BULLETIN OF THE LEBEDEV PHYISICS INSTITUTE
P.N.Lebedev Physics Institute of the Russian Academy of sciences

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1. Title:
NORMAL OSCILLATIONS OF TWO-DIMENSIONAL DUST CLUSTERS WITH A REGULAR POLYGON SHAPE WITH PARTICLE IN THE CENTER
Authors:
N.G. Gusein-zade, V.N. Tsytovich, S.G. Amiranashvili.



Abstract:


2. Title:
RAYLEIGH LINE WING IN A SOLUTION WITH A CLOSED PHASE SEPARATION REGION
Authors:
K.V. Kovalenko, S.V. Krivokhizha.



Abstract:


3. Title:
EFFECT OF AN ELECTRIC FIELD ON OPTICAL INTERBAND TRANSITIONS IN SEMICONDUCTOR HETEROSTRUCTURES
Authors:
P.V. Ratnikov, A.P. Silin.



Abstract:


4. Title:
ELECTROINDUCED SELECTIVE DRIFT OF AQUA-COMPLEXES IN SALT SOLUTIONS
Authors:
V.I. Boiko, M.A. Kazaryan, I.V. Shamanin, I.V. Lomov.



Abstract:


5. Title:
UP-CONVERSION ENERGY TRANSFER FROM THE 4S3/2 LEVEL OF Er3+ IONS IN YAlO3 AND YLiF4 CRYSTALS
Authors:
V.P. Danilov, V.P. Kalinushkin, M.I. Studenikin.



Abstract:


6. Title:
MEASUREMENT OF OPTICAL PATH LENGTH GRADIENTS USING CORRELATION PROCESSING OF DIGITAL PHOTOGRAPHS OF RANDOM PATTERNS
Authors:
V.N. Borkova, A.V. Kraisky, T.V. Mironova, T.T. Sultanov.



Abstract:


7. Title:
APPLICABILITY OF THE CONCEPT OF TOWNSEND COEFFICIENT IN STRONG ELECTRIC FIELDS
Authors:
A.N. Tkachev, S.I. Yakovlenko.



Abstract:
An analytical expression is obtained for the electron-energy distribution function in a strong electric field. The derivation is performed in the assumption that the retardation force in the equation of motion for an individual electron in a gas can be ignored. The distribution characteristic width corresponds to the energy acquired by an electron at a distance equal to the reciprocal of the Townsend coefficient. Calculations of the energy distribution function are carried out for electrons multiplied as a result of gas ionization in a homogeneous electric field at different distances from the cathode. This distribution function normalized to unity is shown to be no longer coordinate-dependent at distances from the cathode exceeding greatly the reciprocal of the Townsend coefficient. This distribution function coincides with the analytical expression obtained. The behavior is coordinate-independent even in a very strong electric field when, in accordance with the traditional viewpoint, the majority of electrons are runaway ones.