A two‐Hilbert space formalism is first used to develop a general class of representations for the quantum mechanics of N‐particle reactive systems. Here the N‐particle Hilbert space ℋN is supplemented by a larger arrangement channel space 𝒞N of vectors with Hilbert space valued components for each N‐particle clustering, and an injection mapping of ℋN vectors into ‘‘physical’’ 𝒞N vectors. Such representations, for which components of the latter vectors carry an appropriate physical clustering interpretation, provide a rigorous and flexible basis for describing the statistical mechanics of reactive fluids, where atoms and molecules are treated on an equal footing (the molecular picture). Corresponding equilibrium multispecies fugacity or virial expansions follow immediately. Here we focus on analysis of the (previously derived) arrangement channel BBGKY hierarchy for a system where recombination and dissociation, as well as exchange reactions, occur. This formulation (coupled with a corresponding scattering theory) automatically suggests a reactive Boltzmann ansatz which incorporates (standard) noninteracting asymptotic dynamics only for two‐molecule nonreactive and reactive exchange collisions. In contrast, e.g., with three molecule recombination, two‐molecule dynamics for all three pairs is included (as required for a description of recombination via gradual stabilization of metastables). Finally we compare the resulting reduced form of appropriate channel space hierarchy equations, for a process involving dimer formation and decay, with the corresponding kinetic equations of Lowry and Snider.

1.
W. Ebeling, W. D. Kraeft and D. Kremp, Theory of Bound States and Ionization Equilibrium in Plasmas and Solids (Academic, Berlin, 1976).
2.
T. A.
Osborn
and
T. Y.
Tsang
,
Ann. Phys.
101
,
119
(
1976
).
3.
J. A.
McLennan
,
Physica A
106
,
278
(
1981
);
J. A.
McLennan
,
J. Stat. Phys.
28
,
257
(
1982
).
4.
T. L. Hill, Statistical Mechanics (McGraw‐Hill, New York, 1956), Chap. 5;
J. Chem. Phys.
23
,
617
(
1955
).
5.
T. A.
Osborn
,
Phys. Rev. A
16
,
334
(
1977
).
6.
R. D.
Olmsted
and
C. F.
Curtiss
,
J. Chem. Phys.
62
,
903
,
3979
(
1975
);
R. D.
Olmsted
and
C. F.
Curtiss
,
63
,
1966
(
1975
).,
J. Chem. Phys.
7.
B. C.
Eu
,
J. Chem. Phys.
63
,
303
(
1975
).
8.
J. T.
Lowry
and
R. F.
Snider
,
J. Chem. Phys.
61
,
2330
(
1974
);
R. F.
Snider
and
J. T.
Lowry
,
J. Chem. Phys.
61
,
2330
(
1974
).,
J. Chem. Phys.
9.
J. A.
McLennan
,
J. Stat. Phys.
28
,
521
(
1982
).
10.
Y. L.
Klimontovich
and
D.
Kremp
,
Physica A
109
,
517
(
1981
);
Y. L. Klimontovich, D. Kremp, and M. Schlanges, in Transport Properties of Dense Plasma (Birkhauser, Basel, 1984), Vol. 47, Experientia Supp.
11.
Let LLoLm denote the three‐particle Liouville (super) operators associated with full, free, and channel m = (ij)(k) dynamics, and Ω,ΩmΩm denote the 1→−∞ limits of eitLe−itLo,eitL,e−itLm,eitLm,e−itLO, respectively. Then one has Ω = ΩmΩ and the corresponding “decomposition” of the recombination superoperator τR = τ(12)(3),(1)(2)(3) = Vr(i2)(3)Ω = τ(12)(3)⋅mΩm where V(12)(3) = [Vl2+V13] and τ(12)(3),m = V(12)(3)Ωm. Snider and Lowry (Ref. 8) write τR = Σmτ(12)(3),mΩm/3 associating the mth term with stabilization (ij)*+(k)→(ij)+(k). However by construction all terms are equal even if different atomic species are involved.
12.
F. T. Smith, in Kinetic Processes in Gases and Plasmas, edited by A. R. Hochstim (Academic, New York, 1969).
13.
D. K. Hoffman and J. W. Evans, in Proceedings of the International Symposium on Few‐Body Methods and their Applications Nanning, Peoples Republic of China, August, 1985 (World Scientific, Singapore, 1986).
14.
R.
Gau
,
M.
Schlanges
, and
D.
Kremp
,
Physica A
109
,
531
(
1981
).
15.
D. K.
Hoffman
,
D. J.
Kouri
, and
Z. H.
Top
,
J. Chem. Phys.
70
,
4640
(
1979
).
16.
J. W.
Evans
,
D. K.
Hoffman
, and
D. J.
Kouri
,
J. Chem. Phys.
78
,
2665
(
1983
).
17.
J. W.
Evans
,
D. K.
Hoffman
, and
D. J.
Kouri
,
J. Math. Phys.
24
,
576
(
1983
).
18.
C. G.
Chandler
and
A.
Gibson
,
J. Math. Phys.
14
,
1328
(
1973
);
in Mathematical Methods and Applications of Scattering Theory, edited by A. W. Saenz et al. (Springer, New York, 1981).
19.
Gy.
Bencze
,
C. G.
Chandler
, and
A.
Gibson
,
Nucl. Phys. A
390
,
461
(
1982
).
20.
N. Dunford and J. T. Schwartz, Linear Operators, Part III, Spectral Operators (Interscience, New York, 1971).
21.
J. W.
Evans
,
J. Math. Phys.
22
,
1672
(
1981
);
J. W.
Evans
,
24
,
1160
(
1983
); ,
J. Math. Phys.
J. W.
Evans
and
D. K.
Hoffman
,
J. Math. Phys.
22
,
2858
(
1981
).,
J. Math. Phys.
22.
D. J.
Kouri
,
H.
Krüger
, and
F. S.
Levin
,
Phys. Rev. D
15
,
1156
(
1977
), and references therein.
23.
For another perspective, one could think of the Osborn specification of a as tracing the system back in time to determine the chemical composition. Only when the system is in (chemical) equilibrium will this composition remain constant during the tracing‐back process.
24.
The possibility of modifying the choice of H(12…n) or H(12…n), to phenomenologically account for many body effects, naturally suggests itself.
25.
When acting on Has eigenvectors [duals] of energy Ek[Eb], we have Ω± = Ω±(Ek) = lime→oΩ(Ek±iε)[Ω̃± = Ω̃±(Eb) = limE→oΩ̃±(Eb±iε)] where Ώ(z) = |+Gas(z)hΟ(z) = |+G(z)h,[Ω̃(z) = |+Ω̃(z)hGas(z) = |+hG(z)], and Gas(z) = (−Has)−1,G(z) = (z−H)−1. One also has S± = |∓2πiδ(Ek−Eb)T±, where the T‐matrices T± = hΩ± can be replaced by ± = Ω̃±h. Corresponding energy‐labeled T matrices, and scattering equations for these, follow from the above discussion of energy‐labeled Möller operators. The transition superoperator has the form τA = T±AAT̃±+T±AT̃±Gas±(E)−Gas±(Ek)T±AT̃±. In the two‐body case, where the single channel (1) (2) is involved [since (12) is removed], one has τ(12)±A = [V12sc12±12±*] = [V1212±12±*].
26.
R. F.
Snider
,
J. Chem. Phys.
32
,
1051
(
1960
).
27.
The idea of substracting out unwanted coarser clustering (albeit nonrecursively) from PA has been discussed in the context of Boolean algebras for commuting projectors. See
C. I.
Ivanov
,
Physica A
107
,
341
(
1981
);
S. Golden, Quantum Statistical Foundations of Chemical Kinetics (Clarendon, Oxford, 1969).
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