All Tables

Table 1: Propagation parameters of MOLSCAT used in our calculations (see the MOLSCAT documentation, Hutson & Green 1994, for the meaning of the parameters).
Table 2: Effective rate coefficients of Eq. (2) (in cm³ s^-1) of ortho-H₂O with ortho-H₂ (j₂ = 1). The levels are labelled with j_{K_-1K₁}. The column "Points'' gives the number of energy points used in the Boltzmann average. The last column gives the data of Phillips et al. (1996). The levels are organized according to increasing energy as in the paper of Phillips et al. (1996).
Table 3: Effective rate coefficients of Eq. (2) (in cm³ s^-1) of para-H₂O with ortho-H₂ (j₂=1). The levels are labelled with j_{K_-1K₁}. The column "Points'' gives the number of energy points used in the Boltzmann average. The last column gives the data of Phillips et al. (1996). The levels are organized according to increasing energy as in the paper of Phillips et al. (1996).
Table 4: Coefficients $a^{(n)}_{j_2=1;j\alpha \leftarrow j'\alpha '}$ (n = 0 to 4) of the polynomial fit (Eq. (3)) to the effective de-excitation rate coefficients of ortho-water in Table 2. The effective excitation rate coefficients can be obtained by detailed balance. The first column gives the final state and the polynomial order n, the following columns give the fitting coefficients for various initial states. The levels are labelled with j_{K_-1K₁}. We emphasize that these fits are only valid in the temperature range from 5 K to 20 K.
Table 5: Coefficients $a^{(n)}_{j_2=1;j\alpha \leftarrow j'\alpha '}$ (n = 0 to 4) of the polynomial fit (Eq. (3)) to the effective de-excitation rate coefficients of para-water in Table 3. The effective excitation rate coefficients can be obtained by detailed balance. The first column gives the final state and the polynomial order n, the following columns give the fitting coefficients for various initial states. The levels are labelled with j_{K_-1K₁}.We emphasize that these fits are only valid in the temperature range from 5 K to 20 K.