SCIENTIFIC ABSTRACT GLAGOLEV, V.L. - GLAGOLEVA, A.F.

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

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S/05 6/6 O/o 3 9,/C C61", 2 6/o 6 3
B006/-1056
A UTHORS Glri&olev , V 101'ozov , A. 11. , Y a rilpol 1.q',.-_Jy,
T IT LE: Reactiong Leading to the Forz-ation :,ef 'he Fb 2 0 5 ir,
P ER, 10 D 1 ~321 L .Zhurnal eksperimental Inoy i teoreticheskoi, 1)60,
Vol. 39, No. 6(12), pp. 1621 - 162,1
TEXT : It was the aim of the authors to investigate more cicsely "he
characteristics of the short-period gamma radiation fr,-_21
thallium irradiated by 1Q..2-.'jTeY protons and from lead, !.rra1laltnd by
14-7-',,'ev neutrons, and to prove that this radiation mas-. t)(- ~ijcribed to
thi! iso~.~er Pb 205,,l,,. The experimental method is describt~,' iti ~~.n e-irlier
Papur (Ref.5), From. a multiple of measurements the D1' this short-
period zadiation coald be determined as (0.911 1 0.01)"Alev; in th-
spectr,,;m of this radiation also lines with 0.75 4 0.01 and
(0.27 L 0.02)11ev may be observed. Investigation is rend%.red m:)re diffi-
cult because of the considerable background. The "qa7f_14fe c--' the
radiation with 0.97 Mev could be determined as (5.2~L.C.5 I.-.isec, a.Dd it waF
205
shown that this isomeric radiation occurs in the react..!:j.,t ~,f Tl, iith
Card 1/ f3

Heactions Leading to the :Formation, of the S/C5 CE 0,'03 6/06 31
Isomer Pb 205M BOC6/3(:56
protons. The minimum proton energy a" -nhi~~h it oc:urs 'vio 'e-,el-inecl
(7-7 + 0.4)111ev. The data obtained can be explained only by assuiming that
205
the isomer2is formed according to the reaction TI (,,n)?b"'~'m. With a
32.3 mg/cm thick thallium target, the cross section c-" tlic r-,:action wa!!
determined as oM = (20 + 4)mb for an energy of 19.2 1',1ev. Further investi-
gations of the short-period radiation were made by bombardinT lead by
14.7-MeV protons; in these experiments, the half-life of radiation was
determined as (5.0+0.2)msec, the maximum intensity corresponded to an
energy of (0-94 + U.02)11ev. Further investigations showed ths~t this
reaction was Pb 206 (n,2n)Pb 205m; its cross section was dezer~ined as
those
C1m (1.1+0.2)b. The results are compared with U obtained by other
authors and are discussed. The authors thank A. F. Klyucharav for his
interest and the accelerator team of the FTI AN USSR (Instituto of
Physics and Technology AS UktSSR) Rri Well as M~. V. "iki~ihova for ex-
perifliental help. There are 1 tablp and 7 referencea: d '1;Cv_`,%t, 2 US, and
1 Dutch.
C'q I, (1 2,1 ~

Reactions Leading to the Formation of the S/056/60/039/006/026/063
Isomer Pb205m B006 3056
ASSOCIATION: Institut khimicheskoy fiziki Akademii naul: SSSi (institute
of Chemical Physics of "Ile Academy of Scittnces U:iSR)
S 1:3 M I T TE'D :Tuly 29, 1960
Card 3/3

AUTHORSt
TITLEs
PERIODICALi
2,: 1,.!6
S/05 6~6 1 C,/rIC., 5 /006/031
B 10213202
Glagolev, V.L., Yamilcl'skiy, P.L.
Study of the reactions (n,2n) leading to thit
formation of isomers
Zhurnal ekBderlmontallnoy I teoreticheskoy fizil(if
v- 40, no- 3, 1961, 743 - 748
TEXTt The authors have pre8ented the investigation M0010110 and the preli-
minary results in previous papers (ZhETr., ~_6, 1046, 1959 and Lb 1621,
1960)1 in this paper, further details are given. The samples w-!tre Om-
barded with neutrons which were emitted in a pulsed bombax(Iment, *,)y D2 ions
of a thick tritium zirconium target. The neutron energy t3pectrum had a
maximum at 14.7 Mev with a half-width of 0.25 Mev. The followinj~ results
were obtainedt The lead isomer which had been formed In the reaction
Pb 208 (n,2n)DLb 207M had a half-life of 0.81+0.02 see, the- ii3omar production
cross section was 6m. 1.7 + 0.3 b. Similar experiments were made with
Card 1/4

22!26
C, 3 1
Study of the reactions ... 31 0211,D3:(',-2
the reaction Bi i I , 2 n ) B It wag found that the onergits of gamma
2 08 m
r~,diation accompanying Bi decay were 0.88+0.02 Mev and 0.1;0+0.02 Mev,
the half-life was 2.6 + 0.1 msec, the reaction cro.3s, oec-'i M W:19
0.66 + 0.12 b. Further experiments were made in oider to de-;!rnine- the
cross , ction of reactions which led to tho? formation of a 1,mir-lived nio.-
biLIM isomer as well as experiments for a more accurate mi?uqur,?m_~nt of the
Na 24m half-life. 10.0 + 0.5 d was obtained for the half.-lift: -)f the iscmar
Nb 92g1 0-94 + 0.1 Mev for the energy of' t;amma radiatiorl acconarly-ing its
beta decay. The reaction cross section Nb93(n,2n )Nt)92g ,,,Az5 found to be
0.56 + 0.06 b. The godium isomer was produced in the riaction
Al 27 (n,-)Na 24m; the Na 24m life time was found to 1)(9 18.3 + (-1.6 i,~,uec, T h
Y88m production cross section was 15 111 ";> 0 . ij b rtuthov~i
calculated the cr,-)3u, section of lead-ioom,.Ir production tikat, this
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SP" "x r" 11~ i 1r)".A P" 3 1
Study of tile reacti,)r-B . . . El C2/B2()2
208 ' 07 111
isomer is prcafitced orily in trip ri~,-Liori PI) (pj2n)P1--c . Th'? vitIlle ob.-
tained was compared with thp orie c:ilculated from the strl~ng-interaction
theory by amt.,~umiv., a two-sta~-E ri'.Oc"~anism (;f nel'.tr"'n ;!V-11:~:Va'ior~ in the
set-.eme was ifie~] wa!; in
(zi,2n) reaction. In thiq ciise al't-07 levol
~'.Jreemk~llt wtth 9hell mo(Aelt P112 (grcjund state)l ~r, )1V 0-57" RO'll
P3/o 0-894 Mev; i,3/, 1.633 Nev (riwtn:;U~ble 8-NIte)l f. 11'~ 2'13~j'-?1'*Vj
I- I [j
9912 2-75 MOV; i111/2 3.60 Mov; d5/2 4.42 Mev;_ g712 4-66 Mev;
d 3/2 5.26 Mlevj furthermore a level with (1'-,,/2) and the energ;r 5 Mev ilt
assumed. The relative probabilitLes for various. types of tranijitions &re
estimated from the relatL)n between the lifetime of a niiol~iue in the
excited state arid the transiti.on energy. The experimente.1 and theoretical
results are in good agreement,, The- authors thank M4V. 1111C.ItO711 for ass 'i.-
stance in the-experiments. V.,N. Sakharov,-B.S. Dthelepov, L.K. Pekex~q
N.N. Flerov, T.M. Talitsyn, L.B. Migdal, L.V. Groahe,,r 'tnd I.S. Shapiro
are mbntioned. Thpr-2 are I fiE~~ire arid 28 r eferenceq., P Soviet-bloc and
20 rloti-Soviet-'-Ioc. The 2 :-,,st re~.ent referer.ces to Pub-
lic at ions rettd a.,, fe) I I ows -- D.- Strnminger, J.M. HoL1a,,l(J.e:r,, G.T. Seaborg,
Card .31A,

221'
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Rev. Mod . P~ y:-. . II.J. Asby ~t R,, v . 1 1.1 616,
ASSOCIA' !0,13 Irj,~tif;it fizi'-l Alc,idcii~ j 4 11 .1
I n i t f C',; "m i I ?hy." i t I A
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7
03 126 1 CCOE:
A',,-,'! i 0,'t Da"Imnovn,A.Yt).; Glagolov,V.M.; 5hafranov,V.D.
O!"G: Nolle
TIYLE: Toroidal j)1;1JlWI tr3PA With NP-3tial magncLic axo.,
SOU12EI: ','hurn;iI L(~Iji u ic lies IWy fiziki, v. 316, no. 9, 1571-15~i,li
TOI:C i'AGS :plasma confinement, flold, mairliotic ste-I'Larator ftc-11,
maLhematic physicu
AT367i',ACT: The authors discuss the confino;ient, of I.:1 ml-'rctic 0" :,lo-,
type 'that can be produced by all Orldles."; solf"loid woun(I zhrou,:.I and al)ollz -I Circulllt-~-
torus as exemplified by tile fi'.-Lir(-. 'rhes;~ fLelL; Call b(J
of the fitrure-eight typo otellarator ficid p~-opo!;(x~ by
(Phys. Fluids, 1, 253, 1951'0 , XVh!Ch t,LO '-l-.CIIdC it.; I Sf)CC.JaI C--ISQ-
V.D.Shafranov (Yaclornyy sinto", 4, Lj.,I prvviotu;ly
ShOW11 that the disj)LlCf!:IlollL of Ulu wir"'ace"; of tile field
0" a solenoid in the pr,~sencc of p1ns.-i-a Ls by the
a and torsion of tho axis of the solenoLd. 1,i tho prescr.-,.
curvatur , derived for tho and tor,10.1 of
paper formi ulas ar(.
solenoids of the considered typa, and tli,, ciisto~-tion of tacl.r
7TI magnetic surfaces in tho presenco of plasma- :L3 discussed. Topo-
C.rd 1/2

1~ I I -'. 15-'.7
ACC ;NR: A1160312161
logically equivalent torus-solenoid Coffiguratiozls in which the Solenoid
of line segments and circle arcs are also treated. It is concliidcd that z'-e
tion of the magnetic surfaces is minimum when the solenold axis riakoj all 11.-~;Icj of
about -15o wish the torus axis, and that n suitable value Of Lho ratio of Lila gaci
,pressure to the magnetic pressure for optimal corditions is 0.1. The aLlz:hors thank
-Ye-G.Lariontsev for his participation in the preliminary calculation Tiork. Orig. art
has: 40 formulas and 7 figures.
SUB CCOS: 20/ SUBLI DATE: 31Auj-65/ ORIG Mr: 005/ al'Ir REF: 001
Card 2/2

L 1836-66 C
ACCESSION NR-. AT5022417 UR/313()/6,t/00(1/674/0001/002,1
AUTHOR: Alikayev, V, V. -, Glap1q,
TITLE: High-frequency paramagnetic stabilization and heatbtg of plasma"-w"Ith
electromagnetic waves
SOURCE- .-Moscow. Institut atomng enqgi. Doklady, IAE-074, 1964. Paraningnit-
naya plazmy elektTomagilit.nyrni volnami,
1-24
TOPIC TAGS: plasma heating, plasina stability, plasma electron teniperature,
magnetic field plasma effect, plasma electromagnetic Nvave
ABSTRACT: It is shown experimentally that In the presence ol I-IFE-4.-MlIzing
fields, convective.- type macroscopic instabilities are either maipleLply absent or areI
strongly attenuated in a plar3ma with a coucentration. n of 1011. to 101.3 c111-3 located in
a magnetic field having the geometry of an adiabatic trap. In the rartge of magnetic
fields corresponding to from 0. 6 to 1. 0, a fast heating of the plumna electrolle
takes place, so that the p7asma pressure Is about 10 times aisi liligh as the pressure of
the HF field on thet plasma. The maximum temperature of the electrone of the heated
Card 1/2

L 18,463-66
ACCESSION NR: AT5022417
plasma fs 1000 ev, At low plasma cone entr aLionr,, when t1m L;mii~11111i:r i--ilectrou
frequency is closo In order of magnitude to the
lifetime of the plasma dooreages in the presetice of HF fields. 'J"IdEi etfxut appears
to be related to mi accelerated escipo of clectrou.-.1 Into tha "dwiffer cono" of the
magnetic trap owIng to collectivo processes. nie effect of rvinoval o! i'las imitablilty
was observed exparimentally. Orig. art. han: 12 figures and L formulit.
ASSOCIATION: none
SUBMITTED: 00 ENCL! 00 SUB CODE: ME.
NO REF SOV: 001 OTHER; 002
Card 2/2 11

L (,)!765-67 B-Pr(l) FJTI)
ACC NR: AP6018350 iiii/(;(,-3!?,'6~~/G,20/CJO.,/o4ol/o4o7
AUIHOR. __ I olev~ Khromkov, I. :i tic
OP.G:
TITLE: Paramagnetic Lffect under the influence of hij-ji frenuency pressure Wid
-electron parmnagnetic resonance in a. platoma
1, ) - '-/
SOUPCE: Atomnaya energlya, v. 2(), no. '~, 060, 401-407
TOPIC TAGS: electron paramagnetic resonance, plasma inntability, prossure effect
ABSTRACT: This is a continuation of earlier wcirk (Ilucl. Fusion, Stippl., Part II,
1962, p. 687) devcted to observation of the prtrt~.majTnetic effect in a plasma under the
influence of the presi,ure of high- f requency fieldr. With an aim ELL providing a laech-
anism for stabilizing allainst flute instability, the authofs investigated experinen-
tally the interaction between microwave fielV (w = 2 x 10 0 sec-1) of a cavity re-
sonator with a dense plasma (n , 1013 -_ 101 cr.-3) in a constiuit malmetic field.
The tests were made in the If 013 mode with a hik;h-frequency map-,netic field amplitude
up to 150 Oe, which produced a parRMILf.,,netic current in the plimtra. The resultant
plasma configuration is described. The increase in the static na4pietic field inside
the plasma, associated with the parama~pietic current, agrees well with the theoreti-
cal value. At w H/W = 0.5 paramagnetic resonance of the electrons wan observed, lead-
1/2

L Oh765_67
ACC NR: kv6018350
ing to a sharp increase of the plasma pressure po to a value corresponding to
2
BirpoHo t~ 0.2. Tile methoe~ of determining the plasma pressure is described. Re-
sonant heating of the plasma electrons by the high frequency field, connected with
the parametric resonance of the electrons, was also observed. Orig. art. haa: 8
figures and 2 formulas.
SUB CODE: 20/ SUM DATE: 03Aug65/ 013IG MY: 0021 OTH REF! 003/
kh
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-GLAGOI0ly V.N. --
Plasmal recation in the myelinization of regenerating wcams.
Dokl. AN S,c;SR 147 no.3:721-723 N 162. (MIRA 15:12)
1. Voymno-meditsinskaya alcademiya im. S.M. HiroTa. Pmdstavleno
alcademikom N.N. Anichkovym.
(WERVE0 (UGFVKRATIO1, (BIOLOGY)) 011JUKAL)

U171OF1/H,,m,i-( ano, Ani-mal. rhpiiclc(~y (Namal aild FIThc~IG61r:al) T
Nervous System. Higher Nervous ActMty. Behavior.
1..bs jour Rel' Znur BioL., tic, 6, Lo)9, ,:.,,,c4cj
Author GlagoLev, V.P.
!list Kiev 'let.-irlinary Institute
Title Obtaining ConditioneOl Ly,~-.iph-SecretinLr; Reflexes ii-. rogs.
Ori6 Dl~ Tr. KJ.yevsk. vet. in-t, 1957, 13, 113-11'1
Abstract A conditioned Lymnfh-secretlnj~ reflex to bell rehifor-
,2.2d by introduction into the ;ein of prep-
ratiov.s (mercusul, celandlne tincture, pptone in sn,411.
(loses) was Produced in (logs. U't-Ir 9-35 (101:11ti-na-tio"S of
conditton,:.d and unconditioned gtimida.itsa cannula was
tied in into the thoracic duct aiid Iymph !iecretion was
measured. After the bell the lymph secretien in:-reased by
This clata allows the utLI1;,,ation of the
Ca rd 112
- 115 -

V.P. Cand Bio -- (di,,sl "Effe-ct, ol' r,%e
nervo Ili 1 Kiev 1~6." hlp!~
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';nevchenKo) 100 co: i6~; ( 91,1 A-I,t- I ;H)
- I ~"i -

GL.',GOL----i, V.P.
Demonstratinlo the work of heart valves. q I o 1 . v a ',, ',c -.) 1 ,. --. o . -) :
8,1-89 S-0 15Q. (MIR,", 1.3:9)
1. kiyevskiy gosuriAr,.;tv,,-rinyy uriiversLtet.
M 1~r--v *I.Prps)
( !l,',l!-TCMT, MPVN---,',TJDlO-V[SF'L ',IDS)

21594
S/109/60/005/010/017/031
E033/E415
AUTHORS: Breydo, I.Ya., Glagolev., V.P., Glukhovskoy, B.M.,
Korollkova, O.S. and Leyteyzen, L.G.
TITLE: Investigation of the Stability of Multi-Stage Photo-
Electron Multipliers
PERIODICAL: Radiotekhnika i elektronika, 1960, V01-5, NO-10,
pp.1698-1702
TEXT., This paper was presented at the 9th All-Union Conference on
Cathode Electronics, Moscow, October 1959.
The stability of the output signal from a photo-ele-etron
multiplier depends on a number of factors: the voltago, the
current, the time of operation and so on. The purpose of this
article is to clarify the effects of these factors on multipliers
with emitters of different materials. Since multipliers are
widely used as scintillation counters, the multipliers were tested
in a special set-up which approximated to oserational conditio-9
with crystals of NaJ(Tl) irradiated by Csl 7 on the cathodes of
the multipliers. Block diagrams of the test apparatus are given
and the apparatus is described. The output current, which
depends not only on the amplitude but also on the frequency of the
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21.59.14
S/109/60/005/010/017/011
Investigation of the Stability ... E033/E415
pulses, i.e. on the intensity of irradiation of the crystal by
y-rays, was also monitored. The results show that there are two
types of instabilityi 1) smooth change in the average value of the
amplitude of the pulses over a period of time and 2) oscillation
of the amplitude about a mean value, which shows as a scatter of
the recorded points for a given curve. The deviation of the
points is apF.~-oximately 0.3 to 1% of the value of the output pulse.
Early tests showed that the stability depended to a great extent
on the previous history of the multiplier. The "settling-down"
time is different for different specimens and for the
specimen the settling-down time on the first day can be very much
longer than on following days. This "training effect" made
investigation of individual specimens impossible and statistical
tests on a number of multipliers were necessary. The results on
80 multipliers of the OY-35 (FEU-35) type with Sb-Cs cathodes
and emitters are presented graphically by histograms of percentage
change in pulse amplitude against numbers of multipliers for output
currents of 0.1 to 2.5 microamps, 0.3 to 0.5 microampa and
0.55 to 6.0 microamps. The maxima of these distributions show
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'?1594
S/109/6o/005/01.()/017/031
Investigation of the Stability E033/E415
greater percentage change for larger currents. The rosults for
60 antimony-cesium cathode and emitter multipliere were similar,
It is concluded that during the first hours of operation the
stability is directly related to the output current arid reduction
in the current density improves the stability. The absolute
maxima of the changes in the output current of the multipliors (lid
not exceed published figures for multipliers with Al-Mjj, silvar-
magnesium and antimony-cesium emitters. The settling-down time
was found to be proportional to the output curret-it. Tests on
multipliers 43Y-24 (FEU-24) with aluminium-magnesium alloy
emmiters showed that they also have appreciable isettling-down time,
but the output current has little effect on it, except that it is
reduced with high currents. For example, a batch of multipliers
with Al-Mg emitters and bismuth-milver-cesium cathodes had an
average settling-down time of 10 to 20 min, after a rest-period
of 12 hours with output currents of 20 to 30 microamps. To
clarify the effect of activation by cesium on the stability of
alloy emitters, a multiplier with a thermo-cathode was prepared.
The stability of the emitter was checked directly in a vacuum with
continuous pumping before and after cesiation. The relative
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2159h
S/109/60/005/010/017/031
Investigation of the Stability ... E033/E415
changes in the secondary emission coefficient foi.- thermo-
activation and for cesiation for one stage of a copper-beryllium
alloy with 100 V and 0.3 mA output current tire shown gri
, lphically.
It is seen that the presenco of cesium I.eadis to ~iri increase In
both the settling-down time and also in the magnitudc of the change
in the secondary emission coefficient. There are 7 figures and
2 references: 1 Soviet and 1 non-Soviet.
SUBMITTED: December 21, 1959
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MARKOV, V.A.; GL&GOL~V, V.S.
Effective use of the State Bank credits. Taknt,prom.
20 n0-5:7-9 MY 160. (MIRA 13--8)
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S/ 1N/6 1/004/004/01j'/0 14
B125/B20",
A H 0 R Ju. A.
TITLi~: Surface of inutual irradiation betvo~en a body and a thin
cylinder
PERIODICAL: Inzhenerno-fizicheskiy zhurnal, v. 4, no. ~, 1)61, 116-lig
TEXT: The author UiVe3 a practically useful, genc-ral equqtion for a
SyStep., ConSi3t4ng of -a thin cylinder and an arbitrary body. T're general
expression for the surface of mutual irradiation i1 of tvo riontransoarent
12
bodies 1 aind 2 reads, as is known: H asl ~ c0!' -11 cos Y2 d (1),
12 = S 2 C2
3 1 82 r
where s I and 9 2 are the mutually visible surfaces of the fir:3t and second
body, resooctively, -1 is the angle bctween the croendicular to the
Y p I
q
element of the surface and the se,,-mnt r of the atraiht line
connecting the .*'-:rot arid second surface elements ds and ds an the first
1 '2
C-Ird 1/6

21781
S/1-70/61/004/004/013/014
surface of mutu.ai irradiption ... B125/3205
and _-.econd surface, respectLvely, cp, is ',ae unrle between the perpendicular
to 602 the fame ~-e~,;:rierit of th( s~rniGht line. The integralzi (1) are
not taFen in t~- form but nave to be calculated for each case by
a differun. ~:o calculate the expressions of interest here, s 213
taken ans "*,,.e of a c.-i.,vier segment, and s 1 as -the surface of any
body in mutual =-!~diation v,'ith the cylinder. The oriCin of -the
cylindrical coordinate s~-sten is assumed at any point of the cylinder axis,
and the z-cocrdirate is direct;d a-long 'the cylinder axis. The surface
element of the cylinder in this coordinate system is ds 2 = (d,12)dz da (2),
where d is the cylinder diameter, The origin of the mobile sp~:'r-_'cal
coordinate system is connecteci with the element d:,,. The plane
perpendicular to tlie cylinder axis is used as plane of the anille tf, of this
sys tem. 'I'h e n if :' ; , ,, [~'
co, 'o'
21.
is found for thl~ rylinder se.'~,mt~n' 1 7, z1 where ti, and "1)2 'are the
Card 2/6

17111
Sz / 17 0/ 6 1 /004/0 04/0 13/014
3 Urfa ce 0 f i a t i 0 11 ... B 12 5/3 20 3
1
integration for a nd ~ are the integration limits for The
2
inte~,,ration li"..,it's i'or ."id oc are interreLated, and art.. comoiled in
Table 1 . Tn t--is table, tho first.- line corresponds to "lie razir,,e where
the Eurface ds2of the cylinder is irradiated only by part of
surface s 1 of an:; body , and where the perpendicular to 6,s 2 is directed 30
that O