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Fig. 1.

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Comparison of the HCNH+ cross sections for selected total energies. We note that σJ = 0 − 5 is the sum of partial cross sections over total angular momenta up to J = 5. The stars depict the impact of including j2 = 0 − 2 in comparison to the constraint of the H2 rotational basis to j2 = 0, while the empty circles estimate the influence of a more exhaustive H2 rotational manifold (j2 = 0 − 4) with respect to j2 = 0 − 2. The dashed diagonal lines delimit an agreement region of a factor of 1.5.

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