Quartic phase compensation with a standard grating compressor
We demonstrate that, by changing the altitude and the azimuth incident angles on the gratings of the conventional grating-pair compressor used in chirped-pulse amplification, an extra degree of freedom is added. This results in a continuous adjustment of second-, third-, and fourth-order dispersions...
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todo:paper_01469592_v22_n15_p1186_GonzalezInchauspe2023-10-03T15:00:18Z Quartic phase compensation with a standard grating compressor González Inchauspe, C.M. Martínez, O.E. We demonstrate that, by changing the altitude and the azimuth incident angles on the gratings of the conventional grating-pair compressor used in chirped-pulse amplification, an extra degree of freedom is added. This results in a continuous adjustment of second-, third-, and fourth-order dispersions, which allows one to compensate for those dispersions that originated in the expansor or in the amplifier medium as a result of material dispersion or self-phase modulation, even with small out-of-plane tilts of the expansor and compressor. Analytical calculations of the high-order dispersions introduced by this compressor and examples for a pulse with a central wavelength at 800 nm are presented. © 1997 Optical Society of America. Fil:González Inchauspe, C.M. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Martínez, O.E. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_01469592_v22_n15_p1186_GonzalezInchauspe |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
We demonstrate that, by changing the altitude and the azimuth incident angles on the gratings of the conventional grating-pair compressor used in chirped-pulse amplification, an extra degree of freedom is added. This results in a continuous adjustment of second-, third-, and fourth-order dispersions, which allows one to compensate for those dispersions that originated in the expansor or in the amplifier medium as a result of material dispersion or self-phase modulation, even with small out-of-plane tilts of the expansor and compressor. Analytical calculations of the high-order dispersions introduced by this compressor and examples for a pulse with a central wavelength at 800 nm are presented. © 1997 Optical Society of America. |
format |
JOUR |
author |
González Inchauspe, C.M. Martínez, O.E. |
spellingShingle |
González Inchauspe, C.M. Martínez, O.E. Quartic phase compensation with a standard grating compressor |
author_facet |
González Inchauspe, C.M. Martínez, O.E. |
author_sort |
González Inchauspe, C.M. |
title |
Quartic phase compensation with a standard grating compressor |
title_short |
Quartic phase compensation with a standard grating compressor |
title_full |
Quartic phase compensation with a standard grating compressor |
title_fullStr |
Quartic phase compensation with a standard grating compressor |
title_full_unstemmed |
Quartic phase compensation with a standard grating compressor |
title_sort |
quartic phase compensation with a standard grating compressor |
url |
http://hdl.handle.net/20.500.12110/paper_01469592_v22_n15_p1186_GonzalezInchauspe |
work_keys_str_mv |
AT gonzalezinchauspecm quarticphasecompensationwithastandardgratingcompressor AT martinezoe quarticphasecompensationwithastandardgratingcompressor |
_version_ |
1782028091724398592 |