2024
DOI: 10.1063/5.0197977
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Fundamental detectability of Raman scattering: A unified diagrammatic approach

Wei Min,
Xin Gao

Abstract: Both spontaneous Raman scattering and stimulated Raman scattering (SRS) are cornerstones of modern photonics, spectroscopy, and imaging. However, a unified understanding of the ultimate detectability of Raman scattering is lacking, due to both historical and technical reasons. Starting from quantum electrodynamics, we formulate the fundamental detectability for both spontaneous Raman scattering and SRS. The key concept is recognizing spontaneous Raman scattering as stimulated Raman process driven by vacuum fie… Show more

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Cited by 5 publications
(10 citation statements)
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“…Despite the broad analytical applications in many research fields, spontaneous Raman scattering is too weak to be used for biomedical imaging. After the invention of the pulsed laser, CRS phenomena including CARS and SRS were discovered. , These coherent nonlinear optical processes could enhance the weak Raman scattering efficiency by up to ∼10 8 . In the CRS process, both the pump and Stokes beams simultaneously interact with the target molecules; a strong optical resonance occurs when the beat frequency Δω = ω p – ω S matches the vibrational frequency Ω of a chemical bond. CARS photons of ω CARS = 2ω p – ω S are generated via a four-wave-mixing process.…”
Section: Basic Principle and Technical Developments Of Srs Microscopymentioning
confidence: 99%
“…Despite the broad analytical applications in many research fields, spontaneous Raman scattering is too weak to be used for biomedical imaging. After the invention of the pulsed laser, CRS phenomena including CARS and SRS were discovered. , These coherent nonlinear optical processes could enhance the weak Raman scattering efficiency by up to ∼10 8 . In the CRS process, both the pump and Stokes beams simultaneously interact with the target molecules; a strong optical resonance occurs when the beat frequency Δω = ω p – ω S matches the vibrational frequency Ω of a chemical bond. CARS photons of ω CARS = 2ω p – ω S are generated via a four-wave-mixing process.…”
Section: Basic Principle and Technical Developments Of Srs Microscopymentioning
confidence: 99%
“…We can provide a semiempirical numerical evaluation of eq 5 to support the measurement results. 3 If we assume we excite small molecules whose electronic state lies around 200 nm by a third-order interaction unit in cm 2 (area) unit in cm 4 •s (Goppert-Mayer) vacuum-coupled vacuum-decoupled extremely small compared to the electronic counterpart (linear absorption) (see Figure 1) comparable to or exceeding the electronic counterpart (two-photon absorption) (see Figure 1) The summation over states can be relaxed, provided the single resonant state has a large enough transition dipole moment as in Albrecht's theory. 26 We assume both the laser excitation wavelength and the chromophore electronic absorption to be 700 nm and the electronic linewidth to be 700 cm −1 , take the transition displacement D as 1.6 Å, and assume Franck−Condon overlap to be 0.1 here.…”
Section: ■ a Quantum Mechanical Treatment Of σ Srsmentioning
confidence: 99%
“…Specifically, N p is the number of pump photons passing through the sample within the dwell time, and Λ, or Raman absorbance, is a dimensionless quantity defined by Λ = n · σ Raman A · true( ω normalp ω normalS true) , characterizing the strength of the Raman response. The detection limit of Raman microscopy can be recast into η · Λ · N p = 1 where η denotes the photon collection efficiency for spontaneous Raman Eq corresponds to the quantum limit that only a single photon is detected during the spontaneous Raman scattering process.…”
Section: Implications To Stimulated Raman Scattering Microscopymentioning
confidence: 99%
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