Phase noise limited frequency shift impulsive Raman spectroscopy

We introduce a method to enable optical amplification of a coherent Raman spectroscopy signal, which we call radio frequency (RF) Doppler Raman spectroscopy. In this article, we consider the perturbation of a probe pulse in a sample due to an excited Raman vibrational coherence as a generalized Dopp...

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Main Authors: David R. Smith, Jeffrey J. Field, David G. Winters, Scott R. Domingue, Frauke Rininsland, Daniel J. Kane, Jesse W. Wilson, Randy A. Bartels
Format: Article
Language:English
Published: AIP Publishing LLC 2021-02-01
Series:APL Photonics
Online Access:http://dx.doi.org/10.1063/5.0038624
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spelling doaj-b3000ffbf6924125a67fee08c19abd332021-03-02T21:48:08ZengAIP Publishing LLCAPL Photonics2378-09672021-02-0162026107026107-810.1063/5.0038624Phase noise limited frequency shift impulsive Raman spectroscopyDavid R. Smith0Jeffrey J. Field1David G. Winters2Scott R. Domingue3Frauke Rininsland4Daniel J. Kane5Jesse W. Wilson6Randy A. Bartels7Department of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USADepartment of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USADepartment of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USADepartment of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USAMesa Photonics, Inc., Santa Fe, New Mexico 87505, USAMesa Photonics, Inc., Santa Fe, New Mexico 87505, USADepartment of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USADepartment of Electrical and Computer Engineering, Colorado State University, Fort Collins, Colorado 80523, USAWe introduce a method to enable optical amplification of a coherent Raman spectroscopy signal, which we call radio frequency (RF) Doppler Raman spectroscopy. In this article, we consider the perturbation of a probe pulse in a sample due to an excited Raman vibrational coherence as a generalized Doppler shift, which connects a time-varying optical path length (the product of the propagation length and refractive index, OPL = n ℓ) with an optical frequency shift. Amplification of a Raman signal outside of the focused interaction is enabled by converting the Doppler frequency shift experienced by a laser probe pulse into a periodic timing jitter. This transit time perturbation is detected through the phase of a RF electronic signal measured at a harmonic of the probe pulse train with a method adapted from precision metrology techniques used to measure laser pulse train timing jitter. Measurement of a timing jitter allows access to much lower noise floors than other coherent Raman techniques, and by exploiting the new capability to scale the signal of a coherent Raman spectroscopic signal, this method opens the potential to detect very weak Raman signals that are currently not observable due to limits of illumination intensity imposed by laser damage to the specimen and noise.http://dx.doi.org/10.1063/5.0038624
collection DOAJ
language English
format Article
sources DOAJ
author David R. Smith
Jeffrey J. Field
David G. Winters
Scott R. Domingue
Frauke Rininsland
Daniel J. Kane
Jesse W. Wilson
Randy A. Bartels
spellingShingle David R. Smith
Jeffrey J. Field
David G. Winters
Scott R. Domingue
Frauke Rininsland
Daniel J. Kane
Jesse W. Wilson
Randy A. Bartels
Phase noise limited frequency shift impulsive Raman spectroscopy
APL Photonics
author_facet David R. Smith
Jeffrey J. Field
David G. Winters
Scott R. Domingue
Frauke Rininsland
Daniel J. Kane
Jesse W. Wilson
Randy A. Bartels
author_sort David R. Smith
title Phase noise limited frequency shift impulsive Raman spectroscopy
title_short Phase noise limited frequency shift impulsive Raman spectroscopy
title_full Phase noise limited frequency shift impulsive Raman spectroscopy
title_fullStr Phase noise limited frequency shift impulsive Raman spectroscopy
title_full_unstemmed Phase noise limited frequency shift impulsive Raman spectroscopy
title_sort phase noise limited frequency shift impulsive raman spectroscopy
publisher AIP Publishing LLC
series APL Photonics
issn 2378-0967
publishDate 2021-02-01
description We introduce a method to enable optical amplification of a coherent Raman spectroscopy signal, which we call radio frequency (RF) Doppler Raman spectroscopy. In this article, we consider the perturbation of a probe pulse in a sample due to an excited Raman vibrational coherence as a generalized Doppler shift, which connects a time-varying optical path length (the product of the propagation length and refractive index, OPL = n ℓ) with an optical frequency shift. Amplification of a Raman signal outside of the focused interaction is enabled by converting the Doppler frequency shift experienced by a laser probe pulse into a periodic timing jitter. This transit time perturbation is detected through the phase of a RF electronic signal measured at a harmonic of the probe pulse train with a method adapted from precision metrology techniques used to measure laser pulse train timing jitter. Measurement of a timing jitter allows access to much lower noise floors than other coherent Raman techniques, and by exploiting the new capability to scale the signal of a coherent Raman spectroscopic signal, this method opens the potential to detect very weak Raman signals that are currently not observable due to limits of illumination intensity imposed by laser damage to the specimen and noise.
url http://dx.doi.org/10.1063/5.0038624
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