Methyl (CH 3) is generated by photodissociation of methyliodide (CH3I) applying an excimer laser operating at 248 nm. The ca 3 is detected using coherent anti-Stokes Raman spectroscopy (CARS). The CH 3 density is deduced by monitoring simultaneously the reduction of the CARS signal of the parent mol
Determination of absolute Raman cross sections using the inverse Raman effect
β Scribed by Lester J. Hughes; Larry E. Steenhoek; Edward S. Yeung
- Publisher
- Elsevier Science
- Year
- 1978
- Tongue
- English
- Weight
- 432 KB
- Volume
- 58
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
β¦ Synopsis
1%~ use a giant-puke ruby laser and a cw dye laser in a unique inverse Raman spectrometer, and determined the absolu:e Rarnan cross section for the nitrobenzene line at 1345 cm-' to be (1.38 2 0.27) x 10" cm2 ST-'_ 1_ intraduc tion The determination of absolute l&man cross sections has long been a challenge to the spectroscopist. In addition to the otivious applications to the understanding of molecular scattering tensors [ 1 ] , these cross sections have found use in predicting stimulated Raman gain coefficients [2], in the determination of absolute two-photon absorption cross sections [3], and in predicting intensities in coherent anti-Stokes Raman scattering [4]. Raman spectrometers of the pre-laser era only allow relative scattering intensities to be recorded, because of the ill-defmed intensity of excitation and uncertainties in the interaction volume. Still, some absolute intensity standards have been suggested to overcome these difficulties_ Using Raman to Rayleigh intensity ratios [5] is a possibility, but is not reliable because of the presence of small-range order of the molecules in liquids and intermoIecular forces. The H2 J = 1 to J = 3 transition has also been suggested as an absolute intensity standard [6] because of the availability of theoretical predictions. Unfortunately, this cannot be used in liquids. Laser Raman intensity measurements [7,8] are not free from systematic errors either, the major ones being (i) the calibration of the response of the detector; i Research supported by the 'J.S. Department of Energy, Division of Bask Energy Sciences_
π SIMILAR VOLUMES
Spectroscopy on a picosecond time scale is eh-to be fenelble by a new technfque. Inverse Raman spectra are obtained when the intense contlnxous spectrum of a self-phase modulated picosecond pulse is coincident in liquid and solid samples with an intense 6300 A picosecond laser pulse.
## Abstract The increase in amplitude of incident and Raman scattered radiation brought about by the dielectric nature of liquids is known as the internal field effect and is responsible for increasing scattering cross section with increasing refractive index. This effect has been investigated quan
By using a Raman spectrometer system whose absolute sensitivity is calibrated, we have measured the absolute Raman scattering cross sections of trimethylgallium (TMG) and trimethylaluminum (TMA) in the vapor phase. The measured cross sections are (dtr/dl2)~sXM~ = 1.3 Γ 10 -29 cm2/molecule sr line an