SCIENTIFIC ABSTRACT STAVINSKIY, V.S. - STAVISSKIY, YU.Y.A.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
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• Document Creation Date: November 2, 2016
• Document Release Date: August 25, 2000
• Sequence Number: 5
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

Calculatl.(jn of the U 238 . . .
Fir. 21. C~ and the excita-
Ir
u,'Lo- func~..Ions of the irdi- -'t
()f U238*.
Lecend. w 6. V 2 ?ev);
1'.ev). Eyp~)ri-
mental data taken frorq L.
Exanbere, . Levin, Ph~,s.
Rev., 109, 2063,(1958)-
Card 3/4
j/089/62/013/004/006/011
3102/B1 08

238 ;D/030/62/01 3/004/006/011
Calculation of the U ...
ii-- 3. I--"a---,iat-4ve ca:)ture
230
for U and partial cross
for X= ;D, 1, 2, and 3. EXperimental
taken from Hughes' Neutron
Atlas.
'lard 4/4
v
cross section 0~
n
sections 61(1)
n y-
data
Cross Section

3 C C,65
3/05-0/62/042/006/030/047
31"'4/B108
J~u it-:vins'-Ay, "'. 6. , Kovalev, V. P.
L.'." Calculation of the fission thresholl and the excitation
enevLc of fr,~- ents in the droplet nuclear model takinE
.,Y C;TI
account of the -.*;ilrner symmetry eneri-j
ZI-Airnal ek'sDerimentallnoy i teoreticheskoy fiziki, v. 42,
no. 6, 1962, 161q - 1617
T 1" Ac-or~"An.& to G. F. %1'eizsdcker (Zs. Phys., 96, 431, 1935) and F. P.
.'.4.Ener (Phvs. Aev., 51, 947, 1937), the totalYcoupling enerFy of a nuclpus
is given by (iv Z)2 ZI
S (a) A'A + A +
E (NIZIcs) otA + OB + aBc((s) -;jjj-
+ eBs (()) (N Z)2
A is the number of nucleons in the nucleus, Z the nuclear charee. The
cons t!:in ts r6 , ire de termined f rom experiments, and are equal for-.
all nuclei. The energy chanE-e with deformation of the nucleus is described
Card 1/2

3/0- -,~ 06/6 2/034 2/Oo6/0 30104 7
.alculation of the fission ... B104/B108
by the coel'-ficients
Z2 Te I Of - Z), I Bs (O.p)- 11, 1
(Bc (Op)
El = DAY- [Bs 0.0 + a -Arl-
(2)
is oblained lor the threshold,energy allowing for the surface term in the
s,y.:i:.etry enerFv. .Tkp is the nuclear deformation correspo-nding to a saddle
ooint. ~:'ince values of B and B are kno-,r;n in publications only for
6 C
sy-,,:etric decay the effect of the last term in (2) is studied here for the
ca3e of symmetric fission only. It is shown that the experimental correla-
t*Lon of the charActeristics of spontaneous fission with neutron excess in
the fission--ble nucleus is obtained if the dependence of the ';iigner symmetry
ene~,r on the nuclear deformation is considered in the mass formula. Ex-
nerimental results and theory are in better aEreement when making this
consideration. There are 2 figures.
3*U31-'A'TTF,D: January 11, 19062
C-rd ?/2

5/056j62/043/001/047/056,
B102/B104
AUTHOA~i: Barkov, L. M., Mukhin, K. If., Oguirtsoy, V. V.,
Romantseva, A. S., Svotlolobov, 1. A., Chuyeva, S. A.,
EM-F.Fev 1,
Shlyapnikovj 11. S.p7L StavInskiy, V. S.,
strunov, L. N.
Tho problem of the D+-meson
PE410DICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 431
no. 1(7), 1962, 335-337
The authors have searched for a D+-meson production or a decay
axong 14,000 paira of photographs. A propane bubble Dhamber with pulsed
ma.-,n~tic field was irradiated with a beam of positively charged particles
'e.0mentum V~1.8 Bov/c) containing up to 9-/. X+ mesons. The processes
looked for were K+ + p-*D+ + 2~t and
+
no
C~--zd 112

5/05 62/043/001/047/056
The problem of tha D*-meBon B102Y3104
The first branch of the decay reaction is the more possible. Neither a
process K* + P--->D' ~2:* nor one of the type K+ + n --~D" + could be
+
found. It iB inferred that the D MeBon production cross section in
29 2
K actions will be smaller than 1.2-10 cm
Institut atomnoy energii (Institute of Atomic Energy)
(R. S. Shlyapnikov); Ob"yedineuriyy institut yadernykh
issladovaniy (Joint Institute of Nuclear Reaearca)
(L. N. Strunov)
3 U BII f'--D .;,Pril 25, 1962
Card 212

KARDASHEV, D.A.; STAVINSKIY,V.O.; ERODER, D.L.; LASHUK, A.I.; SADONRIN, 1,,P.
Analjysis of the excitation functions for levels of the Fb56
nucleus in the case of inelastic neutron scattering in an optical
nuclear model. Atom.energ. 13 no.6s587-5M D 162. (MIRA 15:12)
(Iron-Isotopes) (Neatrone-Scatterin )
(Nuclear optical modelal

L 11946-66 Eh1r(m)/T/EWA(m)_2.
ACC NR, AF6OM36 SOURCE com. - uK/o386/65/oo2/ooq/o4oq/o4.13.L
AUT11OR: V 14 F.
0!eenko, A. S. ; Gus'k0V B. N. ; Likhachev. Matule
Lyubim6v, A. L
47u. A. Sav~~. A. i dktV__-T_5_
ORG: Joint Institute of Nuclear Research (WyedinehW institut yadernykh isaledo-
vaniy) ____ 1, / - qt( ..) 1 .
TITIE: Elastic 18U* scatter + It/
ing of it mesons by protons at high energies
SOURCE: Zhurnal eksperimentallnoy i teoretlebeskoy fiziki. Pialms Y redaktRiyu.
Prilozbenlye, Y. 2, no. 9, 1965, 4og-413
TOPIC TAGS: elastic scattering, pion scattering, proton scattering, scattering cross
section
ABSTRACT: This is a continuation of earlier measurements of the differential cross
sections for elastic Yr+p scattering in a small solid angle about 180* at xt-meson
l.s. momenta 3-15, 4.10, and 4.85 (;ev/c, carried out at the High Energy Laboratory of
the Joint Institute for Nuclear Research, the results of which for 3.15 Gev/c have al~
ready been published (Phys. Lett. v. i7s 68, 1965). In this paper the authors present
the results for 4.10 and 4-85 Gev/c and compare the data obtained at all three ener- I
gies. The measurements at the different energies were made with the same setup, whict
was already described earlier. The ratio of the number of elastic wtmeson b;.ck?Aard-
scattering events registered by the apparatus to the total number of obtained photo-
graphs decreased with increasing energy (1:4.4, lt1l, and 1-.40 at 3-15, 4.10, and
4.85 Gev/cp respectively). ibis vu due not only to the deareas* in the measured

L 11946-66
ACC NRz AP600CY
b
cross section, but to a deterioration of the background conditions as a result of the
smaller spatial separation of the recoil protons from the beam particles. It was
therefore required to apply more rigorous criteria for the selection of the backward
elastic- scattering events than earlier. The effective c.m.s. solid angle of the set-
up, calculated by the Monte Carlo method with account of the Coulomb scattering of
the particles, was 3-87 x 10-3 or for 4.10 Gev/c and 3.04 x 10-3 or for 4.85 Gev/c.
The effective cross sections, corrected for the nuclear interaction of the primary
and back-scattered jy+ mesons and the recoil proton in the hydrogen target and in the
counters, for the muon contamination of the beamp for decay of the scattered pion,
for the efficiency of the scintillation counters and the electronic circuitry, and
for the efficiency of the spark chambers, were (99 1 12), (74 1 ii) $ and (3T 1 12.)
jib/or for 3-15, 4.10, and 4.85 GeV/c, respectively. The previously deduced existence
of a narr(rw,peak of appreciable magnitude in the differential cross section of elas.-~.
p #;jg &t.3.15 04tvic ~&. confirmpa., Authors thank V. Biruievs-'71.,
tic X+ backward scattl, 'e -
Dobrovol'skiy A. op;h~jiVli akurYd., M. Pereva 'dMkc4,- and 'N. Cherayshav-1-
LA9 " , I -
help with the work, Y-, )r compiling the FrWa-M&M performing-the comoutg~
tions, the proton synii'mroo."4e. for stable operation of the accelerator, W the
operating staff of the cryogenic division for supplying the liquid hydrogen. Orig.
-art. has: 1 figure, 1 formila, and 1 table.
SUB CODE: 20/ 9M DATZ: 158ep65/ OTH RXF: 002

SVIRIDOV, F.; STAVIRSKIY inzhener-takhnolog.
Production of semiwool shawls. Prom.koop. no.2:27 7 '57.
WaA lo:5)
I.Direktor trikotazbnQy fabriki no. 20 tresta "Mosgortekstil'prom".
(for Svirldov)
(Knit goods industry)

STAVISXAYA, Ye.
-
Arocessing of the left side of a beef carcass. Mias.ind. SSSR 26
no.l.-58 155. (MMA 8:5)
(meat cutting)

STAVISKAYA,Ye.
-01~
. ; ,
Restoring the quality of lqrd. Mine.ind.SSSR 26 no.4:55 '55.
(KLPA 8:10)
1. Kiyevskiy myamotrest
(I^rd)

S'PAVlSKAYA, Ye.
Norms for spice input and the fla-vor of sausage Products. t-'-ias.
ind. SSSR 34 no-3:22-23 163. (MIRA 16.7)
J- If! -rainskiy n,-,ucilno-issledov~-jtPjlskiy instilut
I

STAVISKAYA, Ye.; POPOV, P.
Information. Mias.ind.SSSR 35 no.1:57-59 164. WRA 17:4)
1. Ukrairiskiy nauchno-issledovatellskiy institut myasnoy
promyshlennosti (for Staviskaya). 2. Komitet po ekonomike I
organizatsii proizvodstva Nauchno-tekhnocheskogo obshchestva
pishchevoy promyshlennosti (for Popov).

STAVISKIY- N., irzh. po ratsionalizatsii i izobretateltstva;
.----KOLODIN,, I., inzh.; REZNIK, F., inzh.
Suggestions of innovators. Grazhd. av. 18 no.6:20-21 Je 161.
(MIRA IJ,: 7)
(Technological innovations)

-l - -t-Isekha, 'fFI'IA,- 0. rabotnik
IAV i I :, 11 t G., pa,~~hsllnik I
p 1. - :. . I ~; .,-Irj~.~ ~:i vn I I
C
---l .1. --- .. - - "Z' je 165.
T "~ r.. ~ r, ,, -,;. 11 - , -,.. Grazhdt, P. 1. 22 nc o6- (' Wam 18%r,j)

LOTOTSKIY, B.V.; MURATOV, Ye.A.
Seasonal variability in the vinilant nature of pathogenic micro-
organisms transferred by argasidae and ixodidae. Izv.otd.est.
nauk All Tadzh.SSR no.8:157-166 154. (MIRA 9:9)
l.Institut zoologii i parazitologii imeni akademika Ye.H.Pavlovskogo
AN Tadzhikskoy SSR I Stalinabadski7 gosudarstvenrq7 meditsinskiy
institut imeni. Abuali-Ibn-Sino.
(MICRO-ORGANISMS, PATHOGENIC) (ARGASIDAB) (TICKS)

MMSUROV, Kh.Kh.; KUTGHAK, S.N.; STAVISKIY9 Ya.D.; 14AKAREVIGH, Ya.A.;
AMINDMANOV, S.A. -
Diagnostic significance of intravital liver biopsy. Zdrav.,Tadzh.
7 no.5:8-13 160. OMA 13:12)
(LIVER) (BIOPSY)

MA113U-ROV, Kh.Kh.; STAVISKIY, Ya.D.; RUDOY, D.G.
N
.e -; method, indications and contra-
edle biopsy of the live,
indications. Trudy Inst. kraev. med. All Tadzh. SSR no.1:24F-
260 162. (14IRA 17; 5)

L 06982-67 EWT (m) IJP(c)
ACC NR: AP6018358 CAI IV) SOURCE CODE: UV0089/66/020/005/0431/0432
7
AUTHOR: Koroleva, V. P.; Staviaskiy, Yu. Ya.
------------
ORG: none
If
TITLE: Measurement of the fast neutron absorption cross section with the aid of a
resonant detector in water
--71
SOURCE: Atomnaya energiya, v. 20, no. 5, 1966, 431-432
TOPIC TAGS: neutron absorption, neutron cross section, neutron flitx, neutron
detector, resonance absorption
ABSTRACT: The authors describe a method for monitoring the intensity of a neutro
n
source; this method is a modification of the "manganese bath" method originally
proposed by E. Amaldi (Phys. Rev. v. 50, 899, 1936). It is shown that it can be
used successfully to monitor exactly small changes in the flux of the fast neu-
trons during the measurement of absorption cross sections. The experimental setup
consists of a water tank (2 x 2 motors) with spherical cavity I motor In diameter,
in the center of which are placed the photonoutron source and the samples. Part
of the water volume is occupied by an aqueous soluticn of a resonant activator
Card 1/2 UDC: 539.172.4:539.17.02

S T A Vi J3' K iU~Y,-UN'~iKIY, A. I.
BOUDAR7LI Al lu.F
70, 1. 1.
NAA~NVV-',
F.T., USACT-N, L.N.
AUTIMI. ",~_STAVISISK va., '~-'MIMBUR,
TITLE I\ - e Experimental Reactor for Fast Neutrons BP - 2. n)
(7,tksperim,--ntalITrjy reaktor na bystrykh neytronakh BP-2- Russia
P_4~10DICAL Atomnaya Energiya, 1957, Vol 2, Nr 6, p; 49'1'1~-5oo (U.S.S.R.)
ABSTFOCT This reactor is intended to be used for physical investigations
with fast neutrons. At fir~.t the active zone of the reactor is dis-
cussed. The heat-separat-,ng elements of the reactor BP-2 consist of
plutonium rods of lo mm diameter and 13o mr length. Besides the plu-
tonium rods there are similarly constructed rods in the active zo-
ne which are made of poor uranium. Altogether there are 1o8 u-
ranium- and plutonium rods which are mounted in a steel tube with
an inner diameter of 130 m!n. The reflector of the reactor consists
of an uranium layer (outer diameter 7oo mm) and a copper layer
(outer diameter looo mm). The reactor is controlled by a control
system and by an emergency system. The operating control organs are
part of a screen which are located near the active zone. The con-
trol system also contains boron-ionization chambers, an electronic
apparatus, and servofeeds. The emergency system enters into operat-
ion if the prescribed or assumed power of the reactor is exceeded.
Circulating mercury is used for the system of heat conduction. This
mercury is then cooled in a heat exchanger with water. The radiat-
ion protection of the reactor consists of the following parts:
Card 1/2 a) a water layer of 300 mm thickness b) a cast iron layer of 44D0 mm

The a-perimental Reactor for Fast Neutrons BP - 2. 89-6-1-24
thickness a) a layer of heavy concrete of l2oo mm thickness. A
special laboratory building was erected for the purpose of hous-
ing the reactor and its auxiliary installations.
Exoerimental Installations: The central experimental channel is
determined for the irradiation of samples with strong fluxes Of
fast neutrons. In the experimental channels in the lateral reflector
of the reactor also samples are irradiated, but also a local os-
cillator may be fitted. Three horizontal channels serve the purpa._a
se of conveying bundles of fast neutrons through the protective
casing of the reactor. The reactor furthermore contains a thermal
colurm of graphite, the dimensions of which are l4oo x 14oo x 2600 mm.
In conclusion the applicability of this reactor is discussed; in
particular physical constants are determined precisely.
( 3 illustrations).
ASSOCIATION Not Given.
PRESERITED BY
SUBMETTED
AVAILABLE Library of Congress.
Card 2/2

LEIJPUESKIJ, A.I. [IeypunBkiy, A.I.1; BIA)CHIVGEV, D.I. [Blokhintsev, D.I.1;
ARISTARGHOV, I.E. [Aristarkhov, 1.11.]- BONDARFIZO, I.I.;
nUCKOVSKI.T, O.D. [Kaz-akovskiy., O.D.J- PINCHASIX, YI.S.;
STAVISAKIJ, Ju Ja. [Stavisskiyo Yu.Ya.1; STUMUR, E.A.;
UKRAJINCEV, F.i* I aln .9 . . y My L.N. (Usachev, L.N.];
MEDONOS, S. (translator]
Soviet experimental- reactor with fast neutrons BR,-2. Jaderna
energie 3 no.8:231-233 Ag 157.

LEYPUNSKIY, A. 1., iaZAC.1T,01TSKIY, 0. D., A.RTLV-LH(W, G. A., 7BELANOVA, T. S., BARISHNIKOV,
A. I., GALKOV, V. I. , STAVISKIY Yu.ya., STLT,',:,BbR, E. A. and SHE,IWO, L. Ye.
"Effective Cross-Section Measurements, of Fast Neutron Radiation Capture."
paper to be presented at 2nd UN Intl.' Conf. on the peaceful usees oil Atomic
Energy, Genera, I - 13 Sept '58.

IWFUNSKIY, A.I.; ABRAMDV, A.I.; ANDRETEV, V.N.; BIMS)INIKOV, A.I.:
BORDARENIM. I.I.; GALKOV. V.I.; GOLUBKV, V.I.; GUL'KO, A.D.;
GUSF,TTUV, A.G.: KAZACHKOVSKIY, O.D.; KOZWVA, H.V.; KRASHOTAROV.
N.V.; KUZIMIROV. B.D.; WROZOV, V.N.; NIKOIAYW, M.N.; SHIRERKIN.
ULIWNTSIW. F.I.; USACHCV, L.K.; YWISOV.
N.I.; SHMMAN, L.Te.
Studies in the physics of fast-neutron reactors. Atom. energ. 5
no.3:277-293 S '58. (MIRK 11:10)
(Nuclear reactors)

21(7) SOV/69-5-5-10/27
AUTHORS: Konoriov, V. N., _Staviss~~-Y-ii--Yz-,, .-.Tolstikov, V. A.
TITLE: Measurement of the Cross Section of t he Radiation Capture
of Neutrons With an Energy of 25 keV (Izmereniye secheniy
radiatsionnogo zakhvata neytronov s e nergiyey 25 kev)
PERIODICAL: Atomnaya energiya, 1958, Val 5, Nr 5, PP 564-564 (USSR)
ABSTRACT: By means of the activation method the cross section for the
photoneutrons of a Sb+Be-source was , 25 keV).
measured (E
A spheriial source of 3 cm diameter w X1
as used, which radiates
about 10 n/sec. The beryllium layer had a thickness of
1 cm. J127 was used as standard of re ference. Activity was
measured by means of the counting tub e MCT-17. The follow-
ing cross sections were measured:
Isotope a Isotope
mb mb
Na 23 1,72 + 0,27 Br79 710 + 33
Card 1/3 A! 27 1,90 + 0,27 Sr s6 400

SOV/89-5-5-10/27
Measurement of the Cross Section of the Radiation Capture of Neutrons With
an Energy of 25 keV
IsotoDe Isotope
mb mb
S--30
L
2;09 +
0751 87
Rb
29,0 + 1A
C137 3:71 + 0,64 Nb93 120 + 12
K41 26 Mo loo 112 + 3
V51 32,5 + 2,1 A-107 1330 + 91
Mr, 5 5 65 + 3 In 115 590 + 20
Ili 64 37 - Ba138 8,6 + 0,4
CU 65 38,6 + 0,3 W186 285 � 58
r7 n68 24,0 + 2,8 Au197 960 + 6
Ga 69 151,0 � 1,2 T1 205 51 + 2
There is fairly goo d agreeme nt between the measuring results
ob;;ained and the da ta given by reference 4. There are 1 table
Card 2/3 and 4 references, 0 of which is Soviet.

.21(4) PHASE I BOOK EXPLOITATION SOV/2583
int*rnationti Conference on the Peaceful Uses of Atomic Zngergy.
2nd, Geneva, 1958.
Daklady sovetakikh uchenykh, yadernyyv reaktory i yadernaya aner-
gatiks. (Rpports of Soviet Scientists; Nuclear Reactors and
Nucle F r) Koscow, Atoftizdat ' 1959. 707 P- (Series. Ital
.1. 2) Errata &l1p inserted. 8,000 copies printed.
General Sdo.: N.A. Doll*zhal, Corresponding Member, USSR Academy of t-A
Salendw~, A.K. Kradinp Doctor of Physical and Mathematical 3clancen,
I
.
A.I. Ldypundkly, Member, Ukrainian SSR Academy or Sciences, I.
Soylkolf Corresponding Member, USSR Academy of Sclanceno and V.3.
Id
A
?
.
.z
.
Parsovo Doctor of Physical and Mathematical Sciences;
Alymblywri %ch. gd.z Ye. 1. Kazell.
NUM301 This book to intended for scientists and engineers engaged
'
in reactor designing, as well as for professor$ and students of
kl&h8r technical schools where reactor design is taught.

-As"* second volans of a slyvolums mlleat4va on. th peamfu
I
-
COVZKAUSt This
I
-
en-
iumes contain the repo
rt
use ar
litzoda energy. The six vo
ap
are
dented by Soviet scientists at the Second International Conf
nee

'
On P0844ftl Uses of Atomic Energy, hold from September I to 13 I,
Volume 2 consists or three parts. The first
1958.1n Geneva.
devoted to Atomic power plants under construction in the Soviet
Union; the second to experimental and research reactors, the ox-
Perlments carried out on them, and the work to improve them; and
the third, which to Predominantly theoretical, to problems or
nual ar reactor physics and construction engineering. Yu. 1.
Is= is the science editor OC this volume. See SOV/2061
for titles of all volumes of the get. References appear at the
"'Of''the articles.

PART 11- EXPERIMENTAL AND RESEARCH REACTORS
rdtarlZU"
V
a~4
'
'
I.I. Bondhren
~3
'
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2
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n,_
-~,
i.
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v, -3. llliWii "
~.O
~
-
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a
:V
t. L.N. rlv~,
-`
Z
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r
r Par m&ntl-PjU5t
Hj'j'Eg6FrM
_29i msntal~

'15
2
Klkoln I.g V A..,,L)miiOvvk~Z,
"' i 'Niki.t*

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. r
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e
or
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No
2
5O2
p
232
dOnchArOV, V.V. and at &I. Some New and Rebuilt Thermal Research
IWARTMT-M-ftPort No
2185)
.
2 3
lkrokhovtch -B.V., V-1 -.,3 A"%L, P-X4..qkPzXQ1X1
Dismantlink an Experimental Oraphtte-uranium
rAQt0Pd Producing Reactor At-ter Four Years of operation (Report
00. 2297) 319
%._A_K, , V.M. aryazev, V.D. Uimentov,
XAA0P'yaV
nkydt
_&2n!d- P
~--An"Tnt'o
jr:Ejqf
siidL,te
k
Ts
kam"
llh
.
r
a
a
le o..
4
y
,
~,
for Obtaining H10i Intdiinity Neutron Fluxes (Report No. 2142) 334
- PART III. PHYSICS AND KNOINMING OF REACTOR DESIGN
Ls"unekly, A.1 A.r.,_ftrNULyjy.M. Andreyev, A.I. Bar
V fr UajkoV V .Y81:Ztkov,
I Golub'ev Ou I ko, A
,
lzo
zovi Sairealtin,
UlCr Iritiev, L.N. Unache Patinov,
V
,
-
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-Ke&itor5*
."t
t;
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09P09 "NO.' 2038)
377
Romogsn*oud Natural Uranium Reactor
and B.L.j0trp,
Y-T.S..

_
ort go. 296) - - 398
i
W
ftV"rFjA-N- Tot-P-AAtolforov, V.P. xatkov,.L.v. Xamovarov,
n&,-Tu.--V._ 1kol'jkiy
' -A.C"Roilkov
V S 0 hkln
,
.
ev-.- AW1 W"iUp-i. atwr '
-water
an
2145)d Kxperlawnts With the Uranium Water Lattice
N
o.
kov T.A. Self-regulation In a WAtOr-water Power Reactor
ro
n
-
-
m
"
A
.
7
w
O.1w
534
199

21(7) SOV/89--7-3-12/29
AUTHORS: Stavisskiy~ Yul )La.~ Tolatikov, V. A,
TITLE: The Measurement of the Cross Sections of the Radiative Capture
of Fast Neutrons by Isotopes of Gallium
PERIODICAL: Atomnaya energiya, 1959, Vol 7. Nr 3, p 259 (USSR)
ABSTRACT: By comparison with the capt 15 cross Irtion of J 127 the
capture cross sections of Ga and Ga were measured, The
samples of the respective gallium isotope and the iodine
sample used for comparison were, at the same time, irradiated
by a fast neutron flux. The occurring P-activities were
measured by means of an end-window-counter. After the decrease
of P-activity, both samples were irradiated in a thermal
neutron flux and the occurring P-activities were newly measured~
By comparison of the activities occurring in both cases, it
was possible to calculate ax(n,y). The protons accelerated
in a Van de GraAf generator furn ished the fast neutrons with
the aid of the reaction T(pn)He . Within the energy range
of from 200 to 1400 kev, the neutron energy could be measured
with an accuracy of + 30 kev, and within the range of
-
an accuracy of + 50 kevo Irradiation
1400 to 200 kev with7
with thermal neutrons took place in fhe thermal column of
Card 1/2 the experimental fast reactor. In order to eliminate the

SOV/89-7-3-12/29
The IMeasurement of the Cross Sections of the Radiative Capture of Past
Neutrons by Isotopes of Gallium
influence of resonance- and fast neutrons-, the llcadmium"~,
method was employed. The results obtained are thown graphi-,
cally. In the case of Ga69 a smooth dependence of the capture
cross section on neutron energy is found. whereas in the
case of Ga71 a sharper decrease is observ'ed in the neighbor-
hood of 5c:O kev, This is probably due to the inelastic scat-
tering of neutrons on the levels 510 and 610 kev of Ga.71.
There are 1 figure and 3 references, 1 of which is Soviet.
SUBMITTED: March 26, 1959
Card 2/2

TOLSTIKOV, V.A.; STAVISSKIY, Yu.Ya-
[Cross sections of radiative capture of fast neutrons
by the MolOO isotope] Secheniia radiatsionnogo zakhvata by-
strykh neitronov izotopom M0100. Moskvap Glav. upr. po,is-
pollzovaniiu atomnoi energii, 1960. 5 P. (MIRA 17:2)

STAVISSKIY, Yu.Ya.; SHAPAR', A.V.
[Capture cross sections of fast neutrons for tungsten and
rr.,olybdenum] Secheniia. radiatsionnogo zakhvata bystrykh
neitronov dlia vollframa i molibdena. Moskva, Glav. upr.
po ispoltzovaniiu atomnoi energii, 1960. 6 p.
(MIRA 17:1)

s/osq/60/009/005/007/020
BO^e5/BO70
AUTHORS: Tolstikov, V. A.
TITLE: Radiative Capture Cross Sections of the Isotopes P
Nb93 ) W186 and T1 205 for Fast Neutrons --79
/1 ---7? VK1
PERIODICAL: Atomnaya energiya2 1960, Vol. 9, No- 5, PP. 401 -- 403
TEXT: The object of the work was to measure the radiative capture
cross sections of the isotopes mentioned in the title for neutrons of
energies of 0-03 - 2.1 Mev. The source of neutrons was the reaction
T(p,n)He3 carried out in a Van de Graaff accelerator. The sample activa-
tion by neutrons of energies En< 300 kev was measured at an angle of
950 with the direction of the proton beam in the accelerator; for neu-
trons of energies En> 300 kev it was measured at an angle of 00. The
error in neutron energy is due to the thickness of the tritium target,
the geometrical dimensions of the sampled and the fluctuations in the
accelerating voltage of the accelerator. For neutron energies of up to
Card -1/6

85563
Radiative Capture Cross Sections of the B/089/60/009/005/007/020
Isotopes V51, Nb93, W 186 , and Tl 205 for B025/BO70
Fast Neutrons
200 kev the error amounted to * 1? - 20 kev; for higher energies it was
! 30 - 40 kev. Activation by +,EeTmal neutrons was -:%arried out in the
thermal column of a fast reactor. 127 and u235 were used as standards
for the cross section measurements by the method of reJative activation.
The zesults of measurement are represented in Figs. 1-4, their accuracy
being 2 - 5%. For neutrons of energies higher than 150 kev the results
for V51 and W 166 agree well with the measurements of Barshall; for
T1205 93
agreement is not so good. The capture cross section for Nb Is
essentially equal to the production cross secbion of the isomer Nb 94*
A Member of the Academy of Sciences of the UkrSSRj and
O~ D. Kazachkovskiyj Doo:--tor of Physical and Mathematical Ssienees~ are
thanked for valuable discussions. There are 4 figures and 11 references:
4 Soviet and 7 US.
SUBMITTED: April 27, 1960
Card 2/6

G'r:h
4
3
2
6
21
0
j 4 J� 7 8 9A
f 2 .1 2 3 4 MS,7~0
Card 3/6
S/08Y60/009/005/007/020
B
B025 070
Legend to Fig.1
Radiative caDture cross section
51
of V for 'Last neutrons as a
function of their energy.
2 3

85563
4
,V 2
~921
4100
6-
2
__l I I 1~1 I _' J
0,01 2 .3 4 567SSOt 2 3 4 5 6 78.9 f,,7
Fig-3
S/089/60/009/005/007/020
B025/BO70
Legend to Fig;3:
Radiative capture cross sec-
66
tion of W 11 for fast
neutrons as a function of
their energy.
2 4 55789
Cara 5

5
f
3
2
10
4
3--
r1w
of 2 3 4 4 55
~67990,f 2 3
Fig-4
C
ard 6/6
85563
S/o8g/60/009/005/007/020
B025/BO70
Legend to Fig.4:
Radiative caDture cross see-
205
tion of Tl for fast
neutrons as a function of
their energy.
2 3 4 56719
Em
__J
-J

84732
Surface Ionization of Cesium During Its 3/057/60/030/010/01.2/019
Diffusion. Through Porous Tungsten B013/BO63
for four values of cesium-vapor consumption is illustrated in Figs-5
and 6. The dependence of the saturation temperature on the current den-
sity is shown in Fig-7. All these Figures also contain comparative data
from Refs. 4 and 5. The authors' studies have shown that during the
diffusion of cesium vapor-through porous tungsten., surface ionization
is practically perfect at the proper temperature. The temperatures of
saturation are higher than in the case of ionization on smooth emitters;
At a current density of 10 ma/CM2 ` temperature changes by--80OC? but at
a current density of 0-25 ma/ _m2, it changes only1tv -500C. The authors
thank I. I. Bondarenkoj Doctor of Physical and Mathematical Scienceaq
Professor N. I. Ionov, and ~. Ya. Zandber 1, Candidate of Physical and
Mathematical Sciences, for discussions. There are 7 figures and 5 ref.-
erences: I Soviet.
SUBMITTED; April 279 1960
Card 2/2

'V, 7- 1-, HEW L.
FAINT
,~E IMT)
A.
'TY, T. TY 0.
UYF ~!,)n ZlDv
V.
',7F
T.
S7!T
G.
p11- charactiStics nf thc BR-5 reactor
r ~ D t 5 b:n I t ~ e d. f o r t- ~ I A---'A Seminar in th
r -.ctors, Vi~nna, 3-11 AUSust 1-,61
(rcuort prrsented ly G. I.
physics Of' Fast and Intermediate
"Cad. Sci. "SST' i-,'OscOw
;1 - ..,

r n T
AZ C 'I'I, A. i., 'AL.?'Y;.-
T-
~AEA !~ev;ir,-jr on t-,:- Pnysics of Fast and
Tnt--:,:e,~4~;+c `eactr~~- P, .-I-n 3-11 Am- llXl.
Acad ,Ici, ";OzFr-OW

33000
S/641/6-, /000/000/027/0 3--
B102/31,38
AUTHORS: Stavisskiy, Yu. Ya,, Shapar'? A. V
TITLE: Fast neutron radiative capt'ire cross section for rungs-len
and molybdenum
SOURCE: Krupchitskiy, P. A., ed. Neytronnaya fizika; sbornik statey.
Moscow, 1961, 310-311
TEXT: The fast neutron radiative capture cross sections were measured in
the range 0,05 to 1 Mev for natural isotope mixtures of ',Y and Mo, by
recording the prompt capture f-quanta. T(pn)He3 reactions were used as
the neutron source, with the protons accelerated by a Van-de-Graaf.
Between 0,.05 and O~2 Mev the neutron energy spread was + 15 kev, and
+ 20 kev between D.,2 and 1 Mev., A CaP 2 scintillation counter was used
for gamma detection. The energy dependence of the radiati-vre capture vl~
cross sections was determined from a comparison with similar data for
U235. The measurements were carried out with "background" specimens
(Bi + graDhite). MeasuTing accuracy was 6 Yc in the lower arid 3 ~-4 in the
Card 1/9

S/641/6I/000/000/027//033
FaElt neutron raaia~_ive capture. B102/B138
upper energy range, For E = 0. 2 Alev t lie J27 radiative cap-cure cross
n
sections were taken as reference values, For Mo onq was 59 t 10 mb, for
(5 n,e = 122 + 21 mb- Professor A, 1. Leypunskly and 0 D Kazzachkr_vski -
W,
Doctor of Physical and Mathematical SciencE~s; were thanked for interest,
V., A. Romanov, A, S, Kulakov and L, A Zhdamirov for assistance. There are
2 figures and 6 references: 3 Soviet and 3 non-Soviet. The two refererice~i
nglish-.language publications read as follows,, ;i D.
E
A, T C Ferguson, Proc Phys- Soc, 10, 639, 1957; S 17 Bame,
L.. Cub',_tt; Phys. Re-,, '-.5, 256..
0, T 9
Card 2/2

33001
5/64 611/000/000/028/0",
1/3 B 10 2 Y131 38
AUTHORS: Tolstikov, V. A., Stavisskiy, Yu, Ya.
TITLE: Fast neutron radiative capture cross sections of the Mo
isotope
SOURCE: Krupchitskiy, P. A., ed. Neytronnaya fizika; abornik statey.
Moscowq 1961, 312-313
TEXT; The fast neutron radiative capture cross sections were measured
100
with the activation method in the range 30 to 2100 kev for Mo The
neutrons were obtained from T(P,n)He3 reactions, the protons being
accelerated by a Van-de-Graff~ The neutron energy spread was + 50 kev
fox- the 400-2100 kev range (target at Q= 00 to the proton beamTand
15 - + 30 kev for 30-400 kev (target at 0=1000 to the proton beam)- The
irradiation of the specimens with thermal neutrons was carried out in the
thermal column of a fast research reactor, The radiative capture cross
sections of J127 were used as reference values; for thermal neutrons
U was taken to be 5.6 _+ 0.3 b for j127 and 0,20 O~05 b for Moloo,
n,
Card 1/2

1

8 9 358
S/08 6!/O1M/O02/OO8/Wq
4-3 BI 02YB209
AUTHORS: Stavisskiy,,__Xu,.y4,., Tolstikov. V~ A., Kononov, V. N~
TITLE: Measurement of the radiative capture cross section of fast
neutrons by 1127
PERIODICAL: Atomnaya energiya, v. 10, no. 2, 1961, 1,58-160
TEXT: In activation measurements 1 127 is suited as a standard; it has an. apt
half-life, sufficiently high radiative capture cross section., and a known
thermal neutron capture cross section. Data on fast-neutron capture are not
yet available and/or the existing data are erroneous or contradictory?parLin.-
ularly in the range of 0,01 - 2.5 Mev, The authors measured (1958 - 1959)
the energy dependence of the radiative capture cross sections for 0.02 - 2,5
Mev neutrons by means of the activation method. A U235 fission chamber and
the 1127 sample were simultaneously irradiated with a fast-neutror, beam and
the arising P-activity was measured with an end-window cointeri The reac-
tion T(p,n)He3 served as a source of fast neutrons. The arrangement of
tritium target (,), 1127 sample (2),and fission chamber (1) was as follows:
Card 1/4

89358
Measurement of the
pro ton bje jam;~-- -
Irradiation by neutrons with
energies >300 kev
s/o69/6i/m/002/006/018
B102/B209
proton beam
3
Irradiation by neutrons with
energies (300 kev
The measurements below 0 and 100awith respect to the proton beam direoti-c-a
lead to an "overlapping" of neutron energies; the agreement of the Or---)ss sec-,
tions in this region proved the measurements to be reliabl e~ The effen-t of
the neutrons scattered from the walls was less than 0.3% and was determined
from the deviation from the I/R2 lawn Standard measurements with thermal
neutrons were carried out at the thermal columnofd fast reactor, Activation
cross section of 1127 by thermal neutrons was assumed to be 5.6t0,3 b (at,,-
cording to Ref. 8), u235 fission cross section to be 582-;,-4 b (a7co.rding to
Card 2/4

89358
slos,01611010100210081018
of 'he B102/B209
Rcf- 9). The error in the obtained value of the radiative caDture cross
oecti the U235 fi i
bion 0-1~* 1127 is, in essential, due to ssion crQss section er-
(10, - 25~')- Fig. 2 shows a.comparison between the results obtained by
,;hc DrCV,,nt .,icasurements (o) and those of other autilors
Th,:. a curve drops monotonically vilith increasing En and may, within accuracy.
of measurement,'be approx*imated throu-h a E-0-7 curve. In conclusion, the
~!.uthors thank A. I. Leypunskiy, 0. D. Kazachkovskiy,.and V. S. Stavinskiy -for
tl,eir interest and discussions. There are 2 figures and 14 references:
5 Soviet-bloc and 9 non-Soviet-bloc.
SU-,3~.'TTTED: July 14, 1960
X
WOO
8
7
6 ------
5
Card 3/4 F
is

8'~'3 5
casurement of the
Card 4/4
S/089J61 /010/002/008/018
B102/3209

~lp

F X

I I T

Of 2 3 4 5 6 7JRPf 2 1 5 578 9f.0 2
;z,-

20181
S/089/61/010/003/011/021
2 B102/B205
. - 4.12.2 415~
AUTHORS: Stavisskiy, Yu. Ya., Shaparl, A. V.
TITLE: Fast-neutron capture cross section for niobium, nickel, and
iron
PERIODICAL: Atomnaya energiya, v. 10, no. 3, 1961, 264-265
TEXT: The energy dependence of the radiative capture cross sectiom for fast
neutrons in a natural isotopic mixture of niobium, nickel, and iron has been
measured by recording the prompt gamma radiation. The reaction T(p, n)
served as neutron source. The'urotons had been accelerated in a van de
Graaff. The average spread of neutron energy was +20 kev. A scintillation
counter with a CaF 2 crystal was used as detector. The measurements were
performed in annular geometry. Measuring technique and evaluation are
describf:O in Ref. 1 (Moscow report). The energy dependence of the radiative
neutron canture cross section was obtained by a comparison with the course
of the U235 cross section. The experimental error of a single point does
not exceed I(Yj'. for Nb and 15P/~ for Ni and Fe. The radiative capture cross
section of 400-kev neutrons, which is 65 mb for Nb, B.3 mb for Ni, afid 5 mb
Card 1/3

20181
Fast-neutron capture ...
S/08 61/010/003/011/021
B102YB205
for Fe, has been used to determine the absolute cross section. The imults
of the authors' calculations are shown in Figs. 1-3 (full circles)
[Abstracter's note: As the three figures are very similar, only Fig. 3 is
presented] for Nb, Ni, and Fe, and compared with the results of Refs. 3-6.
If the cross section for niobium is averaged over many overlapping levels,
then the mean distances of the levels for nickel and iron are comparable
to the energy resolution of the method. The diagrams indicate that in the
range of 150-1000 kev, the radiative capture cross section depends only
slightly on energy. This is primarily due to the capture of neutrons having
a non-vanishing orbital momentum; another cause is the possible increase in
the radiation width with an increase in energy. A. I. Leypunskiy and
0. D. Kazachkovskiy are thanked for interest in the work. There are 3 fig-
ures and 7 references: 6 Soviet-bloc and 1 non-Soviet-bloc.
[Abstracter's note: Essentially complete translation
SUBMITTED: August 23, 1960
Card 2/3

S/ocig/61/010/003/011/021
Fast-neutron capture ... B102/B205
foo I I I ~ I 1 1-11 1 1 =3:1~ .
11
.Fig - 3 4 to
Ne
2
29 Ivu
E, X,?e
Card 3/3
16,00
FV. 3

22673
s/oag/61/010/005/001/015
B100214
6-2.2 0
AUTHORS: Blokhin, G. Ye., Blokhintsev, D. I., Blyumkina, Yu. A-p
Bondarenko, 1. 1. Deryagin, B. N., Zaymovakiy, A. S.,
ov'yev, V. P., Kazachkovskiy, 0. D., Kim Khen Ban,
Krasnoyarov, N. V., LeyDunBkiy, A. I., Malykh, V. A.
Nazarov, P. It., Nikolayev, S. K., Stavisskiy, 4~ a.,
Ukraintsev, F, I., Frank, I. M., S ap ro,
Yazvitakiy, Yu. S.
TITLE: A pulsed fast reactor
PERIODICAL: Atomnaya energiya, v. 10, no. 5, 1961, 437-446
TEXT: The present paper gives a description of the pulsed fast reactor of
the Ob I' yedinennyy institut yadernykh issledovaniy (Joint Institute of
Nuclear Research) which became critical in June, 1960. This reactor,
call ed H6P (IBR) reactor, serves as pulsed fast neutron source (mean
power Z I kw) for physical investigations, particularly for time-of-flight
experiments. its most distinguishing feature is the very amall.contribu-
tion (- 1o-4) of the delaycd neutrons in its normal operation; it is about
Card 1/'~

22P73
A pulsed fast reactor
S/089/61/010/005/001/015
B102/B214
one hundredth of that of the usual steady uranium reactor. The pulses
appear because whenever the reactor becomes overcritical a burst of prompt
neutrons results. The half width of these pulses is 56 psec. The
frequency with which the pulses are repeated can be varied between 0 and
80 pulnev/seo. Fig. 2 shows the construction of this reactor. The
periodic change in the reactivity is brought about by the displacement of
the two U235 blocks placed in t-no disks that can be rotated. The main
block is pressed in the form of a disk, 1100 mm in diame;er, and can be
rotated with a peripheral velocity of 276 m/sea (at 6000 rpm) during which
it passes through the core center. The reactivity change obtainable from
the motion of the main block is 7.4 %, tfiat obtainable from the motion of
the auxiliary block is 0.4 ~-- The stationary part of the core consists of
plutonium lumps in steel jackets. The reactor is started by a rough
regulator, in this case a movable part of the reflector. It gives a
reactivity change at the rate of 13-io-5 -1.3-10-5 sec-1. The manually
operated rod is also a part of the reflector. Two plutonium rods in
electromagnetic suspension serve as scram. They can be separated from the
core with an acceleration of 20 g. Their separation causes a reactivity
Card

22P73
s/oBg/61/olO/005/001/015
A pulsed fast reactor B102/B214
decrease of 2-1.1 1,b; the rough regulator allows a reactivity change of
2.4 %, the manual regulator 0.1 %, and the automatic regulator 0.036 %.
The reactor possesses also a re,:ctlvity booster for the production of one
intensive pulse. The control and shield system is an automatically
functioning electronic arrangement with BF 3 counters and ionization
chambers. The whole reactor is placed in a room of size 10-10-7 m whose
concrete walls allow complete protection from radiation. The most
imp,irtant experimental arrangement consists of a 1000 m long neutron
cox,ductor,'a metal tube, 400 mm in diameter in the first part and 800 mm
in the second part in which a pressure of 0.1 mm Eg is maintained. This
conductor connects a chain of socalled "intermediate pavilions" (at
distances of 70t 250, 500, 750, and 1000 m from the reactor) in which
experiments can be carried out. There Is also an additional neutron
conductor of 100 m length. The reactor chamber is joined to an experi-
mental chamber in which four neutron beams of up to 800 mm diameter are
available. There us such an experimental chamber also above the reactor
chamber. Various experiments were carried out with the reactor and they
are described in the present paper. These are experiments with stand
Card 3/W

22P,73
5,/G~V-61/010/005/0011015
A pulsed fast reactor 3'
.02/B214
assemblies and slowly moving main block for the determination of the most
imnort-nt parameters of the reactor; experiments with a core assembly
(U' oved), experiments with rotating (5000 rpm) main block and a Ra-a-Be
sonumce in the core for the investigation of the effect of the multiplica-
tion factor, etc. The most important results are represented graphically.
For example# Fig. 8 shows the dependence of the half width 9 of a pulse on
the reactivity; the dashed line holds for the istationary case, the
1/3,-2~u3as.,,here v is the velocity
dot-dash line for the case of 0 - K(-r/c,)
of motion of the (rotating) main block; in the quisistationary case
21Em/av where e M is the reactivity at the maximal multiplication
2
factor; & ax , There x is the displacement of the main block. The
reactor has been actually used for the measurement of the total, scattering,
capture, and fission cross sections by the time-of-flight method. Further
experiments 'will be carried out with a view to obtaining increase of power
and decrease of the pulse duration. There are 15 figures and 3 references:
2 Soviet-bloc and I non-Soviet-bloo. The reference to the English-language
publication reads as follois: J. Orndorr, Nucl, Sol. and Engng,2,1"4,450(1957)-
Card 4^~

STAVISSKIY).,Yu.Ya.; TOLSTIKOV, V.A.
Radiativ capty5g croI3~section of 0,03--2 Hav neutrons for the isotopes
Mn55,, Gu95., Ba , Th . Atom.energ. 10 no.5:508-511 IV 161.
(MRA 14:5)
(Neutrona-Capture)

27178
S/057/61/031/009/018/019
6 .~2 B104/B102
AUTHORS: Lebedev, S. Ya.* Stavisskiy, Yu. Ya., and Shutlko, Yu. V.
TITLE: Surface ionization of cesium during diffusion of its vapors
through porous molybdenum
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 9, 1961, 1148-1149
TEXT: The authors studied the temperature dependence of the surface
ionization of cesium during diffusion of its vapors through porous
molybdenum plates (thickness 1 mm, porosity 30%, dimension of pores -1,A),
The temperature of the ionized surface was controlled with a thermocouple.
The temperature dependence of the ion current density was studied for
2
current densities of 0.015 - 16 ma/cm " Figs. I and 2 show the results.
Results reveal that practically full ionization takes place during diffusion
of cesium vapor through porous molybdenum of porous tungsten. Fall
ionization is achieved in molybdenum at much lower-temperatures than in
tungsten. With an ion current density of 15 ma/CM 2 , this temperature
Card 1/3

27178
S/057161/031/009/018/019
Surface ionization of cesium... B104/B102
difference is about 200C. It is explained by a difference in theevaporation
heats of cesium from tungsten and cesium surfaces and different mean
lifetimeB'of cesium atoms on the ionized surface. The authors thank A. 1.
Leypunskiy, Academician of the AS UkrSSR, I. I. Bondarenkd, and N. I. Ionov,
for discueffiorfs. Further, they thank Yu. A. Eyduk who supplied the poro
materials. There are 2 figures and 2 referencest 1 Soviet and 1 non-Sov
The reference to the English-language publication reads as follows: W. B.
Nottingham, Cesium plasma diode as a heat-to-electrical power transducer.
Uppsala, August, 1959-
SUBMITTED: March 20, 1961
Fig.l. Dependence of the ion current on the temperature of the porous
molybdenum surface.
Fi go 2 Dependence of the saturation temperature on the current density.
Legend: (1) Calculated by a formula for smooth tungsten suggested by
Nottingham, (2) values measured by the authors for porous molybdenum, (3a)
values measured by the authors for porous tungsten, (3b) values measured by
Yu. Ya. Stavisskiv and S. Ya. Lebedev (ZhTF, XXX, no. 10, 1960).
Card 2/3

>_j'jo (11,63, ISJ 2, br"Nij 2TI??3
2-0 Do S/057/61/031/010/006/015
-Y30 B100125
kUTHORSt Lebedev, S. Ya., Stavjsskiy_,_Y_u_Ya., Bondarenko, I. I.,
Mayev, S. A., Stakhanov, I. P., and Stumbur, E. A.
TITLEt, Plasma oscillations in ion-beam neutralization
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 10, 1961, 1202-1208
TEXTt The consequences of the condition that the total ion current in a
plasma vanishes have been studied. Electrons and ions are assumed to be
emitted orthogonally from a conductor surface at the velocities v 10 and
V20' Equations of motion and continuity for electrons and ions are
studied. For the potential T in the interviil 0,