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  • 1
    Keywords: Forschungsbericht
    Type of Medium: Online Resource
    Pages: Online-Ressource (30 p. = 2,11 MB) , ill., graphs
    Edition: [Elektronische Ressource]
    Language: German
    Note: Contract BMBF 13 N 7511. - Differences between the printed and electronic version of the document are possible. - nIndex p. 27 - 30 , Also available as printed version , Systemvoraussetzungen: Acrobat reader.
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  • 2
    Keywords: Raman spectroscopy-Congresses. ; Electronic books.
    Description / Table of Contents: Proceedings of the NATO Advanced Study Institute, Bad Windsheim, Germany, August 23-September 3, 1982.
    Type of Medium: Online Resource
    Pages: 1 online resource (623 pages)
    Edition: 1st ed.
    ISBN: 9789400979123
    Series Statement: Nato Science Series C: Series ; v.93
    DDC: 535.846
    Language: English
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 841-851 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Resonance Raman spectra of polymer chains in the single crystals of the diacetylenes FBS (2,4-hexadiynylene-di-p-fluorobenzene sulfonate), TS/FBS [6-(p-toluenesulfonyloxy)-2,4-p-fluorobenzene sulfonate] and TS6 (2,4-hexadiynylene-di-p-toluene sulfonate) are described theoretically by means of a Franck–Condon model, which considers a chain length dependence. The electronic transition energies and matrix elements are calculated by means of a linear-combination-of-atomic-orbitals–molecular-orbital method calculation in the Hückel approach. We are able to describe the Raman excitation profiles as well as the Raman band profiles for two Raman active modes, i.e., the C+C-, and the C 3/4 C-stretching vibrations of the polymer chains. The model also contains a description of a side group vibrational mode which is enhanced by Fermi resonance with the C=C-stretching vibration. Observed Raman excitation profiles can be well simulated by these calculations. An evaluation of the parameters shows a strong influence of defects, which is described by including inhomogeneous broadening in the theoretical model. An interaction between ensemble and intramolecular properties due to defects can be shown. Simulation of the Raman band profiles yields information on the influence of chain length distribution. Changes of position and Raman band profile as well as of the strength of the Fermi resonance can be explained by the enhancement of modes belonging to polymer chains having different chain lengths. A considerable influence of the substitutents results in remarkable changes of several parameters on which the model calculation is based.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 2391-2397 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have recorded high-resolution polarized and depolarized Raman spectra of isotopically pure 35Cl2 using the argon ion laser lines 501.7, 496.5, 488.0, 476.5, 457.9, 363.8, 351.1, and 333.6 nm and the krypton ion laser line 413.1 nm. Overtone progressions can be observed for 413.1 nm and UV excitation. The spectral band shapes of the overtones show a systematic variation with excitation frequency. The relative intensities of the overtone bands have been calculated with second order perturbation theory. The spectral feature of the overtones can be explained by resonance Raman scattering via the repulsive 1Π1u state. The 1Π1u potential was determined with a high accuracy. This is possible because the Raman band intensities are very sensitive to the location of the potential curves of the involved excited scattering states. The spectral feature of the fundamental band excited in the UV region can be explained assuming a destructive interference effect between resonant and nonresonant Raman scattering resulting from adjacent highly lying states. This effect can be monitored via the depolarization ratio of the fundamental transitions, the change in relative intensities between the different Q branches of the fundamental bands and comparison of the observed and calculated overall band intensities of the fundamental and overtone bands excited with different laser lines.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 5636-5649 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Scattering delay times between photon absorption and emission, and transition rates for continuum resonance Raman scattering are derived in a coherent and detailed fashion, within the time-dependent approach pioneered by Heller, Imre, and others. The resulting expressions for the Raman scattering delay times are related to similar expressions for particle scattering delay times derived by Eisenbud, Wigner, and Smith in terms of S matrices. These expressions are valid both for the ideal cases of sharp photon frequencies, and for realistic cases of finite frequency distributions or laser profiles. The Raman transition rates for this type of resonance scattering have a golden-rule-type expression implying the familiar selection rules and symmetry of two-photon transitions, similar to the Fermi–Pauli golden rule for single photon transitions. Applications to 79Br2 yield ultrashort Raman scattering delay times in the 10 fs domain.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 88 (2000), S. 5268-5271 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have observed the relaxation dynamics of coherent longitudinal optical phonons in CdSSe quantum dots embedded in a glass matrix by femtosecond time-resolved coherent anti-Stokes Raman scattering (CARS). The phase relaxation time is directly deduced from the exponential decay of the signal. Oscillations with frequency of the longitudinal optical (LO) phonon are superimposed on the CARS signal. We consider two possible mechanisms, which result in such oscillations. The excitation of a LO phonon wave packet of the fundamental and the overtone would produce quantum beats. The second possibility is displacive excitation of coherent phonons. This mechanism does not contribute to the CARS signal, but it could attenuate it periodically with the phonon frequency. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 2237-2246 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have analyzed the color zones in single crystals of the diacetylene derivative 6-(p-toluenesulfonyloxy)-2,4-hexadiynyl-p-fluorobenzenesulfonate by means of various optical spectroscopical methods in order to derive a plausible model for the origin of this type of chromism. By applying absorption, luminescence, resonance Raman, and coherent anti-Stokes Raman spectroscopy we obtained sufficient information for an understanding of the nature of the color zones. With the help of a nearly free-electron model calculation and a theoretical model for side group torsions, we found that a disturbance of the π-electron conjugation by a defect hindrance on side groups is the proper reason for the observed chromism. Growth defects in {111} crystal-growth sectors with a Burgers vector in the [010] direction cause the shape of the color zones. We found, particularly, that resonance coherent anti-Stokes Raman spectroscopy proves to be a valuable tool for the investigation of electronic and structural properties of the diacetylene crystals.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 6302-6307 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have performed polarized resonance coherent anti-Stokes Raman experiments on the permanganate ion doped in potassium perchlorate single crystals at temperature T=15 K. At this temperature the m (Cs) site splitting of the excited degenerate 1T2-electronic level of the permanganate ion and the vibronic structure are well resolved. We report on the A'-ν1 coherent anti-Stokes Raman excitation profile which shows a strong dependence on the frequency of the pump laser. The simulation of the experimental results is performed by using the transform theory, which enables one to calculate the resonance Raman excitation profile solely from the measured absorption spectrum. According to the well known relation between the third-order nonlinear susceptibility and the Raman polarizability the coherent anti-Stokes excitation profile is given by a simple product of two Raman excitation profiles which are shifted relative to each other. The linear and the quadratic electron-phonon coupling as well as the influence of non-Condon terms were taken into account. Since the transform theory is mode selective in case there are no mode mixing effects the results derived from the description of the Raman excitation profiles and the coherent anti-Stokes excitation profiles are more definite. For this purpose one only needs the model parameters of the mode of interest. The simulation of the A'-ν1 coherent anti-Stokes profile shows that a small amount of non-Condon coupling yields to a better agreement with the experiment.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 88 (2000), S. 764-771 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: CdZnSe/ZnSe quantum wires with two different Cd contents and different wire sizes were investigated by resonance Raman spectroscopy. Depending on the Cd content, the longitudinal optical (LO) phonon signal of the wires shows an asymmetry or a clear separation into two peaks. This separation is caused by an inhomogeneous strain parallel to the layer plane due to the strain relaxation at the wire edges. Thus, the observed signals can be attributed to LO phonons excited in the center and in the edge of the structures. Furthermore, high outgoing resonances for the LO overtones (2LO and 3LO) can be observed. For two wire sizes [(a): length L=100 μm, width W=18 nm; (b): L=49 nm, W=27 nm] excitation profiles of the LO fundamental and of the first overtone of Cd0.2Zn0.8Se quantum wires have been recorded. The excitation profiles clearly show structures attributed to the incoming and outgoing resonances. The intensity ratio 2LO/1LO, which is also a good measure for the electron–phonon coupling in a system, was determined for various wire sizes. The results point to a decrease of the electron–phonon coupling for decreasing wire length (transition from wire to dot). © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 1446-1450 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Resonant micro-Raman spectroscopy was performed on ZnSe/Cd0.2Zn0.8Se quantum wires. The LO phonon frequencies observed for the wires were investigated as a function of the temperature and the wire width. ZnSe/Cd0.2Zn0.8Se quantum wells grown by molecular beam epitaxy were patterned by electron beam lithography and wet chemical etching to obtain quantum wires with widths down to the sub-100 nm region. The sample under investigation consisted of different areas each containing wires with well defined widths. Micro-Raman spectroscopy enabled us to perform measurements on a particular area of the sample. By this method Raman spectra could be obtained as a function of the wire width. The sample temperature was chosen to be between room temperature and 9 K. A splitting of the ZnSe and the ZnSe-like LO phonons of the ZnSe/ Cd0.2Zn0.8Se quantum wires was observed. The size of this splitting was found to depend only on the wire width and not on the temperature. This behavior is due to the strain relaxation, which occurs at the edge zone of each quantum wire. The increasing influence of the edge zone for decreasing wire width is the reason for the wire width dependence of the splitting between the ZnSe and the ZnSe-like LO phonon. As a result, the importance of partial strain relaxation for the discussion of the vibronic properties of the patterned semiconductor systems was confirmed. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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