SCIENTIFIC ABSTRACT KULIK, I.O. - KULIK, M.S.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000927420002-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 2
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

69689
S/126/60/009/03/012/033
E193/E483
Investigation of Certain Physical Phenomena Occurring at High
Temperature on the Surface of Crystalline Substances. IV. Analytical
Study of the Kinetics of "Self-Healing" of Artificial Defects on the
Surface of Solid Bodies
and 1 = 10-4 cm, the following values of y were
obtained for copper, silver, gold andnickelt
YCu. =~10-4i yAg*= 10-31 yAu ze lo-6, yNi -_ 10-3.
There are 4 figures and 8 references, 6 of which are
Soviet and 2 English.
ASSOCIATIONiKharlkovskiy gosudarstvennyy universitet
Kharlkovskiy filial IRYeA (Khar9kov State
Khar1kov Branch of IRYeA)
SUBMITTED: July 3, 1959
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University

87209
S/126/60/010/001/021/027/XX
F,032/E314
AUTHORS: Zillberman, G,Ye. and-KmJJkl,jt.0.
TITLE: on the Relaxation Time of Fast Electrons in a Metal
PERIODICAL*~ Fizika metallov i metallovedeniye, 1960,
Vol. 10, No. 1, PP. 9 - 13
TEXT: The authors consider an electron in a band lying
above the conduction band in the case where the energy of
the electron is insufficient to excite plasma oscillations
and the finite range is due only to collisions with the
conduction electrons. The following cases are consideredt
sr; rs; ss and rr , where rs denotes the case where the
scattering electron lies in the conduction band and the
scattered electron in the band above the conduction, and prior
to the collision,and similarly for the other combinations.
Explicit expressions are derived for the relaxation times for
collisions in the above types of interactions. Yt is shown
that the limitations imposed by the band structure on the
collisions can increase the relaxation time by a large factor.
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67209
S/126/60/010/001/021/027/Xx
E032/E314
On the Relaxation Time of Fast Electrons in a Metal
There are I figure and 9 referencesf 4 Soviet and
5 non-Soviet,
ASSOCIATIONi Kharlkovskiy filial Vsesoyuznogo NII
khimicheskik)- reaktivov (Khar1kov Branch of
the All-Union NII of Chemical Reagents)
SUBMITTED: January 14, 1960
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133728
S/056/60/038/004/021/048
Z(Ooo B006/BO56
AUTHORSt Zillberman, 0. Ye., Kulik, 1. 0.
TITLEt Quantum Oscillations of the Photoelectric Yield of Metals in
a Magnetic Field
PERIODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 3e, No. 4, PP. 1186 - 1200
TEXTt I. M. Lifshits, A. M. Kosevich, and A. V. Pogorelov already pointed
out the importance of investigations of the quantum oscillation effects
for the problem of the oonseryation of the dispersion law of conduction
electrons in certain metals. The best-known of such effects are the
deFaas - van Alphen effect and the Shubvikoy - de Haas effect; the
former was experimentally investigated in the USSR by B. I. Verkhin,
B. G. Lazarev at al. (Hof. 3). The present paper describes the theoretical
investigation of the external p4p~qelectric.effect on metals in a magnetic
field in the ultraviolet spectral range. Let the magnetic field be
assumed to be perpendicular to the surface, so that the electrons are
free to reach the anode. Under these conditions oscillating compounds
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83728
Quantum oscillations of the Photoelectric 8/056/60/038/004/021/048
Yield of Metals in a Magnetic Field B006/BO56
occur in the photoelectric current besides the compounds changing
monotonically with H. One of them is due to those oscillations of the
electron atate number in the magnetic field, which cause the do Haas -
Van Alphen effect. A second one is due to periodic dependence of the
transition matrix element on the magnetic field, and is not interrelated
with the state number; it is a new oscillation effect, which is common to
all optical phenomena and is connected with transitions between the bands.
An investigation of this effect in principle permits determination of the
position of the individual regions of the Fermi surface in the reciprocal
lattice. The third component represents an interference effect. A further
new quantity, which may be obtained from photoelectric experiments (of
the energy distribution of the departing electrons), is the shape of the
isoenergetic surfaces which are lower than the Fermi surface. The
investigation of the quantum oscillations of the volume (external) photo-
electric effect carried out in the ultraviolet for electrons possessing
an arbitrary dispersion law, thus furnishes not only theoretically
interest!,ng results, but also gives indications for experiments. Thus, it
is also pointed out that by means of photoelectric experiments, the
possibility is, in principle, given with comparatively weak fields to
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83728
Quantum Oscillations of the Photoelectric
Yield of Metals in a Magnetic Field
in'vestigate large groups of electrona whose
under usual experimental conditions due to
effect experiments a narrow light ray can be
one block. The effect investigated in this
de Haas - van Alphen effect, actually only
on its genesis (the wave functions). The authors
M. 1. Kaganov for discusaing,this paper. M.
(Ref. 2) are mentioned. There are 5 figures
6 M, 3 British, 1 Swiss, and 4 German.
S/056/60/038/004/021/048
B006/BO56
oscillations are blurred
the block structure. In photo-
produced which covers Just
case depends, as also the
on the dispersion law and not
thank I. M. Lifshits and
Ya. Azbell and E. A. Kaner
and 21 references: 7 Soviet,
&O,SOCIATIORt Kharlkovskoye vyssheye aViRt3ionno-inzhenernoye voyennoye
uchilishche (Khartkov School of Higher Learning for-Airforpe
Engineers). Kharlkovskiy gosudarstvennyy universitet
(Kharlkov State University)
SUBMITTEDs October 9, 1959
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0
36378
S/r,58/6P,/000/005/073/119
AO61/AlO1
AMHORS Kulik, 1. 0., Zillberman, G. Ye.
- ME:
.i.1, Impurity distribution in crystal gro%-Lh from a melt
PERIODICAL: Referativnyy zhurnal, Fizika, no. 5, 1962, 11, abstract 5E90 (V sb.
"Rost kristallov. T. 3", Moscow, AN SSSR, 1961, 85 - 89. Discuss.,
214 - 218)
TZM: The distribution of an impurity over the volume of a single crystal
grolvm from a melt has been determined. In this problem, the decisive factors
are two concurrent processes: -impurity and heat flows. The former flow is deter-
mined by diffusion and thermal diffusion, and the latter by-thermal conductivity
and heat transfer by diffusion. In addition, the presence of a tempeftture field
in the melt - crystal system leads to the distorti6n of the crystallizatlon front
and makes the impurity distribution more complex. The problem is solved by the
method of successive approximations. The effect of heat transfer by diffusion
is neglected altogether, and the temperature field is found from one closed equa-
tion with given boundary conditions. In the problem of diffusion in zeroth ap-
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S/058/62/000/005/073/119
Impurity distribution in crystal growth from a melt A061/AI01,
proximation, pure diffusion with a plane crystallization front is considered.
Corrections for the impurity distribution due to the thermal diffusion effect
and to tho distortion of the crystallization front are obtained in first and
second approximations, respectively.
K. Gurov
[,'ibstracter's note: Complete translation]
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BFLOZOROV, D.P.; KULIK, 1.0.; ZILIBMMAN, G.Ye.
Distribution of impurities in crystals grown from melts. Kris-
tallograftla 6 no.2:279-282 Mr-Ap 161. (MIRA 14:9)
1. KharIkovskiy filizl Instituta khimicheskikh reaktivov.
(Crystals--Growth)

KIJLIKI 1.0.
Momentum distribution function of Fermi particles in'gas_
within tbe~high-density. Zhur. eksp. i teor. fiz, 40 no'5:
3.343-2352 My 11618 (MIU 34:7)
1. Fiziko-t~khnicheskiy institut AN Ukrainakoy SSR.
Field theory)
Coulomb functions)
Partioles .(Nuclear physics))
~

S/056/62/042/OOZ/036/055~
BIOO/B104
AUTHORs Kulik# 1. 0.
TITLE: Some features of the oollootivo energy losses of fast elec-
trons passing through an aninotropic plasma
PLRIODICAL: Zhurnal ek&perimentallnoy i tooreticheskoy fiziki, v. 42,
no. 2, 1962, 543 - 551
TEXT: The plasina oscillations in a gas of quasiparticles (electron plastaa
in a uniaxial crystal) are discussed. The dispersion law for plasma
oscillations, U3 0 (t), is derived with the classical equation of motion.
p p
Expanding 1/('Z_ into series with respect to N11/113 a4/ap - velocity
of quasiparticles) one obtains in zeroth opproximation for k---YO
(Vn)t d.,
where 4 is the unit vector in the di ection of vF is the electron
velocity on the Fermi boundary. The integral has to be taken over the
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31056162104210021'0361055
Some features of the... B108/B104
Yer;ni surface F_(4). At k,~