Generation and Characterization of Phase-Stable Sub-Single-Cycle Pulses at 3000 cm

This paper summarizes the generation of sub-single-cycle infrared (IR) pulses through a laser filament and the detailed properties of the generated pulses. The fundamental (ω 1 ) and second harmonic (ω 2 ) of 30-fs Ti:sapphire amplifier output were focused into nitrogen gas and produced phase-stable...

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Veröffentlicht in:IEEE journal of selected topics in quantum electronics 2015-09, Vol.21 (5), p.1-12
Hauptverfasser: Fuji, Takao, Nomura, Yutaka, Shirai, Hideto
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Shirai, Hideto
description This paper summarizes the generation of sub-single-cycle infrared (IR) pulses through a laser filament and the detailed properties of the generated pulses. The fundamental (ω 1 ) and second harmonic (ω 2 ) of 30-fs Ti:sapphire amplifier output were focused into nitrogen gas and produced phase-stable broadband IR pulses (ω 0 ) by four-wave difference frequency generation (ω 1 + ω 1 - ω 2 → ω 0 ) through filamentation. The spectrum spread from 200 to 5500 cm -1 , corresponding to ~3.5 octaves. The waveform of the sub-single-cycle pulse was completely characterized with the frequency-resolved optical gating capable of a carrier-envelope phase determination. The pulse duration was measured as 6.9 fs, which was 0.63 times the period of the carrier frequency, 3000 cm -1 . The carrier-envelope phase of the IR pulse was passively stabilized, and the instability of the phase was estimated as 154-mrad rms over 2.5 h. We also summarize a particular behavior of the spectral phase of the sub-single-cycle pulse; the phase of high-frequency components of the generated pulses changes continuously and linearly with the relative phase between the two-color input pulses, whereas the phase of the low-frequency components takes only two discrete values. The phase behavior is a unique feature of single-cycle pulses generated with a passive carrier-envelope phase stabilization scheme.
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The fundamental (ω 1 ) and second harmonic (ω 2 ) of 30-fs Ti:sapphire amplifier output were focused into nitrogen gas and produced phase-stable broadband IR pulses (ω 0 ) by four-wave difference frequency generation (ω 1 + ω 1 - ω 2 → ω 0 ) through filamentation. The spectrum spread from 200 to 5500 cm -1 , corresponding to ~3.5 octaves. The waveform of the sub-single-cycle pulse was completely characterized with the frequency-resolved optical gating capable of a carrier-envelope phase determination. The pulse duration was measured as 6.9 fs, which was 0.63 times the period of the carrier frequency, 3000 cm -1 . The carrier-envelope phase of the IR pulse was passively stabilized, and the instability of the phase was estimated as 154-mrad rms over 2.5 h. We also summarize a particular behavior of the spectral phase of the sub-single-cycle pulse; the phase of high-frequency components of the generated pulses changes continuously and linearly with the relative phase between the two-color input pulses, whereas the phase of the low-frequency components takes only two discrete values. 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The fundamental (ω 1 ) and second harmonic (ω 2 ) of 30-fs Ti:sapphire amplifier output were focused into nitrogen gas and produced phase-stable broadband IR pulses (ω 0 ) by four-wave difference frequency generation (ω 1 + ω 1 - ω 2 → ω 0 ) through filamentation. The spectrum spread from 200 to 5500 cm -1 , corresponding to ~3.5 octaves. The waveform of the sub-single-cycle pulse was completely characterized with the frequency-resolved optical gating capable of a carrier-envelope phase determination. The pulse duration was measured as 6.9 fs, which was 0.63 times the period of the carrier frequency, 3000 cm -1 . The carrier-envelope phase of the IR pulse was passively stabilized, and the instability of the phase was estimated as 154-mrad rms over 2.5 h. We also summarize a particular behavior of the spectral phase of the sub-single-cycle pulse; the phase of high-frequency components of the generated pulses changes continuously and linearly with the relative phase between the two-color input pulses, whereas the phase of the low-frequency components takes only two discrete values. 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The fundamental (ω 1 ) and second harmonic (ω 2 ) of 30-fs Ti:sapphire amplifier output were focused into nitrogen gas and produced phase-stable broadband IR pulses (ω 0 ) by four-wave difference frequency generation (ω 1 + ω 1 - ω 2 → ω 0 ) through filamentation. The spectrum spread from 200 to 5500 cm -1 , corresponding to ~3.5 octaves. The waveform of the sub-single-cycle pulse was completely characterized with the frequency-resolved optical gating capable of a carrier-envelope phase determination. The pulse duration was measured as 6.9 fs, which was 0.63 times the period of the carrier frequency, 3000 cm -1 . The carrier-envelope phase of the IR pulse was passively stabilized, and the instability of the phase was estimated as 154-mrad rms over 2.5 h. We also summarize a particular behavior of the spectral phase of the sub-single-cycle pulse; the phase of high-frequency components of the generated pulses changes continuously and linearly with the relative phase between the two-color input pulses, whereas the phase of the low-frequency components takes only two discrete values. The phase behavior is a unique feature of single-cycle pulses generated with a passive carrier-envelope phase stabilization scheme.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JSTQE.2015.2426415</doi><tpages>12</tpages><oa>free_for_read</oa></addata></record>
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subjects Bandwidth
Crystals
Delays
filamentation
fourwave difference frequency generation
Frequency conversion
infrared
Mirrors
Modulation
single-cycle pulse
Ultrafast optics
ultrashort pulse
title Generation and Characterization of Phase-Stable Sub-Single-Cycle Pulses at 3000 cm
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