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  • 2000-2004  (6)
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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 113 (2000), S. 7982-7987 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Previous studies of the hydrogen abstraction from vibrationally excited H2O and HCN by various atoms have probed the vibrational and rotational energy of the product containing the surviving bond to assess the energy disposal and determine the mechanism of the reaction. Estimating the relative translational energy of the products from the Doppler broadening of the probe transitions has allowed the inference of the internal energy of the unobserved product containing the new bond using conservation of energy. The experiments presented here directly measure the vibrational and rotational energy of both the OH product (containing the new bond) and OD product (containing the old bond) from the reaction of O atoms with HOD having four quanta of O–H stretching excitation (4νOH). All of the OH products are vibrationally excited, being formed almost exclusively in ν=2. Nearly all of the OD products are vibrationally unexcited, with 93% in v=0 and only 7% in v=1. The results are consistent with a spectator picture of the reaction in which the new bond receives most of the available energy. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 113 (2000), S. 5018-5025 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Transient electronic absorption of methylene iodide (CH2I2) in CCl4, CDCl3, and C6D6 after excitation of two quanta of C–H stretching vibration with a 100 fs laser pulse allows direct observation of the times for intramolecular vibrational relaxation and energy transfer to the solvent. Intramolecular energy redistribution populates vibrational states with larger Franck–Condon factors for the electronic transition, leading to an increased absorption of probe pulses in the wavelength range of 380–440 nm. A model based on the temperature dependence of the electronic absorption coefficient describes the transient absorption well for all wavelengths. In the model, the temperature rises and decays exponentially with time, reflecting the initial redistribution of energy within the excited molecule and the subsequent transfer of energy from the vibrationally excited molecule into the solvent. The intramolecular vibrational relaxation time for CH2I2 is essentially the same in the solvents CCl4 (10.8±1.5 ps) and CDCl3 (11.2±2.0 ps) and is only slightly shorter in C6D6 (8.0±1.5 ps). Energy transfer to the solvent takes longer, occurring with a time constant of 68±10 ps for CCl4, 51±10 ps for CDCl3, and 23±2 ps for C6D6. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 6678-6688 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The combination of vibrationally mediated photofragment yield spectroscopy, which excites molecules prepared in single vibrational states, and multiphoton fluorescence spectroscopy, which excites molecules cooled in a supersonic expansion, provides detailed information on the energetics and vibrational structure of the first excited singlet state (S1) of isocyanic acid (HNCO). Dissociation of molecules prepared in individual vibrational states by stimulated Raman excitation probes vibrational levels near the origin of the electronically excited state. Detection of fluorescence from dissociation products formed by multiphoton excitation through S1 of molecules cooled in a supersonic expansion reveals the vibrational structure at higher energies. Both types of spectra show long, prominent progressions in the N–C–O bending vibration built on states with different amounts of N–C stretching excitation and H–N–C bending excitation. Analyzing the spectra locates the origin of the S1 state at 32 449±20 cm−1 and determines the harmonic vibrational frequencies of the N–C stretch (ω3=1034±20 cm−1), the H–N–C bend (ω4=1192±19 cm−1), and the N–C–O bend (ω5=599±7 cm−1), values that are consistent with several ab initio calculations. The assigned spectra strongly suggest that the N–C stretching vibration is a promoting mode for internal conversion from S1 to S0. © 2000 American Institute of Physics.
    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 116 (2002), S. 4955-4961 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Vibrationally mediated photodissociation action spectroscopy provides rotation-vibration spectra of jet-cooled ammonia in the 2.3 μm and 3.0 μm regions by detecting the emission of electronically excited NH2(A˜ 2A1) produced by the photodissociation of the vibrationally excited molecules. Vibrational excitation changes the relative photofragmentation yield of NH2(A˜ 2A1) markedly. Isoenergetic photolysis of ammonia molecules with one quantum of antisymmetric N–H stretching excitation (ν3) or two quanta of bend (2ν4) yields three times more excited state NH2(A˜ 2A1) than photolysis of NH3 with a quantum of symmetric N–H stretch excitation (ν1). By contrast, the relative yield is insensitive to initial vibrational excitation of the combination bands ν1+ν2 and ν2+ν3 that contain the umbrella (inversion) motion ν2. The vibrational mode dependence of the NH2(A˜ 2A1) photofragment yield arises from either enhanced Franck–Condon factors for electronic excitation or from an increased probability for the competing nonadiabatic dissociation to form the ground state NH2(X˜ 2B1) product. © 2002 American Institute of Physics.
    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 114 (2001), S. 10835-10844 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Direct observation of all three photofragmentation channels of HNCO gives the relative yields of 3NH+CO, H+NCO, and 1NH+CO at nine different photolysis energies for both thermal and vibrationally excited molecules. Each higher energy channel dominates as it becomes accessible, but vibrational excitation changes the relative yield of 1NH markedly. Photolysis of HNCO(3ν1) at the same total energy yields up to 2.5 times more NCO with a corresponding reduction in 1NH. The relative yield of 3NH and NCO, however, is indifferent to vibrational excitation. The dependence of the yields on vibrational excitation supports a picture in which direct decomposition on the S1 surface produces 1NH+CO and in which internal conversion to S0 leads to H+NCO, by spin-allowed unimolecular decay, and to 3NH+CO, by intersystem crossing and decomposition on T1. The observed vibrational enhancement of the NCO yield is consistent with vibrational excitation impeding the decomposition to 1NH+CO on S1 and, thus, increasing the number of molecules that cross to S0 and decay to H+NCO. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 115 (2001), S. 7086-7093 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Wavelength dependent, transient, electronic absorption spectroscopy of methylene iodide (CH2I2) in CCl4, CDCl3, C6D6, and (CD3)2CO following excitation of the fundamental C–H stretching vibration reveals the time scales of intramolecular vibrational energy redistribution and energy transfer to the solvent. In contrast to the case for overtone excitation, state-specific relaxation to one or a few states that are coupled by low order interactions with the initially prepared state dominates the intramolecular vibrational energy redistribution. This mechanism is consistent with previous infrared pump–probe measurements of CH2I2 fundamental relaxation as are the measured relaxation time scales. We also find a previously unobserved relaxation pathway through weakly-coupled states that have several quanta of excitation in the Franck–Condon active modes, primarily C–I stretch and bend. Although this statistical component is a minor channel in the relaxation, it is the only contribution to the signal at the longest probe wavelengths in CCl4 and CDCl3. Time scales for both intramolecular energy redistribution and intermolecular relaxation to the solvent depend strongly on the strength of interaction with the solvent. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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