PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY
Series: Nuclear and Reactor Constants

since 1971

Русский (РФ)

ISSN 2414-1038 (online)

ADDITIONAL CHARACTERISTIC OF THE SOLUTION OF THE NON-STATIONARY TRANSPORT EQUATION

EDN: CHGKRS

Authors & Affiliations

Popykin A.I.
Scientific and Engineering Centre for Nuclear and Radiation Safety, Moscow, Russia

Popykin A.I. – Leading Researcher, Cand. Sci. (Phys.-Math.). Contacts: 2/8, Building 5, Malaya Krasnoselskaya st., Moscow, Russia, 107140. Tel.: +7 (499) 753-05-24, e-mail: This email address is being protected from spambots. You need JavaScript enabled to view it..

Abstract

S.B. Shikhov in his monograph “Problems of the Mathematical Theory of Reactors. Linear Analysis” established in the most general conditions that the solution of a linear non-stationary transport equation is represented by a semigroup of operators (hereinafter referred to as a semigroup) in a number of functional spaces and studied its properties. The structure of the spectrum of the (non-stationary) transport operator was established, including the condition for the presence of a leading eigenvalue in it. A leading eigenvalue is a simple real eigenvalue greater in modulus than all the others and which corresponds to a (unique) positive eigenfunction. One of the consequences of the established properties is the presence of an asymptotics of the semigroup, determined by a single exponential, to which a positive distribution in the phase space corresponds. This is a useful property of the non-stationary transport equation for substantiating perturbation theory and other methods for solving it. It is used in the qualitative analysis of pulse and some other experiments and has the following simple physical interpretation. When the initial condition is set, after some time the sensor placed at any point in the configuration space will first register a signal proportional to the neutron flux, which will then become exponentially dependent on time.
The article shows that, in certain cases, also quite general, the mentioned semigroup is Markov, i. e. it corresponds to a random (Markov) process. In this case, the transition probability of the Markov process has the same properties as the semigroup under consideration, i. e. it has exponential asymptotics, which is useful when considering this process.
The article uses minimal information from the theory of Markov processes and provides all the necessary definitions.

Keywords
reactor theory, non-stationary transport equation, smoothness properties of the solution of the transport equation, Cauchy problem, operator semigroups, spectrum of the transport operator, cone of non-negative functions, random modeling of particle transport, theory of random processes, Markov process, ergodic property

Article Text (PDF, in Russian)

References

UDC 621.039

Problems of Atomic Science and Technology. Series: Nuclear and Reactor Constants, 2025, no. 4, 4:5