SCIENTIFIC ABSTRACT ALEKSANDROV, Y.B. - ALEKSANDROV, Y. A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000100830014-4
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 5, 2000
• Sequence Number: 14
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

ALEKSANDROV, Ye.B.; BONCH-BRUYEVICH, A.M.; KHODOVOY, V.A.
Spin exchange. Izv. AN SSSR. Ser. fiz. 27 no.8:1070-1077 Ag
163. (MIRA 16:10)

ALEKSANDROVY Ye.B.; KONSTM TINOV, O.V.; FERELI, V.I.; KHODOVOY, V.A.
Modulation of scattered light by parametric resonance. Zhur.
eksp. i teor. fiz. 45 no.3'503-510 S 16100 (MW 16:10)
1. Opticheskiy institut imeni S.I. Vavilova.
(TAght-Scattering) (Cadmium)

ALEKSANDROV Ye B - KONSTANTPILN, O.V.; PEJULI, V.I.; KHODOVOY, V.A.
--1--l- .11'. a P
Modulation of scattered light by parametric resonance. Zhur.
eksp. i teor. fiz. 45 no.3003-510 S 163. (YMIA 16:10)
1. Opticheskiy institut imeni ';;.I, Vavilova.
(Light-Scattering) (Cadmium)

ACCESSION NR: AP4020921 S/0051/64/016/002/0193/0200
i
AMOR: Aleksandrov.Ye.D..; Konstantinov,O.V.; Perell, V.I.
TITLE: Conversion of the frequency of modulation of light by parametric and double.
resonance
SOURCE: Optika I spektroakopiya, v.16, no.2, 1964, 193-200
TOPIC TAGS: modulation frequency conversion, light modulation conversion, radiation;
modulation,' parametric resonance, double resonanc'e, Zeeman effect, magnetic field
splitting, luminescence modulation, harmonic combination, dual modulation, light
scattering, cadmium
ABSTRACT: In resonance scattering of modulated light by atoms whose excited state
is a Zeeman triplet, the depth of modulation ofthe luminescence is resonance-de-
pendent on the splitting magnetic field; the degree of modulation exhibits a maxi-
mum when the modulation frequency agrees with the frequency of the sigma component
of the line. On the other hand, In scattering of light of constant intensity (non-U
modulated), one can obtain ;Dodulated luminescence by applyingp in addition to the
constant splitting magnetic field, an alternating field perpendicular or parallel
Card

ACC.RN: AP4020921
to the constant one. In the former case there obtains "double resonance"; in the
latter case, "parametric resonance". Modulation frequency conversion incident to
parametric and double resonance is discussed and analyzed theoretically; the dis-
cussion is based on earlier publications of the authors. It is shown that incident:
to application of an alternating field, in addition to the constant one, there
should appear In. the luminescence intensity harmonics not only with the frequencies.
of the incident light modulation and field modulation, but also with combination
frequencies. The amplitude of the combination harmonics is resonance-dependent on
the strength of the constant field. The experimental part of the study was carried:
out on a set-up consisting of an oscillator f0eding a coil via an rf amplifier, a
photomultiplier, a tuned amplifier and a detector assembly. The set-up was similar
to that described earlier by the authors ME iTF,45,503,1963). Radiation associated
with the 53Pl__51S
0 transition in cadmium vapor (contained in a tube surrounded by
the above-mentioned coil) was observed. The1purpose of the experiments was not to
obtain detailed data, but only to demonstrat,,the feasibility of modulation frequen-
cy conversion. A modulation amplitude verstW!field strength curve is reproduced. - -- .:
The experimental results are consistent with 169 predictions o:, theory. "In conclu-~
sion, the authors take pleasure. in expressing; their gratitude to A.M.Bonch-Bruyp-
vich for his interest in the work and valuabl'o advice.1,fOrig.art.has: 51 formulas
Card 2/3

ACCESSION NR: AP4020948
S/0051A;4/016/003/0377/0381
AUTHOR: Aleksandrov, Ye.B.
TITLE: Coherent excitation of atomic states by electron impact
.SOURCE: Optika i spektroskopiya, v.16, no.3, 1964, 377-381
TOPIC TAGS: electron impact excitation, transition probability, coherent excitatio4i
,modulated excitation, pumping, Zeeman splittink, line shape, cadium
.ABSTRACT: The present work was a continuation of earlier research by the author
.(Opt.i spektro.14,436,1963) and O.V.)(onstantinov and V.I.Perell (ZhETF 45, 279,1963).
~concerning resonance scattering of modtilated light by cadmium vapor. It was estab-
~1.ished that the depth of modulation of the scattered light has a sharp maximum when;
the modulation frequency of the excitation coincides with the frequency of the troa- :
~sition between the components of the Zeeman triplet of the 53p, state of the atom
.in a magnetic field. The effect is attributed to interference between the terms cha-! *
racterized by different magnetic quantum numbers, specifically, sublevels with m = :
= �1. In the present work there was investigated coherent excitation by electronim-~
pact. The experiments were carried out with cadmium vapor, the observed line being
Card 1/3

ACCEssioN wn. -Ap4w48
the 3261 X luminescence line, associated with the 53p,__51S
0 transition. The modu-
llat,ad electron beam (from a gun) was directed normal to the weak (0-0.5 gauss) mag-
!netic field, which was slowly swept through the expected resonance region. The ra
idiation was detected at 900 to the beam by means of a photomuliplier. The modula-
Ition frequencies were 1 and 2;62 Me. The result of processing one series of measureo~,
!Ments is shown in the Figure (Enclosure 01): the points are experimental; the solid!
5
line Is the theoretical contour calculated for g w 1.5 and 7 m 5.6 x 10 see-1.
i(The second experimental peak is due to the presence of odd Cd isotopes in the vap-
i
!or.) The advantages of the modulated beam (beats) technique over other methods for
14etermining the probabilities for transitions asoociated with non-resonance lines
!are polfitW out. "I take this opportunity to express my deep gratitude to V.A.Bud-
i
inikova for assistance in realizing the electron excitation, V.S.Shevere for consul-:
station and help with the same problem, and to A.M.Bonch-Bruyevich for his attentions
and interest in the work." Orig.art.has-. 3 formulas and 3 figures.
4SSOCIATICK: none
i
iSUBMITTED: 30UaY63 DATE ACQ: OZApr64 ENCL: 01
SUB CWH- PH NR REP SOV: 004 OMERs 002
Card 2/3

ACCESSION N'R: AP4020971
S/U051/64/016/003/0533/0535
AUTHOR: Aleksandrov, Yo.B.; Rozlov, V.P
TITIZ: Contribution to the theory of modulation of luminescence appearing incident
to interference of coherently excited nondegenorate states
SOURCE. Optika i spektroskopiya, v.16, nO.3, 1964, 533-535
TOPIC TAGS: bent luminescence, modulated luminescence, level interference, coher-
ent excitation, nondegenerate system
ABSTRACT: In a series of recent papers by one of the authors (Yo.B.Aleksandrov),
alone and in collatioration with othor investigators (Opt.i spol-tr.14,436,1963; Zh-
ETr-,45,503,1953; Opt.i spektr.16,377,1964; lbid.16,193,1964) there were described
experiments in which there was observed beating of the radiation from a system of
atoms characterized by close sublevels in the excited state. The beats arise as a
result of interference of states. The theory of the phenomenon as regards opticil
excitation was developed by O.V.Konstantinov and V.I.Perel' (Opt.i spelttr.16,193,
1064; ZhETF 45,279,1963) using the density matrix formallfsm. In the present paper
there is proposed a simpler variant of the theory, which is applicable for diffe-
Card 1/2

ACCESSION NR: AP4020971
rent types and ranges of e%citation and, in the opinion of the authors, is more
physically meaningful. The approach is based on the assumptions that lifetimes of
the atoms in the-energetically close excited states are equal, that there is a cer-
ta-in probability for excitation of the atoms to the states 1 and 2 with a definite
phase and amplitude relation (coherent excitation) and that the effective excita-
tion time is much shorter than the lifetime in the excited states. Thus, there are
derived formulas characterizing the luminescence beats under conditions of modula-
tion of the excitation or of the separation between excited sublevels. Beats should
also occur in the case of modulation in phase, rapid rotation of the plane of po-
larization, etc. "We are indebted to O.V.Konstantinov and V.I.Perel' for discus-
sion of the work and critical remarks.'I Orig.art.has: 12 formulas.
ASSOCIATION: none
SUB11MED: 30hlay63 DATE ACQ: 02Apr64 ENCL: 00
SUB CODR: PH NR MF SOV: 005 OVER: 002
Card 2/2

ALEKSAND,F%)V. Ye.B.; BONCH-BRUYEVICHl A.K.; KOZLOV, V.P.
Observation of the signal shape in the presence of a high
noise level by means of repeated oscillographing. Prib. i
tekh.eksp. 10 no.5tUO-113 S-0 165. (MDU 19. 1)
1. Gosudarstvennyy opticheskiy institut, Leningrad. Submitted
Aug.8, 1964.

~L 3665-66 Ewil) IJP(c)
011108:
ACCESSION N11t AP5 UR/0051/�5V018 0545/0551~
00~ Ego/
599.3.84.2 6.48
AUTHOR: Aleksandrov, Te. 6; WOMOV) Ve Ve
q V, (;5"
TITIXs Use*of the method of beats to measure the Stark spl-itting of the cacbsiini
.53p, level
SOURCE: 0
ptika i spektrookopiyap Y. 18p no. 4, 1965P 545-551
TOPIC TAGSt Stark splitting., cadmiva, resonance, luminescence, beat method, 31
ght
modulation, splitting constant
ABSTRACT'i The Stark aplitting of the, 53P, state of cadmiun vas investi at,d by
-inescen UK
observing the degree of modulation of resonance I 4W.0~ed wgen cadmi
vapor is excited with modulated light (the method of beat This Splitting Vas
never investigated before by radio-optical or polarization methods, and in too
&=11 to be.observed by direct spectroscopic methods. The measurements vere zaae
by two methods, one with siamiltaneous application of a constant electric and Yarl-
able magnetic fieldp and the other vith an electric field aldne. Me@ the cUssi-
eal interpietation cannot be applied to the latter casep a,geueral ans4sis of -the,i'
Card 1 2

L 9912-56 .___g~Vn_T1V~"Tr(mYEPF(n)-2 -_.'P(t)/~j-;P(b) 1JP (c) M/W-4/M
AP502 872
1WO05 /Oi~/o6~/64
rxer~__ L) I
AUTHOR: Aleks andr45__)1r_.,,.B.,
ORG., None
TITLE: Beata in luminescence due to phase modulation of the excited state
SOURCE: Optika, i spektroskopiya,, v. 19, no- 3, 1965p 452-455
TOPIC TAGS: luminescence, excited state, light polarization, transitlon radiation,
phase modulation, Faraday effect, q~admium.,,.
ABSTRACT: The author describes the realization of a new methlod of synchronizing in-
tensity beats,in the spontaneous radiation of atoms. The metbod was originally pro-
posed in an earlir.,r paper by the author (with V. P. Kozlov, Opt. i spektr. v. 16, 533
with correction in v. 16, 1068.9 1964) and consists in making -the elementary process
that rroduces the beats govern the initial phase of the beat. The experiment is base
on the cadmium intercombination transition 53P,--5'So in a magnetic field. Cadmium
vapor at 220C is escited by 3261 A resonance radiation from a cadmium lampp directed
along the magnetic field and linearly polarized (Fig. 1). The luminescence is ob-
.served at right angles to the field by means of a photomultiplier. The modulation ofl
the initial phase was produced by oscillating the plane of polariza -on at high fre-
quency with the aid of the Faraday effect in the same eadm ear the absorp-r
ium
tion line. Details of the oscillation of the plane of polarization are described in
a companion jxLper in the same source (Opt. i spektr. v. 19, 4-55, 1965, Ace. AP5022873Y-
The line shapes of the luminescence beats before and after synchronous detection, as
UDC

L 9912-66
ACC NR, AP5022872
ism G
Fig. 1. Block die-gram of experi- zi 4 Z
mental setup. 1 - Cadmium lamp,
2 - lens, 3 - polarizer, 4 - Cad- 7
mium vapor cell, 5 - resonance 6 rememw
vessel, 6 - 975 kcs oscillatorp 12
7 - 500 kcs heterodyne., 8 - fre- e 9 10
quency doubler-, 9 - 25 kcs IF am- Yftq CUMXPM11W
plifier, 10 - synchronous detec- YOSOUWMb 25 XeR &MMOP
WWWO
tor, 11 - mixer, 12 - photomulti-
plier. 9-
well as the line widths (5 X 105 see-3-) vere found to agree vith the published di ita.
Author thanks A. M. Bonch-Bruyevich for advice, support, and interest in the work,
and V. P. Kozlov for critical co ents. Orig. art. has: 2 figures a~nd 2 formlas.
suB CODE: 8um DATE: 29jan65/ ORIG REF: 010/ OTH REF: 004
C,,d 2

ALEKSANDROV, Ye.B.
Astrophysical proof of the second postulate of the special tre-ory
of relativity. Astron. zhur. 42 no.3%676-678 My-Je 165. ~YjRA 1&5)

9911-66-, MWTD, (e)
ACC NRi AP50228 3 SWRCE CODE: IJFVOOQ6~1_6
I ./ i
AUTHOR: Aleksandrov, Ye. B.
ORG: None
.TITLE: Modulation and filtration of resonance radiation with the We of the Faraday
effect
SOURCE: Optika i spektroskopiya,,v. 19, no. 3s 1965, 455-457
TOPIC TAGS: cadmium, Faraday effect) resonance line, light polarization, Zeeman ef-
fect, absoiTition band
ABSTRACT- Ibis is a companion to the preceding paper in the same source (Opt. i vv,sj.
spektr. v. 19, 452, 1965, Ace. AP5022872) and describes the use of the Faraday effect'
in cadmium vapor to modulate and filter out the unshifted resonance lines. The pur-
pose.of the experiment was to develop a technique which can be useful in certain ex-
periments with resonance excitation. The experiment was performed with the cadmium
3261 A r9sonance line. Lihearly polarized light from the cadmium lamp passed through
a_qMartzVcel1 placed together with an electric oven inside a coreless coil to provide
a magnetic field up to 2000 gauss directed along the light lbeam. The magnetle,field
split the excited state of cadmium 53P, into a simple Zeeman triplet whose outer com-
ponents pr-pduced the magnetic rotation and absorption. MaxLmum differential rotationf-
of the plane of polarization could be obtained by varying the splitting and the vapors
density under the given experimental conditions, and by eboi5sing the optimum tempera-~
Card 1/2 UM t 538.6

L 9911-66
ACC NR, AP5022873
ture and a suitable value or, the field it is possible to obtain a significant modulm-
tion of the transmitted light. by applying a varying magnetic field to the cell. An
absorption test has shown thIat practically.all the light produced in the system lies
in the absorption band of the cadmium vaporj, thus testifying to the effectiveness of
the filtration. Orig. art. has: 2 figures.
SUB CODE: 2o/ Sum DATic: 29jan65/ ORIG PXF: 002/ OTH REF: '001
212
!wpm

-L 00541-66 -EWT(T,.)/'T IJP(C)
ACCESSION NRz' AP5019221 UR/0056/65/049/001/0097/0106:
AUTHORS: Aleksandrov# Ye._,B.,- Konstantinov, 0. V.; Perell, V. I
TITLE: Optical orientation of atoms in a magnetic field perpe
ndic
lar to the beam
SOURCE: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 49i
no. 1, 1965, 97-106
TOPIC TAGS: magnetic moment, molecular bi-am, bezun modulation,
gas laser
ABSTRACT: The authors investigate theoretically and experimentally
a new method.of orienting gas atoms in a magnetic field perpendicu-
lar Ito an orienting light beam. This is done by using an alternat-
I.ing magnetic field in addition to a constant one, and modulating
the alternating field while maintaining the beam intensity constant.
It is shown theoretically that if the alternating field makes a-

L
.00541-56
ACCESSION NR: AP5019221
-small angle with the constant field, then the resultant moment
precesses about the constant field and produces large constant com-
ponents of the magnetic moment in the directions of the magnetic
field and of the light. The theory of the process is briefly devel-
oped and expressions are derived for the total moment and its pro-
jections. To check, on the theory, experiments were made on the dc
and ac components of the moment projections on the light beam and
on the constant field in the vicinity of the first resonance., The
experiments were made with a mixturelof cesium vapor and argon,
using an orienting beam which was circularly polarized and contained
only one long-wave component of the resonant doublet. A cesium
electrodeless discharge spherical lamp served as the source. The
experiment setup is described. The test results are found to be in
isatisfactory agreement with the theory. Plots were obtained of the
Idepth of modulation of light on the amplitude of ~he alternating
Ifield, of the dc components of the moment against the constant field,~.
land of the resonant broadening by the alternating field. Orig. art.
3

_L io ~T -2/EFF(n)-2 (k)/EWA(m) _2/EA(h)/
_ra)/EEC(k)__
ACC NR, AP 001660. ETctm) - SMI-Tik(e) SOURCE CODE: Ult/0051/65/019/006/0982/0984
Vqj ~'(7- Y !I
AUTHOR:. Aleksandrov,.Te.'&; Bonch-Bruyevich, A.M.; Koutin, N. N.; Khodovoy, j.;-
ORG: none
TITLE: Stimulated Raman.scattering in a selective resonator
SOURCE':-- Gptika i spektroskopiya, v. 19, no. 6, 1965, 98,2_984
TOPIC TAGS: laser, Raman scattering, stimulated eMiSSiOTI, laser cavity, Ramon
laser
ABSTRACT: The stimulated Raman scattering was investigated at an excitation power
just above the threihold using the following three different setups: 1), a Raman
cell in the resonator of a laser; 2) a longitudinal selective resonator (the term
used by the authors for the case when the Raman laser - Wator is in the direction
of the ruby laser resonator); aM 3)a transverse selectiv Tesonator (the term used for
the case when the/Raman laser resonator is rotated 90* from the direction of the
axis of the rubyNlaser, i.e., a 90* off-axis Raman laser resonator). In the first
setup the gi7a_ntpulses were produced by a ruby crystal. Using two variable-trans-
mission-coefficient filters (transmission coefficient 30-50% at X - 694 mv) the
effective intensity of the 30-300 nsec-duration pulses in the resonator reached
100 Mwt/CM2. The maximum energy per pulse was 3-4 J. Two dielectric mirrors writh
a transmission coefficient of 0.4% at X = 694 mv, 0.8% at X 745 mv (the fundamental
Card J/Z %35-t37 6 .3 5.L.~_35

L 10789-66
ACC W AP6001660
SRS line in benzene), 40% at A 805 mu (first harmonic) and 70% at A 875 m
(second harmonic) were used in the experiments. The SRS in benzene had thresholds
for a specified length of the Raman cell (i) and the laser input power. No SRS
was observed at I < 2; however, SRS.was stable for 5 < 1 < 60 cm. The threshold
power decreased almost linearly with increasing 1. At 1 w 60 cm the of ficiency of
energy conversion reached 10% of. the puwer An the cavity. It - -.4as observed that
an.increase in thielenergy'of theLpulSes from the ruby 1.5-2 times above the :L
threshold resulted in a three-order:inerease in SRS. InLthe longitudinal selective
setup, the additional reflector betweentbe ruby rod.and the Ram."Lcell had a tranS_L
missionLCoefficient of 90% at--A - 694 mp, 10%,at X - 745 V, and 1% at A 805 and
875 mv. In this mode of operation the efficiency of energy conversion was at least
as high as that in the previous case. Two higher harmonics at A = 745 and 805 mp
which reached saturation at ulo% of the input power were observed. Results similar
to those of the
longibidina--setupl.Fere achieved with a transverse selectivesetup. HY.Never,
SRS was achieved in a Raman cell the length of which along the laser beam was only
I cm~ Stimulated Brillouin scattering in benzene was also observed in this setup.
Orig. art., has: I figure. ICS]
SUB CODE:, 20 SUBM DATE: 15Apr65/ OTH REF: 004/ ATD PRESS://1/4W
L-Card

'1Q242.;-6& RDAWTU C -2/T/E111P
)AWN00AWT(WEEC V51LIA W_ 'nly
ACC NRt AP6=19T VGJH~ SOURCE CODE: UR/0056/65/09/005/1435/1444
AUTHOR: kq dr ~Xp~I
;:,Bonch-BrqYev1ch Kostin, N. N.; Khodovoy, V. A.
..ORG: none
TITLE: Investigation of stimulated Raman and Brillouin scattering in (selective
resonators
SOURCE: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 49, no. 5, 1965,
1435-1444
2
TOPIC TAGS: laser, second harmonic nonlinear optics, Raman scattering, Brillouin
scattering, A"or-j,-~a-
ABSTRACT: The stimulated Raman scattering was investigated at an excitation power
just above the threshold using the following three different setups: 1) a Raman
cell in the resonator of a laser; 2) a longitudinal 8 ive resonator [the term
used by the for the case vhen the Raman lase donator is in the direction
of the ruby4uMeqrsesonator); and 3) a transverse selective resonator (the term used
for the case when the Raman laser resonator is rotated 900 from the direction of the
axis ofthe ruby laser, i.e., a 900 off-axis Raman laser resonator] (see Fig. 1).
In the,first setup (Fig. la) the giant pulses were produced by- a ruby crystal 10 to
12 cm long and 12-16 mm in diameter. With two variable-.transmission-coefficient
filters (transmission coefficient 10-80% at A 6943 the effective intensity of
Card -1/4

L 10242--66
ACC NN AP600019T
01
00.0
0,
r
-experimental set
Fig. l.- The UP
0000), a- SRS in the ruby laser resonator;
b- SRS I' n the longitudinal selec-
tive resonator; c - SRS in the trans.-
0000~ verse selective resonator.
V L - reson&tor length for scattered
radiation; 1 - length of the "ac-
tive" path for the scattered radia-
04 Z~Z?Z, tion in the resonator; 0 - mirrors;
0000 r - ccefficient of reflection;
F - variable coefficient of absorp-
0000 tion filters.
CGrd 2/4

L 10242-6
ACC NRt
AP6000197
the 20-200' nsec-duration pulses in the resonator reached 100 Mwt/cm2. The maximum
~energy per'pulse was 5-6 J. Two dielectric mirrors 01 and 02 with a transmission
coefficient of O.h% at A 694 mu, 0.8% at A = 7h5 mu (the fundamental SRS line in
benzene), and 40% at A = 805 mu (the first harmonic) were used in the experiments.
The sensitivity of the detectors was sufficient to register 10-4 of the energy of the
laser pulse. The setul~? shown in Fig.Ila was used to investigate SRS in benzene. It
was observed that an increase in the energy of the pulses from the ruby laser 1.5-2
times above the threshold resulted in a three-order increase in SRS at the funda-
mental frequency. Saturation was reached when the intensity of SRS was about 10% of
the energy input, at which time the second harmonic whose energy output quickly
reached the level of SRS at the fundamental frequency (at saturation), appeared.
When the second harmonic reached saturation the duration and the intensity of the
laser pulses decreased sharply due to the reverse effect of SRS on the ruby laser
pulses. When the length of the Raman cell ~1) was increased, the threshold power
and the pulse energy required to achieve SRS decreased. Also, the larger the cell,
the sm ller the energy above the threshold at which second harmonics were generated.
The SRS was stable when 1 was between 5 and 60 cm. In the longitudinal selective
setup (Fig. lb) reflector 02-replaced 04 and the transmisslon coefficient Of 03 was
very high at A = 694 mp and was at a minimum at A = 745 mg. The gain of SRS at
1 = 5, 20, and 60 cm was at least.as high as in the previoras case, although the pump
Dover and the pulse energy required were considerably smalLer. For example, when the
output of a ruby laser pulse of 30 nsec duration was h0 Mw (1 = 20 cm) three 10 Mw
SRS pulses of 20 nsee duration were observed in the Raman laser cell. Similar re-
de
Card 3/4

L 26i2
~-66 iw(m)/~wp(t) DLUP~l
J-P(0)
ACC NRi AP6015809 SOURCE CODE: U1VO38q66/0D3PWj04ZJ0
AUTHOR:, d=990ftUd~X. Sokolov,- A.: P.
-6G
non
41 ? -
--Cd - "imeeby.~ 3261'
a"MI -Orientation of resonant adiabion'
ik.rSOURCE --ZAxxihal.~_eks
no, i.,-ti6reticheskoy fiz'ikit m,v r a
rue urep, re nanc ight a
rf so b linei I. excit t o
nj.
~_nsnce line, 1. e splitting,
In
~'ABSTRACT' in
authors haV6~ob~a able -"of Cd -
3.2.1 nuclei in
The ~4,, tpredi., orientation
"vapor at a -den" ity j6 id of,'~ci
-0 -cm- -the' darI3~ -- l- ized
8 on iheL~ojder-- f' with a rci -po ar:
method of orientation is similar I n' its 6hbi' outlines ;td`. that
_used by the Yjistler-Brossel group'for',odd mercury.isotopes (Compi. rend. Acad. Scie'"_~
249, ~77, 2,53, 1959). Ole orientation of the cadmium was'Malized In a setup
#+'(Fig. 1) in witich 3-ight from, a high-freVenc -cadmium larap vas passed tbroxigh a
circulm- p6larizer to a euvette with Cd-11-3-: vapor, saturated rut 240C. The transmitted
filt
light was passed through a gas er filled with Cd-13-4 vapor, which selectively ab-
sorbed the byperfine component F = 3/2 of the 3261 A resonance line) thus increasing
ly several times the dependence of the brightness of the transmitted light on the
state of orientation of the nuelei.L The transmitted light was registered with a
T photoreceiver., The presence of orientation wAs established 'by means of a nuclear; res.
7 onance signal, To this endj an alternating magnetic field (4.8kcs) Perpendicular to
CaM 1/2

-.66
L 26128
ACC NR,
JiP6015809
t
Gener,
remepa-
MOP
H, VA.. yn
Fig. 1, Diagram of experimental setup., &4,w 0 . ch'.
de
ivm lamp., 2 -- polarizer Cil Am 1.
1 --, CadmL 3 Er
Cd ON-
cuvette., 4 gas filterp 5 -'photo- Ycuqm-
(b IW
receiver.
4
ity
the light ray was applied to'the cuvette. The constant fielC of variable intens
-.was directed at an angle of 450 to the light-beam axis. With such an arrangement..
the magnetic resonance was accompanied by modulation of the ta-ansmitted light at the
alternating-field frequency, and this served as the resonance signal. A distinct res-
onance signal with.half-width of several cps in a field of 5.2 oe,was observed. ap-
proximatelF corresponding to the published value of the nuclear moment of Cdl-"I-. The
signal exceeded by two orders of magnitude the noise level, the receiver bandwidth
be:~-% apprimdmate1y 1 cps. The authors plan to investigate in the future the charac-
ter L,O the relaxation processes in the system and to attain t more complete orierrta-
tion oi' the ensemble. The same method can be used to orient CdI 7he authors t
M. P. ChoMm for help with the work an;! A. M. Bonch-BrtWevi t for support and interes
SUB CODE: 20/ SM DATE: 3.1 MaX66/ Oni REF: 005
:W
Car

L 29.967-66- E1VT(1) ijp(c)
ACC NR-Ap6oo2883 SOURCE CODE: UR/0286/z~)5/000/021,,/0041/0()41
IhTENTOR: Aleksand?~~T...,Ye. B.; Bonch-Bruyevich, A. DI.;
ORG: none
TITLE: Method of measuring the modulus and direction of
of force of weak magnetic fields.(,.Class 21, No. 1,76976
SOURCE: By-ulleten' izobreteniy i tovarnykh znakov, no.
ICiodo-voy, V.A.
the vecuor
24, 1965, 41
TOPIC TAGS: magnetic field measurement, vector, w-eak magnetic field,
magnetic field intensity, paramagnetism, measurement
V~
ABSTRACT: The method ofAmeasuring, the modulus and direction of the
vector of force of weak ih!15netic fields, based on the optic orien-
tation of atoms, is c aracterIzed by tne fact that the effect of the
action of the measured magnetic field and of the known light intensity
on the paramagnetic atoms is compared and the magnetic field strenSth
is determined by the intensity of the orienting light. These charac-
teristics are incorporated in order to widen the measurement rar.,re ol'
weak magnetic fields.
SUB CODE: 20/ SUBM DATE: 13Apr64'

510041
SOUIRME CODE: UR/Q386A6/003/002/008,
ACC N ,Rt AP7007681:
-t AUTHOR# Aleksand' Y B Bonch-Bryevich, A. M.;:Kostin, N. N.; Khodovoy, V. A.
State "Ordeir of Lenin" Institute of Optics im. S. I. Valrilov (Gosudarstvennyy
bi-dena Lenina Opt cheskiy institut)
TITLE: Frequency shift of optical transition in the,field of a light wave
~i SOURCE: Zhurnal eksperimentalln6y i teoreticheskoy fiziki. Pistma v redaktsiyu, v. 3ol
:1 no. 2, 1966, 85-88
ITOPIC TAGS: optic transition, ruby laser, photowultiplier, optic filter, resonance
~Iline) laser pulsation, magnetic field intensity, light absorption/FS-7 filter, KS-19
I I
ibleaching filter !
ABSTRACT: The authors experimentally investigated the frequency shift of the optical
resonant transitiqn 4S1/2 - 4PJ/2 3/2 of potassium (principal doublet). It can be
be shown that the~expected freque-Acy shift of this transition is connected princ
ipallyi
'with virtual transition induced by the laser pulse from the ground level (01/2
4PI 2,3/2) and th~ excited level (4P3/2 - 6S1/2). The first pair of transitions is
sti~lsufficiently far from the resonances (the transition wavelengths are 7665 and
17699 A, that of the laser is 6943 A). The 4P3/? - 651/2 transition is much closer
to resonance OL = 6939 X). In spite of this, all these transitions make comparable
tributions to the sought frequency shift of the investigated transition, owing to
tcz difference in the oscillator strengths. It is important that the ground and
UDC: none

ACC NRt AP7W7681
excited levels are shifted here by the ruby-laser light in opposite directions.
In the experiment Iight from potassium lamp 1 was passed through vessel 2 with
potassium vapor saturated at 100*C (see the figure). At the selected temperature,,
the vapor absorbedabout 80% of the lamp's resonant radiation. Transmission of
light by vessel :2 was expected to increase during the action of the pulse from laser
3, provided the resultant transition frequency shift is commensurate with the line
width of the lamp iradiation (it was assumed that +.his line was broader than the
absorption line ofithe vapor). The transmission of the resonant light was recorded
with as~hotomultiplier whose output was fed to a pulsed oscilloscope (4 glass
filter
IT No
Card ;e/4

ACC NRI AP7007681,
laser
The scattered
light in the registration channel-was reliably cut out with FS-7
P
F'~~; filters. Prelimilaary experiments have shown, however, that the laser pulsed is
1~1 accompanied by scittered radiation with spectral components lying in the region of
the registered potassium line. The authors used a *cial method of filtering the
resonant line witi the aid of the Faraday effect to combat the mechanism of radiation
occurrence. Afte,- passing through vessel 2, the light beam of the potassium. lamp
was made to pass Through an,auxiliary euvette 6 filled -with potassium vapor and place
between crossed polaraids 5. A local magnetic field of approximately 2 kOe was
applied to cuvettp 6. The magnetic field produced, besides splitting of the absorp-
tion line, strong:;radiation of the p1sne of polarization of the light, but only in
the nearest vicinity of optical resonanco. By magnetic field intensity selection,
the system was mace to transmit almost &11 the resonant line, and to absorb the
extraneous light.!- The entire apparatus behaves like a high-transmission optical
filter with a bandwidth on the'orde:z-of 0.1 cm-1. Under the conditions described,
a distinct signal was recorded, evidencing a decrease in the absorption of the
resonant light by -the potassium atoms in vessel 2 during the time of action of the
laser pulse (20 nsec); the laser operated in the monopulse mode by using bleaching
filters KS-19. To verify that the change in the light absorption was not connected
with some experim6ntal errors the authors checked: (1) that the signal vanished
when -the potassiu~i light was turned off; (2) that the signal vanished when the potas-.-
sium vapor was frozen out in vessel 2 (with the illumination on the photonrultiplier i
maintained at the'previous level); and (3) that the signal vanished when the operating'
mode or lamp 1 walt forced so as to broaden the emission line (the broadening was
confirmed by the observations). The minimum laser radiation power density. at which
CGrd 3/4

ACC NR: AP7007683
the bleach' 5:L ~aal was produced was -10 )W/cm2 corresponding to an electric field
F
j
intensity (~n the ight of 105 v/=. The half-width of the spectral emission line
...I
is estimated at -31 x 10~ cp, so that the observed shift was of the same order
The authors thank P. A. Godina for providing the high grade polaroide. Orig. ;A
has: 1 formula aria 1 fiFn;re.
SUB CODE: 20 UBM DATE, 30NOV65 ORIG REF: 001
OTH REF: 003
Card

ALEKSANDROV, Ye.B.; KHODOVOY, V.A.
Letters to the editors. Opt. i spektr. 18 no.6:1090 Je 165.
(M,IRA 18:12)

ATY, ANDROVj~~q.
-.*-.- -
Upanding the enas of steel tubing with harametal expanaers.
Stan. i instr. 26 no.10:35 0155. (MLRA 9:1)
(Pipe, Steel)

RLEKIRNDROV, Ye-B.
Subject USSR/Engineering
Card 1/1 Pub. 103 - 14/25
AID F - 5359
Author : ileksandrov, Te. B.
Title : Ikivice for turning long shafts of small diameter
Periodical : Stsa. i instr., 8, 37-38) Ag 1956
Abstract : A description of a device which greatly reduces the time and labor
required for turning long, not-rigid, small diameter shafts is
given. Four drawings.
Institution : None
Submitted : No date

ALFKSANDROV) Ye. I.
MEASURING INSTRU1,!ENTS
Weaknesses in organizing supervision of measuring tools. Vest. mash. 31 No- 12, 1951
Monthly List of 11assian Accessions, Library of Conaess, Sept. 1952. Unclassil-ied.

1. iLLEKSANDROV; YE. 1.
2. ussR (6oo)
4. Measuring Instruments
7.. Shortcomings in-organizing the supervisionof measuring equi-6ment. (Remarks on
Ye. I. Aleksanclrov's article). Vest mash No 9 1952
9. Monthl Lis' of Russian Accessions, Library of Congress, April 1953, Uncl.
.U.L Z il -

ALEKSANOZOV, Yo. K.
Spinal anesthesia in labor. Akush. gin., Moskva No. 1:51-54 Jan-Feb 52.
(CLML 21:4)
1. Candidate Medical Sciences. 2. Of the Obstetric-Gynecological
Clinic of Yaroslavl' Medical Institute (Acting Head of Staff--Docent
O.G. Aunapu).

E- - - - AT -$?KSANDROVTEO-- K. PCAUDMATE OF THE MEDICAL SCMCES
Mbr., Department of Ob5tetrics and Gynecology Yaroslavl Medical Institute
91ethods of open care for the navel using surgical clamps and t4innin,"kkush. i
gin. no.4:60-62 JlAg 1952

AIIKWIDROV, Ye.K.
,
Concerning R.N. Iurleva's article on "A now method of treating
the umbiliail. cord.O. Akush. i gin. no.6:90-91 11-D '55 (MLRA 916)
(MIBILIGUS)

ALM(SANDROV, M K.
ALEY,SA,W.OVs YE. K. "Material on the study of the pathogenesis, clinical
aspects, and treatment.of late foxms of virus venereal
3,ymphogranuloma (Nicolas-Favre diseasia) in women (clin-
ical observations in the MNR)." Central Inst for the
Advanced Training of Physicians. Moscow, 1956.
Oissertation for the Ngree of Doctor iAOciences)
Mealcal
Sot Knizhnaya Letopial., No. 18, 1956

Z
/9
ALEKSANDROVt,
,f,,..,dotsent (Yaroslavl'
Surgical treatment of some forms of ulcerative vesidovaginal
fistulas and destruction of the urethra. Akush. I gin. 32 no.5:
49-53 5-0 '56. (MIRA 10:11)
(VAGINA, fistula
vas:icovaginalg with destruction of urothra, surg. technic)
(BIADD]IR. fistula
samo)
(UMHRA. die.
lesions in vesticovaginal fistula, surg. technic)

AMSh OV. Ye.K., doktor med.nauk
Variations in surgery for u.-ogenital fistulas in women [witb
summary in 31nglish]. Akush. i gin. 34 no.l.'71-74 Ja-F '58.
(MURA 11:4)
(zav.
1. Iz kafedry- akusheretva i ginekologii
- dotsent Te.l.
Aleksandrov) Yaroslavskogo veditsinskogo Institute.
(URMICIITAL USYSTAI, fistula
In women, surg. tedhnics (Rug))

EYCMPTA FEDICA See 10 Vol 12/10 Obstetrics Oct 59
1807. TUBAL. RESECTION IN ISTIMIC OTILATC3 1%1*10N OF 'ruBFS AND IN
E CTOPIC PREGNANCY (Itusslan text) - A to k a and ruv E. K. - AKUSIL
I GINEK. 1959. 2 (68-72) Illus. 3
The author recommends an operation for the rltllrti.. normal patency of
fallopian tubes by resection of the obliterated portbn, or the part concerned in
tubal pregnancy. followed by end-to-end ana5tomolis. In experiments patency and
the functional capacity of tubes and cornua were rf,stored In 761,6. In 1937 the author
performed this operation for the first time in the t (SSR. In 10 trionths normal gets-
tation ensued, terminating in normal labour; a su sequent pregnancy resulted in
abortion. Up to 1941,6 operations had been perforr ed, 3 in caces of ectopic pre-
i gnancy. Insufflation in 5 cases revealed that the oi erated tube was patent: in one
patient Insufflation was contraindicated (fresh gonf rrhoea). Salpingoanastomosis
was performed for the 8th time in 190 (ectople pi agnancy). Gestation ensued in
2 yr.. followed by the birth of a live child. The tv !hnique of the operation is des-
cribed.

ALEKS.ANDROV,, Ye.K..
Viral lyq)hograntaoma vener= (NIcolas-Favre disoase) as a pro-
cancerous disease. Vop.wflc. 6 no.2:61-67 F 060. (MIRA .14:2)
(1,YMPHOGWMOMA VENEREUM) (CANCER)

~ AI&SANMY Ye, 1,.
t
Doe of peridural anesthesia In gynecology. Acush,J gin, 36 '
no.4M-73 JI-Ag 960. (MMA 13s12)
(GENITOMWARY ORGANS--SMMff ) (SPINAL ANESTTESIA)

ALEKSAEDROV,-Ye.K., prof. (Yaroslavl')
Some problems of the prevention and treatment of bemorrhages
during prognancy, labor, and postnatal period., Sbor. nauch.
trud. Ivan. gos. med. inot. no. 28:223-231 1 63
(MIRA 19:1)

P(c) GG/BB/GD/JXT(BF)
KC-C-NR, ltwo9442 SOURCE CODE: UR/0000/65/000/i)00/0045/0051
AUTHOR: Aleksandrov, Y(s. K.; Sullpovar, V. L.; Timokhin, V. 1.
ORG: none
TITLE: The fundamental characteristics of a model learning automaton iind certain results of
its learning to discriminate Rattgrne
SOURCE: AN SSSR. Nauchnyy sovet po kompleksnoy probleme Kibernettka. Bionika (Biontes).
Moscow, Izd-vo M, I K, 45-51
TOPIC TAGS: logic circuit, logic element, pattern recognition, algorithyn, electronic feed-
back, automaton
ABSTRACT: Logic circuits made up of threshold elements are used as the basis for a learning
automaton. These bases were proposed by Varshavskiy in 1962. The problem of pattern re-
cognition is solved by finding the logic function wha-ch divides the sets of independent binary
variables Into two classes. Where Varshivskiy used an ideal logic circuit of threshold ele
ments, in the present work the weight factors of the input of every threshold element In the
first layer do not change durlng teaching and can accept only one of three fixed values +1, 0, -1.
With respect to this, the inputs of a threshold element di-Ade into activating (t z=+I), retarding
Q=-1) and blank (~=01. The thresholds of all the elements are the same and re -main constant
1/2

L _3.~3 66
_ . _9JM__
ACC NR; AT6009442
throughout the entire process. Every threshold element realizes the function
n
Yi =sign ~Ixi- 77 1, where ~i is the weight factor of the i-th input; x, is the value of the
binary input variable at the i-th input;," is the threshold value-, n is the number of the inputs of
the automaton and j = 1, 2, 3. ..... n. The specific advantages of this automaton are the large
volume of Information about the signal, the parallel processing principle, and the use of
distributed memory. It should be added that there are individual memory units for storing
weight factors for each threshold element. The automaton was used in 1962 for discriminating
the letters of the Russian alphabet, numbers, and various geometric figures. The methodology
for teaching the automaton Is discussed. Algorithms were used In the majority of cases. Feed-
back was discontinued and every element was checked for Its correct answer to the teaching
sequence. The teaching process was continued for those elements which gave wrong answers.
Curves are given showing the increase in the number of correct answers for the elements of the
automaton. A part of the experiment consisted of finding out whether the automat was able to
recognize new elements of the images already incorporated. This phase of the experiment was
called "checking the automaton for generalization. 11 Under these conditions 60 to 80% of the '
answers were correct. The automaton was simulated n h gh, Td digital computers when the
0 'p
linear law of weight factor change was Lve_r1fi6&.'_ it is shov ;n that emiton becomes more-!,
flexible with an increase In the number of ide-me-fits or the complexity of structure. Orig. art.
has: 6 figures, 4 formulas.
0S7
SUB CODE: 09, 16 / BUBM DATE- MOM / ORIG REF: 001

,-. ALMSANDROV, Ye.P.
Preparation of models for studying the mechanism of sudden death
in imuff icienoy of coronary circulation. Trudy LSGNI 48:227-238
159. (MIRA 34:2)
(CORONARY HEART DISEASE) (DEATH (BIOLDGY))

ALEKSAWR-Qy,j"" FLAVITSKIT, Tu.V.
"Now~~10"FINUM
Detemining parametirs for electric motors used on ctiters ard
cutter-loaders. Ugoll 32 no-5t24-28 My '57. (MLM 10: 5)
(Electric motors) (Electricity in mining)

ALEMAMROV, 76.V.,inzh.; NOVAKHOVSKATA, D.S.,inzh,
Using soup dtock as a plasticizer. Biul.stroi.tekh. 12 no.10:
15-16 0 '55. (mila 12:1)
1. Tre3t "Stroitell."
(Plaaticizero) (mortar)
- A- ~

_I~vUnjy 1y :Lc~h PATELOVSKAYA, M.I., red.;
-ALF-KSAXDAQY,
NOCHALINA) Z.3., tekhn, red.
(Safety manual for roofers] Pamiatka po tekhnike bez-
opasnosti dlia krovellshchika. Izd.3., ispr i dop. Mo-
skva, GosstroUzdat) 19*63. 20 p. ~MIRA 17:3)

ALEKSANDROV . KIR1YA T.A.; KHMIADASHVILI, P.I.
-~-- y ,
Vibration compensator for a drilling tool. Heft. khoz. 43
no.5tl7-20 Itf 165. (MIRA 18:6)

ALIMSUTDROV Tu aviatekhnik
This is how the time is allocated. Grazhd. av. 17 no.8:25 Ag 160,
- (MIRA 13:9)
1. Lineyn6-ekepuatatsionnava i remontnaya Z%Sterakaya, Ioningrad.
(Ieniwad--Airplanea--Maintenance ana repair)

ALEKSAMRQY--Yu.; PILIPUSIIKO, I.; VOLCFENKO, V.; SEMEROV, I.; LIMARENKOV, L.;
YARkOV, G.; YENTSEV, I.j KUMUT, 14,; SHCHEKOTOVIGH, P.; BOBGVICH,7~;
CHEREPANOV, G.
They are raising the level of their qualifications. Zeishch.rast.
ot vred.i bolo 7 no:,5.-61 ~~ 362. (MIRA 15-'11)
(Plants, Protectioh of-Study and teaching)

ZAKHLRKIN,, O.A.; KOLDAYEVA, T.N.; LISOGURSKIY, Z.I.; SKOVORODKIN, P.A.;
POLYAK, M.A.; YURIYEVA, A.K.; PrInimali uchastiye: GAVSHINCYV, I.I.;
. SAVINA., A.S.; ALEKSANDROV, Yu.A.; S~MdWGVAV A.N.
Some peculiarities in preparing rubber mixtures in a two-speed
rubber mixer. Kauch. i rez. 20 no.10:39-41 0 161. (MIRL 14:12)
1. Yaroslavokiy shinnyy zavod.
(Rubber industry-Equipment and supplies)

ALEKSANDROV
Fimt a-*d, P
L ior oneself and a comrade. Voen. zna-,i. 1+2 no.2:
26-127 F 166. (ISIMI 19: 1)

ACC NR~ AP6022040 SOURCE CODE: UR1012C!66/1)00/003/0221/0222
AUTHOR: Aleksandrov, Yu. A.; Kutsenko, A. V.; Maykov, V. N.; Paviovskaya, V. V.
ORG: Phy~ics Institute, AN SSSR, Moscow (Fizicheskiy institut AN SSSR)
TITLE: A water soluible epoxial glue for scintillation counters
SOURCE: Pribory i tekhnika eksperimenta, no. 3, 1966, 221-222
TOPIC TAGS: glue, epoxy plastic, photomultiplier, cerenkov counter, scintillation
counter
ABSTRACT: A water-soluble glue for use in scintillation counters, Cerenko-,l spectro-
meters, and other similar equipment has been developed. The glue provides good, uni-
form optical and mechanical contacts between photoelectric amplifiers and irradiating
or light-conducting media. The glue is made from a DEG-1 epoxial resin (a glycerin
compound) and a DEG-1 hardener. The glue maintains its consistenr--, . 40 to 60 min after
it is prepared; it requires approximately 20 hr to fully harden. It takes from sev-
eral hours to several days to dissolve the glue joints depending on their thickness,
the temperature, and rate-of-flow of water, and the surface area of' the joint that is
exposed to water. The light conducting properties of the glue have! been studied on
scintillation counters and have been found satisfactory. The authars thank Ye. S.
Potekhina, L. A. Skrylova, and Ye. M. Blyakhman for consultations and for supplying
the specimens.
SUB CODE:/g 0 SUBM DATE: 14May65/ 6RIG REF: 001/ OTH REF:
Card 1/1 / I UDOP 539.1.074,

ALEKSANMOT, Tu.A., inshener.
Goatrolling the operation of transformers in urban electric
networks. Bnergetik 2 no.2:19-20 F 154. (MLRA 7:4)
(Blectric transformers)

ALMANDROV, Yu.
I -
Gigantic radioteleocopes. Nauka. i shiznl 22 no-10:54 0 155.(KLRA 01:1)
(Telescope, ItAdio)

SHRETBER, V.;
Urgent problems concerning operation of transformers in city
electric power networks. Zhil.-kom.khor. 6 no.8:14-15 '56.
(MLRL 10:2)
1. Glavrqy inshener treat& "Kavmineoergo" (for Shreyber).
2. Nachallnik takhnicbeakogo otdola tresta "Kavminanergo"
(for Alskeandrov).
(Electric transformers)

MAMSANMOV inthener; SHREYBER. V.P., inshoner.
wwm;:~Zw_
Onerating 6 kv city pover lines in sleet areas. Inergetik 5
no.6:17-19 Je '57. WaA 10:7)
(Electric lines)

ALRMNMOV, Tu., inshener; SHPZYBZR, V., inshener.
%W - - -
ga ~~ I 'A
Sons problems In operating city cable lines. Zhil.-kau. khos. 7
no*2:11-13 '57s (KM io.-4)
(Electric cables)

AUTHORS: S74reyber~ V.P. and Aleksandrov, Yu.A. 94-1-13/24
TITLE: Extravagance in the Construction of Urban Electricity
Distribution Systems (0 nekotorykh izlishestvakh v stroitel'-
stve gorodskikh elektricheskikh setey)
PERIODICAL: Promyshlennaya Energetika, 1958 L40.1
pp- ~?'_'29_'*~USSR)'
ABSTRACT: There are as yet no general rules about the design of
urban distribution systems. Therefore, the erection of lines
for distribution of electricity, radio and communications,
street lighting and supply to electric clocks is not co-ordinated.
Much expenditure can be saved by preparing rules for the com-
bined erection of such lines and siting them to fit in with
street gardens., It is wasteful to use columns only for street
lighting. An example of the multiple use of lighting poles is
shown in Fig.l.
Since it is now necessary to provide concrete footings for
wooden poles, the spacing of poles should be reviewed to avoid
waste. Greater use should be made of reinforced concrete in
various structures. At present the common types of transformer
mounting and distribution equipment use littlexeinforced con-
crete. Existing typical transformer-stations for general
Cardl/2 supply are somewhat extravagant and greater use should be made

..AL%,SANDROV, Yuriy Andre evjq4;,, STRL"I'O', Aleksandr Alekseyevich;
`~VfITSP%6_66V'tio~ich; JLTUFIYBVA, A.M., red.izd-va;
LICLYUKMN, I.A., tekhn.red.
(Experience in the operation of electric networks in the cities
of Stavropol Territory] Iz opyta ekspluatatsii alaktrichaskikh
setei gorodov Stavropollskogo krain. Moskva, Izd-vo H-va kommun.
khoz.RVSR. 1959. 77 P. (MMA 12:10)
(Stavropol Territory--Electric networks)

IT:-,E) c;f cable cabincto In 6 L.ower
r.c!t,vcrks;. Tralr!y !JEI 17:6)
1. Tr,,st ORavminvodoem;z,,".

I_Z',xjj2Z66
ACC NRt AP600157Z 0,) SOURCE CODE: URIOIZO/65/0001006/0084/0089
'AUTHOR: Alcksandrovs Yu.. A.; Kutsenko, A. V.; Maykov, V. N.;
;P -12ovska DtZT.__.*Sa
ORG: Institute of EhXsics, AN SSSR (Fizicheskiy institut AN SSSR)
TITLE: Using an AI-100 pulse analyzer as a storage device
SOURCE: Pribory i tek%nika eksperimenpta, no. 6. 1965, 84-89
~
iTOPIC TAGS: pulse analyzer, cornputer storage device/ Al-100 pulse analyzer
ABSTRACT: The remodeling of an AI-100 pulse analyze for purposes of measuring
Awo simultaneous pulses is de scribed; a fifth program ("storage operatiore') is
introduced into the AI-100. The storage is controUed from the outside, while the
arithmetic unit is used for receiving and recording two simultaneous pulse trains.
The resulting storage device has a constant dead time at its two inputs of 120 t4sec,a
pulse-height range of 1-100 v, and 99 storage addressee for synchronously recardin
the results of measuring two pulses. Tables of operations and commands are given.
Such a remodeled analyzer hits been used for one year in conjunction with two
Cerenkov total -absorption spectrometers (with the 680-Mev FIAN synchrotron).
Orig. art. has; I figure and 2 tables.
SUB CODE: 09 SUBM DATE: 23Nov64 ORIG REF., 002
Card 1 1
UDC-.

L 28055-66 EWT(1)/ETC(m)-6 IJP(C) N
C Ri, AP-5087006 SOURCE CODE: TJR/0120/65/000/005/0045/0048
AUMOR., Al9ksandrov. Yu. A.; 'xut,9_Q'M)CQ, At V.; -ALaykov.' Vt---Nt
Tavlovska7a-, V._V6_
ORG: lu-titote of Phygi o AN SSAP- Mnyntw (Fizicheskiy institut)
TITIE: Time characteristics of Cerenkov.total-gLbtLoxptJm
SOURC3: Pribory I tekhnika ekspr*rimenta, no. 5, 1965, 45-48
TOPIC TAGS: gamma spectroscopy, Cerenkov radiation, Cerenkov counter,
photomultiplier tube
ABSTRACT! In order to Investigate the resolving time of a.Gerenkov-
spectrometer~-a method of coincidence circuits was applied. A spectro-
meter (de bed in PTE 1964, no. 34, p. 38) with a 300-mm radiator was
used. The light from the radiator was collected by the FEU-49 photo-
multiplier tube. The coincidence circuit was formed by the addition of
two FEU-36 photomultipliers which had an adequate amplification factor
and a time spread not greater.than 2 nsec, By such an arrangement a
resolving ti'me of about 4 x 10-9 sec was obtained without diminishing
the 100-pot efficiency of recording the gar-ma quanta in the range from
100 to 600 Mev. After a preliminary theoretical study, the experlmenta~
Card 1/2 UDC: 539.1.074.4

L 28055-66
ACC NRt AP5027006
were conducted and the performance of the coincidence circuit was testa.~.
The experimental curves showed that at the electron energy of 100 Mev,,
a 100-pet efficiency of recording was attained when two additional
FEU-36 photomultipliem were included in the circuit. The dependence of.,
the recording efficiency upon the resolving time was also investigated-
and the curves of "delayed".coincidehoes were plotted for electron beLm
energies of 100 and 500 Yev. In the case of 100 Mev, the best resolv-
ing time was 4.7 x*10-9 sec While at 500 Mev the 100-pot efficienoy.was
attained at about 4 x 10-9 see. The comparison of these results.with
the data published by other authors showed the superiority of the abovG
arrangement. The,authors.expressed their appreciation to Ye. M. Levkin
for the discussion of various problems, to T., I. Kovaleva for the selee-
tion of FEU-36 tubes and.the assistance in measurementi-l-a-n-d to the
personnel operating the 680-Mev synchrotron. Orig. art. has: 3 graphs,
1 table and 1 formula.
SUB CODE: i18 SUBM DATE: 64 ORIG REF: 003 OTH 003-1
U91.
Card 2/2, LIA

'_~VC1fdT DE: UH/6_i20/_66_!ooo/0l2/0050/0054
ACC NR, AP7001938
AUTHOR: Aleknandrov., Yu. A.; Kutsenko, A. V.; Maykov, V. N.;
Pavlovskaya, V. V.
ORG: Physics Institute IAN 98SR, Moscow (Fkzicheskiy institut AN SSSR,
Moskva)
TITLE: A system of correlated Cherenkov spectrometers with analysis of
data on an M-20 computer
SOURCE: Pribory i tekhnika ekoperimenta, no. 6, 1966, 50-54
TOPIC TAGS: nuclear radiation spectrometer, spectrometer, Cerenkov
counter, computer application
ABSTRACT: A system designed to measure correlated Y-quanta or electronsi
in the 100--600-14ev range is described. The system, originally designed I
to study neutral particles generated by a 680 Mey synchrotron, consists,
of two full-absorption Cherenkov spectrometers working either in a-
coincidence or an anticoincidence made, recording and storage logic
circuits, and calculating and output equipment. The recording and stor-i
age logic circuits consist of an AI-100 analyzer with a changeable pro-
gram, linear amplifiers, and transistorized and tunnel-diode logic
circuitry. Control and calculation is performed by an M-20 computer.
Card 1/2 line '. 539.1.074.oh

ACC NR: AP7001938
Input to the computer is on 80-column punched cards. The output equip-,
ment comprises a card punch (the output card punch of the M-20 computer),:.
an EUM-23 electric typewriter, and a number of calculating devices of
t8e PS-100 system. The system output is a 100 x 100 x,y printed matrixi I
Information along the x and the y axes indicates the pulse amplitude
registered by the first and second spectrometers. Some of the system
parameters are: energy resolutions, � 21.5- 9.5%; resolving time of
the two spectrometers connected for coincidence, 5*nsec; dead time
when registering occurrences, 130 nsec; capacity of the operating
intermediate memory, 99 addresses with 16 bits in each; readout time
from the intermediate memory, 10 see (on a. punched card); system process~
time for 10,000 numbers (including input and output time), 10 min.
Orig. art. has: .1 figure
SUB CODE: 18/ SUBM DATE:..17Nov65/ ORIG REP: 007/ OTH REP: 002
Card 2/

30206
S/081/61/000/019/032/085
-~'j oD B11O/B138
AUTHORS: Al(~keandrov, Yu. A., Brilkina, T. G., Shushunov, V. A.
TITLE: Oxidation of organometallic compounds,, 3. Synthesis and
some properties of triethyl lead oxide
PERIODICAL: Referativnyy zhurnal. Khimiya, no. 19, 1961, 145, abstract
19Zh44 (Tr. po kh1mii i khim. tekhnol. (Gorlkiy), no. 3,
1960, 381-387)
TEXT: The oxide of triethyl lead (I) was obtained by reaction of disperse
metallic Na with triethyl lead monohydroxide (II) in benzene. I decomposes
ato,j 200C, reacts vigorously with acetone and acetaldehyde, and reacts
instantaneously with water to form II quantitatively. When reacting with
methyl, ethyl, benzyl, and a,a-dimethyl-benzyl alcohols; as well as with
hydroperoxides of tert-butyl and cc-cumyl, I gives the corresponding oxy
and peroxy derivatives of triethyl lead, which are unstable at 1200C.
The rate of thermal decomposition of I at 70-900C without solvent was
studied. The products obtained consist of an equimolar mixture of
C2H6 and C2H4 (with an impurity of 1-1.5 % of butane), 0.97 mole of
Card 1/2

1102o6
s/m/61/ooo/oi9/032/085
Oxidation of organometallic... BI1O/B138
triethyl lead per mole of used I, and a solid substance containing 87.1 %
of Pb, which is insoluble in organic solvents. The authors assume that
the accelerating effect of I on the oxidation of hexaethyl dilead by 0 2
in n-nonane solution is caused by the ability of I to decompose with
the formation of ethyl radicals, whereby a degenerate chain reaction is
effected. For Report 2 see RZC, 1961, 8Zh231-, LAbstracter's note:
Complete translation.]
Card 2/2

30207
S/081/61/000/019/033/085
'3 -7 B11O/B138
AUTHORS: Aleksandrov, Yu. A., Radbill, B. A., Shushunov, V. A.
TITLE: Oxiiation of organometallio compounds. 4. Oxidation of
hexuethyl ditin vith oxygen
PERIODICAL: Referativnyy zhurnal. Xhimiya, no. 19, 1961, 145, abstract
19Zh45 (Tr. po khimii i khim. tekhnol. (Gorikly), no. 3,
1960, 388-393)
TEXT: The oxidation of hexaethyl ditin (I) with oxygen (II) in n-nonane
solution at concentrations of I ranging from 10 to 100 mole% has been
studied. The oxidation rate of I is described by a first-order equation
according to the concentration of I, and is independent of the pressure
of II within the range of 300-500 mm Hq. In the temperature range of
60-900C, E(act.) is 19-5 kcal/mole. 0 55 mole of diethyl stannic oxide,
0.62 mole of triethyl stannic oxide, and 0.12 mole of acetaldehyde are
formed per mole of oxidizcd I. Water was found qualitatively. The
oxidation of I is not catalyzed by addition of 13.2 mole% of triethyl
lead oxide. Addition of 2.6-di-tert-butyl-4-methyl Phenol lovers the
Card 1/2

30207
S'/081/61/000/019/033/085
Oxidation of organometallic ... B1IO/B138
reaction rate to approximately one-tenth, which is indicative of a chain
iaeohanism of the reaction. [Abstracter's note: Complete translation.)
Card 2/2

oD
AUTHOR:
TITLE:
S/gI96
61/000/023/017/061
1~
B117/B147
Production of triethyl-tin peroxide
PERIODICAL: Referativnyy zhurnal. Khimiya, no. 23, 1961, 230, abstract
23Zh24O (Tr. po khimii i khim. tekhnol. (Gorfkiy),. no. 3,
1960, 642 - 643)
TEXT: A solution of equimolar quantities of anhydrous H 202 and
H.) Sn (I) in ether is shaken with anhydrous Na at -200C for
(C2- 3 120 2S04
[
15 minutes, and decanted. Ether is distilled off in vacuo, and the resi-
due diluted with hexane (II). (II) is distilled from the filtrate at
-100 C and I(C2H5)3 Snj2 02 is obtained. The peroxide decomposes completely
at -00C within 24 hr; at 600C it explodes, with water it decomposes more
slorly than M. [Abstracter's note: Complete translation.]
Card 1/1

)0 0
y
SO V/(,9;-30-2-56/i 8'
AUTHORS: ShUohUnov, V. A., Yu. I.
TITLE: Concerning the Decomposition of the Benzoyloxy Radicals
In Solutions
PERIODICAL: ZhUrn,31 ob3hchey khimil, _1960, Vol 30, Nr 2,
pp 632-634 (usn)
ABSTRACT: Benzoyl peroxidQ on heating di.,;,Sociates into bon'loylox,
j .1
radicals which, in turn, decompose into phenyl radicals
and CO 2'
c,11,G00 (10, (2)
If the above reactions are reversible then, in the pre-
sence of tagged CO 2' the tracer atoms should pass into
the nondezomposed benzoyl peroxide and alzo into the
benzoic ~,cid formed in reaction of the bei-.zoylo.-,y radicals
Card 1/2 with the oolvent.

Concerning, the Decomposition of the
Benzoyloxy Radical,~ ill SOILItIO!10
77*907
9 - 3 0 - 2 - 5 817 8
cgll.'Coo- + Ill( - C6111,C0011 -t- H-
In the pre~;ent OtUdy, benz-oyl peroxide was decomposed by
heating to 70-80c) C~ in the presence of C1402 in various
solvents (carbon tetrachloride, benzene, mixtures of
various alcohols with benLene, etc.). It was established
that reaction (2) wtas irreversible and that, under the
conditions of the experiment, there was no exchange of
C atoms between CO and the L)enzoylc,.,.,y i~adicals. There
are 2 table3; and W
, references, _~ U.S., 2 So,iet. The
3 U.S. referenceo are: L. Jaffe, E. Pro,,3en, M. Szwarc,
J. Chem. Phys., 27, 1116 (195(); N. '~wicbel, J. Turkevich,
W. Miller, J. Am. Chem. Soc., 71, 376 (1S~49); A. Seidell,
SOILlbilitieS of Inorganic and Metallorganic Compounds,
Vol 1, N.Y. (19531).
ASSOCIATION: Gorlicly Scientific Rvoearch Inotiti-ite of Chemistry
(Gorlkovskiy naLichrio-i.osledova'L-.el.lsl~iy institut 1,him-ii)
S'L113MITTED: February 12, 1959
Card 2/2

ALEKSANDROV, Y~.A. Cand. Chem. Sci. (diss) "Liquid-Phase
Oxidation of Hexa-ethyl-diolov, Hexa-ethul-dis-lead and Tetra-
ethyl.-lead by Oxygen." Moscow, 1961, 16 pp (Acad of Sci. USSR)
Instit. of Elementary Organic Compounds) 150 copies (KL 6UDP
12-61, 255)

S Y1 0 0
S/081/61/000/024/011/086
B138/BIO2
AUTHORS: Aleksandrov, Yu. A., Brilkina, T. G., Shushunov, V. A.
TITLE: Oxygen oxidation of distannic ethide, diplumbic ethide and
tetraethyl lead
PERIODICAL: Referativnyy zhurnal. Khimiya, no. 24, 1961, 75, abstract
24B541 (Tr khimii i khim. tekhnol., [Gorlkiy], no, 1,
1961, 3 - iiV
TEXT: The oxidation of distannic ethide (I), diplumbic ethide (II) and
tetraethyl lead (III) by oxygen was studied in solutions of n-C-H-- and
C6H3C13 at 50 - 90 0C. Additions of triethyl-tin peroxide cause'
considerable acceleration of oxidation ofI,although the initial increase
is not suatain6d, the reaction rate returning to normal in the course of
time. The products of oxidation of I are tin diethyl oxide, tin triethyl
oxide, CH3CHO and H20. Activation energy of the process is 190 kcal/mol;
In oxidation of II lead oxide, III, C 2H5OH, CH3CHO, and H 20 are formed.
Card 1/2

S/081/61/000/024/01I./086
Oxygen oxidation of distannic ... B138/B102
The dependence of oxidation rate of II on temperature and initial
concentration is of a critical nature. Considerable variations in the rate
of the process are observed with very slight (60 to 62.5 0C for instance)
variations in these Darameters. Additions of lead triethyloxide accelerate
oxidation of II, and additions of H20 retard it. C 2H6' C2'H 4' C4 H109 CHCIIO~
H20, the 1-hydro-2-oxide of triethyl lead, the 2-hydro-2--oxide of diethyl
lead, and the mono- and dioxide of lead are formed in oxidati~ln of III,,
Addition of solid-oxidation products considerably acceleraies oxidation of
III. [Abstracter's note: Complete translation.
Card 2/2

4290
S/081/62/000/022/026/088
B144/BIOI
~0
AUTHORS: Aleksandrov, Yu. A., Shushunovq V. A.
TITLE: Organometallio peroxide compounds. 2. Synthesis and some
properties of triethyl tin peroxide
PERIODICAL: Referativnyy zhurnal. Khimiya, no. 22, 1962, 227, abstract
22Zh240 (Tr. po khimii i khim..tekhnol. [Gor1kiy] , no. 3,
1961 , 644-651 )
TEXT: (C H SnOOSn(c H ) (11) was synthesized by reacting
2 5 3 2 5 3
(C2H5)3 SnOSn(C2H5)3 (1) with anhydrous H 202- A solution of 2-3 9 1 and
1 equ. H202 in 15 ml ether was agitated for 10-15 min (200C) with 1-1-5 9 LIP
anhydrous Na2 s04 (111); the solvent was evaporated and 10-15 ml of
hexane were added in the presence of 1-1.5 9 111. Within 5-8 min (Of
agitation) II was separated after th% solvent had been evaporated from'
the filtrate. In the synthesis a contact between reaction mixture and air
Moisture was avoided. II hydiolizes readily to give (C 2H 5)3 SnOH and H202
Card 1/2

S/081 /62/000110,12/026/088
Organometallic peroxide compounds. B144/B101
(yield in H202 100.2~6). On heating (6ooc) II explodes. In n-nonane
(0.1l'-0.60' M) II decomposes according to a first-order reaction (E(act)
14 kcal/male) with formation of (C 2H5)3 SnOC 2H 5and (C2H 5)2 Sno in
equivalent amounts. If II reacts with a solution of (C 2H5)3 SnSn(c2H5)3 (IV)
in n-nonane (200C) then I arises. The peroxide II decomposes when
induced and is caDable of initiating oxidation and polymerization reac-
tions. The course of thermal decomposition of II and its reactions with
IV are discussed. Communication 1 see RZhKhim, 1961, 23Zh240-
[Abstracter's note: Complete translation.3
Card 2/2

88569
S/020/61/136/001/017/OIA7
0 B0161BO55
AUTHORS: Aleksandrov, Yu._A., Brilkina, T. G., ar-d Shushunov, V. A.
TITLE: Bistriethyl-lead Oxide
PERIODICAL: Doklady Akademii nauk SSSR, 1961, Vol. 136, No. 1, pp. 89-92
TEXT: Bistriethyl-lead oxide,((C2H5)3 Pb)20, was synthesized with a view to
establishing its properties and studying it in detail. In an earlier work
the authors had found that bistriethyl-lead oxide has a marked accelerating
effect on the oxidation of hexaethyl dilead by oxygen. They assume this
effect to be due to free radicals formed by decomposition of bistriethyl-
lead oxide. Basing on their own resulte, they state that this compound has
never actually been obtained by other researche2.-s (Refs. 2-4), since
bistriethyl-lead oxide hydrolizes in alcoholic and aqueous solutions. The
authors therefore applied a different method: They dispersed metallic
sodium in n-nonane, removing the n-nonane thereafter by decanting and
distilling off, and then poured on dry benzene. To this mixture they added
a triethyl lead monohydroxide portion so calculated that sodium was well
Card 1/3

88569
Bistriethyl-lead Oxide
S/020/61/136/001/017/037
B016/BO55
in excess. In the course of 2-3 h triethyl lead monohydroxide was trans-
formed into bistriethyl-lead oxide which is readily soluble in benzene.
After filtering off the solid residue, and distilling off the benzene,
bistriethyl-lead oxide was obtained as mobile, faintly yellowish-green
liquid with a sharp specific smell. At room temperature, bistriethyl-lead
oxide hydrolizes to triethyl lead monohydroxide (to an extent of 98-99%).
Alcohols and tertiary alkyl- and aryl hydroperoxides act similarly to
water, transforming the bistriethyl-lead oxide to oxy- or peroxy comp _-nnd.;
of triethyl lead, besides triethyl lead monohydroxide. At temperaturc-, 0"
only -101C, several of these reactions occur at an appreciable rate. Tb:.
authors studied the effect of methyl-, ethyl- and benzyl alcohol, dimefty'J.-
phenyl carbinol, tert-butyl-and a-isopropyl phenyl hydroperoxide on
bistriethyl-lead oxide. The following compounds were obtained: ethoxy
triethyl lead, tert-o-butoxy triethyl lead, a-isopropyl-phenyl peroxy
triethyl lead, methoxy triethyl lead and a-isopropyl-phenoxy triethyl lead.
The organic oxy- and peroxy compounds of lead are unstable and decompose
gradually at room temperature in sealed ampoules, accompanied by a color-
change to redbrown. Bistriethyl-lead oxide reacts vigorously with acetone
at room temperature, under formation of triethyl lead monohydroxide. In
Card 2/3

88569
Bistriethyl-lead Oxide
3/020/51/136/001/017/037
B016/B055
the presence of a great excess of acetoneq mesityl oxide and a resin which
was noz further investigated were formed. On heating, bistriethyl-lead
oxide decomposes comparatively rapidl with liberation of an equimolecular
mixture of ethane and ethylenet and 1~ butane. The residue is tetraethyl
lead (Ref. 7). There-are 2 figures, 1 table, and 7 references: 2 Soviet,
2 German, 2 US, and 1 British.
ASSOCIATION: Nauchno-issledovatellskiy institut khimii pri Gor1kovskom
gosudarstvennom universitete im. N. I. Lobachevskogo
(Scientific Research Institute of Chemistry of the Goilkiy
State University imeni N. I. Lobachevskiy)
PRESENTED: july 4, 1960, by M. I. Kabachnik, Academician
SUBMITTED: July 4, 1960
Card 3/3

11-7 ,
7
28732
S/020/61/140/003/013/020
B100101
AUTHORSt Aleksandrov, Yu. A., and Bhushunov, V. A.
TITLEs Triethyl tin peroxide
PERIODICALt Akademiya nauk SSSR. Doklady, v. 140, no. 3, 1961, 595-597
TEXTs Since peroxides of the type R nMOOMRn (R - hydrocarbon radical,
M - metal) are only known for Cdt Si, and Go, the authors investigated the
triethyl tin peroxide (TETP) synthesized by them, (C 2R5)3 SnOOSn(C2H 5)3' The
synthesis was carried out by mixing equimolar amounts of triethyl tin oxide
and anhydrous H,O,, dissolved in absolute ethyl ether, in the presence of
anhydrous sodium sulfate. After 10 - 15 min vigorous shaking, the mixture
was filtered, and a new portion of sodium sulfate was added to the filtrate .
After distilling off the ether at reduced pressure and room temperature, a
small amount of hexane was added, and shaken for another 2 - 3 minutes.
After filtering off the sodium sulfate, hexane was distilled off. The
residue was a viscous, golden-yellow liquid, pure TETP (100-101 % active
oxygen). Its synthesis was achieved according to the reactioni
Card 114

2871~61/14 0/003/013/02
S/020 0
Triethyl tin peroxide B103/B101
(C2H5)3 SnOSn(C2H5)3 + H2 02F==::~(C2H5) 3SnOOSn(C2 R5)3 + H 20 0).
The resulting water was bound by sodium sulfate. The tin content was
53.6 %, the molecular weight 443-4. TETP is very'aasily hydrolyzed by
water without heatingt (C 2H5)3 SnOOSn(c2'q 5)3 + 2H20-4 2(C 2R5)3SnOR + H202(2)
This reaction was used to determine the active oxygen by means of
permanganatometrio titration. TETP is ver~Cunstable and decomposes
completely within 24 hr at approximately 0 - At 600C, decomposition
proceeds most vigorously in a sealed glass phial; an explosion occurs
after 2-3min. In n-nonane solution, this reaction Is much slower. It can
be described by a kinetic reactipn equation of first order. During the
reaction, a white deposit is precipitated from the solution. It is
unBoluble in ordinary organic solvents and was identified as Aiethyl tin
oxide. A second product of thermal decomposition, ethoxy triethyl tin
(boiling point 190-1950C), remained in the solution. It can be hydrolyzed
with water, thus forming triethyl tin monohydroxide. From 1 mole of TETP,
0.93 moles of diethyl tin oxide, and 0.98 moles of ethoxy triethyl tin are
formed. The apparent activation energy of TETP decomposition in n-nonane
is 14 kcal. Polymerization of methyl methacrylate and acrylonitriie is
Card 2/4

S1020 13/140/003/013/020
Triethyl tin peroxide B103/BIO1
initiated by additions of TETP. At room t.emperaturq, TETP reacts very fast..
'with hexaethyldi-tin, giving triethyl tin oxide as a result of the
reactionsi.
(CHb)3 Sn6 + (CaNs SnSn (C&Hl,)& - (C%Hs)a SnOSn (CHa)a + (CsHs)s gn (7)
(C4Hg)jSh + (C&Ht), SnOOSn (Cj4,)j - (C4H,)& SnOSn (CHs)z + (C.IH&)& Sn6 (8)
((~,Hi)sSnO+(CH,),tn--(CH,)&SnOSn((:tHa)s (9)
2 (QHs)sS; (CHI)3 SnSn (C2Ha)s
-QO)
During the reaction of hexaethyl di-tin with oxygen,TETP may.be formed as
n intermediate which, dould not be proved because-of the high reactio'
n
rate. However# oxidation 18 accelerated by additions of TETP. The
methods of these experiments-were described before (V. A. 'Shushunov et al.,
Tr. po khim. i. khim. tekhnol., GorIkiy, 1959, -P- .329; Yu. A. Aleksandrov
et al., ibid., 1960, P. 351). The oxidation of hexaethyl di-tin is
accelerated either by TETP, or by the radicals forined during its transforma-
tion, but not by diethyl- and triethyl tin oxides. which are formed di3ring
this process. The reaction of TETP with hexaethyl di-tin ia accompanied by
.formation of radicals-which initiate oxidation'of hexaethyl di-tinAby.-
a
oxygen. There are 3 figurqs and 3,Soviet references.
Card 3/4

28
/0 7
s 2076611140100310131020
Triethyl tin peroxide B103/BlOl
.
ASSOCIATIONt 'Gorlkovskiy gosudars
tvennyy universitet im. V~ I. Loba6hevftgo
(Gor'kiy: .
St8tq.University,imeni N.. 1. Lobachevskiy)
PRESENTED: February 25, 1961, by B. A. Arbuzov, Acad'emician
SUBMITTEDs February 22, 1961
Caidt*