SCIENTIFIC ABSTRACT SITENKO, O.G. - SITENKO, V.M.

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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

, " / - T ", ! "! !~, (k.. f -
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AKRIYEZER, 0.1.; SITEIIKO _La"nko, O.H.]
Diffraction nuclear processes at high energieB. Ukr.fiz.zh,2r.
no.l.-16-34 Ja-F '58. (PIRL 11:4)
l.Fiziko-tekhnichnir institut All MISR.
(Colligione (Nuclear 1)hysice)

7-1 S -
Al-hi~-ezcr, ~_. I. '~'iterko A. G. SO';/56- 3 5- 1 - 16159
TITLE: Or, t',.e Theory of t,.e Excitation of H~ydro.7an.netic Waves
(K teorii vozbuzhden_Jya gidroma:,nit1nykh Voln)
L
PERIODICAL: Zhurnal ekspc-rimentallnoy i teo.,:etic'.---ieskoy fiziki, 1958,
Vol, 35, Nr 1, pp. 116 - 12o (U.SR)
ABSTRACT; In conductive liquids located i.% an external magnetic
field hydromagnetic and magneto--acoustic waves are able
to propa.-ate (Ref 1). Lundquist (Lundkvist) (Ref 2)
investicated. the behavior of hydromagnetic waves in a
liquid (Hg) durinC,; the mechanical excitation of waves
by means of a revolving disk. it is, finally, possible
to excite hydromajnetic waves ly -means of external variable
currents. in the present paper the latter possibilit,y is
theoretically investi.-lated, anei the intensity of excitaticn is compared

. U (I
with that attained by mechanical means. First, a perfectly
conductive compressible liquid is assumed to exist, which
is located in an external magn~7-tic field and is subjected
to the action of external currE!nts. The initial equations
for the following deliberation* are the hydrodynamic basic
Card 11 2 equations as well as 1-ilaxwell's (Maksvell) equations.

On the Theory of the Excitation of Hydromagnetic Waves SOV/56-35-1-16/59
'7(l,t) is here set up -is Fotwier(Furlye) integral, and also
for the current density j, rk,Lo) the Fourier components are
written down; the wave e 0ation in the perfect liquid
W-1
and, further, an expression for the intensity are derived.
Furthermore, an expression is also derived for the intensity
of excitation as well as for the velocity of the propagation
of the hydromagnetic waves in consideration of a damping,
by basing on the assumption that the liquid possesses only
finite conductivity and is viscous. There are 2 references,
1 of which is Soviet.
ASSOCIATION: Fiziko-tekhnicheskiy institut AP:ademii nauk Ukrainskoy SSR
(Physico-Technical Institute AS Ukrainskaya 99R)
7
SUBMITTED: January 29, 1958
Card 2/2

3 CV5 ~', -3 51- 5 - 33/56
AT!TIIORS Sitenko, ~.. G. , Borezhnoy, Yu. J-
TITI,h: On the Diffraction Spallation of Light Nuclei (0 diffraktsion-
nom rasshchoplenii leukikh yader'
PZ- LI 0 D T1, Z"itirrial eksperimentallnoy i tcor:!ticheskoy fiziki, 1958,
Vol 35, I?Ir 5, pp 1289-1291 (IJSSR'
B~.'TRACT: In the present paper the integra:. crosz; sections of various
proces.~es of the diffraction intaraction. between a deuteron
and a black nucleus is calculatel for any ratios R /R. Here
Rd denotes Mae radius o-, the deu-;eron and R the ragius of the
nucleus. The Coulomb (Kulon)-irteraction was neglected. For
the Iourpose of simplifying calcu'-ations a Gaussian function
was used as a deuteron wave func-.ion. The comparatively
eL~sily obt,:ined expressions for -;he total cross section a t
of all processe2, fol. the cross 3eCtions a n and a p of neutron
an~] proton otrippiin,. ' respectivel.-(, and for the cross section
oe of elastic scattering are exi,,Licitl-7 written down. The cross
lard 112 sections 0 of diffraction 91,allation and the absorption
d

u n V :. e D i f f r,,!. c t i o r, I a t i o n o fLi,-,,Iit Nuclei SOV/56-35-5-31/r;()
cross section G of the deuteron can be calculated from the
relations 0 d + S e = LTt/2, a a + a n + a P ~ CTt/2. Irext, approximat-
ed formulae 'or the limiting cases q >> 1 ani q ~~ 1 ara --iver_
Fo,- tlie parameter q i4 11olAs that q = 4R/_~T R d' As a r-esult
of liffraction tne total cruss iaection of pion-leuteron in-
teraction is less t1laii tile sun of the total cross sections
of the interaction between a rion ain,,' a neutron and a proton.
Diffraction also is Aue to the f~ict that s1rallation of the
flauteron is caused by the scatterinj~~ of a pion by a deuteron
in the ~,rourid state (ad >> Ce in tite domain R < 'Rd the inte-
,ral cro:~n ~;ectiono depoud in a I.A.-h de:-,re- on the selection
of the vl~,ve function of the deutercn Crc-Ain.l stato. '"here are
2 fi~-,,res a-rid 4 references, 1 of Ythich is Soviet.
KharI!,.o-!skiy ~rosudarstvennyy tlniVE~rsitet (Kharlkov State
JTn ivers i by)
31! BM ITTED Ji?ne 2111, 1950
Card 2/2

sov/58-59-8-18374
Translated from: Referativnyy Zhurnal Fizika, 1959, N'r 8# p 194 (USSR)
AUTHORS: Sitenko, A.G., Stepanov, K.N.
TITLE: On the Interaction Between a Charged Particle and an Electronic Plasma
PERIODICAL: Uch, zap. Khar'kovsk. un-t, 1958, Vol 93, Tr. Fiz. otd. fiz.-matem.
Cak., Nr 7, pp 5-13
ABSTRACT.: The article computes the energy losses of a charged particle moving in
a plasma with velocity V. In the computations allowance is made for
the thermal motion of both electrons arid ions. If V>R- Se (Se is the
average velocity of the thermal motion of the electrons), then the
losses are principally caused by the Ji%teraction of the particle with
'> Si the contribution of interaction with
the electrons. When Se~P V >
ions becomes substantial, if V3
S 3 M
(m and M are the masses of tfie electron and ion respectively). The
determination of the magnitude of the losses is also given for the case
Card 1/2 of highly degenerated electronic gas and for the case where the plasma

sov/58-59-8-18374
On the Interaction Between a Charged Particle and an E2ectronic Plasma
moves as a whole. Neither the thermal
ions is taken into consideration in the
being present. In this case the energy
Cherenkov radiation. The bibliography
motion of the electrons nor the effect of the
case of an external permanent magnetic field
losses due to iistant interactions represent
has 9 titles.
B.N. Gershman
Card 2/2

SIMTKO, A. G., Doe Pbys-YAth Set (diss) -- "Direct processes in the interaction
of mcleons with nuclei". KharIkov, 1959. 14 pp (Min Higher Educ Ulw SSRO
KharIkov order of Labor lied Banner State U im A. M. Gorlkiy), 150 copies M., 170
22, 1959, 107)
%A.

21(l.8); 24(5) pnAss 1 Dom sewrianow 507/3369
Tamsoymmaya owzhvuzovskaya konferentaiya po kvantovoY toorli poloy
I tooril. elmental-nykh chasti to. Uzhgorod, 1958
Prabl, savromennoT.taorli slementernyUh chftBtit&. No. 2: Trudy
roblew In the Modern Theory or Elementary
ll
t
a
...
konforen
tartlel*3. Mr. 2; Transactions of the All-UnIon Inter-Vuz
Conference art the Quantum Pi eId Theory and the Theory Of
n Particles) Uzhgorod, 7-karpatakaye ablastnoye Izd-ro,
tW
T

P. 5,COO copies printed.
ZI
19 .
26.t Ta. Lonsadve, Docent; Tech. Xd.z M. Beloun.
FURPOStj This book is intended,ror physicists, particularly those
concerned with problemB In the field of elementary particle& and
the quantum theory.
COVKKAG1: ThIs book contains articles on elementary pKrticloo
originally read at the All-Unlon Inter-Vuz Conference hold at
orod State University on October 26, 1958. Among the topics
Uzh
4
discussed are: the spinor field theory, the fusion theory,
14rents contractions, parity 3tUdl*S. nucleon-nucleon scattering,
etc. ftalish abstracts Accompany each article. References
each article.
SokO4~, O.A. 11" Formulation or Fusion Theory 26
I
14IL3'LdzO YutN~ And B.I. XAUAIAQ~~Appllcatlon
of
'
_
Schw1hgoile Variatjaln--M~
thod to the Pair Theory
30
fokollk, G.A. GentrallxattM Of the Lorent. Group 37
1vanIt&kaM_ ' C?P~ Generalized r-julvalent potential an,
`
tX4 3e4iiinZW-6
f inrinitea1=1 LOreatz contractions Und,.
Notary Motion
MOkOlLk. G.A. ROPrOaWnt,dtiOn Or the complete 14fenta GMUp 52
Sokolik, G.A. Connection B&tween the 'Anomal" Representation
of the Spsze-TIM. Inversion Group and the Pau.11 Transformations 56
and A.'?. Mdik
DOn-C01011412tiOn of Parlty In Rag 58
And R.N. RYndIn. Determination or rarity
Pirclc2ez- 63
L
am'sadze
YU
M
T
P
'
he
-
-
,
assible Versions or the jr
Decay 7b#or7
69
V~M3hIn-_2W!k_-zquations or the Second Order for Spinor
'Vivo rFai-ations
80
-X01OtZ1?v V-0. Conservation Of the Combined parity, se &
run"maOtml IF of the 3y=atr7 in Mature
83
Ge~t*mn_yn" B'V' Polarization Of EldatrOns Of the Txwer
C
onvormlon Subbequon't to
-0 -- r)&Cay- Taking Into Account
t
he Xl*ctrIc ft*ld of tbe
Nucleus
89
"PizetiOn Or the Nucleons Under the
.-~On In the 1119h Mnergy Region 99
n!g_1Ma~_RL-_M4vo l9quatlona r., Xle.~nt.,7 Partial*& log
Ditrashankov; V.S., and ILXt
_j=XPshO,. Some Remarks on the
Xamer Structure of the Nual"n

Solovoy"' 7a' on the SUPOrrIU14 State of an Atom gual 117
ou,
226 j)0,

IJU
1 54
'Jim
NA"
Igo A 1113 1
MIP0,13-Z 5
Art .44 a
-k S
tj 31
N,M 1
A Iflo
04

-ja
3061r. lull
13111
jr
ilk- ~Ijj
ilu m

SITINKO, A.G. [Sytenko, O.H.]
Theory of nuclear reactions involving complex particles. Ukr. fis.
zhur. 4 no.2:152-163 Mr-AP 159- (MIRL 13:1)
l.Kharikovskiy gosuniversitet i FizIko-tekhnioh*skIy Institut
AN USSR.
(*aclear reactions)

[Tartakovslkyi,
Kharskovskiy gosudarstvermyy universitet im. A.14.Gorlkogo.
(Dentcro as--Diffrac tion)

SITENKOP A. G.
"On the Polarization of Nucleons in High Energy 3tripping Reactions,
.Nuclear Fbysics, 9, No. 3, Jon 1959, 412-419 (North BDUArd Publ. Co., Amsterdam)
Abstract: Polarization of Nucleons stripped from deuterons in high energy
encounters with nuclei Is determined on the basis of i;he generalized diffraction
method in which account is taken of spin-orbit interaction.
Physico-Tech. Inst, Ukr SSR Aced. Sci., Khar1kov

21M SOV/56-'36-3-20/71
AM90R: Sitenko, A. G.
TITLE: On the Fission of Nonspherical Nuclei (0 delenii nesfericheski"h
yader)
PERIODICIIL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
vol 36, Nr 3, pp 793-797 (USSR)
A13STRACT: The bombardment of stable nuclei with fast particles may, if
the excitation entergy of the compound nucleus is greater than
the critical fission energy, lead to fission. In a non-
spherical nucleus with rotational de:qree of freedom the centri-
fugal force occurring in consequence of a rotation of the
nucleus may lead to nuclear fission. The fission of a non-
spherical nucleus caused by the abso:7ption of a particle with
great momentum may occur directly without the intermediate
stage of the formation of a compound nucleus. It may theoreti-
cally also be treated as a direct fission process. In the
present paper the author theorelically investigates this
direct fission as a consequence of a transfer of a large
, ular momentum of the nucleus by "he absorbed particle. First,
anr I
the fission conditions of a rotatini-: nonsphericnI nucl.euc)
Card 1/2 (excentricity E2 = 1 - b2/a2, a >, '.1) are investigated. Ex-

On the Fission of Nonspherical Nuclei SCV/505-36-3-20/71
previsions are given for the total energy, Coulomb (nion)
ener.-Y,rotation energy, the variation of energy as a result
of deformati n, and for the critical value for the square of
the torque L?, which leads to fission for L2 >z L2. Further,
the energy o? the nucleon impinging uy3n the nucTeus is in-
vestigated and a formula ic derived fc.r the cross section of
direct fission in the absorption of a fast nucleon. For high
energies of the impin-ing nucleon this expression coincides
with the total absoE
-Ption cross section:
0 a b ( _Vr1 __F_2+Iarc sin F, E ~>> Em
2 E
In conclusion, the direct fission of nonspherical nuclei in
the case of the stripping of neutrons ins investigated. The
author finally thanks A. I. Akhiyezer,,, K. A. Ter-Martirosyan
for discussions, and H. A. Khizhnyak for valuable remarks.
There are 7 references, 4 of which are Soviet.
ASSOCIATION: Kharlkovsl:iy -,osudarstvennyy universit:!t (Khar1kov State University)
SUBMITTED: June 12, 1958
Card 2/2

21M
AUTTIORS: Vysotskiy, G, L,, Sitent"o, A. G. SOV/56-36-4-20/70
TITLE: On the Theory of Direct Nuclear Reactions With the Participa-
tion of Polarized Particles (F teorii pryamykh yadernykh
reaktsiy s uchastiyem polyarizovannykh chastits)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, '959,,
Vol 36, Hr 4, PP 1143-1153 (USSR)
ABSTRACT: In the introduction, the authors dincuss the subjects and the
results of a number of English pape.cs (Refs 1-111) dealing with
similar problems. The present paper was intended to work out
a theory of direct nuclear reactions (strippino reaction and
deuteron formation) in which polarized particles participate;
such reactions are widely used in nuclear spectroscopy. For
their investigations the authors use the method of Derturbed
waves; the spin-orbit interaction is neglected because it
makes a comparatively small contri':.ution to the cross section.
Also Coulomb effects are net-lected because they are insig-
nificant in the case of sufficiently hiCh eneri-ies,, The paper
deal's with a mathematical investiCation of the angular dis-
tributiorl and polarization of the -' )roducts of stripl;ing- and
Card 1/3 capture reactions during- the actio:-i of polarized particles

On the Theory of Direct lNuclear Reactions dith SO'1/56-36-4-28/70
the Participation of Polarized Particles
'ion of
pon arbitrarily oriented nuclei. Vie angular Olistribut
u
protons J.-;roduced in the casp of stripping relations under the
influence of polarized deuterons haE azimuthal asymmetry~ An
investigation of this asymmetry offers the possibility of det-
ermining the spin of the residual niieleus in the final state,
Also other possibilities of usin.r- s-rippino reactions with
polarized detiterons for the purpose of obtaining additional
data on nuclear structure are investi-ated, In detail, it
was found possible to determine the reduced widths for states
with different values of the orbital momentum of an absorbaHe
neutron. The formation of deuteron3 on nuclei by polarized
protons is also characterized by the angular distribution -with
azimuthal asymmetry, The deuterons produced on thhie --iccasion
are polarized, The capture reaction under the influence of
polarized nucleons can be neglected- in order to obtain polarized
deuterons. The various chapters of this paper deal with the
following subjects: The (d,p) strippina reaction with polarized
particles. After the problein has been dealt with in a general
manner, a special investiCation is carried out of three simple
Card 2/3 cases: a) nucleus and deuterons are not polarized, b) the

On the Theory of Direct Nuclear Reactions With SOV/56-36-4-28/70
the Participation of Polarized Particles
nucleus is not polarized and deuterons are polarized, c) the
nucleus is polarized and the deuterons are not. The next part
deals with (d,p)- capturing reactions with polarized particles,
Again the cases a,b, and c are deaLt with specially after a
general investigation.. In the lasi; chapter the angular dis-
tribution and the polarization of protons are finally calculated
for the concrete case of the react-4on B11(d,p)B12 by using the
given parameter values. The resul-;s obtained are shown by a
diagram. The authors thank Yu. BerezhnV and V. Kharchenko
for their help in carrying out numerical computations. There
are 1 figure and 15 references.
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii Nauk Ukrainskoy SSR
Physico-Technical Institute of the Academy of Sciences,
Ukrainskaya SSR) Kharlkovskiy gosudarstvennyy universitet
(Kharikov State University)
SUBMITTED; October 2, 1958
Card 3/3

21(7)
AUTHOR: Sitenko, A. G. sov/56-36-5-i6/76
TITLE: On the Scattering of Fast ir-Mesons on Deuterons
(0 rasseyanii bystrykh IY-mezonov na deytronakh)
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, 1959,
Vol 369 Nr 5, PP 1419-1422 (USSR)
ABSTRACT. Experimental data concerning (ir p) scattering show that elastic
collisions have diffraction character at E,>1 Bev, i.e. that
scattering occurs mainly at small angles (Refs 1-4). BeleAiy
Refs 5, 6) succeeded in carrying out a theoretical analysis'of
qr 9p)-scattering on a general basisq Grishin and Saytov(Ref 7)
~
investigated (p,p) scattering at high energies in a similar
manner; further investigations of (jr9p)-scattering were carried
out by Blokhintsevv Barashenkov and Grishin (Ref 8) andfurnished
results concerning the proton radius and nucleon structure. The
author of the present paper investigates (Tr,cl)-scattering; at
high pion energies it is also d-iffraction scatter-Ing at which
the shadow effects must be taken into account, the existence of
which was pointed out for the first time by Glauber. The
Card 1/2 investigation was carried out by `L-he author in accordance with

On the Scattering of Past fr-Mesons on Deuterons sov/56-36-5-16/76
the method developed by Belenkiy. Expressions are given for the
total-, the scattering-, and the absorption cross section, and
further also for the corresponding angular distributions. The
equations obtained are evaluated by means of experimental data
in references I and 2 for Eir - 1.4 Bevq and results are shown
by two diagrams. The integral (-q-,d) scattering cross section
is found to be equal to the double elastic (Tr p) scattering
cross section. In the (Tr1d) absorption cross section the
shadow effect is distinctly marked. Figure 1 shows the course
of angular distribution in the case of (Tr,p)-scattering and
figure 2 shows that in the case of (irld) scattering. The author
thanks A. I. Akh-iyezer for discussing the results
obtained. There are 2 figures and 10 references, 4 of which are
Soviet*
ASSOCIATION: Kharlkovskiy gosudarstvennyy =dversitet (Khartkovstate
University)
SUBMITTED: October 30, 1958
Card 2/2

211(5), 21(7) SOV/53-67-3-1/4
.'UT-ZOR Sitenko. A. G.
T V17" U The Interaction of Deuterons With Nuclei (Vzaimodeystviye
deytonov s yadrami)
PERIODICAL: Us,~ekhi fizicrv!skikh nauk, 1959, '701 '67, Nr 3, PP 377-444 (USSR)

.',T!STRACT: The present paper gives a very detailed survey of the important
field of deuteron-nucleus interaction; the survey is essential-
ly theoretical. In the introduction the problem as such is
i.,
discussed in short. Cha-,)ter I deals vith 4.,e interaction be-
tween deuterons and nuclei within the ranr--c of low and medium
ener '-ies. First, the elastic scattering of deuterons is inves-
ti~;ated, and the part ~.'.ilayed by Coulomb (Kulon) interaction,
deuter-on structure and its influence upon. elastic scattering,,
the effect of tunneliri~~ throu--h the barrier and the scatterin,-3

(Ruther!~ord (PezerfOlrd)
of nean ener,-
y deuterons on heavy nuclei
,
scatterin~~) are subjected to a short mathematical treatment.
lie 4 11
I followinF jz:,.r2c-raph deals -,-ilth tne strip-inj reactions
(,J,p) and(d,n); `-e t,.o-atep -Procesz A + d --w C ---b B + p
(formation of a cor-M,~n,1 nucleus) and -the iirect .11 + d - 3 + 7D
process are discussed in s'iort, an-! in the following, the
Card 1/4 energy relations, the an,,Tular dis tribut ions in the case of

The I-:teraction of Deuterono '%I/ith lluclei S C) V/'- A
such strip.Anc,", reactions, consideration of spins, the plane
wave apzoroximation method, transition to 'the Serber model, and
consideration of the finite nuclear mash are discussed and a
s:,.ort com:,aricon wit, exDerimental results is made (7iE.-s 4-6).
Further, the consideration of deuteron- and -,proton waves is
investi -ated an,_'~ comillared with experiT.-,ental data; in t-e fol-
loviine it is shown in what way such stripi.Ang reactions may
render an investigation of nuclear structure po'--sible. Further,
this rara.-I-aph leals with the effects ezercised by polariza-
_7ul~r correla!.iona in
tion in strippin- reactions., with anj -
(LI,py) and (d,n,) reactions, with deuteron production in
nucleon-nucleus collisions, as well as with other direct pro-
cesf;es develonin ~~ with the narticination of deuterons. Para-
'Lrral)h 4 teals with (d,p) and (d,n) reactions connected vith
the formation of a compound nucleus. The follo-uinC subjects
are discussed in detail: determination of reaction az~.plitudes,
and the croos sections of such reactions. llara!,'Taph 5 deals
with the inelastic scattering of leiterons. First, the pos-
-ible 1inds of processes are discussed in short, after which
tile excitation of' the nucleus in t*.-,,:~ scatterin-, of deuterons
and deuteron disintegration in scatterinc, are dealt with.
Card 2/4 Para-raph " deals with the interaction between deuterons and
U -

The Interaction of Deuterons With Nuclei SOV/53-67-3-11/4
heavy nuclei. The individual sections of this paragraph in-
vestigate deuteron reactions in the Coulomb field, the (d,p)
reaction on heavy nuclei, and deuteron disintegration in the
nuclear Coulomb field. Part II of thio paper deals with tile
interaction between deuterons and nuclei in the high energy
ran,,2;e. ParajTaph 7 deals with the diffraction interaction of
deuteron3 and nuclei, and in the individual subsections the
author discusses general problems of nuclear diffraction, the
diffraction scatterin.- and diffraction disintegration of deu-
terons, the stripping reactions at high energies, the total
deuteron-nucleus diffraction cross sections, and the inter-
action between fast nucleons with deuterons. Paragraph 8 deals
with the disintegration of fast deuterons in the nuclear
Coulomb field and, specifically, with electric and magnetic
deuteron disirite,-ration, and with neutron polarization in
electromat,netic deuteron disintegration. In paragraph 9 the
author finally investigates deuteron proluction in the case
of collisions between fast nucleons and nuclei and discusses
the methods of deuteron production and direct as well as in-
direct capture. In cliapter III mathematical problems con-
cernin,-~ an integral and the poseudopotential are discussed
Card 3/4 in Short. '-here are 18 fijures and 125 references, 25 of

Th I Deuterons Witil 'Tuclei SOV/5-z-'-7-3-1/'4
e Tlit eraction of ') t)
which are Soviet.
Card 4/4

SITENKO., A.G.[Sytenko, O.H.]; TARTAKOVSKIY, V.K. (Tartakovslkyi, V.K.]
Polarization and quadrupolarization of deuterons in elastic scattering
on nuclei. Ukr. fiz. zhur. 5 no. 5:581-50.0 S-0 160. (MIRA 14;4)
1. Fiziko-tekhnicheskiy institut, AN USSR i Kharlkovskiy gosudarstvennyy
universitet.
(Deuterons--Scattering)

88456
A*~61'00
AUTHORS:
TITLE:
PERIODICAL:
S/056/60/039/006/048/063
B006/BO63
Sitenko, A; G., Gurlyev, V. N.
Inelastic Scattering of High-energy Electrons by Nuclei
Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960-1
Vol. 39, No. 6(12), Pp. 1760-1765
TEXT: A theoretical study has been made of inelastic scattering of fast
electrons by nuclei, which is accompanied by ejection of nucleons from the
nucleus. Such investigations furnish data on the dynamic properties of
nuclei. There are two types of inelastic scattering; inelastic electron
scattering may be accompanied by excitation of higher energy levels of the
nucleus and furnishes data on the nuclear levels. On the other hand, it
may also lead to an electrodisintegration (emission of protons or neutrons)
and thus gives direct information on the momentum distribution of nucleons
in the nucleus, which depends on their spatial correlation. These data are
important to the further development of the theory of nuclear structure,
especially for the mode of two-particle interaction between 'the nucleons.
The electromagnetic interaction between a fast electron and a nuclear
Card 1'/4

88456
Inelastic Scattering of High-energy
Electrons by Nuclei
S/056/60/039/006/048/063'
B006/BO63
proton, which is considered a non-relativistic oarticle, is discussed,
and the ejection probability for this proton is calculated in a
perturbation-theoretical manner. An expression is derived for the matrix
element of tho interaction energy, in which only the two-particle cor-
relation is taken into account. For the limiting case of a high momentum
of the ejected proton one obtains
4e4
dc Z (A- 1) Sg(q K) 6 (AE - s, -..)E,) dkdK, (9)
rAe
g (q K) dr, dr,e(q-K)r-,p.,, (ri, r(10)
1) (2:t)a
S (I + 2x)) fl
2
+ -L (q 2K + i (I + x) JqaJ),rJ U I:'.I
2M
the function K is further studied. This function has a sharp
maximum for q (i.e., when the momentum -of the ejected proton is.equal
to the momentum loss of the electron). -q - 1~ - ~' and ~E - E-El are the
momentum and energy, respectively, transferred from the electron to the
Card 2/4

Inelastic Scattering of High-energy
Electrons by Nuclei
88456
S/0516/60/039/006/04-8/063-
B006/BO63
proton. e, hi and V-are the char e, mass, and wiomalous magnetic moment of
the proton c = 1. 7 r )T r r r
ap( Vi~ 21:_ a( 11 PU2) -'~ap 2), Tk(
exp(iir~) Ta(r) and 7P(r) are the proton and t.ieutron single-part:lale
functions, respectively. One obtains
g SL 1 ~ d' exD(i(` - ~/2)r where S is a quantity
a K -(17 j ) r q-K+ y
~'P 2n
averaged over all momentum values of and F. F)r the distribution function
one obtains
sin % r. %-'A'. sin V r, + os xr,
X2 cos % r, rc
orM x X2 +,,2
(17)
This relation is graphically compared with the empirical distribution
function obtained for C12:
g R - 3/2 a-3exp (_,,_2/cL2) , a2/2A1. 14 K'ev.
Card 3/4

-inelastic Scattering of High-energy S/O 5 6/68Q%~569/00 6/048/0 6 3
Electrons by Nuclei B0061BO6
Also other functions (e.-Ir., a2/2M = 18 Yev) are compared herewith.
12
Calculation of or C on the basis of the shell model yields g(x)
~ . 1, TE -t 2/!'2)exp(_1,2/z~2). -10-13 cm, 12 /2M = 5 Mev.
0, -3 (1 A For R = 3.07
3
Assuming 1 2/21.1 = 9.1 Idev, one obtains good agre,~ment with the empirical
curve. The energy distribution of electrons inelastically scattered on C12
is briefly discussed. A. 1. '-khiyezer is thankei for discussions. There
are 2 figures and 9 references: 1 Soviet, 7 US, and 1 British.
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii nauk Ukrainskoy SSR
(Institute of Physics and Techno".ogy, Academy of Sciences
Ukrainskaya SSR)
SUBLTITTED: July 13, 19060
Card 4/4

ABELISHVILIA T.L.; SITENKO, A.G. [Sytenko, 0. If.j
Electric polarization of deuterons due t:) scattering by a
Colulomb field. Ukr. fiz. zhur. 6 no.1:3-11 Ja-F 161.
(MIRA 14:6)
1. Rhartkovskiy goaudarstvennyy universitet im. A.M. Gor1kogo.
(Deuterons)
(Polarization (El(ictricity))

SITENKO, A.G. [Sytenko., O.H.1; TARTAKOVSKIY, V.K. (Tartakovslkyi, V.K.]
Diffraction interaction of deuterons having semitransparent
nuclei with diffuse edges. Ukr. fiz. zhur. 6 no.1:12-19
Ja-F 161, (14IRA 14: 6)
1. Kharikovskiy gosudarstvennyy universitet im. A. M. GorIkogo,
(Deuterons-Diffraction)
(Nuclei, Atomic)

SITE,NKO,,_A.q. [Sytenko, O'~H.],- KRARCHEDIKO, V,F. I
Possibility of meastiring the polarization arising in the scattering
of a neutron by a neutron. Okr. fiz. zhur. 6 no.1:20-24
Ja-F 161. (MIRA 14:6)
1. Fiziko-tekhnicheskiy institut AN USSR i Khartkovskiy
gosudarstvennyy universitet im. A.M. GorIkogo.
(Neutrons-Scattering)
(Polarization (Electricity))

S/185/62/007/004/003/018
D407/D301
A U T H "-"IR S Sytenko, 'q. iL, and Drobachenko, IQ. V.
T,-ITLE: &n the influence of nucleon correlation on
the photo-effect
I
PERIODICAL; Ukrayinalkyy fizychnyy zhtxrnal, v. 7, no. 4, J1_1
1962, 357-359 \)I
In the Dresent article, the effects due to nucleon
correlation are taken into account. The interaction between
nucleons leads to a replacement of the rectangular momentum-
disLribution of a Permi-gas by a distribution in which the com-
r,onents aith large momenta are present. It was shown by S.
.. ;near 1939) that to the ground.
au babe (Ref. 4: Zs. Phys., 113, 4829
ztate of a nucleus with large mass number corresponds a momentum
distribution of the nucleonic~Fermi-gas at a temperature corre-
sponding to energies of 5 or 8 Pilev. One obtains the following
formula for the integral cross-section of dipole photon-
Card 1/4

S/la5/62/007/004/003/018
Or, the influence of... D407/D301
absorption by the nucleus:
Bx
O(Vl*)(Ivl 0.015A(l + 00 10 -24 Mev - cm2
8 TT 2M 4
B - - 7 -~(r)v(r)r dr. (2)
3 0
Assuming that the temperature e of the nucleus is low as com-
pared to 'he temperature of degeneration (909 the correlation
function assumes the form: 1 2
1
V (r) = - -
2 TI 4nr2 ~r sh(l-r
Card 2/4

Or. the ini"'luence of...
S/185/62/007/004/003/018
D407/D301
P 0 = V2 711 a 0 ~Po (4)
where n is the-mean nucleon-density. For the coefficient B,
one obtains the formula
1 2
sin by
2 3 A2 2
B L! S 0 b a y sh(TrAby) dy. (6)
3 )
0
Numerical values of B, obtained by means of data given in the
references, are listed in a table. Anaiogously, it is possible
Card 3/4

S/185/62/007/004/003/018
On the influence of.... D407/D301
to determine the mean energy of photon absorption, allowance
being made for thermal correlation betaeen nucleons. One obtains
T
lor the mean energy of absorption 71 = 66 7..ev. Thus, taking
4nto account thermal correlalions leads to an increase in the
mean energy of photon absorption. There are 1 table and 6
C~ - -
references: 3 Soviet-bloc and 3 non-Soviet-bloc. The references
L U
to the Ensrlish-language publications read as follows: J.
Levinc-er, H. Bethe, Phys. Rev., 7b, 115, 1950; K. Okamoto, Phys.
Rev., 116, 428, 1959.
A 0,1 T
~'-ATION: Khark-JvsIkyy CErzhuniversytet im. A. M. GorIkogo
(Kharkiv State University im. A. M. GorIkiy)
S U 3 Y I ' T T ----'D August 24, 1961
Card 4/4

2720k
S/056/61/041/002/026/028
Contribution to the theory of... B125/BI36
functions of particle systems undergoing electromagnetic interaction.
V. D. Shafranov calculated the correlation functions of microcurrents from
the equations of motion. F. G. Bass, M. I. Kaganov, and V. P. Silin
investigated plasma fluctuations, taking spatial dispersion into
consideration. The Fourier components of the correlatore of charge
transverse current density in a plasma read
r k' Im 81
I,. = i.- -j- TiI
r (0k), e -26 + pe
4 yi-i- I I + (ak)' - q, (z) - q) (P411 + 0/4) Z, (e + I.
1- (in, 1), IM of
b& 1112 - e, P
To (I - (4)
10), 0 - fl / I's - 2T (Z)I. +
This indicates that at ka>,,l low-frequency oacilla tiona are the moot
important factor in fluctuation spectra of q and J. The correlation
Card 2/9

27204
B/056/61/041/002/026/028
Contribution to the theory of... B125/BI38
function of the charge density reads
r/a,
2 1 1?- -6~ . .611 f q,.~
- 2e no L6 2 r r r' -P M-
4xa,
The spectral distributions of fluctuations of tho electric and magnetic
fields read:
Ime
-+2
I Tv
(9)
IM et
k.
respectively. The resulting correlation functions for the field strengths
read: -r/a
ln(T /T and AW-W (q)
i
2 4 e(1 +, 2
e k T 08 0)
d e
t6 (AW- 6J
(q)) +6 (33).
O
2 2
16R(mc (k2+q2
e
Card 8/9

G
00
06.1
tte
OIA
c 0
TI
IV" v~o 31 f
5 9erI 'A 01, -0sorv*-, ~ 0 t Va e -be
r a iov
B.'r t10,06 to
7a -011 *.,Ile sx1r, L,
17 -r~NXT t A . aeTea
bel -be
110. 5t-aal to 'be COIC'S3.
3'D- -,Oes to Wned Ir AS "YIell
oteD 9 C-r,.u . ,5e0, 0.55 e C
. ae a A-5 -.%~s 9.11
itj t 0,11 je'as T telltjo'l . t,rLe -roS
ell s c I. e 10 . jtxI ox
r",- e fLe . tyle I e '20 te0-
i: eoll tr,e 111a of u V.-a T 11 V,(I scav
ji'l .7,e . .bIe . D )* . the I e0,, t e-r
SI 'fl Vj 0 n-,Ic te
The 0 a nsl scat ca
%I Q 6 'S.116 tre s
eLls .,T 6 t ea- st-a I as I the
ts ~ - 'b"I of
11 rar er, - . stTI ose 11', cl e -rMS e
e Ci
r, C - -rl~ 01 PILIC9 j t'ae -. te Oce-
0 a, .01 sp
Ile OT 0 +
t 5 e Ile
teaL %Z-j ~30 yo~c e5 01
e-rj lo t%je el 91C 2
O-as -J~n 'Z I or,
t Ita 0 'bllt 1
st-rl
ap
s'pec",
06 a
ev to Calculate the nucleOn
L: a nuClear matter, the latter being considered
:,~ , /7 eas at -absolute zero. Subsequently,the
f

S/05 62./043/'001/043/050"
3102
0 tic i)ot'n'lial t""eory Y3104
r, 4:i~eruction on E is investigated, nuclear matter be'n-
u
z; o i- e ;-; to be a --upercondouctin- nucleon gas. Then the assumption of
~'C' .'C 1t0l"- a-M:) L 1-10 f(k,,Kl) bein- constant is dropped and the
I-: con:3i.~cre6 o:; the basis of the Fermi fluid (Landau) oodel.
-n Ithat the ,L~resence of a --ap in the densit
fluctuation spectru-n
I-) vc.i nuclei leads to a diminution of the 'VI of these nuclei
evc!'.-e
wit.,-, zhe W of odd nuclei. There are 5 fi6ures-
.%-'10" -ak.
KharIkovskiy gosudarstvennyy universitet (Kharikov SV -e
University)
T'" - ~D I'arch 4, !962

I-SITZNKO-,-k,G ~-SZYANI YU-TAY (Ghien Yu-tlafl
Coefficients of dynamic friction and diffusion in a plasma. Zbur.
tekh. fiz. 32 no.Usl324-1332 N 162. (MIRA 15M)
1. Kharlkovskiy gosudarstvennyy universitet ineni A.M.Gorlkogo.
(Plasm (Ionized gases))

s/i4l/63,/O06/Oo1/oo5/o18
Z14O/E135
AUTHORS: Sitenko A.G., and Simenog I.V.
TITLE: on fluctuations in a degenerate electron gas
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Radiofizika,
v.6, no.1, 1963, 54-64
TEXT: The authors believe that the space-time correlations
of fluctuations in an ideal Fermi gas have not previously been
considered, in spite of their importance-for the study of
diffraction processes in such gases, e.g. the diffraction of light
or electrons in metals, dIffraction-of nucleons in nuclear
material, etc. A further point of interest is to connect the
macroscopic parameters, e.g. dielectric constant of an electron
gas, with the microscopic theory through the fluctuation-
dissipation theorem. The simplest approach to such a study is
through the method of secondary quantisaticon. The authors first
derive the formulas
2 2
2 0 m2T I + IL/T-(w-k /2m) m/2k 'T
~6 n > In 2 2 12 c t h (12)
kw 2TCk 1 + elt/T-(w+k /2m) m/2k T 2T
Card 1/3

On fluctuations in a degenerate St. S/141/63/oo6/ool/oo.5/o18
E14CIE135
.2 0 MT, (w k2)2 m
kw 7Ck T 2m k2TI .~i
k2 2 m -I
a + I)c t h (13)
2m 2k2T j 2T
for the spectral distributions of density :fluctuations and the
transverse current in ap ideal Fermi gas at arbitrary temperature
T, where 00
X+t W1
(e + tdt.
(x)
0
This is then applied to obtain the dielectric constant of a
degenerate electron gas,-obtaining the well-known-formula usually
derived in the chaotic-gas approximation. The dispeksion of
q plasma oscillations, and the fluctuations of &'completely
degenerate electron gas are also found. rhere are 5 figures.
Card 2/3

297-63 E~n(l),Yg~G(k)/BDS/dC(b)-2/FS(w)-2 'AnTcAsDAm.~3AWL/
L7
~
up
:ACCESSIONNR: AP3004833 S/0141-/63/00i!-'/00!;/0469/0479
i AUTHOR: Sitenko, A. G.; Kirochkin, Yu. A.
TITLE: Dispersion of electromagnetic waves by fluctuati.ons in plasma in the
J
I presence of a magnetic field
i'SOURCE: IVUZ. Radiofizika, v. 6, no. 3. 1963, 469-479
TOPIC TAGS: electromagnetic wave, plasma, plasma fluctuations, thermal I
fluctuations
ABSTRACT: The present work, based on the theory of flactuations deve
loped ~y
A. Akhiezer, et al. (ZhTF, 41, 644, 1961), considers st:-attering of electrornag-
netic waves by fluctuations in nonisothermal plasma in the presence of a magnetic!
field; specifically, scattering by low-frequency Aliven ani magnetoacoustical
fluctuations. Both electron-density and electron-velocity- fluctuations are taken 1
into account, as well as magnetic -field fluctuations. Spe ctral distribution of
L-Card 1/2

L 17297-63
`7]
ACCESSION NR: AP3004833
scattered radiation is determined. Neglecting the, motion of Lone, the electro-
_J.
magnetic field in plasma is described by a set of differeiaial equations. This set,
i is reduced to a wave ~-quation which Is solved and Investigated. Correlation func-
tions of electron-density, electron-velocity, and magnetic-field fluctuations are
expressed interms of correlators of electron and total i:urrents with the use of
Maxwell equations. It is noted that in a strongly nonisothermal plasma, the funda-;
mental line in the spectrum of scattered radiation is spLit into four lines asso-.
ciated with the wave scattering by magnetoacoustical fluctuations. Orig. ar
t.
41 formulas.
has:
ASSOCIATION: Xhaikovskiy gosudarstvenny*y universitet (Y[hirkov State
iversitv)
n
U
SUBMITTED: 07jul62 DATE ACQ: 27Aug6 3 ENCL: 00
:SUB CODE: PH NO REF SOV: 004 OTHER: 004'
Card 2/2
I IL

SITEROY A.G. (Sytenko, O.H.]; KHARCHMKO, V.F.
Polarization phenomena in direct nuclear reactions taking spin-
orbital interaction into account. TJkr.fiz.ztur. 7 no,11:1149-
1159 N 162. (MIRA 15:12)
1. Khar?kovskiy gosudarstvennyy universitet,,
(Nuclear reactions)

3/185/63/008/0011/001/024.
~0 D234/D308
AUTHORS: Sytenko, 0. H. and Drobachenko, O.~ V.
TITLE: Theory of non-local potential
PERIODICAL: Ukrayinslkyy fizychnyy zhurnal,..v..8, no. 10 19639
5-10
TEXT: The authors consider proton scattering by protons assuming,-
that the interaction is described by a non-local potential and-i;-:,
taking into account the Coulomb repulsion. The equation of the ra-
dial function of the 8 state is solved..The effective radius-and
the form parameter are expressed in terms of the coefficients of
the expansion of the exact solution u and the a8-ymptotic one u,
assuming small energies. The:scattering length to, the limit k = 0
is obtained in terms of integrals of Bessel functions, then u
09
u are determined. The-scattering parameters expanded in
19 uot 1
powers of 1/BR are
Card 1/ 3

b (1 - 4 (25)
3 SR
The potential parameters and the effective radius are tabulated
and compared with those for the proton-neutron system. The diffe-
rences are small. but exceed experimental errorij; coulombic repul-
sion decreases S and b. There is 1 table.
ASSOCIATION: Kharkivslkyy derzhuniversytet im. 0. M. Hor1koho
(Kharkiv State University im. A. M. Gorlkiy)-
Khar-
kivalkyy aviatsiynyy instytut (Kharkiv Institute of
Aviation)
SUBDII TTED: July 25, 1962
,--bard 3/3

SITENRO, A.G. [Sytenko, O.H. ; STMENOG, I.V. [Symenoh, I.V.]
Theor7 of fluctuations in superconductors. Ukx. fiz. zhur.
8 noo5;537-548 My t63v. (MIPA 16:8)
1. Khartkovskiy gosudarstvennyy universitet i Institut
fiziki AN UkrSSR, Kiyev.

SITENKO, A.G. [Sy-tenko, O.H.]; DROBACHEDIKO, O.V.
Effect of nonlocal nucleon-nucleon interactt.on on the cross
section of the photoeffect. Ukr. fiz. zhur., 8 no.7.-728-731
Jl 163. (MIRA 16:8)
1. Kharvkovskiy gosudarstvennyy universitet im. GorIkogo i
KharIkovskiy aviatsionnyy institut.
(Nuclear reactions) (Photoelectricity)

SITENKO, A.G.; KIROCHKIN, Yn.A.
Scattering and transformations of waves dur to thermal fluctuations
in magnetohydrodynamics. Zhur. tekh. fiz. 33 no.11:1354-1365 N
163. (MIRA 16:12)
1. Institut fiziki AN UkrSSR i Kharlkovskiy gosudarstvennyy
universitet.

SITENKO, A. G. ; BEIREZHNOY~ Yu. A.
"Concernin.- the Diffrattion Break.LD of Deuterons."
report submitted for All-Union Conf on Nuclear Spectroscopy, Tbilisi, 14-22
Feb 64.
Inst Physics, AS UkSSR

SITEDIKO, A. G. Y K tev
"Ine-:.-.stic scattering of electrons by nuclei and pair correlations in nuclei."
report submitted for Intl Conf on Low & Medium Energies Nuclear Physicsy
Paris, 2-6 jul 64.

L 1593-66 94T(l)/EPF(n)-2/EZ(m)/EPA(W)-2 IJP(c) AT
AW5067590 BOOK EXPLOITATION UR/
~kO A. G..; StwNw-
Akhiyezer, A. L; Akhiyezer, 1. A.; Polovins R.-V.; RIM
Owl
P1 004 (Wfiektivnyye
Collective kolebaniyar plazme) Nbse
Atomizdats 1964. o162 p. illus.., biblio- 1,700 copies printeil.
~Z -Zll
MM 'kto
T71
TOPIC TAGS: plasma physics, plasma oscillation, charged paiticlep. magnetic field
plasma stability,,particle distribution, particle scatter
PURPOSE AND COVERAGE: This book is a presentation of the thleory of linear A
oscillations in "Collisiouless" plasma in which paired collii3ious do not exert
significant influence on its oscillations properties. Three basic problems we :'j
presented in the book; 'natural oscillations spectra,, stabilLty and instability
of various particle distributions, end fluctuations in homogmeous plasma. Me
book will be of interest to scientists working izr-the fields of physical and
technological problems such as: diffusion of radio waves in the ionosphere
end other plaBmasj stellar"radiomissions microrediowave w*:Lificstion and generem
tion with the aid of plasma, acceleration of charged perticla-s in plasma, 'rel&X-
ation in iDla-a. iDlasma dimmosis. etc.
Card 1/2

AP4010286 S/0048/641/028/001/0041/0045
AVMOR: Sitenko, A.G.; Kharchenko, V.F.
TITLE: Bound state of three nucleons and scattering of a nucleon by two others in
a bound state geport, Thirteenth Annual Conference on Nuclear Spectroscopy held In
Xiev)25 Jan to 2 Fab 19837
SOURCE: AN SSSR, Izveattya. Seriya fizicheskaya, v.28, no.1, 1964, 41-45
TOPIC TAGS., three-nucleon motion, nucleon scattering, Yamagunhi potential, nucleon-
nucleon scattering, bound nucleon states, scattering length
ABSTRACT: Investigation of the problem of motion of three nucleons can yield addi-
tional Information on the interaction between nucleons. In contrast to the problem
of two-nucleon motion in the range of low energies, the problem of the notion of
three nucleons proves to he more sensitive to the form of the two-particle potentiaL
Henco the question of selecting the interaction potential to be used for the calcu-
lations in very important. In the present study there Is considered the problem of
the notion of three nucleons on the assumption that theinteraCtiOn between then In
t
deFcribed by a nonlocal potential with separable variables (Y.Yamaguchl,Phys*Rev.,
I
9&'1628,1954). The problem of the motion of two nucleons can be solved precisely
CqM 1/2

Y
AP4010288
'In using this type of nonlocal potential. In the case of the problem of three nucl-
:ebna this potential leads to a system of two Integral equations for the total spin
.W-w 1/2 and one Integral equation for S = 3/2. On the basis of the general equa-
lti'ons there are considered the particular cases of the tritium nucleus and elastic
~scattorlng of a slow neutron by a deuteron. For the latter case there are written
.tho expressions for the amplitudes of elmistic'ocattering of the neutron by the dou-
toron in the doublet and quartet states. The results of the nalculations of the
scattering length are compared with experimental datao The agreement in good for
the quartet casel but poor for the doublet came. Orig.art.hao: 26 formulas and 3
figures.
ASSOCIATION: Kharlkovskiy gosudarstvenny*y universitet, (Dar' 1cov State Univeraity);
Inatitute fisiki AkademLl nauk SSSR UnstLtute of ftsice, Acuideaq of SciencespSSSR)
SUBMITTEDs 00 DATE AM 1OFeb64 EMCM OD
stm CW91 SR REP NOV: 008 OWRI 006
Card 2/2

L~ITEIIKC, Grigorlyevich; 6HESTOPALOV, V.P., P'CC,, :,4"f.
red . ; 'Y IVI-7N, KC , L. I . p re -6
[Electromagnetic fluctuations in a plasma] Ele'.Ctrom-i~;nitllye
fluk-tuatsii v plazrre. KharIkov, Izd-vo Kharlkwskogo univ.,
i965. 194 P. (MIRA 18:5)

L 23014-66 odr(M)/t
ACC NR: Ap6o14825 SOURCE CODE: UA/0367/65/ool/oo6/0994/1001,
AUTHOR: Sitenko, A. G.; KharchenkoL V. F.
ORG: Institute of Physics, AN UkrSSR (Institut fiziki AN UkrSSR)
"and the three-nucleon bound state
TITLE: 'Neutron-deutron doublet--spatte-ing lengt
taking tensor forces into account
SOURCE: Yadernaya fizika, v. 1, no. 6, 1965, 994-1001
TOPIC TAGS: nucleon, neutron acattering, neutron, deuteron, integral equation
ABSTRACT: The motion of three nucleons is considered, the inter-
,action between which is described by-the Yamaguchi potentialg
taking tensor forces Into account. The problem of three nucleons
in the bound state and the seattering of a zero-erergy neutron on
-dim
.a deuteron are reduced to the solution of a systex. of one en-
.sional Integral equations. The doublet neutron-deuteron scat-
tering length, binding energy, And wave function of three nuoleons~
An the bound state are determined.from a numerical solution of--,rJ
theIintegral.equations..Orig..art. has: 2 figures and 18 forinulas.- (tased on
authors' Eng. abst.] [JPRS1
SUB CODE: 20 / SUBM DATE: 17Aug64 ORIG REF: 010 OTH REF: 007
.17

SITENYOS, O.G.; 'STICLOG, I.V.
f", 1%
Rule cf suma and twc-mc-lLor) in nuclel.
nr,.4:603-613 0 165. /k m ~ R A I ?, -. ,~. " ~
.... Institut fizi.M. &K UrSSR,

. C .. i. ] , i*.![;, R(7fif al, t
t
!-;~ , -I- . I " t f C, v I - 'C' V.F.
I of the of three nucle-OnF, taking tensor forces
Ant* account. Ukr. liz. zhur. 10 .5;469--48D My 165.
L L no
(YjIFA 18 t 5)
1. L,stttut ftzikl AN Ukr33',17 Kivev.

--------------
L 60332-65 RtT (I )1E PF(n) _21EWG (m)/M (w) - 2Pz-~/k-4/Pi-4 I'TP(C) 'AT~
ACCESSION NRz AP5018291 uR/(o57/65/03S/0O7A165/W6
.5334,9
AUTHOR% Sitenkoj A. G.; R-adziyevskiy, Ve N6
;-~:' . 1/3
TITLE.- On the fluctuations in a ma that is not In equilibrium
SOURCEt Zhurnal tekhnicheskoy fizikil ve 35, no* 7, 1965~ 1165-1176
TOPIC TAGS.- magnetoactive plasma, fluctuationj plasiaa beaminteraction, plas
charged particlep plasma electromagnetic wave
ABSTRACT: The author4 discuss the electric field and current fluctuations in a
uniform rarefied plasma: in a unifona magnetic field* The plasma is assumed to.
be in a quasi-equilibrium state in which the ion and':electron velocity distrib
tions are different and non-Maxwellian., so that the fLuctuation-dissipation
theorem is not applicable. The electron and ion fluctVations.are first treated.
as independent and their coupling through the action.of the self-consistent _7
field is sub-3equently taken into account Collisidnsl~between the ions and elec-
The general-equations derived for the-current
trons are neglected throughout*
and field fluctuations are rewritten for the specific,case of aplasma thatiis" A=
traversed by a neutral beam of charged particles moving parallel to the applied A
Card 1/3

AcassioN NR-. kp5oi8291
magnetic field, Simple approximate express
tions of this system that are associated with 1"gmuir waves and witfi'magnetic
sound, The interaction Pf different kinds of waves Oith the fluctuations is
discus3eds There is possible not only incoherent scIfItering but-also a-quasi-
coherent scattering with frequency changes associated with Langmuir and Alfven .
waves and with magnetic sound. It is-also possible, for waves of one kind to
give rise to waves of another kind by-interaction with the fluctuations* Equa-
tions describing these processes are derived. The i~iteraction of a moving
charged particle with the fluctuations of a (not necossarily magnetized) plasma
is discussed. When the velocity of the particle is Less than the thermal veloc- I:'
ities in the plasma the fluctuations accelerate the particle* A more rapidly
moving particle loses energy,to the fluctuationsp and these energy losses can
become anomalously large under certain eircumstances,p which are discussed in.
some detail* "In conclusion.. we express our gratitude to A*I&Atg_yezer and
77

L 156Q-" EWT(1)/ETC(F)!WF(n)-2/EWG(a)./T- _IJP(0) -AT
00'' -
.:ACC NR: AP6000219 SOURCE CODE:*Ul~/0056/6~/045/005/-1591/16
1AUTHORS: Sitenko, A. G.; Gurin, A. A.
3/91
,;ORG: Ins-titute of Physics, Academy of Sciences,UkrSSR (Institut
fiziki Akademii nauk UkrSSR) rz
iTITLE: Ef*fect of paz'ticle collisions on plasma f uctuations
!SOURCE: Zhurnal eksperimentallnoy i teoreticheskcy fiziki, v. 49,
ino. 5, 1965, 1591-1600
iTOPIC TAGS: plasma oscillation, particle collisicn, temperature
':dependence, plasma temperature, plasma density, k~Vekk, evcj~io",
JABSTRACT: The authors studied the effect of binary collisions on
fluctuations, using a kinetic equation witt a model collision
iintegral in which the energy and momentum of the particles are con-
~served.- The introduction of a model collision integral makes it
ipossible to study plasma fluctuations for arbitrary values of the
I.effective binary collision frequency, and not merely limiting low or-I
-ibigh values, as in the past. A single component non-isothermal plas-11--
Card__

L 15661-66
ACC NR: AP6000219
CL is investigated. The fluctuation-dissipation t*;.ieorem is used to
find a general expression for the correlation function of the random
'forces. Allowance for the binary collisions between particles leads
ito additional correlation of the random forces in velocity space.
General expressions are obtained for the spectral distribution of
the particle density fluctuations and for the temperature fluctua-
tions and for the dependence of the fluctuation spectrum on the
particle density, temperature, and binary collision frequency. The
relation between fluctuations Inji collisionless plasma and fluctua-.
tions in hydrodynamics is also studie4 as is the scattering of
electromagnetic waves by fluctuations of density and temperature
It is shown that the temperature fluctuations exer-IL-1 an appreciabie
influence on the scattering with small change of frequency in the
case of long wavelengths. Orig. art. has: 2 figurea and 26
formulas.

L 27472-66
ACC M AT6oo8416 SOURCE CODE: MV31YI~6510WIAW000310018
AUTHOR-.' Sitenkop A, G.; S~~j is Y.
------------------- -,'
ORG:
N okle!
'TITLE: Sum rules and two-micleon correlations in nuclei
SOURCE: AN UkrSSR. Fiziko-tekhnicheskly ingstitut. Doklady.. no. 142IT-016, 1~6
DvuMnuklomWe korrelyataii v yadran, 3o-]V
TOPIC TAGS: inelastic scattering, scattering crone section, electron scatteringp..
correlation statistics, spectral distributionp nuclear shell Model., even even
nucleus, spin orbit coupling
ABSTRACT: The authors establish a general relation between Vie cross section for
inelastic scattering of electrons and the spectral distributions of two-nucleon
correlation functions in the nucleus. The cross section for inelastic scattering
of a fast electron by an individual nucleon of the nucleus in first calculated on
the basis of perturbation theory under the aammption that thiv nucleon is non-
relstivistic* This cross section is then expressed in terms of the spectral dis'm
Card .1/

.1 27479.46
Acc m: AT6ooUi6
tributions of the space-time correlation functions for the nucleons In the nuclon
in terms of the current density., spin density,, and spin currerit operators of the,
nucleons. This is followed by calculation of the two-particle correlation func-
tions for the nucleons in the nucleus on the basis of the shell model of the
nucleus. The angular and energy distribution of the electrons in inealstic scat-,.,
tering by even-even nuclei can then be determined on the basis of the obtained
relations. The equations are simplified noticeably if spin-o3~bit interaction ls~
neglected. Byway of an example) some rules for the correlation functions*are
established for the nuclei He,, OIL6,j and-C440j and the influence of the motion of
the center of mass on the correlation functions is considered-with-He4 as. an
ex=ple. Orig. art. has: 3 figures and 43 formalas.
SUB CODE: JIUM DATE: 00 AM Mw.- 001/' OTH 1w: OWL',-
20/
2/2
C,rd
LG

TITLE: inelastic scatteri of electrons by nuclei and two-Varticle correlatims
in nuclei
-SOURCE: AN UkrSSR. Fiziko-tekhnicheskir institut. 3pokladrv no. 142/T-3.o6, 19650
Dvukhnukro_nEWye korrelyatsii v yadrakh, 19-31
TOPIC TAGS: inelastic scatteringp scattering cross section., electron scatteriMp
correlation statistics, spectral distribution, Fermi gas
ABSTRACT: The authors establish a general relation between the cross section for
the Inelastic scattering of fast-,'electrons by nuclei and the spectral d1stribu-.,
tions of two-nucleon correlation functions in the nucleus in the case vhen the
inelastic scattering is accompanied by a transfer of a definLte momentum and a
definite energy from the electron to the nucleus. The expre3sion shows that In-
elastic scattering of electrons by nuclei is connected both with fluctuations of
CQd 1/2

NRs AP6019335 SOURCE CODE: TF,
AUTHOR: Sitenko, A. G.- Berezbn!)Z, Yu. A.
ORG: PNr~~~~~~~iziko-tel&nicheskiy institut A11 UkrSSI)
TITIE: Effect of the deutero4 Internal structure on diffraction scattering
SOURCC-i Yadernaya fizika, v- 3, no- 3. 1966, 521-525
TOPIC TAGSj deuteron, partiole diffraction, neutron interaction, proton interaction,
deuteron scattering
ABSTRACT: The influence of the finite radius of the neutron-proton nuclear interact
Ge- the
in the deuteron and of the deuteron internal structure on the magnitud . of
integral cross-sections of various diffraction interactions between deuterons and
nuclei and on-the differential cross-section.for elastic deuteron scattering is
considerede The authors express thanks to V. A. Yamnitskiv for assistance in pro-
gramming the numerical calculations on an electric co t~j t 4, Origs art* has: 5
figures and 13 forrmUas. fBased on authors' Engs abs, 7._T~~f
SUB CODEs 20 SUBM DATE-' 281TAY65 / oRiG Rriwi oo4 y' oTH REF: ool
Card 1/1

AP6019627 A W SOURCE CODE: UR/0048/1;6/030/002/0328/0330
Sitenko, A.G.; Kharchenko,V.F.
~ORG: Institute of Physics of the Academy of Sciences of tho VkrSSR (Institut fiziki
,Akadeniii nauk UkrSSR)
~TITLE: Taking tensor forces into account in the three-nucleon problem /Report,
wPifteenth Annual Conference on Nuclear Spectroscopy and Nuclear Structure, hold at
:Minsk, 25 January to 2 February 19637
:SOLVRCE: AN, SSSR. Izvestiya. Seriya fizicheskaya, v. 30, no. 2, 1966, 328-330
TOPIC TAGS: nuclear structure, nuclear force, nucleon interaci;ion, three body
problemx tritium
XBSIRACT: The authors (Izv. AIN SSSR. Ser. fiz. 28, 41 C1964); Nucl. Phys., 49, 15
11963)) have previously treated the three-nucleon problem with the assumption of non-
Ilocal central two-body forces. In the present paper they exteD-d their previous
I
~calculations with the aid of the potential of Yoshio Yamaguchi and Yoriko Yamaguchi
~(Phys.Rov. 95, 1635 (1954)) to take tonsor forces into account. The calculation of
~the zero-momentum neutron-deuteron scattering length and the triton binding'onergy
ois reduced in the case of tensor forces, as previously In the case of central forces,:
~to the solution of a set of linear integral equations. The integral equations were
~solves numerically with the aid of a computer, using values of -.-.he parameters in the
Card 1/2
I card

ACC NRI AP7004570 SOURCE CODES UR/0056/6!i/049/003/1591/1600
AUTHORt _51tenkojLA.._9.;.GUr1n, A. A.
ORGs los-t-ituto of Mysics 1Jk_i9S~K_(Inst1tut f iziki AN UkrSSR)
TITLE1 Effect of pArticle collisions on fluctuations in a alAsma
t.- -~f -_
SOURCE: Zhurnal eksperimentallnoyA teore I ieskoy fiziki v. 49, no, 5,
1965, 1591-1600
TOPIC TAGSt particle collision, plasma physics
ABSTRACTt The authors use the kinetic equation with the Bhatnagar-Gross-Krook
collision Integral model as the basis for an Inveattgntion of the effect of pair
collisions between particles on fluctuations In a plasma. The Introduction of the
model collision integral makes it possible to investigate plasma fluctuations for
an arbitrary value of the effective pair collision frequency. The article
Investigates the case of a single-component, nontsothermal plaima. The fluctua-
tion-dissipation relation is used to find a general expression for the
correlation function of random forces. It Is shown that allowance for pair
collisions between particles leads to an additional correlation of random forces
In the velocity space. General formulas are obtained for the spectral distribu-
tions of particle density fluctuations and temperature fluctuations. These
formulas are used to investigate the effect of the magnitude oj! the effective
pair collision frequency on the shapo of the spectrum of particle density and
temperature fluctuations, from the collisionless case to hydrodynamics.
Orig. art. hass 2 figures and 26 formulas. (4~RS: 341,65V
SUB QODE: 20 / SUBM DATEI 08Jun65 / ORIG REFS 003 / OTH REF; 003

L 10241-67
bOT/0258
ACC NRi AP602B553 SOURCE CODZI I%% W09
AUTM: Sitenko, Ae'Ge
ONG: Institute of 1AWsleop M UkrSSRj, Xlev (Institut.risild M MOM)
nnz: seetteriag aW transformation or waves In a magnetosclive plasma
SOURCE: Uspekhi fisiche~kM nm*p ve 89p no. 2v 106,, 22T-4,58
TOPIC TAGS: magnetoactive plasma, plasma wave propagation, electromegaetic wave
scattering, dispersion equation, plassia interaction I
AB8270=: This is a review paper devoted to a theolletical 11mestigatlon of the *loc-
trodynamic properties of a homogeneous magnetoactive plasm The propagation of waves
and excitation of waves by external currents In such a plAsw6 are anelpod on the
basis of kinetic theory. The fluctuations or different ybysical, quantities character-
izing the state of the sagnetoactive plasms. are Investlgatedj as mv processes of tbA
scattering of waves and their mutual transformation by fluct%stions In the plasm.
The section headings are: 1. Zlectrodynamle propez iss of a magnetoactive plasma. (the
dielectric tensor and Its connection with the particle dIstributionp the dispersion
equation,, wave polarizationv and energy flux density). 2. Wives In a magnstosetive
Plasm (hIgh-frerjency and low%-frequeMY maves)- 3- Naltation of wMes In a 00900to-
active plasm by eztcr=Ll cwrm . 4. Fluctustlons In a maWntoactive plasma (eol-
lective cobazen fluctuations and their correlation faft Ionti, effective temperature,
fluctustlon In equMbrims and wellibrIum plammNi)e 5. 1"tterift Wd trensfMom-
UM!2 VRA

L 3.0241-67
ACC Nits Ajp6D26553
tion or electrawWwtIc veyes In a wpetowtive plasms. (excitatlon or Mgh-hvq==T
vayesp scattering and trawranation (if', mic wwes by luc&srent fluctua-- . -
scattering and trawrormation by edierent f2metuations,, scattering and trans-
formation by UwpuJLr fluctuationsp &W scattering and trawformetlan bF lcw-fkSqv=w N
fluctuations). 6. scattering wd trawrormstion or wasnui wwas in a 10111;1111~~*r
plasm (by Inedberent and a -h= M f2wtuations). T. TonzisfiffustlM at IMf 9w
vayes by Imagwir rlue4vations In In mognstoactivi p2smle. Ofti* wt 'b" f.. In
fOrIWAIAS.
v
D",
on-,
SM CMS 2D/
Cold

SITFNKO, M., brigadir
On the right track. Avt.transp. 42 no.1:7 Ja 161.. (NIRA 17:2)
1. BrIgada shoferov 1-go Rizhskogo taksomotornogo park&.

's rT E ri j< C ) -(, -j -
SUBJECT USSR / PHYSICS CARD 1 / 2 PA - 1876
AUTHOR LJASENKO,V I.V_PYT~
TITLE The Electric Suri-f-ace Conductivity of Germanium.
PERIODICAL lurn.eksp.i teor.fis,jl,fasc-5,905-907 (19~,6)
Issued: 1 / 1957
Here the exterior electric field was used as a medium for the reversible
modification of the surface charge. A monocrystalline Germanium plate (with
soldered-on contacts for measuring the Hall effect and eonductivity) was
pasted onto thin mica foils (30 to 50et) by means of polysterol varnish.
A metal plate was pasted onto the reversed side of the inica foil. The Hall
effect and conductivity were measured in the presence of an electric field(at
+ V and at - V on the metal plate) and also without such a field. From the re-
sults of these measur ements the effective value of the mobility ue was de-
termined. The results of these computations are shown for some samples in a
table. Measurements were repeated several times and were found to be absolu-
tely reproducible.
Under the effect of the exterior electric field the resistances of the simples
with electronic as well as with own conductivity increased at + V and di-
minished at - V on the metal plate. Also Hall's electrcmotoric force V x and
the mobility ue were measured. At -V on the metal plate they increased and at
+V they diminished. If a surface zone of electric condt.otivity exists, the mo-
bility of the electrons on the surface is lower than in the interior of the
sample

LYASHENKO, V.I. [Liashenko, M.]; SITENKO. TAT. [Sytezko, T.N.]
Conductivity of a Ge surface. Ukr.fiz. zhux. I no.1:64-70
JA-F '58. (MIRA 11:4)
1.Institut fiziki URSR.
(Germanium--Electric properties)
(Hall affect)

SITENKO, T.N. [Sytenko, T.M.]
Effect of an electric field on Hall effect in Go at various
temperatures [wItb summary In English]. Ukr.fiz.zbxir. 3 no.4:473-M
JI-Ag 158. (MIRA 11M)
1. Institut fisiki All USSR.
(Hall effect) (Germanium) (Ilectric fields)

2 A4
S/181/~,1/003/004/010/030
//CIO //&"d) B102/B214
7 1,J6 (// " / Z
AUTHC.,z;: Sytenko, T. N. and Koshell, 0. N.
TITLE: Effect of the surface condition on the Hall effect and
the magnetic resistance of germanium
PERIODICAL: Fizika tverdogo tela, v. 3, no. 4, 1961, '079-1084
TEXT: It has been shown by the authors in earlier papers that the Hall
effect and the magnetic resistance depend essentially on the condition
of the surface of a semiconductor. The mechanism of the scattering of
excess carriers is important for the interpretation of a number of surface-
sensitivity effects. Therefore, the authors carried out further investiga-
tions of these effects for different treatments of the surface and are
reporting on the results in the present paper. The samples were cut
from, a p-type Ge single crystal; they had a resistivity 42 ohm.cm
and L, volume lifetime 300 Psec. After etching with C-'~'-4 (SR-4)
they had a size of 0.4s 1-0~ 0.017 cm (12-1) and 0.4x 1.?A 0.0165 cm (11-I).
The measurements were made at a constant temperature, (+ 20.5 + 0-5)oc,
in the field of 3000 oe, and at a pressure of 10-6 mm Hg 15 se7c after the
Card 1/6

:! '2104111
S/1 8- 16 1/003/004/CI-:D/030
Effect of the surface ... B102/B214
field had been applied. The conductivity of the samples was measured
alon- with the Hall potential difference. The maximum of the Hall con-
stant nearly coincided with the minimum of conductivity. The results
obtained proved to be well reproducible. By a short action of an electric
field only the filling of the surface states was altered. To influence
the energetic structure of the surface, samples 11-I and 12-1 were etched
once more in boilin;, H 0,, but no essential chcn-es occurred. Under the
U 2 1 U
action of the electric field, a-i electric char.-e ic induced in the semi-
conductor, which is captured in part by surface levels. The dependence
of the conductivity of the space-chargo layer or. "he ban! curvature of
the surface for different volume-carrie.~. concentrations, found theoretical-
ly by Schrieffer (:'Ily-';, Izev- '21 '1 and Garrett and Brattain
(Phys. Rev. 22, 376, 1)55), a.-rees '::eil Lith the ex,)erimental results.
The observed increase in the chan;-e of conductivity relative to the
-minimum, occurring under tlie action of the electric field after etching
in 92029 leads to the conclusion t-put the che-,_ical treatment affects the
concentration of surface levels and their Position. This is also i-d! icated
by the fact that the form of the dependence of thc constant on the
Card 2/6

22044
Effect of the surface
S/181/61/003/004/010/030
B102/B-214
electric field is altered after etching in H202- The results relating
to the measurement of the Hall constant R and (4 are compared with
X
theoretical results of Petritz and Zemel, and those obtained for (,6 P/P)JI
with results of G. Ye. Pikus (ZhTF, XXVI, 22, 1956). Results of the
comparison are shown in Figs. 2 and 3- It is seen that a consideration
of the light holes slightly improves the agreement between theory (Pe.tritz,
Zemel) and experiment. The authors carried out the calculations for
light holes of the following parameters: r = 2.25-10- 2 , b - 7-5 (r is
the concentration and b the mobility ratio of light and heavy holes).
The theory of Petritz and Zemel is discussed in detail. The comparison
of the results with the theory of Pikus showed that the effect of surface
recombination on Z-\?/OH2was insignificant under the present experimental
conditions. It was found further that the different chE.racter of the
dependence of 6?/Y on the external electric field for two different
orientations of the sample in the magnetic field at t
continued to exist even in the absence of any band curvature. The authors
Card 3/6

Effect of the surface ...
22o44
S/181/61/003/004/010/030
B102/B214
thank Professor V. I. Lyashenko, Doctor of Physical and Llathematioal
Sciences, for suggesting the topic and guiding the work; and 0. V.
Snitko, Candidate of Physical and Mathematical Sciences, for advice and
a discussion. There are 3 figures and 14 references: 7 Soviet-bloc and
7 non-Soviet-bloc.
ASSOCIATION: Institut fiziki AN USSR Kiyev (Institute of Physics,
AS UkrSSR, Kiyev)
SUBMITTED: July 28, 1960 (initially) and November 3C,1960 (after
revision)
Card 4/6

Um/nOticu,* - Rosatem IW70 Jul 1947
Medicine - Pleurisy
OX-reLy Ismalm tion or Pleurisy Nodul*~ vith PassW
2hrough Fistulas of Contrasting Nateri&l,O V. N.
X. X. Shatkovskly, Imingrad, 4 VP
'Traabebnwe Delow No 7
3h the process of trestsient or necrotic pleurisy mi
ahrmic amovem it In met Inortant to locate'tbe
area affecied, the degree of the Infection, and thO
Almensimn of the affected area. 7or this x-ray. am-
smInations are conducted. Short description or z-m7
samination procedure. UperAwnts vere conducted at
the Clinic of Practical Surgery inani S. P. r*dorw.
- ]Roentgen EVe (Contd) Jul 107
(Chief of Research: Prof V. N. Mwmwv), U111tary
Jbdioal Academy imeni S. M. Kirov.,
1C

SITENKO, V. M.
Mil. Med. Acad. im. S. M. Kirov (Docent, lst Faculty Surgical Clinic, -c1948-; I-Ibr.,
Chair Facultative Surgery, -cl94-9-; Mbr., Chair Physiology-, -c:1.90-).
"Determination of the Vascular Condition in Endarteritis GblitAwans," Vop.
Neyrokhirurgii, 12, No. 3. 1948;

S.7 I PEI. 1"0 )V.1'.
2f~273, 3~M.?'O, V-'-- Obliteriruyushchiy Endarterilt I Obliter-*Lruyushii
osy '-eyrok',! urgH, '94';j i4o. 4, c. 5-11
- .. Y I - ..-r - I
l--rt,-,riosklero2 Eryushno-, ~Ortv- VOPT i
30. letonis' I'lo. 33, 1949

STtENKOJS V. M.
Sitenko, V. M. - "On a particular functional condition of the arterial vessels of
the extremities in obliterating endarteritis," In the symposiim: V. N. Shamov,
Kiev, 1949, P. 137-44
SO: U-4355v 14 August 53, (Letopis 'Zhurnal Inykh Statey, No- 15p 1949)

SITENKO, V. M.
Sitenko, V. M. - "Experimental data on hemoplastic transplantatIons of the egg,"
In the symposium: V. ". Shamov, Kiev, 191.9, p. 2-19-36
SO: U-4355, U~ August 53, (Letopis 1,7hwnal Inyk-h 3tatay, No. :-5, 19,49)

SITWW, T.M.
low data on the mechwden of the effect of sylgathectaW on blood
circulation In andarteritis obliterans. Test. khir. 71 no.1:26-31
1951, . (CIML 20:8)
1. Of the Departmient of Faculty Surgery lo I Imeni S.P. Pedorow
(Head-V.N. Shamy), Military Medical Academy imni S.M. Kirov.

1. SITENKO, V. M.
2. USSR (6oo)
4. Arteries - Diseases
7* Painful syndrome in endarteritis obliterans.
Vop. neirokhir, 16, Noe 5o 1952
9. Monthly List of Russian Accessions, Library of Congress, J""17 -1953. Unclassified.

SITMITO, V.M., do-ktcr melitsinskikh nauk ( Isming rad.ul. Lebo deva, d. 10-g. Kv. 2 )
Diagnostic errors in endarteritis obliterans. Vest.khir. 75 no-3-98-
102 AP 155- ()MRA 8-7)
1. Iz kliniki 1-Y fakulltetskoy khirurgil (nach.-prof. V.N.Shamov)
Tcyermo-medttsinskoy ordena Lenina ak-ademii im. S.M.Kirova.
(JNDARMITIS CBLITIWS. diagnosis,
errors)

SI M KO. Y.M.. doktor meditainakikh nauk
Surgical ligation of iliac veins In decompensated heart failure
[with oumary in Inglish. P-1551 Yest.khir. 77 no-3:23-25 Mr '56.
(MLRA 9:7)
1. Iz 1-y fakulltatskoy khirurgicheakoy kliniki (nach. - prof.
V.N.qb--ov) Voyenno-seditainakoy ordena Lenina akadenii imeni
S.M.1irova.
(CAR IOVASCULAR DISMAS . Burg.
ligation of iliac veins)
(VAINS, ILIAC, surg.
ligation In cardlovase. dis.)

SITrkNKO, V.M., doktor moditaLnoicikh nauk
I - -- ~- -.- 7 , ~
*Acute arterial obstruction". Z.V.Ogloblina. Revieved by V.N.
Sitenko. Vest.khir. 77 no.4-133-134 Ap 156. (KIRA 9:8)
(IMOLISM) (OGLOBLINA. Z.V.)