Carrier-envelope phase-stabilized amplifier system
✍ Scribed by J. Rauschenberger; T. Fuji; M. Hentschel; A.-J. Verhoef; T. Udem; C. Gohle; T. W. Hänsch; F. Krausz
- Publisher
- John Wiley and Sons
- Year
- 2006
- Tongue
- English
- Weight
- 278 KB
- Volume
- 3
- Category
- Article
- ISSN
- 1612-2011
No coin nor oath required. For personal study only.
✦ Synopsis
We demonstrate a novel scheme for carrier-envelope (CE)
phase stabilization of few-cycle laser pulses from a mode-locked
oscillator. Our scheme utilizes a monolithic, collinear geometry
which obviates the need for splitting the laser output, where a
fraction is used for CE-phase control and the remainder used for
experiment. Rather than using a microstructured fiber and
frequency-doubling crystal to generate the beating signal needed
for CE-phase locking, in our scheme self-phase modulation and
difference-frequency generation occur simultaneously in a single
periodically poled lithium niobate (PPLN) crystal and are used to
generate equivalent signals. Direct phase-locking and
recompression of the output is enabled because the PPLN crystal
transmits the majority of the incident fundamental relatively
unaffected. As a result, the output provides few-cycle pulses with
an unprecedented degree of short- and long-term reproducibility of
the electric field waveform. These unique features, along with the
simplicity of the scheme make it perfectly suitable for use in
seeding CE-phase stabilized amplified laser systems. Results from
a 3 kHz amplified Ti:sapphire system will be presented that
validate our assertions.
📜 SIMILAR VOLUMES
The shape of the field of a few-cycle laser pulse strongly depends on the carrier-envelope phase. For a circularly polarized few-cycle pulse, this phase is correlated with a direction in space. Superposition of two counterrotating circularly polarized few-cycle pulses yields a linearly polarized pul
## Abstract A nonlinear model of the power amplifier in a multi‐carrier transmission system is discussed. It is emphasized that when the amplifier is driven by a signal with a large dynamic range, the third‐order model of its nonlinearity may be invalid. Taking into account high order components of
## Abstract This paper derives the conditions to be satisfied by the amplifier in each stage of a multistage amplifier in order for it to be absolutely stable. It is shown that the stability factor __K__ of each stage need not be larger than unity except for the initial and last stages. By means of