1996
DOI: 10.1016/0030-4018(96)00168-x
|View full text |Cite
|
Sign up to set email alerts
|

Efficient distortion-free amplification of 1.3 μm femtosecond pulses in a Pr3+-doped fluoride fiber amplifier

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...

Citation Types

0
2
0

Year Published

2001
2001
2021
2021

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 10 publications
(2 citation statements)
references
References 22 publications
0
2
0
Order By: Relevance
“…Although adiabatic amplif ication (small gain) gives high-quality pulses, the resulting energy gains are small and the amplif ier length must increase exponentially with input pulse width to satisfy the adiabatic condition. This diff iculty can be overcome by use of the chirped pulse amplification technique 5,6 in which f irst an input pulse is stretched by a dispersive delay line to ensure linear amplification and then the stretched and amplified pulse is recompressed through another delay line that has the opposite sign of dispersion. Because the nonlinearities in the amplif ier are suppressed, efficient and distortionless pulse amplif ication can be achieved.…”
mentioning
confidence: 99%
“…Although adiabatic amplif ication (small gain) gives high-quality pulses, the resulting energy gains are small and the amplif ier length must increase exponentially with input pulse width to satisfy the adiabatic condition. This diff iculty can be overcome by use of the chirped pulse amplification technique 5,6 in which f irst an input pulse is stretched by a dispersive delay line to ensure linear amplification and then the stretched and amplified pulse is recompressed through another delay line that has the opposite sign of dispersion. Because the nonlinearities in the amplif ier are suppressed, efficient and distortionless pulse amplif ication can be achieved.…”
mentioning
confidence: 99%
“…the resulting energy gains are small [5], [6] and the amplifier length must increase exponentially with the input pulsewidth in order to satisfy the adiabatic condition. The difficulty can be overcome using the chirped pulse amplification (CPA) technique [7]- [11] in which an input pulse is first stretched by a dispersive delay line to ensure "linear" amplification and then the stretched and amplified pulse is recompressed through another delay line having the opposite sign of dispersion. Since the nonlinearities in the amplifier are suppressed, efficient and distortionless amplification of femtosecond pulses can be achieved.…”
mentioning
confidence: 99%