Chemical modelling of interstellar clouds, shocked gas and circumstellar
regions require reaction rate coefficients of up to several thousand
reactions over the temperature range 10 - 2000 K, or so. The latest version
of the UMIST database, RATE95, provides the rate coefficients of
3864 gas-phase reactions among 395 species involving the 12 elements H, He,
C, N, O, Na, Mg, Si, P, S, Cl and Fe. With the exception of the elements
Na, Mg and Fe, which are included in the ratefile to produce a source of
ionisation in dark clouds, the chemistries of the other elements are
fairly comprehensive. Neutral molecules containing up to 12 atoms
(CHCN) are included.
2. The rate coefficient file
The file
rate95.data
contains the reactions and rate coefficients.
Each entry in the file has the form:
I, R1, R2, P1, P2, P3, P4, , , , Note
where I is the reaction number, R1 and R2 are the reactants - R2 can
be a cosmic-ray proton (CRP), a general interstellar ultraviolet photon
(PHOTON), or a cosmic-ray-induced ultraviolet photon (CRPHOT) - and
P1 to P4 are reaction products. A FORTRAN program, DELOAD, writes
FORTRAN source code for the time-dependent, non-linear differential
equations, based on the reaction ratefile and species set. The code
writes the conservation equations (X) and the odes (YDOT) and must
have the subroutine and variable declarations and an END statement
added. The code, which was written by Dr Lida Nejad, has descriptions of
its several modes of operation, and is available as the file
deload95.f.
In the implementation available here, a conservation equation is written
only for electrons; all other species have an ode written.
Because of this, the species file,
spec94.data
to be input to
deload95.f
does not contain the species ELECTR, which is declared in
deload95.f.
The resulting subroutine can then be used with an integrator such as the
GEAR package.
Each entry in
rate95.data
is written in the format:
For each reaction, the rate coefficient can be calculated as:-
for two-body
reactions, where is the gas kinetic temperature,
for direct cosmic-ray ionisation
(R2 = CRP),
for interstellar
photoreactions
(R2 = PHOTON), where represents the rate in the unshielded
interstellar UV radiation field, and is the parameter used to take
into account the extinction of the UV radiation by dust particles, and
for
cosmic-ray-induced
photoreactions (R2 = CRPHOT), where is the grain albedo in
the far UV,
typically 0.6 at 150 nm, and is the probability per cosmic-ray
ionisation that the appropriate photoreaction occurs.
The photorates have been determined using the Draine (1978) UV radiation
field,
while the CRP and CRPHOT reactions are given for a standard interstellar
ionisation rate of 1.3 . These rates can be
scaled easily for other choices of the fields.
'Note' is a nine-column entry which gives information on the type and
source of the data and has the form:-
Column 1: An 'M' here means that the rate coefficient has been
measured in the laboratory or, in the case of radiative association, has
been deduced with the aid of an experiment on the analogous three-body
association. For ion-neutral reactions, the rate coefficients are generally
independent of temperature. An important exception are those reactions in
which the neutral molecule has a large, say greater than 1 Debye, permanent
electric dipole moment. In such cases, the rate coefficients generally
increase at low temperatures (Adams et al. 1985). The file
dipole94.data
gives electric dipole moments, where available, for the neutral
species in the database.
Neutral-neutral reactions are ususally studied experimentally at room
temperature and above and therefore application of laboratory-determined
rate coefficients to the low temperature environments of interstellar
clouds is fraught with uncertainty. For example, it is possible that
several reactions listed in the ratefile as not possessing an activation
energy do, in fact, have small barriers (< 100 K) which are not evident
in measurements done at room temperature and above. In addition, some
experimental data are best characterised, in the temperature range over
which they are studied, by a negative activation energy barrier. In order
to prevent a serious overestimate of these rate coefficients at 10 K, we have
generally preferred to adopt an alternative, although still accurate,
form for the rate coefficients.
Columns 2,3: A two-letter symbol for the type of reaction. The symbols
used are: AD, associative detachment; CD, collisional dissociation;
CH, chemi-ionisation; CI, carbon
insertion, involving a reaction between a carbon atom and a hydrocarbon ion;
CP, cosmic-ray-induced photoreaction; CO, positive ion-neutral
reaction in which
H and/or H are the only neutral products; CR, cosmic-ray ionisation;
CT, charge transfer;
DR, dissociative recombination with electrons; HA, hydrogen abstraction;
MN, mutual neutralisation;
NA, neutral radiative association; NE, neutral exchange; NI, negative
ion-neutral; PD, photodissociation;
PI, photoionisation; PM, photodetachment of electron; PN, positive ion-neutral;
PT, proton transfer; RA, radiative association between a positive ion and a
neutral molecule; RM, radiative electron (minus ion) attachment;
RR, radiative recombination with electrons.
Column 4: A label is used to denote the relevance of a reaction. In
many instances the user will be interested in using only a subset of the
reaction file
rate95.data,
and may want, for ease of computation and
analysis, to neglect unimportant reactions. Certain types of reaction
may be excluded from a particular model. For example, reactions with
large activation energy barriers, which are important in shocked gas, and
photoreactions can be neglected in models of cold, dark clouds.
In addition, however, there are reactions whose neglect will not seriously
compromise the results of most models. These are labelled with an 'E' in
this column. This
category is most used for ions, such as NH and HO, which have
rapid reactions with H. The low abundance of all other species X
relative to H in many astronomical regions, means that all ion-X
reactions can be excluded. This criterion is only useful if H is
the dominant form of hydrogen. If a reaction should be included in any
comprehensive model it is labelled with an 'A'.
Column 5: A digit is used to represent the accuracy of the data. We
have used such labelling mainly for the ion-neutral and photoreactions,
although sometimes the accuracy of the formula given may be restricted to a
particular range of temperature. The following scheme has been used:
1. Error < 25 %
2. Error < 50 %
3. Error to within a factor of 2
4. Error within an order of magnitude
5. Highly uncertain
We have not attempted to give the accuracy of the unmeasured reactions.
The ion-neutral rate coefficients should be accurate to a factor of two, but
it is possible that some of the reactions included here have different
products or are unreactive.
Columns 6-9: A label to the source of the data. Labels of the form
'8010' refer to the labelling scheme of Anich and Huntress (1986). An
explanation of the letter codes, such as RJ91, are listed at the end
of the rate file,
rate95.data
and full references are given by, most recently,
Millar,
Farquhar and Willacy (1997). The label 'NIST', used for many of the
neutral-neutral reactions, refers to the National Institute of Standards
and Technology Chemical Kinetics Database - Ver. 6.0 (Mallard et al. 1994).
The ratefile is laid out as follows:-
Reactions 1 - 394. Neutral-neutral reactions.
Reactions 395 - 3197. Ion-neutral reactions, including reactions of
positive and negative ions.
Reactions 3198 - 3634. Electron reactions, ncluding radiative electron
attachment of H, C, O and S, as well as radiative and dissociative
recombination of positive ions.
Reactions 3635 - 3645. Ionisation by cosmic-ray protons.
Reactions 3646 - 3795. Photoreactions driven by the interstellar UV
radiation field.
Several of the reactions contained in
rate95.data
may be endoergic. H-H Lee (Ohio State University) has kindly made available
his data on the heats of formation of astrophysically interesting molecules
and this file is accessible in
heats94.data.
We have used this file to delete several highly endoergic ion-neutral reactions
present in previous releases of the reaction file.
3. The species file
A separate file,
species94.data,
contains 394 chemical species - note that it excludes electrons - in
the reaction set. For brevity, some species are written in 'shorthand' -
C5H4 represents CHCH. The notation used is given in Millar et al.
(1991), Farquhar and Millar (1993) and
Millar,
Farquhar and Willacy (1997).
The dipole moments of the 137 neutral molecules in the species set are
given, where available, in the file
dipole94.data.
The rate file
discriminates between some isomers, such as HCN and HNC, as well as
CHOH and CHOCH, and the dipole moments are listed for
each isomer. In those cases where the chemistry in the ratefile does
not differentiate,
for example the various forms of linear and cyclic CH, H2CCC and
cyclic CH, and CH (HCCCCH) and HCCCC, the
dipole moments of each form are listed in
dipole94.data.
4. Caveats
The file
rate95.data
contains data on several thousand reactions.
The data are presented in a very simplified format and the user should be aware
that in some cases the parameters fit the data only under special conditions.
Some of these are:-
The radiative association rate coefficients are valid only for the 10-50
K temperature range, in general. At higher temperatures different values,
and different temperature dependencies, can apply.
The rate coefficients of the collisional dissociation (CD) reactions
are dependent both on density and temperature and reference should be made to
the original papers, (Roberge and Dalgarno 1982; Dove and Mandy 1986),
for details.
Some of the more important ion-neutral reactions, such as the
N - H and CH - H systems, have rate coefficients which
are not easily parameterised in the form given here. Such reactions are
discussed in detail by Millar et al. (1991).
The dissociative recombination of H with electrons contains to
be a subject of great debate and its rate coefficient is expected to
remain time-dependent for the foreseeable future, although hopefully with
less strong a dependence as in the past.
Photoprocesses are dependent on the detailed radiative transfer of UV
photons which depends, in turn, on the poorly known properties of the dust
grains. Thus, both the pre-exponential () and exponential ()
factors can be different for different dust properties. In some cases
a bi-exponential formula is to be preferred. Van Dishoeck (1988)
discusses these points in detail.
5. Updates
Major updates to the data occur on roughly a two-year period. The next major
revision should be released in early 1997.
6. Contact point
Questions, comments, corrections and suggestions for improvement and
inclusion to the database should be directed
to:
Professor T J Millar Department of Physics UMIST P O Box 88 Manchester M60 1QD England
Tel.: +44-(0)161-200-3677 FAX.: +44-(0)161-200-4303 E-mail: Tom.Millar@umist.ac.uk
Authors of all publications arising from this data should acknowledge
the primary sources, in this case Millar et al. (1991) and
Millar, Farquhar and Willacy (1997).
7. References
Adams, NG, Smith, D & Clary, DC, 1985, ApJ, 296, L31 Anicich, VG & Huntress, WT, Jr., 1986, ApJSS, 62, 553 Dove, JE & Mandy, ME, 1986, ApJ, 311, L93 Mallard, WG et al., 1994, NIST Chemical Kinetic Database - Ver 6.0 Millar, TJ, Rawlings, JMC, Bennett, A, Brown, PD & Charnley, SB, 1991,
A&AS;, 87, 585 Millar, TJ, Farquhar, PRA & Willacy, K, 1997,
A&AS;, 121, 139
Roberge, WG & Dalgarno, A, 1982, ApJ, 255, 176 van Dishoeck, EF, 1988, in Rate Coefficients in Astrochemistry, (eds.)
TJ Millar & DA Williams (Kluwer: Dordrecht), p. 49
T J Millar, P R A Farquhar and K Willacy
14th May 1996
Tom Millar, Tom.Millar@umist.ac.uk
Fri 14th May 1996