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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 86 (1982), S. 507-514 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 94 (1990), S. 6-8 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , 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 95 (1991), S. 7862-7871 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A rotationally resolved fluorescence excitation spectrum of the O00 band in the S1←S0 transition of 2,3-dimethylnaphthalene has been obtained using a cw laser/molecular beam spectrometer. More than 3000 lines were observed, each exhibiting a width of about 3 MHz. Despite the proximity of the two methyl groups, the observed rotational structure can be interpreted satisfactorily using an uncoupled rotor model. However, extensive torsion–rotation interactions are observed. Accurate measurements of these perturbations are used to determine the effective threefold hindering potentials in both electronic states, V3(S0)=652 cm−1 and V3(S1)=391 cm−1, respectively. Rotor–rotor couplings do influence these barriers as well as the patterns of lines observed in the rotationally resolved spectra of higher vibronic bands.
    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 93 (1990), S. 2258-2273 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Both fluorescence excitation and dispersed emission techniques have been used to study the S1←S0 electronic spectra of 1- and 2-hydroxynaphthalene (1/2HN) in the collision-free environments of a supersonic jet and a twice-skimmed molecular beam, using both pulsed and high-resolution cw lasers operating in the ultraviolet. In the jet experiments, we observe that each molecule exhibits two electronic origins, separated by 274 cm−1 in 1HN and by 317 cm−1 in 2HN. In the beam experiments, we resolve the rotational structure of each of the four bands and determine the inertial constants of all eight zero-point vibrational levels, accurate to ±0.1 MHz. We also determine the orientations of the four optical transition moments in the molecular frame. Significant differences in both the inertial constants and the transition moment orientations are observed in each band. Similar experiments have been performed on the hydroxy-deuterated 1/2HN (1/2DN).A comparison of the results obtained for 1/2DN with those for the corresponding bands in 1/2HN makes possible the determination of the center-of-mass coordinates of the hydroxy hydrogen in both electronic states, accurate to ± 0.02 A(ring). Differences in these coordinates reveal that the two electronic origins in each spectrum are caused by the presence of two N–O–H(D) rotamers in both 1H(D)N and 2H(D)N, one with a cis (or syn) geometry and one with a trans (or anti) geometry with respect to the naphthalene frame. We make an unambiguous assignment of each origin to a specific rotamer. The lower energy origin in the spectrum of 1HN is that of the cis rotamer, whereas the lower energy origin in the spectrum of 2HN is that of the trans rotamer. We then use these results, together with those of ab initio calculations on the ground electronic states of all four isomers, to explore the reasons for the differences in their energies, to account for the orientations of their transition moments, and to specify other features of the S0 and S1 potential energy surfaces along the cis–trans isomerization coordinate. Motion along this coordinate requires significant displacement of the oxygen atom and selected ring hydrogens as well as rotation about the C–O bond, in both electronic states.
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  • 5
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Two types of splittings have been observed in the rotationally resolved fluorescence excitation spectrum of the 000 band in the S1 ←S0 electronic transition of 1-methylnaphthalene at ∼315 nm. One type is independent of J and K−1 and is produced by small differences in the A/E methyl torsional level spacings in the two electronic states. The second type is independent of J but dependent on K−1. It has its origin in a coupling of the methyl torsion with overall molecular rotation, which produces even smaller differences in the spacings of the S0 and S1 E levels. A simultaneous fit of both types of splittings yields the threefold barrier heights in the zero-point vibrational levels of both states, V3 (S0 )=295.2 and V3 (S1 )=292.6 cm−1. The ground state value of V3 is very different from that which has been reported earlier.
    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 94 (1991), S. 7721-7733 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved fluorescence excitation spectra of three vibronic bands in the S1←S0 transitions of 1- and 2-methylnaphthalene (1 and 2MN) have been obtained. Each band exhibits perturbations that are produced by an interaction between the restricted torsional motion of the attached methyl group and the overall rotational motion of the entire molecule. A complete analysis of these effects yields values of the torsional barrier heights, the rotational constants, and the torsion–rotation perturbation coefficients of all vibronic levels that participate in the transitions. These values depend significantly on the position of the methyl group attachment, on the electronic state of the naphthalene chromophore, and on its vibrational state, as well. For example, V3 (the threefold torsional barrier) decreases from 809 cm−1 in 00 1MN to 128 cm−1 in 00 2MN. D (the largest first-order torsion–rotation perturbation term) increases from 0.03 MHz in 00 1MN to 406 MHz in 00 2MN, a change of more than 4 orders of magnitude. The V3 values of 00 and 8¯1 1MN are 563 and ≤ 373 cm−1, respectively. A full discussion of these dynamically relevant effects and their dependence upon both electronic and geometric factors is given.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 8026-8036 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A unique view of the nascent acid-base reaction between 2-naphthol and ammonia along the proton transfer coordinate is provided by analyses of the rotationally resolved S1←S0 electronic spectra of their hydrogen bonded complexes cis- and trans-2HNA in the gas phase. Both complexes, in both electronic states, have structures in which ammonia, acting as a base, forms an in-plane hydrogen bond with the hydroxy hydrogen atom of 2-naphthol. The ground state O–H⋅⋅⋅N heavy atom separations are R=2.77 A(ring) in cis-2HNA and R=2.79 A(ring) in trans-2HNA. Electronic excitation of the significantly more acidic S1 state of 2-naphthol produces large decreases in R in both complexes. S1 cis-2HNA has R=2.62 A(ring) and S1 trans-2HNA has R=2.57 A(ring). Comparing these results to the Lippincott–Schroeder potential for the hydrogen bond shows that there is little change in the vibrationally averaged position of the hydroxy hydrogen atom. But decreasing R produces significant decreases in the barrier to proton transfer, in the distance from reactant to product along the reaction coordinate, and in the energy difference between them. We thus conclude that whether or not such transfer occurs is primarily dependent on the ability of the two heavy atoms to come into close proximity during the early stages of the reaction, a condition that is not satisfied in either cis- or trans-2HNA, in either electronic state. This view is supported by observed changes in the shapes of the potential surfaces along the NH3 torsional coordinate that occur on S1←S0 excitation of the two complexes.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 8732-8743 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rotationally resolved fluorescence excitation spectra of two vibronic bands in the S1←S0 electronic transition of 2-hydroxypyridine (2HP), and of the corresponding bands in the hydroxy-deuterated molecule, have been obtained. A comparison of the rotational constants of the two molecules shows that the two bands both originate in the zero-point vibrational level of the planar keto tautomer of 2HP, 2-pyridone (2PY), and terminate in different zero-point levels of 2PY that have different out-of-plane equilibrium geometries at nitrogen. Additionally, all four bands exhibit "anomalous'' rotational line intensities that are shown to result from an in-plane inertial axis reorientation which occurs on absorption of the photon. Likely atomic displacements that are responsible for this "rotational'' Duschinsky effect, which may have significant dynamical consequences in 2PY and other molecules, are discussed.
    Type of Medium: Electronic Resource
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  • 9
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have observed, and assigned, the fluorescence excitation spectrum of the 000 band in the 1B1←1A1 electronic transition of pyrimidine, at a resolution of ∼10 MHz. The rotational constants of the 1B1 state, the lowest excited singlet state, are A'=6352±3, B'=5853±3, and C'=3042.0±0.5 MHz. The magnitudes of these constants are not very different from those of the ground (1A1) state. However, the in-plane a and b inertial axes in the 1B1 state are rotated by 90° with respect to those of the 1A1 state. The spectrum also exhibits numerous perturbations, evidenced by the presence of extra lines, anomalous intensities and lifetimes, and shifts of the main lines from their expected positions. The perturbations are strongly magnetic-field dependent, demonstrating that they arise from an intramolecular coupling of the 1B1 state with nearly isoenergetic rovibronic levels of a lower triplet (3B1) state. Models are proposed to account for this behavior based on a deconvolution of the experimental spectrum and simulations of the observed Zeeman effects. The most satisfactory interpretation of the data (in the language of the zero-order states) is obtained if it is assumed that a single rovibronic 1B1 level is spin–orbit coupled to one or a few 3B1 levels, which in turn are coupled via rotationally dependent Coriolis interactions to a dense manifold of background levels, probably those of the 1A1 state. Because the latter coupling is small, typically less than the linewidths in the spectra, it is manifested only in a K'+1 dependence of the lifetimes of selected molecular eigenstates and the reduced g values required to fit the magnetic-field dependence of their spectra.
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  • 10
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 95 (1973), S. 4057-4059 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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