XII.—On the Theory of Unimolecular Gas Reactions: A Quantum Harmonic Oscillator Model

Author(s):  
N. B. Slater

SynopsisThe writer's theory of unimolecular dissociation rates, based on the treatment of the molecule as a harmonically vibrating system, is put in a form which covers quantum as well as classical mechanics. The classical rate formulæ are as before, and are also the high-temperature limits of the new quantum formulæ. The high-pressure first-order rate k∞ is found first from the Gaussian distribution of co-ordinates and momenta of harmonic systems, and is justified for the quantum-mechanical case by Bartlett and Moyal's phase-space distributions. This leads to a re-formulation of k∞ as a molecular dissociation probability averaged over a continuum of states, and to a general rate for any pressure of the gas.The high-pressure rate k∞ is of the form ve-F/kT, where v and F depend, in the quantum case, on the temperature T; but v is always between the highest and lowest fundamental vibration frequencies of the molecule. Concerning the decline of the general rate k with pressure at fixed temperature, k/k∞ is to a certain approximation the same function of as was tabulated earlier for the classical case, apart from a constant factor changing the pressure scale in the quantum case.

Nature ◽  
1962 ◽  
Vol 196 (4850) ◽  
pp. 159-160 ◽  
Author(s):  
ALFRED BOBROWSKY
Keyword(s):  

Entropy ◽  
2018 ◽  
Vol 20 (8) ◽  
pp. 552 ◽  
Author(s):  
Simon Saunders

The Gibbs Paradox is essentially a set of open questions as to how sameness of gases or fluids (or masses, more generally) are to be treated in thermodynamics and statistical mechanics. They have a variety of answers, some restricted to quantum theory (there is no classical solution), some to classical theory (the quantum case is different). The solution offered here applies to both in equal measure, and is based on the concept of particle indistinguishability (in the classical case, Gibbs’ notion of ‘generic phase’). Correctly understood, it is the elimination of sequence position as a labelling device, where sequences enter at the level of the tensor (or Cartesian) product of one-particle state spaces. In both cases it amounts to passing to the quotient space under permutations. ‘Distinguishability’, in the sense in which it is usually used in classical statistical mechanics, is a mathematically convenient, but physically muddled, fiction.


2009 ◽  
Vol 9 (3&4) ◽  
pp. 336-360
Author(s):  
M.B. Hastings ◽  
A.W. Harrow

We introduce the concept of quantum tensor product expanders. These generalize the concept of quantum expanders, which are quantum maps that are efficient randomizers and use only a small number of Kraus operators. Quantum tensor product expanders act on several copies of a given system, where the Kraus operators are tensor products of the Kraus operator on a single system. We begin with the classical case, and show that a classical two-copy expander can be used to produce a quantum expander. We then discuss the quantum case and give applications to the Solovay-Kitaev problem. We give probabilistic constructions in both classical and quantum cases, giving tight bounds on the expectation value of the largest nontrivial eigenvalue in the quantum case.


1989 ◽  
Vol 1 (5-6) ◽  
pp. 333-336 ◽  
Author(s):  
I. V. Aleksandrov ◽  
A. P. Goncharov ◽  
I. N. Makarenko ◽  
A. N. Zisman ◽  
E. V. Jakovenko ◽  
...  

2015 ◽  
Vol 13 (04) ◽  
pp. 1440001 ◽  
Author(s):  
Aram W. Harrow ◽  
Ashley Montanaro ◽  
Anthony J. Short

The Johnson–Lindenstrauss Lemma is a classic result which implies that any set of n real vectors can be compressed to O( log n) dimensions while only distorting pairwise Euclidean distances by a constant factor. Here we consider potential extensions of this result to the compression of quantum states. We show that, by contrast with the classical case, there does not exist any distribution over quantum channels that significantly reduces the dimension of quantum states while preserving the 2-norm distance with high probability. We discuss two tasks for which the 2-norm distance is indeed the correct figure of merit. In the case of the trace norm, we show that the dimension of low-rank mixed states can be reduced by up to a square root, but that essentially no dimensionality reduction is possible for highly mixed states.


1990 ◽  
Vol 68 (10) ◽  
pp. 5357-5359 ◽  
Author(s):  
Q. Bi ◽  
J. M. Brown ◽  
Y. Sato‐Sorensen
Keyword(s):  

1994 ◽  
Vol 75 (3) ◽  
pp. 1463-1466 ◽  
Author(s):  
Hitoshi Yusa ◽  
Takehiko Yagi ◽  
Haruo Arashi

2002 ◽  
Vol 17 (09) ◽  
pp. 1301-1325 ◽  
Author(s):  
D. MAURO

In this paper we study the classical Hilbert space introduced by Koopman and von Neumann in their operatorial formulation of classical mechanics. In particular we show that the states of this Hilbert space do not spread, differently from what happens in quantum mechanics. The role of the phases associated to these classical "wave functions" is analyzed in detail. In this framework we also perform the analog of the two-slit interference experiment and compare it with the quantum case.


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