Pulse compression via direct measurement of spectral phase and pulse-shaping

Advancements in optical pulse-shapers grant the user arbitrary control over amplitude and phase. This control has allowed for simplified generation of the pulse pairs necessary for 2D electronic and vibrational spectroscopy. It also allows the user to correct for dispersion accumulated as pulses travel through the optical system. Dispersion causes a pulse to broaden and decrease in peak intensity, making it longer than its Fourier-limited width and degrading signals. A common way to correct for dispersion is by applying group delay dispersion (GDD) and third order dispersion (TOD) corrections on the phase mask of the pulse-shaper. However, this method is fraught with difficulties. In this paper, what we believe to be a new and simpler technique for pulse compression using a direct phase determination is presented, which results in a 9 percent improvement in the temporal full width half maximum of a cross-correlation signal.

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Publication Details

Journal
Optics Continuum
Published
2025-08-22
DOI
https://doi.org/10.1364/optcon.570017
Primary Topic
Laser-Matter Interactions and Applications
Type
article
Field-Weighted Citation Impact
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article

Pulse compression via direct measurement of spectral phase and pulse-shaping

Arnaldo L. Serrano, Anna Zepeda
Optics Continuum
Laser-Matter Interactions and Applications
article

Pulse compression via direct measurement of spectral phase and pulse-shaping

Arnaldo L. Serrano, Anna Zepeda
article en

Abstract

Advancements in optical pulse-shapers grant the user arbitrary control over amplitude and phase. This control has allowed for simplified generation of the pulse pairs necessary for 2D electronic and vibrational spectroscopy. It also allows the user to correct for dispersion accumulated as pulses travel through the optical system. Dispersion causes a pulse to broaden and decrease in peak intensity, making it longer than its Fourier-limited width and degrading signals. A common way to correct for dispersion is by applying group delay dispersion (GDD) and third order dispersion (TOD) corrections on the phase mask of the pulse-shaper. However, this method is fraught with difficulties. In this paper, what we believe to be a new and simpler technique for pulse compression using a direct phase determination is presented, which results in a 9 percent improvement in the temporal full width half maximum of a cross-correlation signal.

Optics ContinuumVol. 4(9)
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Laser-Matter Interactions and Applications
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