SCIENTIFIC ABSTRACT BAYTUGANTI, Y.G. - BAYUKOV, Y.D.
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CIA-RDP86-00513R000204110001-2
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RIF
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S
Document Page Count:
100
Document Creation Date:
November 2, 2016
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June 6, 2000
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Publication Date:
December 31, 1967
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MUM$ M.Kh,; SXCRNWCVl M.V.; MUSABLYANTSp R.N.
LAYTY~I 1; Y~9.G!
Safety problems in using oasing lines. Trudy V.NIITB
no.11%3-12
159, (KERA 15:5)
(Oil we2ls--Wpwnt and aupplies)
RANVELY",
Ghoice of efficient and safe devign of pipe alevutors
for under-
ground oil well repairs. Trudy VIIIITB no.13:21-29 l6c.
(m.1RA 14:12)
(Oil wella-Equipment and supplies)
Y~~, Te.G., inzh.;
XABANDV, V.I., insh.; TJMEDVA, A.$., inzh.; RAVIRA
BIRTULISON, Th.A., inzh, -
Attachmente to pumplag jacks. Bezop.truda v prom. 4
no.4:24-25 Ap-
l6o. (Oil welIA-3quipment and suyplies) (KIM 13:9)
KANMTAN, B.Ge, insk.;, BAYTUGANTI, Ts.G., inzh.
Tabe elevators for underground repalring of vells.
Bezop.truda
v prom. 4 no.10:24-25 0 160. (KWA 13 -- U)
1. Vessoyusnyy nouchno-isoledovatellskiy inatitut po tekhnike
bezopmenosti I neftpaoy promphlenuosti, Ba3cu.
(oil wells-3kuipment and ewplies)
BAITU izL*
MANVELYAN. B.G.., Anzho; GIMTIj>tG. a
Fastemng VA~Joe Of, an sia-dria suboaface pmping vnito
Besop.tru&
v yvan, 6 no,,7,.24 JI 162, Wpa 25:7)
1. VasisoyuxWy nauchno-Usladovatellskiy neftyanoy
inatitut po
tekbnike basopamoati*
(oi:L won pmpiv)
ASHiF,BREV, Tu)rmebay Ashimbayevichp nauchn.
sotr.; #MTULESHEV)
Turinmbek BVt i
-y~eshev chp nauchn. sotr.; KOVAIXNKO
sotr.; SHIM, F.S., kand. okon.
naukjp otve redej LEVIN, H.L., red,
[Labor productivity of Kazakhstan's machinery
i*adustr7
m'd the factors of its growth)
Proizvoditellnost' truda v
mashinostroon!i Kazakhstam i faktory es rosta.
Alm-
Ata, Nauka, 1965. 209 p. (MIRA l8t6)
1. Institut ekonomiki AN Kazakhakoy SSR (for
Ashimbayev,
Baytuleshev, Kovalenko).
USSR/Cultivated
Abs Jour
Author
Inst
Inst
Orig Pub
Plants - Foddore. M
Ref Zhur Biol., No 12, 1958, 53687
)!tuliny 1.0.
P
AS Kazakh SM
Peculiarities In the Davelopment of the Root System of
Perennial Cereal Grasses in Grass Mixturee.
Vestn. AV Khtd,*, 1957, No 9, 105-115
Abstract At the agrobiological station of Kazakh
University: the
perennial cereals, tall rye graas and dewgrass) develop
better and produce a large yield of seeds oAid bay when
40 mixed vith alfalfa, but have a less developed and shal-
lower root system than when sown in pure form. The depth
of the root penetration in the case of the tall rye grass
in grass mixture is 100-110 am, and 140-150 am vhen soun
in pure form. In the case of dewgrass the depth cbs
Card 1/2
Ifffeat of alf&1fa on the nitrogen nutrition
of grasses when
growing together, Text*AN Xazakh,SSR 17
no,1133-39 JA 161,
(MIRA 14:1)
(Alftlfa) (Grasses)
BAMLINJ 1.0.
Root system spread of some field c-"Dpiv in the Dshurim
desert
steMs. Izv. AN Kazakh. SSR. Ser. biol. nauk 3 no.1973--85
ja-F 165. (MIRA 1815)
BAYTULINI 1*00
-- I
Root sysIA6w. of #coo dominant plants of 3mbs Plateau
de3ert
asseclatiow. Bat. x1mr. 50 no.Stll.35-1143 Ag 1619
1 igM 32110)
1. Utyublaska7a opytnaya atamtsi7a kormov i pmatbiahobe
KMHEKEZYAN, A.N.; BMURIN, M.N.
Possibility of lightening and simplifying the standard design of
vens on the Zhetybay oil field on Mangyahlak Peninsula. Burenie
no.9:19-21 164. (YJ RA 18: 5)
.1, Vaevoyuznyy nauchno-issledovatel'skly Institut burovoy takhniki.
0. S!".
Baytiml.n.q, 0. Sh.
"E~roblems of the Etiology and.~Omraratlve Evaluation of the
Effective-
ness zf Certain Thera,--3utic SuBstances In
Bronchor-tv-umonla of Calves.I
Min '4icher Edixcation. Alrm-ktR Zooveterinqry Inst.
klma-Jta, 105~
(Dis I
sertation for t~!e degree of Candidatp in Vet,:~rinary
ScienceO -
SO: Knizhnny8 1,4topist No. 27, 2 JU1Y 1955
BAYTUPJI-I, IN. A.
FWurin, N. A. "Festure reri-ne of the canelg" Trudy Alina-At.
vet.-zootekhn. in-ta,
Vol. VI, 1949s p. ?66-77
So: U-3566s 15 March .53, (Letopis 'Zhurm.-I Inykh Statey, No.
13, 1949)
BATTIJIR~N, M. A.
"The Safeky Level in Feeding Vitamin A tio Cattle and How to Obtain
1-to" Cand Agr ScJj Alma-Ata Zooveterinary Instp Alma-Atas 1953.
(RZhBiol, No 4, Oct 5h)
Survey of Scientific and Technical Dissertations Defended at USSR
Higher Educational Institutions (10)
Sol Sum- No.481, 5 may 55
USSR/Disoases of rarm t~nimals. Disaasos of Unknown R-3
Btiology.
Abs Jour a Rof 'Zhur-Biol,, No 20~ 19561 92745
Author j3Wurjina
Inst -M%Wu~.o of Votorinary Scionco of tho Ka-
zakh 13-aneh of tho- All-Union j'wadamy of
Agricultural Sciences imoni Lenin.
Titla I The Combined Tra4tmont -of Bro.hchopnoumonia
in calVess
()-,IL,~ P*ibsTr. in-ta vot. Xazakhsk, fil,, VAMNILI
195?t 81~125431
,~tstraaijtOn one.farwivtho Alma-Ata,-ro'gion up. to
65 porcentlof newborn ealv Ios used to be stri-
ekon vith-,bronchopneumonia. Ylith the back-
ground of* improved foo-ding, 60 sick calves
Card 1/2
Otses, of'-P~ la
'D 396.365, -a
1,40 Pm
Abs, jour
Ref 'Ihur4i6l a; i9,081 96962
Author..
]r
t
13
:
~
~
74
h
Institut,
Itl 41P i
Sa 4i e n
cResearch Veterinary Inst it,
:
WLS
fi
Title
The- Treatwent of Bronchopnewaonia in 014ves
7tth Intratracheal
Injections of Penie-111in,
wid Benolin.
OrIg ?4b.
:,T:~. Kazakbske no-is
vett In-taq 1957, 91
~
P-29-235
TAbstralot
rorty-!t~w~:'ealves, yere -
tre %ted.
4#er their...
~
ier6- d__
keeping -and - f6-6dInj coll~ljfibhs -T
Zlhe.calves v) ore,
intratj~ache ally inlboted,with
35U-4 '00 t~o~s&nd units of rovocalne
salt of
'renicillir dilfted in 5 ml -,)X^ &a ecmolJ-n sus-
pension once
daily-for 5 -onsoovlive-days. In
ordex to inhibit t*i)6~ cough ref.rul
5 ml 'of a
pero out stispensloh of novwalrxi, viler 'e :Lhtro-
diced
1-2 minutes before the.-pent-tin!A injec-
tior, "T h treatment
resultadlr~ -mring 75,~
Cardu,
n_v)&WtK, Ya. !. and PETMVI V. M.
"Bronchial pneumonia in lanbs.11
Veterinarlya, Vol- 37, No. 8. 196o, P. 51
Ove.
KLEYNBOK, Ya.I.; PETROV, V.H., kand.voterinarnykh naak;
HAYTURINA, O.Sh.
kand.voterinanqU nauk; PCOLINOV, I.S., nauchriyy sotrudnijc,-
ATSEN, Ye.A.., nauchnyy sotrudnik
Bronchopneumonia rate in lambs, Voterinariia 37 10.8:51-55
Ag 160. (MM 15:4)
1, Iwtitut vaterinarii Kazakhokoy akademii
sellskokhozyaystvewykh
nauk. 2. Chlen-korrespondent AN KazWR (for Kleynbok).
(Kazakhstan-Lambe-Diseases and posts) (Pneumonia)
BAYTURSUgNff,-X,-
Tryout of creative forcee. Sov.foto 22 no-4122-22 Ap
162,
(MIRA 14:3)~
1. Otveistvennyy eekratarl prav2eniya Soyuza
zhurna2istov
Kazakhoskoy M. (lasakhatm--Photography-Exhibitions)
VOLAFOWCH, M.P.; BAYUKJO Ye.l.; SAUKHLI, T.M.;
PAVLDGRADSKIY, V.A.
,
Longitudinal wave velocities in specimens of
sedimentary r(cks,
saturated with kerosene andwater, at high pressures.
Izv. AN
SSSR. Fiz. zem. no.3:71-?5 165. (MIRA 18:7)
1. Institut fiziki Zemll, AN SSSR i Institut geologii
AN IzerbSSR.
L 2844-M Wr(l)IEWA(h) GV-1
ACCESSION NRt AP5021277 UR/0020/6
AUTHDRSA Vol .arwUhs Me Pej Ba k 3 CT:
TITLEs The velocity of ultrasonic longitudinal waves at high
proaaura.in
and gas reservoir rocks of Azerbaidzhan
S=Et AN SSSR. Doklady, v. W0 no. 5p 1965, lin-lin
TOPIC TAOSt ultrasonic wave.. seismic w& roA, high pressurel in 5
radioeleclp~.
tric; device
I Sllmftea on wm vao.0iti." iwe made on rocks in the.
Gaspiah~--lowlar4'
ud the Baku Archipelago., The rocks were t93ted at pressures up to
hOOO k1K/ce
la
An M-5 radioclectric device was used for measuring wave velocities,
and a IDA
zirconate and tknWate unit with natural frequency or 500 kilocyclas
was used in,
both transmitter and reneivero The sedimentary rocks were cylindrical
cores., 3 cm
in diameter'and 000 00 Tests
-3-15 cm longs taken from depths ranging from 1 35 m
waris made on clay* siltstone, sandebone, and lim-eatond. All
part"ent propertiis
-of -the rocks --wwo- measuredo -- Ex
periments ihowed a sharp -in=eaae in-, v looity. with
a:
pressures -iithiha- greatest-- I= t - - 200%) be:Lag' ob sorred, -i
ve"
w4we (uj 0 U Porous
sand and 6W, Change in limestone proved to be least generally 15-45%*;
SOV/49-59-6-13/21
AUTHOR;,~kyu~k,Ye~.I
TITLE: A Method of Determination of the Elastic Parameters of Rock
Samples.
PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya geofizi-cheskaya,
1959t Nr 6v pp 895-897 (USSR)
ABSTRACT: A method is described where the measurement of the velo-
city of transverse waves is not required. It is based on
the laboratory conditions of measuring the propagation of
the lonritudinal waves calculated from the formula
L
VPM W- ;' (I - a)/p(l +- a)(l - 2,or)j 1/2.
The samples of rock used in the investigations were syenite,
sandstone.and an alloy of aluminium for checking . The
measurement consisted of determining the ratio a/% PK
(a - radius of a sample, %P, - wavelength of P. wave).. It
was established that the velocity of
V EM did not vary with
Card 1/3
SOV/49-59-6-13/21
A Method of Determination of the Elastic Parameters of Rock Samples
the frequency. The latter was measured with the gauges of
50, 125 and 250 kh. The range of the ratio aA PM was 0.1
to 2.0. The results are shown in Fig 1, where the ordinate
represents the velocity of the longitudinal wave and the
abscissa - the ratio aA The following elastic para-
meters were determined (table on p 896): density p .4.
Poisson cogfficient cy , Young's modulus E , shear modulus
0 . velocity of transverse waves VS 0 volume compress-
ibility 0 , The ratio of VP, /V, was found to be 1.60 -
1.68 which agrees with the results found for real conditions.
Card 2/3
. . BOV/49-59-6-13/21
A Method ot Determination of the Elastic Parameters of Rock Samples
Thanks are given to M. P. Volarovich and 0.- 1. Silayew-for
valuable advice. There is 1 figure, 1 table and there are
7 references, of which 5 are Soviet and 2 English.
ASSOCIATION: Akademiya nauk SSSR, Institut fiziki zemli (Acadenw of
Sciences, USSR, Institute of Physics of the Earth)
SUBMITTED; April 26, 1958.
Card 3/3
2- f
UP
H1,11P ju v
!A--r
al 10 IV 1 131
ass's
Mill 5
v 0
TV
ski
-a I!Vt
.V 31 1 1
'C
Studying the e2Aetio properties of rock samples from a deep bore-
hole at high pressures* Izv- AN SSM. Bar. geofiz. no.12:1736-1761
D-1600 (XMA 23929)
I* Institat fitiki Zewli AN 88SR*
(Rocks-Testing) Ollastic waves)
30 o
AUTHORS:
TITLE:
PERIODICAL:
84664
S/020/60/135/001/017/030
B006/BO56
Volarovich, M. P. and Bayuk, Ye. I.
The Influence Exerted by a Uniform Pressure of up to
4000 kg/cm 2 Upon tlielilastio Properties of Rock Samples
Doilady Akademii.tauk SSSR9 1960, Vol. 135, No. 1,
PP. 6548
TEXT: The authors investigated the elastic properties of rock samples
under high universal pressur by measuring the propagation rates of
longi-
tudinal waves: V 172 - the propagation rate in a thin bar and V~
IV b - (E/ Q) ] /
VP 05. ) 1 2 _ the propagation rate in an infinite
medium (E - Young's modulus, 9 - density, 0 - Poiaaon coefficient);
the
experiments took place in a high-pressure chamber, in which the
pressure
could be varied from normal to 4000 kg/cM2. The ultrasotic velocity
was
measured by means of a pulse method, where a modified M KA-5 (IKL-5)
type
device was used. As transmitter and receiver ammonium dihydrophosphate
Card 1/4
84664
The Influence Exerted by a Uniform Pressure
B/020/60/135/001/017/030
of up to 4000 kg/cm2 Upon the Elastic Boo6/BO56
Properties of Rook Samples
crystals were used; for the purpose of measuring Vp b, the
authors operat-
ed with 100, and for measuring Vp m with 600 kc/sec. The samples
investi-
gated had the shape of circular cylinders with 3 cm diameter and
16-20 cm
l(Ingth. The various ore samples are numbered (of. Table 2). The
results
of measurements are shown in form of diagrams, the assignment of
the
curves to the samples takes place according to the same numbers.
Fig. 1
shows the propagatio.1 rate of longitudinal and transversal
waves as func-
tionsof the pressure brought to bear upon the samplo. In
general, the cu,
within the range below 1000 kg/Om2 showud a steeper rise; in the
further
course, the pressure dependence of V is insignificant or V is
entirely
independent of pressure. Fig, 2 shows the Young's modulus and
the modulus
of shearing as a function of pressure. The course taken by this
curves is
similar to that in Fig. 1. The reaulto of the measurements of
the Poisson
coefficient at various pressures are given in Table 2:
Card 2/4
84664
The Influence Exerted by a Uniform Pressure
3/020/60/135/001/017/030
of up to 4000 kg/OM2 Upon the Elastic B006AO56
Properties of Rock Samples Pratumirp Irv/nM2
Rock
1
500
1000
2000
4000
Gabbro 82
0.31
0.30
0.29
0.29
0.29
Gabbro-diorite 38
0.29
0.28
0.28
0.28
0.28
Granite 247
0.24
0.22
0.22
0.21
0.21
Granite 248
0.12
0.?1
0.19
Granite 249
0.12
0.16
0.19
0.19
0.19
Quartzite 22
0.19
0.19
0.19
0.18
Sandstone 213
0.18
0.18
0.17
0.15
0.15
Sandstone 105
0.19
0.19
0.19
0.16
0.16
Sandstone 94
0011
0412
0-15
o.16
0-17
,arl 206
0.19
0.19
-
0.19
0.19
arl 207
0.21
0.19
0.19
0.19
- I
There are 2 figures, 2 tables, and 6 Soviet references.
V\/
ASSOCIATION: Institut fiziki Zemli im. 0. Yu. Shmidta Akademii
nauk SSSR
(Institute of the Physics of the Earth imeni 0. Yu. Shmidt
of the Academy of Sciences USSR)
Card 3/4
8466h
The Influence Exerted by a Uniform Pressure S/020/60/135/001/017/030
of up to 4000 kg/CM2 Upon the Elastic Boo6/BO56
Properties of Rock Samples
PRESENTED: May 18, 1960, by P'. A. Rebinderg Academician
SUBMITTED: May I'l, 1960
Card 4/4
MAROVICH, ~~Yej.j LIMIN, A.I.
1--
MAotie propn-ties of rocks and the atmarptlon of
elastic
vayes by tbam at %Igh all-romd p"sawes.. Prim.
ulltraakust.
k leal. vashch. no.1335541 161. (HIRA :16s6)
(Rocks-Elastle Properties)
(Mastia va"s)
VOLAROVICH, M.P.; BAYUK,, Ya.I.; ZHDANOV., A.A.; TOMASHEVSKAYA,
I.S.
Study of the elastic properties of rocks of the K21a Penin-
sula under hydrostatic pressure up to 7000 kg./cm . Izv.
AN SSO . Ser. geoflz. no.8tU78-1181, Ag t64 (MIRA 17t8)
1. Institut fiziki Xamli AH SSSR*
AFANA59M.~ G.D.; BAYUKI., 19mcrys B.P.; VOUROVICHv M.P.,
ULz8v=9
BIV,
Phy3ical 'propertieB and the absolute age of certain rocks In
India and Ceylon. Uv. AN SSSR Ser. geol. 29 no.3t22-42 W16A
(HIM 17 23)
I* Inatitut geologii rudnykb mestorozhdaniyj petrograftij.
minera-
logii i gookhimii AN SSSR i Institut fisiki. ifwli AN SSST4
Hookwa.
s1b=10#1j55joo511W11061
AOMMCK IM. AP4034338
"AUMOR: Afaaw 1yev# Go Do (Correspodding member); Volarovich, K.
Pej Boyuk*, Too ~A;.
Galdln.p N. Ye.
TME: Investigation of velocities of elastic vaves In ultrabssic
rocks or the
lWnahesorsk Pluton under bigh (allal%d) pressure
SOUM: AN MR. Doklady*0 ,f. 355# 00. 5j. *&p 1058-W1
VaVe
TOPIC TAGS: elastic vaye velocity, scismia research,, tran vereal,
veloc*tY*
langitiYA"W wave velocity, rock &p, geology.. geophysics, high
prewir6j, VUM=p
Monabegorsk pluton., tectonics
ABSTRACr: In preparation for the cadng geological-geogbysical
(deep sclowe
probing) of the Baltic rbield., the authors howe'lavestigated the
velcelty of
elastic V06VOll in ultrassic rocks of the Monebegorak pluton
located In the central'
p&A of the " Peninsula. M)e age of this rock (by the radioactive
A4.Mthod)
is about 3 x IV yeane The veloolt;f of both -fitudinal &A
trensverse Vane
.A
vas datenzimA under pr*snum vp to 4..000 Me velocity of the 104AW
VaVes averaged 7OWto em al"o. and that of the trawvms VMS
C. d -1/0
VOLAROVICHIO GALDIN, N.Ye.
Effect of high pressure on the elastic properties of
rock samples
collected along the outline of the area of deep
seismic sounding
in northern Karelia. Izv. AN SSSR. Fiz. zem.
nc.1:109-115 165.
(MIRA 18:5)
1. institut fiziki Zemli AN SSSR.
"AUY 11,
WD W.j i N. BAYI)K$ A
wavtio 'n 1 and ga.A reservoirs
ze..-baijanw. high prL,.zs-m-es. All 'SZ:R 163 no-5t-131- 133
I Ag
(MIRA 1888)
'If.-Ititut V.,zlIk! 1"'wPit All' SSSR 1 Institut geo!3gii AN rbSSR.
Sulnttte3 Noemly~r 10,
ACC NRs AT6034505 S-Oul~CEFCODE-l.'"UR/0000/66/000/000/0064/0075
AUTHOR: Afans'yev, G. D.;_1M9j,_.YqtJ * Belikov, Bs P.; Borsuk, A.
He; Volstrovichs
t,s
'11. P,; Zalesskiy, A. V.; Pavlogradskiy, V. A.; Sinyanov, I. Z.
ORG; none
TITLE: Preliminary data obtained by correlating physical
properties of rocks from
;Northern Caucasus with geological and geophysical data
7
SOURCE: AN SSSR. Otdolenlys nauk o Zemle. Nauchnyy sovat po
'Aomplakenym issladovant-
yam zemnoy kory i verkhney mantii. Clubinnoye stroyeniye Kavkaza
(Abyssal structure
of the Caucasus). Moscow, Izd-vo Nauka, 1966, 64-75
TOPIC TAGS: Reophysics, seismic prospecting, petrology,
stratigraphy,
/Caucasus
ABSTRACT: The most important of the different age associations of
igneous rocks in
some of the structural zones of Northern Caucasus (the piedmont
region, the foot-
hills, the transverse depression zone, the granitoid zone and the
axial zone of the
Major Caucasus ridge) are described. The post-Selurian,
posi;-Lower Carbonaceous,
pre-Triassic, post-Lower Jurassic, pre-Middle Cretaccoxis and
~;enozoic formations are
described. The magmatic geology of Northern Caucasus is compared
with geophysical
data. A new scheme is suggested for the deep structure of the
territory. The
ancient basement is shown to consist of Hercynian and older
formations. In
-Card 1/2
ACC NR: AT6034565-
particular, a substage of lower Hiddle Paleozoic formations is
differentiated. It
differs greatlyin respect to its physicaLl properties from younger
rocks of Upper
PaleozDic and Mesozoic ages. In the region of the Major Caucasus
this substratum has
been completely reworked by upper Paleozoic granitic intrusions.
Tht ancient rocks
outcrop in a few areas; however, to the East the Caledonian
basement is covered by
Mesozoic and possibly Upper Paleozoic formations. It is believed
that the deep
seismic sounding conducted near Ellkholovo has located the buried
extension of the
Caledonia structure of the Western Caucasian foothills. Orig. art.
has: 6 figures
and I table.
SUB CODE: 08/ SUBH DATS: 26Feb661' ORIG REF: 020/ OTH REF: 001
BAmov, i,
Fadtory Managemant
Efforts of the wipply divisiss Of A Plant to economize wAterials.
Za ekoz.mat.
No. 2, 1952.
MS!Ihly List of Russi&A Accessions, Library of %;osgress,
December 1952. Unclassified.
EA;;-VaH A*.;L
To
- ---- -------
L 8603-66 E~tr(l)/EtIT(m)/EIIP(tll/E.~IP(b) IJP(c) JD
ACOMION RRi AP,9Drft.1171 'UR/0339/65/000/ock/0076 1
AMCR1 henko M. A,
TITM Determination of the tempero4ure dependence of the
first'constant of the
zagnetlp crystallogmphic wdsotrW an polycrystalline litbivm-alumimna
ferrites
SOMM V M. ritikap no. ho 20% 7641
TAGS# taTeraft" dependence, xNmetic ~"~s rgM ferriter lithium con-
tain' alloy., aluminum containing &1lay). magnetic ofiturationj,
magnetic suseept-
Ibility
ABI37RACT: Experimental results we presented of measurements of. the
temperature
dependence 0 the first constant cof wAgnetic crystaUogrspbic
anisotropy (k3L in
a series of polyorystallfte ferritea Lio.OY*2.5_&Al&04L, wbere a -
Oj 0.21, 0.11P 095P
amd 0.6. 2he measurements won wAde by the method of approach to
saturation In the
temperature Interval from 170 to "QKj, in a pulsating mgnetic Meld.
7he tests
Nor madeAna cQwbIAW4Q-&3A-ac-(2500 -cps) -flelde --- 7he -results
abow tbat-in--
fielde 1000-2000 oe the diffe"Aftel susceptibility can be described
by the ex- f
preselcm R a A/RF + B/91 + C/H' (As B.. 0 constantsp H magnetic
field intensity)
and tbat the teopmUre dependence of k.% Is in satlsfactai7
quantitative agreement
Crd 3/2
,I ~- Card 42
66 ~J%~) -J-D M JO
M0
AM NRs APS004469
9: Ult/0048/66/030/0 06ii7/(KH;7
AIMEOR: .1styakov. N.S,.--: Rusov, 0.1.
ORG: I MYSICS Institute of -the Siberian Mellon-of -the S�SR Academy
of kelp-nces
(Inatitut-fiziki Sibirskogo otdolonlya,Akadeali nt4jk SSSR)
TITW: Forronalnetic resonance In multilayer film systems
(Transactions of the
Pecond All-UnIon SMalum on the Physics of Thin Forromwetto 11169 hold
at Irkutsk
110 JUIT. to. 15 JU1Y 19") A
SOUM: AN SSSR, Izventlya, Sorlya Micheakaya,v. 30, no. 1, 1966, 64-67
TOPIC TAM forromagnatIc film, mAgnotic thin film, Iron nickel allay,
cobalt, so2y-
bdonum, quartz, laminated nater1r.1,forronagnotic roxonance,superhigh
frequency`
ABSTRACT: The authors have Investigated the ferromagnetic resonanc 'e
at 9 MR& of thin
for r.-,**p*t1c Olus and vu t4loyer film systems consisting of alto''
to layers offj!=w
'"o
% S~e-,films were Vacuum evaporated at 10 0000
yaglLellS *11=4~knd guar -qmm ag in a I
The -
magnetic floldlat the rate of40 pa onto glass substrates heated to
200C#
forromagaietic. resonancii a6morptiou: iiief neas'urod"In a
rectangular citvity., resonator ex-
cited in the T,Zit'A iode'an-A having a.Q factor of 1000. The
7-ma-diasister
circular films,-fa-stmed to the end of a brass rod, were Introduced
Into the resonator
,through a 7 so d1aneter bole In the 4md wall. The resonator was
tuned with a teflon
rod inserted through a hole In the side walle The magnetic field was.
modulated at
Card 1/3
L 274201-46
ACC MRs AP6004469
435 Rz'w1th 6--speclal windIng &?Ad Wang1ven a saw-tooth form by
varying the current in
the main windit*. - The resonance curva.s. w.erc_dIspIa?ed on. an
oscilloscope or.recor
with inr uIll1voltmeter. .Slngle-6Uyer films of composItion
16Fe-_79_X_i-_3Mo,1=dS_
17F(TrONWoWt~Ickness from 400. to 2000 A were investigated. For the
No-coutainin g
f i-las Igo- rZonant vu4MetIc f Ield decrtased with Increasing
thickness from 1214 Oe fwr
a 400 1 film to 818 Oe for a 20001 film and the width of the
resonance ranged between
33 and 47 Oe. This small width of the resonance absorption line In
favorable for.
practical applications. Data are veported on only tbree Co-containing
;Ilms. Of these,,
Ithe thickest (2000 1) showed two absorption peaks separated by
60-80-00. No explanatiom
for this in offered. A 6oo A film had a 34 Oe wide absorption line at
886 Os and a
film of unspecified thickness 'between 1000 and 20M, A had a
38-Oo-wide absorption line
at 861 Oe. Multilayer film systems having up to 10 layers were
Investigated. In these
systems the metal films were approximately 2000 .4 thick and the
intervening quartz
films w-..re from 2500 to 2000 .4 thick. As the nVaber of layers was
increased the ab-
sorption line became deeper and wider and began to evince complex
structure. -A ten-
layer system clearly showed four resonance peaks separated by 60-80
Oe. 7bis behavior
fie ascribed partly to dipole-dlp~ple interaction between.
neighboring layers,,as Bug-
ly to.
gested by D.Chen and A,H.Morrish (J. Appl. Phys., Suppl., 33 N 3
(1962)), and part
the influence of the conditions of deposition. It was found that if
thevacuum was
broken between deposition of metal and deposition of quartz the
structure of the Mb-
vorption curve of the resulting multilayer system was considerably
different from.that
of a system which wai deposited vithout breakift the vaculim.
Auxiliary %xporlmeuts
with single-layer 20P*-SONi and 3(Wo-45HI-25Co films with and without
quart;.
L 1?410-66
ICC NRs OW4469
showed that the Presence of the quartz considerably reduced the
strength
of the resonant fiold and increased Ch* width of the reaonance~ Tb* J
resonance lines of two-layor systems with quarts between the layers
occurred at approximately th* same fleld,Atr*ng~b and were-of
approximately
the same width'-as those of the corresponding single films witb qnartz
coverings..
SUB 00'D3-, 20/
ATb PRESS% 426o
iA -A
-L-24 8-66 VTM/EW(2 ~/VPO)
7
ACC MAt APbOL4256 SOURCE.C.'. CODEF UR101091667011700510930/DiF31
AUTHORt -Chistyakov# Nd Sq; -Ignatchanko# Ve As; B&Zgkov, 0* Agj
kV3oV&6 So G 0
ORGI none
TITLEt Certain UH? properties of multilayer
SOURM Radiotekhnika-L.elaktronika, V. 116, no 5~j 19669 950-951
TOPIC TAGSs magnetic,'thlh film
ABSTRACT: Tranimismi"' A'ad reflectioll factors of single-layer and
oultilayer v2agnstLc*fLltd6 were measured in a waveguide system
operating
at I - 3 cm. Individual films were made by sputtering l7Fe8ONL3Ho
alloy on a SlAss substrate heated to 200C in a vacuum of 10-5 mm Ug
and in a magnetic field of ev 100 oe.: Multilayer films were made by
insulating.eath filta layer by.a layer of SiO 1000 A thick. Experi-
mental data (see Fig.,I) shows that the transmission factors for
Multi-
layer films (point 1-10 layers, 1000 1 each; point 2-40 layers,
500 each) substantially exceeds the same factor for- a single layer
~_104 filM (solid line) By breaking the film into layers, but
keeping the same total-thickness$ skin depth is increasede This feet
was substantiated by'switebing the films ia'a-cavity resonator and,
L-card I 12 VDCI: 539.216.22:621&3184
noting the resonator frequency shift. The shift for multLlayer films-
is greater than that for equivalent single-layer film and shift
linearity is preserved-up,to total film thickness of.3 k 104 (30
layers 10,00 each) a- 'OrLgi arto hast 2- figures#, JBDJ.
SUB CODEs 09/ 'SUBH 'DATIEs IIAP'r65/ ORIG REP 1005/ ATD PRESS:
ar
C
d
- . ~- ~& 1;&A . ---
Investigation of enargy azd anL-ular -fistributims 02
jr"-mesonz produced by protons with energies of 470
and &SO VeV (11/50)
C.~~,-,U'T-,Symposiiri oil High EnerGy Acceleratom and
Pion
Physics.
Geneva 11-23 June 56
1n. Brancb #5
rwr.c
01-
KY
7
1
-
-
slam
--et!rA
'T L
NzL'I gin,!~m ~n
51
OAYOKO~
ALM HOR
BAJUKOV, J.D., 00ANESAN, J.C., NAPKIN, A.4. PA 203 8
TITLE
The $,bsorption of y-Quanta with the j&verage Energy of 500
MeVin
Lead
, and Aluminium. (Russian)
Copper
PERIODICAL
,
.
Zhurnal Eksperimentallnol I Tooret. Fiziki, 1957, Vol 32, Nr 1
PP
183-183 (U.S.S.R.)
Received 3/1957 Reviewed 3/1957
ABSTRACT
y-Vanta
originate from the decay of neutral pions which were produced
in
the inner target of a phasotron by 660 MeV protons. These Y-quanta
were recorded by a pair-like y-apectrometer with 12 channels, on
which
occasion the spectrometer was at a distance of 23 m from the
target. Be-
fore the collimator, which was fitted behind a
protective wall of 4 m
thickness, a device was arranged, by which
the bundle of y-quanta was
periodically interrupted by means of a
lead absorber. The y-quanta record-
ed by the spectrometer in the
case of fully covered and not fully opened
bundles were counted
separately.
For the determination of the coefficients of the
absorption of the y-quan-
ta in Cu and Al the semicircular lead
disk in the rotating device was re-
placed by absorbers of copper
and aluminium. The frequent change of ab-
sorber3 made it possible
to carry out measurements without a monitor and
to diminish the
number of measuring errors. The bundle of y-quanta passing
through
the collimator was purified from electrons and positrons by means
of a special magnet. The authors obtained the following values (
in cm*/g)
for the coefficients of the absorption of y-quanta with
the energy of
- 500 150 Mev:
3
Card 113
y
PA - 2038
The Absorption of y-Quanta with the kyerage Energy of 500 MeV in
Lead, Copper, and Aluminium.
Pb 0,1115 1 0,0025, Cu 0,0510 1 0,0025, Al 0,0295 � 0,0017.
The absorption of the y-quanta at Ey - 500 MOV takes-place
essentially by
the production of electron-positron'pairs. As shown by
computation results,
absorption by photo effect and Compton effect amounts to -, 1,2
O/o in
the case of Cu, and to -. 2 O/o of the total absorption cross
section ir
the case of Al.. The cross sections for the absorption of
y-quanta found
here agree w93.1 with the computed results obtained bf H. DAVIES,
H.BM,
L.MaIMON, Phys.Rev., 93, 788 (1954).
It remains to be added that the data for 500 MeV y-quanta which
agree with
computation-e were obtained in the case of permanent pre,,tence
of a lead
absorber of 5,55 g/cma thickness in the bundle. If suche'a lead
absorber,
by wbich the bundle-is filtered, is lacking, cross sections which
are
larger by 10 0/0 SA obtained. When measuring 41-he absorption
cross section
of 2~O MeV y-quanta, no influence was found to be exercised by
the additio-
nal absorber by which the bundle is permanently covered. The
cross section
of the absorption of 280 MeV y_cpanta obtained here agrees with
the re-
sults obtained by J.W.DE-WME, A.ASKIN, L.A.BACH, Phys.Rev., 83,
505
(1951). The reason for the increase of the absorption cross
section of
500 MeV y-quanta when an additional. lead filter was lacking
could not be
explained.
Card 2/10
PA - 2038
The Absorption of y-Quanta with the Average Inergy of 500 Hev
in L ead , Copper, and Aluminium.
ASSOCIATION United Institute for Nuclear Research, Laboratory
for Nuclear Problor-:.
HWENTED BY
SUBMITTED
AVAILABLE Library of Congress
Card 3/3
AUTROR
--BAYUKOVI 7r# Dot SINLYEV A.N.r TYLPKIN A.A. PA - 2699
.
TITLE
Experim-entid-Compari son of the Energy Spectra of
3-Quanta
resulting fron th* Decay of Neutral Pions (which were
created
by 660 MoV-Protons 911 Carbon- and Lead-Nuolei).
(Eksperimoutall-noye sravn*niye suerastiabookikh op*ktrov
kv&ntoy ot xispada x - mozonov, abrazovannykh na yadrakh
ugleroda i ovintsa. protonami a onergiyey 660 MoV. Russian.)
PZRIODICAL
Zhurnal Eksperim, i Toorot. Piziki 1957, Vol 32, Nr
29
PP 385 - 386 (USSR).
Received: 5/1957 Reviewed: 6AM
ABSTRACT
Yor a more exact comparis n of 2-quants created on light &Ad
heavy nuclei the authors :arried out relative measurements of
the
fluxe of quanta within the various domains of the spectra
t
menti:n*d a
vee
The angle of observation in the direction of notion of the
protons amounted to 0 . Measurements were carried out by means
of a magnetic dcuble spetatrometer with 12 channels, The
targets
consisting of lead and graphite fitted Anto the vacuum
chamber
of the accelerator were-txoh d very minute.
At low
energies of j- qu
t& E < TO Nov) a difference is
-
noticed on the 41--q to i tod3n oarbou and lead, This dif-
forono* in connected ap W ontly with the modification of the
angular distribution of the neutral pions.
CARD 1/2
PA - 2699
Experimental Comparison of the Energy 'Spectra of a -quanta
resulting from the Decay of Neutral Pious (which were created by
660 WeV-Protens on Carbon- aud Lead-Nuclei).
This modification in due to the interaction of the bombarding
protons with the nucleons of tb* nucleus on the occasion of
strong abserptiol of mesons. The hard I.- quanta with the angla
of observation 0 are essentially created on the occasion of the
decay of these neutral pious which are created on that side of
the
nucleus which Is averted from the bombarding protons and in
heavely screened off 'by the remaining nucleons of the nucleus,
The soft quanta, however, are essentially created on the
surface J thoLnUoleUe which in exposed to the protons* There-
ferev a relative increase of soft 3-quanta in the spectrum
is observed on the occasion of tLe creation ef neutral pions
on heavy nuclei.
Considerable differences are to be expected also in the energy
distributions of the mesons created on light and heavy nucleie
The energy,%stributions of the neutral pions created under aa
angle of 0 n carbtn-~ and lead-nuolsi do not differ noticeably.
Possibilities for a more oleo& study of these pion spectra are
shown. (I table)
ASSOCIATION: United Institute for Nuclear Research
PRESIM29D BY: -
SUMTM: 2. 11. 1956.
AVAILARM: Library of Cougr*nne
CAN 2/2
AUTHOR BAYUKOV, Yu.D., KOWDATIT, U.S., Tr.AFK'IN,, A.A. 56-4-5/52
TITUS TI% investigation of the rsnergetic and Angular
Distribution of v*eaon3
Formeo,On Carbon Nuclei by Protons With An Y-nergy of 47o and 66o
NeV.
(Issledovanip anergetichaskikn i uglovykn rasprodelaniy
ff*ezonov,obrazo-
vannykh na yadrakft -iglaroda protonami 3 awrgLYW470 i 66o MeV
-Russian)
PsKIODIGAL Zhurnal Eksperim.i. T*oret,FWki,l957,,Vo1 32,,Nr 4,pp
667-67i(b-ts-s-R.)
Received 7/1957 Reviewed 0/1957
ABsTRACT The results obtained by tne Investigation of energetic
spectra on the oc-
casion of tne decay of iyll-mesons produced on carbon nu.clei by
protons
with the energy of 66o WeV 13 discussed.The method of spectral
analysis
was u3sa.The neutral moacne have a very short life(5,,lo-15 see.).
The experimental scheme is shown in form of an illwtratior.The
carbon tar-
get is inside the vacuum chamber of the accelorator and waj-
irradiated with
protons of the average enrgy of 66o MeV. The y-quanta formed in
the 'target
penetrated through an opening into a concrete wall or 4 a
thickness and
collimated through a diaphragm -4jito a lead block.The collimated
bundle or
y-quanta.,wnich was purified from charged particles by the
magnetic field
of a special clectromagnot,ponetrated into the converter of the
12-cnannal-
led pair-spectromfiter.The apectrometer was set up at a distance
of 23 m
from the target in the direction of the tangent to the orbit of
the protons.
The author beer* gives a doWlea description of the pair
spectrometer used,
The differential cress section for the production of y-quanta on
the carbon
nuclei by protons with an energy of 66o MtV for 18L' in the
laboratory sy-
ca rd 113 stem amounts to d8 Z/a&)(l8o")-(l-5+ op2).io-87
=4/sterad. The ratio of
The Investigation of the Energetic and Angular Distrioution
56-4-5/52
Of AISSOW Formed On Carbon Nuclei by Yrotons Witn An k;nergy of
47o
and 66o Rev..
the flux of Y-quanta under the angles 0 and 1do" is equal to
5sl+Ux3*
The energy spectra of the y-quanta is tnan analyzed.
l.Dependence of the spectrum on the angular- and energotic
distribution of
tne"*osons.It follows that with the isotropic distribution of
the wu-me-
sons,indapandent of their energy distrioution,tne spectrum of
the y-quan-
ta is or symmetric shape with respect to the energy 1/2F_,,.
2.Uompari3on of tn* energy spectra of y-quanta on tne occasion
or tne de-
cay of if'-semons produced by protons with the energy of 470 Uev
on tne nuc-
lei of beryllium.Mustration 5 shows that tho energy spectrum of
the y~
quanta of the decay of mesons pr~)duced by photons with the
energy of 470
90(center of mass system) on the nu,)loi o.' caroon.At a proton
energy of
470 NOV energies are produced,whicn. tire an a proximation to
tne maximum
possible energy attainable oy the meson in tne reaction.Witn an
energy or
66o NO of tne proton3,me3onB with considerably lower energies
are formed
than is possible as a maximum,
3.Snergy spectra of e-zesons produced ay protons with the energy
of 770
and 66o W.Mustration 7 shows the energy distribution of
wll-aesors in
the center of mass sy3te:.& for --arbon3 oy protons with the
energy of 4?o
MeV.0n the same illustration it shows the spectrum of
ffO-me3ons.The energy-
and angular distriuution ol 0- mesonawhich had been measured at
a proton
energy of lejo M9V shows that the nesons produced in this case
which are
neutral on the occasion of the collision of nucloons,absorb the
greatest
Card 2/3 pan of the free energy of the collisiton., as well as
Aso the greatest an-
A
The Investigation of the Energetic and Angular Distribution
564-5/7~2
v4-Xesons
of
Formed On Carbon Nuclei by Protons With An Energy of 47o
and 66o iiev.
gular momentum.Tne same phenomenon is observed in the case of
lower pro-
ton energiesoAt proton energies of 470 Moll the spectra of
ffu-,mssow pro-
ducect on composed nuclei dixfor only slightly from spectra
computed on the
assumption that mesons are produced only with maximum energies,
so that at
a proton energy of 66o M*V a considerable dirference between tne
spectra
ootainea and those ccmputed at the same conditions is ObServeci.
At a proton energy of 66o M*V ti4-maons with an energy that, is
consideraD-
ly lower than that which is possible as a maximum are mostly
produced.Con-
sequently it follows that in the case of tne production of mesons
by tho
proton energy of 66o MeV tne nucleons in tne final state acquire
a high
kinetic energy andstherefore0al3o high momenta.Witn an increase
or proton
energy fromWo to 66o X*V the anplar distribution of the
ffl-mosons chan-
ges considerably.
ASUOCIATION United ln3tituts for Nuclear Research
FRESM39D BI
bUBKITTMD 28.1o.1956
AVAILMz Library of Congress
Card 3/3
AUTHM
Xu.DU TYAPKINp AsAss
BAYUKQVj
TITIZ
_
The Energy Spectrum of y-quanta of the Decaying ,O-Meson Created by
the
Interaction of 660 MeV protons with Hydrogen Nuclei
(Energsticheskiy spi:ktr y-imantov ot rasp&" YO-mezonov,
obraz3vannykh
protonami a energ4v 660 MOV n& ya&Wdi vodoroda.
Russian),
PatIODICAL
Zhurne Eksperim, i Tooret, Fiziki, 1957, Vol 320
Nr 5; PP 953 - 956
(U.S.S.R.)
ABSTR&CT
The y-quants, were measured
with the help of a scintillation telescopet
on which occasion the
production of vo-msons took place in such a man-
ner that two
targets one of polyten and one of carbon, were one after
the other
exposed to the inner of the phasobron. Besides, a number of
double
targets was alterningly irradiated in such a manner that., simul-
tansously with the change of targetj also the y-counting device
could
be adjusted to this pair of targets*
The angular distribution
of One w0-mesons created by the collision of
660 May protons with
H-nbclei has t1w form
I + (Os3 + Oal) Coll 0
The wo-masons spectrum
h;8 a marked maximuoi at $v 75 MOV,
Furthermore it was established
experimentally that the angular distri-
Card 1/2
bution of the
vfO-meaona created by p-p interaction is isotropic,
56-5-1/55
The Energy Spectrum of y-quanta of the Decaying wO-Xeson Created
by the
Intaraction of 660 NO protons with Hydropr Nuclei
ASSOCIATIOW United Institute for Nuclear Research
HWENTED Br
SUBMITTED
AVAILABL9 Library of Congress
Card 2/2
SOV/120-58-6-4/32
"AUTHORS: u Kozodayev, M. S., Markov, A. A., Sinayev,
A. N.9 in, A. AO
TITLE: A Multichannel 3~air y-Spectromiter. 1. Calculation of the
Main Characteristics of the y-Spectrometer (Mnogokanallnyy
parnyy gamma-spektrometr. I. Raschet osnovnykh kharakteri-
stik-gamma-spektrometra)
FERIODICAL: Pribory i takhaika eksperimenta, 1958,, Nr 6, pp 23-29
(USSR)
ABSTRACT: la a pair y-spectrometer the energy of the quanta is de-
termined by measuring the total energy of the courponents of
the electron-positron pair formed in a thin converter. The
first 2-chaimel pair spectrometer was built by Dzhelepov
(Ref4). Later spectrometers built on this principle were
widely used in measuring the s
.pactra of hard y-rays (ReLfs.2
to 8). The electron and the positron leaving the converter
were deflected by a magaetie field in different directions
and for certain values of their energy they enter ionisation
counters connected in coincidence. For a given intensity of
the magnetic field and a fixed position of the counters, such
a spectrometer will record a fraction of the pairs produced
by y-rVs in a given energy range. In a simple 2-channel
Card 1/6 spectrometer In which one channel records the electrons
and
SOY/120-58-6-4/32
A Multichannel Pair y~spectrometer. I. Calculation of the Main
Characteristics of the y-spectrometer
the other the positrons, an increase ia the accuracy of
measurement is associated with a marked decrease in the
efficiency. Good energy resolution and high efficiency can
only be s:Lmultaraeously achieved in a multioban-nel
meter. In such a spaatrometer the efficiency may be inez~eased
by a factor r_jn2 without loss of resolution-,, where z~, and
n are the numbers of eleatron and positron counters. I-,
sich a spectrometer se'veral energy intervals may be i
at the same time. A number of suoh multichannel spect::~:-,.
meters have been described (Refs.5, 6 and 8). The
of a y-speetrometer as a measuring instrument is diAe3, ~,,
~.nf-d
by its effioienoy an& spoetral sensitivity. In
multichannel system it is necessary to take into aeoox
characteristics for the various pairs of channels of the
spectrum. In this connection, a discussion is given In the
present paper of the dependence of the efficiency and spec-
tral sensitivity of the separate pairs of channels on various
Card 2/6
SOV/120-58-6-4/32
A Maltichannel Fair y-spectrometer, 1, Calculation of the Main
Characteristics of the y-speetrometer
parameters of the spectrometer:
1) Spectral sensitivit-V: the basic diagram of a y-speetro-
meter considered in M paper is shown in Fig.l. in whieb
the meanings of the symbols employed are indicated. In view
of the finite width of the counters, the spectrometer records
y-quanta in a certain energy interval from E y min to
RY max . The corresponding spectral sensitivity curve is
then shown in Fig.2a and is of triangular form with a dis-
persion given by
1/6 L2/(r, * r 2 )? where 1-0 is the width of a
61
0
coUnter and ri and r2 are the distances from the con-
verter to the oentres of the counters, respeetively. The
effect of the width of the converter upon the spectral
sensitivity is examined and it is shown that a converter of
a finite width introduces a spread into the spectral line
in the high energy region of y-quanta. As the angle 9
between the di--nection of motion of the y-quanta. and the
Card 3/6 straight line connecting the centre of the converter with
SOV/120-58-6-4/32
A Multichannel Pair y-spectrometer. I. Calculation of the Main
Characteristics of the y-spectrometer
the counter increases, the spread of the spectral line de-
creases. At (p - 900 the width of the !:,-ectral serisitivity
curve is independent of the converter width. The effect of
the converter width gives a distribiCoion of tiNe form shown
in Fig.2b, which has a dispersion given by:
4- 4
2 GOtg (P
2 2
180r1 'rP
The effect of multiple
scattering in the converter is estimated and expression._-
are derived for this effect also. Finally,, an estimate ie
given for the radiation loss experienced by the electron-
positron pair on traversing the converter,
2) Efficiency; in this section the Bethe-Heitler expression
for the probability of formation of a pair by a y-quantum, of
Card 4/6
SOV/120-53-6-4/32
A Multichannel Fair y-spectrometer. I. Calculation of the Main
Characteristics of the y-spectrometer
energy E is used (Ref.13) with a modification described
b Bethe Yet al in Ref.22.
3~ Multichannel system: in a multichannel spectr6seter the
electrons and positrons formed by y-quanta of a given energy
are recorded by a number of combinations,of pairs of counters.
The electronic circuit of such a spectrometer Aduld rdeord
coincidences between pulses from each eleetron counter with
pulses from any positron counter. Thus, any combination of
one electr6m:counter and one positron counter is, in fact, a
2-channel spectrometer. For a given geometry a spectrometer
containing n channels records y-quanta in n-1 energy in-
firvals of different mean energy. In practice, one seeks to
find the form of the spectrum and the absolute intensJt7 in
dne of the energy intervals. To find the form of the spec-
trum it is sufficient to know the relative efficiency of
recording for the different energy intervals, and this is
given by Eq.(10). In order to obtain the absolute intensity
in one of the energy intervals it is necessary to know the
total absolute efficiency of recording of y-quanta in one
of the energy intervals. "Ohis problem is not treated.
Card 5/6
SOV/120-58-6-4/32
A Multichannel Fair y-spectrometor. I. Calculation of the Main
Characteristics of the y-spectrometer
V. V. Mellnikov is thanked for carrying out a number of
calculations. There are 2 figures and 22 references, of
which 4 are Soviet, 1 German 1 Soviet translated from
English and the rest are Engiish.
ASSOCIATION: OVyedinennyy institut yadernvkh issledovaniy
(United Institute for Nuclear Studies)
SUBMITTED: December 27, 1957.
Card 6/6
SOV/120-58-6-5/32
AUT ov Yu. D . Kozodayev, M. S., Markov, A. A. Sinayev, A.N.,
Tyapkin,
TITLE: A Multichannel Fair y-Spectrometer. II. Description of a
12-channel Spectrometer (Unogokanalln,7y parnyy gamma-spek-
trometr. II. Opisaniyi dvenadtsatil-anallnogo spektrometra)
PERIODICAL: Pribory i tekhnika eksperimenta, 1958, Nr 6, pp
30-40
(USSR)
ABSTRACT: Application of a multichannel pair spectrometer in
synchro-
cyclotron work presents a number of specific requirements as
far as counters of the ionising particles and the electronic
system of the spectrometer are concerned. Since the beam
intensity is high and consists of short pulses of 200 to
300 lis each at a repetition frequency of 40 to 80 pulses per
see it follows that the apparatus must be very fast. ..It is
desirable that the input blocks should have resolving times
not greater than 1 lis. The large background intensity in
synchro-eyelotron work means that it is always necessary to
use a special selection system which records only electron-
positron pairs. 'For this raason, in the spectrometer each
component of a pair should be recorded by a number of counters
in coincidence with sufficiently low resolving time. The
Card 1/7 present paper describes a 12-channel y-spectrometer
which has
SOV/120-58-6-5/32
A Multichannel Pair r-Speetrometer. II. Description of a
12-channal
Spectrometer
been used over a number of years in studying the spectra of
hard y-rays and neutral Ir-meson decays (Refs .2-6). The
first variant of the spectrometer was built in lc)49. In 1951
and 1954 the spectrometer was modified to improve its --harac-
teristics. The spectrometer described here satisfies com-
pletely the above requirements and is based on the design
calculations given in the previous paper (Ref.1) in th--'-s
issue.
1) Magnetic ustem and Reometa of the instrument.
The magnetic field is produced by an SP-56 electromagneT,.
Fig.1 shows the disposition of the counters for two ty-lies ot
demountable pole pieces. The gap between the poles ia _~_- o~,-
and the maximum field in the gap is 18 000 oersted. Tite
electromagnet current is stabilised to 0.1%. In studies of
~;ray s~e tra, in the energy region 20 to 200 MeV, 29 = JL800
iglb Zd in the energy region 100 to 450 MeV, 2(p - 900
Fig.la In thG former case semi-circular focussing of
Card 2/7
SOV/120-58-6-5/32
A Maltichannel Pair y-Spectrometer. II. Description of a
12-channel
Spectrometer
electrons and positrons was used, and this led to increased
efficiency (Ref.1) because it was posRible to use wider and
thicker converters. For y-quqnta in the energy range 450-
600 MeV, 2v - 900 but the counters were at a larger distance
from the converter. Copper converters were used (0.1. 0.3
and 0.5 mm, depending on the energy).
2) Resolving power and efficiency.
Fig.2 shows curves of the total spectral sensitivity for the
7th energy interval for various values of E YO and thick-
nesses Tk of the copper converters. These curves are based
on the theoretical data given in the previous paper and are
obtained by a statistical combination of the partial distri-
butions due to a) width of the counters, b) width of the con-
verter, c) multiple scattering and d) radiation. As can be
seen, the form of the total spectral sensitivity curve is
VexV nearly triangular which means that the total spectral
sensitivit7.is governeA mainly by the width of the channels
t. (see Fig.1 of previous paper, p 24, this issue).
Card 3/7
SOV/120-58-6-5/32
A Multichannel Pair y-Spectrometer. II. Description of a
12-channel
Spectrometer
3) Counters and selection system. The counters used were
proportional counters having a Fylindrical stainless steel
cathode, 10 mm in diameter and a molybdenum filament 0.1 mm
in diameter. They were filled with (CH2(OCH3)2) at a
pressure of 160 to 200 mm. The working voltage was 1600 to
2000 V. Th~ counters have an effective dead time not ex-
ceeding 10 see. The efficieney of the counters for par-
ticles with relativistic ionisation reaches 918% in a coin-
eidence scheme with a resolving time of 5 x l&-7 see. The
delay of the pulses due to dri;(t of electrons through the
coun-ter San is less than 10-Y. The counters give. electri-
cail pulses with amplitudes between 10-4 and 1 V. The large
difference in the amplitudea requires the use of amplifiers
having a wide dynamic range and an amplification of a few
thousands. 6-fold coincidences were used and the number of
random coincidences in each 6-fold channel was 0.02 pulses
per see. The number of eleetron-positron pairs recorded per
Card 4/7
SOV/120-58-6-5/32
A Multichannel Pair y-Speetrometer. II. Description d a
12-channel
Spectrometer
sec depended on the efficiency of the spectrometer with
respect to the y-quanta in the measured energy interval and
the form of the spectrum and was in the range 0.1 to 10 pairs
per see.
4) Bleetronio scheme.
A block diagram or the electronic part of the spectrometer is
shown in Fig.3. Tts) left-hand portion of this diagren shows
6 co-ordinate counters of the electron series (a, - ad, 6
co-ordinate counters of the positron series (Bi - 3.) and
4 selection counters (All, AnI V and 'U"). Each of these
counters in practice consists of a gr,)up of counters whose
filaments are connected. A recorded electron or positron
should pass through 3 counters (1 co-ordinate and 2 selection
counters). A pair is recorded if a 6-fold'coincidence-takes
place. Negative-going pulses from each counter are ampli-
fied by a corresponding amplifier-converter (Fig.4). These
amplifiers have a rise time of 2 x 10-4 see. Pulses from
all the 16 amplifier-converters are applied to the main block
which is at a distance of 1.5 m from the amplifier-converters
Card 5/7 (Fig-5). Pulses from the selection counters are
applied to a
SOV/120-58-6-5/32
A Multichannel Pair y--Spectrometer. II. Description of a
12-channel
Spectrometer
4-fold coincidence scheme while pulses from the co-ordinate
counters are applied to mixers and in addition through.delay
lines to a hodoseopic system consisting of 2-fold coincidence
circuits and output uftivibrators. The pulse at,the output
of a mixer appears in the presence of a pulse in at least one
of the co-ordinate counters of a givenseries. Pulses from
both the mixers and also from the 4-fold coincidence scheme
are applied to a 3-fold coincidence scheme which produces the
final output pulse. It follows that the latter pulse appears
when a 6-fold coincidence takes pl4c6,1.4p.when a particle
passes through at ledst one of the co-ordinate dountera in
the electron series, through one of th) co-ordinate couaters,
of the positron series, and all the counters of the se'Leetion
system. The resolving time of the above coincidence schemes
is 5 x 1o-7.
5) Method of measurement and treatment of results.
Fig-7 shows the experimental 4trrangement. In Ws figure 1
is the proton trajectory, 2 is the target, 3 is the synchro-
cyclotron chamberl 4 is a concrete wall, 5 is a collimator,
Card 6/7
SOV/120--L58-6-5/32
Multichannel Fair y-Spectrometer. II. Description of a
12-channel
Spectrometer
6 is a diaphragm 7 is a clearing magnet which removes
electrons and positrons from the beam, 8 is an additional
screen, 9 is the convertor and 10 is the spectrometer
electro. magnet. Pig.8-shows a typical result obtained for
the energy spectrum of y-quanta from neutral V-meson decays.
The mesons were produced by 660 MeV protons at a carbon target.
The spectra are measured at an angle of 180-00 to the direct-
ion of motion of the protons. G.F.Zorin, B.A.Erasnovidov,L.
A.Fadeyev and G.N.Stepanov are than ed for their assistance.
There are 8 figures, 4 tables and 7 Soviet references.
ASSOCIATION: Ob'yedinennyy institut yadernvkh IssledovaniY
(United
Ifttitute for Nuclear Studies)
SUBMITTED: December 27, 1957.
Card 7/7
85699
3/0~6 ;0/038/006/042/049/XX
BOO 7B070
24~ 4 op 0/0, /M/ /M)
AUTHORS: Bayukov, Yu. D., Leksin, G. A.
TITLE: The Possibility of Using Nuclear Reactions to Obtain Data
on in Interaction
PERIODICIL: Zhurnal eksperimentaltnoy i teoreticheskoy fiziki, 1960,
Vol. 38, No. 6, pp. 1907 - 1908
TEXT: Nuclear processes are considered in which transferred momenta
are
small also for large energies, and from whose theoretical
interpretation
it is possible to obtain data on it, xK, and KK interactions, as is
shown
here. This is shown for the process where a pion is produced by a
pion.
Use is made of the formula of Chow and Low which gives tho
relationship
between the cross 3ection for this process and the in interaction
cross
section for the case of small transferred momenta (Ref.1). It is shown
that this formula can be applied without much error for the
production of
a meson by a meson on a nucleus, and that it is thus possible to
obtain
data on in interaction from the total cross section for a nuclear
reac-
tion of the type x + A 4 x + % 4 B. This is true especially for the
Card 1/2
The Possibility of Using Nuclear Reactions
B/056j6O/O3e/Joo6/O4?/O49/XX
to Obtain Data on xx Interaction Boo6/BO7O
12 - - 12
reaction x + C 4 1 + X + N .Moreover, in momentum approximation?
the formula of Chew and Low must be multiplied by
00
S2 . f I tf (r)eipr f(r)dr)2before integration. This function
gives the
0
probability that the nucleus whose ground state is described by
the wave
function t(r) continues to remain in the ground state even when a
momentum p is transferred to it. As is shown in a diagram, S2
falls
rapidly with p. Only for p larger than 3 is this function
greater than
zero (for the case of the C12 nucleus considered here).
K.A.ftr-MMItos an
is thanked for advice ind help. There are 1 figure and 2
references:
I Soviet and 1 Us.
SUBMITTED: February 23, 1960
Card 2/2
27698
S/120/61/000/003/008/041
9032/13.14
AUTHORS: ._Rayukov, Yu.D., Leksin, G.A. and Suchkov, D.A.
TITLE: Characteristics of Spark Counters Operated-..~ylith,
Pulsed Supplies
PERIODICAL: Pribory I'tekhnika eksperimenta, 1961, No.,
pp. 66 - 68
TEXT: The authors have investigated the characteristics
of various spark counters operated with pulsed supplies. The
principle of the experiments is illustrated in Fig. 1. The
plane-parallel electrodes forming the spark gap were placed
in a glass container which was evacuated and then filled with
air, nitrogen, carbon dioxide, helium, neon and argon at
4arious pressures, p, respectively. The polished brass
2
electrodes were 55 x 55 mm in size. In addition, a further
4;ounter having dise electrodes, 30 mm in diameter and made from
aluminium foil 7 P thick, was tested In open air. The distance
between the electrodes was varied between 2 and 6 mm and the
Card 1/7
27698
S/120/61/000/003/008/041
Characteristics of .... F,032/93i4
high-voltage pulse wasderived from a -r(-K-1 400/116
(TGI-1 400/16) thyratron controlled by A telescope
consisting
nf- two scintillation counters C1 and C 2 0 The thyratron
pulse was delayed by 0-5 "ec relative to the passage of
the
particle through the counter. All the experiments were
carried out with coomic-ray particles. In some cases, a
constant clearing Voltage V 0 (0 to 2 kV) was applied to
the
counters-The limitivgxesixtor R 2 could be varied between
fractions of an ohm and 1*4 k-Q . The remaining
parameters are
indicated In Fig. 1. The spark discharges of ~he counter
were
recorded continuously, by ear, or by counting electrical
pulses
induced inthe antenna of a scaling unit. Rig. 2 shows the
results obtained for the efficiency R defined as the
ratio
of the recorded particles to the total number of
particles
passing through the counter (R2 = 0, Vo = 0, T,= 0.5
lisee)
Card 2/7
27698
S/12o/61/000/003/oWo4i
Characteristics of E032/9314
Fig- 3 shown typical efficiency curveb for various'
clearing voltages and high-voltage pulse delays, -C
The efficiency of a spark counter can be approximately
calculated from the formula
1 - exp -n (d - v PI
where n in the number of ion pairs produced in the
discharge gap,
v = Ke in-the charge drift velocity which depends on
the clearing field c = V0/d and the
mobility K
By comparing this formula with the results shown in Fig. 3,
one can estimate the mobilities of the charges i!I the spark
gap. For air at STP it is found that K 3- a cm /sec , while
for argon at p = 400 mm Hg K X 10 cm. /see.
Fig. 4 shows the efficiency as a function of the delay -r-
I
-inUsoc, for R2 = 0, V0 = 0 and d = 6 mm - Acknowledgments
to M.S. Kozodayev for discussions and interest in the work.
Card 3/7
27698
S/120/61/000/003/008/041
Characteristics of .... E032/E314
There are 4 figures, 3 tables and I non-Soviet reference.
SUBMITTED; juiy 4, ig6o
Fig. 1:
--t:: ~f-ikjW~AW .LPN.
_t I U===
BAIUKOWS U.D.; LMINs G.A.; SUCHKOV$. D.A.; SHAIAMOV.,
Ya.Ya.,* SHEBANOV, V.A.
--------
Backward elastic scattering of 2.8 bey/c %' -mesons on
neutrons.
Zhur.ekspA t#or.fiz. 1+1 n0-1352-55 Jl 161o (KML .14:7)
19 Latitut tooreticheakoy i ek8perimentalluoy fiziki AN
SWRo
(Mbsons-Scattering) (Neutrons)
Bk=OV. ; LMMIN.9 G.A.; SHAUMOV, Ya.Ya.
Elastic scattering of T- -Monona by 2o8 Bev./c noutrono.
Zhur.ekap.i teordis. 41 no-4:1025-1030 0 161. (MIM
.14:10)
1
1. Institut tooraticbeekoy i okoperimentallnoy fiziki
AN SSSR.
(Mooonso-Scattering) (Neutrons)
s/95Y61/041/006/019/054
B102 B138
AUTHORSi Bayukov, Yu. D., Leksin, G. A., Shalamov, Ya. Ya.
TITLIt Investigation of the react 'ion 7-+n--)ir+n+miP with a
beam of
mesons with a momentum of 2.8 Bev/0
PERIODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki,
v. 41,
no. 6(12), 1961, 1787-1792
NaT t The reaction *_+n -#1r+n+mirQ, m-1 t2 f was studied by
means of a 50 cm
long, 17-liter freon bubble chamber without magnetic field. The
bombard-
ing pions had a momentum of 2.8 + 0-3 Bev/o. The gamma quanta
arising in
I? decay were recorded with quit; high efficiency. From the
stereophoto-
graphs taken 221 single-pronged stars were selected,
representing pion
interactions with quasi-free neutrons. Only in two cases was KO
formation
recorded, so strange particle formation could be neglected in
evaluating
the results. The gamma and pion angular distributions were
meuured and
the multiplicity of the reaction was determined. Resultst In
the rN
o. m. 9. the angular gamma quantum distribution was anisotropic
and
Card 1/3
S/056J61/041/006/019/054
Investigation of the reaction ... B102/B138
asymmetric, the forward-to-baokward ratio was 1.76 + 0.30. In
the
laboratory system the angular r and e distributioni coincided
within the
limits of statistical error. The anisotropy in Ir angular
distribution
increased with the energy of the Tr" meson. The anisotropy in
gamma
distributions tended to decrease with increasing number of
gamma quantas
1-7+0-4 for stars with one quantum, 1.7+0.5 with two and
1.5+0.7 for stars
witS 3 - 5,r-quanta. In the lab-system-it was also greater for
stars with
Nioir-emission angles than for