SCIENTIFIC ABSTRACT AKIMOV, V. V. - AKIMOVA, A. A.
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S
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December 31, 1967
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SCIENCEAB
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VA80/60/033/011/001/014
A003/AO01
AUTHOR.- Akimo-v 11 V
TIME. g The Hardenb-zg Number axd Density of Glasses~
CaamazA cation 11.
PERIODICAL. Zhurnal prikladnoy khimii, 1960, Vol. 331, No. 11, pp.
2404-2412
mm~ The opti~5al constants of glasses of the system Na2O-B20 -Z'0
had been
v 3
lnvesllgat~~d earlier (Ref, -~~esp
1) . The hardening number and the dansity of
-s was st-adied here, "he coet-ant 1m-ol&r%) of Na2O var-led from
I to 40 B 0
assr $1 2-;~
f-om 33 to 85. T'Ph6 hax-Jer-ing number of Sod'.=-b G a
frcm 0 to 50 &-~A SiO
? -4
glasses is 10 30 -AzO and rises to 70 - 73 ' 10 for gla,-sps
containl-rzg simul-
taneously 17 2% Na2O and BPOA. A temperature inoraase b?yond tb--
burn- ing
tempera-t~ur-, causes a. decrease ol the r,~-.fractive
prop~n--11,4-s- glass-es. The
Peaks on '11,e r~~fraotiva index curvas are smcothed and their
ma:jd a are sh'V.;,~d to
IM L
sp~-,~m wi-Ich havl- h!gh--~r ra--P-na6tive
the sl& e~' tha gl-q-qses of the Na O-B203
2
Lndi~~,,~s :~cxnpar,3d to glasses of the Na20:S02 syst-em. The
dam.sity of the glasses
st,Lzdied various f'ram 2.1457 to 2.5497. The --h&Ds of ttiz
d-t:0-sIty -n-,7ires is sLrnilar
to the, of the index ourv-as. Betds a:rc- olserv-d w.1--h the
transition to
Card 1/2
S/080/60/033/011/001/Olit
AOO3/AOO1
The Hardening Number and Density of Sodium-Boron-Silicate
Glasses. Communication
11.
glasses of the leached region. The peaks and bends are
clearly visible in
compositions with the following ratios: Na2O : B 0 = 1 : 1;
Na,?O : 810'-) - 1
2
Na2O : B203: S102 = 1 : I : 2. This fact confirms ~he
presence of certaiR
compounds in the glasses which determine the properties and
their change.,3. The
smoothing of the peaks and bends corresponding to certain
compounds is explained
by the dissociation of the latter, and the shift of the
extrema by the inequality
of the absolute values of the properties of the extreme
components. The investi-
gation showed that sodium-boron-silicate glass has a complex
molecular compotd-tion.
Besides the mentioned compounds it conta*ins the products of
their diusociati.on.
The author expresses its gratitude to L. I. Demkin, Doctor
of Technical Sciences
who guided the present work. There are 21tables, 6 figures
and 12 references:
7 Soviet, 4 English, 1 American.
SUBMITTED: October 15, 1959
Card 2/2
RUMYAh'TSEVA,, N.P.; AKIMV, V.V.
Some materials for the study of the poliomyelitis
outbreak In
Nakhodka in 1960, Trudy VladIF.MG no.2050-1~6 162.
(MIRA 18 s 3)
1. 1z Primorskoy krayevoy
satitarno-ep-l-demi.ol-ogicheakoy stantsil.
A I 'E ~-! 0 11 V. 11. ; D 0 R (2 ROVA , V - S
SLO11:07, 1'. ; ! A
Epidemiologic characteristics of tivl-lvvj-~e
el-,celYn'llitis in
thritime Territory. Med. puraz. i paraz. bol. 33
ro.2: 169-177
Ili, - Ap 164 18-1)
1. Otdel entornologil. ( zav. - prof. V.111.
Bellaemisheir [deceased])
Tnstituta meditsinskoy parazitologii 1 tropicheskoy
meditisny
L-ueiii Ye.I. lbrtsimmkogo (direktor - prof.
Sergiyev)
l'i-nisterstva zdravookhrancniyu -SSSR, Vuokva, i
Primorskaya
skruyevaya saniturrio-c-pideziiolcgi-ches'r-aya
stantsiya (E~lavnyy
vrach V.V. Akimov).
PROKOSHKIN, D.A.1 VASILIYEVA, A.G.; AK1MOVP- V.V.
~,.: t
Strength and plasticity of alloyed steels following a
low-
temperature thermomechanical treatment. Metalloved. i
term.
obr.-met. no.1101-33 N 165. (MIRA 18:12)
1. Moskovskoye vysaheye tekhnicheskoye uchilishche
im. Baumana.
L 02983-67 EWT(m)/EWP(w)/T/EWP(t)/ETI/EWP(k) 1,JP(c) JD/HW'
ACC NR. AP6032461 SOURCE CODE: UR/0129/66/000/009/0051/0054
AUTHOR: Prokoshkin, D. A.; Vasil'yeva, A. C.; Akimov, V. V.;
Shinkarevich, Yu. B
ORG: none
TITLE: Effect of on'temperature in thermomechanical treatment
on mechanical
propertiep, and nil-ductility transition temperature of alloyed
structural steel
J'N
SOURCE: Metallov6deniye i termicheskaya obrabotka metallov, no.
9, 1966, 51-54
t &
TOPIC TAGS: structural steelf ~tYfel thermomechanical
A temperature thermomech~ani~dal ~trezatment, util-
CA-YO-71 t
t
mechanical property/40Kh5NSMF steel
ABSTRACT: Several series of specimens of 40Kh5NSMF (0.46% C,
5.2% Cr, 1.6% Ni,
1.5% Mo, 0.557. Mn, 1.32% Si, 0.2% V) steel were austenitized
at 1050C and subjected
to thermomechanical treatment (M) , rolled at 550-1050C with
50% reduction, quenched
and then tempered at 200-300C. The tensile strength and yield
strength were found
to increase and ductility to decrease with decreasing
deformation temperature (see
Fig. 1). The NDT temperature dropped with increasing
deformation temperature from
-20C for steel rolled at 550C to -50C for steel rolled at
800-1050C. The
strengthening effect of thermomechanical treatment was not
eliminated by repeated
hardening. However, the higher the temperature of DIT, the more
stable the effect.
Repeated hardening with short 5-min austenitizing at 1050C
lowered t~e tensile
Card 1/7 Mr.- 6?1.7RQ!fii;9.11L_?Q
L 02983-67
ACC NRi AP
di, .2 kg/MM2
250 d.1 I
0
2 1
2!0
2
IPft 2
an
7 5.
Deformation temperature
Fig. 1. Effect of deformation temperature
on tensile strength (0b), yield strength
(00 2), elongation (6), and notch toughness
(c~L5 of 40Kh5NSMF steel tempered at 200C (1)
or 300C (2) after thermomechanical treatment.
strength of steel rolled at ~50 and 1050C from 250 and 232
kg/MM2 to 215.and
227 kg/mm2, respectively. Orig. art..has: 3 figures and 2
tables.
SUB CODE: 1l/ SUBM DATE: none/ ORIG REF: 005/ OTH REF: 001/
ATD PRESS: ~5099
MISEYCHIK, A.N.; DOVGAL', V.I.; AKIMDV, V.V.
-------
Heater for preheating the coo1ing system liquids of
tractor engines.
Trakt. i sell)(hozmash. 32 no-5:13-15 MV 062. (MIRA 1515)
1. Gosudarstvennyy soy-uznyi ordena Trudovogo Krasnogo
Znameni
nauchno-isaledovatellskiy avtomobilInyy i institut (for
MoiseychiV.). 2. Onezhskiy traktornyy zavod (for
Dovgall, X.~imov).
(Tractors--Cold weather operation) .
Le t9 protect the r-.vur-% ,)f' tne- f-.I%rJ
0-khr. prir. na Dal'. VoFt.
OC Wt
aT),
Frimors"kaya ki~ttyevayi- kya
PSHENICHM, A.Ya.; KALININ, M.N.; SMIRNOV, V.G.;
AKIMOV, Ye.T.;
SEMENYUTA, N.N.
Shaft sinking with the use of a shaft lining
formwork. Gor.ahur.
no.402-36 Ap 164. (KRA 17:4)
1. Vaesoy-uznyy na-achno-4soledovatellskiy
gorncoetallurgichaskiy
institut tsvetnykh metallov (for Pshenichnyy,
Kalinin, Smirnov).
2. Trest Svinetsshakhtostroy (for Akimov). 3.
Glubochanskoye
sh,Ahtostroyupravleniye (for Semenyuta).
SOV/127-59-4-6/27
AUTHORS:-
Akimovq Ye. T. and
Lisovskiy,G.D., Mining
in
TITLEs
A Comparison of the
Exploitation Qualities of a
Sifting Grate With a Reinforced
Concrete Slab
With a Slot* (Sravneniye ekspluatatsionnykh
kachestv grokhotnoy reshetki i zhelezobetonnoy
plity A
propusknoy shchel*yu,)
rPiRIODICALs
Gornyy zhurnal, 1959, Nr
49 PP 35-37 (USSR)
AASTRACT:
Sifting grates installed on
ore-chutes in under-
ground galleries were usually put out
of order
after a short time by falling pieces of ore,
Their
repair caused serious losses of working
time. VNIItsvetmet
proposed to cover these
ore-chutes with slotted reinforced
concrete slabs
which permit only pieces of ore of the
prescribed
size to pass, Their installation was more ex-
GaIrd 112
pensive than that of sifting grates, but on
SOV127-59-4-6/27
A Comparison of the Exploitation Qualities of a Svifting
Grate
With a Reinforced Concrete Slab With a Slot.
the whole they proved to be more economical, as
no repairs were required for a long time. This
method is used in many mines abroad. Different
types of sifting grates were proposed by:
M.I. Agoshkov, M.Ye. Mukhin and G.G.Petrenko.
There is 1 photo, 1 set of diagrams and 2
Soviet references.
MSOCATION: VNIItsvetmet, Ust'-Kamenogorsk.
OW 2/2
AKIMDV, Te.T., inzb.
Lining rectangular shafts with sectional
reinforced con-
crete, and upraises with betonite. Shakht.stroi.
no.1:29-31
ja 16o. .(MIRA 13:5)
1. VaeaMmyy nELuchno-iosledovatellskiy inatitut
tavetny"
Installov.
(Czech os lovakia--Shaf t sinking)
AKDIOV, Ye.T.; KUDINOV, A.A.
I ~-
New technology for shaft sinking. Sbor. trud.
VNIITSVETNET
no.4t66-81 159- (KMA 160)
(Shaft sinking-Equipment and supplies)
I AKIMOV, Ye.T., inzh,; LISOVSKIY, G.D., inzh.
Now methods for roofing ore chutes. Bezop. truda v
prom. 4 no. 5:22
My 1609 (Mining engineering) (MIRA 14:5)
AKIMOT, Yu.A. (poselok Neftvanikov Kok-Tah)
i_--, wmv"Wlow~.
Uning Dufssux needle for an ether drip. Fellds i akuab.
23 no.8948
Ag 158 (MIRA 11:8)
(SYRINGES)
.41440
s/iao/62/ooo/oo5/o2l/o36
E192/E382
AUTHOR- Akimov, Yu.A..and Stepanov, B.M*
TITLE: A wideband oncillographic cathode-ray tube
PERIODICAL. Pribory i takhnika eksperimenta, no. 5, 1962,
128 - 130
TEXT: The tube employs a diDflection system based on a line
with distributed parameters. "The'deflgction plates are in the
,...'form of a section of a strip line having a wave impedance of
75 J1 these are gradually tapered and matched with coaxial
lines which are led out through the glass envelope by means of
coaxial outlets (Fig* 1). The investigations showed that
provided this deflection.system was properly construc'ted it did
not show any resonance effects or proauce reflec 'tions of the .
signal from the tapered-sections of the line. The actual tube
has two electron guns with two identical deflection systems.
*The guns operate at accelerating voltages of ~O kV and produce
a tracq 0.2'-'0.5 mm thick at the screen; the writing speed
can be as high as 50 000 km/sec. The diameter of the screen
*s 170 mm. The system does not use a post-deflection acceleration
l/ 2
s/12o/62/000/005/021/036
A wideband oscillographic 4-4. E192/E3W'
stage in order to reduc6.the distortion of the signal image at
the screen. The transi-e tim foof the electrons through the
deflection system is 3 x'10- see. The uppbr frequency limit
for the signals displayed'by the tube is therefore
approximately
equal to 1 500 Mc/s. The sensitivity with respect to the signal
plates is 0.045 mm/V, so*that signals having an amplitude of
1 000 V can be observed. The-tube is-provided with an
additional
pair of deflection plates which are used for calibration by
shifting the level of the investigated signal or by using a
sinusoidal waveform for producing time-markers. There are
4 figures.
SUBMITTED: November 5, 1961 qU,7U1AdPffVaxCUaA6- Si(r] I
JVIVOF due. Fttcs hation
E t T'Jind 1,1b as
OlIg
Fig. 1 ,~t669~
a S,
Card 2/?. t4i Ai p a
AK32401r,, Mi.A.
Case of congenital, elephantiasIs of the fingers In a
child.
Ortop., tram i protez-. no.ls73-74163. (KMA 16:10)
1. 1z khirurgicheskogo otdeleniya kafedry detskikh bolezney
(zav. - prof. A.I.Perevoshchikova) lzbevskogo meditainskogo
institute. (rektor - kand.med.nauk A.M.Zagrebin).
4r
AKIMOVP Yu. A.
Differential diagnosis of congenital pyloric stenosis in
infants.
]Qdrurgiia no.6:124-125 Je '62. (MIRA 15:7)
:1. Iz detskogo 1-hirurgichoskogo otdeleniya Izhevskoy
gorodskoy
detskoy klinicheskoy bollnitsy No. 4 (glavnyy vrach P. 1.
Maslova) i kliniki detskikh bolezney (zav. kafedroy - prof.
A. I. -Parevoshchikova)
(PYLORIC STENOSIS) (DIAGNOSIS, DIF""TIAL)
Treatment of hypertension with d1coline. Sov. mod. 24
no.6-128-134
je l6o. (MIRA 13:9)
1. 1z gos itall,noy torapevtichoskoy kliniki (dir. - prof.
P.Ye.
Lukomskiy~ 'II Moskovskogo meditsinskogo instituta imeni
N.I.
Pirogova. (HYPERTENSION) (AUTONOMIC DRUGS)
AKIMOV, Yu.I.; ORWV, L.L. (Moskwa)
Clinical oignifioance of electrokymography in the diagnosis
of
trieuspid stenosies Klin.med. no.7tnO-116 161. (MIRA, 14--8)
1. Iz goopitalinoy terapeyticheskoy kliniki (dir. - prof.
P-Ye.
Ijukomakiy) 11 Moskovskogo meditsinskogo inatituta imeni N.I.
Pirogova.
(HEIRT-VALVES-DISFASES) (ELECTROKYMOGRAPHY)
AKMV.. Yu.ls;_,~=Vp L.L.
Meatrokymograpby in the bealtDr subjeate Thrap,arkh., 33
noaRt
58-72 T "61a (KMA 34,t3)
is lz goo itallnoy terapevtiohookoy klinW (clir., - prof&
PoYss
Luk r1 Mookovskogo moditainakogo institute imeti Nal.
Pirogova.
AKIMOV, Yu. I.
The diagnostic value of the systolic plateau on the
oeft auricular
electrolquogram, Cor.vana 4 no.2:85-93 162.
1. Internal Clinic., 2nd Medical Institute N. Ie
Pirogov) Moscow*
(XIMOGRAPHr)
AKIFIOV)__Yuj~.,-, O=V, L.L.
Elektiokymography; survey of the literature and analysis
of our
data. Sov. med. 25 no.7:8-19 Jl 161. (MAA 15,1)
1. Iz gorpitallnoy teiapevticheskoy kliniki*(dir. -
chlen-korrespondent
AMN-SSSE, prof. P.Ye.Lukomskiy) II Mdskovsko'go
meditsinskogo instituLa
#eni N.I.Firogova.
: (FIZUROKIMOGRAPHY)
ANMOV, Yu.I.
Electrokysograms of patients with rheumatic nitral
and aortic
lesions, Kardiologia, 1 no,3:58-72 Yq-Je 161* (MIRA
15:3)
1. Iz gospitallnoy terapevticheskoy kliniki (dir. -
prof.
F.Ye. Lukomskiy) II Moskovskogo meditsimkogo
instituta imeni
N.I. Firogovao
(BIECTROKDIOGRAPHY)
(MITRAL VALVE-DISMSES) (AORTA-DLSEAM)
AK.IMDV, ru.I.; ORIoOV,, L.L.; BMrCHEV,, V.V.
Normal electrolcymogram and its characteristics in
athletes.
Vop.kard. 2-go MMI no.2sl9-51 162. (MM 1-6s1)
(ELECTROKYM3GRAPHY) (ATHLETES)
~4
AKIMOV, Yu.I.
Electrolqwgram of patients suffering from rheumatic
heart
disease. Vop.kard. 2-go MGMI no.2s53-99 162. (NIRA
16:1)
(MCTROUMGRAPHY) (RHEUMATIC HEART DISEASE)
AKIMV, Yu.I.; M&WVA, M.N.; OALOV, L.L.
Electrokywgram of patients suffering frnm chronic
pulmonaZ7
and cardiopulmnary,irsufficiracy. Vop.kerd. 2-go
HGMI no.2s
129-138 162. (MM 161l)
(ELECTROXIMMUPM) (HMT-DISMES) (TUmr-%--nT-RFMES)
ORIAN, L.L.; BULYCHEV, V.V.; AIIIMIV Yu.I.
Ballistocardiogram ofa healthy person and its
characteristics
in athletes. Vop.kard. 2-go MMI no.23139-154 162. (MM
16:1)
(BALLISTOCARDIOGRAM) (ATHLETES)
ORLOV, L.L.; LKIMDV, Yu.I.- SOLOVIYEV, V.V.;
FEDOROV, V.D.
j
Ballistocardiogram of patients suffering from
rheumatic heart
disease. Vop.kard. 2-go MMI no.2:155-176 162.
(MIRA 161l)
(BALLISTOCARDIOGRAPHY) (RHEUMATIC HEART DISEASE)
4XITHOXI-L" (Moskva) G-165, Kutuzovskiy prosp., d. 39/30
kv.337); FEDOROV,,
N.D.
Comparison of the--electrokymogTaphic changes with the
anatomical
and with the pressure in the left auricle and pulmnary
artery in
mitral stenosis. Grud.khir. no.4:51-58 J1-Ag 162.
(MIRA 15;10)
1. Iz gospitallnoy terapevticheskoy kliniki (dir. -
chle*-korr.
AMN SSSR prof..P.Ye.Lukomask1jv) i gospitallnoy
khirurgicheskoy
kliniki (dir. - prof. T.S.Mayat) II Moskovskogo
meditsinskogo
inatituta imeni N.I.Pirowova,
(ELF,CTR06MGRAPHY)
(BLOOD PRESSURE)
(PULWNARY ARTERY)
(MITRAL VALVE-DISEASES)
AK~40T,,Xu.-J,; ORLOV, L.L. (Moskva)
Electrokymography in the diagnosis of diseases of
the cardin-
vascular system. Vrach. delo no. 1:33-37 Ja 164.
(MMA 17:3
1. GospitallnayTi ter4pevticheakaya klinika (zav.
- chlen-
korrespondent AMN SSSR prof. P.Ye. Nkomskiy) 11
Moskovskogo
meditsinskogo instituta imeni N.I.Firogova.
SOLOVIYEV, V.V.; AKDAOV, Yu.j.,* ORIDV, L.L.;
YURASOV, V.S.
Diagnosis of tricuspid stenosis. Kardiologiia
5,no.2:35~-43
163 (MIRA 17:2)
1. Iz gospitallnoy terapevticheskoy kliniki ( dir.
- chlen-
korrespondent MIN SSSR prof. P.Ye. Iukomskiy) II
Moskovskogo
meditsinskogo instituta imeni N.I.Pirogova.
i~iagncs~ s iz a- er62 -- 15-ocar-al t, s.
an i iy, t. av4
N '~,co fA -1:8L 1z
IRA
%z&
~*',N SSSR r,~.If.
1. AXIMOV. YU.
2. ussR (6oo)
4. Kochetov, Vsevolod
7. "The Zhurbinn." Vaevolod Kochetov. Reviewed by Yu. Akimov.
Rabotnitse. No. 12
1952
9. Monthl List of Russian Accessions, Library of Congress,
April -1953, V--~cl.
IV, t"
INSTRUMENTATION: SCINTILLATORS
"Effective Detector for Fast Reutrons", by Yu.K.
Akimov, A.S. Kuznetsov,
and G.A. Leksin, Institute of Nucl *~i_ Academy of
Sciences
ear Prob, M.
USSR, Pribory i Tekhnika Eksperimenta, No 2,
September-October 1956,
pp 70-71.
This detector was developed at the Institute of Nuclear
Problems in
1952 and has an efficiency of 20%. It consists of a
long (approximate-
1Y 70 cm) liquid scintillator-converter and a
photomultiplier. It re-
cords both charge-exchange protons and charged
particles fron "stars"
formed by neutrons in the large convertor volume. This
dete..--tor had
certain shortcomings, which were eliminated as
described in this arti-
cle.
Card 1/1
AKIMOV, Yu.K.
)kltichannal coincidence systess. Prib. i takh. skep.
no.1:95-96
4-7. ~ 137, OwA io3 6)
1. Oblyedinenw li~ st-it-ut-yadernykh issledovaniy.
(Ileatron-tubs circuits)
USSR/Nuclear Phys-fcd- Instruments and Installations C-2
Methods of Wasurement and Investigation.
,Abs Jour Referat'Zhur Mika, So l...1958, 299
Author Akinov, YU.K.
Inst Joint Institute for Nuclear Research.
Title High Speed Transmitting Circuit for an Amplitude An&lyzer.
Orig Pub Pribory i tekhn. ekaperimmta, 1957, No 2, 116
Abstract A block dia em is given for a device with a resolution
time of 10-Irstconds. Pulses from the spectrometer arrive
simultaneously at -two anti-coincidence circuits,. the out-
put of the first being connected vith one of the inputs of
the second; if the first anti-coincidence circuit does -
not receive at the very saw instant a pulse from the te-
lescope of the counters that separate the investigated par-
ticles, then the signals from the spectrometric counter
Card 1/2
Act M 0 ya,
AUTHOR: 120-4-30/35
TITLE: A Fast-acting Differential Coincidence Circuit
(Bystrodey-
stvuyushchaya differentsialInaya skhema sovpadeniy)
PEIZIODICAL: Pribory i Tekhnika Bksperimenta~ 195?
pp. ~81!4'~USSR).
ABSTRACT: The principle of the action of the circuit is similar
to
that proposed by Bay (Refs. 1$ 2). The input elements of the
apparatus are two coincidence circuits. Each of these is
connected to two pulse detectors, one directly and the other
via a delay cable (Fig.1). The result of such connections is
that the output pulses of both circuits will be equal in am li-
tude at coincidence but different at non-coincidence (FigM.
The difference in the pulses is obtained by the differential
stage. After amplification, the difference pulse, which is
the anti-coincidence signal, suppresses the pulse which is
being transferred from one of the coincidence circuits to the
counting apparatus. The result is that only coincidence pulses
which are not accompanied by difference pulses are recorded.
The circuit diagram is given in FiZ. 3.
The circuit recorded the self-coincidence of pulses from a
counter, which consisted of a photo-multiplier B-1 and a
Card/l/33olution of terpherLyl in phenyleyclohexane,
scintillating under
U
A Fast-acting Differential Coincidence Circuit. 120-4-30/35
6o
the action of irradiation from Co The photo-multiplier was
loaded by a 75 9 cable. The amplitude of the pulses waB,(-,
0.5 V.
The x1f-coincidences were broken by cables of different lengths
Z. (Fig-3). The count rate of the pulses in relative units con-
sisted: -with I = 01 -1, with I = 5 cm - 0.3, with t = 10 cm
- 0.02 and with Z = 10 cm tended to zero, which corresponded to
a time resolution - 2 x 10-10 sec.
Yor recording cdncidences from two scintillation counters-, it
is necessary to consider not only the time variation but also
the amplitude variation of the coincident pulses. if this
difference is not very great, then it can be limited to some
value of the resolving time due to amplification of the
discrim-
ination of the difference signal. With large variation, it is
necessary to make the signal symmetrical by using forming lines
and to move these pulses relative to each other as measured on
their half-widths KFig.2). The circuit is primarily useful for
analysis of fast particles with time-spans differing by
at "e'- 10-9 sec. There are 3 figures and 2 non-Slavic
references.
Vard2/3
A Fast-acting Differential Coincidence Circuit. 120-4-30/35
9 ASSOCIATION: United Institute of Vuclear Research
(Obl'yedinennyy institut yadernykh issledovaniy)
SUBMITTED: February 27, 1957.
AVAIIABLE: Library of Congress.
Card 3/3
AKIMOV, Yu, K., SAVCHENKO, 0. V., and SOROKO, L. M.
With Polarized Protons of High Energy,"
Investigation of the Reaction P+-Vd Oger
Nuclear Physi 8, Vol. 8, No 6, November 1958, pp 637.
Joint Institute of Nw lear Research, lab of Nuclear Problems.
Abstract: The angular dependence of the asymmetry in the emission
ofirt-mesons in the
reaction p+ d was measured on a polarized proton beam at energies
536, 616 hnd
654 MeV. Direct proof of the existence of the d-state of the mesons
in the reaction p+ p-.,v
1Z-++ d has been obtained. The results of the experiment are in
agreement vith the aasump-
tion that the amplitudes of the a- and d-transitions are
considerably less than the XZF++
amplitude of the transition %---:04 (3sl,p)2'. The limiting values
of some partial cross
sections have been estimated.
AUTHORS: Akimov, Yu. K., Savchenko, 0. V., SOV/56-35-1-12/59
boroxo, U. M.
TITLE: Investigation of the Reaction p+p 4 d+~ + in a
Polarized
Proton Beam (Issledovaniye reaktaii p+p -4 d+n+ na poly~-
arizovannom puchke protonov)
PERIODICAL: Zhurn-al eksperimentallnoy i teoraticheskoy
fiziki, 1958,
Vol 35, Nr 1, pp 89 - 96 (USSR)
ABSTRACT: The authors fil%t discuss various earlier papers
dealing
with the reaction p+p 4 d+n+~1), as e:9,. the investigation
of (1) at EP = 46o to 66o MeV (Ref 1) f n++d 4 P+p at
3n+ -174 - 307 Mev (Ref 2); investigation of (1) at
E - 314 MeV with a polarized proton beam, observation of
aRymmetry as a result of Apterference between s- and p-state
(Ref 3), analogous investfgations at 415 MeV (Ref 4),
e-scattering on protons in the d-state (Refs 5,6) etc. The
present paper contains a report on the investigation of
the angular dependence of the asymmetry of the n+ of (1),
Card 1/4 viz. for E p'- 536, 616 and 654 MeV; the primarily
un-
Investigation of the Reaction p+p --~ d+n + in a
SOV/56-35-1-12/59
Polarized Proton Beam
polarized proton beam of 637 MeV was supplied by the synchro-
cyclotron of the Ob"yedinennyy institut yadernykh issle-
doyaniy (United Institute of Nuclear Research). The
experimental arrangement is given in figure 1; the manner
in which experiments are carried out is described. The
polarized proton 5beam had the following intensities:
536 mev : 0,9.10 , 616 MeV:5,5.jo5.-, 654 MeV:2,8.lo5
protons /cm2sec. For the two first Ienergies the graphite
scatterer had 22,9 9/cM2, and for 654 MeV 7,3 9/cM2. The
results obtained by measuring asymmetry are represented
by figure 3. For the 3 E -values the following cross
sections were obtained: P
da/d-Q-0,24 + cos2g;,v 0,22 + cos 20;,-,)0,27 + Cos20;
Crtotal-.2,42.10_27CM2 , 3,14-10- 27cm2 and 3,1.10- 27CM2
(0 is given in c.m.s.). The results obtained by these ex-
periments prove the existence of a d-state of the TE+
from reaction (1) and agree with the assumption that
the amplitudes of s- and d-transitions are considerably
Card 2/4 smafter than those of the OD 2 4 2S 1 P2 )-transition.
For
Investigation of the Reaction p+p 4 d+n+ in a
SOV/56-35-1-12/59
Polarized Proton Beam
the differential cross sections the following limiting
values were obtained:
a(1 so 4 3SIpo)), 10-3.at(pp-~ dn+)
a(s + d));,5,4-10 -2 -at (pp --~ dn+)
a(1D 4 3S P )4 0,945-ct(pp -) dn+)
2 ,' 1 2
In conclusion,the authors thank M.G.Mes'hcheryakov, V.S.
Neganov, and L.I.Lapidus for discussing the problem and
N.P.Klepikov and S.N.Sokolov for working out experimental
resulta. There are 5 figures, 3 tables, and 16 references,
10 of which are Soviet.
ASSOCIATION; Ob"yedinennyy institut yadernykh issledovaniy
(.United
Institute of Nuclear Research)
Card 3/4
AUTHOR: Akimov Yu K SOV/120-59-2-31/50
TITLE: The R~gistration~'of Counting Errors in Scaler Circuits
(Registratsiya proschetov v pereschetnykh skhemakh)
PERIODICALt Pribory i tekhnika eksperimenta, 1959, Nr 2,
PP 113-114 (USSR)
ABSTRACT: The use of a coincidence circuit (c.c.) in a counter
increases the order of accuracy when counting pulses
randomly distributed in time. Pulses may be lost if
they follow one another within an interval less than the
resolution time of the counter. In Fig 1 the input
pulse train is applied in two ways to a c.c., directly
and also after stretching and shaping. The output of
the c.c. gives the second of two adjacent pulses; the
first is obtained as the output of an anti-coincidence
circuit (a.c.c.) whose inputs are the stretched pulse
and the resolved second pulse. Pulses will only be lost
now if more than one occurs during a "stretched" interval)
T. The relation betweer, the number of pulses registered
by the first counter (a.c.c. output) and the total
Card 1/2 registered is given by Eq (1) . Assuming a Poisson
distribution the number registered of the second counter
SOV/120-59-2-31/50
The'Registration of Counting Errors in Scaler Circuits
should be as Eq (2). The way in which the counter
outputs and loss rate vary with the product of countered
total and delay time is shown in Pigs 2a, 2b. When
counting 150 000 pulses per see the proposed scheme5
with a delay time of I V , gives a performance equal to
that of a single over couriter having a resolving time
of 0.7 times 10--?sec (accuracy in each case is 1%).
The conclusions ha:ve been verified using a 6AZP valve as
Card 2/2 c.c. and a PS-10 000 as a counter.
There are 2 figures.
ASSOCIATION: Ob"yedinenn institut yadernykh issledo'vaniy
(The Unitedy~nstitute of Nuclear Research)
SUBMITTED: March 28, W8
05462
")OV/120-59-3-33/46
AUTHOR: Akimov, Yu. K
TITLE: oincidence Circuit for Small-amplitude Pulses
(Skhema sovpadeniy dlya impullsov maloy amplitudy)
PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 3,
p 134 (USSR)
ABSTRACT: Two models of the circuit are described. Fig 1
shows
the first in which the anode of one photomultiplier
(Al) is jo7i'ned to the last dynode of the other
photomultiplier; the output pulse is taken from the
last dynode of the first photomultiplier. There is
only a very small output unless the two photomultipliers
give coincident pulses. This simple circuit has
disadvantages, and the one actually used is seen in
Fig 2. Here the output from single pulses is very much
smaller (0.01 - 0.02 V) for single-phase heights up to
8 V. If the single pulses have a height of only 0.03 V
(minimum) the output coincident pulses have a height
of 0.025 V. There are 2 figures and 2 references, 1 of
which is Soviet and 1 English.
ASSOCIATION: Ob"yedinennyy institut yadernykh issledovaniy
(joint*
Institute of Nuclear Research)
SUBMITTED; March 28, 1958
21(7) .
AUTHORS: _AkjjA;vvj-YU*.""-Krf Marish, K. S. SOV/56-37-1-8/64
Savchenkop 0. V., Soroko, L. M.
TITLE:
Measurement of Deuteron Polarization in the Reaction
p+ p
--),-d+ x+ at a Proton Energy of 670 Mev (Izmereniye polya-
tronov v reaktsii p + p --jo d + x+ pri energii proto-
rizat eii de
nov 670 NeV
~
PERIODICAL:
Zhurnal eksperimentallnoy i teoreticheskoy fizikil
19599
Vol 37P Nr I, pp 46-53 (USSR)
ABSTRACT:
The authors give a
report about results obtained by measure-
ments of the vector
polarization of deuterons originating from.,
the reaction p+ p
---.* d+ n+ carried out at angles of 12109
1400 30', and 1620
in the oms. In the introduction some theore-
tical discussions,
basing upon the approximation method by
Tripp (Ref 1) are
gtven. The experimental device is shown b
figure 1 and is, like
the measuring apparatus (block schemed
(Fig 2) discussed in the
following. The proton beam used had
an average energy of 670
Mev and an intensity of 5-1010/sec-
onds. Figures 3 and 4 show
the measuring results; figure 3:
i< T > figure 4: H(04).
Measurements of the vector
11 dn+ d
Card 1/3
polarization of
deuterons, and the data on the angular
Measu~ement of Deuteron Polarization in the Reaction
SOY/56-37-1-8/64
p + p d + at a Proton Energy of 670 Nev
distribution of the reaction in the case of a non-polarized
proton beam make it possibie to determine the amplitude of the
noTiresonanoe p-t3%hsition So -->.3S P,. The contribution of
this transition to the total reaction croas section is about
I*%, exactly: (1.0+0 6 ).jo-2 a The transition amplitude
0:45 tot*
1S _.o. 3s po grows somewhat (e'-1-7) if E increases from
0 "0.W 1 P
340 to 670 Mev, but its complex phase varies with respect to
the amplitude of the transition 1D 2 -.&' 3S IP2 by 200. The
measured angular dependence of the deuteron vector polarization
is not in contradiction to the assum 3tion that the amplAtudes
of the transitions 3F2 _v. 3SId2 and F 3 _)... 3S1d3are equal to
zero. The authors finally thank V. I. Komarov for his ass~st-
ance in carrying out measurements, and L. I. Lapidus, M. G.
Meshcheryakov, and R. M. Ryndin for discussions. There are 5
figures and 15 references, 8 of which are Soviet.
Card 2/3
Measurement of Deuteron Polarization in the Reaction
SOV/56-37-1-6/64
+ d + %+ at a Proton Energy of 670 Nev
ASSOCIATION: 6.i"ye.dinenny'y institut yadernykh
issledovaniy (Joint Institute
of Nuclear Research)
SUBMITTED:, February 17, 1959
Card 3/3
AXIMOV, Yu.K.; SAVGIIENKO, O.V.; SOROKO, L.M.
d + d-4,r + H94 Reaction at a deuteron energy of 400
Mov. Zhur.
ekap. i teor. fiz. 38 no-1:304-306 Jan 160. (MIRA 14:9)
1. Ob."yedinennyy institut yadernykh iasledovaniy.
(Nuclear reactione)
0-) 0 V Y
820Y1
C
S/056/60 038/02/48/061
IA 0/ 6 10 0 B006/BO14
kUTHORS: -Ikkimov, Yu. K., Savchenko, 0. V., Soroko. L. M.
TITLE: Tho Reaction P + d -0 t + R at a Proton Energy of 670 Mev
PERIODICALs Zhurnal eksperimentallnoy i teoretichaskoy fizikio
19609
Vol. 38, No. 2, pp. 643-644
TEXT% The cross sections of the reactions p + d - t + n+ (1) and
p + d -,,Re3 + 1co (2) have been compared earlier, and a ratio of
2:1 has
been obtained. The cross sections were measured at 340, 450, and
600 Mev
(Refs. 1-6). In the present "Letter to the Editor" the writers
report on
a comparison of these two reaction modes at E - 670 Mev. The
proton beam
11 p
used had an intensity of 10 protons/see. The secondaries produced
in
targets of heavy polyethylene and carbon were identified with
regard to
momentum, specific ionization, and range. The yield of low-energy
tritium nuclei was measured in the laboratory system under the
angles
5-40 and 110. The absolute cross sections were cVibrated
according to
the deuteron yield of the reaction p + p -+ d + whose angular
Card 1/2
82031
The Reaction p + d --!p t + n+ at a S105616010381021481061
Proton Energy of 670 Mev B006/BO14
distribution is well known at E p - 660 Mev. The following
was obtainedt
dd(120)/dfl - (9-3 � 1-5)-10- 30 cm 2/8 teradian and
dd(25')/dft -
- (3-1 + 0-5)-10- 30 cm 2/8 teradian. These data and those
obtained at
other e7nergies are illustrated in a Fig. With increasing
Ep the fraction
of forward emitted protons rises. If the cross sections for
Ep . 670 Mev
are calculated according to the theory of momentum
approximation,
d6(120)/da .. 3.1-10- 30 and dd(250)/dn - 2.4-10-30 cm 2/8
teradian are
obtained. The difference between theory and experiment is
ascribed to the
fact that the contribution of the meson-producing reaction
p + P - n + p + n proceeding besides the reaction p + p --~
d + 7t was
neglected. There are 1 figure and 9 references: 4 Soviet
and 5 American.
ASSOCIATIORt Ob"yedinennyy institut yad; kh issledovaniy
(Joint
r~n
TnAtitute of Nuclear Resea ch~
SUBMITTED: October 15, 1959
Card 2/2
AXIMOV, Yu.K.; KOMOV. V.I.; SAVCHENKO. O.Y.; SOROKO.
L.H.
Separation of particles according to the ionization
value in
some scintillation counters. Prib.i tekh.eksp.
no.4:71-77
Jl-Ag 160. (MIRA 13:8)
1. Obuyedinennyy Institut yadernykh issledovaniy.
(Scintillation counters)
AKIMOV, Yu. K.
Cand Phys-Math Sci - (diss) "Methods of time and
amplitude sel-
ection of scintillation counter impulses in experiments
with
the synchro-cyclotron." Z-Dubna, 19617 12 pp; with
diagrams;
(Inst of Theoretical and EXDerimentaT Physics of the
Academy of
Sciences USSR); 160 copies; price not given; bibliography
at
end of text (28 entries); (KL, 5-61 sup, 1.71)
2069o
5/120/61/000/001/028/o62
AUTHORS: Aklmov, Yu.K., and Kuznetsov, A.S.
TITLE: A 20-Channel Amplitude Analyser
PERIODICAL: Pribory i tekhnika eksperimenta, 1961, No.1, pp-92-95
4
TEXT: This article describes an impulse amplitude analyser
based on scintillating counters using organic scintillators.
The operating principles and preliminary developments were
described at the Third Scientific-Technical Conference on Nuclear
Electronics in Moscow. March 1957. The particles to be recorded
pass through a number of scintillation counters, one of which is
a spectrometric counter. The impulses from this counter pass
through a preliminary amplifier to a transmission circuit
controlled by signals from a coincidence c1rcuit to which the
outputs from the other scintillating counters are applied. After
linear amplification the impulses pass to a threshold device which
acts as follows. If the amplitude of the impulses is below -the
threshold the impulses pass through it as through an ordinary
amplifier; when they exceed the threshold amplitude the impulses
are reduced by a constant amount. As a result of this the
Card I/
20690
S/120/6.i/ooo/001/028/oU
A 20-Channel Amplitude Analyser E194/E184
amplitude of impulses for the llth channel is equal to that of
impulses for the first; for the 12th the amplitude is equal to
that for the 2nd, and so on. Simultaneously, by means of an
additional signal the distribution device is reconnected from the
first to the second decade of channels of' the counter. An
impulse generator whose output alters linearly ivith time is
provided for adjustment of the instrument. The spectrometric
counter consists of a plastic scintillator, a light guide of
transparent plastic and a photomultiplier type tyy-ll (FEU-11.).
The shape of the scintillator was such as to compensate the
difference between the amount of light reaching the photo-cathode
from the lower and upper parts of the scintillator because of
increased light flashing in the upper parts. The pre-amplifier
is based on a double triode 6146F1 (6N6P) and is intended to
transmit impulses from the photomultiplier to a cable through
which the impulses are delivered to the transmission circuit.
The threshold device is described. Impulses of positive polarity
are applied to two inputsi to a discriminator and,through a
Card 2/
20690
S/120/61/ooo/001/028/062
E194/E184
A 20-Channel Amplitude Analyser
delay line of 0.5 lisec to a valve which is normally shut to a
current of 50 pamps. If the amplitude of the impulse is below
the
threshold of the discriminator the valve acts as an ordinary
Amplifier. If the discriminator operates, the valve is
additionally blocked by the amount of impulse voltage reaching
its
cathode from the discriminator. The amplitude of the impulse
from
the discriminator is formed by a diode giving an impulse of
rectangular wave-shape equal in amplitude to the initial
current.
The resultant impulse that acts on the valve at the end of the
delay line is the difference between the amplitude of the input
and the formed impulses. The value of this difference is such
that
impulses of amplitude somewhat greater than the threshold value
pass through the first channel of the distributor device. An
anti-coincidence and a coincidence circuit are used to convert
the
first channel to the llth, the second to the 12th and so on.
These circuits are briefly described. In the distribution device
the input impulses pass through a delay line consisting of 11
elements, connected by tappings to dividers which reduce the
Card 3/
20690
S/120/61/000/001/028/o62
cigli/E184
A 20-Channel Amplitude Analyser
amplitude of the impulses according to a pre-determined law.
The impulses are connected to a common mixer on the output of
which
there appear a series of impulses at regular time intervals
diminishing in amplitude. The discriminator passes only those
impulses of amplitude above the threshold value. The impulses
that
pass the discriminator follow two paths, one direct and the
other
with the delay to the anti-coincidence circuit, the undelayed
impulses being restrictive. Thus there appears on the output of
the anti-coincidence circuit only one last impulse which is
passed
further to the special device. From the output of the threshold
device signals are applied to one of the inputs of the
coincidence
circuit; the other inputs of this circuit receive signals from
tappings from the delay line. As a result coincidence occurs in
only one of the circuits 1-20. Consequently the number of the
channel corresponds to a definite range of amplitude of input
impulses. The bandwidth of these channels is the same. The
last,
20th, channel records all impulses with amplitude greater than
that
of the 19th channel. Tests were made with a proton beam with a
Card 4/
. 20690
s/i2o/6i/ooO/OOl/o28/o62
E194/E184
A 20-Channel Amplitude Analyser
mean energy of 670 MeV. A polyethylene target was irradiated.
The deuty-ons and protons with an impulse of 900 MeV6s
leaving the
target at an angle of 100 pass through a system of collimators
and magnetle f:Leld and were recorded by the scinti.Ilation
counters. Under these conditions the specific ionisation loss
of
deut:rons is 2.2 times greater than that of protons. The
resultant characteristic is given in Fig-7, in which the
count is
plotted against the channel number. The first peak
corresponds to
protons and the second to deu-tprons. The somewhat high count
in
the tenth channel occurs because the threshold of the first
discriminator was set somewhat higher than necessary. Both
peaks
occur against a certain background ofparti.cles. The relative
half-width of the experimental curve for deutrons is 205o. The
relative half-width of the calculated curve of ionisation
losses
in a scintillator for deutxons with an impulse of 900 MeV/s is
about 105/o and the scatter of the actual mean loss (that
result
from the deu-brons not being monochromatic) can also be about
10%.
Card 5/
20690
S/12o/6i/000/001/028/o62
E032/E114
A 20-Channel Amplitude Analyser
Recently, a group of Italian authors have described a single
channel analyser with logarithmic scale constructed on a
similar
principle to that described here (A. Alberigi et al. Ref.5).
The author thanks O.V. Savchenko for assistance and A.N.
Sinayev
for useful comments.
There are 7 figures and 5 references; 3 Soviet and 2
non-Soviet.
ASSOCIATION: Oblyedinennyy institut yadernykh issledovaniy
(Joint Institute of Nuclear Research)
SUBMITTED: December 12, 1959
Card 61X
AXn4OV,, Tu.K,,j SAVCIWMOp 0,V.; SORONO, L.M.
4oarch for.4komalieo.in the energy depovdance of the cr'080
Aection of the*reaction p + p 4 d + + P the'threabold
region of the formation of 71,M480A paits; Zhur. ekop, i teors
fist -40L not 5 s 1530-1632 1.4y. %lo (MIRA 14:7)
.1
I, Qb*ysdine~W inatituit derafth ispledovaniy,
(nuclear reaotionar (Protons) (Me0ons),
AK.U40V, Yu.Y,.; KOMAROV, V.I.; MARISH, K.S.;
SAWIMNIM, O.V.; SOROKO, L.M.
Sbarch for anomalies in the spectn= of 1-13 maclei
e=itted
in the reactien 1,.t ~ -->. 113 + yr ~tlo at a
proton energy
of 670 Hev. '-,'hur. o~--sp. -i toor. fiz. 40
no-5:1532-1535'1,17
f6l. - (MIRA -14:7)
1. Obnyedinennyy institut yadernyll issledovaniy.
Oluclear reactions) (Mlesons) (Protons)
28752
S/056/61/041/003/005/020
B125/B102
C600
AUTH6RS: Akimov, Yu. K. $ Savchenko, 0. V. , Soroko, L. M.
TITLE: Experimental verification of the principle of charge
invariance in the reaction d +d -+-He4 +Ito at a deuteron
energy of 400 Mev
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v.
41,
no. 3(9), 1961t 708-724
TEXT: The reaction d +d --1-He4 +Xo (11), which is forbidden
according to
the law of invarianoe of the total isotopic spin, has been studied
on a
400-Mev deuteron beam. L. I. Lapidus (ZhETF, 31, 865, 1956)
suggested
this reaction for verifying the charge invariance. This reaction is
only
associated with one charge state of particles so that the
perturbation
due to the difference between neighboring charge states is
automatically
excluded. This reaotion has already been dealt with in the
proceedings
of the Kiyev and Rochester Conferences on High-energy Physics in
1959 and
1960. This article presents fiew results on the reaction (11) and
an the
Card 1/4
28752 S/056/61/041/003/005/020
Experimental verification of the... B125/BI02
cross sections of the reactions d +d -*,He4 +1 (Ed -400 Mev)
(12) and
p +He3 --P-He4 +X+ (13) at Ed-674 Nov. The authors restrict
themselves to
a class of phenomena, for which the principle of charge
invariance leads
to the production of piona by nucleons and light nuclei. A
two-section
magnetic quadrupole lens with an aperture of 80 mm focused the
deuteron
or proton beam to the target. The secondary charged particles
produced in
the target were sorted out by a brass collimator, were
magnetically
deflected, passed through a steel collimator, and were finally
recorded in
the concrete shield by scintillation counters. The deuteron beam
emerging
from the synohrooyclotron had an average energy of 405.3 �0-5
Mev. The
charged particles were sorted out according to their effective
momentum,
their specific ionization, their range, and their time of
flight. They
were recorded by scintillators, a six-oounter telescope, etc.
A. N. Gorbunov and V. N. Spirodonov analyzed the energy
dependence of the
electric quadrupole transition in the reaction I +He4*--VH3 +P.
Conclusions; 1) The total cross section of the reaction d +d -
He4 +7C 0at
EIto "80 Mev in the center-of-ma8s system does not exceed the
cross section
Card 2/4
28752
S/056/61/041/003/005/020
Experimental verification of the... B125 B102
of the electromagnetic process d +d --P-He 4 +1, whereas the
expected ratio
between the cross sections of these processes must be about 102 if
they
are not forbidden. 2) The total cross section of the reaction
p +He3 -IP-He 4 +R+at the same pion energy in the center-of-masa
system is
7-10 3 times greater than the upper limit of the cross section of
the
reaction d +d -*He 4 +n 0. This difference cannot be explained
only by the
structure of the colliding nuclei. 3) The upper limit of the total
cross
section of the reaction d +d --v-He4 +n0 amounts to -3~ of t he
cross
section calculated for the "allowed" process. 4) All the facts
discussed
here are indicative of a rigorous forbiddenness in the reaction
d + d --0- He4 + R0, and, thus, confirms the law of invariance
oftthe total
isotopic spin in the production of pions 0by nucleons and light
nuclei.
5) There exists no isotopically scalar no meson with a rest mass of
100-150 Mev. The authors thank L. I., Lapidus for discussing the
experi-
mental program, V. P. Dzhelepov for interest and assistance,
R. M. Sulyayev and B. S. Neganov for assistance in experiments with
Card 3/4
28752
S/056/61/041/003/005/020
Experimental verification of the... B125/B102
gaseous He3, and also Kim Ze Pkhe and 1. V. Puzynin, co-workers
of *the
OIYaI computer center, for-computations. There are 11 figures, I
table,
and 26 references: 12 Soviet and 13 non-Soviet. The three most
recent
references to English-language publications read as follows:
H. S. Kohler, Phys. Rev., L18, 1345, 1960; A. V. Creve, B. Ledley,
E. Lillethan, S. M. Marcowitz, C. Rey. Phys. Rev., L18, 1091,
1960;
D. Harting, J. C. Kluyver, A. Kusumegi, R. Rigopoulos, A. X.
Sacks,
G. Tibell, G. Vanderhaeghe, G. Weber. Phys. Rev., 119, 1716, 1960.
ASSOCIATION: Ob"yedinennyy institut yadernykh issledovaniy (Joint
Institute of Nuclear Research)
SUBMITTED: April 21, 1961
Card 4/4
CK
AKMV,, Yu. K.J, XDMAROV, V. I., MMAKSH, SAVCHOM, 0. V., SORORD, L.
M.
"r/-Anomalies of the 113 -Spectrkm in the Reaction p + d H3+ t -IT'
at the Proton Energy of 670 Wv3l)"
report presented at the Intl. Conference on High Energy
Physics,.Geneva,
4-11 jay 1962.
Lab. of Nuclear Problems J-&,--r lms,~- N&cler
,,e /fe see,
AXDIDV) Yu. K.p BAVCHEM, 0* Vep SOROND, L. Mo
"Experimental Verification of the Charge Invariance Principle in the
d + d 7r0 + He4 Reaction for 4oo Mev Deuterons
report presented at the Intl. Conference on High Energy Physics,
Geneva,
4-13- July 1962
Joint Institute for Nuclear Research
Laboratory of Nuclear Problems
AXINDV, Yu. K., SAVCHENM, 0. V. and SOROND, L. M.
"Search for Anomalies in.the Energy Dependence of the Cross Section
of the F -1 r --ard t^action Near the Theshold of Two Pion
Productionx)
report presented at the Intl. Conference on High Energy Physics,
Geneva,
4-11 July ig6p
Joint Inst. for Nuclear Research
Lab. of Nuclear Problems
6 7 7
S/089/62/012/005/009/014
B102fB104
0 0
AUTHORSs Akimov, Yu. K.1 Butslov, M. M., Savohenkol Oo Vol
ro -ro-k o-,_ L -o) & .
TITLE: Controllable luminescence chamber with a scintillator of a
3
working volume of 2500 cm
PERIODICALC Atomnaya energiya, v. 12, no- 5, 1962, 413-415
TEXTs An apparatus working with a controllable scintillation chamber
(Fig. 1) which can be used tophotograph charged cosmic particles is
described. The scintillator measures 130-150-150 mm and is composed
of 20,000 filaments, packed in layers as ABAB.. with A44B. The layers
are.separated by black paper sheets to absorb scattered light. The
.filamentsl,,,l mm in diameter, are made of a polymer on basis of
poly4tyrana + 1~ tetraphenyl butadiene or 2% terphenyl and 0.02%
ROROR.
Since the de-excitation times are (3-5)*10-9sea and the delay times
in the
control circuits are less than 0.1 vsec, the chamber can be controlled
by an image memory with a very short storage time.. The image from any
/7
Card 1
SIO,691-621'012100510091014
Controllable lurirescence chamber with ... B101,/B104
(3) coincidence circuit, (4) block for control pulse delay, (5)
pulse
generator, (6) hi~31i-volta&e pulso generator, (7) EEOP, (8)
objective,
~9) deflecting plate of electron-optical shutter, (10),
multi-stage EOP,-
11) coil, (12) photographic apparatus.
m4ff:RF r5if"Himm
.ILI L11AA-L
FIG.1
3
-VIV
Card 3/3
Yu.S., red.; CIIISTYAKOVA,
K.S., tekhn. red.
[Scintillation methods for high-energy particle recording]
Stsintilliatsionnye metody registratsii chastits bol'shikh
energii. Moskva, Izd-vo Mosk. univ.) 1963. 170 p.
(MIRA 17:2)
I/
C~ r a r-~ a C) c I:
a sharp peaY seen ror an eT-.erQ~ of
C.,d
ACCESSION NR: APS006536
The peak width at the semi-peak points, cover:.-.g atlouT 330Kev
or i5i, was deter-
inined basivally by Caulo)mb -scattering of protons transmitted
to the target and by
:'~Miz~arisc;r. (case of partic'es emit-e-l
SUBY,ITTED; 03Dec64 ENCL: 01 SUB CODE: NIP, EC
SC V: 1~1
Card 2/3
L 4298M5
AC(=SSION, nt APS066536 MCLOSUIRE: 01
Fig. 1. Spectra of partic-les-emi-tTed
at an az.gie of 87.70 from a target
kICfi2) bombard'ed, by a'beam of lOGev
n %
Protokis 1. a--energy distribution measured
a semdconductor cownter; b--dis
-t~r ~,), mear. ~'---ee paths in a 15~
diluted gelatin phctoemuision
Ifb
Card 3/3 .1; J;
ACC NRI AP6013494 LIR/0120/66/000/002/0060/0063
AUTHOR: Akimov, Yu.K.; Van Tszhenl-va, Sidorov, A.I.; Bpshtevn,
14.1.
I- - .
ORG: Joint Institute of Nuclear Studies, Dubna (Obl'yedinennyy
institut yadernykh
issledovaniy)
TITLE: Optical characteristic* of semiconductor detectors of
nuclear particles and
their relation to surface phenomena
SOURCE: Pribory i tekhnika experimenta, no. 2, 1966, 60-63
TOPIC TAGS: semiconductor device, opt-cal detector, photodiode,
alpha particle
detector, photodiode quantum output
ABSTRACT: This is a study of spectral characteristics and
effective nuantum output,
,~ , of thick sensitive layer light detectors, ordinarily used as
nuclear particle
detectors and made from p -type silicone doped with lithium. The
detectors, with sen-
sitive layer thickness between 1 and 6 mm, were irradiated by
light at tile butt. Rela-
tive spectral sensitivities and quantum output 41 were measured
using current Hilger
and Zeiss optical instrumentation. The results were presented in
graphs. A decrease
of q, in the short wave region was observed, which is considered
related to surface
phenomena. This fall of quantum output in the short wave region
is stronly influenced
by the details of the etching process. Between 800 - 1000 nm
(nanometers)n1was close
to unity. It is concluded that the devices can be used in the
spectral region of bet-
r-4 1 1*3 11DC7 530.1-074-5
ACC NR: AP6013494
ween~,-800 - 1100 nm .(and in some cases in the regiont%-400
-.1150 nm) as efficient .
low inertia light receivers, detectors and counters of the
number of arriving quanta,
linear over a wide range of light signal intensities. Authors
thank A.I.Kalinin, L.P.
Svyatova and L.P. Sidorova for discussions and aid in
measurements. Orig. art. has 3
figures, 4 formulas and 1 table.
SUB CODE: 09, 18, 20 SUBM DATE: O9Nov65 ORIG REF: 006. 0TH
REF: 004
S/139/59/000/05/005/026
3032/Z114
AUTHORS: Moskalev, V.A., and Akimov, YU.M.
TITLE: A Double.Chamber 10 MeV Steroobetatr--
PERIODICALs Izvestiya vysshikh uchebnykh zavede
Fizika, 1959, Nr 5, pp 26-30 (USSR)
ABSTRACT: A brief description is given of a betatron which was
brought into operation towards the end of 1957.
Details are given of the electromagnet, the
electromagnet supplies, the control circuitry, the
vacuum system and some preliminary results obtained
with the machine. A photograph of the stereobetatron
is.shown in Fig 1. The magnetic characteristics.have
been described in an earlier paper (Ref 2). The
radius of the equilibrium orbit in both of the
accelerating systems is.13 cm and the maxinum induction
on the orbit is 2700 gauss. The accelerator control
circuitry is shown in Fig 3. The vacuum system
consists of two independent chambers made of molybde
glass. The pressure is(2 to,5) x 1o-6 mm Hg. The
Card angular distribution of the intensity in the horizontal
1/2 plane is shown in Fig 4. The dose rate at the distan
of 1 m is 3-3.5 r/min for each of the accelerating r0
68868
B/139/59/000/05/006/026
E032/9111+
AUTHORS: Akimovj YL M _Xononov, B.A.; and Sokolov) L.S.
TITLE: On the Extraction of the Electron Beam from a
Betatron Chamber ~q A/
PERIODICAM Izvestiya vysshikh uchebnykli zavedeniyj
Fizika, 1959, Nr 51 PP 31-31+ (USSR)
ABSTRACT: The Tomsk Polytechnical Irotitute has been studying
electron
beam from
methods for the extraction of the
the betatron chamber. Three of these methodst which
have been found to be the most satisfactory, are
described in the present paper.
1) The electrostatic method is based on the extraction
with the aid of a special capacitor. The construction
of the capacitor) the vacuum chamber etc. have been
described in the literature (Refs 1 and 2). In this
method it is possible to obtain the following beam
parameters (15 MeV betatron) t beam current 4 x 10-9 amp,
cross-section of the beam at a distance of 2 cm from
the exit windoy 6 x 10 mm, divergence in air 5'0 in the
Card vertical plane and 80 in the horizontal plane. The
1/3 electron beam extracted into the atmosphere contains up
to 60% of electrons which have reached the and of the ~11/
68868
S/139/59/000/05/006/026
B032/1114
On the Extraction of the Electron Beam from a' Betatron
Chamber
extractor gives a well-focussed beam and a good
extraction efficiency. Its properties are still
being investigated.
There are 5 figures and 3 references, of which 2 are
Soviet and 1 is English.
ASSOCIATION; Tomskiy politekhnicheskiy institut Imeni S.M.
Kirova
(Tomsk Polytechnical Institute imeni S.M. Kirov)
SUBMITTED: December 27, 109 (19582) Vr
Card 3/3
69145
S1139159100010610011034
19032/Elll+
AUTHOR: Akimov, Yu.m,---
TITLE: On the Extraction of Electrons from the Betatron Chamber
by the Nonsymmetric Displacement Method
PERIODICAL: Izvestiya vysshikh uchobnykh zavedeniyj Fizika7
1959, Nr 6, PP 3-1+ (USSR)
ABSTRACT: A description is given of a vacuum chamber for the
extraction of 100% of electrons accelerated in a betatron.
The vacuum chamber is shown in Fig 1, in which 1 is the
wall of the chamber, 2 is the injector, 3 is the
displacing coil, 4 is the electron beam extracted from
the chambers 5 is,the exit windows and 6 is an attachment
for setting up a torroidal extractor. The nonsymmetric
displacement of the electron orbit at the end of the
accelerating cycle is carried out with the aid of a
special coil consisting of four turns. A current of
400 amps is passed through this coil and the azimuthal
dimension of it is 1000. It was found that in all
Card cases the azimuthal position of the deflecting coil is
1/2 not critical. The author considers,that this method ma
be used to obtain 100% extraction, provided the form of Y411
69145
S/139/59/000/06/001/031+
E032/R114
On the Extraction of Electrons from the Betatron Chamber by
the
Nonsymmetric displacement method.
the beam is not a primary consideration. The beam is
in fact very divergent in the horizontal plane.
This paper was presented at the Inter-Collegiate
Conference on Accelerators) held in Tomsk kFebruary,
1958).-
There are 2 figures and 1 Soviet reference.
Card
2/2
ASSOCIATION: Tomskiy politeky-nicheskiy institut imeni S.M.
Kirova
(Tomsk Polytechnical Ins titu ;2_jmgnj-2A.-AKov)
SUBMITTED: December 27, 1958 0/
1
AUTHOR: Akimov, YU.M.
TITLE; Fn-6-i-e-Wssr lh6- ifficiency
the Acceleration Plocess
69-47
b/J-39/59/ooo/o6/oO3/034
1032/E114
of Capture of Electrons into
in a Betatron 19
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy,
Fizika, 1959, Nr 6, pp 10-13 (USSR)
ABSTRACT: The efficiency can be increased with the aid of a
contractor and the problem has been considered by a
number of workers (Refs 19 2 and 3). Experiments were
begun in 1956 in order to increase the intensity with the
aid of a magnetic contractor. The method is based on the
expansion and subsequent rapid contraction of the
equilibrium orbit in the betatron at the instant when the
electrons are captured into the acceleration process.
The orbit was expanded by passing a current pulse
through a coil placed at the centre of the betatron pole
pieces as shown in Fig 1. The experiments confirmed the
results reported by Logunov et al (Ref 3). For low
emission currents the intensity increases by a factor of
Card 20 or more, while for large emission currents the factor
1/2 is 2-3. Using this contractor, an intensity of 32-36
roentgen/min at one meter from the target has been
69147
S/139/59/000/06/003/034
B03 2/9114
Increasing the Efficiency of Capture of Electrons into the
Acceleration Process in a Betatron
obtained with the 15 MeV betatron of the Tomsk
Polytechnical Institute. Without the contractort the
intensity was 12-15 roentgen/min at one meter from the
target. Fig 5 shows the dependence of the intensity on
the time of injection. In this figure the intensity
(vertical axis) is plotted as a function of time in
microseconds (horizontal axis). Curve 1 was obtained
with a contractor, and curve 2 without it.
This paper was presented at the Inter-Collegiate
Card Conference on Accelerators (Tomsk, February 1958).
2/2 There are--7--f1g`u-r-e-s-a-n-d7 references I of which 2
are
English and 1 is Soviet.
ASSOCIATION: Tomskiy politekhnicheskiy institut imeni S.M.
Kiro
(Tomsk Polytechnical Institute imeni S.M. Kirov)
SUBMITTED: December 27, 1958
g
7~
I-A -4104 97 415~ 06q/Ad6bjA_)
4M0/
621.384.6
SOURCE: Ri~f. zh. Elektronika I yeye primennniye. Svc)dnyv tam, Abs. qA407
A J ~' H A jaov, Yu. M. 1 &3rbunov, V.- 1.
TTTLE: W-or trends in the development of Induction accelerators
CITED SGU`CE: Sb. Elektron. uskorit-eli. M., Vyssh. strikola, 1964, 166-171
TOP'C acce2erator, induction accelerator, betat:-:~n
T~_ SLA-. -~N T' -,- -e-,-.rted. ~.hat the Tnmsk F,c'vf echn,_c a
_C* "cc~ S. Inj a:: cl~
7 rl.: C
f? e r a:),, i' t' ander ndus tr I a' operatLor, con~_-11-7-,-, 2,.a _-i
enanc e
~nl additirr., there a-re specific requirements wh1ch de:-:--' n a
.--a-r*_~_c~LM.-
a7,-pi'catlon c-f the accele lectron beam Is ~:f-en -eenio-' f_~.- modical
rator (an el
purpc.ses kccrdlng to the above requirenents, -he n - f ._Jeqi~r. and the
Cord 1/ 2
AR4049416
of some fundamental parameters ctf the )belatron Darts are
consideredt
--.n ec- rla imf~ c On tool c i e.:! r, qm
vac,-.,~n sis *-err-
a a he "e'. a' - -n-
is tatulated.
SUB CODE i yp ENCL Or-'
'/2
.Card 2
AKIMOV, Yu.0.
Are welders must have special installation belts.
Bezop. trade v
prom. 2 no. 6:37 Je '58. (MIRA 11:7)
1. Glavnyy inzhen'er stroitellno-niontazhnogo
upravlaniya No.'l
treats Karegandashakhtostroymontath.
(Electric welding-Safaty maaBures)
4z~~Yo ~' 1b -
Erecting rape-baulage aupporta by, adding bottom nections.
Novo
talth.,innt.i spetsorab.v stroi. 21 no.7:9-11 JI '59.
(MIRA 12110)
1. Treat K&rnganda9~k1htostrqyjaont&zh.
(Mine haulage) (Building, Iron and steel)
AKDIOVI Z. V.
"140ch&n6im of Usorption Of Silver Sulphate u on Soles of
Ferric ffyctroxide.v
Krestinsk-aya., V., N. and 11akimv, z. V. (P. 705
SO: Journal of General Chemistry (Zhurnal Obshchei Khimii)
19440 Vollulae 14,t no. 1-2.
)kMOV, Z. V.
"The Mechanism of the Adsorption of Silver Sulphate on Sols
of Silicia and Acid of
Aluminium. krdroxide." Krestinskaya, V, N., and Hakimov, Z.
V. (P. 122)
SO: Journal of General Lh2!ftatry (Zhurnal Obshchei MiimU)
1944, Volume 14, no. 3-
, AKD40VA, A.A.
Structure of silk ribroil. Zhur.VKHO 10 n0-41471-472
165. (WRA 18:n)
1. MoalcovsXiy gosudaretvennyy univeraitet imeni M.V.
Lomonosova.
AKTM-MTA, A.A.
AITTMOVA, A.A.: "The hydrophilization of rubber for uf-.e
in the production of
artieicial leather". Mosemy, 1955- Min Higher Education
USSR. Mosapw
Technological Inst of Light Industry imenj L.M.
Kaganovicb. (Dissertations
for the Degree of Candidate of Technical Sciences).
SO: jj~bnay;q_letopis, No 43, 3 November 3935. Moscow.
/V/0 y
AKIMOVA, L.N.; GAVRIWV. N.I.; AKIMOVA, A.A.
On some propertlin or W-bensylated peptides. Part 2. Zhur. ob.
khim. 27 no.8:2268-2173 Ag '57. (K.m lorg)
1. Koskovskiy gosuday!,stvenun pniversitat.
(Pptides)
i k/ 0-1 -, .1"5 /~ , q -
AUTHORS: Kuznetsov, V. I., Akimova, A. A. 7r,,-,-12/26
TITLE: Organic Coprecipitants Mrj;anicheskiye soosadItell)
Communication 6. Th, Cop-cecipitation of UrLnivn during its
Determination in Sea Water (Socbshcheniye 0. Soou~_~;hdoniye
urana pri ye.-o opredelenii v mo.,:skoy vode)
PERIODICAL: Zhurnal Analitielictikoy Khimii, 195C, Vol. 13, jIr
1, PP- 79-82
0! ~Jslz)
ABSTRACT: The present paper describes the elimination of
uranitua from
sea water with simultaneous separation frona the salts
dissolved in sea water. A number of elements which are present
in sea water in very low concentrations is precipitated to-
gether with uranium. The uranium content of sea water in so
low that its.direct determination is neither possible in
water nor in a dry state after the evaporation of the water.
There are different methods for previously enriching uranium.
Desides several anorganic precipitants (references 1-4)
organic co-precipitants are especially suitable for the an-
richirent of uranium. At an excess of thiocyanate ions uranium
Card 1/4 in acid solutions forms a weakly dissociated complex
anion
Organic Coprecipitants. 75-1-12/26
Communication 6. Th Ccprocipitation of Uranium during its
Determination in Sei Wa.er
UO (SCN) and can therefore be precipitated together with
2 3
the precipitates of not easily soluble thiocyanates of heavy
organic cations. Such organic cations are, for example, the
dyes methyl violet, crystal violet, methylene blue,
rhodamines,
saffranines and many others (refs. 5-8). The precipitation of
uranium as a complex thiocyanate anion even takes glace
quantitatively from very much diluted uranium solutions. Thio
fact was proved by radiometric measurements with the aid of
the ur4nium isotope U233 (a-emitter, half-life period
1,6.1o-~ years). The a-counter used permitted the
investigation
of the precipitation of uranium up to uranium solutions with
a dilution of 1:1010. In the case of this dilution the pre-
cipitation was still quantitative. The decomposition of the
organic precipitates took: place in a muffle furnace at 500-
-6oo0c. The uranium is then determined in the residues. The
precipitate of methyl-violet thiocyanate so effectively co-
-precipitates uranium that this method was employed for the
purification of the reagents used for determination from
Card 2/4 uranium-traces. In sea water which usually has a
p:7-value of
Or,Ganic Copvecipitanta. 75-1-12/26
Communicati,n 8. Thr Coprecipitation of Uraniu:.. during its
Determination in Sea 17a.er
7 to 8 uranium mainly occurs in form of colloidal solutions.
However, for the elimination as co.-nplex thiocyanate anion
it
must be ionized. The formation of a true solution car simply
be attained by acidification with hydrochloric acid. The
determination of the enriched uranium takes place radio-
metrically or by means of the fluorescence ;,icthod in a
sodium-
-fluorido pearl. Together with uranium all elements are
eliminated which can form complex thiocyonate-anions or in-
soluble thiocyanates, as for exampIc mercury, silver,
bismuth,
zinc, cadmium, molybdenum, iron(III) and some other elements.
As the content of sea water in these elements is eztrcrely
low, their co-precipitatior( doon not render the subsequent
uranium determination difficult. The co-precipitation of a
nilmber of other elements can be effectively prevented by
per-
forminC the precipitation in the presence of conplexone III.
Pollutions by iron can be prevented by the use of purer
methyl violet or by conversion of iron into the second
sta.r-e
(o. by means of ascorbic acid). The experimental conditions
Card 3/4 of the elaborated method are described in detail.
There are
Organic Coprecipitants.
Communication 8. Tho oDpeecipitation of Urarium during its
Determination in Sea Water
75-1-12/26
2 tables and lo references, 3 of which are Slavio.
ASSOCIATION:
SUBMITTED:
AVAILABLE:
Card 4/4
Moscow Institute for Goochemistry and Analytical ChcTistr,-
imeni
V.I. Vernaaskiy AS USSR Moscow (Institut Geol'thimii i
analiticheskoy khimii im. V. 1. Vernadcko~;o All SSSR,
Moskva)
January 2, 1957
Library of Congress
1. Uranium - Determination 2. Uraniix-a - Precipitation