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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 4699-4713 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: By utilizing the lineshape theory of Shafer and Gordon [J. Chem. Phys. 58, 5422 (1973)], pure rotational pressure broadening and shifting coefficients for the infrared spectral lines of HF in He have been calculated using the close-coupled (CC) method, the centrifugal sudden (CS) approximation, and the corrected centrifugal sudden (CCS) approximation of McLenithan and Secrest [J. Chem. Phys. 80, 2480 (1987)]. Comparison of the results obtained from these three methods were made at the total angular momentum dependent, kinetic energy dependent, and temperature dependent levels. In the latter comparisons, a semiclassical method was also included. The CS results agree very well with the CC calculations for the pressure broadening coefficients, but deviate slightly for the pressure shifting coefficients. The CCS results were essentially identical to those obtained from the CS approximation calculations. The semiclassical method was accurate to within about 15% of the CC values for the pressure broadening coefficients. The pressure shifting coefficients have been found to be very sensitive to the number of closed channels included in the calculations. As well, while collisionally inelastic contributions to the effective cross sections were not found to be negligible, their effect on the final calculated pressure broadening and shifting coefficients was found to be insignificant for this particular system at room temperature.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 4112-4129 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A series of centrifugal sudden (CS) and infinite-order sudden (IOS) approximations together with their corrected versions, respectively, the corrected centrifugal sudden (CCS) and corrected infinite-order sudden (CIOS) approximations, originally introduced by McLenithan and Secrest [J. Chem. Phys. 80, 2480 (1987)], have been compared with the close-coupled (CC) method for the N2–He interaction. This extends previous work using the H2–He system [J. Chem. Phys. 93, 3931 (1990)] to an interaction which is more anisotropic and more classical in nature. A set of eleven energy dependent cross sections, including both relaxation and production types, has been calculated using the LF- and LA-labeling schemes for the CS approximation, as well as the KI-, KF-, KA-, and KM-labeling schemes for the IOS approximation. The latter scheme is defined as KM=K=max(kj,kjI). Further, a number of temperature dependent cross sections formed from thermal averages of the above set have also been compared at 100 and 200 K. These comparisons have shown that the CS approximation produced accurate results for relaxation type cross sections regardless of the L-labeling scheme chosen, but inaccurate results for production type cross sections. Further, except for one particular cross section, the CCS approximation did not generally improve the accuracy of the CS results using either the LF- or LA-labeling schemes. The accuracy of the IOS results vary greatly between the cross sections with the most accurate values given by the KM-labeling scheme. The CIOS approximation generally increases the accuracy of the corresponding IOS results but does not completely eliminate the errors associated with them. For some cross sections, the CIOS results are more accurate than the corresponding CS or CCS results.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 3931-3949 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A detailed examination is made of the corrected centrifugal sudden (CCS) approximation originally introduced by McLenithan and Secrest [J. Chem. Phys. 80, 2480 (1987)]. A brief review of the method is given, and comparisons are made between eleven energy dependent cross sections calculated using the exact quantum mechanical close-coupled (CC), centrifugal sudden (CS) and corrected centrifugal sudden (CCS) procedures for the H2–He system. Further, three L-labeling choices, initial, final, and average L-labeling, are compared within the CS and CCS approximations. The energy dependent cross sections include those of both the relaxation and production type used in the description of the shear viscosity, thermal diffusion and thermal conductivity and their magnetic field-effects. These cross sections are then thermally averaged, and comparisons are again made at the temperature dependent level. These studies show that the CCS approximation provides significantly improved results over those of the CS approximation for the average L-labeling scheme, but provides poorer results for the initial and final L-labeling schemes.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 5907-5918 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The relaxation of hydrogen and deuterium nuclei in HD–He gas mixtures is studied both experimentally and theoretically in the temperature range 90–300 K. A rationalization is given for the temperature dependence of the proton and the deuteron relaxations in terms of the relative strengths of the proton and deuteron intramolecular couplings and the role played by those HD molecules in the ground rotational state. Using a recent ab initio potential, quantitative agreement is found between the temperature dependence of the spin–lattice relaxation time of the proton in HD, as calculated theoretically and determined experimentally. A similar comparison between the calculated and experimental temperature dependence of the spin–lattice relaxation time of the deuteron in HD gave only semiquantitative agreement. It is suggested that the difference in quantitative agreement may be attributed to the selectivity of the respective predominant relaxation mechanisms to slightly different aspects of the anisotropic components of the interaction potential.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 7125-7135 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: This paper examines the role of the potential surface of the rigid rotor He–H2 system upon a variety of transport and relaxation cross sections, including some involving field effects. The technique of functional sensitivity analysis is used to explore these issues. Three different levels of cross sections were studied: microscopic, thermally averaged, and effective cross sections. The cross sections studied were found to be sensitive to differing components of the potential energy surface, with some cross sections being more sensitive to either the slope or the magnitude of the potential components. The degree of information loss in the progression from microscopic to bulk observables is highly dependent on the individual phenomenon.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 4699-4712 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A detailed comparison of the predictive powers of two recently determined potential energy surfaces [J. Chem. Phys. 88, 5465 (1988); 89, 3505 (1988)] for the N2–Ne interaction has been carried out. In particular, the following has been tested: calculations using these two surfaces against experimental values of the total differential scattering cross section at 75.8 meV, the temperature dependence of the interaction second virial coefficient over the range 90 K to 323 K, the temperature dependence of the binary diffusion coefficient and the mixture viscosity over the range 280 K to 973 K, the mixture thermal conductivity at 300 K, and viscosity and thermal conductivity field-effects, rotational relaxation, and collision-broadening of the depolarized Rayleigh line over a restricted temperature range. Forty-five effective cross sections that determine the bulk transport and relaxation phenomena have been calculated by classical trajectory methods for temperatures varying from 77.5 K to 973 K. Second-approximation calculations of the mixture transport phenomena using these calculated cross sections give impressive agreement with the experimental results over a wide temperature range for both potential surfaces. While one potential gives better agreement with the scattering data, the second virial coefficient data, the bulk transport data, and the depolarized Rayleigh collision-broadening data than does the other potential, the opposite is true for the rotational relaxation and field-effect data.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 5754-5761 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Measurements of the nuclear magnetic resonance (NMR) longitudinal relaxation time T1 have been carried out for D2–He gas mixtures at temperatures of 293 and 220 K for two concentrations of D2 in He and the results extrapolated linearly to infinite dilution at each temperature. Full quantum close-coupled scattering calculations have also been carried out for an ab initio D2–He interaction potential. The agreement found between measured and calculated relaxation times is excellent at 293 and good at 220 K. Based on the level of agreement found between theory and experiment, it can be concluded that the molecular hydrogen–helium ab initio potential energy surface employed in the present D2–He calculations as well as in earlier H2–He calculations [J. Chem. Phys. 81, 5275 (1984)] represents well the effects of both the spin–rotation and combined dipolar/quadrupolar intramolecular interactions, which dominate the spin relaxation, respectively, of protons and deuterons in the hydrogen isotopes. At the same time, the present results indicate that the disagreement found earlier [J. Chem. Phys. 92, 5907 (1990)] between calculated and measured deuteron T1 values for HD–He mixtures must arise from the specific nature of the HD–He potential energy surface.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 9304-9312 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Pure rotational spectra have been calculated for the three isotopomers of the Cl2–Ar van der Waals complex formed by Cl2 in its ground electronic state. The potential energy surface involved is a sum of pairwise Morse atom–atom interactions, which are merged asymptotically into an anisotropic van der Waals form. The Morse atom–atom interactions have been refined by adjusting their parameters to obtain agreement with both excitation spectra and recent microwave transitions observed for the 35Cl2–Ar van der Waals complex, whereas the anisotropic long-range part of the potential surface has been taken from ab initio results [Mol. Phys. 80, 533 (1993)]. The present model potential surface predicts a T-shaped structure for the complex, in agreement with experiment. Excellent agreement has been found between the calculated and experimental microwave transition frequencies for the 35Cl37Cl–Ar complex. Good agreement has also been found between the experimentally determined bond energy, bond length, and average "bond angle'' governing the overall geometry of the complex and the corresponding quantities determined from dynamical calculations based upon the present potential surface. The new potential surface has also been utilized to predict the microwave spectrum of the 37Cl2–Ar isotopomer. © 1996 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 5752-5760 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An earlier anisotropic N2–Kr potential energy surface [Chem. Phys. Lett. 88, 197 (1982)] of Lennard-Jones form, obtained by inversion of molecular beam differential scattering data, has been found to provide calculated transport–relaxation phenomena in good agreement with experiment, but leads to calculated second interaction virial coefficients which are significantly too low, and does not provide adequate agreement with recent microwave van der Waals spectral data. A modification of this surface to include a recent ab initio determination of the C6 dispersion coefficient, and to bring in the virial and microwave data, gives a new potential surface that is in good agreement with all available experimental data. © 1995 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 103 (1995), S. 8477-8491 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An exchange–Coulomb model potential energy surface has been developed for the N2–Ar interaction. This potential energy surface is based upon recent results for the Heitler–London interaction energy, long-range dispersion energies, the temperature dependencies of interaction second virial, binary diffusion, and mixture shear viscosity coefficients, microwave spectra of the van der Waals complex, and collision broadening of the depolarized Rayleigh light scattering spectrum. The adjustable parameters in the final potential surface have been determined by fitting the temperature dependence of the virial coefficient (within experimental uncertainties) and the frequencies of three representative lines of the microwave spectrum of the 14N2–Ar van der Waals complex. A fine tuning of these parameters was achieved by considering the temperature dependence of the binary diffusion and mixture shear viscosity coefficients. Calculated frequencies for all observed microwave transitions of the various N2–Ar isotopomers lie within 0.1% of the experimental values. Excellent agreement is obtained with experimental values of binary diffusion and mixture shear viscosity data for all temperatures and compositions. Agreement with the bulk gas relaxation phenomena, while not outstanding, is acceptable, given the accuracy with which these phenomena are currently determinable. Detailed comparisons are made with predictions of the two best literature N2–Ar potential energy surfaces. This new potential surface gives the best overall agreement with experiment for N2–Ar mixtures. © 1995 American Institute of Physics.
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