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Resonance Raman scattering time-resolved

Shreve A P and Mathies R A 1995 Thermal effects in resonance Raman-scattering—analysis of the Raman intensities of rhodopsin and of the time-resolved Raman-scattering of bacteriorhodopsin J. Phys. Chem. 99 7285-99... [Pg.1176]

Tripathi G N R and Schuler R H 1982 Time-resolved resonance Raman scattering of transient radicals the p-aminophenoxyl radical J. Chem. Phys. 76 4289-90... [Pg.1227]

The metaiioporphyrins form a diverse class of molecules exhibiting complex and varied photochemistries. Until recently time-resolved absorption and fluorescence spectroscopies were the only methods used to study metailoporphyrln excited state relaxation in a submicrosecond regime. In this paper we present the first picosecond time-resolved resonance Raman spectra of excited state metaiioporphyrins outside of a protein matrix. The inherent molecular specificity of resonance Raman scattering provides for a direct probe of bond strengths, geometries, and ligation states of photoexcited metaiioporphyrins. [Pg.266]

Probing Metalloproteins Electronic absorption spectroscopy of copper proteins, 226, 1 electronic absorption spectroscopy of nonheme iron proteins, 226, 33 cobalt as probe and label of proteins, 226, 52 biochemical and spectroscopic probes of mercury(ii) coordination environments in proteins, 226, 71 low-temperature optical spectroscopy metalloprotein structure and dynamics, 226, 97 nanosecond transient absorption spectroscopy, 226, 119 nanosecond time-resolved absorption and polarization dichroism spectroscopies, 226, 147 real-time spectroscopic techniques for probing conformational dynamics of heme proteins, 226, 177 variable-temperature magnetic circular dichroism, 226, 199 linear dichroism, 226, 232 infrared spectroscopy, 226, 259 Fourier transform infrared spectroscopy, 226, 289 infrared circular dichroism, 226, 306 Raman and resonance Raman spectroscopy, 226, 319 protein structure from ultraviolet resonance Raman spectroscopy, 226, 374 single-crystal micro-Raman spectroscopy, 226, 397 nanosecond time-resolved resonance Raman spectroscopy, 226, 409 techniques for obtaining resonance Raman spectra of metalloproteins, 226, 431 Raman optical activity, 226, 470 surface-enhanced resonance Raman scattering, 226, 482 luminescence... [Pg.457]

The Raman scattering strength of E,(LO) in the vicinity of the fundamental bandgap has been investigated in resonant Raman scattering as a function of temperature between 77 K and 870 K [35], Studies of photocarrier thermalisation have been performed by time resolved Raman spectroscopy [36],... [Pg.54]

Itoh, T., Kikkawa, Y., Biju, V., Ishikawa, M., Ikehata, A., Ozaki, Y. (2006). Variations in Steady-State and Time-Resolved Background Luminescence fi om Surface-Enhanced Resonance Raman Scattering-Active Single Ag Nanoaggregates. J.Phys. Chem. B 110 21536-21544. [Pg.65]

Lutz M, Kleo J and Reiss-Husson F (1976) Resonance Raman scattering of bacteriochlorophyll, bacteriopheophytin and spheroidene in reaction centers of Rhodopseudomonas spheroides. Biochem Biophys Res Comm 69 711-717 Lutz M, Chinsky L and Turpin PY (1982) Triplet states of carotenoids bound to reaction centers ofphotosynthetic bacteria Time-resolved resonance Raman spectroscopy. Photochem Photobiol 36 503-515... [Pg.219]

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]

Fig. 2. Photon molecule interaction processes. (A) Normal Raman scattering, (B) discrete resonance Raman scattering, (C) continuum resonance Raman scattering. All these processes are amenable to direct scattering experiments generally, only (B) can be easily studied by time-resolved observation. Fig. 2. Photon molecule interaction processes. (A) Normal Raman scattering, (B) discrete resonance Raman scattering, (C) continuum resonance Raman scattering. All these processes are amenable to direct scattering experiments generally, only (B) can be easily studied by time-resolved observation.
A number of different characterization methods have been performed on poly(thiophene) and poly(alkylderivative)s. NMR of electropolymerized poly(thiophene) films has been studied by Hotta et al. and Osterholm et al. An infrared study about vibrational key band on poly(thiophene) films and FT-IR spectra were also published. Resonance Raman scattering on poly(methylthiophene) and x-ray scattering on poly(thiophene) were performed x-ray photoelectron spectroscopy has been reported on FeCls-doped poly(hexylthiophene) and electrochemically obtained poly(thiophene) [20]. Time resolved fluorescence studies on thiophene oligomers are given by Chosrovian et al. [79]. For studies on oligothiophene films see [80,81]. [Pg.762]

Figure 10.15 Resonance Raman detection of populations in electronically excited states and following creation of state molecules by laser excitation at frequency Probing molecules at frequency will generate intense resonance Raman emission at if the - transition is El -allowed, because is in near-resonance with the energy separation between vibration less and some vibronic level of S2. Probing at frequency tu will generate similarly intense emission only if appreciable population has accumulated in by intersystem crossing from S, since a is in resonance with the T — T, energy gap. This excited-state selectivity of resonance Raman scattering has rendered it a useful tool for monitoring time-resolved excited state dynamics. Figure 10.15 Resonance Raman detection of populations in electronically excited states and following creation of state molecules by laser excitation at frequency Probing molecules at frequency will generate intense resonance Raman emission at if the - transition is El -allowed, because is in near-resonance with the energy separation between vibration less and some vibronic level of S2. Probing at frequency tu will generate similarly intense emission only if appreciable population has accumulated in by intersystem crossing from S, since a is in resonance with the T — T, energy gap. This excited-state selectivity of resonance Raman scattering has rendered it a useful tool for monitoring time-resolved excited state dynamics.
Hegarty, J., McGarvey, J., BeU, S., et al. (1996). Time-resolved resonance raman scattering of triplet state anthracene in supercritical CO2, J. Phys. Chem., 100, pp. 15704—15707. [Pg.867]

Okamoto H and Yoshihara K 1990 Femtosecond time-resolved coherent Raman scattering under various polarization and resonance conditions J. Opt. Soc. B7 1702-8... [Pg.1230]


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See also in sourсe #XX -- [ Pg.326 ]




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Resonance scattering

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Time-Resolved Resonance Raman

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