2001
DOI: 10.1364/ol.26.000465
|View full text |Cite
|
Sign up to set email alerts
|

High-efficiency, single-stage 7-kHz high-average-power ultrafast laser system

Abstract: We demonstrate a simple and practical single-stage ultrafast laser amplifier system that operates at a repetition frequency from 1 to 10 kHz, with millijoule pulse energy and as much as 13 W of average power. The repetition rate can be adjusted continuously from 1 to 10 kHz by new all-solid-state pump laser technology. This is to our knowledge the highest average power ever obtained from a single-stage ultrafast laser amplifier system. This laser will significantly increase the average power and the repetition… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
29
0

Year Published

2003
2003
2016
2016

Publication Types

Select...
5
3
1

Relationship

2
7

Authors

Journals

citations
Cited by 117 publications
(29 citation statements)
references
References 23 publications
0
29
0
Order By: Relevance
“…This experiment uses a Ti:sapphire ultrafast laser system producing pulses of energy of 3 mJ and 25-fs pulse duration at a repetition rate of 1 kHz and at a center wavelength of 790 nm (34,35). The pulse is split into pump and probe pulses, with the pump pulse focused onto an SF 6 gas jet at an incident intensity of Ϸ5 ϫ 10 13 W⅐cm Ϫ2 .…”
Section: Resultsmentioning
confidence: 99%
“…This experiment uses a Ti:sapphire ultrafast laser system producing pulses of energy of 3 mJ and 25-fs pulse duration at a repetition rate of 1 kHz and at a center wavelength of 790 nm (34,35). The pulse is split into pump and probe pulses, with the pump pulse focused onto an SF 6 gas jet at an incident intensity of Ϸ5 ϫ 10 13 W⅐cm Ϫ2 .…”
Section: Resultsmentioning
confidence: 99%
“…Important contributions to the success of these oscillators are their large optical bandwidth, leading to the direct generation of few-cycle pulses, and the excellent phase stability achievable with feed-back [4] and feed-forward stabilization schemes [5]. However, a major drawback of Ti:Sa amplifiers is the high thermal absorption and thermal lensing in the gain medium, which restricts the average powers to a few tens of Watts even with cryogenic cooling [6], thus limiting high-pulse-energy operation to repetition rates significantly lower than 1 MHz. Recently, Yb-based laser technology has rapidly progressed as a powerful competitor to the well-established Ti:Sa technology.…”
Section: Hz Tomentioning
confidence: 99%
“…The femtosecond transient absorption apparatus used a homebuilt ultrafast laser system based on the design of Backus et al 40 Briefly, 15-fs pulses were produced in a mode-locked Ti: sapphire oscillator (KMLabs TS pumped by 4.5 W, 532 nm output from a Spectra-Physics Millennia V laser). The pulse train was amplified using the chirped-pulse-amplification scheme at a repetition rate of 1 kHz.…”
Section: Experimental Techniquesmentioning
confidence: 99%
“…The pulse train was amplified using the chirped-pulse-amplification scheme at a repetition rate of 1 kHz. This was achieved in a home-built multipass Ti:sapphire amplifier 40 pumped by the 10-W, 527-nm output of a Spectra-Physics Evolution X laser. The resulting pulses had a pulse width of 70 fs and a pulse energy of 750 µJ and were centered at a wavelength of 800 nm (1.55 eV photon energy).…”
Section: Experimental Techniquesmentioning
confidence: 99%