SCIENTIFIC ABSTRACT GOLDANSKIY, V. - GOLDANSKIY, V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000515610017-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 26, 2002
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SOY/'20--127-5-29/58
Tunnel Transitions Between Systems Which Are Described by Morse--Potential
Curves
(Physics Institute imeni P. N. Lebodev of the kciLdemy of
Sciences, USSR)
PRESENTED: April 11, 11059 by V. N. Kondrat'yev, Academicimi
SUBMITTED: April 1, 1959
Card 3/3

GOLIJ,UISKI-Y, V. 1.
"On Two--~roton Rg(iioactivityll
report submitted for the 2nd USS)H Confert,i-cc -,-.n Nticlt-ar Rcac,"I.cns 1,t Low anj
lnt-ermlt-it~~ Encrgieg, Moscow, 21-2P Ju3y 19t-,.

ILI'

5/1:.'0/60/000/03/004/055
EO'2/E514
AUTHORS: Golldanskiy, V._L. , Karpukt-c, Pa%,L,)vskaya,V.V..
TITLE: Determination of the Energy Dependence of the Efficiency
of Recording of High-Energy Gamma Rav '?
PERIODICAL: Pribory i teklinika eksperimenta, 1960, 140 3, PP 23-26
AbSTRACT: A new method is described for Oetermi,ning the energy
dependence of the efficiency of recording of high-ener.~y
gamma rays (35-50 MeV) using a coincidence telescope,
The method is based on measurements of Compton scattered
gamma rays. The Compton cross-section is well-known and
is given by the Klein-Nishina formula. At small angles
the scattered gamma rays have a relatively large energy,
Thus, for example, at a scattering angle of 9 = 3' and
incident gamma ray energy of 250 MeV, the energy of the
scattered gamma ray is about 150 MeV. Thus by placing
a gamma ray telescope at art an,[,'Ie of 30 to the beam axi-s,
and by varying the maximum onergy of the brems-stralilting
from a synchrotron, one can examine a. wide energy range,
Card 1/2 The experiment was carried out in the gamma-beam of the
W

S/120/60/000/03/004/055
E032/E514
Determination of the Energy Dependence of' the EFficieiicy of
Recording of High-Energy Gamma Rays
261-
) MeV synchrotron at the Physics Institute, Ac.,Sc-,
USSR~ The experimental arrangement is shown in Fig, -1.
The gamma ray beam from the synchrotron target was
collimated by a lead collimator, its maximum energy
being set to 250, 200, 1r.)0, 11,5, 80 and 60 MeV. T h t!
gamma rays scattered at angles less than 30 were
detected by the four-counter tel-esCOX)e shown in Fig, L'
The efficiency of recording of gamma rays between
35 MeV and 150 MeV was measured as a function of enert~v,
and the result obtained is shown in Fig 5~
Acknowledgment is made to A.V.Kutsenko, A.Samiullin,
S,P. Balatlyev and Ye. M. Petrov for help during the
measurements.
There are .5 figures an(] (I Engliih references,
ASSOCIATION: Fizicheskiy institut AN SSSR (Physics. Institute
SUBMITTED: Ac,Sc., USSR)
MaY 25, 1959
Card 2/2

,6()/(,C)c --,
3/026/
j)043/DCO'~--
,~jje i)lscovery of the Antiproton
There ~,T~e
mentionea.
Soviet -~,2fel~ences,
;~-,rd 2/2

IJ
AUTHOR, I da us
TITLE - V,,e L imi. ts o If 5 tab i I i ty , t he Tli Ha i
a G i v i ty o f Ne ut ro n - d e f i c i E., nt Di c~ t o p c-s o f L 11; ti
111?
PERIODICALt r n a L u k s p e r i.n,~ i i t a IU Y I f11 e ti" 'i " y
Vo 1 39 , 140 2 ( 0 p 4 )7 0
TEXT: By applying the principles of isotopic invaj-2.-tr~c--! I riuc'-4-1
the author has been able to d'erive A Very Simplo re'.0 jOn!3'hip the
ersi~s of neutrons and protons -r, distant
binding ~n
AE - E ylA,' E :E.
np n 0 iN" coul C 0 u IZ
AE s t h e dl -f fe r enc e o f t h e b I
coul N z -1 nj)
neutron in the nucleus !1~ and t~iat 2f the Zth prrot~:n -.P, L.,--rcr
nucleus YL
'The first two terms C~-aracteriza
z
when a proton is rt~moved froi-,i th,~ ziaclt!us , thI.
Card 1/3

832 G~
The Limits of Stabil-,ty . the Prot3n- and S, 0~6/6("/Cj
Proton Radioactivity of Nr~utrun-defici,'nl B 0 0 0 j 0
Isotopes of Light Nuclt--,i
accuracy of and may be approximat,~-ly !'oI-w;!'.1
PJ 1 2(Z-1~(?Z-1)- U I " i III t t, I
rip
difference of distant m-irr,r nucl-i a1sc follows ~r-m the
irivariance!,
(7 1- odd A
Z *N N, Iz
A/ All
and AM for evt--n A. r-u-1i I is -'ry
21 fA/2,1;'~AA/2-11 A/2-1~'~A/2f-
confirmed by the available experimt--ntal material W -'. t h
help of the formula given here, the author t 0 f
s t ab i I i ty w i t h r,?s p c c o de,-,.ay w i t h --a i s s 1 on c'l' pr') ~-'q e neut ror:
def icient is o topos of ilght nuc 19 i , and prtLdic t-; r, :-C-:; o- abo~~T.
90 isotoDes of this kind (See Table 2) ift, discu,;!;-o of
observing proton radi.,)activity --ind iwl,,~,ates 9how
(for oxampl-, Beo---*Li P) For I)Ie
Card '-1/1

202
Tht= Limits of Stabil ity ~h~
Proton Radioac t i.v ty of Neut. ron --,ief i c~ i et,t 0 C; 1, 0c
Isotopes of'
oto:)es are i n d d i
33 ( 34"
Ca C r- F
S e65(62?) 67 6 r,- ?h P::iain i)rot)(7,r+ es o f-,,j o - p r c) t.,:) r. ar-
I K
dis cus s ed and , h~ p r -,b lems of proba~ i I ity a ri P- ~ I , i;
p r o b 1 e ms of pr,~paration of neutror. I!-, ic.- titI
stable light nucle-i Nith H or He n uc I -- ia r- also authir
thanks Ya B Zel~dovich for discussions A 1 3az' '-s ir~nt:cned There
are 2 tables and 1; re4prences: .1 Eoviet and ':JS
ASSOCIATION% Fizicheskiy institut im. P N LEbed-ja nauk SSS-~
(Ins..t-itute of Physics P N Lebedev of ~hf? Ac~I~if-mr,-[
Scienc~,,,, of' the USSR)
S UBIMITTED -I: a r c, h -2 89 110
Card 3/~

87030L
S/190/60/002/007/015/017
B 022 0/ B 0 ',-, 7
AUTHORS: Barkalov, I. M., Berlin, A. A., Golldanskiy, V,-_~
'.1 - , ,
Dzantiyev, B. G.
TITLE: Radia'4nn Polyme-ri2at-~on of Phenyl Acc-tyl!ine
PERIODICAL: Vysokomo1ekulyarnyye soyedirieniya, 1"Iel"O, Vol. 2, No- 7,
PP- 1103-1107
TEXT- Purpose of 'his paper was "lie investigation of kinetics and the
mechanism of the radiation polymerizatlion of phenyl acetylene which was
initiated by electrons with an eneri;y of 1.5 was carried
out in special cuvettes (Fig. 1 a). The electron beam was introduced
through a plane-parallel wLndow 0-5 aim thick. For accurate thermo-
stating within the range of positive temperatures, a different type of
cuvette was used (Fig. 1,b) . The temperatures of the polymerization were
-196 to +850C. The reaction yield was not. hi.-h-ar than 1C, - 1X, , since in
all exnerimento tj,, 4nitial staCe of polymeri,-,ation .;as investigated. The
radiation dose was determined by a chemical dosimeter (0.02 nole/l of
Card 114

HT z43L
Radiation Polymerizition of P~',enyl S/1!)0/60/00,1/007/015/017
Acetylene B020/'BO52
I I -
CUSO 4 00.002 mole/I of FeSO 4 0and 0.09 n 1 H.)SO, " which recommended
by the In3titut im. L. Ya. Karpova (Institute imeiii L. Ya. Karpov). The
de 3;
veloping Fe ' was photometrically examined by a 'SF-LI) Spectro-
photometer. The IR spectra of polyphenyl ace%7lene were studf-ed by Yu. Sh.
Moshkovskiy. The polyphenyl acetylene yield rises proportionally to the
dose of wide ranges (107 - 106 roentgen) (Fig. 2). Even with the largest
doses applied, no noticeable destruction of the developed pol-Yner was
observed. This seems to prove the absence of effective inhibLtor additions
whose presence would be indicated by the S-shape of the curve. In the
presence of atmospheric oxygen, the polymer yield is increased to the 1-5-
to 2-fold under otherwise equal conditions. With a certain dose, the
polymer yield does not depend on it,% quantity, not ever. at teml.,eratures
near the melting point or when the liquid monomer is exposed to radiation.
The dependence of the polymer yield on the quantity of the dose was also
investigated (Fig. 2) at 0 and -780C. The extremely low dependence of the
polymerization rate of phenyl acetylene on the temperature is also
typical. Experiments were carried out regarding the polymeri:,ation of
phenyl acetylene in nonane and ethyl acetate. In theoe two solvents the
Card 2/4

670M
Radiation Polymerization of Phenyl S/-1qO/6C/002/007/015/017
Acetylene B020/BO52
polymer yield differed widely from that expected on the basis of the ad-
ditivity law (Fig- 3). A very effective radiation enert3-y transfer (the
radiation is absorbed by the solvent molecules) to the. phenyl acetylene
molecules is observed. Substances with structures of the polyacetylene
type have the same properties as aromatic hydrocarbons, namely that of
taking up the energy of ionizing radiation. The laws of ph(niyl acetylene
polymerization in many respects are specific, sometimee even !he opposite
of those of the usual radical polymerization. Summing tip one nay say that
the polyphenyl acetylene yield is approximately 0 - 9 nolecules when the
radiation is 100 ev. In the liquid phase., polymerizatior and initiation
rates are proportional. The activation ene:rgy is as loir as approximately
700 kcal/mole. A mechanism was suggested which explains the Unusual
results by the specific properties of ha-hly conjugated products during
the polymerization of phenyl acetylene. in these products a strong de-
localization of unpaired elements takes place, and the reactivity of
similar molecules is reduced with an increase in their length.
There are 3 figures and 6 references: tj Soviet and 9 US.
Card 3/4

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0
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:~r t r
in r o n - m r~
117.
in f r r"E. f
as of n,,,--, t r c n - ;-ric; n t
i~3 h~ C'n y vaiiz-,~!,- f0-1 -C

BAZ'., A.i. ; G(VDAIL)K17, V, I ~ i zll;, (If I 01.'i I f~ , b1. h.
Undiscovered isotopes of niiclei. Usp. fiz, nauk 77
nr,.2:211-234 0 160. (MIRA 16. 8)
(I Sot op~;,5)

GOLIDANSKIT, V.I., prof., doktor fiz--matam.nauk; ZHDANOV, G.B., doictor
fiz.-matem.nauk (g-Mosk-va)
Sample of scientific foresight. Fiz. v. oldcole 20 no.):' -11 MY-Je
5
16o. (HIRA 13'-11)
(11articles (Nuclea:r physics))

6 9cc
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~ cations ~O-meson i s 2, 1 0
-en,,L;~-z ~~ccordinj; to :IIIJ :1 1. 1 J -
decay modes ar-~ ~.-ri' ten do-.,;r,.
0
T
o r I S al S t Cal
0
theory of multiple processt~f3, ti'.e I: c m r a re h- Fe pr:)'esses w4t'n
C--xperiment al J aa n c e r n. i n nn a-,icn of
T ~le m-!an v 1 1 1 r"
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15 1.1-11, '!"H
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s r n ann j,,.i I o n 1-n a~-Y-i ~2 --iS
fluence ol d f r e add i o n s i. eg e - 'r h
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act. on tl~~
n u m a rin i n
t i , n s a nd -t' c~, T,-J 5how P- c on i so n i c) x i
r edu 7 t i --) n -. f. a i- t, j r9 sand characl~~!ras-i:,q ,17 -i I t, Ife 2,
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Aq~ie0l,13
SOlUtions,
Concentration o a u a td C.1 n. 0 1
in re+0. 4 5 c n; 4- 0 . 'I (1 7,
I f~' 7 t
ba 4 n, I re al, o an.:
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Card 3/4--

83608
9/056/60/038/005/o,ii/050
1- 070 B006/3065
AUTHOR; V, 1,
- -------------
TITLE. Superheavy 13otopePof Hydrogen and Helium
PERIODICAL: Zhurnal eksperimentallnoy i teore*ichegk,:,y t-,zik, 1960
Vol. 38, No~ 5, PP. 1637 - 161g
TEXT: Data on the neutron pairing energy may be used to estimate the
stability of numerous isotopes (especially H5. H7, and He8) against
neutron emission- The present "Letter to the Editor" sbcws that this
method offers usable results for the above-mentioned ii3otope5. Pig.
shows the pairing energy E as a function of Z of the -irst s-,x neutron
shells (from is to 2s P) for all elements from ~,yd:.-ogen tc potassium.,
112 1/2
(E denotes the difference between the binding energ-,eiz of -h'! (2m+2)nd
Q (.2m+l)st neutron). It maybe seen that nuclei with'odd t,rot~,nnum-
He6
bers have a smaller EU than those with even proton numbers. I : The
pairing energy is not-higher than 2.86 Vev and n~,t lovi:!r thax I. 5,1 Me -,r
6 9i he -uirement that
(the values for He and Li respectively). Thus, t", req
Card 1/3
V~(

836o8
Superheavy Isotopes of Hydrogen and Helium S/056/60/01,8/005/041/050
B006/BO63
the He 7 4 lie6 ~ n decay energy be smaller than -1 .4 !111~v is, a rivcq3oary
condition, and that this energy be not hither than ,0.8 -'s a suff,-
a
cient condition for the stability of lie ,A comparison betwe;~ n the
sses of Li Ile and n along with the cort
ma -7. 6, -ection for interd: -
tion indicates that Hed is stable if the first level
T i~') for A~-7
is not higher than 12.7 14ev, and that it is safely 6tatie if thp 1ovel
is below 12 Mev If the level with T - 3/2 exists, the He? 4 -He" , n
decay has an orier6y of about 1.1 Mev, arid from the condition of slAbili
ty it follows that the pairing energy of the two last rieutrong is not
lower than - 2.2 Mev- The problem of tile stability of He a rOlLains Ull
solved, Some experiments which might contribute to ita explariatiin are
given... if5: Also in this case Ep- 2.86 Mev (this ID thE! Value C,Dr Ht~ 6
which is the even nucleus with the same number of neutrons).. Further-
more H) can be only stable if the ener~zy of tile H if d--av 4A
4 3
not higher than - 1.~t Mev. A comparison between the maii5~s H= H
Card 215
I

836oR
Superheavy isotopes of Hydrogep and Helium S/056/6C/038/005/04' Ir" 0
S006/Bol')5
and n along with the correction for Coulomb inter-kct,,-:!n
,an op -n1v stable -,f tile with Tf-1 for a-2zirti:-Io~ -3
I
-- 2. ? Me vThe 'a,t that no He" levels arf, known f~lr th.,B 7an~-E
tha' H- ,,g unstablc,. The upper limit. oil' tile le-;-el With 11'~ullitoi
be - 25.2 Mev The stability against the H 5 .4 115 -.n -,h~
energy of the level with T ~ 3/2 for A~c, which is Kev, A-- 1 data
lndi(~ate tha,, this nucleus is unstable. If the R 7 nu,~IeuE wfire s'~,abi~
it would be fcund in reactions of the mode Be 9(It-*2p) in
Ya F- Zel~dov4ch and A, A, OEloblin are thanked for Th e
are 2 fiEures and 6 references: 2 Soviet, 3 US, and 1 D'.~',,h
ASSO CT ATION; Fi zicheski.y institut im, P , N. Lebedeva Akade-m~ I nau'- SSSF.
(institute of Physics imeni PI IN Lebedev of tli--!
of Sciences USSR)
SUBMITTED: January 16; 1960
0
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V~

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AUT-40RS: -G K D
TI TL E: !a S t I - -p Scatt"t-In". ft*
the Pc 1 -a z ab i I ', ty :)f
P-RIODTC-L; h-,; r r, ;2 k s 7. ei m, r,
TEXT: The a d t- -d Ae~crl :tl
of scatterinE experiments, f the d --'~ t--r:; tc r- F
I . - ! ~
elastic '~p scat t,~rJ ne. 3 9~-- * i -n i3 -a n ~I c F' r7~ r i F, f t'- e
'-i th t h ry The :,b ;~-ct of thr~
data EivinE a def in i t Irlif ~-mat , cr, c- tll~.i~- z a b I t C -cn
Th,:~ Pxpe--'im~n ILL ':u t '~n t1-:,
th,~ tzamma f
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The
7
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El a fit c p Sca t r ~: r in r, 0 i
,10 1-0 "Iev ~imi t
o
F'c,~ 1) e
0 n ve r r
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electlrcni c a s c n r, F
t r c n s c :0 0 e c
an e
r a i n e a--- The ---x
gh I 'r -m
e L
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71 1 !,'1 7
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PERIODICAL:

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TEXT: A
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thermal
r
r I I -
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to a then:!,il nol~i r:-, 0 C)
-in c e
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rap,-.-,t -it t'l-) 2^11 -I IlItI. con~,,Iinx of PoIntion Resoirob,
H,qyo:7 G4. Prlt. ~-Il A,,,,,,,

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s! i c hee 1 s 'u v o t r o nu II C ~l e r -
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it 'i'dil 'Le or.-I !-.-in 1 i n i !l o n ~! r i3,
Card 2/8-

2.2291
7
an! tra:-,z t i ~-~ns o -.'-,e E,' ~__n] '.'2 'o-: n c 0 rI -
io n I ev e 1 s e 1 v c I, + J
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CC,
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c o r, f i 7,1 r i 0 n 1 e,:;~ S Z~ 7
or j
o n I r: L
c o n f I r a 11 v e a L e t -s t i i 1
carj zl/,q

22291
5/055 '/ 6 1 /0 7 0 4/0
Some -oroblems of the isomericm 3 12 5,,32,-,)',
10 87. 10*(
+ 2
Ar 1 (0)
is is'
also in neutron transfer procQz~~;,:S o'
83 (9/2 +
,I'r (9/2 + 'j +
c-cnon cri t 4-a 1f1i Ic of n C'I' e c.:;
CeCt4,
,)n op
rons and Z oro s i c
Z) 11 ZI (AP )(It
(N, Z) - - (N Z) p Z)
-- 21?
1. Z)
+211 rvI
f
114
The dissertation of candidate Y... :,7orozov ins i tu
t. .1 ~ '7,
4 tu,
SSST .,enerno-fiziche-c - n ZI
~Z - ',fockovskiy i,iz,,
o-~* CI-iemical p,.,jyoico of the AS USSR !no -Y94',s and
Card 5/8

22251
3/0.53/6 1 /073/00~~/004/007
Some Problems of the isomerism of... 7; 1 5/ 32 01
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On -,-e proidem of plyrierization at low temperatures.
Rev ch-:,mie 7 no. 2: 501-511 W~
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