{ "id": "epzpqpg3vd", "slug": "anti-stokes-raman-scattering", "title": "Anti-Stokes Raman scattering", "updated": "2026-10-21", "topic_path": [ { "id": "physical", "label": "Physical world and mathematics", "api_url": "https://www.edgepedia.org/api/v1/topics/physical" }, { "id": "physical.physics", "label": "Physics", "api_url": "https://www.edgepedia.org/api/v1/topics/physical.physics" }, { "id": "physical.physics.matter-and-radiation", "label": "Matter and radiation physics", "api_url": "https://www.edgepedia.org/api/v1/topics/physical.physics.matter-and-radiation" }, { "id": "physical.physics.matter-and-radiation.atomic-and-molecular", "label": "Atomic and molecular physics", "api_url": "https://www.edgepedia.org/api/v1/topics/physical.physics.matter-and-radiation.atomic-and-molecular" }, { "id": "physical.physics.matter-and-radiation.atomic-and-molecular.molecular_physics", "label": "Molecular physics", "api_url": "https://www.edgepedia.org/api/v1/topics/physical.physics.matter-and-radiation.atomic-and-molecular.molecular_physics" }, { "id": "physical.physics.matter-and-radiation.atomic-and-molecular.molecular_physics.vibrational_spectroscopy", "label": "Vibrational spectroscopy and molecular vibrations", "api_url": "https://www.edgepedia.org/api/v1/topics/physical.physics.matter-and-radiation.atomic-and-molecular.molecular_physics.vibrational_spectroscopy" } ], "geo": [ { "id": "geo.nongeo.t1800.physical.physics.matter-and-radiation", "label": "Non-geographic · 1800 to 1945: Matter and radiation physics", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo.t1800.physical.physics.matter-and-radiation", "path": [ { "id": "geo.nongeo", "label": "Non-geographic", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo" }, { "id": "geo.nongeo.t1800", "label": "Non-geographic · 1800 to 1945", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo.t1800" }, { "id": "geo.nongeo.t1800.physical", "label": "Physical world and mathematics", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo.t1800.physical" }, { "id": "geo.nongeo.t1800.physical.physics", "label": "Physics", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo.t1800.physical.physics" }, { "id": "geo.nongeo.t1800.physical.physics.matter-and-radiation", "label": "Matter and radiation physics", "api_url": "https://www.edgepedia.org/api/v1/geo/geo.nongeo.t1800.physical.physics.matter-and-radiation" } ] } ], "excerpt": "Anti-Stokes Raman scattering is inelastic light scattering in which a photon gains energy by annihilating a thermally excited vibration, and its intensity ratio to Stokes scattering serves as a contactless thermometer.", "snippet": "Anti-Stokes Raman scattering is inelastic light scattering in which a photon gains energy by annihilating a thermally excited vibration, and its intensity ratio to Stokes scattering serves as a contactless thermometer.", "node": "physical.physics.matter-and-radiation.atomic-and-molecular.molecular_physics.vibrational_spectroscopy", "markdown": "# Anti-Stokes Raman scattering\n\nAnti-Stokes Raman scattering is inelastic light scattering in which the scattered photon leaves with more energy than the incident photon, having annihilated a thermally populated molecular or lattice vibration; the line appears blue-shifted at \\( \\omega_{\\mathrm{p}} + \\omega_{\\mathrm{osc}} \\), where \\( \\omega_{\\mathrm{p}} \\) is the pump frequency and \\( \\omega_{\\mathrm{osc}} \\) the vibrational frequency.[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) Because the anti-Stokes photon requires a thermally excited vibration, its intensity tracks the phonon (A quantum of vibrational energy in a crystal lattice) population, and the ratio of anti-Stokes to Stokes intensity provides a contactless optical thermometer that works on flames, liquids, solids, and devices without contact or emissivity knowledge.[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) • [3](https://link.aps.org/accepted/10.1103/PhysRevLett.133.206902)\n\n| Key fact | Value |\n|---|---|\n| Scattered frequency | \\( \\omega_{\\mathrm{scat}} = \\omega_{\\mathrm{p}} \\pm \\omega_{\\mathrm{osc}} \\); the plus sign (blue shift) is the anti-Stokes line[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) |\n| Temperature formula | \\( I_{\\mathrm{AS}}/I_{\\mathrm{S}} = ((\\omega_{\\mathrm{p}}+\\omega_{\\mathrm{osc}})/(\\omega_{\\mathrm{p}}-\\omega_{\\mathrm{osc}}))^{4} \\cdot e^{-\\hbar\\omega_{\\mathrm{osc}}/kT} \\); third power of frequency for photon-counting (CCD) detection[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) • [4](https://pmc.ncbi.nlm.nih.gov/articles/PMC8066910/) |\n| Usable Raman bands | Below ~200 cm⁻¹ at 77 K, ~600–800 cm⁻¹ at 298 K, ~1300–1500 cm⁻¹ at 600 K[5](https://www.spectroscopyonline.com/view/raman-thermometry-understanding-mathematics-better-design-raman-measurements) |\n| Typical excitation | CW visible lasers at 488, 514, 532, or 633 nm; notch filters with OD > 6 for Stokes and anti-Stokes detection[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) • [1](https://link.springer.com/article/10.1186/s11671-019-3039-2) |\n| Calibrated accuracy | ±50 K up to 1000 K and ±100 K above, validated to 1500 K on six samples[6](https://cpb.iphy.ac.cn/EN/10.1088/1674-1056/accd55) |\n| Spatial resolution | Diffraction limited, down to ~300 nm; better than 10 nm with tip-enhanced Raman geometry[7](https://pubs.aip.org/aip/jap/article/128/13/131101/1027194/Thermoreflectance-techniques-and-Raman-thermometry) |\n| CARS gain | About 10⁹ higher conversion efficiency than spontaneous Raman, with fluorescence discrimination[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) |\n\n## How it works\n\n[Energy conservation](https://www.edgepedia.org/energy-conservation) fixes the line positions; momentum conservation restricts which phonons participate. If the photon gains energy by annihilating a phonon, the scattered line appears at higher frequency (the anti-Stokes process); if it loses energy to a phonon, the Stokes line appears below the pump.[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) Raman lines therefore appear in symmetric pairs about the Rayleigh line at \\( \\nu_{0} \\pm \\nu_{M} \\), with the anti-Stokes member at higher wavenumber and considerably weaker intensity.[8](https://www.s-a-s.org/assets/docs/0470027320_Raman_Spectroscopy_Theory.pdf)\n\nThe intensity asymmetry is thermodynamic. The phonon occupation follows [Bose–Einstein statistics](https://www.edgepedia.org/bose-einstein-statistics), \\( n = \\{\\exp[\\hbar \\cdot \\omega_{\\mathrm{ph}}/(k_{B} \\cdot T)] - 1\\}^{-1} \\), so anti-Stokes scattering requires \\( n > 0 \\).[9](https://pubs.acs.org/nalefd/article-22/8/3260/729402/Tip-Enhanced-Stokes-Anti-Stokes-Scattering-from) The ratio of anti-Stokes to Stokes intensity becomes \\( I_{\\mathrm{AS}}/I_{\\mathrm{S}} = n_{q}/(n_{q}+1) = \\exp(-\\hbar \\cdot \\omega_{\\mathrm{ph}}/(k_{B} \\cdot T)) \\), which directly reflects the local phonon population and hence the temperature.[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) In full form the ratio carries a frequency factor as well: \\( I_{\\mathrm{AS}}/I_{\\mathrm{S}} = ((\\omega_{\\mathrm{p}}+\\omega_{\\mathrm{osc}})/(\\omega_{\\mathrm{p}}-\\omega_{\\mathrm{osc}}))^{4} \\cdot e^{-\\hbar\\omega_{\\mathrm{osc}}/kT} \\).[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) Published treatments differ on the power of the frequency factor: the fourth power applies to energy-based detection, while photon-counting (CCD) detection calls for the third power, \\( (I_{\\mathrm{S}}/I_{\\mathrm{AS}}) = (\\nu_{\\mathrm{S}}^{3}/\\nu_{\\mathrm{AS}}^{3}) \\cdot e^{\\hbar \\cdot \\omega_{0}/(k_{B} \\cdot T)} \\) with \\( \\nu_{\\mathrm{S}} = \\nu_{R} - \\nu_{0} \\) and \\( \\nu_{\\mathrm{AS}} = \\nu_{R} + \\nu_{0} \\).[4](https://pmc.ncbi.nlm.nih.gov/articles/PMC8066910/) • [3](https://link.aps.org/accepted/10.1103/PhysRevLett.133.206902)\n\n## How it is done\n\nA continuous-wave visible laser (commonly 488, 514, 532, or 633 nm) excites the sample through a high-NA objective in a confocal arrangement, with a cooled back-illuminated CCD collecting the spectrum.[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) Detecting both sidebands requires a notch filter centered on the laser line (optical density above 6); long-pass edge filters with transition widths under 3 nm suffice for Stokes-only work.[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) Volume Bragg grating notch filters reject [Rayleigh scattering](https://www.edgepedia.org/rayleigh-scattering) well enough to measure spectra down to ±10 cm⁻¹ from the laser line at about 3 cm⁻¹ resolution.[10](https://journals.sagepub.com/doi/10.1177/0003702820933908)\n\nCalibration is the central step. The measured ratio must be corrected for the instrument's spectral response, captured in a setup-dependent constant (written \\( A \\), \\( C \\), or \\( \\gamma \\) in different papers) that depends on laser polarization, CCD and grating efficiency, excitation wavelength, Raman peak position, and temperature range.[4](https://pmc.ncbi.nlm.nih.gov/articles/PMC8066910/) • [7](https://pubs.aip.org/aip/jap/article/128/13/131101/1027194/Thermoreflectance-techniques-and-Raman-thermometry) • [6](https://cpb.iphy.ac.cn/EN/10.1088/1674-1056/accd55) [Calibration](https://www.edgepedia.org/calibration) against crystalline silicon is described as indispensable for accuracy;[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) a water-spectrum calibration over 20–200 cm⁻¹ needs only 15 min of acquisition, 50 times shorter than an N₂ rotational-Raman calibration, and reproduces thermocouple temperatures to about 1 °C.[10](https://journals.sagepub.com/doi/10.1177/0003702820933908) Laser power is held below the heating threshold (1 mW in one TiO₂ study), and the fluorescence or thermal baseline is removed before ratios are computed.[11](https://www.mdpi.com/2227-9040/12/9/191) • [12](https://iopscience.iop.org/article/10.1088/1742-6596/500/19/192011/pdf)\n\n## Origin\n\nThe possibility of light scattering with a large frequency change was placed on firmer ground in the Kramers–Heisenberg dispersion theory.[13](https://link.springer.com/chapter/10.1007/978-3-032-09188-8_6) • [14](https://royalsocietypublishing.org/rspa/article/122/789/23/2478/The-production-of-new-radiations-by-light) • [15](https://iopscience.iop.org/article/10.1070/PU1998v041n12ABEH000516)\n\nThe priority context was contested. Three groups were searching for frequency-changed scattered light around 1928, in India, Russia, and France.[16](https://www.ufn.ru/ufn03/ufn03_10/ufn0310f.pdf) After Charles Galton Darwin's October 1928 Nature report, Raman wrote a priority letter on 13 November 1928, published in January 1929.[13](https://link.springer.com/chapter/10.1007/978-3-032-09188-8_6) Raman and Krishnan's third Nature letter, \"The Negative Absorption of Radiation\", interpreted the anti-Stokes satellites as interaction of light with excited molecules through the negative absorption Einstein had predicted.[16](https://www.ufn.ru/ufn03/ufn03_10/ufn0310f.pdf) Of the discoverers, only Raman received the 1930 [Nobel Prize in Physics](https://www.edgepedia.org/nobel-prize-in-physics).[15](https://iopscience.iop.org/article/10.1070/PU1998v041n12ABEH000516)\n\n## Variants\n\nCARS (coherent anti-Stokes [Raman scattering](https://www.edgepedia.org/raman-scattering)) is a third-order nonlinear variant in which the signal arises from the induced polarization \\( P^{(3)} = \\chi^{(3)} \\cdot E_{\\mathrm{p}} \\cdot E_{\\mathrm{s}}^{*} \\cdot E_{\\mathrm{p}} \\) at the anti-Stokes frequency \\( \\omega_{\\mathrm{as}} = (\\omega_{\\mathrm{p}} - \\omega_{\\mathrm{s}}) + \\omega_{\\mathrm{p}}' \\); for a bulk liquid the CARS signal was estimated to exceed spontaneous Raman by nine orders of magnitude.[17](https://pmc.ncbi.nlm.nih.gov/articles/PMC2642972/) CARS microscopy was implemented.[17](https://pmc.ncbi.nlm.nih.gov/articles/PMC2642972/) • [18](https://www.frontiersin.org/journals/physics/articles/10.3389/fphy.2020.598420/full) The first CARS temperature measurement, of H₂, was reported by F. Moya, S. A. J. Druet, and J. P. E. Taran in 1975 in Optics Communications.[19](https://doi.org/10.1016/0030-4018%2875%2990034-6) Resonance-enhanced CARS, demonstrated in 1976 by B. Hudson and colleagues in the [Proceedings of the National Academy of Sciences](https://www.edgepedia.org/proceedings-of-the-national-academy-of-sciences) for dilute solutions near an electronic transition, adds high signal-to-noise, fluorescence rejection, and low average power.[20](https://doi.org/10.1073/pnas.73.11.3798)\n\nStimulated and tip-enhanced forms extend the method. Femtosecond stimulated Raman scattering (FSRS) picosecond thermometry, demonstrated in 2011 by N. C. Dang and colleagues in [Physical Review Letters](https://www.edgepedia.org/physical-review-letters), measures condensed-phase temperature from Raman loss to Raman gain ratios of low-frequency modes on picosecond timescales, with no material-dependent parameters or prior calibration.[21](https://doi.org/10.1103/physrevlett.107.043001) Tip-enhanced Stokes–anti-Stokes (SaS) scattering from a single carbyne chain increased anti-Stokes signal by a factor of 3290 and the anti-Stokes/Stokes ratio 22-fold, enabling calibration-free thermometry.[9](https://pubs.acs.org/nalefd/article-22/8/3260/729402/Tip-Enhanced-Stokes-Anti-Stokes-Scattering-from) One important boundary: in stimulated [Raman spectroscopy](https://www.edgepedia.org/raman-spectroscopy) the same thermal populations generate the red- and blue-shifted components, so their ratio cannot be used to extract temperature; coherent thermometry instead requires anharmonic signatures such as vibrational hot bands, with hot-band amplitude ratios \\( \\Delta p_{j+1}/\\Delta p_{j} = e^{-\\hbar \\cdot \\omega_{v}/(k_{B} \\cdot T)} \\).[3](https://link.aps.org/accepted/10.1103/PhysRevLett.133.206902)\n\n## Applications\n\nCombustion and high-temperature gas is the classic use: a pulsed Nd:YAG anti-Stokes instrument measured furnace gas temperatures near 1500–1800 K at atmospheric pressure with a standard deviation under 1% for ~200 s averaging, using the anti-Stokes rather than Stokes component to exclude cold atmospheric nitrogen and gated detection to reject combustion background.[22](https://opg.optica.org/ao/abstract.cfm?uri=ao-38-9-1467) CARS thermometry serves turbulent flames and, more broadly, chemical imaging of tissue and thermography of electronic and optoelectronic devices.[18](https://www.frontiersin.org/journals/physics/articles/10.3389/fphy.2020.598420/full) • [1](https://link.springer.com/article/10.1186/s11671-019-3039-2)\n\nSolids under extreme conditions include laser-heated diamond anvil cells, where calibrated anti-Stokes/Stokes thermometry probed the anharmonic behavior of hBN at high temperature and pressure.[6](https://cpb.iphy.ac.cn/EN/10.1088/1674-1056/accd55) In flames, single-laser CARS achieved ~600 µm spatial resolution, about ±2% precision, and ±3% accuracy from 300 to 2200 K, and hybrid fs/ps CARS reached 2.2% precision and 3.3% accuracy at 2400 K.[23](https://www.mdpi.com/2304-6742/12/7/622) On 3D Si microtube nanomembranes, Stokes/anti-Stokes thermometry with a 532 nm laser measured local temperatures reaching ≈1288 K with ≈5 µm spatial resolution, exceeding conventional infrared thermography.[24](https://nanomem.fudan.edu.cn/_upload/article/files/f0/e9/5eb4182f435aaf7cc2538e714c4f/9bf49e69-2025-4197-9b89-59b9911fbcac.pdf) In biology, water-spectrum calibration supports intracellular temperature measurement,[10](https://journals.sagepub.com/doi/10.1177/0003702820933908) and AuNPs functionalized with a 2 nm sol–gel TiO₂ layer were validated as anti-Stokes/Stokes probes from 25 °C to 240 °C under external thermal and thermoplasmonic heating.[25](https://pubs.rsc.org/en/content/articlelanding/2025/cp/d5cp02372f) The Stokes/anti-Stokes amplitude ratio also reads out the temperature of optically cooled Si₃N₄ membrane mechanical resonators down to a few vibrational quanta.[26](https://journals.aps.org/pra/abstract/10.1103/PhysRevA.92.031802)\n\n## Limitations and alternatives\n\nThe anti-Stokes signal is weak. Raman scattering is feeble, accompanied by Rayleigh scattering typically 3–5 orders of magnitude more intense, and anti-Stokes scattering is much weaker than Stokes, which reduces the accuracy of intensity-ratio thermometry in practice.[8](https://www.s-a-s.org/assets/docs/0470027320_Raman_Spectroscopy_Theory.pdf) • [27](https://par.nsf.gov/servlets/purl/10191854) Most Raman thermometry therefore relies instead on calibrated peak-position shifts, and the ratio method is limited by the weak anti-Stokes signal and the need for careful spectral calibration.[2](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport) Baseline removal is critical: for Teflon at 600 K, precision was under 1% but accuracy was worse than 5% (about 35 K low) because of inadequate fluorescence baseline removal.[12](https://iopscience.iop.org/article/10.1088/1742-6596/500/19/192011/pdf) Laser-induced heating is a direct failure mode; a maximum local temperature increase of 15 °C was detected at 800 nm excitation when power exceeded the 1 mW threshold.[11](https://www.mdpi.com/2227-9040/12/9/191) The ratio also breaks down for resonance Raman scattering, where Stokes and anti-Stokes processes occur at different pump photon frequencies, and a wavelength dependence of the Raman cross-section can produce anomalous ratios.[1](https://link.springer.com/article/10.1186/s11671-019-3039-2) • [4](https://pmc.ncbi.nlm.nih.gov/articles/PMC8066910/)\n\nNon-equilibrium populations undermine the assumption of one local temperature. Strong non-equilibrium exists among phonon branches in single-layer graphene under laser irradiation.[27](https://par.nsf.gov/servlets/purl/10191854) Materials with negligible Raman signal, such as amorphous materials and metals, are poor candidates.[7](https://pubs.aip.org/aip/jap/article/128/13/131101/1027194/Thermoreflectance-techniques-and-Raman-thermometry) Contactless photothermal alternatives, thermoreflectance and TDTR/FDTR, cover samples from ultrathin films down to 1 nm to phononic crystals, though photoexcited carriers can create non-thermal phonon populations that affect the Raman ratio.[7](https://pubs.aip.org/aip/jap/article/128/13/131101/1027194/Thermoreflectance-techniques-and-Raman-thermometry)\n\n## References\n\n1. [Raman Techniques: Fundamentals and Frontiers](https://link.springer.com/article/10.1186/s11671-019-3039-2)\n2. [Raman spectroscopy for thermal transport characterization: Principles, techniques, and applications (Journal of Applied Physics Tutorial)](https://pubs.aip.org/aip/jap/article/139/8/081101/3381058/Raman-spectroscopy-for-thermal-transport)\n3. [Temperature Dependence of Coherent versus Spontaneous Raman Scattering (Batignani et al., PRL 133, 206902, 2024)](https://link.aps.org/accepted/10.1103/PhysRevLett.133.206902)\n4. [Contactless Temperature Sensing at the Microscale Based on Titanium Dioxide Raman Thermometry](https://pmc.ncbi.nlm.nih.gov/articles/PMC8066910/)\n5. [Raman Thermometry: Understanding the Mathematics to Better Design Raman Measurements](https://www.spectroscopyonline.com/view/raman-thermometry-understanding-mathematics-better-design-raman-measurements)\n6. [Anti-Stokes/Stokes temperature calibration and its application in laser-heating diamond anvil cells (Chin. Phys. B, 2023)](https://cpb.iphy.ac.cn/EN/10.1088/1674-1056/accd55)\n7. [Thermoreflectance techniques and Raman thermometry for thermal property characterization of nanostructures (Tutorial, J. Appl. Phys. 2020)](https://pubs.aip.org/aip/jap/article/128/13/131101/1027194/Thermoreflectance-techniques-and-Raman-thermometry)\n8. [Raman Spectroscopy: Theory](https://www.s-a-s.org/assets/docs/0470027320_Raman_Spectroscopy_Theory.pdf)\n9. [Tip-Enhanced Stokes–Anti-Stokes Scattering from Carbyne (Nano Letters, 2022)](https://pubs.acs.org/nalefd/article-22/8/3260/729402/Tip-Enhanced-Stokes-Anti-Stokes-Scattering-from)\n10. [A Simple Calibration Method of Anti-Stokes–Stokes Raman Intensity Ratios Using the Water Spectrum for Intracellular Temperature Measurements](https://journals.sagepub.com/doi/10.1177/0003702820933908)\n11. [Near-Infrared Multiwavelength Raman Anti-Stokes/Stokes Thermometry of Titanium Dioxide (Chemosensors, 2024)](https://www.mdpi.com/2227-9040/12/9/191)\n12. [Raman temperature measurement (Moore & Schmidt, J. Phys. Conf. Ser., 2014)](https://iopscience.iop.org/article/10.1088/1742-6596/500/19/192011/pdf)\n13. [The Raman Effect: How Virtual Transitions Became \"Virtual\" (for the First Time)... (1928–1929)](https://link.springer.com/chapter/10.1007/978-3-032-09188-8_6)\n14. [The production of new radiations by light scattering., Part I](https://royalsocietypublishing.org/rspa/article/122/789/23/2478/The-production-of-new-radiations-by-light)\n15. [Seventy years of combination (Raman) scattering](https://iopscience.iop.org/article/10.1070/PU1998v041n12ABEH000516)\n16. [The discovery of combination scattering of light in Russia and India](https://www.ufn.ru/ufn03/ufn03_10/ufn0310f.pdf)\n17. [Coherent Anti-Stokes Raman Scattering Microscopy](https://pmc.ncbi.nlm.nih.gov/articles/PMC2642972/)\n18. [Coherent Anti-Stokes Raman Scattering Microscopy and Its Applications](https://www.frontiersin.org/journals/physics/articles/10.3389/fphy.2020.598420/full)\n19. [Gas spectroscopy and temperature measurement by coherent Raman anti-stokes scattering (Optics Communications, 1975)](https://doi.org/10.1016/0030-4018%2875%2990034-6)\n20. [B Hudson and colleagues (1976). Resonance enhanced coherent anti-Stokes Raman scattering.. Proceedings of the National Academy of Sciences.](https://doi.org/10.1073/pnas.73.11.3798)\n21. [N. C. Dang and colleagues (2011). Femtosecond Stimulated Raman Scattering Picosecond Molecular Thermometry in Condensed Phases. Physical Review Letters.](https://doi.org/10.1103/physrevlett.107.043001)\n22. [Spontaneous anti-Stokes Raman probe for gas temperature measurements in industrial furnaces (Appl. Opt. 38, 1467, 1999)](https://opg.optica.org/ao/abstract.cfm?uri=ao-38-9-1467)\n23. [Advances in Femtosecond Coherent Anti-Stokes Raman Scattering for Thermometry (MDPI, 2024)](https://www.mdpi.com/2304-6742/12/7/622)\n24. [Non-Destructive Thermal Evaluation on Laser-Stimulated 3D Functional Nanomembranes via Stokes and Anti-Stokes Raman Scattering (2025)](https://nanomem.fudan.edu.cn/_upload/article/files/f0/e9/5eb4182f435aaf7cc2538e714c4f/9bf49e69-2025-4197-9b89-59b9911fbcac.pdf)\n25. [Gold nanoparticles combined with ultrafine TiO2 layer: a reliable probe for Raman thermometry (Phys. Chem. Chem. Phys., 2025)](https://pubs.rsc.org/en/content/articlelanding/2025/cp/d5cp02372f)\n26. [Optomechanical Raman-ratio thermometry (Phys. Rev. A 92, 031802(R), 2015)](https://journals.aps.org/pra/abstract/10.1103/PhysRevA.92.031802)\n27. [Raman-based thermal characterization review (NSF public access repository)](https://par.nsf.gov/servlets/purl/10191854)\n\n---\n*Topic: Encyclopedia › Physical world and mathematics › Physics › Matter and radiation physics › Atomic and molecular physics › Molecular physics › Vibrational spectroscopy and molecular vibrations*\n\n*Initially written Sep 29, 2026 · Edited: Oct 15, 2026; Oct 21, 2026*\n\n*Copyright 2026 EdgeChat AI, a subsidiary of Biostate AI.*\n\nLicense: Edgepedia Community License 1.0, https://www.edgepedia.org/edgepedia/license\n", "same_as": [], "url": "https://www.edgepedia.org/anti-stokes-raman-scattering", "markdown_url": "https://www.edgepedia.org/anti-stokes-raman-scattering.md", "license": { "name": "Edgepedia Community License 1.0", "url": "https://www.edgepedia.org/edgepedia/license", "summary": "Free with credit, commercial use included. AI training is open to everyone. 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Edgepedia Community License 1.0.", "speakable": "Anti-Stokes Raman scattering is inelastic light scattering in which a photon gains energy by annihilating a thermally excited vibration, and its intensity ratio to Stokes scattering serves as a contactless thermometer." }