Issue 
A&A
Volume 497, Number 3, April III 2009



Page(s)  911  925  
Section  Atomic, molecular, and nuclear data  
DOI  https://doi.org/10.1051/00046361/200810680  
Published online  18 February 2009 
Rotational excitation of orthoHO by paraH (j 0, 2, 4, 6, 8) at high temperature
M.L. Dubernet^{1,2}  F. Daniel^{2,3}  A. Grosjean^{4}  C. Y. Lin^{2}
1  Université Pierre et Marie Curie, LPMAA UMR CNRS 7092, Case 76, 4 place Jussieu, 75252 Paris Cedex 05, France
2  Observatoire de ParisMeudon, LERMA UMR CNRS 8112, 5 place Jules Janssen, 92195 Meudon Cedex, France
3  Departamento Molecular and Infrared Astrophysics, Consejo Superior de Investigaciones
Cientificas, C/ Serrano 121, 28006 Madrid, Spain
4  Institut UTINAM, UMR CNRS 6213, 41bis avenue de l'Observatoire, BP 1615, 25010 Besançon Cedex, France
Received 25 July 2008 / Accepted 17 December 2008
Abstract
Aims. Our objective is to obtain the best possible set of rotational (de)excitation statetostate and effective rate coefficients for temperatures up to 1500 K. We present statetostate rate coefficients among the 45 lowest levels of oH_{2}O with H_{2}(j_{2}=0) and
,
as well as with H
_{2}(j_{2} = 2) and
.
In addition and only for the 10 lowest energy levels of oH_{2}O, we provide statetostate rate coefficients involving j_{2}=4 with
and j_{2}=2 with
.
We give estimates of effective rate coefficients for j_{2} = 6, 8.
Methods. Calculations are performed with the close coupling (CC) method over the whole energy range, using the same 5D potential energy surface (PES) as the one employed in our latest publication on water. We perform comparisons with coupled states (CS) calculations, with thermalized quasiclassical trajectory (QCT) calculations using the same PES and with previous quantum calculations obtained between T=20 K and T=140 K with a different PES.
Results. We find that the CS approximation fares extremely badly even at high energy for j_{2} different from zero. Comparisons with thermalized QCT calculations show large factors at intermediate temperatures and factors from 1 to 3 at high temperature for the strongest rate coefficients. Finally we stress that scaled collisional rate coefficients obtained with He cannot be used in place of collisional rate coefficients with H_{2}.
Key words: molecular data  molecular processes  ISM : molecules
1 Introduction
This is the first effort on such a large scale to obtain the highest possible accuracy for collisional excitation rate coefficients of an asymmetric molecule with a rotationally excited diatomic molecule. This effort is justified by the importance of water in various astrophysical media. Water is a key molecule for the chemistry and the energy balance of the gas in cold clouds and star forming regions, thanks to its relatively large abundance and large dipole moment. A wealth of observational data has been obtained by the Infrared Space Observatory (see for example: Tsuji 2001; Spinoglio et al. 2001; Cernicharo & Crovisier 2005; Wright et al. 2000), the Submillimeter Wave Astronomy Satellite (Melnick et al. 2000) and the ODIN satellite (Sandqvist et al. 2003; Wilson et al. 2003). In the near future the Heterodyne Instrument for the FarInfrared (HIFI) will be launched on board the Herschel Space Observatory. It will observe with unprecedented sensitivity spectra of many molecules with an emphasis on water lines in regions such as low or high mass star forming regions, protoplanetary disks and AGB stars. The interpretation of these spectra will rely upon the accuracy of the available collisional excitation rate coefficients that enter into the population balance of the emitting levels of the molecules. In the temperature range from 5 K to 1500 K, the most abundant collider likely to excite molecules in media with weak UV radiation fields is the hydrogen molecule, followed by the helium atom.
A pioneering rigidbody 5D PES was obtained by Phillips et al. (1994) for the excitation of the rotational levels of H_{2}O by H_{2}. Using this PES, Phillips et al. (1996) computed rate coefficients for rotational deexcitation among the first 5 ortho and para levels of water with H_{2} (j=0, 1) for temperatures ranging from 20 K to 140 K. Dubernet & Grosjean (2002) and Grosjean et al. (2003) extended this work down to 5 K and pointed out that such low temperature rates are highly sensitive to a proper description of resonances.
Recently an accurate 9D PES for the deformable H_{2}  H_{2}O system was calculated by Faure et al. (2005a). This PES combined conventional 5D and 9D CCSD(T) calculations (coupled cluster with perturbative triples) and accurate calibration data using the explicitely correlated CCSD(T)R12 approach (Noga & Kutzelnigg 1994).
As a first application of the 9D PES, high temperature (1500 K < T < 4000 K) rate coefficients for the relaxation of the bending mode of H_{2}O were estimated from quasiclassical trajectory calculations (Faure et al. 2005a) and the role of rotation in the vibrational relaxation of water was emphasized (Faure et al. 2005b).
Another application of this 9D PES was to construct an accurate 5D PES suitable for inelastic rotational calculations by averaging over H_{2}and H_{2}O ground vibrational states. As was pointed out in Faure et al. (2005a), this stateaveraged PES is actually very close to a rigidbody PES using stateaveraged geometries for H_{2}O and H_{2}.
Using this newly determined 5D PES for H_{2}H_{2}O, Dubernet et al. (2006b) provided an extended and revised set of rate coefficients for deexcitation of the lowest 10 rotational levels of o/pH_{2}O by collisions with pH_{2} (j_{2}=0) and oH_{2}(j_{2}=1), for kinetic temperatures from 5 K to 20 K.
The new PES of Faure et al. (2005a) leads to a significant reevaluation of the rate coefficients for the excitation of H_{2}O by paraH_{2} (j=0). Indeed for the 1_{10} to 1_{01} transition observed by the SWAS satellite, the new PES increases the deexcitation rate coefficient by a factor of 4 at 5 K and by 75% at 20 K compared to the previous results of Dubernet et al. (Dubernet & Grosjean 2002; Grosjean et al. 2003), leading to a total increase at 20 K of 185% with respect to the Phillips et al. (1996) results. The deexcitation rate coefficients of other transitions induced by paraH_{2} can increase by as much as 100% or decrease by 30%. For collisions with orthoH_{2}(j=1) the new PES has a smaller effect on the deexcitation rate coefficients with a maximum change of 40%. The influence of the new PES on collisions with both pH_{2} (j_{2}=0) and oH_{2} (j_{2}=1) is expected to become less pronounced at higher temperatures.
Faure et al. (2007) provided rate coefficients for rotational deexcitation among the lowest 45 rotational levels of o/pH_{2}O colliding with o/pH_{2} in the temperature range 202000 K. This set is a combination of various data: 1) data obtained with quasi classical trajectory (QCT) calculations with the H_{2} molecule assumed to be rotationally thermalized at kinetic temperature and calculated between 100 K and 2000 K; 2) the values at 20 K are CC calculations from Dubernet et al. (2006b) for the first 5 levels and are equal to values at 100 K for all other levels; 3) scaled H_{2}OHe results from Green et al. (1993) for the weakest rate coefficients. A preliminary comparison (Faure et al. 2007) with current CC calculations concerning low lying levels of water at high temperature showed that QCT thermalized rate coefficients were accurate to within a factor of 13 for the dominant transitions, i.e. for those with rates larger than a few 10^{12} cm^{3} s^{1}.
Our current objective is to obtain the best possible set of rotational (de)excitation statetostate and effective rate coefficients for temperatures up to 1500 K. We provide statetostate rate coefficients among the 45 lowest levels of oH_{2}O with H_{2}(j_{2}=0) and , as well as with H_{2}(j_{2} = 2) and . In addition and only for the 10 lowest energy levels of oH_{2}O, we provide statetostate rate coefficients involving j_{2}=4 with and j_{2}=2 with . We give estimates of effective rate coefficients for j_{2} = 6, 8.
2 Methodology
2.1 Collisions with H_{ 2}
Our calculations provide statetostate collisional rate coefficients involving changes in both the target and the perturber rotational levels, i.e. where , represent the initial and final rotational levels of water, j_{2}, j'_{2} the initial and final rotational levels of H_{2}, and T is the kinetic temperature.
The statetostate collisional rate coefficients are the Boltzmann thermal averages of the statetostate inelastic cross sections:
where E is the kinetic energy, is the Boltzmann constant and is the reduced mass of the colliding system.
These statetostate collisional rate coefficients follow the detailed balance principle and reverse rate coefficients
can be obtained from forward rate coefficients by the usual formula:
(2) 
where g_{j1}, g_{j2} are the statistical weights related to rotational levels of H_{2}O and H_{2} respectively, and the different are the rotational energies of the species.
Some astrophysical applications might rather use the socalled effective rate coefficients
which are given by the sum of the statetostate rate coefficients (Eq. (1)) over the final j_{2}' states of H_{2} for a given initial j_{2}:
These effective rate coefficients do not follow the detailed balance principle and both excitation and deexcitation should be explicitly calculated. It should be recalled that in the temperature range between 5 K and 20 K (Dubernet & Grosjean 2002; Grosjean et al. 2003), the effective rate coefficients follow the principle of detailed balance within the calculation error, because there are no transitions to the j_{2} = 3 rotational level of oH_{2}, and transitions to the j_{2} =2 rotational level of pH_{2} are negligeable.
Table 1: Energy levels of owater obtained with the Kyrö (1981) Hamiltonian.
Finally, averaged deexcitation rate coefficients for o/pH_{2}O by rotationally
thermalized o/pH_{2} can be obtained by averaging over the initial rotational levels
of o/pH_{2}:
with , where Z is the partition function over either ortho or paraH_{2} states. These averaged deexcitation rate coefficients are those directly calculated by Faure et al. (2007) with a QCT method.
2.2 Description of the calculations
In the current calculations we use the same expansion of the Faure et al. (2005a) 5D PES as in Dubernet et al. (2006b), where details can be found. For this PES, inaccuracies in inelastic cross sections might come from different sources: propagation parameters, description of the rotational Hamiltonians of the 2 molecules, sizes of H_{2}O and H_{2} rotational basis sets, level of approximation in quantum calculations where the coupled states (CS) approximation might be used instead of the exact close coupling (CC) method. Additional errors might be introduced in rate coefficients if the kinetic energy grid is not fine enough near thresholds, resulting in poor low temperature rate coefficients, or not extended to high enough energies, leading to wrong high temperature results.
Our quantum calculations are carried out with modified versions of the sequential and parallel versions of the MOLSCAT code (Hutson & Green 1994; McBane 2004). Parameters of the propagation are optimized as was done in Dubernet & Grosjean (2002); Dubernet et al. (2006b); Grosjean et al. (2003). Identically to Dubernet et al. (2006b), the H_{2} energy levels are the experimental energies of Dabrowski (1984) and the H_{2}O energy levels and eigenfunctions are obtained by diagonalisation of the effective hamiltonian of Kyrö (1981), compatible with the symmetries of the PES (Dubernet & Grosjean 2002; Dubernet et al. 2006b; Grosjean et al. 2003). The first 45 levels of orthowater are given in Table 1. The reduced mass of the system is 1.81277373 a.m.u.
2.2.1 Basis set convergence: Methodology in choosing an appropriate basis set
The basis set is a direct product of rotational wavefunctions of water, characterized by the rotational quantum number j_{1} (the lowest value of j_{1} is one for oH_{2}O) and the pseudoquantum number which varies between j_{1} and j_{1} (alternatively, we may use the pseudoquantum numbers and with the correspondance ), and of rotational wavefunctions of hydrogen characterised by the rotational quantum number j_{2}. To a single j_{1} rotational quantum number is associated a ladder of increasing rotational energy levels corresponding to successive values of characteristic of oH_{2}O, and it should be remembered that 2 to 3 adjacent ladders might overlap. A ladder includes j_{1} values of for even j_{1}, and j_{1} + 2 values of for odd j_{1}. CC calculations are carried out at a given total energy, a given parity and a total angular momentum . The coupling scheme involves a first coupling between the monomers leading to an intermediate quantum number j_{12}, such that , and a subsequent coupling to the orbital angular momentum such that . We call B(n,m) a basis set where n is the maximum value of j_{1}, m is the maximum value of j_{2}, and B(n,m) includes all the coupled states. The convergence of the basis set usually involves keeping a number of closed channels above the total energy at which the collisional crosssections are calculated. These closed channels mainly influence the collisional process in the strong interaction region via coupling of the potential. The potential couplings between ( ) energy levels decrease with increasing and , therefore for the simple case of a B(n,0) basis set we find that a good convergence is reached with 10 energetically closed channels of water. The basis set B(n,0) with an energy cutoff above the 10th closed channel of water is called a B^{*}(n,0) [10] basis set (see notation below). Another important question is the accuracy of crosssections with respect to the number of closed channels of the H_{2} molecule. Phillips et al. (1996); Dubernet & Grosjean (2002) already showed that the j_{2}=2 level has a strong influence on inelastic crosssections involving no energy transfer in H_{2}. Therefore these authors chose basis sets of the type B(n,2), while Grosjean et al. (2003) used a B(n,3) basis set. Generally at least one to two closed H_{2} rotational channels would be required in order to ensure convergence to better than 5% of inelactic cross sections involving energy transfer in H_{2}. This would be particularly important if the purpose of our calculations was to find inelastic rate coefficients of H_{2} averaged over water transitions. However for our purposes it is sufficient to use a basis set which is reduced by the application of an energy cutoff, following Dubernet et al. (2006b). We define B^{*}(n,m)[p,q,r] to be a subset of B^{*}(n,m) containing, for j_{2} = 0,2,4 respectively, all states of B^{*}(n,m) up to the first p, q and r states whose internal energies lie above the sum of the total energy and E (j_{2}>), where the total energy is taken respective to the ground state of water and pH_{2}.
Table 2: Rotational (de)excitation crosssections (in ) of oH_{2}O calculated with different basis sets: (1) a complete B(6,2) basis set, (2) a B^{*}(6,4)[all, all, 5] basis set with an incomplete ladder in j_{2}=4, (3) a B^{*}(9,4)[10, 10, 5] basis set with incomplete ladders for j_{2}=0,2,4. The transitions are labelled by the quantum numbers (j_{2}j'_{2}) where primes are final states.
Some behaviors of crosssections for different basis sets and low lying levels of oH_{2}O are shown in Table 2; they are representative of the whole set of crosssections. At total energy cm^{1}, these crosssections show less than 0.5% difference between B^{*}(6,4)[all, all, 5] and B^{*}(9,4)[10, 10, 5], which includes the open channel 7_{07} and closed channels involving incomplete ladders up to a maximum value of j_{1} equal to 9. This result could be considered as trivial but it clearly shows that the convergence procedure of readjusting the number of closed channels for each total energy is solely necessary for total energies covering the opening of molecular channels whose transitions we are interested in; above the highest threshold of interest the basis set does not need to be increased.
Figure 1: Statetostate rate coefficients (cm^{3} s^{1}) of the 3_{30} to 1_{10} transition of oH_{2}O as a function of temperature (Kelvin). The full line indicates the statetostate rate coefficients for , and the broken line corresponds to . The lines in parts a) and b) are calculated with a B^{*}(6, 4)[all, all, 5] basis set. Part b) also shows rate coefficients obtained with a B(6, 2) basis set (squares and diamonds) at low temperature. 

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Another question is the accuracy of crosssections with respect to the inclusion of the j_{2}=4 level in the basis sets. Table 2 shows that j_{2}=4 has the strongest effect on transitions from j_{2}=0 to j_{2}=2. Overall the inclusion of the j_{2}=4 level induces an effect of about 10% to 20% on the strongest statetostate rate coefficients involving energy transfer in H_{2}, i.e. for (and up to 60% for the weakest). This effect is directly transfered to the effective (de)excitation rate coefficients when they are dominated by those statetostate rate coefficients. This happens when there is internal energy transfer between excitation of H_{2} and deexcitation of oH_{2}O. This is illustrated in Fig. 1 for the water transition 3_{30} to 1_{10} where is larger than .
2.2.2 Basis set convergence: choice of basis set
It is not possible to obtain the same fully converged rate coefficients for all transitions among the first 45 levels of oH_{2}O. Therefore we adopted different strategies. For transitions among the first 20 levels of oH_{2}O, we adopted one closed channel for H_{2} with a maximum value of j_{2} equal to 4. For H_{2}O the basis set combined at least one closed j_{1} level and a cutoff in rotational energy equivalent to 10 rotational levels for j_{2}=0, 2 (reduced to 5 closed rotational levels for j_{2}= 4) above the total energy considered in the calculations, i.e. a B^{*}(n,4)[10,10,5] basis set. This method was employed over the whole range of energies for the deexcitation of the first 10 levels while for deexcitation from the 11th to the 20th levels of oH_{2}O it was employed up to a total energy of 950 cm^{1} only. Due to prohibitive computing cost for total energies from 950 cm^{1} up to 8000 cm^{1}, the reduced basis set B^{*}(n,2)[10,10] was used for deexcitation calculations from the 11th to the 45th levels of oH_{2}O with pH_{2}.
Table 3: Summary of the sets of statetostate (STSR) and effective rate coefficients (ER) available in BASECOL. Column 1 labels the set of statetostate rate coefficients. (K) and (K) indicate the lowest and highest temperatures at which calculations and fits have been performed for the relevant sets of data. The column ``Transition'' indicates the number of levels among which rate coefficients are provided. T1, T2, T3, T4 indicate the expected accuracy: T1 for the 20 first levels of oH_{2}O, T2 from the 21st to the 30th level, T3 from the 31st to the 40th, T4 from the 41st to the 45th. A1 means ``20% at most for the most significant rates, i.e. larger than 10^{14}'', A2 means ``not good but contribute only 4% to effective rate coefficients'', the notation X(Z)Y means X% accuracy below a temperature of T = Z Kelvin and Y% accuracy above T = Z Kelvin.
2.2.3 Choice of method
CC calculations give exact results but are computationally very expensive when they are associated with very large basis sets. Usually CS calculations are prefered for calculations at total energies located far enough from the transition thresholds; therefore the CS method cannot adequately describe collisional deexcitation among the lowest 45 levels of water for total energies up to 2000 cm^{1}. Moreover we find that the CS method degrades the quality of rate coefficients involving excited rotational levels of H_{2} with and without energy transfer in H_{2}. For non negligeable rate coefficients the errors range from 50% to 100%. Therefore our choice was to use the close coupling method over the whole range of total energies.
The failure of the CS method has already been observed by Kouri et al. (1976) for diatomdiatom collisions in the case of HClH_{2} (Table XI) for transitions that are dominated by the strong long range interaction (j_{2} = 1, 2). Heil et al. (1978) suggested that the breakdown of the CS approximation is initiated in the short range part of the PES and that the long range anisotropy increases this breakdown. However they assumed that CC and CS would agree better at higher energies. Obviously this is not the case for the present system. It should be noted that even for atomdiatom collisions, Dubernet et al. (2001) showed that CC and CS total inelastic crosssections among the lowest rotational levels of H_{2} colliding with He did not converge at high temperature, though the results were close. In fact, the CS method involves approximating angular momentum terms in the total Hamiltonian, and in particular omitting Coriolis terms. When the angular momentum of the hydrogen molecule is introduced into the problem, the validity of these approximations for the angular momentum coupling is likely to be compromised. The large energy spacing of the rotational levels of hydrogen will exacerbate these effects.
2.2.4 Choice of total energy points
CC calculations are carried out over essentially the whole energy range spanned by the Boltzmann distributions (Eq. (1)); the highest energy point calculated is at 8000 cm^{1} and cross sections are extrapolated at higher energy in order to achieve convergence for deexcitation from the highest water energy levels. These extrapolations do not degrade the accuracy of rate coefficients because the concerned cross sections behave regularly. We carefully spanned the energy range above the inelastic channels and added more points in the presence of resonance structures. The total energy grid below the 10th threshold has been described in Dubernet et al. (2006b); between the 10th and the 20th threshold energy steps vary from 0.5 to 2 cm^{1}, from the 20th to the 25th they range from 2 to 5 cm^{1}, above the 25th threshold they vary from 10 to 40 cm^{1}. We paid particular attention to having a fine description of low energy behaviors of cross sections connected to j_{2}=2 for rotational levels of H_{2}O up to 600 cm^{1}. Nevertheless for j_{2}=2 the energy grid is coarser than for j_{2}=0, though still allowing an adequate precision (see Table 3). Overall there are about 1592 energy points.
3 Discussion
3.1 Results for j_{ 2} = 0, 2, 4, 6, 8
We use the methodology described above to calculate sets of statetostate rate coefficients (Eq. (1)) in the temperature range from 5 K to 1500 K for deexcitation transitions among the 45 lowest levels of oH_{2}O with j_{2} = 0 and , as well as with j_{2} = 2 and . In addition and only for the 10 lowest energy levels of oH_{2}O, we obtain cross sections involving j_{2}=4 with , j_{2}=0 with and j_{2}=2 with . Because of the sparse energy grid of cross sections involving j_{2}=4, we estimate that the related rate coefficients are only correct for temperatures above 1000 K. All rate coefficients involving energy transfers with are very small and can be ignored up to 1500 K. The statetostate rate coefficients involving energy transfers from j_{2}=2 to j_{2}=4 or from j_{2}=4 to j_{2}=2 contribute only 4% to the effective rate coefficients; nevertheless we provide them for the sake of completeness between 1000 K and 1500 K. They should only be used to calculate the effective excitation and deexcitation rate coefficients of oH_{2}O out of the j_{2}=2, 4 level as their accuracy is quite low.
Figure 2: Ratios of effective deexcitation rate coefficients (Eq. (3)) for the first 10 levels of owater and for temperatures ranging from 20 K to 1600 K. Black lines give the ratios / and red lines give the ratios / . The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 3: Ratios of effective deexcitation rate coefficients (Eq. (3)) / from the 46th to the 990th deexcitation transition and for the following temperatures: T=100 K (black), T=200 K (red), T=400 K (green), T=800 K (blue), T=1600 K (cyan). The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Additionally we use the breathing sphere approximation (Agg & Clary 1991b,a), i.e. we average the PES over j_{2}=4 in order to complete the set of deexcitation cross sections of oH_{2}O with j_{2}=4 and , which allows us to obtain rate coefficients for temperatures between 5 K and 1500 K. This procedure is fully justified by the small magnitude of cross sections involving energy transfer with from j_{2}=4.
From the calculated statetostate rate coefficients, the effective rate coefficients corresponding to j_{2}= 0, 2, 4 can be calculated using Eq. (3). The ratios of effective deexcitation rate coefficients (Eq. (3)) ( ) over effective deexcitation rate coefficients ( ) for the first 45 (10) levels of orthowater are given in Figs. 2, 3. Table 4 provides the correspondance between labels of the 990 transitions and labels of the energy levels given in Table 1.
Table 4: Labels of first and last deexcitation transitions from a given level (as given in Table 1). This table is the key for reading the figures giving ratios of rate coefficients as a function of transitions labels.
Ratios can be very large for water transitions for which no internal energy transfer occurs between H_{2} and H_{2}O; these large ratios are due to the strong long range part of the PES for j_{2} = 2. These ratios can as well be very small when internal energy transfer strongly enhances rate coefficients. The alternating large and small ratios lead to the patterns observed in Fig. 3; these patterns are particularly noticeable for deexcitation from high lying energy levels of water. Indeed deexcitation effective rate coefficients are strongly influenced by the corresponding statetostate rate coefficients for all owater levels above the opening of the j_{2}=2 level of H_{2}, while , effective rate coefficients are mainly influenced by respectively the and statetostate rate coefficients.
Effective rate coefficients of oH_{2}O linked to j_{2}=6, 8 may also be obtained using the breathing sphere approximation between 5 K and 1500 K. Indeed Dubernet et al. (2001) (in Fig. 2) showed that total inelastic crosssections of H_{2} with j_{2}=4, 6 colliding with He are negligeable in the energy range from 0 cm^{1} to 5000 cm^{1} and we can assume a similar behavior in the present case. Nevertheless this work is not performed in the present paper and the magnitudes of the relevant effective rate coefficients may be evaluated using multiplicative factors with the following guideline, based on available comparisons among our calculated rate coefficients between j_{2} =2 and j_{2} = 4: the user may vary the effective rate coefficient by 20%50% (mostly increase) from j_{2} =2 to j_{2} =4, and so on up to j_{2} = 8.
Table 5: Unnormalized population of the rotational states of pH_{2} relative to j_{2} = 0, at different temperatures and assuming thermodynamic equilibrium.
The BASECOL database (Dubernet et al. 2006a) will provide full tables of the rate coefficients sets mentioned in Table 3.
3.2 Accuracy of results
Apart from the usual checks of convergence with respect to propagation parameters, basis set and total angular momentum, the statetostate rate coefficients have been carefully checked by detailed balance. It should be recalled that the quality of rate coefficients at low temperature is linked to the number of energy points close to the molecular thresholds, and we have an excellent energy grid for j_{2} = 0 and a sparser but still good energy grid for j_{2} = 2. We have a very good grid for j_{2} = 4, due to the use of the breathing sphere approximation at total energy close to water thresholds. The maximum values of the estimated errors are given in Table 3 for transitions starting from different levels of oH_{2}O (T1, T2, T2, T4) and for the various sets of statetostate rate coefficients (1 to 7). Sets (5) and (6) have very low accuracy, which is not a cause for concern for the present application since they provide a very small contribution to the effective rate coefficients. The accuracy of the effective rate coefficients (ER) reflects the accuracies of set (1) and of set (2) to a lesser extent. The accuracy of the effective rate coefficients (ER) is mainly connected to set (4) because set (3) rate coefficients give a small contribution to the effective rate coefficients. The accuracy of the effective rate coefficients linked to j_{2}=4 can be estimated to be around 40%.
3.3 Thermalized rate coefficients
We will not explicitly provide deexcitation rate coefficients of oH_{2}O with thermalized H_{2} (Eq. (4)). The values of in Table 5 indicate that we can provide accurate averaged deexcitation rate coefficients (Eq. (4)) up to 300 K400 K for transitions from the 11th45th level of oH_{2}O, and up to 800 K for the 10 first levels, the accuracy being that of the statetostate rate coefficients. When levels j_{2} > 2 start to contribute to thermalised rate coefficients, the uncalculated effective rate coefficients for j_{2} > 2 might be estimated using the guidelines given in Sect. 3.1. Another possibility at high temperature is to directly use the QCT rate coefficients of Faure et al. (2007), being aware of their limitation. Extensive comparisons between our averaged deexcitation rate coefficients and the QCT results are given in the following sections.
3.4 Overestimation of rate coefficients by QCT calculations
The calculations of Faure et al. (2007) are described in the introduction. At 20 K a comparison between the present results and the Faure et al. (2007) results only indicates whether those authors were right to claim that their linear extrapolation from 100 K lies within a factor of 2 to 3 of the true values. In order to compare quantum and QCT results obtained with the same PES, we must remove the scaled H_{2}OHe results from their published set since the scaled H_{2}OHe rate coefficients are used for 65% of the transitions at various temperatures. Figure 4 shows the ratios of averaged CC rate coefficients over thermalized QCT rate coefficients for temperatures 100 K, 200 K, 800 K and 1600 K (note that averaged CC rate coefficients involve j_{2}=0,2,4 for transitions among the first 10 levels of water and j_{2}=0,2 for all other transitions). We find that the QCT method systematically overestimates, by up to a factor of 10, some of the strongest rate coefficients and underestimates rate coefficients involving internal energy transfer between oH_{2}O and H_{2}by factors as large as 100 at T=100 K. The agreement between the two sets of rate coefficients improves with increasing temperature and above T = 800 K most rates are within a factor of 3.
Figure 4: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over QCT calculations of Faure et al. (2007) as a function of the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3}s^{1}). 

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Figure 5: Comparison of deexcitation rate coefficients (in cm^{3} s^{1}) at T=800 K from the a) 5_{14}, b) 7_{16}, c) 9_{18} and d) 6_{25} levels of owater. The full lines (with circles) correspond to our CC averaged rate coefficients (Eq. (4) as explained in the text), the dashed lines to the set of deexcitation rate coefficients of Faure et al. (2007), the dotted lines to the scaled He rate coefficients of Green et al. (1993). The abscissae correspond to the index of the transition with quantum numbers indicated in Table 6. 

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The overestimation of some of the strongest thermalized rate coefficients concerns a few transitions over the whole range of temperature. This effect is not related to the missing j_{2}=4 quantum effective rate coefficient since the overestimation exists for temperatures below 400 K. Figure 5 compares our CC averaged rate coefficients with the set published by Faure et al. (2007) and with scaled He rate coefficients of Green et al. (1993) for transitions from the 5_{14}, 7_{16}, 9_{18}, 6_{25} levels. These last 2 sets coincide for some transitions since Faure et al. (2007)'s set includes both QCT calculations and scaled He rate coefficients for the weakest transitions. QCT calculations systematically overestimate transitions from the 5_{14}, 7_{16}, 9_{18} levels to the lowest level of a j ladder (indicated by arrows), with the strongest overestimation corresponding to a transition in the same ladder (bold arrows). Table 6 gives the initial and final quantum numbers of the involved transitions. These overestimations seem to exist for initial j having odd values only. Indeed for even j no such overestimation is observed, as can be seen in part (d) of Fig. 5 for deexcitation from the 6_{25} level. We suspect that these systematic overestimations are an artefact of the binning procedure in the QCT calculations of Faure et al. (2007).
Table 6: Quantum numbers of levels involved in the transitions of Fig. 5 a), b), c) overestimated by QCT calculations. Primes indicate quantum numbers of the final states.
Figure 6: Ratios of effective deexcitation rate coefficients (Eq. (3)) of oH_{2}O with H_{2}(j_{2}=0) over scaled waterHe rate coefficients (in cm^{3} s^{1}) (Green et al. 1993) as a function the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3} s^{1}). 

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Figure 7: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over data sets published by Faure et al. (2007) as a function the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3} s^{1}). These data sets include both the quasiclassical calculations (crosses in squares) and scaled waterHe rate coefficients (crosses without squares) published in Faure et al. (2007). 

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Table 7: Levels involved in some of the transitions largely underestimated by scaled He calculations and to a lesser extent by QCT calculations at 100 K. We provide ratios of averaged CC rate coefficients over QCT and scaled He calculations at 100 K, as well as the values of the corresponding averaged CC rate coefficients (in cm^{3} s^{1}).
3.5 Underestimation of rate coefficients by scaled He and QCT calculations
The deexcitation rate coefficients of H_{2}O + He of Green et al. (1993), scaled by a factor of 1.344 to correct for the differing colliding system masses, have systematically been used in astrophysical applications to mimic rate coefficients of H_{2}O + H_{2}. Phillips et al. (1996) had already pointed out that this method was not correct for temperatures up to 140 K. Figures 6, 7 show that scaled H_{2}O + He rate coefficients underestimate both the j_{2}=0 effective and thermalized rate coefficients, with ratios as large as 1000. The largest ratios occur for transitions dominated by internal energy transfer between H_{2} and H_{2}O. This induces larger rate coefficients for the concerned water transitions and the effect is particularly noticeable for deexcitation from high lying levels of water and for transitions involving favorable quantum numbers, i.e. , small.
Examples of transitions largely underestimated at 100 K by both scaled He and QCT calculations are given in Table 7. The ratios of CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} over QCT calculations of Faure et al. (2007) are nevertheless smaller than the ratios of CC averaged deexcitation rate coefficients over scaled waterHe rate coefficients (Green et al. 1993). Apart from the overestimation cases analyzed above, QCT calculations generally are an improvement over scaled He calculations. It is unfortunate that very few rate coefficients can be calculated via QCT calculations.
Figures 8 to 13 compare our averaged rate coefficients with the set published by Faure et al. (2007) and with scaled He rate coefficients of (Green et al. 1993) for some of the 990 deexcitation transitions from the first 45 levels of orthowater. Again we recall that these last 2 sets coincide for some transitions since Faure et al. (2007)'s set includes both QCT calculations and scaled He rate coefficients for the weakest transitions.
3.6 Comparison with the H_{ 2}O + H_{ 2} effective rate coefficients of Phillips et al. (1996)
Comparison with effective rate coefficients of Phillips et al. (1996) can only be performed for the first 10 levels of oH_{2}O and for temperatures in the range 20 K to 140 K. The ratios of effective rate coefficients, given in Table 8, decrease slightly with temperature. This certainly reflects the decreasing influence of the difference between the two different PES (Faure et al. 2005a; Phillips et al. 1994) as temperature increases. The first line of Table 8 shows that the j_{2}=2 level cannot be ignored in the calculation of the averaged rate coefficients above T=120 K.
Figure 8: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of (Green et al. 1993) (red line) for all 990 deexcitation transitions from the first 45 levels of owater at a temperature of 100 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 9: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) given for the first 45 deexcitation transitions from the first 10 levels of owater, for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 10: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 46th to the 105th deexcitation transitions from the first 15 levels of owater for temperatures ranging from 200K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 11: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 191st to the 300th deexcitation transitions from the first 25 levels of owater for temperatures ranging from 200 K to 1600K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 12: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 596th to the 780th deexcitation transitions from the first 35 levels of owater for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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Figure 13: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 781st to the 990th deexcitation transitions from the first 35 levels of owater for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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3.7 Fitted rate coefficients
The statetostate rate coefficients
for the deexcitation of oH_{2}O with pH
_{2} (j_{2} = 0, 2, 4) and
are fitted to an analytical form very similar to the one used by Mandy & Martin (1993):
The fits are performed using numerical rate coefficients calculated at 100 temperatures ranging from to which are indicated in Table 3. The fitted coefficients are such that the maximum error between initial data points and fitted values is minimal. A maximum value of N=14 is necessary in order to obtain good accuracy over the whole range of temperature. The fitted rate coefficients were subsequently compared to numerical rate coefficients calculated with a step of T=1 K from to and the maximum error found is less than 0.5%. We emphasize that these fits have no physical meaning; they are only valid in the temperature range of the relevant , and should not be used to perform extrapolations. The complete sets including levels up to the 45th will be available in the BASECOL database (Dubernet et al. 2006a). The quality of the fits can be checked on line through the graphical interface.
Table 8: Ratios of the 5 effective deexcitation rate coefficients of Phillips et al. (1996) over our averaged rate coefficients (1st line) for oH_{2}O with pH_{2}. The ratios of Phillips et al.'s results over our effective rate coefficients (Eq. (3)) for j_{2}=0 for oH_{2}O with paraH_{2} are given on every second line.
4 Concluding remarks
We provide statetostate rate coefficients among the 45 lowest levels of oH_{2}O with H_{2} (j_{2} = 0) and , as well as with j_{2} = 2 and . In addition and only for the 10 lowest energy levels of oH_{2}O, we obtain statetostate rate coefficients involving j_{2}=4 with and j_{2}=2 with .
For the given PES the accuracy of quantum rate coefficients, explicitly given for different temperatures and transitions, is rather homogeneous and lies between 5% and 40% for the first 40 levels of oH_{2}O. For the available transitions, we strongly recommend use of the present sets of effective rate coefficients instead of either the scaled H_{2}OHe data of Green et al. (1993) or the set published in Faure et al. (2007). For temperatures above 400 K, thermalized rate coefficients start to include j_{2} > 2 effective rate coefficients for which we do not provide exact quantum results for all transitions. We advise the user to use multiplicative factors in order to estimate these missing effective rate coefficients. Above 400 K the user can also choose to use the set published in Faure et al. (2007), being aware that the weakest transitions are given by scaled H_{2}OHe rate coefficients which are sometimes wrong by large factors. As expected we find that the scaled He rate coefficients (Green et al. 1993) are neither representative of the effective rate coefficients nor of the averaged CC rate coefficients.
Finally we find that the CS approximation fares extremely badly even at high energy for j_{2} not equal to zero. We will investigate the breakdown of the CS approximation in another publication.
We are currently carrying out similar calculations for oH_{2}O with oH_{2} (j_{2}=1, 3) and for pH_{2}O with o/pH_{2}.
Acknowledgements
Most scattering calculations were performed at the IDRISCNRS and CINES under project 20060708 04 1472. This research was supported by the CNRS national program ``Physique et Chimie du Milieu Interstellaire'' and by the FP6 Research Training Network ``Molecular Universe'', contract Number: MRTNCT2004512302. The authors thank P. Valiron and A. Faure for critical reading of early drafts and the referee for pertinent remarks. Since the submission of this paper, P. Valiron has passed away and we dedicate this paper to his memory.
References
 Agg, P. J., & Clary, D. C. 1991a, J. Chem. Phys., 95, 1037 [NASA ADS] [CrossRef]
 Agg, P. J., & Clary, D. C. 1991b, Molec. Phys., 73, 317 [NASA ADS] [CrossRef]
 Cernicharo, J., & Crovisier, J. 2005, Space Sci. Rev., 119, 29 [NASA ADS] [CrossRef]
 Dabrowski, I. 1984, Canadian J. Phys., 62, 1639 [NASA ADS] (In the text)
 Dubernet, M.L., & Grosjean, A. 2002, A&A, 390, 793 [NASA ADS] [CrossRef] [EDP Sciences] (In the text)
 Dubernet, M.L., Tuckey, P. A., Jolicard, G., Michaut, X., & Berger, H. 2001, J. Chem. Phys., 114, 1286 [NASA ADS] [CrossRef] (In the text)
 Dubernet, M., Grosjean, A., Daniel, F., et al. 2006a, in Rovibrational Collisional Excitation Database: BASECOL  http://basecol.obspm.fr (Japan: Journal of Plasma and Fusion Research Series, series 7) (In the text)
 Dubernet, M.L., Daniel, F., Grosjean, A., et al. 2006b, A&A, 460, 323 [NASA ADS] [CrossRef] [EDP Sciences] (In the text)
 Faure, A., Valiron, P., Wernli, M., et al. 2005a, J. Chem. Phys., 122, 221102 [NASA ADS] [CrossRef] (In the text)
 Faure, A., Wiesenfeld, L., Wernli, M., & Valiron, P. 2005b, J. Chem. Phys., 123, 104309 [NASA ADS] [CrossRef] (In the text)
 Faure, A., Crimier, N., Ceccarelli, C., et al. 2007, A&A, 472, 1029 [NASA ADS] [CrossRef] [EDP Sciences] (In the text)
 Green, S., Maluendes, S., & McLean, A. D. 1993, ApJS, 85, 181 [NASA ADS] [CrossRef] (In the text)
 Grosjean, A., Dubernet, M.L., & Ceccarelli, C. 2003, A&A, 408, 1197 [NASA ADS] [CrossRef] [EDP Sciences] (In the text)
 Heil, T. G., Kouri, D. J., & Green, S. 1978, J. Chem. Phys., 68, 2562 [NASA ADS] [CrossRef] (In the text)
 Hutson, J. M., & Green, S. 1994, MOLSCAT computer code,version 14 (United Kingdom: Collaborative Computational Project No. 6 of the Science and Engineering Research Council)
 Kouri, D. J., Heil, T. G., & Shimoni, Y. 1976, J. Chem. Phys., 65, 1462 [NASA ADS] [CrossRef] (In the text)
 Kyrö, E. 1981, J. Mol. Spectrosc., 88, 167 [NASA ADS] [CrossRef] (In the text)
 Mandy, M. E., & Martin, P. G. 1993, ApJS, 86, 199 [NASA ADS] [CrossRef] (In the text)
 McBane, G. 2004, MOLSCAT computer code, parallel version (USA: G. McBane)
 Melnick, G. J., Stauffer, J. R., Ashby, M. L. N., et al. 2000, ApJ, 539, L77 [NASA ADS] [CrossRef] (In the text)
 Noga, J., & Kutzelnigg, W. 1994, J. Chem. Phys., 101, 7738 [NASA ADS] [CrossRef] (In the text)
 Phillips, T. R., Maluendes, S., McLean, A. D., & Green, S. 1994, J. Chem. Phys., 101, 5824 [NASA ADS] [CrossRef] (In the text)
 Phillips, T. R., Maluendes, S., & Green, S. 1996, ApJS, 107, 467 [NASA ADS] [CrossRef] (In the text)
 Sandqvist, A., Bergman, P., Black, J. H., et al. 2003, A&A, 402, L63 [NASA ADS] [CrossRef] [EDP Sciences]
 Spinoglio, L., Codella, C., Benedettini, M., et al. 2001, The Promise of the Herschel Space Observatory, ed. G. L. Pilbratt, J. Cernicharo, A. M. Heras, T. Prusti, & R. Harris, ESASP, 460, 495
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All Tables
Table 1: Energy levels of owater obtained with the Kyrö (1981) Hamiltonian.
Table 2: Rotational (de)excitation crosssections (in ) of oH_{2}O calculated with different basis sets: (1) a complete B(6,2) basis set, (2) a B^{*}(6,4)[all, all, 5] basis set with an incomplete ladder in j_{2}=4, (3) a B^{*}(9,4)[10, 10, 5] basis set with incomplete ladders for j_{2}=0,2,4. The transitions are labelled by the quantum numbers (j_{2}j'_{2}) where primes are final states.
Table 3: Summary of the sets of statetostate (STSR) and effective rate coefficients (ER) available in BASECOL. Column 1 labels the set of statetostate rate coefficients. (K) and (K) indicate the lowest and highest temperatures at which calculations and fits have been performed for the relevant sets of data. The column ``Transition'' indicates the number of levels among which rate coefficients are provided. T1, T2, T3, T4 indicate the expected accuracy: T1 for the 20 first levels of oH_{2}O, T2 from the 21st to the 30th level, T3 from the 31st to the 40th, T4 from the 41st to the 45th. A1 means ``20% at most for the most significant rates, i.e. larger than 10^{14}'', A2 means ``not good but contribute only 4% to effective rate coefficients'', the notation X(Z)Y means X% accuracy below a temperature of T = Z Kelvin and Y% accuracy above T = Z Kelvin.
Table 4: Labels of first and last deexcitation transitions from a given level (as given in Table 1). This table is the key for reading the figures giving ratios of rate coefficients as a function of transitions labels.
Table 5: Unnormalized population of the rotational states of pH_{2} relative to j_{2} = 0, at different temperatures and assuming thermodynamic equilibrium.
Table 6: Quantum numbers of levels involved in the transitions of Fig. 5 a), b), c) overestimated by QCT calculations. Primes indicate quantum numbers of the final states.
Table 7: Levels involved in some of the transitions largely underestimated by scaled He calculations and to a lesser extent by QCT calculations at 100 K. We provide ratios of averaged CC rate coefficients over QCT and scaled He calculations at 100 K, as well as the values of the corresponding averaged CC rate coefficients (in cm^{3} s^{1}).
Table 8: Ratios of the 5 effective deexcitation rate coefficients of Phillips et al. (1996) over our averaged rate coefficients (1st line) for oH_{2}O with pH_{2}. The ratios of Phillips et al.'s results over our effective rate coefficients (Eq. (3)) for j_{2}=0 for oH_{2}O with paraH_{2} are given on every second line.
All Figures
Figure 1: Statetostate rate coefficients (cm^{3} s^{1}) of the 3_{30} to 1_{10} transition of oH_{2}O as a function of temperature (Kelvin). The full line indicates the statetostate rate coefficients for , and the broken line corresponds to . The lines in parts a) and b) are calculated with a B^{*}(6, 4)[all, all, 5] basis set. Part b) also shows rate coefficients obtained with a B(6, 2) basis set (squares and diamonds) at low temperature. 

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In the text 
Figure 2: Ratios of effective deexcitation rate coefficients (Eq. (3)) for the first 10 levels of owater and for temperatures ranging from 20 K to 1600 K. Black lines give the ratios / and red lines give the ratios / . The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 3: Ratios of effective deexcitation rate coefficients (Eq. (3)) / from the 46th to the 990th deexcitation transition and for the following temperatures: T=100 K (black), T=200 K (red), T=400 K (green), T=800 K (blue), T=1600 K (cyan). The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 4: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over QCT calculations of Faure et al. (2007) as a function of the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3}s^{1}). 

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In the text 
Figure 5: Comparison of deexcitation rate coefficients (in cm^{3} s^{1}) at T=800 K from the a) 5_{14}, b) 7_{16}, c) 9_{18} and d) 6_{25} levels of owater. The full lines (with circles) correspond to our CC averaged rate coefficients (Eq. (4) as explained in the text), the dashed lines to the set of deexcitation rate coefficients of Faure et al. (2007), the dotted lines to the scaled He rate coefficients of Green et al. (1993). The abscissae correspond to the index of the transition with quantum numbers indicated in Table 6. 

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In the text 
Figure 6: Ratios of effective deexcitation rate coefficients (Eq. (3)) of oH_{2}O with H_{2}(j_{2}=0) over scaled waterHe rate coefficients (in cm^{3} s^{1}) (Green et al. 1993) as a function the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3} s^{1}). 

Open with DEXTER  
In the text 
Figure 7: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over data sets published by Faure et al. (2007) as a function the CC averaged deexcitation rate coefficients of oH_{2}O with pH_{2} (in cm^{3} s^{1}). These data sets include both the quasiclassical calculations (crosses in squares) and scaled waterHe rate coefficients (crosses without squares) published in Faure et al. (2007). 

Open with DEXTER  
In the text 
Figure 8: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of (Green et al. 1993) (red line) for all 990 deexcitation transitions from the first 45 levels of owater at a temperature of 100 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 9: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) given for the first 45 deexcitation transitions from the first 10 levels of owater, for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 10: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 46th to the 105th deexcitation transitions from the first 15 levels of owater for temperatures ranging from 200K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 11: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 191st to the 300th deexcitation transitions from the first 25 levels of owater for temperatures ranging from 200 K to 1600K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 12: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 596th to the 780th deexcitation transitions from the first 35 levels of owater for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
Figure 13: Ratios of CC averaged deexcitation rate coefficients (Eq. (4)) of oH_{2}O with pH_{2} over the set of rate coefficients published by Faure et al. (2007) (black line) and over scaled He rate coefficients of Green et al. (1993) (red line) for the 781st to the 990th deexcitation transitions from the first 35 levels of owater for temperatures ranging from 200 K to 1600 K. The abscissae indicate the labeling of the deexcitation transitions as indicated in Table 4. 

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In the text 
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