Nascent rotational distribution for LiH(v = 0-3,J) states from collisions with H2(E = 4300 and 4800cm-1)

Fig. 11 Rotational distributions of LiH from collisions with (a) H2(E = 4800 cm-1) and (b) H2(E = 4300 cm-1), respectively. For both H2 energies, the weak collision pathway accounts for ~ 81% of collisions with LiH(v = 0) products, while the strong collision pathway accounts for ~ 19%.244