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Stimulated resonance Raman scattering

Yanagi, A. Yoshiki, S. Hotta and S. Kobayashi, Mirrorless lasing from thiophene/phenylene co-oligomer crystals based on stimulated resonance Raman scattering, j. Appl. Phys., 96, 4240-4244 (2004) with permission from the American Institute of Physics [Pg.468]

Molecule Point group max of ASE (nm) Raman shift (cm Raman-active mode [Pg.469]


Scattering Phenomena.—A review has appeared of the scattering of depolarized light by simple fluids.437 Pre-resonance Raman spectra of NH3, CH8NH2, form-amide, cw-dichloroethylene, propargyl alcohol, and pyrazine 438 resonance Raman scatter of I2 in solution and in inert matrices 439 time-resolved resonance fluorescence and resonance Raman 440 and stimulated resonance Raman scattering 441 pseudo-Raman spectra in stacked benzene molecules 442 and birefringence in CS2 443 have been the subjects of recent reports. [Pg.38]

Figure 10.7 Normalized fluorescence (a), excitation (b) and optically pumped PL spectra (c, d) taken from platelet crystals of BP1T. The spontaneous fluorescence (a), AST (c) and SRRS (d) spectra were taken at Xex = 365, 355 and 460 nm, respectively. The excitation spectrum (b) was taken for the fluorescence band at 493 nm. Reproduced from H. Yanagi, I. Sakata, A. Yoshiki, 5. Hotta and 5. Kobayashi, Polarization dependence of Stimulated resonance Raman scattering from a single crystal of bi-phenyl-capped thiophene, Jpn. J. Appl. Phys., 45, 483-487 (2006) with permission from The Institute of Pure and Applied Physics... Figure 10.7 Normalized fluorescence (a), excitation (b) and optically pumped PL spectra (c, d) taken from platelet crystals of BP1T. The spontaneous fluorescence (a), AST (c) and SRRS (d) spectra were taken at Xex = 365, 355 and 460 nm, respectively. The excitation spectrum (b) was taken for the fluorescence band at 493 nm. Reproduced from H. Yanagi, I. Sakata, A. Yoshiki, 5. Hotta and 5. Kobayashi, Polarization dependence of Stimulated resonance Raman scattering from a single crystal of bi-phenyl-capped thiophene, Jpn. J. Appl. Phys., 45, 483-487 (2006) with permission from The Institute of Pure and Applied Physics...
Figure 10.14 (a) PL intensity and FWHM of the emission peak at 565 nm taken from the AC7 crystals as a function of Xex- (b) Changes in kem of the emission peaks that appeared at various X x- Reproduced from H. Yanagi, A. Yoshiki, S. Hotta and S. Kobayashi, Mirrorless lasing from thiophene/phenylene co-oligomer crystals based on stimulated resonance Raman scattering, J. Appl. Phys., 96, 4240-4244 (2004) with permission from the American Institute of Physics... [Pg.469]

H. Yanagi and A. Yoshiki, Stimulated resonance Raman scattering from epitaxially oriented crystals of bi-phenyl-capped thiophene, Appl. Phys. Lett., 84, 4783-4785 (2004). [Pg.475]

A. A. Maksimov and 1.1. Tartakovskii, Stimulated resonant Raman scattering of hghtin anthracene crystals, Phys. [Pg.475]

After an initial peak at delay times where the pump and the probe fields overlap, the pump-probe signal is seen to split up into two components a dominant, slightly oscillating feature centered at the electronic gap A of the 5q-52 transition u>2 4.8 eV), and a weaker red-shifted contribution, centered at L02 3.4 eV. As is shown below, the first component at o 2 A is mostly due to stimulated resonance Raman scattering, thus reflecting... [Pg.771]

Walmsiey I A, Wise F W and Tang C L 1989 On the difference between quantum beats in impulsive stimulated Raman scattering and resonance Raman scattering Chem. Phys. Lett. 154 315-20... [Pg.1230]

Becker, M., Gaubatz, U., Bergmann, K. and Jones, P.L. (1987). Efficient and selective population of high vibrational levels by stimulated near resonance Raman scattering, J. Chem. Phys., 87, 5064-5076. [Pg.270]

LA. Wamsley, F.W. Wise, and C.L. Tang, On the Difference between Quantum Beats in Impulsive Stimulated Raman Scattering and Resonance Raman Scattering , Chem. Phys. Lett. 154, 315 (1989). [Pg.199]

Unlike the typical laser source, the zero-point blackbody field is spectrally white , providing all colours, CO2, that seek out all co - CO2 = coj resonances available in a given sample. Thus all possible Raman lines can be seen with a single incident source at tOp Such multiplex capability is now found in the Class II spectroscopies where broadband excitation is obtained either by using modeless lasers, or a femtosecond pulse, which on first principles must be spectrally broad [32]. Another distinction between a coherent laser source and the blackbody radiation is that the zero-point field is spatially isotropic. By perfonuing the simple wavevector algebra for SR, we find that the scattered radiation is isotropic as well. This concept of spatial incoherence will be used to explain a certain stimulated Raman scattering event in a subsequent section. [Pg.1197]

Savchenkov, A. A. Matsko, A. B. Mohageg, M. Maleki, L., Ringdown spectroscopy of stimulated Raman scattering in a whispering gallery mode resonator, Opt. Lett. 2007, 32,... [Pg.120]

J. B. Snow, S.-X. Qian, and R. K. Chang, Stimulated Raman scattering from individual water and ethanol droplets at morphology-dependent resonances, Opt Lett 10, 37-39 (1985). [Pg.386]


See other pages where Stimulated resonance Raman scattering is mentioned: [Pg.456]    [Pg.463]    [Pg.464]    [Pg.467]    [Pg.1120]    [Pg.456]    [Pg.463]    [Pg.464]    [Pg.467]    [Pg.1120]    [Pg.498]    [Pg.448]    [Pg.1196]    [Pg.471]    [Pg.744]    [Pg.532]    [Pg.1206]    [Pg.1210]    [Pg.3038]    [Pg.318]    [Pg.164]    [Pg.104]    [Pg.384]    [Pg.601]    [Pg.623]   
See also in sourсe #XX -- [ Pg.456 , Pg.474 ]




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Stimulated Scatterings

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