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  • American Institute of Physics (AIP)  (23)
  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 7615-7615 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    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 90 (1989), S. 1313-1321 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Fluorescence excitation spectra are reported for several J'≠0 rotational members of the 000 band of the S1(1B3u)←S0(1A1g) electronic transition of pyrazine at a resolution of about 10 MHz. The transitions studied, namely R(0)–R(2) and P(2)–P(4), are each split into a large number of sharp lines ascribed, as in the case of the previously studied P(1) (J'=0) transition, to coupling with the lowest triplet state T1(3B3u). Despite this complexity, we show in this paper that it is possible to separate the lines into clusters of transitions that terminate in the same K' component of the electronically excited, mixed S1–T1 state. This demonstrates that K' is a good quantum number, at least at low J' in the zero-order S1 state. From this analysis, we determine the rotational constants of the S0 and S1 states. We also determine: (i) the relative cluster intensities; (ii) the coupled T1 level densities; and (iii) by using standard deconvolution techniques, the S1–T1 coupling matrix elements, each as a function of J',K'. Cluster intensities decrease with increasing J', but K'=0 clusters are significantly less intense than K'≠0 clusters in the fluorescence excitation spectra. Observed triplet level densities in each cluster exceed by an order of magnitude the calculated density of rovibronic states if selection rules appropriate to the D2h point group are taken into account. Neither the observed level densities nor the coupling matrix elements (which vary from less than 5 MHz to more than 500 MHz) show a clear-cut systematic dependence on J' or K', although K'=0 levels appear to be more strongly coupled than K'≠0 levels. Possible explanations for these results and their implications for intersystem crossing dynamics in the isolated molecule are discussed.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 1362-1367 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A rotationally resolved fluorescence excitation spectrum of the 000 band in the A 1A'←X 1A' (S1←S0) transition of 1-fluoronaphthalene, at ∼3138 A(ring), has been observed using a newly constructed laser spectrometer operating in the ultraviolet. The band in question is a hybrid band exhibiting 75% a-type and 25% b-type character, and consists of ∼4000 lines at a rotational temperature of 9 K, each with a FWHM=3 MHz, all of which have been assigned. The band origin is at 31 866.508±0.002 cm−1 (vac), and the rotational constants are A‘=1920.6, B‘=1122.2, C‘=708.5, A'=1891.5, B'=1102.1, and C'=696.6±0.1 MHz. The S1←S0 optical transition moment is rotated away from the a inertial axis by an angle of ±30°, an effect that could have dynamic consequences. Some operating characteristics of the spectrometer are described.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 2169-2184 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The low energy portion of the high resolution S1←S0 fluorescence excitation spectrum of benzophenone recently reported by Holtzclaw and Pratt [J. Chem. Phys. 84, 4713 (1986)] is modeled here using a simple two-degree-of-freedom vibrational Hamiltonian. The Hamiltonian features a 1:1 nonlinear resonance between the two low frequency ring torsional modes of the molecule in its S1 state. Line positions and intensities of the two major spectral progressions are well reproduced using parameters similar to those derived from earlier matrix diagonalizations. The comparison of the theory and experiment results in a determination of the displacement of the S1 surface relative to the ground electronic state along the symmetric torsional coordinate and permits a calculation of the excitation spectra of various isotopically substituted molecules not yet measured in the laboratory. A clear picture of the relationship between the dynamics on the S1 surface and the spectroscopy of benzophenone is revealed by comparing a time domain analysis of the experimental data with wave packet dynamics on the model S1 surface. This comparison provides new insight into energy flow in the isolated molecule and permits a qualitative simulation of the effects of collisional quenching on the fluorescence spectrum. We also discuss, using a classical trajectory analysis, the resonance dynamics of the torsional modes and note the existence of heretofore undetected local modes in the high resolution spectrum.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 113 (2000), S. 3658-3669 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved fluorescence excitation spectra of several torsionally active bands in the S1–S0 electronic transitions of toluene and toluene-d3 have been recorded in the collision-free environment of a molecular beam. Analyses of these data provide accurate values of the internal rotor constants F; the barrier heights V6; the frame rotational constants AF; the overall rotational constants B and C; and the torsion-rotation coupling constants AF′; in the m=0 and m=±1 levels of the S0 state and the m=0, ±1, and 3+ levels of the S1 state. Comparison of the AF, B, and C values in the m=0 levels of the two states shows that S1 toluene is quinoidal in form, with shorter ring "parallel" C–C bonds than "perpendicular" ones, unlike the S0 state. The preferred conformation of the methyl group is staggered in both states, but the V6 values are significantly different; V6(S0)=−4.874 and V6(S1)=−26.376 cm−1. Comparison of the F, AF, and AF′ values in the different torsional levels of the S1 state shows that, below the barrier, the methyl group tilts and the ring bond lengths change with increasing displacements along the torsional coordinate. Above the barrier, the precessional motion of the CH3 is quenched but larger ring distortions are observed. Thus, the data are consistent with an enhanced hyperconjugative interaction between the benzene ring and the methyl group in the S1 state. This interaction is substantially modulated by the relative motion of the two attached groups, providing a facile route to IVR. © 2000 American Institute of Physics.
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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. 11147-11156 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved S1←S0 electronic spectra of the nitrogen complex of aniline have been observed. The spectra are split into two subbands due to internal rotation of N2. The analysis of the rotational constants reveals that N2 is located above the ring plane of aniline and in the symmetry plane of aniline in the equilibrium position. Barriers hindering internal rotation have been obtained from fitting experimental transitions frequencies using a semirigid C2v top–Cs frame internal rotation model. Upon excitation into S1, the distance of N2 to the ring decreases and the internal rotation barrier increases by a factor larger than 2. Possible reasons for this behavior are discussed. © 2001 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 1874-1883 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Several vibronic bands that appear within 300 cm−1 of the electronic origin in the S1←S0 fluorescence excitation spectrum of 1-naphthoic acid (1NA) and carboxyl-deuterated 1NA have been examined at full rotational resolution. The data show that all bands belong to the s-cis isomer of 1NA. They also show that all bands are torsional in nature; i.e., that they involve displacements along either the S0 or the S1 carboxyl torsional coordinate, φ, or both. Unambiguous assignments of the bands follow from the observed inertial defects, from which the torsional potential energy surfaces of both electronic states are derived. In S0 s-cis-1NA, the naphthalene and carboxyl groups are not coplanar. The s-cis minima are at φ=±17°; the barrier to planarity is 13.2 cm−1. In contrast, S1 s-cis-1NA is a completely planar molecule, with φ=0°. The barrier for s-cis to s-trans isomerization is ∼1450 cm−1 in the S0 state and ∼2200 cm−1 in the S1 state. The validity of the two derived potential energy surfaces of s-cis-1NA has been tested by comparing the observed inertial defects with those computed using the torsional eigenfunctions. Excellent agreement is obtained, confirming the one-dimensional approach employed.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 7061-7067 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Based on a study of the high resolution S1←S0 fluorescence excitation spectrum of p-toluidine (p-methylaniline) and related G12 molecules, we propose that the threefold axis of the methyl group is tilted slightly with respect to the symmetry axis of the molecular frame, and exhibits a kind of precessional motion in the course of its hindered internal rotation. We derive a new Hamiltonian to describe this motion and show that it is consistent with previous modifications of the traditional torsion–rotation Hamiltonian first proposed by Wilson, Lin, and Lide [J. Chem. Phys. 23, 136 (1955)]. Applying the new Hamiltonian to the S1←S0 spectrum of p-toluidine, we have determined the sixfold barrier heights V6(S0) = ( − ) 5.6 and V6(S1) = ( − ) 43.9 cm−1, values that are similar to those of toluene and other 4-substituted toluenes.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 8454-8461 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved fluorescence excitation spectra of several vibronic bands in the S1←S0 electronic transitions of styrene (STY) and phenylacetylene (PA) have been obtained. Confirming earlier low resolution results, we find that the origin band of PA is a b-type band but that the corresponding band of STY is an a-type band, showing that the S1 state of PA is 1Lb in character (like that of most other monosubstituted benzenes) but that the corresponding state of STY is 1La. The observed changes in the rotational constants of PA and STY that occur when the photon is absorbed are consistent with these assignments. Reversal in the electronic character of the S1 state in STY is attributed to the presence of the "off-axis" conjugating –CH(Double Bond)CH2 group, a suggestion that is supported by the observed polarizations of higher vibronic bands in both molecules. © 1999 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 3229-3236 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A rotational analysis of three vibronic bands (000, 720, and 510) in the phosphorescence excitation spectrum of glyoxal (CHO–CHO) has been performed. From this analysis we deduce the rotational, spin-rotation, and spin–spin (plus spin-orbit) constants of the lowest triplet state of the isolated molecule. 3Au glyoxal has been shown to exist in nearly the same trans-planar (C2h) configuration as the lowest excited singlet state. Both geometries are very similar to that of the ground state. The dynamic implications of these structural findings are discussed. We also compare the spin splittings determined in this work with those previously measured in the condensed phase, using optically detected magnetic resonance methods.
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