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See fig. S1 for the J = 0 reaction probability, fig. S2 for the J-shifting reaction probability curves, fig. S3 for the partial wave decomposition of the HF(v′ = 2) forward-scattering peak at the collision energy of 0.52 kcal/mol, fig. S4 for the 3D scattering wave functions at 0.26 and 0.46 kcal/mol for J = 0 from converged time-dependent wave packet calculations, and fig. S5 for projection of J = 0 scattering wave function at the collision energy of 0.26 kcal/mol (corresponding to the ground resonance state) to HF vibrational states and at 0.46 kcal/mol (corresponding to the excited resonance state).
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note
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Supported mainly by the Chinese Academy of Sciences, the Ministry of Science and Technology, and the National Natural Science Foundation of China. M.G. and R.T.S. acknowledge the support of Academia Sinica. We thank K. Liu for many insightful discussions, and C. Zhou, W. Dong, and X. Wang for their help during the experiment.
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