2020
DOI: 10.1088/1361-6455/aba127
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Tunable, few-cycle, CEP-stable mid-IR optical parametric amplifier for strong field applications

Abstract: We present a robust, three-stage optical parametric amplifier driven by a Ti:Sapphire ultrafast laser system that implements passive carrier-envelope phase stabilization and directly generates five-cycle mid-IR pulses by dispersion compensation. The source is based on potassium titanyl arsenate crystals and exploits intra-pulse difference-frequency seed generation in the mid-IR. This source will be particularly suited for applications in strong-field physics, such as high order harmonic generation and photoele… Show more

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Cited by 19 publications
(9 citation statements)
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“…Another novel scheme to note is carrier–envelope-phase stable difference-frequency generation and optical parametric amplification technology [162] , which generates phase-locked multi-THz (10–30 THz) radiation with strong intensity [163166] . The same technique is now being expanded to the mid-IR frequency range [167,168] , dramatically enhancing the capability of quantum control of the lattice sector of quantum materials.…”
Section: Background Knowledgementioning
confidence: 99%
“…Another novel scheme to note is carrier–envelope-phase stable difference-frequency generation and optical parametric amplification technology [162] , which generates phase-locked multi-THz (10–30 THz) radiation with strong intensity [163166] . The same technique is now being expanded to the mid-IR frequency range [167,168] , dramatically enhancing the capability of quantum control of the lattice sector of quantum materials.…”
Section: Background Knowledgementioning
confidence: 99%
“…In our experiment, the FID of methane was driven by the high energy mid-IR KTA-based OPA source presented in a previous paper [25], pumped by a commercial 800 nm chirped-pulse amplified Ti:Sapphire laser system at 1 kHz repetition rate (Amplitude, Aurora). The output pulses from the OPA are tunable between 2.4 and 3.9 µm, with a maximum energy content of 300 µJ and a minimum duration of 60 fs after dispersion compensation (five optical cycles at 3.4 µm).…”
Section: Time-domain Spectroscopy Through Broadband Fwmmentioning
confidence: 99%
“…Recently, thanks to technological advances, high-energy ultrafast sources in the mid-IR (3-10 µm) based on optical parametric amplification (OPA) or optical parametric chirped pulse amplification have become available [23][24][25][26]. These sources grant the opportunity to explore the excitation of molecular vibrations with unprecedented field strength.…”
Section: Introductionmentioning
confidence: 99%
“…This paper is devoted to investigating the HHG during the interaction of the femtosecond laser field with oriented asymmetric diatomic molecules in the presence of an external static electric field. The relevance of these studies is associated with the development of powerful sources of pulsed low-frequency terahertz (THz) and mid-infrared (mid-IR) radiation, capable to influence the HHG by infrared laser pulses [4][5][6][7][8]. Our numerical study is based on the solution of the three-dimensional time-dependent Schrödinger equation (3D TDSE) for the model oneelectron system, whose parameters are adjusted to simulate a carbon monoxide (CO) molecule.…”
Section: Introductionmentioning
confidence: 99%