2018
DOI: 10.1016/j.jqsrt.2018.08.023
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Ab initio line-shape calculations for the S and O branches of H2 perturbed by He

Abstract: Highlights• Close-coupling calculations of pressure broadening and shifting coefficients • Close-coupling calculations of Dicke parameters • Data for anisotropic Raman S (j=0-5) and O (j=2-5) lines for purely rotational transitions, fundamental band and first four overtones

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Cited by 22 publications
(37 citation statements)
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“…Quantum-mechanical calculations of collisional dephasing have been performed for numerous systems [13,26], including CO-Ar [20,21,27,28]. In contrast, treatments accounting for both dephasing and the effects of VCs were mostly limited to the hydrogen molecule and its isotopologues [19,22,[29][30][31], which are not representative of systems relevant to atmospheric studies.…”
Section: Introductionmentioning
confidence: 99%
“…Quantum-mechanical calculations of collisional dephasing have been performed for numerous systems [13,26], including CO-Ar [20,21,27,28]. In contrast, treatments accounting for both dephasing and the effects of VCs were mostly limited to the hydrogen molecule and its isotopologues [19,22,[29][30][31], which are not representative of systems relevant to atmospheric studies.…”
Section: Introductionmentioning
confidence: 99%
“…For the H 2 -He system, the PES is three-dimensional; i.e., it depends on the distance between the center of mass of the hydrogen molecule and the helium atom, R, the intramolecular distance, r, and the angle between the inter-and intramolecular axes, θ. To carry out the close-coupling quantum scattering calculations [66], the PES is projected on Legendre polynomials and averaged over the rovibrational wave functions of the hydrogen molecule [3,32]. The generalized spectroscopic cross-sections, σ q λ , for the electric quadrupole lines considered here (q = 2), as functions of the initial kinetic energy, E KIN , are determined from S-matrix elements [32,60,64].…”
Section: Methodsmentioning
confidence: 99%
“…To carry out the close-coupling quantum scattering calculations [66], the PES is projected on Legendre polynomials and averaged over the rovibrational wave functions of the hydrogen molecule [3,32]. The generalized spectroscopic cross-sections, σ q λ , for the electric quadrupole lines considered here (q = 2), as functions of the initial kinetic energy, E KIN , are determined from S-matrix elements [32,60,64]. For the zero rank of the velocity tensor, λ = 0, σ q λ reduces to the pressure broadening and shift cross-sections (PBXS and PSXS, respectively) [3,65,67,68], while for λ = 1 it provides the complex Dicke cross-section [31,32,59,60,64] (RDXS and IDXS for its real and imaginary parts, respectively).…”
Section: Methodsmentioning
confidence: 99%
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“…We extend the calculations of the generalized spectroscopic cross sections reported in Refs. [15,26] by taking into account the centrifugal distortion for all the bands and by including the hot bands. We extrapolate the ab initio results to populate very weak lines, i.e., higher overtones, v ≥ 6, higher rotational numbers, J ≥ 8, and high-v hot bands, v ≥ 6; following the standard HITRAN notation, we denote the final and initial states of a transition with primes and double primes, respectively.…”
Section: Introductionmentioning
confidence: 99%