, 71 (13): 1994-1997.
|
[6] |
Zeng Z, Cheng Y, Song X, et al. Generation of an extreme ultraviolet supercontinuum in a two-color laser field [J]. Physical Review Letters, 2007, 98 (20): 203901.
|
[7] |
Takahashi E J, Lan P, Mücke O D, et al. Attosecond nonlinear optics using
|
|
gigawatt-scale isolated attosecond pulses [J]. Nature Communications, 2013, 4: 2691.
|
[8] |
Takahashi E J, Lan P, Mücke O D, et al. Infrared two-color multicycle laser
|
|
field synthesis for generating an intense attosecond pulse [J]. Physical Review Letters, 2010, 104:
|
|
233901.
|
[9] |
Wei P F, Miao J, Zeng Z N, et al. Selective enhancement of a single
|
|
harmonic emission in a driving laser field with subcycle waveform control [J]. Physical Review Letters,
|
|
2013, 110: 233903.
|
[10] |
Feng L Q, Chu T S. Generation of an isolated sub-40-as pulse using two-color laser pulses: Combined chirp effects [J]. Physical Review A, 2011, 84 (5): 053853.
|
[11] |
Chang Z H. Chirp of the single attosecond pulse generated by a polarization gating [J]. Physical Review A, 2005, 71 (2): 023813.
|
[12] |
Feng L Q, Liu H. Generation of the ultrabroad bandwidth with keV by three-color low intense mid-infrared inhomogeneous pulse [J]. Optics and Laser Technology, 2016, 81: 7-13.
|
[13] |
Feng L Q. Molecular harmonic extension and enhancement from H2+ ions in the presence of spatially inhomogeneous fields [J]. Physical Review A, 2015, 92 (5): 053832.
|
[14] |
Feng L Q, Li Y, Meng F S, et al. High-order harmonic and attosecond pulse generations
|
|
from Rydberg state driven by the spatially inhomogeneous field [J]. Modern Physics Letters B, 2017, 31 (4): 1750029.
|
[15] |
Feng L Q, Chu T S. Nuclear signatures on the molecular harmonic emission and the attosecond pulse generation [J]. Journal of Chemical Physics, 2012, 136 (5): 054102.
|
[16] |
Feng L Q, Chu T S. Intensity improvement in the attosecond pulse generation with the coherent superposition initial state [J]. Physics Letters A, 2012, 376: 1523-1530.
|
[17] |
Lu R F, Zhang P Y, Han K L. Attosecond-resolution quantum dynamics calculations for atoms and molecules in strong laser fields [J]. Physical Review E, 2008, 77 (6): 066701.
|
[18] |
Antoine P, Piraux B, Maquet A. Time profile of harmonics generated by a single atom in a strong electromagnetic field [J]. Physical Review A, 1995, 51 (3): R1750-R1753.
|
[19] |
Mairesse Y, Bohan A D, Frasinski L J, et al. Attosecond synchronization of high-harmonic soft x-rays
|
[J] |
Science, 2003, 302 (5650): 1540-1543.
|
[20] |
Jin C, Wang G L, Wei H, et al. Waveforms for optimal sub-keV high-order harmonics with
|
|
synthesized two- or three-colour laser fields [J]. Nature Communications, 2014, 5: 4003.
|