Hyperfine structure of the mossbauer spectra of 119^Sn^(4+)in Сr_(2)O_(3)
Hyperfine structure of the mossbauer spectra of 119^Sn^(4+)in Сr_(2)O_(3)
K.P. Mitrofanov, P.B. Fabrichnyi, E.V. Lamykin, A.M. Babeshkin, and L.P. Fefilat'ev
The d—Λ—d system
The d—Λ—d system
N.N. Kolesnikov and S.M. Chernov
Use of photomultipliers for superheterodyne reception of modulated light
Use of photomultipliers for superheterodyne reception of modulated light
V.A. Dianova, V.N. Parygin, and A. Savenok
On the motion of asteroids of the hecuba type
On the motion of asteroids of the hecuba type
I.A. Gerasimov
The equations of scale and conformal invariance in Bogolyubov's axiomatic approach
The equations of scale and conformal invariance in Bogolyubov's axiomatic approach
N.V. Krasnikov
Velocity distribution in a fluid flow with a free surface
Velocity distribution in a fluid flow with a free surface
L.A. Bukina and N.K. Shelkovnikov
Carrier heating in ferroelectric semiconductors
Carrier heating in ferroelectric semiconductors
V.L. Bonch-Bruevich
Efficiency of the alternating-current ferromagnetic frequency multiplier
Efficiency of the alternating-current ferromagnetic frequency multiplier
E.Yu. Smirnova
The maximum power and efficiency of a polyphase ferromagnetic frequency multiplier are calculated in the square hysteresis loop approximation.
Show AbstractPropagation of high-frequency disturbances along a flat electron beam
Propagation of high-frequency disturbances along a flat electron beam
V.L. Kuznetsov
A solution of Vlasov's linearized kinetic equation is given for propagation of high-frequency disturbances along a flat high-density electron beam moving in an external electrostatic field for the case of complete passage of the current and current limiting by the collector potential. An example of disturbance propaga tion in an accelerated electron beam is considered.
Show AbstractToward a microscopic theory of the optical potential
Toward a microscopic theory of the optical potential
F.A. Zhivopistsev
Expressions are obtained in the Green's function formalism for the optical poten tial with consideration of the contributions from inelastic scattering processes with excitation of particle-hole states of the target nucleus. The dependence of the optical potential on the energy is governed by the interaction of the particle with more complex states of the intermediate system that are excited in the direct processes.
Show Abstract