SCIENTIFIC ABSTRACT KOROLEV, F.A. - KOROLEV, F.YE.

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000824810016-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 14, 2000
• Sequence Number: 16
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

24(4)
OTHOR K o ro 1 e vF - A~ SOV/55-58-3-14/30
TITLEt High-lonachromatio Interference Light Filters and Their
1pplication in Technics (Interferent&ionnyye svetolilltry
vysokoy monokhromatichnosti i ikh primeneniye v tekhnike)
PERIODICALs Testnik mookovskogo univernitet&,Seriya mat--ratik-i mkh%,ek!,
sAtroiandis, fiziki, whinti ,1958,Nr 3,pp 97-116 (UISR)
ABSTRACTt The author develops a theory of the ordinary interference light
filters which allows to calculate in advance the width of the
pass band, the distance between the single pass bands, the
transmission coefficient in the maximum of the band, the
contrast factor, the aperture etc. A method for the production
of the considered light filters is proposedl dielectrio airrors
were applied instead of metallio ones whereby a 3-4 times im-
provement of the results was obtained. Furthermore a theory
of the multiplex light filters is established in 3 cases
(filters of different thicknesep equal thickness, almost equal
thickness); on the basis of the theory all the filtor para-,
meters-can be calculated in advance. High-monochromatic multi-
plex light filters with dielectric mirrors are experimentally
Card 1/2 realized. All the theoretical results are confirmed by the ex-

High-Monochromatic Interference Light Filters SOV/55-58-7/-14/30
and Their Application in Technics
perizents carried out. The following Soviet researchers are
mentioned A.V. Giltvarg, A.B. Severnyy-, S. Baranov, N. Melan-
kholin.
There are 7 figuresq and 101 referencest 14 of whioh are
Soviet, 49 American, 9 French, 9 English, 7 German, 5 Czech,
5 Japanese, 2 Italian, and 1 Brazilian.
ASSOCIATIONt Kafedra optiki (Chair of Optics)
SUBMITTEDs July 6, 1957
Card 2/2

P.A.; AnHOVv Te.N. [deceased]; MUOV, V.S.; KULIKOV, O.P.
~,
Experimental InvestigstIon of optical emission by electron@ in
a synchrotron with an energy of up to 270 Mev. Fix.abor. no.4:
24-28 158, (MIRA 12:5)
1e Fizicheqkly fakulltat Mookovskogo ordena Lenina i ordena
Trudovogo Krasnogo Znswent gosudarstvermogo universiteta
imeni M.Lonoposova.
(Electrons) (Synchrotron)

68876
B/139/59/000/05/021/026
9201/2191
AUTHORS: Tjorolay. and Zheyenbayev, Zh.
TITLE: Use of a High-Frequency Dischard with Hydrodynamic
Compression as a Light Source for Spectroscopic Analysis
of Solutions
PERIODICALs Izvestiya vysshikh uchebnykh zavedeniyt Fizikaj
1959, Nr 51 PP 134-138 (+ 1 plate) (USSR)
ABSTRACT: A new light source (Fig 2) is described; it can be used
continuously for long periods2 producing spectra of
conducting and non-conducting solutions. The light
source uses an 11.2 Mals single-electrode ("Jet")
discharge; the high-frequency oscillations are produced
by means of an oscillator UKV based on a GK-3000 tube
(circuit in Fig 1). A. quarter-wave two-conductor line
is coupled to the oscillator circuit and the high-
frequency discharge occurs at one end of this line. To
stabilise the discharge, to raise its temperature and to
ensure long working periods, air and the evaporation
Card products are pumped away through a channel bored in the
1/3 electrode. This produces a concentric flow of ambient
air towards the discharge axis (Fig 3). The resultant

68876
S/139/59/000/05/021/026
3201/3191
Use of a High-Frequency Discharge with Hydrodynamic Compression as
a Light Source for Spectroscopic Analysis of Solutions
compression of the discharge zone raises its temperature
and luminance very considerably. The electrode is
cooled by means of running water (Fig 10 and this means
that the source can be used continuously for long
periods. k solution or other substance (for example a
owdered ore, sand, etc) is placed in a Plexiglas vessel
ig 5) in which an auxiliary electrode 9 is located.
G
The auxiliary electrode 9 is fully immersed in the
solution, ore or sand, and it serves to concentrate the
discharge. The discharge power can be regulated within
wide limits so that the most convenient discharge
conditions can be used. Fig 6 shows itbe form of the
discharge under various conditionsv and Figs 7-9 are the
spectroErams obtained with a DFS-2 spectrograph using
0.1-10-7% solutions of sodium (Fig 7)? 0 .10-4-
solutions of lithium (Fig 8) and 0.01-lo'ki solutions of
Card potassium (Fig 9). The results shown in the spectrograms
2/3 are summarized in Table 11 which shows that the
Sensitivity obtainable with the source described here is

use Of 68876
3113
4 LIgh, I"gh-FrequencY Discharg 2201/jug,
9159100010510211026
source for SPectroscopice with Hydrodynamic
higher t 4nalysis Of SolutIOCOInpress on as
ares han "at Of analyses using 1
"CkMovledgelnent ZIS
his advice.
There Is Inade to flames or carbon
Ich are 9 figures, G.S. SOIntsev for
card -13 are sov, 3 1 table and 17 referencesp of
cet and 4 English.
3/3 Soviet referen es In footnotes (There are also
ASSoCIATIolV8 on P 138)
Nos-kOvsklY gosunIver.sltet 1men 14
S'jB-k!1TTj,;T): (Moscow ..State UnIvers1t 1r Imenj 'Lomonosova
February 16,, 1959

24(7), 21(l) SOV/51-6-5-2/17-1
AUTHORS Korolev, F.A. , Kozlov, B.A. a:atj Odints3v, A.I.
-~
r
TITLE On the Shape of the Line Profile in an Atomic Beam (K voprosu o
forms iconturs linii v atomnem p--:!hkq)
MiOMCAL: Optika i Spektroskopiya, 1959, V..)l 6, lir 5, pp 576-579 (USSR)
ABSIMACT: The spectral line profile produced by excitation ke.g. by electrons)
of an atomic beam was discussed theoretically by Minkowski and
Bruck (Ref 1). Xhoy obtained an expression for the intensity distriblutim
in the line assming that the exit slit of the furnace which produced
the atoraic beam was Darallal to vie line of observation and that tha
width of this slit was small. 0dintcov showed recently kRef 2) that
in order to obtain intense atomllc beams it is necessary to place the
exit slit of the flirna.-.% at :-Ight-anglse to the line of observation.
The present paper Afollows up OZInts~vls work by deriving an approximata
eslation (Eq 2) for the line shr-ps Prod-ac6l in an excited atomic bearn;

it is assumed that .6
1U24 " , *,era ai is the dimension of the
furnace slit in the direction at r1ght-angles to the line of observatior.-
i.e. its length, and t is thaf distan..:* from the furnace slit to t~,s line
of observation. Eq 2 involves a, and 8,2 which are the dimensions cf
Card 1/2 the furnace slit and the slit in a diauhra&m outside the furnace

310 f.? 149
Jk.- a 4 0 V 0-,,'/V;z I - 7 -.6 - 1/ 3 6
AUTHORS: Korolev, F.A., Kozlov, B.A. and Odintsov, AJI
TITLE. investigation of the Contour of the Cadmium Red Line. Using an
Atomic Beam y
PERIODIC.,'%L: Optika i spektrosicoplya, 1959, Vol 7, No 6, pp 721-724 (USSR)
ABSTR!XT: The red line of cadmitun at 64Z8 4c is uaed as a i-ia-volanf&th standard and
consequently knowledge of its true contolar is of graat iiaport-Ince.
In 1935 Minkowski and Bruck (Ref 4) used an atomic bout source to find'
that the half-width of the 6438 X line was 16.4 ), 10-3cm-1. This value
is much greator than the sum of the aouaratus and Doooler half-widths,
i.e, the red line of cadmium has complex structure and a considerable
7.1idth. The present authors x~sod an improved version of tliinkowskl and
Bruckl~i raethod to study further the contour of the 6438 A line of
natarally occurring cadmium (a mixture of GdI06, GdI08, OdI10-114,
Gd.116 isotopes) . An atomic bosin, described o-Lrlier by Odintsov
(Ref 6) vas used to excito the lined It Fabry--Perot etalon was used:
it had 15 cm separation between the plates and the reflectivity of the
dielectric mirrors was 0.0~, The apparatuo lualf-width of the atalon vas
1.5 x 10-3cm-1 (Minkowski ard Bruck's etalon had a separation betne,3n
plates of 11 cia and an apparatus half-aidth of 3 x 10-3em-l) * Ar.
t;% rd 1/3 ISP-51 spectrogrqph mith a UF-84 carnara (f n 800 min) served a, a

67149
Invostization of the Contour of the Cadmium Red Lino, Ulein4 tin Atomic Bosua
wonochroinator. Tha interfarograms wero se:trint:id .*dth an VF-2 mloro-
photometer; the contour of the 6438 4 line ohown ill Pi6 I ie the
moan of the results obtained froia four Intorfar,'3i~rawa. Fig 1 shows
that the contour of the red line of cadmium Ic sirongly aaymotric,
Indicating unresolvad fine structure, and its half-,,Adth Is
(11.8 0~5) x 10-3cm-l- The latter value differj appcerlably from
16.4 10-3r
.;m-.1, given by 11inkowski and Bruck (R-.f 4) ; the lower valtie
raportad above is due to the higher resolation of the aD 'paratus 4sed
by the pr-_-)sont authors. The empirical contour (coyltin'AOU3 curvG) in
compared with a thooratical one in Fig 2, The theoretical (dat~had~
is the reault 4 superoosition of tj-,:; isotopic ccilloonenta of the
cadmium line, each of ;hich hai a natural half-widt-h of 2.6 x 10-3cm-1;
in derivation of the theoratical contour the apparitu!z arld the Dopql&r
half-.Adths Tiero also allo-.,ed for, Tho theoretical contour agrealz
quita mell 1-ith tha wpirical ono and an even bottor coincidence Uln
be obtained by displacing "th.3 c-,).,tras of of tho Sdd --so-'OtAr-
caitooliogru.,, tnv1jr,!:-- io,1--jr ",,.j -0'-f 1.0-1cla--. The
'nat-lyal ~~idth of Vr:- --mt:,, of the 6438 line pla,?es a thocrettir.,).l
Gard 2/3 ~r

WCESSION MRs AR40347.44 8101241WO001OWBOWN]a
JOURCZv Rate the Nekhanes Abs* SW9
&UTHORs Korolay..F.-Ae a Meyeabap'Ve Zhe
TITIM High-frequeney discharge with hydrodyA&aio compression for the pwTose of
zoltation of spectra and for speetral. analysis
:
ITED SOURCSs Dokle Meshvuse 11suchne konforenteii po, spektrookopli 1, spektre
nalizue Tow.wko Tomekiy un-tg. 1900, 41-42
0 ,
TOPIC TAGSt plusma. physics. hidb-frequeney discharges high-tesperature physics
TRANSLATIONs Results are given of research an high-frequency discharge with hydroe,
d,vnamia compression of plasma as a source of excitation for'smission spectral -.
analysis* 7ho effoot of compression Is attained by using,exhauoting of gas@* from-\I
the discharge gap through a narrow duat of one of the elsotrodeso The temperature
of the plasma, In within the range of (7-8 - 104)0 Ko Righ stability of ra"ation,
the excitation of Incandescence of l1nes with high energy of the upper levels. and
other features of this type of discharge that are adventapow for preatioal,
purposes are notode
t~_rd_ 1/2

KDROLEV, F.A.; KURAMV, A.B.
-7
Producing short (on the order of 3.10 sec.) light pulses by
means of a spark d1scharge and an oscilloscope, I%v,vy9.ucheb.
zav.;fiz. no.2:44-47 060. (NIBA 13:8)
1. Moskovskiy gosuniversitet im. M.Lozonosova.
(Xectric discharge lighting)
,I

69967
8/170160/003/01/03/023
2.4, 3 zo o B022/BOO7
AUTHORS: Korolev, F, A., Klementlyeve., A. Yu.p Meshcheryakovaq T. F.
TITLE: 1;1D.i-electric Nultilayered Interferenag Light Filterlhor the
Visual and Near Infrared Region of the Spectrum
p
PERIODICAL: Inshonerno-fizicheakiy.zhurnalg.1960, Vol. 3p No. 1, PP- 55 - 61
TEXT: In the present paper the method of producing dielectric interference light
filters hating a position of the maximum of the light transmissivity band Am of
the light filter given with an accuracy of +-10 A and a sample surface uniformity
of the order of 5 - 10 A, as well an the ap7paratue used, is described. The de-
vice for the production of dielectric coatings consists of a metal plate, the
pre-vacuum pump RVN-20~,' the high-vacuum unit ILA-05-01 "8 and the diffusion pump
of the type ~- ?7The vacuum is measured by means of manometer tubes of the
types LT-211and LK-2-land the standard vacuometer of the type VIT-13~ Also the
motor of the tyie---MIT-20,4is used. Control of the multilayer light filter with
respect to transmiseivity in carried out by means of the device schematically
represented (Fig* 1)9 where, among 9other things, a type PS-1.01;lgalvanometer with
scale, having a sensitivity of 10 a/mm, is used. For the determination of the
Card 1/2

86277
S/188/60/000/005/006/010
2,rO (/0 6 2-) 11,6 36 91) B019/BO56
AUTHORS: Korolev, F. A._L Kireyev, P. S. 1~-
TITLEt Fabry-Pbrot Standard From quartz Crystals
;I -Al
PERIODICALt Vestnik Moskovskoao universit1ta. Seriya 3, fizika,
astronomiya, 1960, No. 5, pp- 53 - 59
TEXT: For the production of spectroscopes with a resolution of from
R - 5-10 7 to 5-10 8,- the Fabry-Pgrot standards with large interspacing
between the mirrors and a high reflection capacity of the mirrors are
necessary. For this purpose quartz crystals are especially well suited,
but they have the disadvantage of birefringence. In a voluminous
mathematical -,alculation, such conditions are endeavored to be found at
which birefringence and the rotation of the polarization plane of light
through the quartz have no influence. On the basis of the results obtained
the authors find it possible to use quartz crystals in a spectroscope with
high resolution; in this case the angle of inclination of the two quartz
plates must be roughly 10- . According to the orientation of the plates
Card 1/2

86 277
Fabry-P6rot Standard From Quartz Crystals S/188/60/000/005/006/010
B019/BO56
with respect to the optical axis of the crystal, R-10 6 to 108 may be
obtained. If the spectroscope consists of plane-parallel plates, bire-
fringence and rotation of the polarization plane exert no influence upon
the resolution. Standards in form of plane-parallel layers, which were
covered on two sides with layers of mirror, permitted a resolution of
R - 104. The testing of such standards in fine-structure investigations of
spectral lines within the visible and ultraviolet spectral range showed
very good results. There are 2 figures and 4 Soviet references.
ASSOCIATION: Kafedra optiki (Department of Optics)
SUBMITTED: February 26, 1960
Card 2/2

68306
0*11/,51 -6 -1 -0-0
AUTHORS: Korolov, F.A. and Kulikov, O.F.
TITLE: Inirestiration of the Ratio of Intensities of the Polarized Goir-nponoiet-'
of Radiation Emitted by a "Luminous" Electronl-\
-PERIODICA
~L: -7 (ULSR)
Optika i speictroskopiya, 1960, Vol 6, Nr 1, pp

AE TILA. G T Electromagnetic radiationlof electrons accelerated ke.g. in
synchrotrons) was considered theoretically by Ivanenko and
Pomeranchuk in 1944 (Ref 1). Classical theory predicted teat the
spectrum of radiation emitted by accelerated electrons consists of
closely spaced lines with fraquencies tan = ne/R, where n is an
integer, c is the electron velocity along an orbit in an accelerator
and R is the radius of that orbit. The ainount ol" aneray radiatod
by such an electron in a unit tirao is i)roportional to the fourth
powor of its kinatle enerGy. Tho frequency at v-;hich a i,,iaxDuwn in
the ~~portrurii occurs is proportional -to the third povior of the
criargy. For electron enerGiez gre,.itar thar. 30-50 M-3V the frequoncy
at which the miai.Wum occurs, lies in the visible roElon, i.e. the
radiation can be obser7ed visually (hence the name:
electronG). Tne oloctron vkdiation ia polarl-tod, i.e. the electric
Card 1/3 ve,.tor is 3ither pArallel to the i.~IaCnetlc field and perpendicular
e_

68306
1 - "; - I - I/zwi
jriveutl~-,ation of tho Ratio of Intensities of the Polarim! ~omponenU of Radiation
Q -
Emitted by a "Luminovu" 31octron
to the electron Volocity (Tt -component) or it is porparid i cu.19 r to both
the ma--notle field and the electron velocity (S -,,;om-,on,5nt) . Zacl-,
or the3e Qomponents has a chamcteristic anGular diatrib-ation of intanalty.
The total intenitty of the 6-canponent la graxter than the totP1
intensity of tha 4-component; the ratio of thij,.~,a total intensities
,,hould ha equal to 7 (Ref 16). The prosont authors rrieaaared the ra-tio
of intonsities Of the olarizad conloonentz- af-, a function of .%,avelength
Y, 00
bet,ween COOO a A 40 ~~ lasilli; 150, 200 and 250 MoV e3-3etrorri. Tho
n1notrons wore accelaratod In a iyachrotron tit tlm Phy-Ocri Inst-Ituto
of Ac. Se, U.S.S.R. (FUN S~.SR) -which could prodii~,.e alavtrons Both
onergier up to 280 MoV. The optical part of' tno ayp_qra'U,.i:; (Fir 1~
cariui,utod ~t a (xartz spectraZraph ISP-22 -Ath a *.'iollaaton pris"m (B)
placed between a collimator mirl~or (0~~) aril a Corm. priam (n) of
~he spnctrcFrrx*- -\ typical apactrcgra~ is gi-ven in Pit--2, where 1
donotez the iron spectrum used for wavelength 2 denoter.
the spectrum of an lmmD usee fct caii,bration,
3 ard 4 Janote, tho spoetea of the it- and zf 2X 'MoV elactrom.
Because of iti low disporblon th-3 opil-'Inal ;jystoui failed -to r1solva
indivl-lqal lines avyl, of
appear.3 a.- a

84690
Y,Sb,0 S10511601009100510111019
AUTHORS: Klementlyeva. A.Yu., and
le, Pak 'of , TF. X
TITLE: Interference L4&ht Filiters1with a Transmission Band
Widt
of 1.5 1 dt
PERIODICALs Optika i spektroskopiyaq 1960, Vol.99 No.5, pp 648-652
TEXT.@ Interference filters with a narrow transmission band
(20-30 1) were reported in earlier papers (Refs 1, 2). Later the
transmission band was narrowed down to 8-10 J1 in the middle of the
visible region. In some applications an even narrower trans-
mission band is required. The present paper gives a theoretical
design calculation for interference filters with very narrow
(1-3 1) transmission bands. This theory was employed to produce
multilayer dielectric light filters with transmission bands from
13 1 (55% transmission) to 1.5 1 wide (15% transmission). The
transmission maxima occurred in the region 5600-5900 1. These
filters were made by alternate evaporation of ZnS and cryolite
in vacuum. Their structure is given in column 2 of Tables 1 and
2, where H denotes a W/4 layer with a high refractive index
Card 1/2

\1 KOI`OLZEV~.; KIR a-EV, F.S.
I--- ~
Fabry-Perot etalon made from crystal-line quartz. Vest. Mosk. un.
Ser. 3: Fiz., astron. 15 no.5:53-59 S-0 '6C. (MIRA 14:2)
1. Moskovskiy gosudarstvennyy universitet, kafedra optiki.
(Quartz crystals)

8102016011331031031013
B019/BO56
AUTHORS: Tershov, A. G Korolev, F. A., Kulikov, 0. F.,
Shkur6kiyj B. I'
TITLE- Experimental Investigations of the Compression of the
Electron Cluster in a 28o-Mey Synchrotron Iq
PERIODICAL: Doklady Akademii nauk SSSR, ig6o, vol. 133, No- 3,
pp. 554 - 557
TEXT: In the present paper, a new method of studying the cross section of
the electron cluster in acceleration is suggested, and several experi-
mental results concerning the compression of the electron cluster are
given. The experiments were carried out on the synchrotron of the
Fizicheskiy institut im. P. N. Labedeva AN SSSR (Institute of Physics
imeni P. N. Lebedev of the AS, -,USSR). Several formulas for calculating
the betatron oscillations are mentioned and discussed. When carrying out.
the experiments the electron radiation in a porcelain chamber was observed
through a window and photographed by means of a motion-picture camera. The
blackening of the pictures was measured by means of a microphotometer,
Card 113 V10C

Experimental Investigations of the S/020/60/133/03/03/013
CGmpr*ssion of the Electron Cluster in a B019/B056
280-Hey Synchrotron
and Fig. 1 shows the photograph of an electron cluster and the results of
measurement. The elliptical shape of the cluster corresponds to the cross
section of the chamber of the accelerator. In Fig. 2 the experimental re-
sults are compared with the theoretical calculations of the dependence of
the relative amplitudes of the oscillation types on the duration of
acceleration. It is found that the radial dimension of the cluster of the
accelerated electrons decreases rapidly according to the adiabatic law.
Besides, the center of the cluster is compressed more rapidly than the
peripheral parts. The perpendicular diameter of the cluster decreases
approximately according to the adiabatic law. Further experiments showed
that the compression of the electron cluster in a progressive electron
drift is the same as when no premeditated drift of the electrons exists.
The authors thank M. S. Rabinovich, Doctor of Physical and Mathematical
Sciences, and Professor P. A. Cherenkov for making work on the accele-
rator possible. There are 2 figures and 7 references: 6 Soviet and
1 American.
Card 2/3

,,KGROLEV, F.A.; YERSHOV, A.G.; KULIKOV, O.F.
Experimental study of electron oscillations in cyclic accelerators.
Dokl.AU SSSR 134 no.2:314-317 S 160. (MIRA 13:9)
1. Moskovskiy gosudaretvennyy universitat im. N.Y.Lomonoo-ova.
Predstavleno akad. N.N.Bogolyubovyu.
(Electrons) (Particle accelerators)

20771
5-, S-g
S/051/61/010/003/oo4/oio
E032/E514
AUTHORS: Korolev, F. A. and Kvaratskheli, Yu.K.
TITLEt The Plaamatron as a Light Source for Spectroscopic
Investigations
PERIODICAL: Optika i spektroskopiya, 1961, Vol.10, No-3, PP-398-402
TEXT: The plasmatron employed is shown schematically in
Fig.l. It takes the form of a closed chamber formed by metal
rings I and 2 and the insulator 3. The arc is excited
between the anode 5 and a graphite cathode 4 which is in the
form of a washer. When argon in introduced into the chamber at a
pressure of 0.3 to 0-5 atm, the discharge taken the form of the
jet 1, which is joined to the cathode by the thin conducting loop
11 and is surrounded by a corona made up of vapours of volatile
ubstances III. 'A study was made of the possibility of exciting
spectrum of high melting point materials and also materials which
are difficult to excite. The specimens to be investigated were
in the form of slag powders mixed with Co 0 and graphite powder.
These were inserted into the aperture in K; anode and the distance
between the electrodes was*chosen to be 3 mm. The spectra were
Card 1/4

20771
The Plasmatron as a Light Source... S/051/61/010/003/004/010
2032/2514
photographed in the mcn-aal (ISP-22) spectrograph. A detailed
description of the design of the plasmatron and its operation in
given in Ref.13. Figs. 21L,b and show the external
characteristics of the discharge (a dependence of length t and
diameter d of the plasma on the current I at 0.7 atm and washer
diameter 1.6 mm; 6 - dependence of J and d on the diameter D
of the aperture in the washer at 20 A and 0.7 atm; 6 - dependence
of -9 on the pressure p. These graphs show that temperature
equilibrium exists throughout the plasmatron jet. The temperature
was measured using the Fel and Fell lines for which the transition
probabilities have been given by N. N. Sobolev (Ref.14). It was
found that the temperature is very dependent on the gas pressure*
Inspection of Figs. 2 to 4 will indicate that the plasmatron can
be used for the spectral analysis of a wide class of high melting
point materials and, in particular, slags. The plasmatron can
also be used to determine the relative oscillator strengths.
There are 7 figures, 2 tables and 16 references: 7 Soviet and
9 non-Soviet.
SUBMITTEDt May 5, 1960
Card 2/4

K01101W, F.A.;.,. YERSHOV,, A.G.; KULIKOV, O.F.
Investigating variatIions in the axial and radial dimensione
sions of an electron cluster in synchrotron acceleration.
Zhur. eksp. i teor. fiz'. 40 no.6.,1644.-1652 Je 761.
(MIRA 14:8)
1. Moskovskiy gosudarzt7ennyy universitet.
(Photogrammetry)
Webtron beams)
(Synchrotron)

KOROLEV, Fedor Andreyevich; DROZHZHIV, Yu.11.p red.; TATURA, G.L.p
. .. . ...... ;~ ~e~.~r-ed.,- I.G., tekhn. red.
(Physics couse; opticsp atomU and nuclear physics] Kurs fiziki;
optika, atomnaia i iadernaia fizika. Moskva, Uchpedgiz, 1962.
503 P. (MIn 15:6)
Obysica)

BABUSHKIN, Aleksandr kfanselyevich, dots.; BAZHULIN, Pavel Alekseyevich,
prof.; KOROLEV. Fadgr AndrWyInh- prof.; LEVSHIN, Leonid
Vadimo , prof.; PROKOFIYEV, Vladimir Konstantinovich, prof.;
STRIGANOV, Arkadiy Romanovich, doktor fiziko-matem. nauk;
GOLIDENBERG, G.S., red.; GWRGIYEVA, G.I., tekhn. red.
(Spectrum analysis methods]Metody spektrallnogo analiza. (By]
A.A.Babushkin i dr. Pod red. V.L.Levshina. Moskva, Izd-vo Mosk.
univ., 1962. 508 p. (MIRA-16:2)
(Spectrum analysis)

S/908/62/000/000/008/008
B163/B100
AUTHORS: Korolevi F-A., Yershov, A. G., Kulikov, 0. F..
TITLE: Experimental investigation of the electron ose illations in
the 680 Mov synchrotron
SOURCE: Uskoritel elektronov na 680 Mev; sbornik statey. Ed. by
Z. D. Andreyenko. Moscow, Gosatomizdat, 1962. 75-87
TEXT: The radiation of relativistic electrons with energies above 100 Mev
can be directly observed or photographed,,through an optical sight glass.
in the vacuum chamber; The system uses, a mirror inside the chamber, for
observation in the direction of the beam axis. With the high-speed camem
r_)~L-i (SKS-1),.150 to 4000 frames can be shot per second. A series of
photographs, shows that at 100,lSev the beam has a slightly elliptic cross
section with themajor axis in the radial direction. When about 165 Mev
is reached the second acceleration stage begins, and strong radial
synchrotron oscillations appear, greatly increasing the radial major axis,~.
while the-beam cross section becomes dumbbell-shaped rather than elliptic.
With increasing energy, the damping of synchrotron and betatron
Card 1/2

S/906/62/000/000/008/008
Experimental investigation of the ... B163fB190
oscillations causes contraction, and the minimum radial cross section is
found at 433 'Yev, and 506 Rev for the vertical cross section. In the
last stuage the beam cross section is slightly increased again.,, The.mean
square radial and, -axial -oscillation amplitudes 'were determined. from the
photographs, and compared with theoretical pr,,dictions. The theory of
Kolomenskiy and Lebedev, wh-ich take3 radiation damping into account, is
found to be-in good agreement with the experiment. Slight deviations are
due to the experiments being made in a real synchrotron, while the theory
assumes an ideal one. One reason for the undamped axial oscillations may
be the warping of the 'magnetic symmetry plane in the real synchrotron with
consequent amplification of axial osoillations under the influence of the
quantum excitation of radial oscillations. Synchrotron oscillations
appearing in between the first and second acceleration stages are damped
More.slowly than predicted. This maybe because the theory assumes
small amplitudes, while they are actually comensurate with the range of
stability. The predicted radiation damping of electron oscillations and
excitation of radial synchrotron and betatron oscillations by quantum-
fluctuations of 'he electron radiation at high energies are at any rate-
confirmed experimentally. There are 8 figures.
Card 2/2

3/056/62/043/005/014/058
B102/B104
AUTHORS: Korolevt F. A.9 Kulikov, 0. F., Yarov, A. S.
TITLE: Investigation of polarization pro?erties of synchrotron
radiation from high-energy electrons
PERIODICAL: Zhurnal eksperimental"noy i teoreticheskoy fiziki, v. 43,
no- 500t 1962s 1653-1656
TEXT: The synchrotron radiation emitted by electrons from the-680-Mey
electron accelerator of the FIAN was investigated cinematographically
((K( -1 (SKS-1) camera, 500 frames per sec). 'The relative intensities and
the angular distributions of the radiation were determined for both
polarization components (6,n) of the radibAing electrons. The latter were
obtained after microphotometric treatment of the pictures from
representations of both components in a direction corresponding to the
vertical (the angular distributions in the horizontal plane were very
much distorted). The experimental results were compared with theoretical
data from Sokolov's formulas (of. A. A. Sokolov, Vvedeniye v kvantovuyu
elektrodinamiku - Introduction to quantum eleotrodynamics-, Fizmatgiz,
Card 1/3

S/056/62/043/005/014/058
Investigation of polarization B102/BI04
1958, ~26) and agreed well except for the n-component at small electron
energi'es (cf. Fig. 1): the 900 minimum that should exist according to
theory was not observed, and in no case did the minimum reach zero as it
should. As could be shown by measurements of the intensity ratios
min/,max
IR n . over the whole cycl e, the absence of a zero minimum can be
attributed to axial vibrations of the electrons- The angular distributions
as well as the polarization characteristics observed agree with those
found by A. A. Sokolov*and 1. 9. Ternov (ZhETF, 31, 473, 1956). There
are 3 figures and 1 table.
ASSOCIATION: Moskovskiy gosudarstvennyy universit6t (Moscow state
University)
SUBMITTED: June 21, 1962
Fig. 1. Angular distributions of intensities of a- and n-components of
radiation at different instants of acceleration for,1-4360R.
Solid lines: calculations according to Sokolov;.I given in relative units.
Card 2/3

ACCESSION NR: AP3005668 4/0168/63/000/004/0014/0017
AWHOR: Korolev, F. A.; Gridnav., V. 1.
LITELS: Optical and radio-frequency characteristics of a multiray interferametor with
diffraction mirrors on thin diels6trio plates
SOURCE: Moscow. Universitot. Ventnik. Seriya III. Fizika, astronomiya, no. 4,
-1963, 14-17
TOPIC TXS: interfarometer,, diffraction mirror,, metallic film diffriv-.tion Mirror
ABSTRACT: it new type of Fabry-Perot intarferometer with metallic film diffraction
mirrors has been developed. The mirrors are mica platcs 501L thick, coatad with a
silver fil-a 200-300 1 thick. Such mirrors ansura totul reflection of electromagnetic
waves from 4 to 32 rm. The film is in the form of Q diffraction grating. The resol-
ving power (quality factor) of this 1nterferomoter with a mirror 70.mm in diameter,
measured at 8 and 4 mm wavelengths, was approximately 200, almost 3 times an high as
for a diffraction grating. For a mirror of the same diameter as a diffraction grat-
ing, the resolving power will be 50 times greater than that of the diffraction grat-
ing. The dependence of resolving power on the ratio of the mirror diameter to the
wavelength and on the transmission coefficient of mirrors is shown, and the Values
Card 1/2

ACCESSION NRs AP3W5668
for tha transmission coefficient of the interferomatar dapanding on the transmission
coefficient of the mirrors "a measured. Orig. art. has. 2 fimwes,, 7 formulas,
and 1 table.
ASSOCIATIM none
SUBIMTED: 1 ON ov 6P 2 DATE ACQt 06UP63 ENCL: 00
SUB CODE: PH NO AV SOV: 002 OrKER; 002

KOROLLVf F.A.; KHOMKIY G,I,; SKOKOV~ I,V,
-1-11- "". ;~
Use of the phase met od of multiwave interferometry for measuring
low gas densitiese Izv, vyso ucheb, zav.; fiz. no.5t6l-63 16
kRA 16-.12':'
1. Moskovskiy gosudarstvennyy universitet imani M.V.Lomonosova.

BDS_
L 12932-63
ACCESSION. M.- AF3004 S/0109/63/008/008/1480/
1-483
AUMOR: Korolev, F.-A.; Gridnev,,V. 1.
10 ft 1~
TME: Multibeem interferometer.used as a high-q resonator
SOURCE: Radiotekhnika i elektronika, v. 8, no. 8, 1963t 1480-1483
TOPIC TAGS: multibeam Interferometer, high-0 resonator, reflector diffraction
grating, resonator, Interfetometer, diffraction grating
ABSTRACT: In order to -build resonators with a high Q factor based, on multibeem
interferometers, interferometer reflectors were produced by the deposition of i
thin silver films on dielectric surfaces. These films were transparent to visi-
ble li&ht 'out reflected lonGer waves. In order to obtain a quantity of inter-
ference. beams, gratings vith widths of W t-n 100 11 placed 1 to 5 = apart were
made on the films. The folloving conclusions were reached: 1) An lnterferometer~
with such reflectors represents an effective electromagnetic wave resonator in
various spectral ranges. 2) The interferometer 0,.factor increases proportionally'z
to the square of the ratio of reflector diameter to wavelength. 3) The inter-
ferometer permits optical adjustment of the beam and observation of the beam
Cord 1/2

ggg

KORULEV., F.A.; KROPISKIY, G.I.; SK04OV, I.V.
Amplitudp method of multiple-beam interferometry. Opt. i spektr. 14 no-3:
416-418 Mr 163. (MIRA 164)
(Interferometry)

KOROLEV, F.A.; D'YAKOVA, S.M.; GRIDNEV, V.I.
Identification of radiations in the far infrared region using the
method of residual rays. Vast. 140sk. un. Ser. 3: Fiz., astron. 18
no.30-5 MY-Je 163. (MIRA 16slo)
1. Kafedra optiki Moskovskogo universiteta.
,q
w-, M

_~OROLEV F.A.; GRIDNEV, V.I.
- -.- -- -1 --.. - P
Optical and radiofrequency characteristics of a multiwave
interferometer with diffraction mirrors mounted on thin
dielectric bases. Vest. Mosk. un. Ser. 3: Fiz., aatron.
18 no.4:14-17 JI-Ag 163. (KM 16:8)
1. Kafedra optiki Moskovskogo universiteta.
(Interfe'rometer)

ACCESSION XR; AP4020939 S/0051/64/016/002/0335/0340
c
d
c
AUTHOR, Korolev, F.A.; Gridnev, V.I.
TITLE: Fabry-Perot interferometer with diffractlon'sirrors
SOURCE: Optika I spektrookopiya, v.16, no.2, 1964, 335-340
TOPIC TAGS: interferometer, Fabry;-Perot lnterferometer,~ diffraction mirror Inter-
ferometer, millimeter wave Interferometer,' far infrared Interferometer, millimeter
spectroscopy, far infrared spectroscopy
ABSTRACT: Prism type spectrographs are entirily unsuitable for working in the sub-
millimeter and millimeter range; echelette type grating instruments can cover this
,range, but are inherently limited as r4gards resolution.. Hence It was deemed of
interest to develop a Fabry-Perot type interferometer for the milliineter range. In
the present paper an interferometer employing reflectors in the form of multiple-
gap meta2lic mirrors, prepared by vacuum evaporation auto quartz (or otheg) sub-
strates, is described. The reflecting bands are silver films 200 to 300 A thick.
The apparatus in diagramed in the Enclosure. Some of the parameters (dispersion,
effective dispersion region and resolution) of the experimental setup are given. A

ACC.NR: AP4020939
---resolution of 2160 for 8-mm waves with a separation of 108 mm between the reflecton
was obtained. Thus, the potential resolution of such interferometers is tons or
hundreds of times greater than the beat resolution of diffraction instruments. The
resolution increases in proportion to the square of the ratio of the reflector d
meter to the wavelength. The resolution increases with separation between the re-
flectors and with increase of the reflection coeffibient. In the case of the test
apparatus, the transmission factor was 40-50% for a reflection coefficient of 95%.
Orig.art.has: 11 formulas and 4 figures.
ASSOCIATION: none
SUBMITTED: l6Nov62 BATS AOQ: 02Apr64 ENCL: 01
SUB CODE: PH,SD NR REP SOV: 000 Of=: 002
1z

ACCESSIQX NR: AP4032361 S/0051/64/016/004/0553/0558
AUTHOR: Korolov, F. A. ; OdintsoV, Y. L ; Fursova, Ye.v.
TITLE- Determination of the transition probability for the 736 Angstrom reoonanc*
line of noon
SOURCE: Optika i spektrookopiya, v.16, no.4, 1964, 555-558
;TOPIC TAGS: optical transition probability, level width, oscillator strength, rose-
:nanco line, noon, atomic spectrum
'ABSTRACT: The transition probability for the 736 2 resonance line of noon was do-
-tormined earlier by W.Schuts (Ann.Phys.18,705,1933) and H.Schillback (Ibid.18,721,
1033). They obtained a value of (8 * 4) x 108 see-1, which corresponds to an oscil-'
:later strength f = 0.21 0.1. However, in view of the procedure employed, the reli~i
ability of this result is not sufficient for Verifying the theoretical calculationx4
of A.Gold and R.S.Knox (Phys.Rov.113,834,1959). Accordingly, the present measure-
ments were undertaken to oblain a more reliable and accurate value. The transition
probability for the K* 736 A line was determined vith reference to the width of the
departure 'level: 3s' The natural width of this upper level was found by in-
Cwd 1/2
.ACCESSION XR-.'AP40328Gl
'vestigatina the contours Of-devOral visible lines, specifically, the 6717 & 6266
,and 6500 & 6163 R pairs, &11 associated with tra=itions feeding this level SM
each pair doparting from the saw 3p level. The source was'an atomic boam, which
has the advantaCe that it allows
of Obtaining lines with a very small Doppler width.
iThe spectroscopic equipment consisted of a sealed Fabry-Porot etalon and an'Isp-51
sP0ctr09=Ph Mot MonOdIrOUtor); the radiatloA Was detected by moans of a photo-
multiplier viewing an electron-optlc&l image converter. The final averaeo valuo ob-,
-tained for the natural width Of the 2kS1[l/2]l level in (3.3 * 0.3) x 10-3 eel,
which corresponds to a value'of (6.6 * 0.6) x 108 eel for the tra it, probaL,
na on
:lity and I - 0.16 * 0.014 for the osclllatOt 5trsngth- Tho'corresponding theoreti-
cal values of Gold and I== am 4,3 x JL
08 400-1 and f 1-0-s somewhat lower.~
~.Qrig.art.has: 3 figurej!.
ASSOCIATION: mons
DA-M ACM 0711ay64 E=: 00 f
MM CODS: op,
X.R JOW SOV: 002 003'
NO

I 43oo6-65
ACCESSION IM: AP5010113 U-R/0109/65/010/004/0767/0766
AUTHOR: Korolev.- F. A. l'Orldnev,, V.-, L
TITLE- Radio-optical multibeam interferomoter with diffraction mirrors on th"in
SOURCE: Radioteldinika~ i: VM I
0 4. 905, -767!-768
TOFIC TAGS: interlorometer, diffraotion mirror radio optical interforemeter~_
ABSTRIM: An improvement:of thaf authors I interferomater described, elsewhere is'.
briefly reported. instead of quarts or mica, a 100- p plwdglas film is used mas a
backing for the silver diffraction mirror. A maximum transmission factor of 9Vj-.i in'
the first order was obtained under these conditions: wavelength, 8 rm; udrror tloh
width, 0. 1 =.; Glot spacing, 4 u-mit reflector diameter, 100 A transmission-
factorlmirror-spacing plot and theoretical considerations are supplied. Orig.
art. has: 1 figure and 2 for=2as. (031
ASSWW11011: none
EXCL.- 00
SUBMITTED: O&May64
so REF SM. 003 GTHERt 000 ATD PRESS,. 3238
card III

7`17
L~ 4564-6 Q/ "91 JL
BD /MF k 6 PI-4/Pm-4/Pr!
-7 ~WT17/,--A (M) -2 tii4li P
F
I-ACCESSION NRI. AP50IL500 UF,/Ot88/651000/002/0()35/;,fd3:9
AUTHOR: Korotev, F, Ao; Hamedzade, S
laser and its dependence on.
11he -artission spectrum of a ruby
i the re son a tor7p-
SOURCE: Moscow,, Universite.t.. Vestnik. Seriya .3. Fizika astronomiyar~
no. 2, 1965p,35-39
-TOPIC TAGS4. ruby laser$ Fabry Perot interfirometer, multiptex,
resonator model
ABSTRACT: A study.was made of~the emission spectrum of a ruby-laser-'
(around A 6943 X) as afunction of *the properties of theresonatort;
The experimental equipment,(multiplex) is shown in Fig. I of the,
r.'Olosurel# The multiolen:consisted-of two simple Fabry-Perot etalons,
with expansion rings (one: variable, the other a constant 2,1-mm
operating in the cross -ed and V-shaped modes. For a given position
of the objective L(f - 300 mm), an interference pattern vas:set up at*
a point where t:--- two Luterfere -nee bands cross. A hyperfine struc ture--
1correspond;ng uo varioualmodes in-the'resonator was observed at these.
. . .......
z _77 ..77777='

L 45641-65
ACCESSION 'URS AF5011500.-,~
'points. tile observations-veremade by means of cameras using A-7W
lastronomical film.. I The ruby crystal was 11.8 mm in diameter a n d 1110 Mr
Ilong. The resonator consisted of two external d-Lelectric,mirror .s
fmounted in special holders. The transmissivity of one mirror was 17ti
:while the other mirror was opaque. The coefficient of reflection of
i -
,the interferometer mirrors was 93- 95% for the wavelength under,in-
~vestigation* The experiments were conducted when the pumping energy
:exceeded the threshold-energy 2 times. The..experimental data show thal
,ithe spectral composition.of stimulaced emission from, a rtiby depends.on,
!the structure of the resonator. Thus, spectral lines obtatned at
a V-shpped, crossed multiplex Oriz . 2.3 and 4 mm;
!varLous thicknesses of
2~3 and 10 mm; 2.3 and 30 mm) were separated by 0.024, 0.023, and
!0.008 cm-11 respecti'vely...These'dL-spersions corresponded to resonatori
'1with lengtho.of 20.5,-21*12, 'ind 62.12 cm, respectively. Origslart,
1has: 6 figures* [YKI
tet
'ASSOCIATION: - Kafedra Optlkl,, ffoskovskiy gosudarstvennyy unLverst
(ChnlT of Optics, Moscow State University)
S j B V,,~ TTE D i2IFeb64 ENCLt 01 SU3 CODE: EC
N r; W"-' SOV: 005 008 ATD PRESSI 3244
cG,,d 3

L U09-66
'ACCESSION N 9 'W~2~lt 3 UR/0188/65/000/005/6091/0092-
r
621.378.32
,:AUTHOR: Korolev, F. A.; Mamedzade, A. M.
:TITLE: Narrowing the emission hand of a ruby laser with a complex resonator
!SOURCE; Moscow. Universitet. Vestnik. Seriya III. Fizika, astronomiyal no. 59
j1965, 91-92
iTOPIC TAGS: ruby lase light interference, light filter, luminescence-
laser$
quenching
[ABSTRACT: It is shown thdt multiple interference color filters made up of two sing] 4
!filters with nearly equal effective thicknesses can be used for narrowing the emis-
sion band in a.ruby laser with a multiplex resonator. When the Incident light is
tnormal,to the re-flecting surfaces of.the mirrors, fulfillment of the condition
n1h,
nA 77plit
iresults in quenching of m excess emission.maxima in each of the light filters, whe
mlo, t-1, n2 and hj,a~ih2~-.me~&rsl;ndic~s of--refraction and geometric thicknesses~re-l
Card 1/2

1 13651-66- - EWT(1) WG - -- - - - -
ACC NR. Ap6oox84 SOURCE CODE: UR/Ol3q/6i/6&6/
AUTHOR: Kdrolev, F. A.; Fan Van Tkhlk 50
ORG: Moscow State Universitj im. M. V. Lomonosov (Moskovskiy gosuda Liver-
sitet)
TITIE: Measurement of the coefficients of coherent intensification of neon lines in
a helium-neon mixture Y;1 S'
SOURCE: I=. Fizika, no. 6, 1965, T5-79
TOPIC TAGS: laser emission coherence, helium) neon, emission linep stimulated emis-
sion
ABSTRACT- The authors investigated the selective excitation of neon atomsat:-levels
close to the 21s level of metastable helium atoms, energy transfer from which to nor-
mal neon atoms results in population Inversion of many neon 28 levels investigated
by others (R. A. Macfarlane ez al. Proc. IRE v. 50, 2111, 1962, and earlier papers).
The study was undertaken because the earlier results have shown that In addition to
the 6328 A line, which is very strongly amplified in the presence of helium, other
lines with upper levels 383, 3S4, 36s, and 4d3 are also amplified. The authors then
investigated the populations of the lower levels 2p in the presence of helium. To
check on the assumption that other lines with upper levels 3s and 4d should have an
.population-inv~rsiuA., the authors developed a new methods in which the line-intensity
ratio is determined while varying the length of the luminescent column Inside a Fabry-
Perot interfero,metere The method is -briefly described. A.tube'. Ulled

_L , -13651-66
FACC NRtAF6002084
with a helium-neon mixture at -2 mm Rg, with confocal mirrors of radius of curvature
approximately 1 meter, was used. lbe mirror served simultaneously as the entrance
and exit windows of the tube. The tube diameter was approximately 5 mm. To check on
the amplification of certain lines under conditions when the 6328 A line is at the
threshold of coherent generation, an additional mirror M was employed (Figure). The
pressure and current were chosen such that
coherent generation of the 6328 1 line
started only when the mirror M was oper_
ating, and when the latter was covered
with black paperj the generation ceased.
In this experiment this occurred at pres-
sures -2 mm Hg and current -10.Ma. The radiation from the tubes was focused on the
slit of a spectrograph (DFS-3) and photographed on film. Results were obtained for
43 lines corresponding to the various transitions. In the case of the 2p--le tran-
sitions no amplification was obtained. In the case of the lines with 3s__4p and
4d--3P transition, the amplification is obtikined, in 'agreement with earlier
data by the authors. The amplification coefficients -for the
different lines were comparect under conditions when no generation occurred at aiW
lines. It is pointed out in the conclusion that the population can differ greatly if
generation occurs at any of the lines. Orig. art. has: 1 figurep T formulas,, and 2
tables. (021
SUB CODICt 20/ SUE14 DATE: 07VW641 ORIG MWt OOV OTH W: 007 ATD PMS
.Card PJ2 q-~_O ~/97

KUL KOV, O.F.- YAROV, J1.36
Stueyang the and eccelpration (Al' ;4ia';trops In, a
eynobrotron by means clu h~ -gh-spead mot'or-pict,~ro Ftcgojrr-r.,ply.
Usp.nauoh.fut. 9tl92-197 164.
(MIRI 16:1.3)

KOROLEVp F.A.; FAN-VAN-TKHIK
I-- -------- -
Measuring the coefficients of coherent intensification of
the neon line in a helium - neon mixture. Izv. vys. vcheb.
zav.; fiz. 8 no.6:75-79 165. (MRA lr-,:1)
1. Hoskovskiy gosudarstvennyy universite" imeni H,V. Loi,-lo-
nosova. Submitted March 7, 1964.

L 1729-66 FAT(m)/EWP(i)/1NP(t)/94P(b) IJP(c) JD
'ACCESSION NR: AP502244o uR/mg/65/01' 009AT18/1-TI-9
0/
539.216.22:535.669422
AUTHOR: Korolev F. A.,, qridnev,.V. I.
- IW, 1-7 ,
1TITLE: Transmission of electromagnetic waves by thin silver fi3j
-'71
SOURCE: Radiotekhnika i elektronika, v. 10, no. 9, 196571 8-1719
TOPIC TAGS: microwave technology, EM wave generation, silver, semiconductor thin
film, microwave transmitter
ABSTRACT: The transmission coefficients of thin silver films were studied for the
0. 8-, 1.2-, and 3.2-cm waves. The films were vacuum deposited on mica and fused
quartz substrates. Film thickness varied from 10 to 300 A. The results indicated
that the experimental transmission coefficients were higher than the theoretical
for smaller film thicknesses and lover for larger thicknesses (see Fig. 1 of Enclb-
sure): Orig. art. has: 1 figure and 5 formulas, [TS)
ASSOCIATION: none
SUBMITTED: O8Dec64 ENCL: 01 SUB CODE: GSO EO
NO REF SOV: 003 OTHER: oo6 ATD PRESS4,0q4-1
Card
F~~ A,

L 1729-66
WCESSION NR: AP50224ho
T, %
ff
1W W. -TO
d, A'I
Fig. 1. Transmission coefficient (T)
of silver.films for microwaves as a
function of film thickness (d)
I - Experimental cur,~e; II and
UO I III theoretically determined curves.*
Card 2

L 2W-66 IMT(1)/aiT(m)/EPF(c)/EFA(w)-2/&P(t)/E6r?(b)/BiA(M')*-2 IJF(C)
ACCESSION mRs Ap5o16168 uR/oo51/63/O18/d06/O9Q/0973
535-338:546.291
AUTHORt Korolevs F. A&; Odintsoys Ve -10
TITLE: in-V'e8't1'9a"'ti-0-hZ-rthe Width Of helium a ectral lines with el~~;ron it
"Ugn_in an stgmic beam
801MCRI(I %-ItikA i spektrookoplya., v- :7 1965s 968-973
TOPIC TAGS't heliumj line 'broadening,, excitation spectrump line width,, Doppler
effeetp byperfine structure
ABSTRACT% The widths of sever&L isolated helium lines emitted by an atomic beam
were investigated experimentally. The apparatus employed was described elsewhbre
(Opt. i spektro ve 10) 403) 1961)o The results disclosed an appreciable Doppler
broaddhing of the lines# due to collisions between the atoms and the exciting
electronne Thin broadening vus, calcu2Ated theoretically for the helium linen
A ~22 1 A (21Pr-31N)i
"'2 A Pl--4.%), 5016 A (21So--32Fj)j 5047 A (21PI-41so)) 6670
7281 21PI-34SO)p and for all the cmiponents of the % line* The natural width
of the 21P.% level wao determined., together with the associated transition proba_
bility for the helium 5&4 A resonant line. The value of the width was found to
be (9-8 1 0.5) x: 10-3 ca'l. The transition probability van, found to be (1,85 :k L
Card 2/2

KOROLEV F.A ; ODINTSOV, A.I.; MITSAY, V,N*
Some characteristics of a helium-neon laser. Opt. i spektr. 19
no.101-77 J1 165. (MIRA 18:8)
M

.~,T.OLEV F A Mk,IEIDZADE, S.M.
1krrowing of the emission band of a ruby laser with a (,omplox
reaonator. Vast. Mosk. un. Ser. 3: Fiz., astron. 20 no.5:91-92
S-0 165. (MIRA 18:11)
1. Kafedra optiki Moskovskogo universiteta. Submitted Feb-ILITY
25, 1965.
1

AL 2668o-66 FBD/ZWT(l)/EW T(m)/EEC(k)-~2/T/E14P(k)/EWA(h) IJP(c) WH/WG
C NR: AP6607177 SOURCE CODE: UR/0188/66/000/001/0105/0109 I
1AUTHORS; Korolev, F. A.; Mamedzade, S. M.
iORG: Department of Optics MGU` (Kafedr optiki MGU)
!WTLE: Separation of monochromatic ruby laser radiation with the aid
iof a wedge shaped multiplex interfero-EMr with topposing.dispersiont.
ISOURCE: Moscow. Universitet. Vestnik. Seriya III. Fizika,
lastronomiya, no. 1, 1966, 105-109
ITOPIC TAGS: ruby laser, laser radiation, spectrum analysis, line
spectrum, continuous spectrum,
JABSTRACT: The wedgelike multiplex interferometer with topposing
dispersion' was originally described by one of the authors (Korolev,
.y
Vestn. Mosk. un-ta no. 8, 101, 1953) and consists of two simple Fabr
i
Perot interferometers in tandem. The method of separating a radiation
component by means of such a system (Fig. 1) is explained and its
theoretical basis and operation are briefly described. It was used
to investigate'the emission spectrum from a ruby laser ancl to sepmte Z-
Card, 1/2 535.854:621.378-325-OOff

L 2668o-66
AP60611-ff--
N-R-.
J
L
Ruby 4v- 17 -B
0-vama ~am
F-P F-P Camera
Fig. I. Optical diagr= of setup with wedge multiplex-interfercmeter~l
!monochromatic components from its radiation as well as from the radia".
Jtion of a mercury lamp. The ruby-las 'er radiation components were
separated both in the case when theresonator was made up of the
end faces of the crystal ruby itself (from the continuous spectrum)
!
and when the'mirror was made u of surfaces of specially prepared
glass cylinders (line spectruz. A check has shown that the separated
component does not contain extraneous frequencies and it is concluded:
that the procedure described Is suitable for the separation of mono-
chromatic radiation'from either a continuous or a line spectrum.
10rig. art. has: 6 figures and 2 formulas.
SLM CODE: 20/ -SUBM DATE: 310ct64/ ORIG REP: 006/
Card 2/2-.-A
g~q,

L 33192.-66 MC (k) -2/1_-1P(Q/E WT (l)/EWT(M)/FDD/T/n'1P(e) lip(c) Wam
S66 iCECO~D&Uk 14[0-00110011
1 ACC NR.AP60fl541 A
AUTHOR: Korolev, F. A.
........................ ..
ORG- (Moskovskly gosudarfitTeidWY
_KoscoK.St!L~Q jjqkyersit~v, im. - _V. Lamonois-ov
universitet)
TITLE-. Generators wid aWlifiers of coherent light
SOURCE: Elaktrichestvo, no. 4, 1966, 1-11
TOPIC TAGS: laser, gas laser, ruby laser, laser theory
ABSTRACT: A general description based on well-known published sources and intended
to familiarize engineers with laser problems covers the following points: invention
of laser; principle of operation; conditions for generation of coherenj radiationj,
n~fjlasers ~L5
laser types (solid-state, gas, semiconductor); characteristics of
characteristics of gas lasers; characteristics of semiconductor lasers; laser
resonators; laser-generated modes; laser anplifters and their excitationj high-
power pulsed laBerl laser uses. Principal sketcheal diagransp photographst and
formulas are given. Orig. art. hast 16 figures and 37 formlas.
SUB CODE: 09,20PU13M DATE: 04May65 / QRIG REF: 03
Card
Ar-C-'NR, AP7007041
SOURCE CODEt UR/0202/66/000/004/0016/0022
AUT110R.-__!qRMjp
OdIntsOV9 A* I*; K*Iovt Ke
ORO: ]Phy-q1cO-T0uhnIC&l InstitUt*t AM Turk= (Fisl -t khnicheskoy I titut
AN TurkSSR) k0 e na
TITLE: lftfluGftce Of resonator misalignment on the output power of &
neon-helium laser
SOURCE: AN TurkSSR. IZv0stiYa. Seriya fiZIkO-t0khnIcheskIkhs khimicheakikh,
i geologicheskikh nauk3 no. k, 1966., 16-22
TOPIC TAGS: gas lasers laser R and L) -
SUB CODE: 20
ABSTRACT: An Investigation of the extent to which disruption of Ideal
alignment of a laser resonator mirror system Influences the properties,
primarily the output powers of the oscillation, A neon-helium laser
generating in the visible light at 6328A was Inv6stigated. The expert-
mental setup consisted of a lasers a device for measuring small Inclination
angles of the mirror, a vacuum System and a Power suPPIY. The discharge tub* of
the laser was 4 millimeters In diamter and 88 centimeters long. The
generator PoVer as a function of Inclination of one of the mirrors was-
Investigated with various lengths Of laser resonator. The least length was
133 centimeters. It was determined that the requirements for alignment of
mirr0rs In a laser with spherical mirrors varies considerabl7. In the case
Of generation of many transverse types of oscillations co
to 3 minutes of arc) misalignment of the mirrors can be nsiderable (up
other cases, the MaXimUm tolerable misalig tolerated. in
The Itatting angle decreases with dscraasing nt may be lasg than one minute,
Card generator power and with
-1/2
~0

NR.
I~c*reaslng resonator lengtho Misalignment Is much more critical in a re-
sonator with lane parallel mirrors. Orig. art. hast 5 figures and 6
r rmuLas. YPHSs 38,33Y

9192-66
L
- MIMIMMIM.MIMUMMIX7
EV2(l)/EWT(m)/EWP(b)/EWP(t) IJP(0) JD
Ai SOURCE-CODE: up/oor,8/65/OO0/OO8/DO23/DO23
SOURCE: Ref. zh. Fizikaj. Abs. 8D
q 5"V9
AUTHORS: Kor ol"t'. F.__&;.Odintsov, V. I.; Furaovaj Ye. V.
ORG: none
TITLE: Determination of the probability of transition from the 1B2 level of neon4
to the ground state from the patural.width of the a Oral lines
CITED SOURCE* TV. Komis. kopii. AN vyp. 1., 19&, 2T3-280
_Komis. po, spektEqsrc._____Lq8SR,_ t. 2,
V ~ "
TOPIC TAGS: line width, sp2e_'qQl line, transition probability., neon, electron bom-
bardment
TRANSIATION: An investigation was made of the contours of several spectral lines of
neon and the probability of transition from the 1s2 level to the ground state was
estimated from the natural width.of the spetetral lines. The light source was.an
atomic beam of neon, excited by electron botibardment. The high-resolutlon Instrument
was a Fabry-Perat etalon. The glow was recorled with the aid of an electrooptical
converter. The natural width of the ls2 level-vas found to be 4 X 10-3 =71, correa-
ponding to a transition-probability 0.75 X 109 Bee-'.
.SUB CODE: 20/ SUM DA72: none/ ORIG REF: 000/ OT11 REF: 000
' ~11_ M-M ~~
Vr'

KDt~,'OLSV, F-F
BULATOV, ICF, . rednkt n ~Wizq~ 1, 1,
HALTSHU,
MELINIKDV, N.J.; SIATtIll, M.N.; -SUVROVSKIT, A.Te., SRI-
BAWT, A.A.; SHCOXIN, S.T.; GONCHARDT, N.K. ; redaktor; TINOT,
imiojaktv rmdaktor.
V., retlaktD~. Wi
[General technical training in eecondary schools: work praztice
of city and rm-al schools] Politakhaichaskon obuchente v eradnei
shkole; Iz apyta raboty goro-i,!~kikh i eellakikh shkol. Mookwit,
1956. 279 p. (K6RA 9,5)
LAkademlya pedagogicheakikh nauk RSFSR, Moscow,
(T"ehniCAl AdIIO-AtiAn)
:--kZ F~~
NAN* 1-14m ~i

KCRGLEV, FhljLli( FILM70,Vicll N/5
830
Jb
USPEKHI NARODNOGO OBRAZOVANlT-A V
SSSR ZA 40 fI. E. SOROg LET CP,ROGaSS
OF PUBLIC EDUCATION IN THE USSR FOR
40 YEARg IMOSKA, -IZNANIYE", 1957.
46 F. (VS--E50v.UZNCrTE OBSHC!fFSTVO FO
RA5F'RObTRANl'NIYU POLITICBESKIKH I
NAUGHUM ZNANIY, SER. 2, NO. 30)
BIBLIOGPAPHICAL FOOTNOTES.

~'~ , ~, LI, 1 r I.'
;-,. , 'I,! 'y , L 11
j~ I . -
Nlovaya sisterar, narodro. u v 333il: 6i~orvii: dc!!,a:~-,,C--fOV T StatCy.
(it. red. "I.;,.. Goncliarov 1 F.F. Korolev. irlo3~xa., Izd-vo Ai`-. id.-'3'), 1560-
602 i~,.
i
Cn fl,,!leaf: Aicademiya Fedaf-o~-icheslcilid. liaLk ?,3 -~ SR.

L --35537 65
T P_TrbST-_V 5A0 (b) /DrP WN-5/P?-4/Pr-h/Ps-4 jn~~
ACCESSION YR: A.P5008221 S/0286/65/000/005/0085/0085
AUMORIS: Trej~Xakov~ . M.; Korolevf F. F.; Ypvt?Zev, B. 1. 1 SwikovskJ-y, A. A.
TITLE. A method of testing_producte,for hermetic sealit Class 42, No. 166925
S,OUI-va-Z: Byullater-I izobreteZIIiT_i t-Xkv kh znakov, no- 5, 1965, 85
arny
TOPIC TAGS: sealing, hermetic sealing, leak deteato
r,_I_~elium low discharge
ABSTRACTLt This Authcr Certificate presents a method of testing products for
hermet-~c seal with helium under high pressure. For more accurate determination of
leak-ge in a product, a glow-discharge is produced in the helium molecules leaking
cu~di 'he openings in the product (with the help of an electric field). The glov
discharge produces a luminescence which indicates the presence of leake.
ASSOCIAIVIONs Organizateiya gosudarstvennogo komiteta po aviatsicnnoy rekhnike SSSR
Literprise of the State Comaittee for Aviation Tedhaolog, SSSR~
5 'Ulal F1 MD t14Jun63 INCL: 00 SUB CODE: IE
NOW 60vt 000
Card 1/1
QTW t 000

XOROLvV, F. 1.
Wire Rone
Reconditioning tying wire for log rafts. Lps. Y)ron. 12 no. ? 1952.
Monthlv-L-I-s-t 1_40 1111!38ian Arcessionst Library of Conpres a- Au--ust, 10.52. UNCLASSIFUM.

-77
CC NRs AP5025311 SOURCE CODY: Uft/Oi93/65/0"00/0,D9/0025/0026
AUTHOR: ksenkov Yu. I. Korolev, F. I.
1yq J_3_-
3
ORG: none
TITLE: UKP-2 ultrasonic flaw detector for small-diameter steel wire
J3~_ L T
SOURCE: Byulleten' tekhniko-ekonomicheskoy informatsii, no. 9, 19651 25-26
TOPIC TAGS: wire, steel wire, wire flaw, flaw detection, flaw detector, ultrasonic
flaw detector
ABSTRACT: The UKP-2 ultrasonic tester for evaluating the structural homogeneity of
and detecting surface defects in steeTwires 0.5-3.0 mm in diameter and 1000-5000 mm
long has been developed. The wire is irradiated through a liquid medium obliquely to
its axis with longitudinal, transverse.- and torsional-ultrasonic waves causing so-
called "wire waves", which are very sensitive to surface and inner defects in the wire.
The waves reflected from the defects produce impulses on the detector screen. The
UKP-2 makes It possible to detect surface defects as shallow as 0.01 mm and small in-
clusions and to root out defective -wire during processing. Orig. art. has: 1 figure.
(WW]
SUB CON: IF_,&F/SUBM DATE: none./ ORIG REF: 000/ OTH REP: 000/ ATD PRElk:
Card. 1/1 tw s 681.2-868.6a621.9-422'.,
_N

KQROLP-,V, F. K.
K-rolevo F. K. "Rated streszes in the links of likk gears used in L metal-workingZ
P, 11 Nauch. zapiksi Kharlk mekhan.- Hashinostroit. in-t v01.1x, Is~juo 1,
machines, a.,
1948, p. 99, 116 ---Bibliog: 7 items
SO: U-3566, 15, March, 53 (Letopis *Zhurnal Inykh Statey, No. 14, 191+9).

XOROLEV, F.I.. doteent, kandidat takhnichaskikh nauk; BONDARI, M.P.,
fmididiat tekhnicheskikh nauk, redaktor; GALIFZM, Te.I., inzhener,
retsenzent; KHAYMOVICH, Te.M., professor, doktor'tekhnichookikh
nauk, reteensent; ILSTIRZNKO. D.M., takhnichookly redaktor
(CalculLations for transverse planing machines] Raschet poperechno-
strogalInykh atankov. Kiev, Goo. nauchno-tekhn. izd-vo mashino-
strott. lit-ry. 1952. 100 p. (Microfilm] (MLRA 7:10)
(Planing machines)

KOROLFV, F.K.
Theory of the turninc, of a MUI tiP05itiWi table of a! machine-tool
unit. Trudy KhPI. Serom"o 19 no-5:(I-~4 "C'9. (MIRA 14:9)
(Machine tpols

AROUIVe F.K.; TSYMBAL. I.L.
Modernizing multiple-position swivel table of semiautomatic machine-
tool unite. Stan.1 IWtF- 31 no.12:24-25 D 160. (MIRA 13:11)
(Machine tools)

--KOROIEV-,-F.K.; FESTUNOV, V.M.
Device for measuring the acceleration of rotating shafts.
Mashinostroenie no.4:116 Jl-Ag 162. (KRA 15:9)
(Shafting) (Electronic instruments)

ROFIDLZVl F. K.; MSTUNOV, V. M.
------ 315 in Machining with power
Causes for the breakdOWn Of dri
heads. Mashinostroit9l' no.lOs25 0 '62- (MM 15:10)
(Wiiling aW boring)

. I
GR-fSPKC- YLi.~.; MSIYANOV, O.No; KOWIEV, F,F.
How to prevent the breakdown of driUs and pcrwer packs.
M&~~!Inoatroitall no.702-33 J1 '64. (WRA 17.8)

KOROLPhV F.L..gvardii polkovnik meditsinskoy slushby; LITYINWiCO, N.M.,
SHLTAXEIOVOT, B.Ye.,n
polkovnik meditsinskoy;slazhby; wwor
meditsinskoy sluzhby; RATSVLISRVILI. G.A.,starshiy leytenant
maditsinskoy sluzhby.
Piffect of necrectomW on the course of thermal burna; experimental
studies. Toon-med. shur. no.2:23-27 7 156 (KMA 10:5)
(BLWS, experimental,
off. of naphrectozy) (Hue)
(XIDUYS' effect of excision.
on exper. burns) (Rue)

XORCLAv,,X44~j,)*kpov YEMITANoV, V.T., polkovnik, red.; VOLKOVA,
T*Yeo, tekhn.red,
[Reconnaissance by observation] Hazvedka nabliudeniem. Koskva,
Toen.izd-vo N-va obor.SSSR, 1959. 114 p. (KIRA 13:5)
(Military reconnaissance)

I_9ROLEV, K.P., doktor tekhn.nauk; SLOMYANSKIY, A.V., doktor tekhn.nauk
Requirements for the new high-speed locamotives. Zhel.-dor.tranap. 45
no.1203-39 D 163. - (MIRA l7t2)

SOV/129-59-?-1/16
AUTHORS: Kuritsyna, A,D., Candidato of Technical. sciences',
.Korolev, F. V. and Korsunskaya, K-A., Engint~ers
TITLE: Diffusion Processes in the Bimetal "Steel-kluminium
Alloys"During Heat Treatment (Diffuzionnyye protsessy
v bimetalle "stall-alyuminiyevyye splavy" pri
termicheskoy obraboti;)
PERIODICAL: Metallovedeniye i Termicheskaya Obrabotka Metallov,
1959, Nr 2, pp 2-7 (USSR)
ABSTRACT: Anti-friction bimetal, used for producing liners of
bearings of I.C. engines, is manufactured by rolling
with high rates of reduction (5g-60 to 80%) at room
temperature and also at 250-300 C, i.e. at temperatures
below the hot working temperature of steel. As a result
of this technological process the steel base of this
bimetal strip becomes considerably hardened and, as can
be seen from the graph, Fig 1. assumes a high anisotropy
of its mechanical properties. This complicates
considerably processes of stamping of bearin6 liners
from such strip. Experience has shown that in order
to re-establish the normal stamping properties of the
Cardl/8 liners, the bimetal strip should be annealed at a
"RW= in"" mpg M, I
4

SOV/129-59--2-1/16
Diffusion Processes in the Bimetal "Steel-Alumin3-um Alloys"
During Heat Treatment
temperature which ensures full recrystallization of the
steel and complete re-establishment of its mechanical
properties. However, such heat treatment would result
in a loss of the adhesion between the steel and the
aluminium alloy. Therefore, it is necessary to select
the chemical composition of the sub-layer in such a way
that annealing of the bimetallic strip is practicable,
The authors investigated the progress of diffusion at
the boundary between the steel and the aluminium alloy
and its dependence on external factors, i.e. temperature
and duration of holding at a given temperature and also
the composition of the metals in contact, These studies
were carried out at junction zones of Steel 08 with the
alloy ASS-6-5 and of Steel 08 coated with aluminium AVOO
and the alloy ASS-&-5, the latter being a new aluminium
base anti-friction alloy. In the second case the
diffusion processes were studied at the boundary between
the steel and the aluminium as well as at the boundary
Card2/8 of the aluminium and the alloy ASS-6-5, The latter
Diffusion Processes in the Bimetal "Stee SOV/129-59-2-1/16
During Heat Treatment 1-Aluminium Alloysil
studies were necessary for establishing the minimum
permissible thickness of the intermediate aluminium
layer. Furthermore,, the possibility was studied of
applying higb,,ppeed heat treatment regimes which exclude
tbosecond stagW diffusion, namely, volume diffusion;
the first'stage being surface diffusion. It was thereby
assumed that the forming very thin intermediate layer
of iron aluminideb, which are located on a plastic
base,, will not affect appreciably the flaking off of
the aluminium. alloy from the steel. On the basis of
the carried out experiments, it was concluded that
the processes of diffusion at the area of contact of
the bimetallic strip and the aluminium alloy ASS-6-5
depends on the temperature and the heating time and
Consists of various stages. During the first (low
temperature) stage an intermediate layer forms as a
result of very small displacements of atoms of iron
and aluminium, caused by the transition
from the random distribution of the atoms along the
Card3/8 surface of contact towards an ordered distribution,

SOV/129-59-2-1/11~
Diffusion Processes in the Bimetal "Steel-Alwainium Alloys
During Heat Treatment
results in the formation of an intermediate
point-shaped layer of the reaction phase of a small
thickness which depends on the non-uniformity of the
real processes of plastic deformatioL. The second stage
is characterized by the formation of additional
interaction zones,, which form as a result of an
increase in the holding time or the temperature and a
consequent slightly larger displacement of the atoms
than in the first stage; this brings about formation
of phases of iron aluminides in the form of a thin
layer covering almost the entire surface of contact
between the steel and the alloy (Fig 4). A further
increase in temperature (550 to 600 C for the Steel 08-
alloy ASS-6-5 and for Steel 08-pure aluminium) brings
about the third stage of the process, which is associated
with the higher speed of diffusion of aluminium in the
layer of the new intermediate phasewhereby, in the
aluminium layer there will be a relatively wide zone of
Card4/8 loosened sections caused by unilateral diffusion and

SOV/129,-59-2.-.*'L//--- 6,
Diffusion Processes in the Bimetal "Steel-Aluminium Alloys"
During Heat Treatment
it is this which produces the separation of the aluminium
alloy from the iron aluminides which form as a result of
diffusion. The fourth stage of the diffusion phenomena
at the boundary ste8l-aluminium takes place at
temperatures of 650 C and higherl at these temperatures
there is a mutual diffusion between alwiiinium. and iron
but the diffusion of -the aluminium is higher than the
diffusion of the iron and the growing phase penetrates
deep into the steel. The authors of this paper %%
established experimentally that the speed of'reactiye
diffusion at the contact zone iron-aluminium is
influenced by silicon and antimonyl antimony speeds up
the reaction b~ reducing the initial temperature,of the
process to 510 0, whilst Si slows down the process,
The authors also studied the influence on the speed of
the diffusion processes of inetals of -the transient
group (Ni. Mn. CO etc.), i.e. metals with variable
valency in the alloys. In selecting alloying elements
for increasing the critical temperature of formation of
Card5/8 aluminides at the boundary of the two-phase region, the
hypothesis of A. A. Bochvar (Ref 8) was taken into

SOJ/129--59--2-1/16
Diffusion Processes in the Bimetal "Steel-Alumin-Jum Alloys"
During Heat Treatment
consideration, according to which diffusion processes
will be the slower the more complex the composition and
the structure of the rejected phases and the more these
differ in composition and structure from the initial
solid solution. For studying the relations governing
diffusion the following additions to the aluminium were
chosen: Mn. Mg, Cu, Ni, Fe, Si and the combinations of
Si + Mn and Si + Co in various quantity ratios. These
materials were cast 9 chemically analysed and, following
that', the ingots viere rolled into strip. Strip made
of the Steel 08 was clad with -these alloys and the
clagded metals were heat -treated, Dur:Lng heating to
525 C for a duration of 30 mins flakinG off of the
aluminium layer occurred in the case of it being alloyed
with Mn, Mg, Cu 6Ni and Fe. If the heat treatment was
effected at 575 C for 30 mins, flaking off was observed
only for the alloys containing 61. Heat treatment at
57500 for four hours led to the formation of a layer in
Card6/~ the case of the alloys Al--SJL--Mn and, to a very slight
SOV/129-59-2-1/16
Diffusion Processes in the Bimetal "Steel-Aluminium Alloys"
During Heat Treatment
extentpin the case of alloys of aluminium, with Si and Co.
During 1956-1958 the authors repeatedly verified the
influence of heat treatment on bimetal consisting of
steel with a base of the following chemical composition:
0.50/6 Mn, 0.5% Si. rest Al. This bimetal strip was
produced .by cladding a strip of 10 + 0.1 mm thick
ASS-6-5- alloy on one side ,th a 1 mm thick (steel)
layer. This combination ofFtotal thickness of 11 mm was
rolled to obtain a final combined thickness of 2 and
2.5 mm respectively. The first pass') with a reduction
of 40% was effected in the cold statel the.subsequent
second and third passes down to the final dimension were
effected after a re-heat to 250 0C. The bimetallic strip
produced by this method was investigated f the point
of view of presence of an intermediate FR
layerPof a hard
and brittle phase of iron aluminides, Metallographic
investigation of the zone of contact and of the sub-zone
at an amplification of 1250 times showed complete
absence ~of aluminides; diffusion of antimony
Card?/8 into the sub-layer could not be detected either. Results

SOII/129-59-2--1/16
Diffusion Processes in the Bimetal "Steel-Aluminium Alloys"
During Heat Treatment
obtained in testing the strength of the joiLtbetween
the steel and the alloy after annealing confirmed the
high quality of the strip produced by this method.
There are 7 figures and 8 references., 7 of which are
Soviet, 1 English.
ASSOCIATION: Institut Mashinovedeni.ya AN SSSR (Institute of
Mechanical Engineering, Ac.Sc,, USSR) and
Moskovskiy metalloprokatnyy zavod (Moscow Metal
Rolling Works)
Card 8/8

S/ 1 22/60/GGO/G 12/003/018
A UTTIORS - Ru, in it-s~-' y~ N'. 'M. ; Kii-rit,syn a. A. D U and id' at es rif T---'rz I ic-11 Sc
FI*ur!:IE-v., F. V.I. ani Kov-2z%.;-~-~k-iy;:i, K. N.. Dq-4rleers
TUITS allov 'rilm-"11
PERIODICAL.
tha4-, IiVe kInd, is zmIrp~w:L4 I'vely "0 Pa-
t- LE,:Ue J~,! '-'7JTW, ii,-d a!; o~. r:F- i-c! cw -
scordr-IP, -t- in TI "n
Sbaf-I bear-IrLw~
atithor-s point ct-4--', tlh-,O pro-bl-m ca% ti~ a
special Nc~rk-,inl' 15 lay;%r of an alloy ()f 1 3a w i n In or w 1 n rld iliq
or Simply pure tln, az i-, p.!.v.t4Act~-i tty M,'.or~z, U,S,A, 5eariags with
'11,ov wi*:n zind 3CA Sn toad u-en tested 97
9
bushlriF c,. i i,- t. n. I
!IPobeda" :.q r a rid wo Ft r o an k ~~ I 1 -1 f I j) o,i rr, aw ~i~, ~ xr,~- I n wo: k wl t In babbl. k.
lirv:d rorlJ --f* Ilnll"g wit-11 11-h4- wiF-.' rv.-T arA ".~- "OkfAng
layer separa';--i af * er 2C) - -40 kra, dr.-3pi ~ e an jw~c-, ', a,i~ r of Arlt~ (AMK) al-
C a nd I/ q

Investigation of !steel - k,19n-Sr, alum',110-m alloy blm,?~Ial A 16'/A 130
loy, Th~- AW alloy c-7%nt;ft1r1S (%).- 0,~, - 1 .0 _-31~ 0.5 - 1.0 Mn, -1-te rest is Al.
It was st-.att~d la tfW; !,v j1j..- -~n prac t, lca 1. 1 y did
not have any c-ffEct or, 41he 1-and. and wltH r I-v-h r rad;ictlor, a.-troyed ti-
metal; annealing of wlth Sn ir, al.lurtiz)-um anlif-I.- xi a~lcjy wealkeneri bond.
Rai:aed Sn ccii~-,erit in a1loy tiad -a s'~r~,ng neeat.%,e sff-ct on Nine bond.
The experimental da-~a derionstraied tha-. tond 1.e%w~'~-n a"uml-nuru and b-a5e can
be considerably Improved by red-.zc1na. Hae Sn ccriten- lr~ t-!~e z,,irf-ace of, blanks pre-
liminarily to rolling toget-hir wii,h base. '11he author3 t~ave developed a method for
squeesJng liquid Sn out. ~-.)f about- I rrm dec;p -s-urface layer of high-Sn all4minum alloy
at 300 - 4000C. The res4lt Is Sn con",ent. in the Surface reduced from 20 - 30% to
2 - 3%, and Sn distributlor. In matal as ahown in Fig. T-his alloy contained
20~') Sn, the curve rhows Sn dfstribu~~ion in I mm deptt. on tkic- zsar!ace. Annealing
at 5500C needed for recrystallLzation of s,,eel band improved bond very much when
the h4.&--Sn layer was so -treated, and mechanical strength in the Joint was higher
than of the antifriction alloy. Blanks of high-Sn aluminum alloy with a layer of
AMK coated on were onnealed at 3500C and rolled together with armco Iron with abMt
60% reduction. Bimetal bands were subsequently finally rolled to gage and anneal-
ed at 500 - 570' to recrysta-l-lize steel. It is expected t.hat the method will make
aluminum antifriction alloys applicable for a wider range of fric-,ion couples.
Card Z/3

89421
s/i36/61/000/002/002/oo6
E021/E335
AUTHORS: Kuritsyna, A.D., _Korolev, F.V.,,,Korsunskaya, K.N.
and Rudnitskiyj N.M.
TITLEs The Technology of the Production of a Bimetal of
Aluminium Antifriction Alloys and Steel
PERIODICAL: Tavetnyye metally, 1961, No. 2. pp. 66 - 68
TEXT: The technology of the process of producing bimetals
of steel and high-tin aluminium alloys was investigated and
a comparison of the technological properties of antifriction
aluminium and intermediate alloys was given.
A semicontinuous method of casting --~s tried. The table gives
the compositions and conditions usec,. Melting was carried o
in a high-frequency furnace. The weight of the welt was
70 - 80 kg and billets 70 x 260 mm were cast. The rate of
casting was 10 - 13 m/h except for pure aluminium which had
a rate of 3 m/h. The billets were water-cooled. Pouring
was carried out through a funnel with a 12 mm diameter hole.
From the results it was shown that the high-tin alloys and the
Moren 400 alloys had good casting properties and a low
Card 1/4

89421
S/136/61/000/002/002/oo6
The Technology of .... E021/E335
temperature of casting. The billets were rolled to 10 ma
strip. The surface had no porosity or cracks before rolling.
Alloys with 20 and 30% tin were cold-rolled. Reduction of
the first pass was 10% and on subsequent passes - 15%.0 The
remaining alloys were hot-rolled after holding at 450 C for
two hours. Moren 400 alloy exhibited hot shortness during
hot rolling, and deep cracks when cold-rolled.
It was shown that to produce a good joint in the bimetal, the
tin content on the surface of the high-tin alloys should be
decreased. The alloys werz- hot-rolled with AMK alloy with
reduction of 70% on the first pass and 28% on the second pass
to give a good joint, and subsequently rolled to 2 mm.
The strength of the joint between the alloy and ANK alloy
was tested before forming a bimetal with steel by heating to
550 OC for 30 minutes. Steel strip 6 mm thick was used for
the bimetal. The joint between the steel and the AMK alloy
was produced by a first pass in the cold state with 60%
reduction, a second pass with 30% reduction, and then it
was cold-rolled to 1.9 mm. The joint was tested by heating
Card 2/4

89421
The Technology of ....
S/136/61/000/002/002/Oo6
E021/E335
to 550-570 0C for 10-30 minutes. The strip produced in this
way was used for the production of bushings for bearings in
experimental r_A3 (GAZ) and 595-1 (ZIL) motor..
There are I table and 2 Soviet references.
Table: The Composition of Alloys and the Regime of Casting of
Aluminium Alloys
Name of Chemical Composition Canting Rate of Pressure of
Alloy Charge tempera- drop of cooling
Billet ture,0C billet, water, atm.
mr/h
Pure Al cu-o.ool6 800 3 0.8
Aeolo
(AVOOO) FO-0.04
si-0.04
Al- rest
High-tin Sn-20 An-17.32 740 13 0.8
alloy Al-rest Al-rest
Card 3/4

89421
The Technology of ....
S/136/61/000/002/002/oo6
EOZI/E335
High-tin Sn-30 Su-26.3 740 10
alloy Al-rest Al-rest
Moren 400 si-4 Si-4.26 Boo 10
Cd-0.5 Sn-0.13
Al-rest Cd-0.50
Al-rest
AMK Mn-0.5 Mn-0.5 780 9-10
Si-0.5 si-o.8
Al-rest Al-rest :11w
r- Sb-6 Sb-4.57 920 9_10
(ASs 6-5) Pb-5 Pb-4.52
Mg-0.5 mg-0.94
Al-rest Al-rest
iLND si-4 Si-3.8 800 10
(Moren 00) Al-rest Al-rest
.1flAntimony added to aluminium heated to 1 000 0C.
Card
0.8
0.8
o.8
019
0.9

301J
S/136X2/000/004/004/004
Y E021/E435
AUTHORS; Pogodin-Alekseyev, G.I., Gavr�lov, V.M.,
Korolev, F.V, .
TITLE: The use of low-frequency vibrations in continuous
casting of beryllium bronze
PERIODICAL: Tsvetnyye metally, no.4, 1962, 69-73
TEXT: Vibrations were used in order to try and eliminate the
columnar structure in the billets, which makes subseqaent
rolling more difficult. The metal,was melted in a high-frequency
furnace with a graphite crucible of 60 kg capacity. The billets
produced were up to 400 mm long. Vibrations were produced'from
an eccentric vibrator. The frequency could be varied from
0 to 100 c/s and the amplitude from 0 to 2 mm. The temperature.
of the molten metal was held at 1050 to 10600C and that of the
pouring funhel at 650 to 7500C since freezing occurred in the
funnel at 16ifer tempeiatures. With amplitudes of 0.7 to 0-8 mm
and frequen6ies of 25, 50 and 75 c/s the vibration arrangement ,
worked satisfactorily. With this amplitude drops of liquid'metal
were ejected at 100 c/s; at higher amplitudes ejection occurred'
Card 1/2

5/129/62/Ooo/oio/ooi/oo6
E193/E383
AUTHORS: Kuritsyna, A.D., Candidate of Technica-1 Sciences,
Rudnitskiy, N.M., Korolev, F.V. and Korsunskaya, K.N.,
Engineers.
TITLE: Infld'ence'of the treatment-of certain bimetallic
materials on the bond strength
PERIODICAL: Metallovedeniye i termicheakaya obrabotka metallov,
no. lo, 1962, 8 - 11
TEXT: The object of the present investigation was to study
the effect of annealing on the strength of bond between the
components of variows bimetallic strips fabricated by the usual
pressure-welding (cold-rolling) method. -The following were
included in the experimental materialls: pure aluminium; alloy
V Mn); Al-20% Sn alloy: Moren-400 (Al-11% Si);
~401K W-0-5% Si-O-50% 0
10 In the fi at
h"_-6-5 (ASS-6-5) alloy (Al-6% Sb-5% Pb-0-5% Mg)- r
series of experiments the Al/Al, Al/Al-20% Sn and Al-200' Sn/ANLtK
bimetal strips were studied, the last of these being fabricated
with and without a treatment which entailed tinning of the
.Al-200% Sn alloy surface with tin squeezed out of the alloy itself.
Card 1/3
s/i2'9/62/0O0/olo/ooi/oo6
Influence of the treatment E193/F,383
Wedge-shaped sandwiches were used in every case so that the
reduction in the first rdlirg-pass varied from 401,La at one end of
the strip to 80% at the other, a*uniform reduction of 360.4 being
given in the second pass. Shear-strength tests were carried out
on suitably prepared bimetal specimens, both in the as-rolled
0
condition and after 30 min annealing at 350, 450 and 550 C . The
shear strength of each individual metal given similar treatment
was also determined. -The results canbe summarized as follows:
1) the shear-strength of-cold-worked pure aluminium was not
affected by the annealing, that of the AMK alloy increased from
8.3 kg/mm2 after rolling,to ll-.kg/mm 2 after annealing at 550 OC9
thb corresponding figures for the Al-20%1 Sn alloy being 7 and
5 kg/=a2 2) the shear strength of the bond in bimetal specimens
after any given treatment corresponded to the strength of the
weaker component given similar treatmentf the AMK/Al-20Y. Sn
bimetal strip prepared without surface-tinning treatment was an
exception, its atrengt~ falling rapidly with inc E easing annealing
temperature (8.4 kg/mm after ri6lling, 2.8 kg/mm after annealing
at 550 OC)i 3) the bond strength of the bimetal specimens was not
Card 2/3

POGODIN;..ALEKSE)CEV, G.I.; GAVRILOV, V.M.; KOROLEV, F.V..
Use of low-frequency vibrations during the continuous casting of
of beryllium bronze-, TSvet. met. 35 no.4:69-73 Ap 162.
(MIRA 15:4)
(Beryllium bronze) (Continuous casting)

4.CCESS.ION NR: AP4005832' S/.0129/63/000/01210'039/0041
AUTHO.~: Kuritsy*na, A. D.;,Rudnitskiy, N. M..; Korolev,.',.F. V.
Korsunskaya,,.K.~N.
TITLE: -'Structure'snd properties of heat-treated aluminum-tin aniffriction
all oy,
go URCE.: Metalloved. i termich. obrab.. metallov, no. i2,,'1963, 39-41
TOPIC TAGS:. aluminum tin alloy, antifriction aluminum alloy; antifriction
alloy, alloy structure, alloyproperty
AB~TRA&: S'ullyls Study (A. Sully, "Journal of.Inatitute 'of Metals", 1949,
76) pertainIng.to the structure' and propqkties of heat-treated aluminum
tin antifr'iction alloys which has applications in bearing for ppLrbureto r- type
engines wa's r-examined. The microstructure examination showed that cast
structure fail in proportion to increase in shrinkage which 'produced a very
fine sta,nnous eutectic. Obsertion with respect to sweating indicates that tin
Card
W

ACCESII'-ON NR: AV005032
s.weatin decrewie's parallel to the increase of shrinkaje during -annealing.
A~v-igorous sweating of tin with large droplet formation can be observed with
weakly 66forrhed cast samples during annealing at 350C and holding time Of
30 min tes All ys with-9916 shrinkage scan be annealed at 5~0-570C wlth6ut
ii Lo
high losses. Mechanical properties of d1loys with 20 and 301/6 Sn have a
high ductility after*final shrinkage (90%) which increases after annealing
at 35OC;(the aluminum grain recrystallization temperature). ..,A_pplication of
high degrees of deformation (9916) for Al alloys containing Rlore than 2070
Sn assures a discrete distribution of the stannous phase after anne'aling at
550-570C with. a holding time of 30 minutes. Orig. art. has: 2 figures.
ASSOCL~TION: None
SUBjVUT-TED::.'00 DATE ACQ: 09Jan64 ENCI~: 0.3
SUB CODE: A~L, MA NO REF SOV: 000 OTHER: 001
Card 2/2

LYUBESHKIN, V.A.; KORQLEV,J~V.; KORSUNSKAYA, K.N.
Effect of deoxidizer!iIa on the mechAnical properties of lead-containi
nickel silver. TSvet. not. 36 no.1:614k Ja 163. (MM 16: 51
(Copper-nickel-zine alloys-Motallurq)

L-212o6--65 OUT (V)/FPR/T/E'i7P (-)/Eri7P(k)/Z'-7P (b) P r VP
ACCESSIONINR: "5000947-IJP(c) MOOD/fal S/0136/64/000/012/0083/008a-
AUTHOR: Tikhonov, B.S., 1corolov,.F.V., Kors6skaya, K.N. U
TITLE: Sheets and strlOa of bran& 34A solder for soldering aluminum and its alloy s_
SOURCE: Tsvetnyye metally, no.12, IM, 83-85
TOPIC TAGS: -aluminumt. aluminum: solder, aluminum alloy solderinff, solder-rolling, -
aluminum soldering, silurhin,/solder 34A
ABSTRACT: ;Solder 34A is a common material for soldering almninum and its alloys but it
is diffiCUIL to u.se since it cannot be produced in the form of wire or foil owing to its low
ductility. Therefore a method was devised for producing the solder in the form of a
three-layer foil which forms a ternary cutectic (6% Si, 28% Cu. 667b Al) on melting.
Hypoeutectoid 8% silumin (Si-Al alloy):and highly pure copper (99.99%) were used to
produce the 34A solder as a three-ply rolled foil. nlia ratio of these starting materials
was calculated on the basis of the parameters of the equipment and chemical composition,
of ' .104A solder (26-30% Cu, 4. 54. 0% Si, balance Al) for assembling the pack for rolling.
From this calculation, a thickness of 13 mm (12 mm silumin and I mm cop-per) was
selected. Good welding together of the two metals during hot rolling was possible only if
the contacting surfaces did not oxidl ze during heating. The copper, which oxidized at
C.rd 1/2

41-14

L.61~02-65 EWk- W . 0/101a (i--) (=)/E'PF 1'C-)/EF9(k)-2/EVF (n)-2/T/
/DiT
M7966 (b y7r2
- )-2/2 AWO/wA iir'Vi~-h/Po -h/Pf-4/Pr-4/Fq-V
ACCESSION IiM: AnOI769k Peb -4 PU-4/Pl.h up/oo5i/65t'oiq/(*j/wTijoM,
YP
3GTB/1JF(C) /JD 62j. 37 5.9-535
AUTHOR:
F. A. Odintaoirt A* 31 Hitsay N.
TITLE: Investigations of certain characteristics of a he4um-FIton 1aser
SOUMS: Optike i spektroakopiya' 7 1--~
V~ 3-92 no. 1" !965
~TOPIC TAGG: helium neon laser
las,er.~'grfs laser multimode operation, heliur~~
neon
7-5")
AMSTRACT: The authors Investigated the dependence, of the power generated at 6328 At
(3521-2p4 transition) on the diseharge current, the pressure mixtures and the par-
tial pressures of He and He (in the He/lie concentration interval from 2:1 to 15:1),,
in a laser excited with a dc discharge and having eAernal spherical mirrors 'With
dielectric coatings of 99% reflectivity. The investigation was carried oul. with
nearly confocal geometry and with simultaneous generation of many oscillation modesa.
The generation power vas meaaured with a photocell in conjunction with a galvano-
meter. Me restats showed that the generation power has a ma imum vith respect to
either the current, the mixture presaurep or the partial pressures. The poaitioa
and magnitude of the maximum depend on the values of the other parameters. The, ef-
fect of varying the distance between mirrors, with the discharge length constantp
;Card
cord

L 37718..66 EWT(m)/E'i4P(v)ZT/t~4P(t)/FTI/EWP(k) IJP(,,) .1 r) / Ifm
ACC NRs AP6016334 SOURCE CODEs UR/0149/65/000/006/01C
ATFMORS: Zakharov, M. Ve (Professor); 1q
Korolev F. V.;.Chizhov, S. I.; Tikhonoy, B*~S-; 13
Stepanova, M. V.; Sliozbergi S!F_~"F"
ORG: Mone titute of Steqj and Aljgyqj,_Chair for the Metallurgy of Nonferrouet
Rarep and Radi otive Metals (MoBkovokiy institut stali i eplavov, Kafedra.
metallovedeniya tovetnykhp redkikh i radioaktivnykh metallov)
TITLE: New transmission-coppe alloysp their alloying principlesp properties, and
uses 117 14'
SOURCE: IVUZ. Tovetnaya metallurgiya, no. 6, 19659 106-113
Ine"9A. sfor goo,46zm& . 'rW6'&".qd_ -v*r*l 4.s4_1r~,3
TOPIC TAGS: Acopper alloyp nickel containing alloyp chromium containing alloy / Br.
.copper alloy, Mts-5k copper alloy
ABSTRACT: The alloyiqg techniques, properties at different temperatures, and stabili
.under contact weldingf8f a number of transmission copper alloys were investigated.
The investigation supplements the results of V. M. Glazovp U. V. Stepanoval and H. V.
Chuprakova (Izv. AN SSSRIOTN, No- 3, 1962). The experimental results are sumarized
in graphs and tables (see Fig. 1). It was found that the most thermostable transmis-
sion alloys are Mts-M and Br.NBT, situated on the quasi-binary sections of Cu--Cr2 zr
Card 1/2 TMQt 449-3

L 52685-66 FWT(m)/E'-"P(w)/.r/E'~.,;!--kt) I 'i I T F` I CjD/.qW,/JG
Nl __r
ACC NR- AP6012729 SOURCE CODE: UR/0136/66/000/004/0074/0076,;-,-'
AUTHOR: Kucherov, V. I.; Zakharov, M. V.; Chizhov, S. 1.; Korolev, F. V.;
Tikhonov, B. S.; Ryabo;&, P. So
ORG: none
TITLE: Mechanical properties of the alloy Br.NBT at various temperatures
SOURCE: Tsvetnyye metally, no 4, 1966, pp 74-76
TOPIC TAGS: beryllium bronze alloy, copper alloy, welding electrode, mechanical
property, cold working, metal heat treatment/Br.NBT beryllium bronze~lloy, Mts2
copper alloy, Mta3 copper alloy t~l
ABSTRACT: This alloy, produced from the wastes of berylli bronzes, is de
oigned for
use as electrode material for the spot, seam and butt welding--g-f -qtainlesslWd high-
Itemperature steels with low heat conductivity and hi h trenj It differs from the
a t ~Y_
Mts3 per alloys (also used as electrode materiaA in hat it ha a higher content
of NiT.4-1.6%) and Be (0.2-0.4%) and contains Ti .05-0.15%) 1 tead of Mg. The
article presents data on the mechanical propertFe-sof the Br.NBT room and elevated
temperatures as a function of four different cold and hot working regimes of specimen
of this alloy (regime I semicontinuous casting combined with quenching, tempering
35'24'725'295:620.1
L 32685-66
ACC NRt AP6012729
at 5000C, 3 hr; regime 2 as above, followed by cold forging to 507. and tempering
at 4500C, 3 hr; regime 3 semicontinuous casting, hot rolling at 800-900*C with
907. reduction in area, quenching from 900-9200C and tempering at 470'C, 3 hr; regime
.4 -- as above, with 807. reduction in area, and with quenching followed by cold
rolling with 507. reduction in area and tempering at 430*C, 3 hr). Findings: regimes
3 and 4 appear to be optimal, since then ultimate strength UB Of the specimens
Ancreases by an average of 5-8 kg/mm2 in the 20-6000C temperature range and is not
accompanied by a decrease in the indicators of plasticity; the Br.NBT specimens thus
'qtreated acquire a strength (aB - ~75 kg/mm2) that exceeds the strength of Cu-CO-Be,
imts2 and Mts3 alloys at elevated temperatures (aB - -55 kg/.2). its high strength
at temperatures as high as 600% combined with its moderate electrical conductivity
-(45-50% of the electrical conductivity of pure annealed copper) and comparatively low
cost, make the alloy Br.NBT an excellent material for the electrodes used in the
welding of stainless steels and high-temperature alloys. Orig. art. has: 1 figure,
2 tables.
SUB coDa: 11, 13/ s= D&TZ: none/ ORIG RZF: oo4/- an Rw: 002
LG-

30(12) SOV/25-59-7-21/53
AUTHOR: -,Korolev, F 0Ye.,,Member (Magadanskaya Oblast')
TITLE: Pro or Con? (A Letter to the Editor)
PERIODICAL: Nauka i zhizn9, 1959, Nr 7, p 58 (U;3SR)
ABSTRACT: The article gives a review on the now book., the "Novgorod-
tsy'19 by B.M. Prilezhneva-Barskaya containing 127 pages
and published in 1957 by the LeninGrad Section of the
Detgiz Publishing House for children of medium age and
elder. The author severely criticizes this historic
novel for the glorification of monks durin- the period
when Novogorod was an independent republic 0(XIII-XV
century); he then states the opinion that this book
might exercise a bad influence on thc~ younZ Communist
blood who should be educated in a strictly atheistic
spirit. In conclusion, the author expresses surprise
that V.N. Bernadskiy, Doctor of Historical Sciences
and scientific editor of this book, failed to furnish
Card 1/2