Multiple scattering mechanisms causing interference effects in the differential cross sections of H + D2 → HD(v' = 4, j') + D at 3.26 eV collision energy (original) (raw)

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Measurement of the state‐specific differential cross section for the H+ D→ HD (v′= 4, J′= 3)+ D reaction at a collision energy of 2.2 eV

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Differential cross sections for H+D[sub 2]→HD (v[sup ʹ]=2, J[sup ʹ]=0,3,5)+D at 1.55 eV

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Measurement of the state-specific differential cross section for the H+D2→HD(vʹ=4, Jʹ=3)+D reaction at a collision energy of 2.2 eV

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Collision energy dependence of the HD(nu'=2) product rotational distribution of the H+D2 reaction in the range 1.30-1.89 eV

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Collision energy dependence of the HD(ν[sup ʹ]=2) product rotational distribution of the H+D[sub 2] reaction in the range 1.30–1.89 eV

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Integral rate constant measurements of the reaction H + D2 → HD (v′ = 1, j′) + D at high collision energies

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Evidence for Scattering Resonances in the H+D2 Reaction

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Collision-energy dependence of HD(ν[sup ʹ]=1,j[sup ʹ]) product rotational distributions for the H+D[sub 2] reaction

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Measurement of the state‐specific differential cross section for the H+D₂→HD(v′=4, J′=3)+D reaction at a collision energy of 2.2 eV

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Measurement of the cross section for H+D[sub 2]→HD(vʹ=3,jʹ=0)+D as a function of angle and energy

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Direct electron-impact collision cross sections involving vibrationally excited D2(v) molecules relevant to D− sources

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Disagreement between theory and experiment in the simplest chemical reaction: Collision energy dependent rotational distributions for H+ D~ 2→ HD (nu'= 3, j') …

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H+D2 reaction dynamics. Determination of the product state distributions at a collision energy of 1.3 eV

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State-resolved differential cross sections for the H+D2 (v=0, j) → HD(v′, j′)+D reaction from quasiclassical trajectory calculations

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H(2s)formation inH+-H and H-H collisions

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