SCIENTIFIC ABSTRACT G.N. CHAYKOVSKIY - V.I. CHAYKOVSKIY

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000308210019-7
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 12, 2000
• Sequence Number: 19
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

CH.A.YKOVSKIY,,,,q,~.N?. -
Experience in the surgical treatment of cholecystit1s
and its
late results. Vest. khir. 93 no.12:24,29 D 164.
(MIRA 18; 5)
1. 1z kbirurgicheskogo otdeleniya (zav. -
kand.med.nauk T.As
Grasmik) 3-y gorodskoy bollnitsy goroda Nizhuego
Tagila (glarky-j
vrach - M.M.Famin).

ACCESSION NR: AP4041720 S/0181/64/006/007/~131/2145
AUTHORS: Kovarskiy, V. A.; Chaykovskiy, 1. A.; Sinyavskiy, E. P.
TITLE: Quantum-kinetic equations for processes with nonradiative
recombination
SOURCE: Fizika tverdogo tela, v. 6, no. 7, 1964, 2131-2145
TOPIC TAGS: recombination coefficient. quantum,statistics, kinetic
theory, phonon, polaron, nonradiative recombination
ABSTRACT: Several reasons for the inadequacy of the standard
kinetic-equation formalism to non-optical transitions between dis-
crete spectrum states are pointed out. The authors then propose to
describe the processes accompanying multi-phonon nonradiative com-
bination by means of a system of integral quantum-kinetic equations
based on the formalism of the quantum density matrix, a formalism
in which.the quantum-mechanical and statistical calculation stages
!Card 1/3.

ACCESSION NR: AP4041720
are combined. The method used is essentially that of Kubo (J. Phys.
Soc. Japan, v. 12, 570, 1957). A graph representation is obtained C
for the recombination coefficients.with the aid of the technique
of Konstantinov and Perell (ZhETF v. 39, 197, 1960), modified by
Lang and Firsov (ZhETF v. 43, 1843, 1962) to cover multi-phonon
jumps in the case of low polaron mobility. The free relaxation
of the band carriers, which are in quasi-equilibrium with.the
crystal lattice at the initial instant of time, is considered. .A
criterion is considered for the applicability of perturbation the
ory
to the theory of multiphonon-nonradiative transitions. "The authors
thank Yu. A. Firsov and I. G. Lang for valuable information in con-
nection with the covputation procedure, and also A. I. Ansellm
!and Yu. Ye. Perlin for a discussion of the calculation of the re-
combination coefficients*" Orige art. bass S figures and 76 for-.
Mulas.,
.ASSOCIATIONs Zn~tLtut :fLsikL L watemsWiL AN NOMMAS Ushumm (trosti-
Card

;:ACCESSION NR: AP4041720
~tute of Physics and Mathematics, AN XoiwR)
SUBMITTED: 27Dec63 ENCL: 00
ISUB CODEz GP REP SOVs 009 OTMOU 002
k
I-Cw.d -3/3-.-.

KOVARSKIYF V.A.; ~ ~AYKOV~SKIY, ~J.A.
Generation-recombination noises In a magnetic
field. Fiz.
tver. tela 7 no&8r2499-2504 Ag 065.
Recombination relaxation An a quantlzed magnetic
field.
lbid.:2505-2512 (MIRA 18tq)
1. Inatitut prikladnoy fiziki AN Moldavskoy SSR~
KiahJnev.
I
I

I
L 6329-66 EWT(I)/EP'A(m)-2.' IJP(c) AT
ACCESSION NR: AP501071 UR/03.81/65/007/008/2499/23(*
VVI 5
AUTHOR: Loy~arskiyy V. A.
2_1~40= k.". x
TITLE., Generation-recombination noise In a magnetic-field
no.
SOURCE: Fizika tverdogo tela)-v. 196~, 2499-2504
a)
~ 1" - Tti2p fit
70PIC TAGS: electron recom'bin j correlated noise, quantum oscill ion,
spectral
distribution., autocorrelation function, strong magnetic field
ABSTRACT; This is a continuation of earlier work (Tez. dokl. VI
coveshchanlya po
teorii poluprovodnikov. Izd. "Kartya Moldovenyaske., " Kishinev,,
1964) dealing with
singularitiesof carrier recombination in a quantized electric field.
In the pre- i
sent article, the theory of quantum fluctuations developed by one of
the authors
with Ye. V. Vitin ibid; Izv. AN MR, ser. fiz. No. 12p 111
1964) is
applied to an investigation of the influence of the magnetic field on
the frequency,
,spectrum and the relative magnitude of thenoise connected-with
carrier recombina-
tion and generation processes. 'By introducing an autocorrelation
function for the
quantum fluctuations and enTlaying a diagram technique., the authors
obtain an ex-
pression for the spectral density of the noise intensity# An analysis
of the re-
sults shows that the noise level depends on the magnetic field. It is
Vointed out
that there are still not enough data to determine the numerical
parameters in the
qard

6330-66 EWT(1)/,EPA(w),A;2/EWAW-2 IJP(c) AT
2
ACCESSION MR: AP501072'' U*18l/65/oo
7/008/. 505/25121,"
~AUTHOR: V. A.; T
Eovarskiy_
<
TITLE:, Recombination relaxation in a quantizing magnetic field
SOURCE: Fizika tverdogo tela. v .7,,no. 8, 1965, 2505-2512
.TOPIC TAGS: strong UZI' -"&I'
Petic pld lectron
I carrier dexisityp matrix function,, _!~ ------
recombjMtionj relaxation process.,.phonon interaction., carrier
lifetime.
ABSTRACT: The density matrix method is used to investigate the
recombination re-
laxation of carriers which-are initiaLly in a state of
quasi-equilibriun with the
crystal lattice. The calculation is based on the Fermi quasi-level
method. The
,recombination mechanism is assumed to be a single-phonon (or
single-phaton). capture!
:by local levels. It is established that the time constant depends on
Vhe magnetic
ifield. An example in which the lifetime of the carriers is delayed
bythe quan-
tizing magnetic field is presented. "The authors thank A. 1. Ansellm
Vho called
their attention to the possible signqlar##s~ of recombination kinetics
in a quanw.
tizing magnetic fieldj, and Y. L- Bonch-A12~eb_for a valuable
discussion of the .
S-S
resultso" Orig. art. has: 1 figure and 43 forwig~s.' 9V
ASSOCIATION: Institut prikladnoy fiziki AN MSSRj, Kishinev (Institute.
of Applied
'Plwsics Ali MSSR)
d 312
c
a

ACC NRi A216024010. SOURCE CODE: oooo/65/000/000/0033/0040*
UBI
AUMOR: PWkwvsklyp I._ A.
=3 ------
TIM: Derivation of quantum kinetic equation for pmesses with
sinale-phonon re-
combination
SOURCE: Al Nold=* Institut ]MiNjgftM fl%W6 Teoreticheskiye I
eksperiment&I'Mye
IssWovanlys, fiticheskIM waystv pd1npravod*ikovykh materialm I
druSikh kristallm
(Mmoretical and =Werimm*al studies an ftileal prcparties of
semiconductor materi-
au and abber emssu). nal"Vo 216." aw"a Mum"F011% jpub 38650 33-40
TOPIC TAGS: quantum statistiess, Boltzmann equation,, integral
equation, electron scat-
tering# electron recombination# electron capture, electron
emianion, phonon interac-
tion
ABSTRACT: In view of the ftet that Boltzmann's kinetic equation,
which In customar
used for the description of recombination In Impurity
semiconductors has a licdted re-
gion of application, especial1y In tAe Presence of a quantizing
Mwetic field, the
author derives a set of quantum kinetic equations, in which the
quantum w3a statist.1-
c&l approaches are combirAdj, using for the derivation the wthod of
0. V. Kanstantinuw~
and Ve Is Perel* (MMF v. 39P IM, 2960). 2w system treated Is a
crystal containift-
Impurity levels at & single depth that does wt mood the magnitude
or the Debwe
rho=. He thn Introftm the K=xtutlaw-Farell. slogliep-particle
mistrices OA 06-
3/2

tablishes for then a system &; differential equations of the Djrson
tnw. 7h9 dingram
technique and the correspondence rules are the same as established
by Kanstantinaw
and Perell. These integral equations describe the kinetic phenomena
of scattering#
capturep and emission of electroins for the crystal vith Ingwity
centers. A dis-
tinpishing feature of this system of equations In that the explicit
form of all the
coefficients contained In then In k=m. the equations for the
diagonal Ustrix ele-
ments are used to estimate the .toutribution of the recombination
mechanism of the im-
purity wAtterir4g. Vaile a gwmral soIntion, of the rema;tant Jvb
eneous integral
equation Is difficult to cbt4dz# some simplification can be
obtained by maki use of
the fact that watterin by oselUstlaw (or bV imurities) and
recombimtIon scattww
ing are Awsically Indepeadwit. 2he final wwression for the awrent
shMS that the
main camtributiou to the reembimtIon sce;ttering isedlansin is made
by a term inverso-
ly propor lonal to the qantas-aUtIftical probability or caTler
ca;ptv" by the in-
I purity center. 2be autbor p.Um to use the darived equations to
investigate the
kizatles or tb4 scousto-elecAvIcal ezYwt In arlstals. 2M wAthar
thanks V. A. Xb-
_UX*&X Ow eowtl~ lubmat In the vwk. Orig. m%. bass 9 figures and
2,9 rar%-
M CM: 2D/ DA2B% 9SMW =Mrs W on M W2

CUYKOVKIY. I.Yee-, YATSIKOs N-P,
N&nufacture of glued beat frame fOr ch&irs. Der-pron. 9
n0-10.'8-
9 o 160. (MIIU 13: 10)
(Vocdvorking mchinery)

MDROZOVp N.A., kand;tekhn.nauk; USHERENKO, Z.I.,
inzh.; CHAYKOVSKIY,_I.Ye.
inzh.
Semiautomatic Ane for machining bent and glued parts
in the
manufacture of furniture. MekhJ avtom.proizv. 16
no.8:10-14 ,'
Ag 162. (MIRA 15:9)
(Furniture industry)

MOROZOVS N.A.# kande tekbno naukj USHERENKO, Z.1., inzh.;,,
CRA YKOVSKIY
I*Yoo# Who
Now zaabines for manufacturing bent and glued furniture parts.
VWkh. I avtom. proizv. 18 no.L18-23 Ja 164.
(MIRA 17:8)

CHAYIPTS11Y, I.A., inzhener; VERN K, A.B.. inzhener.
--
Devices for hoisting In lastall1mg hydroelectric power
station
.equipment. Makh.trad.rab..10 me.4:28-29 Ap 156. (KM 9:7)
(Holsting.muchisery)

14-
CHAYIOVKIT,'K.iA.. inz mar.
bort knockout grating. Lit.prolsw. no.4:15-17 AP 157.
(MLRA 10:5)
(Foundry mochinery &ad supplies)

OWN"
OVA
U uot
&6V ;~~5 40
00 - C
Same. tug too
400 GUSTO
ISS0110 the
tot)
tic Ote"O
Cox
WOO' IOAOteTp
tat tue *"0-. .$.ti
SVOO ;4~W!S- ihe"
tus
'MOV voew ~'t %eve - apao VAO
Th4-% exi-cal to
caw sit* gel-~
Ot
tap$ C~OaMce sa& tug
fall ;Vc~~Of V, t
of tag .~Mowrs ;miex
saw 4eve

-- - ---- -- - - --- --- -- --- - - - -
A
f ModernizatiOix or the Magnetic Uniory Device (Cant.)
SCW/5158
2. Operation or *lowntary circidto used In to)pe control
devices 13
3. Control device fitted vith a cold-cathode tube 23
AVAnMIX: Library or Congress (MWSM)
Card 313 " ft 91

GOLTSHEV, Leonid Konstantinovich,, inzh.;
CHAYKOVSKIY, L.F.j, inzh.,
ea
retsenzent; KOVILICHUKI LeYa., J
MATUSEVICH, S.M., tekhn. red.
[Electronic calculating machines] Elektron:nye
vychislitell-
iWe mashirq. Kiev, Gostekhizdat USSR9 1963. 425 P.
(HIIIA 17: 1)
(Electronic computers)

GOIYSBEV., Leonid Konstantinovich; CHAYKO-yg~ml ,
L.F., inzh...
retsenzent,
[Electronic digital computers] Elektromye tsifrovye
vychisli-
tellnye mashiny. Izd.2.v ispr. i dop. Kievo
Tekhnikaj, 10,65.
40 p - (MMA 18.5)

I Card .2/2
L~ I . . ,

CHAYKOVSKIY, L.P.9 inah.
Pegulated d.c. voltage converter. Pribornstro-erde
n:,.7i24-25 J-1 165.
(MI-RA 1817)

CHAYKOVSKAYA*.,M.A..[Chaikovslka, M.A.]
Effect of various preservatives on microorganJsms.
Farmatsev.
zhur. 1.9 no.1,04-38 164. (tM 171ll.)
1. Kafedre tekhnologii lekarstvemykh form J. galenovy'kh
preparatov
Kiyevukogo inrtdtuta usoverslienstvovaniya vr%%rhey
(zaveduyusho-hA-Y
kafedroy prof. G.A. Vaysman (Vaisman, H.!.]).

Omoymay. Pa.
the **nett-totion of pulpefangers..Sakh-Prom. 30
nOO9S 9)k ~ 156i (KM 10:3)
1. Naydansiskly sum- ayy savodi
AaaW lidustry-SqcLipmat and supplies)

CIIAYKOVSY,IY2 S. [Chaikovs!kYip S-I~ ROMANENKOs, I.p
inzh.-mekhanik
Speed up the production of tiles. Sil.. bud. -11 no. 2.16 F t6l.
(HIRA 14,,2).
1. Nachallnik Kirovagradakogo ob3mzhkolkhozproyekta (for
Chaykovskiy), 2e Upravleniye stroiteltstva Kirovogradskogo
oblaellkhozupravloniya (for Romanenko).
(Kirovograd Province--Tiles)

NARUSOV, Yu.B., inzh.; CHAYKCVSKII.L S-A-, inzh.; KAMENTSEV,
V.P., kand. tekhn.
nauk
Sectional vibration tray for manufacturing blocks of spans for
bridges.
Transp. stroi. 15 no.7t25.-27 J1-165. (MIRA 18:7)
1. Dmitrovskiy zavod zheleznodorozhnykh konstruktsiy (for
Narusov,
Chaykavskiy). 2. Vsesoyuznyy nauchno-issledovatellskiy institut
transport-
nogo stroitellstva (for Kamentsev).

-IN v v a FN x
OVRUTSKIY, M.Sh.; CHAIKOVSUT. S.I.
TawAng of heat-stable youfts, Leftays Proin, 12, Wo.5, 23-4
157..
(CA 47 n0,19810257 153) (MMA

USSR/General Problems. Methodology. History.
Scientific A
Institutions and Conferences. Instruction.
Questions Concerning Bibliography and Scien-
tific Documentation
Abs Jour Fef Zhur-Xhimiya, No 3, 1958, 6837
Author A. Mal'skiy, V. Qjj~jy~ski~j L. Tvlel'tser,
S. Chuk-lin
Inst Odessa Technological Institute of Food and
Refrigeration Industries
Title Odessa Technological Institute of Food and
Refrigeration Industries
Orig :,-ub Kholodillnaya tekhnika,, 1957, No 3, 32-33
Abstract To the 40th anniversary of the Great October
Socialist Revolution. A general review of tui-
tion and scientific activities.
Card 1/1

P,5(2) SOV/66-59-5-4/35
AUTHORS: Chaykovskiy, V., Candidate of Technical Sciences, Shmyglya,
A.,
---m%Tn-e-e-r-,-1'av-76-v, K. , Engineer
TITIE-. Comparative Tests of Valves of.Various Designs
PERIODICAL: Kholodil1naya tekhnika, 1959, Nr 5, pp 17-21 (USSR)
ABSTRACT: In order to evaluate the serviceableness of valves of
various makes
and designs, as used in Freon machines, a series of comparative tests
have been conducted in the laboratory of the Odessa Refrigeration
Machine Building Plant im.Stalin. The valves were divided in 4 groups:
The ist and 2nd groups comprised various types of the suction and
discharge valves. The 3rd group contained valves manufactured by'the
Austrian firm HSrbiger and the 4th group valves designed by Engineer
A. Shmyglya. Thecharacteristics of the 4 types of valves are shown
in Table 1. The tests were conducted with compressor 2FV-10 at certain
fixed initial and final temperatures, -15 Ob and 300 C. A timing
device
recorded the time necessary for bringing the pressure in the receiver
from 0 to 5 atmospheres. The best time - 22.5 seconds - was made by
group 4 valves. Table 2 shows the results of comparative tests
obtained
by the 4 groups at temperatures indicated. The highest volumetric and
Card 1/2 energy coefficients of the compressor 2FV-10 were obtained
with valves

j
Comparative Tests of Valves of various Designs
SOV/66-59-5-4/35
of group 4 with reduced dead space. The discharge coefficient of the
Freon compressor falls sharply with the increase of dead space
starting
from 3.5% for example. The reduction of dead space in Freon
comDressors
of average output to below 2% holds practically no advantage.
There are 4 photos, 2 tables and 1 graph.
ASSOCIATION: Odesskiy tekhnolbg 1cheskiy institut pishchevoy i
kholodillnoy promysh-
lennosti (Odessa Technological Institute of the Food and
Refrigeration
Industries) (Chaykovskiy, V.), Odesskiy zavod kholodillnogo mashi- ,
nostroyeniya imeni Stalina (Odessa Refrigeration Machine Building
Plant
im. Stalin) (Shmyglya, A. and Savkov, K.)
Card 2/2

KAI-TMTBW. V.; CHMOVSKIT, F. - SHKTGLTA, A.
~ *IIW,.of testing platon-type refrigeration
compressors. Khol.tekh.
37 2003:61-63 MY-Je 160. (MIRA 13:7)
(Air compressors)

'ViRyKov SK%Y,
wqwuvw
4 0 as ad aw
3wimi i *"*, Z% Ti. ~tr
004 ca to wwgb aw pw . .....
meow.
is tome
of %b9 Reve famel
am aim aw vow ftn' OPP.
waWW and, of do b" .1" wali-d
by wal 00 S, Asm
am ad 1118

CHAYKOVSKIY-, V. D. and IDROUSHKO, P. 0.
"Refinery of Superior Quality Production," Sakh. promo., 26,
No 3, 1952

1. CHAYNOVSKIY, V. D.
2. TJSSR (600)
4. Efficiency, Industrial
7. For more accurate work and economy of material. Sakh.prom. 26
no. 11, 1952.
9. Monthly Lists of Russian Accessions Library of Congress.
March 1953, Unclassified.

(-Iq.kYIK0V-.1,IY, V. D.
CHAYKOVcKIT, V. D.: "Methods of teaching surface areas and
volumes in recondary schools",
Kiev, 1955. Kiev-4te+e Pedagogical Inst imeni A. M. GorIkiy,
Chair of Methodology
in Mathematics. (T)issertation for the Degree of Cindidnte of
Science of
Peaagogical Sciences)
SO: Knizhnava betolAsO, No. 41, IR Oct 55

LTUIMILOV, D.S. (Vinnitea);g4k .(Berdyansk);KUNINOV,
G.I.(Shadrinak)
Problem with prv~ctical contents. Nat. v shkole no.6.*QO
N-D 159
(NathomtIcs-Problem, exercises, etc.) (MIU 13:3)

+&u2SRRj- INow ymdH.
r t~/., F
E-ppi
R92385
Kholodil'rWye rriashiny. i ustanovkd dlya sellskogo
khozyayBtva by L. Z. Vielltser
V. F.-Chakovsk . Kiypv,'YLasbgiz, 1956.
103 P. diaFrs., tables.

CHAYKOVSKIY, V.F., kand.takhn.nauk, dotsent
Designing apparatus for testing refrigerating
compressors.
Trudy OTIP I W 8 no.1:37-42 '57. (HIRA 12-8)
lo Kafedra kholodlllzwkh mashin Odesekogo
tokhnologichookogo
instituta pishchavoy I kholodil'nov prorWahlennosti.
(Compressors-Testing)

--
-49HAi~~ - - -V-
RO Y411~, , V, za.
. . C H41
"The Volumetric Efficiencies of Refrigerating Compressors
having, a Varying
Capacity."
Report submitted for the 10th Intl. Refrigeration Congress,
Copenhagen,
19 August - 2 September 1959-

IVIIUKLIH, S.G., prof.;-CHAYKOVSKIY. V.F.. dotsent
"Refrigeration engineering. Vol. 1. Techniques of the
production of
artificial cold." Reviewed by S.C. Chuklin,
V.F.Chaikovskii. Khol.
tekh. 38 no-5:66-67 S-0 161. MRA 15:1)
1. Zaveduyusbcbiy kafedroy IholodII'nykh ustanovok
Ode5skogo tekhno-
logicheskogo instituta pishchevoy i kholodil'noy
promyshlennosti
(for Chuklin). 2. Zaveduyushchiy kafedroy kho)odil'nykh
mashin
Odesskogo tekhnologicheskogo instituta pishchevoy i
kholodil'noy
promyshlennosti (for Chaykovskiy).
(Refrigeration and refrigerating machinery)

CHAYKOVSKIY, V..F., kand.takhn.nauk, dotsignt; SHMYGLYA,
A.A., inzh.; VODYANITSKAYA)
- - I-- N.I., inzh.
Values of the meaft temperature of the walls of a Freon
uniflow compressor.
Trudy OTIPiKhP 12:33-36 162. (HI.RA 17:1)
1. Kafedra kholodillnykh mashin OdessIcogo
tekhnologicheskogo instituta
pishchavoy i kholodillnoy promyshlennosti.

CHAYKOVSKIY, Y.F~-A,*And.tekhn.nauk, dotsent; KUZISTSOV, A.P.,
inah.; LOS', V.I.,
V.D., inzh.
Enthalpy-concentration diagrnm for the Freon 12 - Freon 22 mixture.
Trudjr--OTIPiKhP 12:37-47 162. (MIRA 17:1)-
1. Kafedra kholodillnykh mashin Odesskogo tekhnologichoskogo
institutA
pishchevoy i kholodillnoy promyshlennosti.

CHAYKOVSKIY, V.F., kand.takhn.nauk, dotment; KUZNETSOV,
A.P.p inzh.
- -- j- ! -1 1
Low-temperaturs generators of cold. Trudy OTIPiKhP
12:22-32 162.
. (MIRk 17tl)
1. Kafedra kholodilvnykh mashin Odesakogo
tekhnologicheskogo initituta
pishchavoy i kholodillnoy proaWshlennosti.

CHAYKOVSKIYO V. F. and OZIETSOV, A. R.
Utilization of Refrigerant Mixtures in Refrigerating
Conmression Machines.
report presented at the Ilth Intl. Congress of
Refrigeration, Munich, Gemuny,
27 Aug - 4 sept 1963.

.GHAMVBKIYP V.F., kand,tekbn.nuk; XUZNETS01j, I.F.., inah.
Mlization of refrigerant mixtures in compression
refrigeratIM19,6Ptems,
lbol.takh. 40 no.l.-9-n JA-F ~63. WU W3)
1. ,~desskiy tekbuologicbeekiy institut pishcbevoy i kholodillnoy
pro4ablennosti.
(Refrigerants)

SAVKGV, K.I., inzh.; GHAYKOVSKIY V.F kand. tekhn.
nauk
Determining the angular velocity of the shaft of
refrigerator
compressors. Khol. tekh. i tekh. no.1:43-47 165.
(MA 18:9)

(A)
SOURCE CODE:
UR/0413/66/000/00410024/0024
AUTHOR: Chaykovskiy. V. F Kutnetsov, A. P.; Dankovskly, V. B.
ORG: none
TITLE: A refrigeration unit which mses a two-component coolant. Class
17, No 178031
SOURCE: Izobreteniya, promyshlennyye, obraztsy, tovarnyye znaki, no.
4, 1966, 24
TOPIC TAGS: refrigeration equipment, coolant, vapor condensation, gas
compression,
refrigerant gas
ABSTRACT: This Author's Certificate introduces.a refrigeration unit
which uses a two-
component coolant. The device contains a compressor for the
two-component vapor, a
water- or air-cooled condenser where the high-boLling component is
li~quified, a vapori.
zing condenser for liquefaction of the-low-boLling element by
vaporization of the high-
boiling component, 4 vaporizer for cold production and regenerated
heat exchangers in
which both components are recooled. The overall dimensions are
reduced and the power
indices are improved by using a booster at the input of the
ccmpressor for compressing
the vapor of the low-boLling component.
UDC: 621.574.9-146.2

CHAYKOVSKIY, V.G.
Eliminate shortcomings in the system of loading arches,
Transp.
stroi. 14 no.4:59-60 Ap 164. (MIRA 17%9)

A.JTHORS: Byg, L.S,,,and Chaykovskiy, V.G. 120-6-11/36
T'MB: On the Working Li.e of Argon-Ck(OCH 3)2 Filled Counters
of Radioactive Radiation (0 sroke sluzhly schetchikov
radioaktivnogo izlugheniya s argon-metilalevym napol-
neniyem)
PERIODICAL: Fribory i Tekhnika Eksperimenta 195~, No.6.
pp. 49 - 54 ?USSR -
i~,>~'TRACT: The working characteristics of self-quenching
counters
deteriorate with age. A number of workers (Refs. 1 and 2) have
noted that these changes are: increase in the threshold voltage,
increase in the plateau glope, etc. Such changes are usually
observed after 107 to 10 pulses a~d determine the working life
of a counter. High-voltage self-quenching GM-counters are
usually filled with an inert gas such as argon plus a small
proportion of some organic vapour such as ethyl alcohol, iso-
pentane and others. At the moment of recording of an ionising
particle, dissociation of the organic molecules takes place.
As a result of the irreversible breakdown (in the discharge)
of the organic molecules the working characteristics of the
counter c4ange. ccording to the existing ideas in each dis-
harge 10'; to M 6 organic molecules are broken down. In
Card 1A

120-6-11/36
On the Working Life of Argon-C%(0CH3)2 Filled Counters of
Radio-
active Radiation.
counters of normal dimensions there are 10 20 molecules of the
quenching material *Rd therefore all these molecules ought to
dissociate after 10111 counts. However, normal working of the
counter is disturbed much earlier. In the present papew the
authors give results of a mass-spectrometric analysis of the
gas mixture during the working of the counter. The counters
which were used for this experiment were of the usual co-axial
form. The tungsten anode was 0.1 mm. in diameter and had a
working length of 80 mm. The cathode was in the form of a
layer of copper deposited on the inner wall of the glass
envel-
ope. This system is shown in Yig.l. Counters were filled
with 15% (by pressure) chemically pilre CH2(OCH 3)2 and the
pressure was brought up to 100 mm HS by the addition of argon.
Two groups of counters were used. The first group consisted of
60 counters and was used to study changes in the chemical
composition of the filling and the characteristics of the
counter as functions of the number of counts. The second
group,
consisting of 70 counters, was used for both the above
purposes
Card 2/4

120-6-11/36
C.~. the Working Life of Argon-CH2(OCH3)2 Filled Counters of
Radio-
a,Aive Radiation.
and the study of changes in the amplitude and the count ate as
functions of the number of recorded counts. Results of these
measurements are summarised in Figs. 2, 3, 4, 5 and 6. Fig.2
shows the change in the characteristics of counters as a
function of the number of recorded counts. It can be seen that
the threshold voltage increases by 50 to 60 volts, the length
of plateau decreases by about 260 V and the plateau slope
increases from 2 - 3 to 18 - 20% after 2 x 100 counts. Mass
spectrometric analysis has led to the conclusion that the amount
of dissociating organic molecules is proportional to the number
of recorded counts. In the gas mixture of the counter, sub-
stances with mass numbers 16 and 28 appear, and these worsen
t!.Le counter characteristics. There are reasons to suppose that
Ghe mass number 16 corresponds to oxygen which has a strong
influence on counter characteristics. The ageing of the counter
is connected not only with the dissociation of the organic
component but also with changes in the surface of the cathode.
The present experiments have shown that, with the right exploit-
ation of argon-CH2(OCHI,)2 filled counters, they can be used for
Card3/4 recording up to (1 to 2") x 108 counts.

120-6-11/36
On the Working Life of Argon-CH2(OCH 3)2 Filled Counters of
Radio-
active Radiation.
S.A. Vekshinskiy and M.I. Men'shikov collaborated in this work.
There are 6 figures, 2 tables and 6 references, 2 of which
are Slavic.
SUBMITTED: May 3t 1957.
AVAIIABLE: Library of Congress
Card 4/4

SOV/120-59-1-15/50
AUTHOR: Chaykovskiy, V. G.
TITLE: Thermal Stability-of Halogen Counters (Termostoykost' galog-
ennykh schetchikov) -
PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 1, pp 65-66
(USSR)
ABSTRACT: Three groups of counters were investigated;
Group I. In this group the counters had nickel cathodes,
10 mm ii! diameter, kovar anodes 0.5 mm in diameter, the work-
ing length of the anode beingogO mm. They were outgassed
and subsequently heated to 25 in chlorine. In order to
remove volatile products, additional heating at 140-1500C
was carried out before the final filling at a pressure not
-4
exceeding 10 mm Eg. The counters were filled with a mix-
ture of Ne, Ar (0.1%) and Br2 (0.03%) at a total pressure
of 600-650 mm Hg.
Group II. Counters of identical construction. The addit-
ional heating to 1500C not carried out.
Group III, Counters of Type STS-1 with the geometrical di-
mensions as the above but having stainless steel cathodes.
Figs 1-3 show the results obtained. Fig 1 shows the depen-
Card 1/3 dence of the threshold voltage on temperature for the CTC-1

Thermal Stability of.Halogen Counters
SOV/120-59-1-15/50
counter (2) and the Group I counter (1). Fig 2 shows the
dependence of counter characteristics on temperature of the
surrounding medium. Ciiiwe 1 shows the dependence of the be-
ginning of the plateau on temperature for a STS-1 counter
and a Group I counter, and Curve 2 shows the dependence of
the end of the plateau on temperature for a similar pair of
counters. Curve 3 shows the dependence of the efficiency
of Group I counters on the temperature of the surrounding
medium. It is concluded that changes in the characteristics
of halogen counters as the temperature increases are due to
the evaporation into the working volume of the products of
interaction cC the halogen with the material of which the
counter is made and desorption of excess chlorine. Prelim-
inary removal of these products by heating,extends the thermal
Card 2/3

SOV/120-59-1-15/50
Thermal Stability of Halogen Counters
stability of thecounters up to 170-2000C. There are 3
figures and 2 Soviet references.
SUBMITTED: November 21, 1957. -
Card 3/3

o5435
SOV/120-59-3-6/46
AUTHORS: Dmitriyev, A. B., Tolchenov, Yu. M., Filatov, A.
I~,
and Chaykovskiy, V. G
TITIE: Coroi~-a-Cotnt-01~6-Tf~~bngly ionising particles
(Koronnyyeschetchiki sillnoioniziruyushchikh
chastits)
PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 3,
pp 35-40 (USSR)
ABSTRACT: A description is given of a number of corona
counters
designed on the basis of the work reported in Refs 3 and
4. The SAT-7 a - particle counter is shown in Fig 3.
It consists of a glass envelope with a ferrochrome ring.
A 10-*ll It thick mica plate is attached to this ring and
forms the end-window of the counter, The ring serves as
the output contact for the metallic cathode which is
evaporated onto the glass and the mica. The anode is
in the form of a hemisphere 1 mm. in diameter (in Fig 3,
1 is the glass envelope, 3 is the anode, 4 is the
cathode, 5 is the ferrochrome ring, and 6 is the mica
window), The SAT-8 counter is designed to measure the
Card 1/4 intensity of beams of strongly.ionising
particles, Its

SOV/120-59-3-6/46
Corona Counters of Strongly Ionising Particles
cathode is in the form of a metallic cap made from
ferrochrome which carries a mica window 3 4 IL thick
and 4 mm in diameter. The anode is similar to that
in the SAT-?. The slow neutron counter SNM-9 has the
usual cylindrical geometry, Its cathode has a diameter
of 18 mm. and is made of stainless steel. The element
sensitive to slow neutrons is a layer of amorphous
boron deposited on the inner surface of the cathode,
The thickness of this layer is grj8ter than the ranGe
of the products of the reaction B (na) Li?. All the
three counters are filled with a mixture of neon with
a small admixture of argon (not greater than 2%). The
corona noise usually does not exceed 5 mV in SAT-?
15 MV in SNM-9 and 25 mV in SAT-8 counters and can be
easily cut off with a suitable discriminator,, The
maximum amplitude of the working pulses is 100 -' 300 mV
which corresponds to a gas amplification coefficient of
Card 2/4 about 1000 -:- 3000,, Fig 5 shows the dependence
of' the

0505
SOV/120-59-3-6/46
Corona Counters of Strongly Ionising Particles
a - particle pulses and noise on the supply voltage in
the case of the SAT-7 cou4ter. Best results are obtained
with a load of 5 x 1OF34 -~'-109 ohm. With such load
resistances,'the voltage ranges are 450-.'1000 and 700
2500 volts for the SAT-8 and the SNM-9 counters
respectively. The plateau slope is practically zero.
In the case of the SAT-7 counter a 1 Meg resistance is
sufficient and the length of the plateau is 300 -*
450 volts. The counters have a resolving time of about
1 ji see. The efficiencies are as follows:-
SAT-7, 25 -' 30% (uncollimated 5 Mev alpha particles),
SAT-8. 100~(uncollimated 2 Mev alpha parti-c:les),
SNM-9, 0.25% (thermal neutrons).
L. S. Eyg, L. K. Pyatibokov, V. I. Vinogradov, V. I.
Popov, V. T. Fedoseyev, V. N. Korneyev and L. A.
Card 3/4 Fomina are thanked for their assistance,

0505
SOV/120-59-3-6/46
Corona Counters of Strongly Ionising Particles
There are 7 figures and 8 references, 5 of which are
Soviet (1 a translation from English), and 3 English~
SUBMITTEDg April 25, 1958
Card 4/4

05438
SOV/120-59-3-9/46
AUTHORS: Dmitriyev, A. B-, Peskov, D. I.,, Kheyfets, A.B.
and
Chaykov.skiy, V. G.
TITILE: Dose Characteristics of Low Voltage Halogen
Counters
(Dozovyye kharakteristiki nizkovolltnykh galogennykh
schetchikov)
PERIODICAL: Pribory i tekhnika eksperimental 195.9, Nr 39
pp 47-49 (USSR)
ABSTRACT: The dose characteristics of the low-voltage
halogen
counters STS-1, STS-2, STS-5, STS-6, STS-8, SGS-5,
SGS-69 SBT-10 and SGS-7 have been measured and are now
reported. The parameters of the first six counters
were given by Dmitriyev (Ref 2. a review paper), The
SGS-6 counter is similar to the SGS-5 but its cathode
has a longer working length. The SBT-10 s designed
to detect soft P-radiation and has a 30 cJ mica window,
It consists of ten sections placed in a common envelope.
The cathode of each section is in the form of a half-
cylinder, 5 mm in radius. The anode of each section
is 55 mm long and has a separate output terminal. In
the SGS-7 counter the cathode and the anode are in the
form of discs 10 mm and 0.5 mm in diameter, respectively,
Card 1/4 The gap between the discs is 1 mm. The electrical

05438
SOV/120-59-3-9/46
Dose Characteristics of Low Voltage Halogen Counters
parameters (threshold, length-and slope of the plateau)
of SBT-10,, SGS-6 and SGS-7 are analogous to the parameters
of all the low voltage halogen counters described in Ref 2.
Table 1 gives the main parameters of the counters. The
first colilmn gives the type of the counter, the second
column the cathode diameter in mm and the third colimn
the working length of the anode in mm. The counting
rate was measured using the PS-10000 meter, the input
sensitivity being 0.1 V and the resolvingotime 1 11sec.
The irradiation was carried out using Go sources whose
activity was 0,01-5 Ra g equiv, The dose was determined
to within + 10~6~ In the experiments the SBT-10 counter
was connecTed as shown in Fig 1. while all the remaining
counters were connected as shown in Fig 2. The dose
characterist cs and the plateau slope were determined
using R = 1A Ohm, Figs 3 and 4 show the dose character-
istics of the'above counters measured at the working
voltage. It is clear that in the majority of the counters
there is a maximum counting rate on the dose characteristic,
Card 2/4 This is explained by the considerable reduction in the

05438
SOV/120-59-3-9/46
Dose Characteristics of Low Voltage Halogen Counters
pulse height at-large counting rate. Under these
conditions the potential difference across the counter
is not fully established. Since halogen counters give
pulses with unequal amplitudes (Ref 3) it follovis that
some of the pulses may fall below the threshold of the
detecting device. Table 2 gives the dose characteristics
of the counters, where column 1 gives the type of the
counter, column 2 the dose range in lir/sec, column 3
gives the counting rate at the appropriate dose in
pulses/sec and column 4 the maximum counting rate in
pulses/see. Table 3 gives the dependence of the plateau
slope on the dose, in which the first column gives the
dose in jLr/sec and the second and third columns give
the plateau slope in percent/Volt for the STS-5 and SGS-5
counters, respectively (the headings of columns 4, 5 and
6 are the same as those of 1, 2 and 3). Table 4 gives
the resolvIng time of the counters. Column 1 of this
table gives the type of the counter, columns 2 and 3 the
resolving time in jisec at 100 pulses/sec and at maximum
counting rate, respectively (columns 4, 5 and 6 have the
Card 3/4 same headings as 1, 2 and 3). The load resistance
has a

05438
SOV/120-59-3-9/46
Dose Characteristics-of Low Voltage Halogen Counters
great effect on the dose characteristics (Figs 5 and 6
in which the curves are plotted in ascending values of
the load resistance). In the detection of large doses,
the anode voltage must be well stabilized because in
this case the plateau slope is considerably increased.
It is noted that the plateau slope and the character of
bits change with increasing counting rate differs from
counter to counter since it largely depends on the
technology of manufacture and the conditions under which
the counter is used. However, it follows from Table 3
that the plateau slope increases with increasing dose
(i.e. increasing counting rate).
There are 6 figures. 4 tables and 4 Soviet references9
one of which is a tianslation from English.
SUBMITTED: April 4, 1958
Card 4/4

c26. a2c2 9 k
i
AUTHORS.-' Tolchenov,
20680
S/120/61/000/001/014/o62
E032/E114
Yu.Me, and Chaykovskiy, V.G,
TITLE: A Gas Discharge Gamma-Ray Detector With a
Logarithmic Sensitivity
PERIODICAL: Pribory i tekhnika eksperimenta, 1961, No*l, PP-51-52
TEXT: The detector (counter) is in the form of a two-
electrode gas discharge system with a strongly nonuniform electric
field. The counter can be filled with any of the non-self-
quenching gases normally used in Geiger counters. P1g.1 shows
the arrange~nent for the recording of y-rays by the corona
counter.
A voltmeter which measures the potential difference between the
electrodes is connected in parallel with the counter. In the
simplest case, an electrostatic voltmeter can be employed. if
the applied voltage exceeds the voltage necessary to initiate the
corona discharge, and the load resistance R is greater than or
equal to 109 ohm, then in the absence of ionizing radiation the
voltmeter will indicate a constant voltage Vs. The introduction
of a y-radiation leads to an increase in the current through the
counter, and consequently the voltage indicated by the voltmeter
Card 1/ 6

20680
S/12o/ 61/ 000/001/ 01 4/o62.
E032/E114
A Gas Discharo; e Gamma-Ray Detector With a Logarithmic
Sensitivity
changes by, say, &V. LW depends logarithmically on the
intensity of the y-radiation, and its magnitude reaches 100
volts
or more when the intensity changes by an order of magnitude.
Qualitatively, the operation of the counter can be described as
follows. When the applied voltage is less than VS, the counter
operates as a proportional counter. Under these conditions the
volt-ampere characteristics are as shown schematically in Fig-3.
In the absence of y-radiation the volt-ampere characteristic has
the form of a rapidly rising curve which for V > Vs goes over
into the usual characteristic of a corona discharge, which is
not
very dependent on the y-ray intensity. The dotted lines in Fig-3
show the dynamic characteristics of the counter for various
applied voltages and loads OMI > R2). The introduction of
radiation leads to the displacemat of the working point from A
to B (or from A, to Bt, etc.) and the current passing through
the circuit changes from ii to some value i which is determined
by the y-ray intensity. At the saine time, the anode potential
decreases by 6V = V - Vs. The new position of the working
Card 2/6

20690
S/1.20/61/000/001/014/o62
E032/E114
A Gas Discharge Gamma-Ray Detector With a Logarithmic
Sensitivity
point (HO) corresponds to the proportional region. Two factors
influence the change in the current, namely, an increase in the
y-ray intensity gives rise to an increase in the cut-rent, but
on
the other hand this increase in the current in the proportional
region reduces the gas amplification coefficient (Tolchenov,
Ref.2). As a result, the dependence of &V on the y-ray
intensity is logarithmic. As can be seen from Fig-3, the higher
the supply voltage the lower the load resistance R and the
higher the upper working limit of the instrument. Fig.2 shows
the change in the anode voltage &V as a function of the y-ray
intensity (r/hr) for different values of R (ohms) as shown.
These results were obtained with a cylindrical counter, 26 mm
i=
diameter and 130 mm long, filled with a mixture consisting of
Ne + 2% Ar at 500 mm Hg. The value of Vs was 700 volts and the
applied voltage was 750 volts. The lower working limit under
these conditions was about 0.1 r/hr. Fig.4 shows the change in
the anode voltages &V as a function of the y-vay intensity
(r/hr) for a counter 26 mm in diameter and filled with helium,
Card 3/ 6

2o68o
S/12o/6l/ooo/00.1/014/062
E032/Eii4
A Gas Discharge Gamma-Ray Detector With a Logarithmic
Sensitivity
argon and krypton respectively (pressure = 300 nun Hg).. With a
suitable design, a range of 0.01 to 1o6 r/hr may be covered.
Acknowledgements are expressed to Yu.N. Sachkov for discussing
the
method of measurement, and to V.N. Korneyeva for assistance in
the
experiments. V.G. Khrushchev, K.A. Trukhanov and A.D. Turkin are
thanked for laboratory facilities provided.
There are 4 figures and 2 Soviet references.
SUBMITTED: February 1, 1960
Card 4/6

S -M
I 10 ~

20680
S/120/6.1/000/ooi/oiW62
~EOWE114
A Gas Discharge Gamma-Ray"Detector With a Logarithmic Sensitivity
AV
w

ACCESSION NR- AP40068 Iz
SIOIZO/631000/0061000510OIZ
AUTHOR: Tolchenov, Yu. M.; Chavkovskiy, V. G.
TITLE: Corona counters for slow neutrons
SOURCE: Pribory* i tekhnika eksperimenta, no. 6. 1963, S-12
TOPIC TAGS: corona counter, neutron detector. slow neutron,
radiation
measurement, neutron counter, neutron detection, slow neutron
counter
ABSTRACT: A short description of Soviet-make corona. counters is
offered.
Their advantages over proportional counters are seen as: (1)
High gas -
amplification factor not much affected by variations in the
supply voltage;
(2) Stable operation in the presence of a strong gamma
-radiation background;
(3) High theirnal stability. Table l in Enclosure I gives the
fundamental charac-1
teristics of the couniers; Table 2.esents schematic data for the
circuit
diagram shown in Enclosure Z. T7e high gas -amplification factor
of the corona
ceird I

ACCESSION NR.' AP4006812
counters permits using low-sensitivity (30-50 mv) recording devices. it
is
claimed that corona counters can replace proportional counters in most
applications. Orig. art. has: 12 figures, 3 formulas and 2 tables.
ASSOCIATION: none
SUBMITTED: 29Jan63 DATE A(^Y. 24J&n64 ENCL: OZ
SUB CODE: NS NO REF SOV: 004 OTHER: 002
cam 2/f

ACC N.R: AP5027009 SOURCE CODE: UR/O12O/65/OOo/o05/o0T1/OO73
AUTHOR: Klyukvina, Ye. F.; Chaykovq%_ V,. G. Rikollekiy, A. Po;
Yevlanov. I. Ya.
ORG, none
TITLE: Construction and technical.characteristics of a proRortipnal
Rgunter
SOURCE: Pribory i tekhnika eksperimenta, no. 5, 1965, 71-73
TOPIC TAGS:, gas discharge.counter, proportional counter
ABSTRACT: A proportional counterdesigned for detection of 1-10-kev
x-radistion is,
described. To meet the requirement of a large-area input aperture of
minimum thick-..,
ness, the design contains acathode equipped Iwith two 10-p Al film
apertures 25 x 16 m
each. To reduce attenuation of fluorescent radiation by the
surrounding air, the
counter itself is placed in a vacuum while the remainder of the unit
is sxxbjected to'
normal atmospheric pressure. Provisions are made,for connecting the
output of the
counter to a scintillation counter.. The active elements of the
counter are a stain-*
less steel cylindrical cathode 25 mm in diameter, a tungsten wire
anode 0.05 i3~m in
diameter, and a gas mixture of 90% Ar and 10% CH4 which is passed
through the counter
'interior at a rate of 5-20 cm3/min. Fig. 1 shows the output pulse
height as a fun.c-
tion of the.ap~lied potenti al,' The linear region corresponds to a
gas avalanche fac-
tor range of (1.3-1.6) x 104. The efficiency of the counter ab a
function of wave-
length is shown in Fig. 2. The effectiveness of the counter in
detecting hard radia-
Card 1/2 UDC: 539.1.o74.822.3:621.386

L 4968-66

CHAYKOVSKIY V.G.
Repair of bridge spazwo Pat' i put.khos. 7 no.1:23 16;. (MIRL
16:3)
1. Nachallnik proizvodstvenno-tekbnichookogo otdela mostopoyesdo6
stantsiya Brest Belorwmkoy-dorogi,
. (Railrcad, bridgew-Mmintenance and repair)

CHAYKOVSKIY, V. 1.
CHAYKOVSKIY, V. I.: "An analysis of the
interference-reBiStance of
the autocorrelation metbod of receiving impulse
signals". Kiev,,
15~559 Min Hig7her Education Ukrainian SSR. Kiev
Order of TA-mi n
Polytechnic Inst,, Chair of Radio Receiving
Equipment* (Dissertation
for the Degree of Candidate MIECHNICAL Sciences)
SO: KhI Letopis' No& 51, 10 Decenber 1955

LI.SSR/Electronics
Card 1/1
Author
Title
lnfor,-,ation Theory
Periodical
Abstract
Pub. 90-2/9
FD-2494
: Chaykovskiy, V. I., Active Member, kNORiE
: Reception of pulse signals by the mutual correlation method
: Radiotekhnika, 10, 16-20, Jun 55
: Determination of the ratio of signal to fluctuating noise
during
the reception of pulse signal, applying the mutual correlation
method is discussed. The aim of this research was to analyze
the
noise rejection of pulse signal reception with the aid of the
mutual correlation method. The values for the signal-to-noise
ratio thus-obtained are compared to the corresponding values
of
the output of an ideal band-pass filter. An expression is
derived
which shows that the signal-to-noise ratio at the output of a
correlation receiver under certain conditions is more
favorable
than that of an ideal filter. Graphs. Five references: 2
USSR
institution : All-Union Scientific-and Technical Society of
Radio Engineering
and Electric Communications imeni A. S. Popov (VNORiE)
Submitted : November 16, 1954

IA r/x c X)!~, r-- I yV,
.Category : USSR/Racljophysics - Statistical phenomena in
radiophysics 1-3
Abs Jour : Ref Zhur - Fizika, No 1, 1957, No 1808
Author : Chaykovskiy, V.I.
Title : Rolbe Rejection o a Filter Auto-Correlation Receiver for
Pulse Signals
Orig Pub : Radietelchnika, 1956, 11, No 4, 20-30
Abstract The signal-to-noise ratio is determined at the output
of a simple cor-
ri,6ation receiver, which has aq averaging element consisting of
a low-
pass filter. By signal-to-noi~e'ratio is meant the ratio A of
the square
of the maximum increment in the de component at the output of
the receiver
in the presence of a useful signal to the average square of the
fluctuations
at the output in the absence of a useful signal. Assuming that
the fluctu-
ation noise has a uniform spectral density, and assuming the
input (band)'
filter of the receiver and the averaging element to be ideal
filters, the
author derives an expression for the dispersion of
theLlIuctuations and for
the maximum value of the increment of the dc component at the
output of the
system under investigation. These values make it possible to
determine A.
It turns out that the opti;mum value of the time delay'r at
which A = Amax,
depends on the bandwidth -of the input filter. If the
input-filter has an
optimum bandwidth, the above system has no advantages over a
receiving set
with a square-law detector. Increasing the Vandwidth of the
input filter
Card 1/2

Category : USSR/Radiophysics - Statistical phenomena in
radiophysics 1-3
Abs Jour : Ref Zhur - Fizika, No 1, 195T No 3BOB
i
(4~) a.,;i- 43, where a is the duration of the usef~xl-signal
pulse), one
can obtain a certain improvement in the noise rejection (up to
a factor
of 2) over a receiver with a square-law detector-.
Card : 2i2

PA - 2293
AUTMR1 KAMOVSKrrX,I,., CUMVBKIY,V.I,, Regular Members of the
Society
for Radiotechnoiogy.
TITM The Method of Increasing the I-mmity frcs Disturbance of
the Auto-
correlation Reception of ImptAlso Signals. (Xetod povysheniya
pamek-
houstoychivouti avtokorrelyatsionnogo priyama impul'anykh
signaloys
Russian).
PIWIMICAL: nika, 1957, Vol 12, Nr 2. pp 22-27 (U.S.S.R.)
Received: 4 / 1957 Reviewed: 4 / 1957
ABSTRACT: It is shown that, with the aid of a'samewbat
complicated construction
of the correlation reception system, it in possible to
eliminate the
usual faults and to increase the J-1nity from disturbance of
the
system. (Usual faults: if time of delay in greater than the
optimum
time, the immunity from disturbance of autooorrelation
reception
decreases to zero if the time or delay boomen equal to the
duration
or the useful aIignal).'This in attained by switching an a
synchronous
key-devioe into one of the channels of the system. The range of
application in, however, limited by the class of the
synchronous
pulse system. kt first it in shown merely by approximation
that the
dispersion of the noise integral is diminished in the case of
re-
generative reception* and that therefore the 4-unity from
disturb-
anoe increases in the moo of the method suggested. This is
proved
with accuracy in the course of the second part of the paper.
Yrom
cut 1/2 the attached diagram it may be seen that a
regenerative autooorrela-

PA - 2293
The Method of Increasing the Immi ty f rom Disturbanov of the
Auto-
correlation Reception of Impulse Signals.
tion. system warrants an additional improvement of immunity
from dis-
turbance amounting, to = 30% in the case of the optium value
of the
transparency band of the input filter and a proper selection
of the
time of delaye whereas the latter is somewhat less than the
immimity from disturbance of an integral system in the came of
the
ordinary autooorrelation system. Prom the diagram it may
further be
seen that in the case of a brgadening of the transparency band
the
aforementioned improvement increases still. further and
becomes equal
to two in the case of a band of infinite breadth. (5
illustrations).
MODUTIM. Not given
PROM= Dr:
SUAKITM: 10 100 1956
AVAUANA Library of Congress
Card 2/2

SOV/142--58-5--5/23
~490)
AUTHORi Chaykovskiy, V.I.
TITLLPt
Noise-killing FeatUre Of an Integral Self-Correlated Reception
System
PUTODICALs Izvestiy vyssikh uchebuykh zoved9a$yr%diotekhnika,
1958, Nr 5,
pp 5511-554 (USSR)
ABSTRACT: The article presents one of the possible variants of a
correlated
reception system , an integral self -correlation system with
detect-
ing of the impulse signal and black-our. ox tne Iluctuating dis-
turbance. Following the principal scheme of the elementary self-
correlating reception system (Fig.1), the last apparatus has to
register the short-time self-correlation factor miscellany of the
signal and the disturbance y (t). The~presence of a synchroniza-
tion channel allows the realization of the coincidence of the
neutralization interval T with the interval of active transmis-
sion. The advantage of the signal disturbance relation at the '
output of this receiving syMtm in comparison with the correspond-
ing relation, at the output -of & normal integral receiving
system
Card 1/2 has its place only at the transparency band of the
input filter,
I

SOV/142-58-5-5/23
Noise-ki1ling Feature of an Integral Self-Correlated
Reception System
pushed to an optimum by Siforov (jdW d >8.6). The maximum
advan-
tage appears as a conserquence of weakening the disturbances
at the
installation output, combined with a barely'existing
reduction of
the useful signal. The disadvantage of the system is, that in
case
of absent synchronism between the intervals of useful
transmission
and the intervals ofineutralization, not all the advantages
of the
method appear.,The article in reco=ended by the Kafedra radio-
priemnykh ustroystv KiyevLjjq7W!n& Lenina politekhnicheskogo
instituta (Chair if ip ices at the Kiyev Polytechnical
Institute of the Order of Lenin~. There are I block diagram, I
graph, 15 equations and 6 references, 4 of which are Soviet
and 2
,English.
SUBMITTEDs February 21, 1958
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9(2)
SOV/142-58-6-4/20
AUTHOR:
Chaykovskiy, V.I.
TITLE:
Determination of
the Minimum Detectable Ratio of

Signal to Noise at the Input of a
Radiometer (Opre-

deleniye minimallno razlichimogo otnosheniya sig-

nala k pomekhe na vkhode radiometra)
PERIODICAL:
Izvestiya vywhikh
uchebnykh zavedeniy - Radiotekh-

nika, 1958, Nr 6, pp 659-664 (USSR)
ABSTRACT:
The purpose of the article is to determine the cor-

relation
between the intensity of a treshold signal

of random nature, acting on
the input of a radio-

meter with a square-law detector, and the
probabili-

ty of detecting this signal at the output of a re-

gistering
instrument during a given time of analysis,

and with a known intensity
of noise in the radio-

meter channel. The probability of correctly
deter-

mining the fact of the absence or presence of,the

desired signal
is a function of signal intensity,

noise intensity, and the time of
analysis. Deter-
Card 1/4
mination of this functional relationship is
one

BOV/142-58-6-4/20
Determination of the Minimum Detectable Ratio of Signal to Noise
at the Input of a Radiometer
purpose of the article. A block diagram of the
radiometer circuit (Figure 1), consisting of in-
put filter, detector, averaging device, and re-
gistering instrument, is very briefly discussed
by the author. Readings of the registering instru-
ment are proportional to the output voltage of the
averager, and as both signal and noise are of a
random nature, these readings will also have a
random nature over a finite time of analysis.
Readings will fluctuate about a certain average
value, equivalent to the value of the average power
of the mixture of desired signal and noise. Pres-
ence or absence of the desired signal can be de-
termined from the magnitude of a particular value
of reading; a reading higher than a certain con-
trol value corresponds to the presence of the Sig-
nal, and vice versa. Taking the probabilities of
Card 2/4 correctly determining the presence or absence of

SOV/142-58-6-4/20
Determination of the Minimum Detectable Ratio of Signal to
Noise
at the Input of a Radiometer
the desired signal as equal, the author derives
expressions for the minimum detectable ratio of
signal to noise for a radiometer with the averag-
ing device, and a radiometer with a low-pass filter
in its place (eq. 10,11). It is concluded that
as small a signal as desired may be detected pro-
viding sufficient averaging time or a sufficient-
ly narrow pass-band in the averaging filter; at
a given signal/noise ratio, an increase in the
probability of detecting the desired signal de-
mands a corresponding increase in the duration of
the analysis; improvement of the signal/noise
ratio at the output of the radiometer in comparison
with the corresponding ratio at the input is greater;
the greater the relative analysib time, or in the
case of the radiometer with a low-pass filter, the
less is the ratio of the band of the averaging
Card 3/4 filter to that of the input filter; with appropri-

SOV/142-58-6-4/20
Determindtion of the Minimum Detectable Ratio of Signal to Noise
at the Input of a Radiometer
ate choice of averaging interval (time) and pass
band of the averaging filter the maximum sensitiv-
ities of a radiometer ideal integrating device
and a radiometer with low-pass filter do not prac-
ticall-y speaking differ from each other. This
article was recommended by the Kafedra radiopriygm-
nykh ustroystv K1,yevskogo ordena Lenina politekh-
nicheskogo instituta Pair of Radio - Receiving Equip-
ment of the YJ4w Order of Lenin Polytechnical In-
stitute). There is 1 block diagram, and 4 refer-
ences, 2 of which are Soviet and 2 English.
SUBMITTED: February 21, 1958
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24374
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E192/Z382
AUTHOR: Chaykovskiy, V.I.
TITLE; Methods of Experimental Determination of
Correlation Functions
PERIODICAL: Izvestiya vysshlkh uchebnylch zavedeniy,
Radiotekhnika, 1960, Vol- 3, No. 5, pp. 425 - 434
TEXT: The mixed moment of the second-order W-ri) , which
represents the average value of the product of two random
functions fl(t) and f,(t) shifted in time by an amount
~M , is of importance in 4.110 statistical theory of communi-
cations. Pov the stationary processes this moment can be
obtained as a result of the time-averaging of the product of
these two functions, shifted in time by in the following
form +T
F12(,t) = lim f1(t)Yt + 't-,) dt
T_,tcx,~ 2T
_T
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Methods of .... E192/E382
The ergodic theorem shows that M(L-) and FCO are
equivalent. In the case when f I(t) = f2(t) , Eq. (1)
represents the so-called autocorrelation function F 11 (-"') .
It is known from the Wiener-Khinchin (Ref. 3 - A.M. Yaglom,
UMN, 1952, 7, No. 501), 3; Ref. 4 - U.R. Bennet, Basic Concepts
and Methods of Theory of Noise in Radio-engineering,
Sov.Radio,1957)
that the autocorrelation function of a random process can
also be represented as
+ M,
F11h.) PW cos w'%, dw
- Ck--
where PW is the energy spectrum of the function. The
equipment employed in the evaluation of correlation functions
can be divided into three groups, depending on the underlying
principle of their operation.,
A) the devices based on the principle of the two-dimensional.
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24374
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E192/E382
probability density;
b) the devices employing the principle of the spectral
function, and
c) instruments based on the multiplication principle.
As regards the devices of the first group, their basic element
is a system for determining the two-dimensional probability
density W2(fIf2t in each point of the three-dimensional
space fl, f2, -c, This usually consists of a device
determining the conditional probability density of the signal
f1 (or f.) for a fixed 'r- and an instrument determining
the unidimensional probability density of the signal f.
(or f2). In this type of equipment the signal fIand
signal f2 . delayed by an amount ^t~, , are applied to the
device which determines the conditional probability den.9ity
W(f 1/f2) which, together with a multiplier M, I integrator I
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Methods of .... E192/E382
a generator of linearly changing voltage LG, forms a system
evaluating the conditional average value of f I in the
interval of f, , which comprises the region of the most
probable values of the process and its vicinity. A second
channel of this type of correlator consists of a device
determining the probability density of the quantity f2w(f 2)
a multiplier M2 and another generator of linearly changing
voltage LG, . The signal at the output of the second
channel is proportional to the quantity f 2 W(f2) . The
voltage of LG2 changes within the same limits as the voltage
of LG, but the rate of its change is much slower, so that the
voltage of LG, can be regarded as constant during one period
of LGIL a The generators LGl, LGV. and integrators I, and I.
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Methods of .... E192/E382
are synchronized by a signal provided from a synchronising
circuit. The output signals of the two channels are
multiplied by a multiplier M3 and are integrated with respect
to f2 in order to determine the average value of fl(t)f2 (t 4
+ M), which is equal to the correlation functlon for a fixed-~_-.
+00 +010 1
M (PC) f2w(fddf2_~ fJLW(fl./f2)df,
If the delay time C. is varied, the signal at the output of
the device'represents, therefore, the cross correlation
function for f. and f2 . The principle of a corvelator
can be based on Eq. (2). In this case, the equipment consists
of an automatic spectrum analyser which produces the amplitude
spectrum of the input signal; this is followed by a squaring
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Methods of .... 1:192/E382
circuit where the power spectrum is obtained; the amplitude
spectrum of the latter is then produced by another automatic
spectrum analyzer which is equivalent to the autocorrelation
function of the investigated process. The correlators based
on the multiplication principle can be of two types: those
operating sequentially and those performing instantaneous
analysis. In the second case, it is necessary to employ a
set of fixed delay elements for N&T, with a monotonically
increasing delay. As regards the correlators of the first
type, these simply consist of a delay circuit, a multiplier
and an integrator (with an indication circuit). This
correlator is much simpler than that based on the instantaneous
analysis principle. However, the sequential-analysis correlator
has the disadvantitge that the time taken by it for determining
the value of the correlation function is n times longer
than that of the more complex correlator. Multiplier
correlators can also be designed differently. Thus, for
example, the correlator can be constructed as follows. The
investigated signal f and a portion of the signal f
1 2
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Methods of .... E192/E382
(with suitable polarity),j76 applied to a subtraction circuit
i!!~, ; the amplitude and polarity control of f2 is performed
by means of a calibrated sy=.netrical potentiometer and a phase-
inverter circuit. The difference produced at the outputaCA. is:
A(t) = f1W -.ar 2(t)
and this is applied to a squaring circuit, an integrator
and, finally, the indicating device. it can be shoi-m that the
minimum of the mean square value of
2
A (t) corresponds to the case when the multiplier a is
equal to the correlation coefficient 11,,, Consequently,
the measurement of the correlation coefficient is equivalent
to the setting of the above instrument in such a way that its
indicator gives a minimum; the 6oefficient a is then read
on the calibrated scale of the potenxiometer. The above
multiplier correlators are not suitable for the measurements
of the autocorrelation functions of slowly changing processes*
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In this casev it is possible to base the correlator on the
following formula:
N
F 5' anh11 (t)
n=O
The resulting correlator consists of N channelsi the
investigated signal fIis applied to the input of these
channels and their outputs produce expansion coefficients
a a a Each channel consists, therefore, of a
of JL9 n
filter having a suitable impulse response hn(t) , a
multiplier N nand an integrator In . The correlator also
comprises another set of filters having impulse response hof
hjq h. whose input is excited by a short pulse 6(t)
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Consequently, periodic signals corresponding to hol his
h2v ... are formed at the output of each filter. Another
set of multipliers M2 perform the multiplication of the
n
expansion coefficients a n and impulse responses hn . The
products of the multipliers are then added in a summation
circuit. The resulting signal is equivalent to the auto-
correlation function of fjL . The determination of a
correlation function can also be performed by digital devices.
In this case, each point of the correlation function is
evaluated by averaging a sufficiently large number of the pairs
of products of the values of the investigated process f(t);
the correlation function is given by
F(T) a b CO
nn
N n=1
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where a. and bn are discrete values of f(t) , shifted in
time by 'r- with respect to each other. Instruments of
this
type can have a very high accuracy (error of less than
1%).
There are 9 figures and 19 references: 9 Soviet and
10 non-Soviet. The four latest English-language
references
are : Ref. 6 - T.M. Burford and V.C. Rideont, J. Brit.
Instn.
Radio Engra., May, 1955, 15, No. 5; Ref. 7 - T.M.
Burford,
J. Applo Phys. Jan., 1955, 26, No. I.; Ref. 13 - T.P.
Goodman,
J. Applo Phys. July, 1956, 27, Noo 7; Ref. 14 - D.G.
Lampard,
P122, PC, 1955, 102, No. 1.
ASSOCIATION: Kafedra radiopriyemnykh ustroystv
Kiyevskogo
ordena Lenina politeklinicheskogo instituta
tChair of Radio-receiving Devices of the "Order
of Lenin" Kiyev Polyteelmical Institute)
SUBMITTED: December 21, 1959
Card 10/10

CHAYKOVSK.IY V red,,; POLYANSKAYA, L.O., red.; STPURODUB, T.A.,
[Determination of the parametersi of random processeslopm-
delenle pam-etrcyv sluchkinykh protsessov; sbornik statel.
Kiev, Gostekhizdat USSRj 1962. Translated from the English.
(MIRA 15:9)
(Random processes)