SCIENTIFIC ABSTRACT LYSOV, A.G.  LYSOV, M.I.
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SCIENTIFIC ABSTRACT
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LYSOVP A.G.
New cuttingoff tool and its holder. Mashinostroitell
no.9:25 S 164. (FURA 17.10)
LYSOV , A.G.
Boring attachment. Mashinostroitell no.4iN AD 165. ft MJRA 18: 5)
LYSOV, A. I.
Diagnosis and treatment of severe injuries of the urethra and
abdominal cavity during bouginage and introduction of the_oysto
scope. Urologiia 25 no.2t24,28 ~hAp 160. (MIRA 13:12)
(URETHRA,WOUNDS AND I&TURIES) (BLADDEREXPLORATION)
(ABDO=WOUNDS AND INXURIES)
:LYSOV, A.I.
Uue of the Horner method in solvirig alp,,ebraic coagru~;reb cT higher
order. Uch. zap. Orsk. gos. y/ed. Inst. no.5:7373 I ~') ", 0(mIRA 18:3)
ACC.NRt AP70021.77 SOMCECODETM[OI46t66/009/006/0059/0063,
AUTHOR: Roytr.,an, M. S.; Tsimbalist, E. I.; Lysov, A. 1.
ORG! Tomsk Polytechnic Institute (Tomskiy politekhniche8kiy institut)
TITLE: Photoelectric converter as a control element for electrical circuits
SOURCE: IVUZ. Priborostroyeniye, v. 9, no. 6, 1966, 5963
TOPIC TAGS: photoelectric method, electric device 'C~Y&0~ Q:%'VC'j
ABSTRACT: The characteristics of a photoelectric converter designed for use in
control and measuring circuits are described. The fourterminal con
verter consists of an SF22 photoresistor (output terminal pair) en
closed in a capsule together with an NSMtype lowvoltage incandescent
lamp which operates at either 6v, 20 mamp, or 9v, 60 mamp (input terminal
pair). The converter is characterized by a slight temperature dependence$',
absence of galvanic coupling between the controlling and the controlled !
loop, a relatively low time constant, and a high linearity. Some char
acteristics of the converter are: input impedance, 200400 and 80 
170 ohm for 6.3v, 20mamp and 9v, 60mamp NSM lamps; maximum transfer
factor, about 10; temperature instability at an ambient temperature of
NOOK is ~S 0.15%, average photoemf, 2 Vv (for photoresistors illuminated.),
with 9v. _ 60mamp . lamps); maximum inj?ut power, 2040 mw. Orig. art. has:.
2 figures and 2 formulas. SUB CODE: 09/ SUBM DATE: lOMar66/ 010 REP 005
Cc3rd i /I Mr. AA1_9_nAq_9 hTn TMrQC r,1 I I
MOP A. Y.
Lysov, A. M. "For n1churinist methods in the scientific research of karakul
raising".. Karakulevodstvo i zverovodstvo, 1949., No, 1,, p. 1012.
SO: U3042, 11 Merch 53, (Letopis'nykh Statey, No. 10, 1949).
j~ysov, ,. 1:.
24137 Ll,',90V..A. l,. Rabota ple;:2.hoza "Rla~nrLnaall po LduchohmIJ~u otada ovots
(Turlaa. SSIO Karal,ul(,,vo,,IL,,ro 1 wrovolk,"'vo, I)lp, "(D. "'., S.
. Jj,Ioj,Iot 7T . 12, 1911C).
So u i0 ,
USSR/HLmian and ;miual Physiolo~,fy. rnIc Nervous Systou T12
,,'~bs Jour : Ref 71iur  Biol., No 14, 1958, iio 65759
.',Uthor : Lysov _14., .ntreyev M.N.) Panin B.V.
Inst 1 O~u  ulu~~ S Iz. Al  K~j .9.'ALY
Title : .*. Study of Conditioned 4otorFood Roflexas in Sheep
Ori3 Pub : Ftziol. zh. SSSR, 1956, 42, No 11, 9971001
Abstract : By usin[~ a photoelectric recorder, a description f%nd plan of
which are included in the Imper, rcflex latent perioci,
number o' turns to the feodor nnd the tiLle the aniLrl s,
I pent
nt the feeder are all nvE froz.: a kyno.,rnp strip. Ihe ar
ron.al"Ient of the soundproof chfz~bcv and control ~~ncl f~ra
c.13o described. Slavutshmya
Card 1/1
LYSOV, AA, kLbiologichesIdkh nauk
I
Institute controls breeding stations. Zhivotnovodstvo
2j no.7:5862 J1 161. (MMA 16:2)
1. Direktor Nauchnoisaledovatellskogo instituta
kara*1evodstva. (Uzbekistan,Karakul sheep)
BURGVITS,, A.G.; ZA'VIYATOV,, G.A.; JZNZ A.N. (Che3yabinsk)
"On the development of the lWdrodynamical theory of the highapeed oilfirm
bearings"
report pi6sented at the 2nd AllUnion Congress on Theoretical and App3ied
Mechanics, Moscow, 29January  5 February 1964
LYSOV, A. P.
EPM1 electric rockloading machine Moskva, Ugletekhizdat, 1952. 215 P. (5417779)
TN345,.L9
1. Mining machinery.
I I
/It, c v , P
.I ) 6 ) /t
LATYSH, A, I P.

Idned guide supports for mine hoists. U9011 32 no.10:47 0 '57.
(MIRA 10:11)
1. Toretskiy mashinoetroitellnyy zavod.
(Mine hoisting)
LYSOV,A.S., inzhener; SHEYDIN,S.A., inzhener
Electric lighting of metalwork shops. Svetotekhnika 1 no.1:23
F '55 (KWU 8:9)
1. Magnitogorakiy metallurgicheakiy kombinat
(Metallurgical Plante) (Electric lighting)
LYSOV,,,A.S,., inzh.; MURINETS, S.V., inzh.; YERSHOV, A.G., inzh.
Comparing various automatic control systems of conveyer cha.ging of the
sinter into blast furnaces. Stall 23 no.12:10731077 D 163.
(MIRA 1712)
1. Magnitogorskly metallurgichaskiy kombinat.
S/l2o/62/0O0/O04/oo6/o47
E039/E420
AUTHORS: Malyshev, I.F., Popkovich, A.V., Roshall, G.Ya.,
Zheleznikov, F.G., Lyzov,A.V.,Tsepakin, S.G.,'
Solnyshkov, A.I., goytsov, A.S., Astakhov, Ye.Ya.,
P1ironov, B.V., Lapitskiy, Yu.Ya., Batalin, V.A.,
KhoroshlSov, V.S.
TITLE: The electrostatic.accelerator Injector of the proton
synchrotron
PERIODICAL: Pribory i tekhnika eksperimenta, no.4, 1962, 3745
TEXT: An electrostatic accelerator used as an injector in the
7.0 Gev proton synchrotron developed in 1956 byNTIIEFA 'is
described. The pressure chamber is 2200'miii in diameter and
7400 mm high and is intended for working pressures of up to
16 atm. Insulating gas is N2:CO2 mixture with a ratio of partial
pressure of 3:1 The main column is of conventional segmented
construction using polymethylmctacrylate. Values of the
dependence of the voltage produced on the gas pressure shows that
4 IIV is obtained at 6.5 atm and 5.7 MV at 16 atm and a relative
humidity of < 10%. The charge transporter belt is a six layer
Card 1/2
S/120/62/000/004/006/047
The electrostatic accelerator ... E039/E420
fabric driven by a 3000 rpm 10 KW motor at 20 m/sec. The
accelerating tube and its electrode system is described in detail:
it is 300 min inner diame er with 44 segments and the residual
pressure is 2 to 5 x 10~ min Hg. A Penning type discharge is
used in tho ion source which provides 03 mA total ion current on
continuous operation or 20 mA pulsed; the proton component being
10 to 12'/'0 and 65% respectively. The energy of the injected
particles is stabilized to about 0.1%. Results of operation in
196061 show that beam currents of 4 to 5 mA are obtained at 4 MV.
There are 10 figures and 1 table.
ASSOCIATIONS: Nauchnoissledovatellskiy institut elektrofizicheskoy
apparatury GKAE (Scientific Research Institute for
Electrophysical Apparatus GKAE)
Institut teoretiche5kOy i eksperimentallnoy fiziki
GKAE (Institute of Theoretical and Experimental
Physics GKAE)
SUBMITTED: April 6, 1962
Card 2/2
MALTSHEVJ, I.F.; POPKOVICH, A.V.; ROSHALI, G.Ya.; ZHELEZNIKOV, F.G.;
JXSOV,,.A.V.; TSEPAKIN, S.G.; SOIJYSHKOV, A.I., BOYTSOV, A.S.;
ASTAKHOV, Ye.Ta.; MIRONOV, B.V.; LAPITSKIY, Yu.Ta.;
GATALIN, V.A.; KHOROSHKOV, V.S.
Electrostatic acceleratorinjector in a proton synchrotron.
Prib. i tekh. eksp. 7 no.4:3745 JIAg 162. (MIRA 16:4)
1. Nauchnoisaledovatellskiy institut elaktrofizicheskoy
apparatury Gosudarstvennogo komiteta po ispollzovaniyu
atminoy energii SSSR i Institut teoreticheskoy I eksperimentalf
noy fiziki Gosudarstvennogo komiteta po ispolIzovaniyu atomnoy
energii SSSR.
(Particle accelerators) (Synchrotron)
LYSOV B.  ZHIMSKIY, V.
How we organize audits. Fin. SSSR 22 no.9t7l74 S 161.
(VIRA 14:9)
1. Glavnyy kontrolerrevizor Kontrollnorevizionnogo upravleniya
Hinisterstva finansov RSFSR po Saratovskoy oblasti (for Lysov).
2. Starshiy kontrolerrevizor Kontrollnorevizionno&o upravleniya
Ministerstya finansov RSFSR po Saratovdkoy oblasti (for Zhimskiy).
(Saratov ProvinceAuditing)
LYSOVI B.
Seven annaul, quotas before the end of the sevenyear plan. Avt.transp.
4 no.8:45 Ag 162. (MIRA 16:4)
(Transportation, AutomotiveProduction standards)
,r 71~
AUTHORS: Sokolov, A. A,, Lysov, B. A,
TITLE: Compton Scattering of Longitudinally Polprized Photons on Elec
trons vith Oriented Spin (Konptonovskove rasseyardye prodollno
polyarlzovannnyhh fotonov ;,a elektroriakh s oriyentiravannym spinor.)
PERIODICAL: Zhuraal eksperimental:noy i teoreticheskoy fizilci. 1953,
Val. 34, Nr 5, PP 13511354 (USSR)
ABSTRACT: In cormection uith the discGvery of 'the nonconsei~ration of parity
the further development of quantuaelectrodynamica of electron5
and photons with a langitudLnal polarization is becoming a prob
lem of topical interest. To consider the lorign.tudinal polariza
tion of the electrons in the cor4)utation of the matrix elements,
not the formula by Casimir (Kazimir) but the fox.=.Cla (21,12)
from the book by A,,A. Sokolov and D,D. Ivaaenko ( 'Ref 3) has to
be ueed, s denoting tte eigenvalue of the opera~or
)/i,  2. Tus operator describes the drrable projeation
of the elez;tron spin uk3n its direction of motion. This formaiLa
can be used in cases where the electron initialiy :~s at rest.
For this case the formala is irritten down explicitly. Then an
expression for the corrxesponding matri;< elemeut is given. From
Card 1/3 these expresslons a gencralization of 'the formila by ~aeirtNishlna
SOV/563451  59/61
Compton Scattering of LrngJtudin~_'y Polarized Photonz on Elecrrcas
with Oriented Spin
(K2eynNishina) can be derived. Sts.rting vilth these expressions the f Drmula
by KleinNishin mi be generalized to that. case where the initial spin of
the electron hEs the given crienation s ard where the fina:i, spIn states
are summed up. in the scettering of a pola ni zed x1idivition the orienta
tion of the spin has no J.nfluen~.e upjvi 'Itle utcgm'L 1,mf of sca".tering.
A formO.a for the comput9tion of the xAte of the ciTculemr polarization of
the scattered radlaticoj. is given. In the nonrelatk~ristio case there is
)s2 Th *.he ultrarelei
obtained Pnonreleti,distiv =, 2 oll + cr
vistic case the scattered radiatl'on, irill, in the case of vide sapattering
angles, partly be ciiculaxly pclarized., As jrverse problem to tjftr prob
lem investigated, aborve the twophoton F.,ixib:Uation of 11cagitudinsaly
polarized positrons on electrons at rest vith a given epin direction is
discussed. An expression. for the corresponding crosssectioa 's given.
In the exRnlxed case a polarization and ast azimithal. asymmetry exist.
This makes possible to apply the twophoton. aariIbIletiju of the positrons
at, oriented electrons for the experimental determiaption of the degree
Card 2/3
SOV/5634559/6a.
Compton Scattering of Longitudinally Polarized Photons on Electrons
with Oriented Spin
of longitudlnal polarization of positrons. There are 6 references, 4
of which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet (Moscow State
University)
SUB14ITTED: February 27, 1958
1. PhotonsScattering 2. ElectronsProperties 3. Nuclear
spins 4, Mathematicslpplications
Card 3/3
24(5)
AUTHOR: Lysov, B. A. SOV/5636149/62
TITLEs The Energy Losses of a Particle Which Are Connected With
the Excitation of Longitudinal 'daves (Energeticheskiye
poteri chastitsy, svyazannyye s vozbuzhdeniyem prodollnykh
voin)
PERIODICALs Zhurnal eksperimental 'noy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 1, PP 321322 (USSR)
ABSTRACT: It is necessary to develop a theory of the Cherenkov effect
which can be applied to the emission of longitudinal
electromagnetic waves by an electron. In this case, the usual
Lagrangian L  (e ~~  T2) / 8,g carnot be ap~;lied since the
energy density of the field (6 + 7~)/876 would be equal to
zero for a longitudinal fielcl . In order to avoid these
difficulties, the author uses the Lagrargian of W. Fbk and
B. Podoltskiy, generalizing it for the case of an isotropic
12 _42 71 2 )2
medium: L = t(n E) H  (div A I n A denotes
c
ard 1/3 the vector potential, r the scalar potential, n  the
refraction index (n in the present raper is an operator).
If there are no free charges 0 the equations
The Energy LosseS Faxtirle IyThich Aare Connected SO'j 162
With the Excitation of Longitudinal Waves
2,,2 W) ____)
A (n Q /c k 0 and
1)2 (a
T44 = t(div A ruqc Dt) /81~can be deduced from the
abovementioned Lagrangian. The solution nf these 2 equations
is written down explicitly, and for the energy of the
longitudinal field the expression
H = 5.(c ht/n) (t' 2) is f ound. tzand ck.;~ln denote the
K
momentum and the energy of the longitu!l~nal photon. The
author puts a).= 4 Y/X in order explicitly
9 XOF 9 NO 0
to satisfy the long�tudinal condition. The operators
g and g! satisfy the Bose (Boze) commutation relations.
The phenomenologic quantum electrodynamics developed in
paper is formally equal to the theory of A. Sokolov and
D. Ivanenko, the difference4bein only constituted by the
meanings of the operators a and 11. In the case of a
longitudinal field there is no specific quantum correction
that is proportional to,42 and which can be connected with the
Card 2/3 electron spin in IVhe case of a transverse field. There is a
The Energy Losses of a Particle Which Are ConneQted zOV/,636149/62
With the Excitation of Longitudinal Wa~es
very essential difference between transverse and longitudinal
fields. In classical approximation, there is no threshold
irradiation in the case of Cherenkov irradiation of transverse
waves. For longitudinal waves, however, radiation remains
finite at the threshold and in classical approximation. The
author thanks A. A. Sokolov for his great interest in this
paper and for his stimulating advice, and Yu. M. Loskutov
for a useful discussion. There are 9 Soviet references.
ASSOCIATION: Moskovskiy gosudarstvennXy universitet (Moscow State University)
SUBMITTED: Sdptember 3, 1958
Card 3/3
21M
AUTHOR: Lysov, B. A. SOV/5637245/56
TITLE: Polarization Effects During the Direct Transition of P +
Into an ElectronPositron Pair
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 37, Nr 2(8), PP 571572 (USSR)
ABSTRACT: Ya. B. Zelldovich has recently directed attention to the
possibility of converting a p +ppair into an electronposi
tron pair through a virtual quantum. This problem proves to
be of interest also without a limitation to the nonrelativis
tic approximation, as Ya. B. Zelldovich has done. The matrix
element describing this process can be determined directly
from the matrix element of the exchange portion of the Bhabba
interaction, if the initial electron and positron functions
are replaced by the wave functions of the mesons. It is easy
then to find an expression for the probability of the trans
formation from V+ p into e+e. In the centerofmass system
dw  (e4dQ/8c' t'L3K')S+s is obtained if the rest mass of the
A
Card 1/4 electron and positron is ignored as compared to their energy,
Polarization Effects During the Direct Transition of sov/5637245/56
Into an ElectronPositron Pair
the spin portion of the matrix element being given by
S . 9+ b b 1+ a b . CE denotes the fourvector composed
11 A e V e V
of the Dirac matrices and b the spinor amplitudes of the
respective particles. In order to find the probability of
the transformation fr6m g+p into e+e the corresponding
symmetrical combination of the spinor amplitudes is directly
substituted into the above formula dw  (e4dQ/bc_WL3K')S'S
11
in the third orthostate, when the projection of the total
spin of the mesons upon their direction of motion is zero. If
the direction of motion coincides with the zaxia,
b(s)  ? 3ab(s) holds. For the probability of the trans
ition of.the third orthostate
dw s .(e4dQ/4c VOK 2) (1  k2/K + k 2 /K2) (I _ 0082 G) is
0 P 11 A OP A +
found. The probability of the transformation from 4 into
Card 2/4 an e+epair in the orthostate is markedly dependent upon
Polarization Effects During the Direct Transition of SOV/5637245/56
Into an ElectronPositron Pair
the projection of the total spin of the mesons upon their
direction of motion. If this projection is +1, the electrons
will mostly be emitted in the direction of &otion of the meson.
If, however, the total projection of the meson spin upon their
direction of motion la zerof the electrons will mostly be
emitted in a direction perpendicular to the direction of motion
of the electrons. In the nonrelativistic approximation
(kV>O, Cos2 Q__**1/3) the probability of a p+p_  e+e trans
ition is equal for all three orthostates, amounting to
WS . 4xe4/3cT)2L3k , which is in agreement with the valuefamd
Oil +  +
by Ya. B. Zelldovich. The transition probability for A p e e
in the para8tate is zero not only in nonrelativistic
approximation, but also in the general case. The author
expresses his gratitude to Professor A. A. Sokolov for
valuable help and suggestions. There are 2 Soviet references.
Card 3/4
Polarization Effects During the Direct Transition of SOV/5637245/56
p+p Into an Electronpositron Pair
ASSOCIATION: Uoskovskiy gosudaretvennyy universitet (Moscow state
University)
SUBMITTED: May 13p 1959
Card 4/4
LIM 0 S/139/61/ooo/ool/oWoA
2b E032/E514
AUTHOR: LYsov. B. A.
TITLE: Polarization Phenomena in the Photoelectric Effect
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Fizika,
1961, No.1, PP7176
TEXTt The discovery of the nonconservation of parity in weak
s of
interactions has led to very intensive study of various kind
polarization phenomena. In particular, a number of papers have
rect;ntly appeared on the polarization properties of photoelectrons
and their dependence on the polarization of the initial photons.
In their~classical papers Sauter (Ref.1) and Bommerfel&* (Ref.2)
discussed the case of linear polarization of the original photons
and the polarization of the emitted,photoelectrons was not inveqtl_r~
gated. The first attempt to take into account the circular
polarization of the incident photons is due to McVoy (Ref3).
However, this author used a rather rough approximation and complete
ly neglected the Coulomb distortion of the electron wave function in
the final state. This approximation is said to be untenable when
the energy of the incident photons is in the relativistic region.
This is the reason why the results obtained by McVoy are in
Card 1/4
89698
S/139/61/ooo./ool/006/0.18
E032/E514
Polarization Phenomena in .....
with the results obtained by Sauter and Sommerfeld.:.
contradiction
An agreement can only be obtained in the nonrelativistic case.
McVoy's results reported in Ref3 have recently been modified by
Fano et al. (Ref.4). However, the present author states that the
final formula for the degree of longitudinal polarization of the
photoelectronswhich was obtained in Ref.4 contains an error. In
the present paper th4 author investigates the longitudinal
polarization of photoelectrons ejected from the Kshell by
circularly polarized quanta. The Born method is employed in the
second approximation. Polarization effects are taken into account
using the theory of Dirac particles with oriented spins, as
developed by Sokolov (Refs5 and 6). It is shown that the degree
of longitudinal polarization of the photoelectrons is given by
b. 2) (1 ~Ii Cos
Apt (EI) 2
W7 COS 9)
2
Card
9/61/000/001/006/ol8
S/13
Polarization Phenomena in ..... E032/E514
where +1, dependin' on whether the incident photon has a right
ihanded or a lefthanded circular polarization, y is the ratio of
~the energy of the photon to the rest energy of the electron and
V/c. The differential crosssection for the photoelectric
,effect, including terms describing polarization of both the
rays and of the ejected photoelectrons,is given by
,.incident
do an Z3 sin, 0 X
(2
2
/12 COS@
d2
22) (1 COS 8)
+S1 +  (T. +(T
.1+2) 2
w6re
V
In the nonrelativistic case when Y