SCIENTIFIC ABSTRACT GULYAYEV, V.V. - GULYAYEVA, L.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000617320017-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: September 21, 2001
• Sequence Number: 17
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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GOLOVANENKO, S.A.; CHERNOV, A.N.; SAPOZHNIKOV, VA; SINITSYNI, V.G.1
vp_ -VAIVS -,-. -
Extrusion of bimetal shapes. Kuz.-shtam. proizv. 5 no.10:
7-9 0 '63. (NIRA 16:11)

GOLOVANENKO,, S.A.; CHERNOV, A.N.;.P~LYAYEV, V.V-
Hot extrusion of shaped steel and alloy parts. Kuz.-shtam.
proizv. 5 no,.11:7-10 N 163w (MIRA 17:1)

ACCESSION N11 AP40 19027 s/w 2/6VOoo/boe/bo 45/oo47
AUTHORSt Grishkov, A. L;, Ghernovs A. N.j GuXr&"V#.'V. V.
TITLM Pressure indicator for high speed hydraulic presses
SOUICEi Nuznechno-shtampovochnoye proizvodstvo, no. 2, 1964p 45-47
TOPIC TAGS: hydraulic press, pressure indicator, stamping, manometer, recording
manometer, foil indicator I
ABSTRACTi A pressure indicator was designed by TsN'IICh14 for moasuring the foFco
applied and the pressing velocity in the 150-ton hydraulic press P66~B used for
hot sbamping of forrous metals and alloys at up to 300 M/sec. The work-Jr-C
principle of the indicator is based on the variation in the elastic deformation
of a thin-walled contaihor under the action of the internal pressure of the liquid
inflowing from, the main cylinder of the hydraulic press* The pressure indicator
(see Fig. 1 of the Enclosure) consisted of a block (1) and a cup (5) with t1lin
elastic walls anda rigid bottoma The cup is attached to (1) by the nut (2). Two
foil indicators (4) are fiiodito the thin wall and two (6) to the rigid bottom of
the cup. All the indicators are lacquored and. covered wiUi lacquer-saturated
L CoM 1/3

Card 2/3
ACCESSION NRI Ap4ol9O27
cloth. The terminals of the bridge so formed are led to a Is-prong junction on the
casing(7). The measu~aments obtained with this device are quite accurate and the
device itself is siaple, compuabs and abelti.e, It can be used for measuring
press=es in various lVdraulic mechaniums with working speeds up to 300-400 =/sec.,
Orig. art. hass 3 figures.
ASSWIATIONs none.
SUBMITTEDs 00
DATE ACQ s 27Mar6h ENGLt 01
SUB COM M
NO REF SOVt 001 0MIM.- 000

ACCRASION Mgt A019027 ENCWSURE 1 01
~4
7
Fig. 1. Sectional view of the presswe indicator*
le blocks '2. hut; 3. gasket; foil incUcatorl cup;
6. compensating foil indicators; 7* protective cauinge
313
J,

CHEENIOV, A.!. ; (;ULYAY---TV, V.7.
,.,fj th'od ol* dcLormInitg thf7- adhosivu streng-th of 13~
bimetullic profiles. Zav. lab. 30 ro.11:13941 164' (MIU 18:1)
1. TSe~- ,tralln,tv nauc'tiiio-isil(,,dov.FL'.ollskiy institut 1-h-ernoy
metullur,-.U im. I.P. Bardina.

L 36139-66- - ikp e
ACC NR- AT6016765 SOURCK CODN- Ui/27'Y6/65/0001042/0092/0100,//4
AUTHOR: Chernov, A. N.; Golovanenko, S. A.; Gulyayev, V. V.
ORG: none
TITLE% Features of the fabrication of bimetal alinpes by the hot p
_!"j!~nE~ method
SOURCE: Moscow. Toentrallnyy-nauchno--..i-as.ledovatellskiy tjj!jtitut_ -chernoy-p~eX!1~1ur-__,-
gli. Sbornik f-rqtdov, no. 42, 1965, Proizvodstvo bimetallov (Production of biwet-ils). i
92-100
TOPIC TAGS: chromium steel, nickel steel, bimetal, metal extrusion, metal pressing
Khl8N9T steel, St. 3 steel
ABSTRACT: The article describes the experimental study of the hot pressing of bimetal
shapes performed at the Scientific Research Institute of Ferrous Metalluigy in 1963.
The technique employed was that of direct extrusion in an 800-ton vertical hydraulic
press, from a container with an inside diameter ofj~0 am. Rods measuring 50-25 mm in
diameter, with various thickness of cladding layer, were thus produced from such
materials as, chiefly, St. 3 steel as the core and Khl8N9T Ni-Cr steel'4~s the clad-
ding sheath. The extrusion was performed on using a container heated to 400*c and a
die heated to 250-300%. The pattern of distribution of the cladding layer along the
length of the bimetal rods was investigated by comparing the variation in the cross-
Cmd 1/2

L 36139-66
ACC NR: AT6016765
-sectional area of the base-metal core under various conditions of extrusion and
correlating it with the formulas for the volumetric content of the cladding and base
materials. It was thus found that the flow pattern of metal through the die hole is
major factor In determining the lengthwise pattern of distribution of the cladding
heath and hence also the geometry of the base-metal core; it can be optimized by
:
retarding the flow of the core metal during the initial stage of extrusion. In view
of the considerable advantages of the hot pressing of bimetal shapes as compared
with their hot and cold rolling, it is expedient to organize this pressing on an in-
dustrial scale. This will make It possible to: 1) expand the current variety of bine-
tals; 2) obtain bimetal shapes with various combinations of metals, as well as with
intricately shaped cross sections which cannot be obtained by rolling; 3) produce
small loto of bimetal shapes at lower cost compared with rolling: 4) reduce by 40-50%
the unit consumption of expensive and scarce metals and alloys. orig. art. has:
6 figures, I table, 2 formulas,
OB COOS*. 13, ll/ SUM PATS: am*/ OILIG a9r: 003
Sheath RoULIUL%k
Di aigilar Metals 11

L 36140-66 E,VP(e)/K*T(m)/EWP(w)/EWP(V)/T/ENP(t)/ETI/EWP(k) JJP(c) JDYHM
ACC NR
- AT6016766 SOURCE CODE: UR/2776/65/0001042/0101/0106
AUTHOR: Chernov, A. X.; Colovantako, S. A.; Gulyayev, V. V.
ORG: none
TITLE: Investigation of the bonding strength of layers in hot-pressed bimetal
SOURCE: Moscow. Teentrallniz nauchno-isoledovatellskiz ins. oy metallur 1i
Sbornik trudov, no. 42, 19b5. Proizvodetvo bimetallov (Production of bimetals), IN!-,
106
&30-q,,Ajr,
TOPIC TAGS:, chromium steel, nickel steel, metal pressing, adhesion, metal bonding,
bimetal, metal cladding / St. 3 steel, Khl8N9T steel
ABSTRACT: By contrast with rolling, during pressing the core and sheath of a round
bimetal shape get bonded together simultaneously over the entire contour in the pre-
sence of a uniform distribution of radial compressive stresses in the area of deform-
i ation. As a result, during pressing the shape of the core remains virtually undis-
torted and the adhesion (bonding) between the care and sheath is greater. In this
connection, the authors i eatigated the strength of th adhesion of sheath to corn
for bimetal rods of *t, 31steel and Khl8N9T Cr-Ni steell4oduced by hot preusing in
an 800-ton vertical hydraulic press. To this-e-nU, the rod specimens were subjected to
core-extrusion and twistina testai The extrusion tests and twisting showed thnt shear
Card 1/3

L 3614o-66
ACC NR: AT6016766
resistance depends not oplypn the degree of relative reduction in area but alt.- mi
the content of the cled0ingklayer. Thus, for rods of 25 mm diameter subjected to
pressing with & 91% relative reduction in area, shear resistance increases vith in-
crease in volumetric content of cladding layer (Fig. 1). Reason: as the content of the!
~4
Fig. 1. Shear resistance as a function of volusetric content a of the cladding
layer:
a - during extrusion of core; b during twisting
2/3

L 3614o-66
ACC NR' AT6016766
hard component increases, the pressure that must be exerted on the bimetal also in-
creases and this, in its turn, contributes to increasing the adhesion between the
layers. Adhesion strength is also markedly affected by ouch factors an the quality
of surface treatment and the techniques of the assembling and welding of the original
bimetal blanks. on the basis of these tests*it may.be concluded that the minimum re-
quired stren)gth of the bonding between the layers, which for bimetal sheets of St. 3
and DIUM, ,*teelo amounts to 15 kg/mm2, can be attained for rods with even a rela-
tively thin cladding layer (a - 0.3) by applying a relative reduction area amounting
to 70-80%, which corresponds to reduction by a factor of 3.3-5.0. As the volumetrLc
content of the hard component (cladding material) increases from 0.3 to 0.7, bonding
strength increases 1.3-1o4 times. orig. art. has: 5 figures.
SUB ODDR: 13, 11/ SUM DATE: none/ MIG REY: 002
Joining of Diesimilar Metale/I
Card 3/3

GULYAYFV, Y(-.A.
Character of chan~,as in the nonhem~oglobir. iron contlant of
blood serum in lymphogranulomatosis. Probl. gemat. i Fere I..
ki,ovi no.2:36-37 165- (M1RA 18: 11)
1. Gospitallnaya tera~evtlcheska'va klinika (zav. - prof. A.I.
Germanov) Kuyhyshevskogo meditsirtskogo instituta.

BLANK, E.M.; YUOVSKIY, Yu.I.; GULYAYEV, Yu.A., inzh., retsenzent;
CHILIKINA) N.D., inzh., red.; STEPANCHENKO, N.S., red.
izd-va; DFYKINA, U.F., tekhn, red,
(Handbook for mold makers] Spravochnik formovshchika. Mo-
skva, Mashgiz, 1963. 182 p. (MIRA 17:2)

GULYAYEN, YU.B. (Saratov)
'I L -
Free torsional vibrations of a circuha c o r. e w 1' -_ h a -_ y Ir 4 !: a ',
, A
special-type anisotropy. Irmh.zhur. 5 no.],192-195 165,
(M,IRA 18,14)

ALEKSEYEVA, V.G.; GULYAYEV, Yu.V.
Socond All-Union Conference on Photoelectric and Optical
Phenomena in Semiconductors. Radiotekh. i elektron. 7 no.4:
722 Ap 162. (MIRA 15:3)
(Semiconductors--Congi-esses)

~ i IV I I ,..
GU-LTAYIEV, Yu.V.; P(J'S V I
Amplification of surface waves in Zhur.eksj-,. i
teor.fiz. 47 no.6:2251-2253 D 164. (MIRA 18:2)
2. Insfitut radiotekhniki i el.ektron!kL AN i InstAtut
fizLko-teklinicheskikh i nadlotekhrlicheskLkh _izmer:-,-nJy.

-6
USSR/Miscellaneous - Radio clubs
Card 1/1 Pub. 89 - 6/32
Authors : Semenov, N., and Gulyaev, YA.
Title t DOSAAF radio clubs and other organizations
Periodical -i Radio 2, page 10, Feb 1955
Abstract t The activities of the local radio club of the Khabarovsk province,
develol:ment of radio skill by radio amateurs and the discussion of
problems related to radio communications, are presented. Illustration,
Institution:
Submitted:: .....

GULTATBT, Ye.A,
Nonhemoglobin serum Iron and total blood Iron in norinal subjects.
Terap.arkh. 31 no.11:65-69 N '59. (MIRA 13:3)
1. Iz gospitalinoy torapevticheakoy kliniki (zaveduynshchiy - prof.
A.I. Germanov) Khybyshevskogo meditsinakogo instituta i lu7byahevskoy
oblastnoy stantall perelivaniya krovi (zaveduyushchly N.Y. Yedorovskays.).
(IRON blood)
I

GT-TLYAYEV, Yu.
New system In the accounting of transportation operations. Za rul.
17 no.10:25 0 159. 01DU 13:2)
l.Stars4i7 goeavtoluspektor, Sverdlovsk.
(Traffic accidents)

GULTAYXV, Yu.F., starshiy tekhnik-leytenmt
Flight preparation ourfit. Yest.Vozd.71. 41 no.2:60 F '59-
WRA 1214)
(Airplanes-Maintenance and repair--l-P-quipment and supplies)

L 26124-466 EPF (n) -'2',/E'dT(1)/ETC (m)--6
ACC NRt AP6015806 SOURCE CODE:
(X)3/010/04]D/041-3
AUTHOR: _Gu1yayav0...Xu. G.; Epshteyfi, E. M.
ORG: nstitute-of Radio Engineering and Electronics, ca of Sciences SSSR
(Institut radiotekhniki i elektroniki Akademii nauk SSSR)
I/
TITLE: Acousto-thermal effect in semiconductors
SOURCE: Zhurnal eksperimentallnoy i teoretichenkoy fiziki. Pisima Y redaktsiyu.
Prilozheniye., V- 3,, no. 10) 3,966) 41o-4i3
TOPIC TAGS: thermal acoustic effect., pbonon drag, temperature gradient, semicon-
ductor crystal
ABSTRACT: The authors show that excitation of a monochromatic flux of phonons in a
crystal by an external source produces, besides the well known acousto-electric ef-
fect.. also a temperature gradient under adiabatic conditions. In analogy with the
acousto-electric effect, they call this phenomenon the acousto-thermal effect. lbe.
results of this effect are presented analyticaLly for a non-piezoelectric crystal in
vhich the carriers are characterized by an isotropic effective mass and a relaxation
time that depend on the energy, and in which a b~Tersonic wave propagates. * re- -
garding such a wave as a current of monochromatic phononu and by calculating the in-
tegral of the collisions between the electrons and the phonon current, the antisym-
metrical part of the distribution function is obtained, ftom which the electric cur-
rent density and the beat flux density are calculated. It is found that the effect

L 26124-66
ACC NR, MF15-806
reverses sign vhen the frequency of the byperanund is raiijed. The magnitude of the
effect in estimated at approximately :L04j_(deg/cm)/(*/cm2).- The authors thank V, L.
L
Bonch-RMevich for a discussion of the works Orig. art. has: 4 formulas.
SUB CODE: 20/ SUM DATE: 25Mar66/. ORIG RU: 002
Card 2/2 (1

.L 40282-65 -~,O
ACCESSION NR: AP5006171
AUTHOR,. ~~Gul aye Yu. P. (Saratov)
Y
iLwi6l'cyl nd
TITLE: Free torsional vibrations of a circular con'
anisotropy of a particular kind
SOURCE., Inzhenernyy zhurnal, v. 5, no.: 1, 1965, 199-195
TOPIC TAGS: torsional cone vibration, cone. natural' frequency,
sotropic cone vibration, orthotropic cone vibratlon!:
ABSTRACT- The problem of determining the~natural ftraquelIncy Of a. ;cirl-
cular cone possessing cylindrical anisotropy such; til-iat Ats :axis cpin4- i
.it radial plan'e
cides with the geometric axis of the cone and all: s
are elastic-symetry plams is discussed ., All p6ints of the baze 0f; -the cone, are, i
rigidly fixed. It is assumed. that the :cone ctoss flectiOns ,Ire not
distorted under torsional vibrations and that therii area no radial I dil-
placements.. The problem is reduced to an analogouii bone!. for an 160-
tropic cone with a 4.1fferent meridional croso seiztilctn V :means 0i I
corresponding transformation of variables, A g a a ei- a Iab 1u tion p i the
problem of free -tortiional vibrations is obtained f,rom Which the.'
C001 -.1/ 2.

1 1
SOLU'rav, Yu.P. . kand. tePbn. nauk; GULYAYEV, Yu.P., kund. takhn. nauk
Calculation of risern for steel Ingots. Stall 25
no,4231q-322 Ap 065. (MM lag 11)

GULTAYRV, Tu.V.
Scattering of current carriers on impurity centers. Fiz. tver.
tela, I no.3:422-431 Mr 159. (MIRA 12:5)
l.Institut radiotakhniki i elaktronikl, Moskva.
(Crystal lattices) (Somicanduct6re)

81359
AUTHORS:
TITLE:
3/181/'60/002/03/15/028
Boo6 B017
Bonch-Bruyevich, V. L.~ Gulyayevp Yu* V.4
On the Theory of Impact Recombination in Semiconductors
PERIODICAL: Fizika tverdogo tela, 10,60, Vol. 2, No. 3, PP,, 465-473
TEXT: In the introduction, the authors briefly discuss some papers
dealing with the influence exercised by the Auger effect on recombination
processes in semiconductors. The present paper deals with the problem of
impact recombination in semiconductors, taking into account the inter-
action between free carriers. Furthermore, the authors attempted to
estimate the amount of the exchange term on the capture of minority
carriers as well as the influence exercised by Coulomb forces on the
capture of such carriers by charged centers. First, the impact
recombination coefficients in neutral impurity centers are calculated
by using the same approximation methods as in Refs. 4 - 6, According
e
to Ref. 8 ~ (r) L exp(-qr)cos qr is chosen as interaction potential;
r
.11K
Card 1/3

8 59
On the Theory of Impact Recombination in 3/1811'60 002/03/15/028
Semiconductors B006/BO17
q - Y72 7Wme2 1/4 , n is the concentration of free carriers. An n-type
( F- 17)
semiconductor is considered, i.e., recombination takes place at neutral
centers. At a sufficiently high concentration of majority carriers, the
recombination cross section is determined by the capture cross section
of the minority carriers (holes). The processes contributing to the
matrix element of the transition (from state n into state k) are
schematically shown in Figs. 1 and 2. A general and some special
expre ssions were obtained for the recombination coefficient. The capture
cross section in n-type germanium at 3000K, P - m/m. (ratio between
effective and true carrier mass) - P 0.2, trap depth Et:!'-0-3 ev
(A E = 0.66 ev) is estimated to be ap lo-34n, CM2; cp =~ lo-17cm2 at
no = 107 cm-3. In the second chapter, the coefficient of impact
recombination is again calculated by using another trap model ("trap
radius" small compared with the thermal wavelength of' the free carriers).
In the third chapter, it is assumed that the recombination centers are
charged, and the capture mechanism is investigated for this case. It
was found that the charge sign of the trap exercises no influence on V
Card 2/3

On the Theory of Impact Recombination in .9/18 6 2/03/15/028
Semiconductors 3006YB017
the impact-recombination mechanism. In a capture of carriers at charged
centers, the recombination coefficient is reduced by the action of the
Coulomb field (compared with neutral centers). This reduction is, howevert
within the error limits of the computations. There are 2 figures and 12
references: 6 Soviet, 3 US, 2 British, and I Polish.
ASSOCIATION: Inatitut radiotekhniki i olektroniki AN SSSR Moskva
(Institute of Radio Engineering and Electronics of t
AS USSR, Moscow)
SUBMITTED: May 23, 1959
Card 3/3
4
P

201U
6/181/61/003/002/009/050
~43 0 0 (a P, d ./ 0 35, B102/B204
AUTHOR: Gulyayev, Yu. V.
TITLE: The statistics of the electron - hole recombination on
impurity centers in semiconductors
PERIODICALt Fizika tverdogo tela, v. 3, no. 2, 1961, 382-383
TEXT: The carrier recombination on multiply charged centers in semicon-
ductors has recently been repeatedly investigated, but the physical sense
of the trapping coefficients introduced in the case, in which to a given
charge state of the trap there correspond several excited states, was in-
sufficiently well explained. In the present paper, the lifetime of the
minority carriers in the latter case was calculated, and the sense of the
corresponding trapping coefficients was explained. A non-degenerate
semiconductor with sufficiently small trap concentration was investigated
under steady conditions. The index n numbers the various excited states
of the trap which capture j electrons. Por the trapping rate U( n ) for
ni
electrons from the conduction band in the nj-th state of the tr&D and
Card 1/_4

20112
S/181/61/003/002/009/050
The statistics of the electron - hole ... B102/B204
the trapping rate U(P) of the holes in the same state
U(n) . Z C(M'J-11n, nj n-P jnj,.l (1)
nj m J) fpm,j-l n
V(P) . Z:D(n,jjmpj-1) P-P (2) is obtained. Here C(...)
nj m NJ M,J-lpjnm
and D(...) are the ordinary quantum-mechanic trapping coefficients for
electrons and holes respectively in the nj-th state of the trap,
multiplied by the trap concentration and averaged over the states of the
carriers in the corresponding bands (if before electron- or after hole-
trapping the trap is in the state (MIJ-1)); n and p denote the total con- Vr
centrations of the electrons and holes and P nj the non-equilibrium
probability for the nj-th state, and
nj,,, No exp E. (J) - E. (I - 1) (3)
kT
IV exp
pis" 01M. kT (4).
Card 2/4

20111
S11811611063100210091050
The statistics of the electron - hole ... B102/B204
Here E n(J) and gni are the energy and the multiplicity of the degeneration
of the nj-th state in the trap, NC and Nv the effective numbers of states
in the bands. It is further assumed that the transition of the trap from
one state to another without a change in the number of trapped electrons
occurs within a considerably shorter time than a transition with change of
the charge state of the trap. The Fermi quasilevel Pi may then be
introduced for the charge state of the trap, which permits simplifications.
In the case of small deviations from epilibrium, the lifetime of the
pairs thus results in I P')
(no -f- P.) (5)
D -'no -4- PO
jC-,!PO
Cj Po'
'J-tC(M,j-1jn,J), (6)
D.j=ID(n, jim, j-1), (7)
M
0
where Pni is the equilibrium probability of the nj-th state of the trap.
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20111
S/18 61/003/002/009/050
The statistics of the electron*- hole ... B102YB204
Here CAj is the quantum-mechanical coefficient of electron capture onto
the nj-th trap level. averaged over the different excited states of the
trap with (J-1) electrons, i.e. over the initial states of the trap. As
P0 depends exponentially on temperature, the coefficient C may also
m,J-1 nj
depend exponentially on temperature. D nj is the trapping coefficient of
the holes onto the nj-th level of the trap, Summated over the various
states of the trap with (J-1) electrons, i.e. over the final states.
Cnj and Dni have a clear Dhysical senset they are averaged quantum-
mechanical trapping coefficients. The author thanks S. G. Kalashnikov
and V. L. Bonch-Bruyevich for discussion. There are 5 references:
1 Soviet-bloc and 4 non-Soviet-bloc.
ASSOCIATION: Institut radiotekhniki i elektroniki AN SSSIR Moskva
(Institute'of Radioengineering and Electronics of the
AS USSR, Moscow)
SUBMITTED:
.Ca=d 4/4
April 7', 1960

GULYAYEV, Y14V.
Statistics of electrons and holes in semiconductors with dislocations.
Fiz.tver.tela 3 no.4:1094-1100 Ap 161. NIRA 14:4)
1. Institut radiotekhniki i elektroniki AN SSSR, Moskva.
(Semiconductors) (Dislocations in crystals)
.1: ~ ~. 5: ~j , ~ -
-~ v;* -

---/181/62/004/005/07)1/055
B108/B112
AUTI:0:1: Gulyayev Yu V
T I '_"L7 On the theory of carrier recombination on linear dislocations
in se!-Aconductors
PE-RIODICAL: Fizika tverdoeo tcla, V. 4, no. 5, 1962, 1285 - 1289
T'~".11'2: -The effect ot' the Coulomb barrier at. a dislocation on the electron
ca,~ture uc)on a char,:-led linear dislocation is calculated by a quantum
mechanical method (V. L. 3onch-Bruyevich. I-FTT, sb. 1!, 182, 1959) in
quasi-classical ap,-,ro-xination. G,-%ing to the tunnel effect, the Coulomb
barrier is rather weak when the temperatures are not too low ("'~ 1000i:)
in the linear dislocation case, as well as in the case of impurity centem
.'.t low teimperatures the efCect of the Coulomb barzier at the dislocation
incroases considerably. T'-is is due to the change in shape of the barrier
at low temperatures owing to deionization of the donor impurities and in-
crease of the screening radius. ',7hen the temperature is lowered from
100 to 12-50K, the electron capture coefficient may decrease by some
orders of magnitude. There is I table.
Card 1/2

S/161/62/004/005/031/055
Gn the theory of carrier ... B106/B112
ASSOCIATION: institut'raadiotekhniki i elektronilki ANI 555R (Institute of I
Radio Engineering and Electronics AS US'SR) :ioscow
3U3';4ITT7-D: January 2, 1962
Card 2/2
.J,.

L 18393-63 EWT(1)/M(k)/EDS/E3(w)-2 AFFr/ASD/E;'-:'D-3/'IjP(C)/S,-JD/'AY,,L
Pi-4/Po-4TPab-4/Pz-4 AT
ACCESSION NR: AP3003718 S/0109,*63/008/00-,'/1179/1186
AUTHOR: Boncl.-Bruyevich, V. L.; Gulyayev, Yu. V. 7q
TITLE: M echanism of generating plasma oscillations in a semiconductor
SOURCE: Radiotekhnika i elektroaika, v. 8, no. 7, 1963, 1179-1186
TOPIC TAGS: p)asma oscillation, semiconductor
ABSTRACT: Tr~,nsformation of energy supplied to a semiconductor into plaEma-
oscillation energy was investigated by D. Piner, and J. R. Schrieffer (Phys. J~ev.
1961, 124, 5. 1387). The present article deals with the subject on a wider scale;
it considers theoretically all possible types of oscillations with an allowance for
recombination of carriers. Bipolar-plasma waves in an isotropic homeopolar
semiconductor are generated by a stream of electrons. The hydrodynamic
approximation is used in setting up the initial differential equations describing
concentrations and average velocities. Both types oi plasma oscillations,
Card 1/2

L 18393-63
ACCESSION NR: AP3003718
floptical" and "acoustical, 11 are dealt with. Conditions of excitation of oscillations
are examined, and the critical drift velocity (10 5 -1CP cm/sec) is found. Effective
mass of donors is determined. It is inferred that: (1) generation of low-
frequency plasma oscillations is easily realizable; (2) the possibility of generating
high-frequency o.,;cillations is not clear. "The work was resumed on the initiative
of S. 0. Kalashnikov to whom the authors are greatly indebted for his support and
discussing the results and the possibility of experimental verification. The
authors are thankful to M. Ye. Gertsenshtey and V. 1. Pustovoyt for their per-
mission to read their work before its publication. 11 Orig. art. has: 33 formiilas.
ASSOCIATION: none
SUBMITTED: 26jun62 DATEACQ: OZAug63 ENCL: 00
SUB CODE: G---- NO REF SOV: 006 OTHER: 003
Card 2/2

L 22186-65
IJP(c'j ATF
ACCESSION MR: A~5001848 5/0056/64/d4-7/006/2253/2251,
-AUTHOR:,~
V Fustovoyt
r
TITLE::
~MPUUC65tion of 'surface ~waves'in semic
ond.uctors.
n
Zhur al eksperime allno i teoreliA6sk ' .4 ;4
nt OY fiMiki*
no, 6p 15Kt
22,51~2253
-TOPIC TAGS: surface wave, wave an~plification, semiconeluctov~ e.nsi~',
carrier d
carrier mobility, sound speed, piezoelectricity
ABSTRACT, It is shown by a quasihYdrodynamic analyals.06t.4urfst0e: waves c 0m bei
ConGJS~L
amplified in a layered system Uing oft' aVain sad,con, ina.~,~~er and:n~
semi-inf inite piezoelectric (or vice versa), using. the, phenmenon'. Oherebythe
electric field the., accompanies an elar,,tic wave in the: piezio,electric penetra;tes
into the semiconductor, in Xhich tWcarriers move in a, definite: ilimction. This'
is analogous to the amplification of acoustic -waves obaer;,re~, In -1.,j-.miconductors
ienen the carrier drift velocity exceeds the phase velocity~ Of: the': acoustic k~ye.
In the case considered here amplification will take place when thik directioriaJi.
velocity of the carriers in the superconductor exceeds the It llasc:,ipelocity of the
Card 1/2

L 22186-65
ACCESS1014 NR: AP5ooi848
it
SUrface values If- am 1 efiected'i'l,the: power f 61
P ification is* petl,
.s 0 0
semiconductor can be markedly r_educed:by using a emic: ndu6t r wii~~: large q a~'ri-ieti
mobilit~r. For example, for pure InSb with apProximate ca~,~iLw d~ji~ity 1012
and mobility j04 cm2/v.see the power dissipation is about 0~117/clil which is~
ower than in the case of CdS. It.is pointed out,
much 1 in'thie: coni!:D~sion that a
similar analysis can be koplied to other types of surface
Particularly,
plasma waves. I'We thank V. L. Ginzbi= , S. G* hnil;q r, V L., l;B e.,~~qh
Kalar _Onch:rgrL
and L. V. Keldy*s for a discussion of the work." Orig. arv. haz; .4 figures!'
ASSOCIATION: Institut radiotekhniki i elektroniki (1n3tJ Wtp,
eering and Electronic ut f1z;Lko-
of Ra -,s,, n of Sciences SS;3R):
_~e_khnicheskikh i ra6iotekhnicheskikh i=ereniy_-___-- :J-,
Phyfl.clitechnical",
Cjq
_4pLc Lio Measurements).
sumnTED: 2oTun64
SUB CODE: GPI SS NR REF SOV: 004 A:; nl:MR: 001
2/2
Co?d

4TW/T/90-0) UP(a) AT
L 65261,65 Z
I ACCESSION: 14R., 05014233
AUTHOR.# Gulya
Vt
in
iTITLE: The Faraday effect on "hot" alectrons
A is ii'llvredakt T u.
SOURCE: Zhurnal eksperimentalinoy i tooratichaskoy: f iziIJ i
Prilozheniye, v. -1, no. 3, 1965, 11-15
!TOPIC TAGS: semiconductor theory, electron gas, Faraday eff5tict, pol6rira-
tion
.ABSTRACT: The various*characteristics,of a semiconductor (eiVctr,1.cik'l conduct'ivit!r,:
magnetoresistance, tbermomagnetic affect, etc.) may bE! ~ C003i1N!rab1y! altered by
,:beating the electron gas in the semiconductor ' The atithcor ekaminfis:1 the effect
:which heating of the electron gas has on Faraday rotatioT; pfjhe plane of p I~Irlztl-
tion of- an electromagnetic wave passing through the -The: degr--!! of'z
"ho"ness" of the electron gas is given by the electron tC1nrfei:'41tux!6 IT i4hich%difftirfl
from the lattice temperature To. It is assumed that the Maghotic ifield. is and
ithat the frequency of the electromagnetic wava iis rather lu, :-,:'N'i.t quantuin:~ ef -
So
)feats may be disregarded. A unipolar semiconductor is ccnsidixed"n which the cur-
Card
1/2- .. .....-

L 65261-65
-- ------- -- j
ACCESSION NR4. AP5014233
Irent carriers have an isotopic effective mass ~r, 4, band tho i6erse 1 tion
x4se relaxii
I q' The atitlior,
Itime Is related to the carrier velocity.by the _exPreSSiOl T I
11imits himself to an examination of weak heating.of tht olq!ctron'~ka;s~ It is found
Ithat the polarization plane may be rotated on, the order of 1.11 /cffl. ( 6der bptimian:
it -4 41 ').
1conditions) in extremely weak fields (e.g. in InSb at 401(,,_j: ab6~it, 10 On: A
iweak external electric field causes a rotationjwthe polai4;iati6o, plane, ofAt1he j
;electromagnetic wave~which is proport*onal tozthe square of,4he ftield atrength.
15. L. Bonch-Bruvevicl shits!and
"The author thanks S. G. Kalashnikoyv ~i,- big
1-717
a das.
i.4. Kogan for discussing the work." Grig. rit' ha's )Mtj
!ASSOCIATION: Institut radiotekhniki i elektrcniki Akadeinii''TaukAMR
I Institute j
iof Radio Engineering and Electronics, Academy of kiencea,sISR)
CODE;: qs- EM -
jSUBHITTED! IgHarSS 00
SOB
OTIMR: :002
*No REF SOV., 002
~/2
M

IL 2424-66 1,7WT%tj) j IJP(c)
ACCESSION NR: AP5021138 TJW03861651002100 ooo3/=6
AUTHOR: GU3-V&VL-V. YU. V. S,
i TITLE: Possible existence of "necond" spin waves in fo?rramgnets
SOURCE: Zhurnal eksperimentallnoy i teoreticheskoy fiziki. Pintma T redaktaiYus
Prilozheniyep v. 2) noo 1) 1965P 31-6
TOPIC TAGS: spin wave theor7p sound wave) spin phonon interaction, ferromagnetism,
collision integral
ABSTRACT: The author eNamines the possible existence of secondLar7 excitations in
the system of magnone in a ferromagnet. In analogy with giecond soundy these
secondary excitations are called "second spin waves" to distinguish them from the
"first" waves) the .magnons themselves. Neglecting magnetic dipale-dipole inter.-
action between the spins of the atom and the spin-orbit interaction) it in show".1
that in some temperature range above the Curie point the ivagnon gas in the ferro-
rognet is perfectly analogous to a gas of molecules tbat collide relative37 fre-
quently with one another and rarely experience inelastic collisions actompanied
by a change in the number of particles. Just as second sqund rames can propagete
in ouch a gaep second spin wuvea -can propagate in tho rmgwn. The. Yelocity of the!
spin waves at room temperature is estimated to be of the onler of 10'9 am/see for
Card 1/2

L 2h24-66
ACCESSION NR: AP5021138
most ferromagnets. Relaxation times of the order of ID-1-1 and 3X6 are estimated
for intermagnon collisions in which the number of magn=a is conserved, and for
scattering involving a change in the number of magnona (in the total magnetic
moment of the system)j respectively. It is also shomi that the dispersion of the
second spin waves is linear) and that thece waves should iminifest themselven as
macroscopic waves of the magnetization., of the spin specil'ic heat (or the spin, il
temperature)p and of similar thermodynamic quantities. Masurement of the veloci-!
ty of second spin waves could yield independent information on the *agnitude of
the exchange integral I. In addition, one can apparently expect a unique resonant!
interaction in a crystal between second spin waves and ordinary mound waves tlmt
also possess a.linear dispersion law and a npoy equal propagation velocity. "The',
author is grateful to V._L.-.Bonch-Bruyevic ,81.' G. Kalaiftdkov...A. V. Vashkovsklypi I
and Ia. A. Monog 6- forMUM-777
_~3"or a discussion of the work." Orig. tat. M165 G*
9-,1, C:5- (021
ASSOCIATION: Inotitut radiotekhniki i elektroniki Akademli nauk SSSR (Institute
of Radio Er4ineering and Electronless A,,1,adMW of scieffielposs )
SUBMITTEDi 14May65 BUM 00 am COD91 124153
NO REF SOV--.- 003 OTHM 001 ATD PRESS-
Card 2/2 ft

L 9253-66 EV1T(1)/E-'1A(mj-2 IJP(c) Al____
ACC NRs APS022722 SOURCE CODE: UR/0181/65/007/009/2772/27
./ 1/' ti VY' 5-- ~--- A
AU'rHOR: Gulyayev, Yu. V.; Zillberman, P. Ye. 4
_9' il lt~
.
U
ORG: Institute of Radio Engineering and Electronics, Moscow (Inatitut radiotekhniki
i elektroniki) ---
TITLE: Resonance amplification of Rayleigh ultrasonic waves by a bean of charged
particles passing close to the surface of a crystal
SOURCE: Fizika tvardogo tela, v. 7, no. 9, 1965, 2772-2779
~ I r Ll 1, j.". .' _-
TOPIC TAGS: semiconductor theory, ~Uleigh wave, ultrasonic amplification, cadmium
sulfide, plasma charged particle, Plasma resonance, electron beam
ABSTRACT: The authors study the interaction between surface Rayleigh) waves ina
CdS type crystal and a beam of electrons passing through fissures of arbitravy width
inside the crystal. When a fissure is wide, the curve fvv amplification as a functior
of frequency is a set of non-overlapping spikes. Under optimum conditions, the ampli-
fication may be as high as 1%,400 db/cm. However, In practical instances it is of the
order of 1 db/cm at Al Mc. It is shown that convective instability may appear at re-
sonance (coincidence of frequencies and phase velocities) of the Rayleigh and plasma
waves in the beam. Dispersion curves are plotted for studying the nature of this
instability. It is found that the maximum amplification is reached at the lowest re-
C.rd 1/2

L 9253-66
ACC NR- AP5022722
sonance frequency. The authors are grateful to V. L. Bonch-Bruyevicb for discussing
22 fomu-las. w YJ
the work. Orig. art. has: 2 figures,
SUB CODE- 20/ SUBM DATE: 12Apr65/ ORIG MF: 004/ OTH REF: 003

L 36546-66 E'IIT(I', Ij~c) M1
-ACC NR: Ap6o16836 SOURCE CODE: UR/0046/66/012/002/0253/0255
AUTHOR:- Gul-vavev. Yu. V.
ORG: Instft~f6_'o_f Radio Engineering and Electronics. AN SSSR (Institut radiotekhni-
ki i elektroniki AN SSSR)
TITLE: Rotation of the plane of.polarization of sound in a magnetic field in piezo-
electric semiconductors
SOURCE: Akusticheskiy zhurnal, v. 12, no. 2, 1966, 253-255
TOPIC TAGS: piezoelectric crystal, cadmium sulfide, ultrasonic wave propagation,
dispersion equation,_,dielectric constant, semiconductor carrier, carrier scatteringl
'6~j _ -r
'7a'u'vo w6vel _c r/90M/9'5:'vE Id- w4ve-
ABSTRACT: The semiconductor considered is CdS oriented in such a way that its
crystallograpic axes coincide with the coordinate axes. A plane-polarized trans-
verse ultrasonic 'wave propagates along the Z axis, and constant magnetic and elec-
tric fields Ho and F4D are applied along the same axis. A dispersion equation is
obtained for the coupled electromagnetic and sound waves in terms of the left- and
right-hand polarization components of the plane-polarized wave and the complex di-
electric constant for these waves. The strong interaction between the electromag-.
netic and the sound waves occurs when the separate dispersion curires for the sound
,-Card 2/2 uDc: 534-:L6: 537-311-33

L 36546-66
ACC NR: Ap6o16836
12
wave and for the electromagnetic waves intersect. In view of the weak coupling
between the sound and helicon waves, a resonant interaction between them is possible
only in a sufficiently large constant electric field. An expression is obtained
for the rotation of the plane of polarization of the sound wave under such condi-
tions. It is concluded that observation of this rotation by experiment would yield
information on the piezoelectric constantup on the carrier scattering mechaniBm,
and other data. The author thanks S. G. Kalashnikov and V. L. Bonch- rich for
a discussion of the work. Orig. art. has. formulas.
SUB CODE: 20/ SUBM DATE: 05AprOV ORIG REF: 003
2/2/ ~U,,P

XCC kR'1__-AP6O36158*6 SOURCE CODE: UR/018
011/3366/3372
AUTHOR: Gulyayev, Yu.'V.*
ORG: Institute 'of Radio Engineering and Electronics AN SUR, Moscow (Institut radio-
tekhniki i elektroniki AN SSSR)
!TITLE: Contribu tion to the theory or transport phenomena connected with the dragging
...of.electrons by 'ultrasonic waves in solids.
..SOURCE: Fizika tverdogo tela, v. 8, no. 11, 1966, 33a-3372
2.0PIC TAGSt transport phenomanon, kinetic theoryp electron Interaction, phonon dragj,
electron,gasp ultrasonic'effect, electron mobilityp acoustic propagation
ABSTRACT.:.,The author develops the kinetic theory of certain transport phenomena con-
nected with the transft?-of momentum from sound waves to conduction electrons and Thai
resultant draggii*,-of the latter in the direction of the sound. The ana4aia is con-
fined to wavelengths which are much longer than the electron mean free path. The
sound vaves are excited in a crystal situated in an external magnetic field perpen-
dicular to the direction of the.sound flux. The sound intensity is assumed veak and
heating of the electron gas by the wave is neglected. In view of the fact that the
ultrasound wave exerts a differw* dragging force on electrons with different ener-
gies, this leads to violation of the relations derived for this effect by G. Weinreicl
(Rwst -Rev* Ye 207$ 3Wp 195T) j, since the latter vere based on collectivt action of
the electrons,, where" actually at each instant of time there exist in the crystal
wd .1/2

. . . .. .... .. ..
ACC NRt ' AP6036986
spatially separated groups of electrons of different energy, characterized in general
by different relaxation times, and consequently by different mobilities. The pos-
sibility that a 'propagating sound wave in a degenerate conductor can give rise to Lt.
longitudinal teVerature gradient is predicted. It is shown that in the case of a
degenerate electron gas, the acousto-electric effects of Ettingshausen and Peltier
(and similar effects which are connected in principle with the energy scatter of the
eiectrons) differs from the magnitude of the effects predicted in this paper by Ithe
square of 'the ratio of the Fermi energy to the thermal energy. The author thanks V.
,L. Bonch-BruVevich,, L. V. Keldysh.. A. I. Morozovp and E. M. Epshteyn for a discussion
of the work. Orig. art. haq: 16 formulas.
SUB CME: '20/ SUN DATE: 28Ma66/ ORIIG MW: 004/ OM RM 005
Card 2/2

SHEREDEKO, V.14., Inzh.; GULYAYEVA, A.G., inzh.
Two-stage filtration of fate without intermediate receiver.
Manl.-obir. prom. P4 no.10:38-39 '58. (19RA 11:10)
1. Ktiybyshavakiy zhirovoy kombinat.
(Kuybyshev--Filtnrs and filtration) (Kuybysbnv--Oil and fats)

-,;- y - --, .. - -
-- T ~ , , t ,-L .
"Treatment of Superior Prognathism," Stomatologiya, 110. 3, 1948. chair orthoped
Stomatol. Ploscow Stomatological Inst.

ALEKSAIIDROV, B.M., nauchnyy sotrudnik; ALKKSANDROVA, T.N., nBuchnyy
sotrudnik; BELYAYEVA, K.I., nauchnyy sotrudnik; GORBUNOTA, Z.A.s
nauchnyy sotrudnik; GORtHMA-FMS3VA, L.I., nauchnyy sotrudnik;
GOREMVA, L.N., nauchnyy sotrudnik; GULYAUVA. A.M., nauchnyy
sotrudnik; DKITRKNKO, Yu.S.. nauchnyy sotradnik; ZABOLOTSKIY, A.A.,
nauchnyy sotrudmik; MAKAROVA, Ye.F.. nauchnyy sotrudnik; NOVIKOV,
P.I., nauchnyy sotrudnik; PGKROVSKIY, V.V., nauchnyy sotrudnik;
SMIRNOV, A.F., nauchnyy sotrudnik; ST]WAIIOVSLAYA, A.F., nBuchnyy
sotrudnik; URBAN, V.V., nauchnyy sotrudnik. Prinirasli uchastiye:
BALAGUROVA, M.V., nauchnyy sotrudnik; VXBRR, D.G., nauchnvy sotrudnik;
POTAPOVA, 0.1., naucbnyy sotrudnik; SOKOLOVA, V.A., nauchnvy sotrudnik;
FILIMONOVA, Z.1., nauchnvy sotrudnik; POPEMKO. L.K.. nauchnyy sotrudnik;
ZITSARI, N.A., red.; PRAVDIN, I.F., red.; FAIDWSHOY, A.P., red.;
..d3VCHENKO, L.V., tekhn.red.
(Lakes of Karelia; natural features, fishes, and fisheries] Ozera
Karelii; priroda, ryby i rybnoe khoziaiBtvo; spravochnik. Petroza-
vodsk, Gos.izd-vo 11arellskoi ASO, 1959. 618 P. (MIRA 13:8)
(Continued on next card)

AT-4-YSANDROV, B.M. --- (continued) Card 2.
1. Russia (1917- R.S.F.S.R.) Karellskiy ekonoaicheakiy admi-
nistrativnyy rayon. Sovet narodnogn khozvaystva.. 2. Karallskoye
otdelaniye Vsesoyuznogo nauchno-issledovatellskogo institute ozeraogo
i rechnogo rybno-go khozyaystva (for Aleksgndrov, Aleksandrove, Be-
1yayeva, Gorbunova, Gordeyeva-Pertseva, Gordeyeva, Galyayeva, Dmitrenko,
Zabolotskiy, Kakarova, Novikov, Pokrovskiy, Smirnov, Stefanovskaya,
Urban). 3. Karel'skiy filial AN SSSR (for Balagixrova, Veber, Potapova,
Sokolova, Filimonova, Popenko).
(Karelia--Lakes)

GULYAYEVA, A,,14., DMITRrIM0, Yu.S.; KMERSKI-Y, 1.A.
Results of the inti-oduction of the Baikal whitefish In
Lake Ukshozwro (southern Karelia). Zool. zhur. 42 no.6:
877-881 163~. (MIRA 16%7)
1. Karelian Department of tho State Research Institute of the
Lake and River Fishery Management, Petrozavodsk.
(Ukshozero., Lake--Whitefishes)
(Fish introduction)

KORINEYEV,
,Tli V
t1kov.
I-V p ru:i.
V.S., red.
[-y 4
Indus the
on si U jk%r
r

L 06431-4' ? FWT 00/:!:~!'( t ii P( C) JD/Jc"
--ACC NRt AP6026708 3011RCE CODE; Ua/oi8i/66/008/008/2472/2473
AUTHOR: Gulygev&LA. ~.; Ivleval V. S.; Iglitsyn, 14. 1.
ORG: State Scientific Research and Design Institute of the Rare Metal Industryt
Moscow (6osudarstvonnyy nauchno-issledovatellskiy i proyektnyy institut redkometalli-
cheskoy promyshlennosti)
~'J
TITLE$ Lifetime of excess charge carriers In InSb single crystals with Ge and ki im-
purities
SOURM Fizika tverdogo tola, v. 81 no. 81 1966s 2472-2473
TOPIC TAGS? indium. compound, antimonide, carrier lifetime, recombination
AILSTRACTZ The object of the work was to determine the affect of doping InSb singl&
crystals with Go and Au impurities on the recombination of excess carriers. p-INIpo
samx)les were obtained from the original n-type material (electron concentration
1014 cra73) by this doping. The carrier lifetimes 7-, were measured at 77-3001K by sta-1
tionary methods of measurement of -the photomagne tic off ect (r .) and photoconductivity I
(T ). The lifetime of electrons is inversely proportional to
' Ue concentration of tra~s.~--
A 77'K, in sampi3s doped with Go, the quantity 7er-OM changes by less than order
of magnitude as the Ge concentration increases by a fkctor of 200. This indi2ates
that . the recombiiiation does not take place on Go atoms. The lifetime data show that
the Ge impurity does not affect the recombination of excess carriers. In the 77-170'41
Card 1/2

L 06-aR-61
ACC NR.- AP60267o8
range, the lifetimes in swmples doped with Go and Au are approximately the savae, It
0
is concluded that in this range, Go and Au have no offect on the recombination of ex-
cess carriers, which tikes place either on structural defects or on a residual impur-
ity. Orig. art. hast 2 figures.
SUB COM 20/ SUBM DATES 31Jan66/ ORIG REFS 0021 CTII REFS 003
Card

kCCESSION NRt AP4034947
S/0181/64/006/005/1552/1554
AUTHORS: Gulyayeva, A. S.; Iglitoyft, M. I.; Petrova, L. V.
TITLE: The lifetime of charge carriers in disequilibrium in single crystals of
indium antimonide
SOURCEs Fizika tverdogo tela, v. 6, no. 5, 1964, 1552-1554
TOPIC TAGSs charge lifetimep temperature dependence, photogalvanomotric determina,-
tion, photoconductive aeterminationp charge carrier adhesion, Auger recombination
ABSTRkCT: The temperature dependence of the lifetime of nonequilibrium charge
carriers in InSb was investigated. Naturally alloyed (zone-melting) single crystali
13 14
of both p and n types having a basic carrier concentration of 7 x 10 4-5 x 10
per cm3 were studied in the 78-300K temperature range. Measurements were made by
photogalvenometric (FM) and photoconductive (FC) methods. A 500-watt tungsten lights
source was modulated at 1100 opa. The magnetic field was 0-205 webera/m2o The
samples were 14 x 4 x 1-5 mm3 parallelograms polished and cleansed with CP-4k.
Comparison was made with theoretical relationships presented by S. Kurnick and R.
Zitter (J. Appl. Phys., 27, 278, 1956) and by R. Zitter, A. Strauss, and A. Atto-rd
(Phys. Rev., 1159 226, 1959). Typical results are shown in Figures I and 2 on the
Card 1/5

;ACCESSION NRs AP4034947
iEnclosures. The character of the curves was the same for both measurement methods.
.For all samples (except a few n-type ones near the liquid nitrogen temperature)
!results differed (-r due to the adhesion of secondary carriers. At higher
FC >rFM)
!temperatures the difference disappeared, and the lifetime reached a innim of;
1 -7- -7 zed t
14 x 10 '1 x 10 see between 170 and 200K. The results,'when analy ogether
;with the ,eneral theory of recombination and the previous experimental data, showed
~that it vaa necessary to consider two separate temperature ranges. Below 250K,
irecombirLLtions of local centers predomin ted. The defining parameters w6re charge
:concentration, energy state, and degeneracy multiple. In this study samples con-
ained uninvestigated residual contaminants, so that the parameters remained unknown.
;By assuming that recombinations occurred at the centers with the same parametere as
i,those given by R. Laff and H. Fam (Phye. Rev., 121, 53, 1961), calculations we
:made to give electron r and hole.,r lifetimes. Experimental values and theoret-
n P
;mcal calculations differed by a value greater than could be explained by normal
ierror. At temperatures above 250K Auger recombinations are most important. Orig,
Z
jart. hast 2 figures.
ASSOCIATION: Gosudarstvenny*y nauchno-iseledovatelskiy i pr(Wektny*y institut,
:redkometallichookoy promy*shlennoati Moscow (Stato scientific Restarah and Desip
Card

!ACCESSIO*N'NR-l --'A24034'947
IIustitute of the Rare Metal India tx7)
ISUBMITTED: 21Dec63 DLTE ACqt 201lay"
SUB CODEt SS, NO REF SOVs 001
Card 3/5
ENCLs 02,
Omm 004

ACCESSION NR: AP4034947
Fig. 1. Temperature charLateriatics of
lifetime in p-type InSb.
(1) 1~ and -r ; (2) I-FG; (3) 1--
FM n p
1! 2.5 x 1o14 cm731 I-
"A D, FM
Card 4/5
ENCLOSURE s 01
k7-$
vs
7- P

ACCESSION URs AP4034947
ENCLOSUREt 02
IVA,
z
Fig. 2. Temperature charaoteristion of lifetime
in)U-type InSb.
0 -rrM; (2)
14 -3
X N 1.2 x 10 ca
D A
r
--rd 5/5

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is IIUIJMtjJ6 JIM
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sfir'A lost. .11mmst (U. S. S~ It.) N- 110.5 3.13
e ll -*W 1937~ [it 111IN 111olmstraph a thcull.
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GULYAMIA, A. V.
Gulyayeva, A. V. - "On certain prospectin indications of floursrwrll, Trudy VBPsoyUz.
nauch.-issled. in-ta mineral. syrIya, Novaya seriya, Issue 1, 1949, P. 3-6, Bibliog:
7 items.
SO: U-4631, 16 Sept. 1953, (Letopis Inykh Statey, No. 24, 10/49).
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KRAS" GAll I.I.L., I o :
pr'ly."; V.I.; S1!JDS1JIT'SKT,, ').S.; ','TL(ATDOV.,,,
V.Z,- GUL'M-EVA-,--.E-.G,; KOUMTAROV, K.D.
Clinion.1 vieLhod of diennosing intraocular -tinors iisin,-, radic-
active phosphorus. Vest.oft. no.3:3-9 It-Jr-, 162. ITE'A
1. Kafedra glawr4di bolezrey 1. kz~fedrv, neditsinskoy radiologi--
TSent-vallnogo instituta usovershenstvovardya vr--..cliey (for Kr-asroxr,
Grishina, Sivoshinskiy). 2. Moskovskaya glamaya 1dinicheskrya
bollni-tsa (for 11i'lovidova). 3. Vst-soyiwri3"j
sk,17 instituta nieditsbiskogo instrumentariya ~. oborudovani.-
(for Agranat, GLi-lyayeva Kolontarov).
(Eyri-miml (PHOSP"10,T?us--Isoq,cq"~~.,.s

GULYAYXVA, F.Ye.
Changes in the rate of blood flow under the influence of neurotropic
substances. Terap. arkh. 28 no.4:41-114 156. (MIRA 9!9)
1. Iz gospital9noy terapevticheskov kliniki (dir.-deyst-7itellnyy
chlen AMN SSSR prof. A.L.Yqasnikov) I Moskovskogo ordena Lonins,
meditainskogo institute Imeni I.M.Sechenova.
(BLOOD CIRCULATION
flow rate, off, of US funct., determ. with aminoacato-
phenetidin & amobarbital sodium)
(CIRITRAL NERVOUS SYSTAK, physiol.
off. on blood flow rate. determ. with aminoaceto-
phenetidin & amobarbital sodium)
(ACI&TOPHISILTIDIN, deriv.
aminoacatophonetidin, off. on CHS in determ. of CNS
regulation of blood flow)
(EMITURATES, off.
amobarbital sodium, on CNS In determ of ONS regulation
of blood flow)

?4A~Db
30469
s/l3q/6l/ooo/oo5/oo5/0l4
E194/E135
AUTHORS: Dunayev, F.N., and Gulyayeva, G.P.
TITLE: The influence of-elastic compression on the initial
reversible magnetic susceptibility of ferro-magnetics
PERIODICAL: Izvestiya vysshikh uchobnykh zavedeniy, Fizika,
no-5, 1961, 44-48
TEXT; On the basis of Ye.l. Kondorskiy's theory,
S-V. Vonsovskiy (Ref.2: ZhETF, Vol-17, 1094, 1947) developed a
theory of initial reversible magnetic susceptibility which took
account of weak magnetic fields as well as of elastic stresses,
which also displace the domain boundaries. The-theory has been
checked in tests made with tensile stresses but hitherto
compressive loads have not been tried, and this is the object of
the present article. The experimental materials were chosen to
cover a range of constants of magnetic aninotropy'and of
magnetostriction. The samples were mechanically worked and heat
treated in various ways. The initial tests were made on work-
hardened samples with high internal stresses. The work hardening
was set up by rolling or forging. Then all samples were given
Card 1/7'

30469
The influence of elastic compression.. S/139/61/000/005/005/014
E194/E135
No.1 annealing for 6 hours at 600 OC in a vacuum of 10-4 = Hg and
reinvestigated. All the samples were then given No.2 annealing,
two hours at 900 OC in vacuum, and retested. Samples of
66-permalloy were also given annealing No-3 at 550 OC for 20 min,
cooling at a rate of 100 OC/hour*in a longitudinal magnetic field
of 25 oersted, to set up a magnetic texture. Table I gives the
composition of the materials investigated, the sample sizes and
coercive force in various conditions. The magnetic permeability
was measured by the ballistic method and the initial permeability
was determined by extrapolating the permeability measured in weak
fields to zero field. The maximum error of determination of
permeability was about 6%. A special rig was devised to apply
compressive stresses to the samples, most of the samples being
covered with tubular guides to avoid bending. The error in
determination of the stress was about 1%. The coercive force was
determined to give a qualitative assessment of the influence of
internal stresses after the various heat treatments. Curves of
magnetic induction and magnetostriction were determined to find
the character of the magnetic texture. The magnetostriction
Card

30469
The influence of elastic compression... S/139/61/000/005/005/014
E-194/R135
curves were determined by means of wire strain gauges. Fig.2
shows curves of the initial permeability of transformer steel with
4.1% Si as function of the compressive loading in kg/MN2. Curve 1
relates to the work hardened specimen, curve 2 after No.1
annealing, and curve 3 after No.2 annealing. It will be seen that
the two annealings considerably relieve the internal stresses and
increase the initial permeability. Similar curves were obtained
for transformer steel containing 3.4% Si, for the dynamo steels
and for the armco iron. Similar relationships are also obtained
for the 66-permalloy which was not subject to thermal magnetic
treatment except that the initial susceptibility of the work-
hardened specimen was practically independent of the load. In the
initial part of the curve for armco iron there is a clearly
expressed maximum. These results are explained in terms of
Vonsovskiy's theory: they correspond to the results that would be
expected for materials with a positive magneto-striction constant
X100 and an axis of easy magnetisation of the type [100] .
Fig.4 shows the relationship between the initial permeability of
electrolytic nickel and the compressive load. Curve I is for the
Card 3/7'.

30469
The influence of elastic compression... S/139/61/000/005/005/014
E194/E135
work hardened condition, curve 2 after No.1 annealing, and curve 3
after No.2 annealing; again the load is given in kg/MM2. Nickel
ha negative magnetostriction and an axis of easy magnetisation of
th: type [111] and for this case Vonsovskiy's theory indicates the
presence of a maximum in the curve of the initial permeability of
the nickel as function of the compressive load, as is indeed
observed. Curve 4 on Fig.4 was obtained on a specimen which had
received No.2 annealing and was then slightly work hardened by
bending, and it will be seen that this reduces the value of the
initial permeability and displaces the maximum relative to
curve Ytowards higher loads, as is predicted by Vonsovskiy's
theory. It is concluded that the experimental data are in good
qualitative agreement with Vonsovskiy's theory. Ya.S. Shur and
D.D. Mishin are mentioned in the article for their contributions
in this field.
There are 4 figures, I table and 9 references: 8 Soviet-bloc and
the following English language reference:
Ref.5: E. Williams, Phys. Rev., Vol.52, 747, 1004, 1937.
Card

30469
Th6 influence of elastic compression... S/139/61/000/005/005/014
E19VE135
ASSOCIATION; Ural'skiy gosuniversitat imeni A.M. Gor1kogo
(Ural State University imeni A.M. Gor'kiy)
SUBMITTED: July 19, 196o
Card

-111728
S1 I 37/6VOOV002/1 44/ -14.,
A052-/A 10 1
Aul-HOPS- Korzh, P. D_ Gulyayeva, G. P,
-i~ -'hr thenmonlectric method of determining Sb In Pb-Sb silloyn
-7F i3Z,-.~AL Referallivnyy zhurnal, Metallurgiya, no. 2, 1(62, 111, 1 tr, t. --K'-
(`Sb. nauchn. tr, Magnitogorskiy gornom,~fallur;;. in-- no. 21
1961, 12-19)
The thermoelee*ric method of determining Ob in Pb-5b allcy~s 1~~
de:3r,,rtb~~d. The method is based on measuring the relation tetween the thc-rmo-
-~le~:tromotive for2e -and Sb concentration. Three methods of ccn~ncttng samples
wi-h a ccmpar,-~son element were tried. 1) Sn soldering, 2) a conta-,t ty
m,,?ns of' ms~-hanical clamps, 3) a contact through a molten metal. By th? third
me-,hod the alloy sample and the comparison element were s.itm-~rged, with one eni,
into a molten Wood's alloy. The thermoelectromotive force of Pb-Sb samples wa~-
rn~-a-su---d on the 11PTa -1 (PP'.PV-1) direct current potentiometer by the compensa-
tion method. Bi was used as comparison element. The Sb content was studled -,r
binary allcys --ontaining 4.7 - 8.5,14 Sb. The calibration curve is plotted as
formed by the sample and B1 electrode was hea-.ed r.,
Pollowz on,,

~;/I 37/62/000/002/ 1441141,
Ni~
- -h~rmaelle-! ric method ... AO 52/A 10 1
0 -11 W~- I -, 1 h,-:.1 ends te Ing at 180C. 7he thermcele--tromo'ive- for- was
Mc V~,~--d 10 lr~* -, IMeS. it waz found that the thermoelectrorn~)!.,.-~te Of
--ti I-ys decr,eases with an tn,,reased Sb conlent I,v 'ILH- lirear. 11w. 11n,
ol~ InctivLdual determinations from the mewn value dL-d not ex--eed
0 Tht:re are 6 references.
LAc-s!.-a:~'-I~rf- note., Complete translation]
a-j 112

KQRZH, F.D.; OUAXEVA,_~~J.,- GINIYATULIN, I.N.
Thermcelectric method for determining antimony in lead-antimony
alloys. Zav,lab. 29 no.3:289-291 163,6 (KM 14:2)
1. Magnitogorskiy gorno-metallurgiches4y institut.
(Antimony-Analysis) (Lea-4timany alloys)
(Thermoelectricity)'*

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L 28537-66 EWP(j)/EWT(m)/T/F1JP(t)/ET1 DPW NIJDIAY-C--D
ACC NN AT6013804 SOURCE CODE: UR/0000165/000/000/0296/0304
r
AUTHOR: Rozenfel'd, I. L.;. Persiantaeva$ V. P.; G
ORG: none
TITLE4. Protective properties of inorganic inhibitors In the presence of extraneous
ions
SOURCE: Korroziya metallov I splavov (Corrosion of metals and allo-1, no. 2.
Moscow, Ixd-vo Matallurgiya, 1963, 296-104
TOPIC TAGS: corrosion Inhibitor, Lon, sodium compound, sulfate, chloride,
electrolyte
ABSTRACT: Inorganic inhibitors, which chiefly Include aodium and potassium salts of
acids whose anions contain atoms of elements V IV and VII of the periodic table, are
widely used to protect metals against corrosiain neutral media. Yet despite the.
numerous studies of these inhibitors, the interaction between inhibiting and ag-
gressive media still has not been adequately investigated and hence the effectiveness
of the inhibitors in various electrolytes cannot be predicted. To fill this gap, the
authors investigated the corrosion rate of Fe as a function of inhibitor concentra-
tion for's fixed concentration of aggressive ions (Cl"', i6h, . In addition the
protective concentrations of inhibitors for various concentrations of aggressive ions
were investigated; this made it-,,10osible to derive a nathematical relation for
Card 113

- L 28537-66
F-ACC NR, AT6013804 0
calculating the required amount of inhibitor for real systems. Thus the dependence
of the protective concentration of such compounds as Na2WO4, Na3PO4, Na2.MO04, NaH2PO4
on the content of sulfate ions (SOZ-) in the solution is expressed by the equation:
Y = 0.17X + 0.003, where Y is molal inhibitor concentration, and X is molal concentra
tion of aggressive ion. For the aggressive ion Cl" the corresponding relation is:
Y - 0.38X + 0.005. The accompanying electrochemical tests pertained to electrode
impedance which, as was anticipated, differed depending on whether the inhibitor form
phase layers or adsorption layers at the surface of the protected metal. The corro-
sion rate of metal as a function of inhibitor concentration in a solution of
30 mg/liter NaCl and 70 mg/liter Na2SO4 was found to decrease in all cases -- except
monosubstituted phosphate and sodium vanadate -- with increasing inhibitor concentra-
tion (Fig. 1). Thus, the investigated inhibitors may be arranged in the following
series of increasing protective capacity:
Na3PO4 k' qi_2HPO4_X_NA2WO4 >-NajMoO4-> NaHIP04 > Na2VO4-
It is found that these inhibitors markedly alter impedance when the current applied
is small, do not affect capacitance characteristics in the presence of high fre-
quencies but somewhat reduce ohmic resistance at these frequencies. Such changes in
impedance indicate that inhibitors-of this type (XO n') alter the polarization
4,
tharacteristics-of the system. Orig. art. has- 9 figures.
Card 2/3

ACC NRt AT6013804
4
2
td r-41.5
0
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Fig. 1. Metal corrosion rate as "a function of inhibitor
concentration in solution containing 30 mg/liter NaCl and
70 mg/liter ka2SO4:
I - trisodium phosphate; 2-'Y sodium tungstate,-, 3 - mono-
substituted sodium phosphate; 4 disubstituted sodium
phosphate; 5 sodium molybdate; 6 sodium vanadate
SUB CODE: '11; 07'~ SUEH DATE: 19Jul65/ ORIG REP: 005/ OM 006
REV:
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GULYAYEVA, L. A.
"Vanadium, Nickel, and Copper in Petroleum ut the Wala zind Volga Region" VIA
AN, 1-2, NP, 6, 19111., Tnglt, MITIaral Y'viala, Anfil ilat, USSR.

GULYAYEVA, L. A.
"Disbribution of Boron in the Waters of Azerbaydzhan Oil-Fields and its
Correlational Value, Dok, AN, 35, No. 3, 1942,

(11.9-YAY]WA, I.. A.
"Boron Distribution in Recent Organogenic Deposits," DoIc AN. 37, No. 1, 1942.

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SLA "tALLUACKAL ulfsa?Wt CLAISSIOPKA111001 It ue 0
t Owl I I a r" .1 if 00'11
" 1111 a I IA ' I j ,1 4 t, 1
10 03WI 1 1, 0411
0 0 0:6 0 00 0 0 0600
60,6 0, 0 0 0 04 0

FW-W-,W-
J41$ )4'"*)Ib Sal LF 11 It a 11 41 -1
lp to 11 a
c- AA fie CC W t( d 0
Pt 90 Ctafrellstar that atilat anj bilullivas of that
Urmal-vop fee- accordit4 10 micrOcIt"Itaitla. L. A.
(Ittlyerva Cipt. %filters] Flaul-. Av;&d. St.
441, 1:1 .1,; 11 it, dkk
y
N-k X S S-R, 48, 11 111, 841".1 N, Al*.
"it' 41111 611111111111, W th, Ural-VAig. r,KwI, 1111hly
vArluldr, although Ni ltluy, rNt_l, Cli,
I tic V: N
j;:; rww i, failly const. III CalIKIIii((-ffPUI allot I.-At" ilvar-
I- iman oils %':.Ni pvrtlliall
-It,
Ni illifival fit v tif tall %*41111 t., hox"Lat i'm it,
goo
Oil
sell Ire*
:too
luee
tta.,
- ---- -----
It.
4 alI
An I 1 9
IC
of w a 't a it it aalto n
le 110 0 0
I'D 0

GULYAYNY
Boron content of recent marine sediments. Dokl. AN SSSR 60 no.5:
833-835 KY '46. (KLRA-lOt8)
1. Institut goryuchikh iskopayemykh Akademli nauk SSSR. Predstav-
leno akademikom S.S. Namtkinym.
(Boron) (Sedimentation and deposition)

Distributim of amall somrite of nickel and comr in
Upper Permian depoeilts 91 Tatar A 3 S lt~ I.. A. Guly.,-
it.-mill F, S. ItkinA Wad.
---~Md. Naak S.S.S.R. 70, W-MISMI.-AnAlywal r,---
,,ults arr given for small aints. of C4 and M. .1kamph,
rutln,r high in Cu (atxjyc W-111) X 10-8%) do not
vitrichiAwnt ("Utive) in 141. AAMI as a nuAtter Ali Lart. CAI -
el richtif carl,on.Atr rocks show i jecline of Ni to 111 61 ;
lcvirl,; only in gIvIxmits od clAy type olwi a Arriativrly litIch
~.i IA,vA Act"ugxiny Cu. In c-Arimmutes the Ni /Cu rmw
is 11.1018-41.3, while In 04yi it is unity or higher. '%'I I,
thus lAoinul to the terrigenoui (Awit; carixxi,tres f--in .4
zone in whk,h is un. nl Co froni Ni Wkr% place ohnin I Ilic
%rcon,14ty mintro pf(WA-4..-S.
R S U 4 ~ r~

UULYZMTA, L.A.
Chloride content in Devonian sediownts. Doklady Akad. Namk S.S.S.R.
80,911-13 051. (MMA 4:10)
(CA 47 no.13:6318 153)

u1
rx
6-t,
wt A
.is

_hYF-

--
~
pctfr
7
Obfifical Absto
willm from-2 to 5, lqftifi~ (W
Isai(trrmin Ifem

Vol. 48 too. Rw
Vatic& (mm
,
Z -am Iffrs oat
116k

Apr. 10
1954 -
ett - V or NI t I u
I
f
r.4
1 it, hut (Itt tht Cott-
a b
O
t
1
9
i'
l ch
U (MIry. 11 IM it Ikii o
d
f
f
a 1
1:
t It
em
w
al
y
V
Ni
l
I
am
M
Mmralogical And Geologica
7 t- fl
9frmAq:2t. u14 o
I
f r-
.
=A
a, *
cevic0c emcco wAs m%
. m this ccr (l. A mmpaciwi
C4 Or Or1r.. mamr4ntAls d: r0
pe ciatcam
Im-We g ~Irmm thcTe
a WO'll'i
olly
) jave
t P't D
Car the 0MUMPOO" t ixt D
Wan h .
?
jA CarbuitiNfom
not rdst XqUaby

-11(1053)-tkol, dcpo~jlkof Attracted;: j
'
atteatiou ~iut:o A. D. Adlvulpl'%~if C.A. 21
4
sped
J.. '1WAI t la tit
~,1804) mignett tO:fl%S poilonill~ the Pfin4 0 ~1 It it
t ,m-,idrtlcrn of paroleum-forming org. vater. Th:;i Ident
'
Io~
Ojas mot bven accipted by later p1trulwin I 1,ts
'4and litholquts. G.'s own UL-Witm. Investill-.i
)PS, 01%
~Wibtd lu V16 pa X. Of the DeVOUIATI an I Csrh(W-CMUS (tell
'
-
,
!
J A
,
w
.
A
pwitti W 01A. Vr,% -Vojr., provIn".4, Lim tIOL ci-Ohl

rttain thdr migni[c;ium Lis (mi: of t1ij. f,,,.etj III tilt:
'latlon of pet-okuln-fortaing mitcrUl tindcr
'
'
,
fy, - , 11-ins lw--
.dacing canditiou. The charz4~1(,-L-tlcs a F 0-

' 'bOndance of pyrite and an nbsenct of gro,ind. jaums.'
'
I

"t ground fauna may bu cAtatul hl, :,O~.
to absence of -V flwtum
T
CV&Ssuf If's ar lix h,ell ShnIvil tly \. ~E.
Y.

I - 11 ~ , , II
,r~uljayuva, LA. -- "Geo(--:e in is" r, or 2kvrige I I ms it; )t' t w Di vr).:i an it I I ::;~,
orals Alom, tne ;ol,;a.11 Dr 5ci, Pefrolem Inst., Acact ""ci l-,,i, 2o Jan ~4.
(Vi!.C;,~si--rt'llYAYA- -~OSKVA, 1~) Jan 5.4)
Source: SUM 168, 22 JulY 1954

1~ : I I M ! i I iii I i I I ill A!" I tZ11 M if W V I f4v'.0I
- - - - - - - - - - - - - - - -

Yff-
-Y F)
Ar,

blulitum 17 U ta r1jud),
AM.
P46
,
patason r-i cmi aLd ptinilcuir. befiavi"r in znalficifal oxid!-
tiov.-Cc:duri bin
sys-,Cmii leads tv fte Lcmilu-jim ctul there ure
.
EW-mitly ox3cliv-41 a0ive ccru macim; L- ELI] hilijia Chassi
which um miticfd iii the tkvi. ruirgt :f 1111
~.1 Il'),titti-01 (EL) ~A lip to A-2,N) 111,1 Th,: (1111:1 'I.Wwr
efogn um%t Uil-q. whik!) i~m ol:hk4id in 111m I'll-Igit.
ThIii oil lichavlog fit4ft-tted thd prav~lci,,im.1 fedtiozil cocuph.
in Imtroltuat, i~fth ~Ltow= Ert dun that W weeia W whicl; the
oil inter--c(s. Ptr(ozdy juccc siipro~cjltmi and jt~e
.Kairu
,
field oil arld tho Lawa Volp 110-009, Villkh arti wx id;"

fir,
61
friffly.1110i 9tire J'w,
Ov.

GULYAYXVA, L. A.
"Microelements" of petroleum and bitumen of the Permian and
Carboniferous of the Ural-Volga Valley region. Trudy Iust.
nefti 3:188-206 154. (KIRA 8:6)
(Volga Valley--Petroleum--Analysis) Wral Mountain region--
Petroleum--Analysis)