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Physical Chemistry Chemical Physics
Volumn 9, Issue 42, 2007, Pages 5664-5671
On the origin of the forward peak and backward oscillations in the F + H2(v = 0) → HF(v′ = 2) + H reaction
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EID: 35448999633     PISSN: 14639076     EISSN: None     Source Type: Journal    
DOI: 10.1039/b709427b     Document Type: Article
Times cited : (43)
References (26)
  • 14
    • 35448990987 scopus 로고    scopus 로고
    • In the same sense, the complex energy poles present a tool better suited for the analysis of scattering of wavepackets at a fixed angular momentum, which involves integration over the collision energy
    • In the same sense, the complex energy poles present a tool better suited for the analysis of scattering of wavepackets at a fixed angular momentum, which involves integration over the collision energy
  • 21
    • 35448957800 scopus 로고    scopus 로고
    • n have peaks which disappear in the coherent sums of the two terms. In principle, one can simultaneously remove this peak behaviour, e.g. by introducing the amplitudes defined by different expressions in different angular regions. This would, however, complicate the theory by making it non-analytic. Also, there is no unique prescription for decomposing the unfolded amplitude f into a resonance and non-resonance parts in the transitional region (see ref. 10)
    • n have peaks which disappear in the coherent sums of the two terms. In principle, one can simultaneously remove this peak behaviour, e.g. by introducing the amplitudes defined by different expressions in different angular regions. This would, however, complicate the theory by making it non-analytic. Also, there is no unique prescription for decomposing the unfolded amplitude f into a resonance and non-resonance parts in the transitional region (see ref. 10)
  • 22
    • 35449004199 scopus 로고    scopus 로고
    • Note, however, that the quality of the Padé reconstruction has been improved in this work. In particular, a larger number energy points have been used, and the 3D plots in Figs. 4 and 5 are less noisy than Fig. 9 of ref. 5
    • Note, however, that the quality of the Padé reconstruction has been improved in this work. In particular, a larger number energy points have been used, and the 3D plots in Figs. 4 and 5 are less noisy than Fig. 9 of ref. 5
  • 23
    • 35448980479 scopus 로고    scopus 로고
    • n) ≈ 0. In both cases the integration over λ in eqn (19) cannot be extended to -∞ as was assumed in deriving eqn (8) and (9)
    • n) ≈ 0. In both cases the integration over λ in eqn (19) cannot be extended to -∞ as was assumed in deriving eqn (8) and (9)
  • 24
    • 35448951451 scopus 로고    scopus 로고
    • R
    • R

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.