SCIENTIFIC ABSTRACT NOSKOV, D. G. - NOSKOV, M. M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001137320013-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 3, 2017
• Document Release Date: August 1, 2000
• Sequence Number: 13
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

10SIOT, D.G.m Aster domennogo teakha, Geroy Sotsialisticheakogo Truda,
All through life. Sov.profealuz7 26 no.5:10-12 Kr 140.
(KM 130)
1. Chusovs1dy, metallurgicheeldy simod,
(Chusovoy-Steel Industry-Labor productivity)

IJIDSKOVI F.11., assistent
Effect of variation in modulating-voltaCe amplitude on the
results of the measurement of distances with the SVV-1 geo-
dimeter using the null method. Izv. vys. ucheb. zav.; geod.
i aerof. no-4:27-39 16.~. (MITYL 18:2)
1. Novosibirskiy institut inzhenciov geodezii, aerofotos"yem-
ki i ka-,tografii. Pekomendovana kcfedroy fiziki i radiogeodezii.

2 2 002 5
Zq,92*101,1117) 3/154/61/000/002/001/001
D050113
AUTHOR; Noskov, F.P.p Assistant
TITLEj On the rotation of the plane of polarization in the lower
atmospheric layer
PERIODICAL: Izveatiya vysehikh uchebnykh zavedeniy, geodeziya i aerofoto-
s"yookat no. 2p 1961, 65-68
TEM The author examines whether there is a rotation of the plane of
polarization and a consequent'distortion in a heterogenous medium (air) of
a polarized light beam as used in geodimeters for covering given distances
twice, This problem is of practical intereatt because it may lead to cor-
rections for refraction* It shall be assumed that the direction of pro-
pagation of a plane-polarized beam AO in a first medium (with the refraction
index n1) forms the anglecp,'- with the outer normal ON to the boundary sur-
face in the poinf of incidence 0 of the beam (fig.1) and that in the second
medium (with the refraction index n2) the beam travels in the direction OB
forming an angle i with the inner normal ON'. The angle A r-4 -i appears
as a total refraction. It shall be further assumed (fig.2) that the angle
Card 1/6

22025
S/154/61/000/002/001/001
On the rotation of the plane uf polarization ... D051/D113
between the plane of oscillation of 'lie electric vector and the plane of
incidence of the beam is equal tt,() - In this case, the wave falling onto
the 'boundary surface can be conceived as the sum of two waves of identical
period with an identical initial phasev but wi+h a different amplitude and
different planes of oscillation of the electric vector, the vector of one
component wave oscillating in the plane of incidence of the beam and the
other in a plane perpendicular to the plane of incidence. The modulus of
the amplitude of the electric vector will be
for the first wave
for the second wave
E ME Cos
E -2 sin (2)
If the directions of both refracted waves are assumed to be coincidentp the
amplitudes of the waves beyond the boundary will change differently. Accord-
ing to Fresnel's formuleeg the amplitudes of the refracted waves Ef and El
are expressed through the amplitudes of the incident waves E and EP
p 8
Card 2/8

22Q5
3/154/61/000/002/001/001
On the rotation of the plans of polarization so@ D051/DI13
in the following way
Ef E 2 sin i cosoe,
;~o P sin(cc+ Q coo (4- 1)
Ef WE 2 sin i cooc/4
a sin(pC, + i)
These formulae show that? during the passage through the boundarys both
components of the wave lose part of their energy (due to reflection), but
in a different way# and, finallyt it results that the plane-polarized wave
changes the plane of polarization when passing through the boundary* Look-
ing at this phenomenon in greater detailt it can be seen that
in the second medium
EfPEI oosO
EI.WEI sinQ
Card 3/8

22025
S/154/61/000/002/001/001
On the rotation of the plane of polarization 000 D051/DI13
(01 - angle between the plane of refraction (and incidence) and the plane
of vector oscillation in the second medium.)e By substituting formulae (1)
and (4) in formula (3)# we obtain
Et Cos ~o = E cos ~2 sin i coqoC- (5)
sin(dL+ i) cos(cA.- i)
El sin@' = EsIn(9 2 sin i cosaG (6)
sin (cK, + i)
Dividing (6) by W we obtain:
tg tg ~ coo(o(-- i) tg 8 cos A r (7)
or
oos A r tg 0
tg
Equation (8) shows how strictly the refraction of the beam and the plane of
polarization depend on the passage of the beam through the boundary. The
total refraction A r of a beam in an atmospheric layer near the Earth's
Card 4/8

2201215
S/154J61/000/002/001/001
On the rotation of the plane of polarization #do D05l/Dll3
surface is L6 minutes at distance of 20 km between the points and a re-
fraction coefficient of 0-15. This means that cos&r will always be poo-
itive and its absolute value near to unity,, It also shows that the plane
of vector oscillation of a plane-polarized beam.always rotates towards the
plane of incidence of the beam (independent of the ratio of the refraction
indices) andt consequentlyp we always have the expressions
0 0
where A& (always positive) the angle of rotation of the plane of pola-
rization on the passing of the beam through the boundary. Since toth a r
and 60 are small valuesq we transform the expression (8) by expanding in
a series cos D6 r and tg 0 1 - tg(O _,66P) and limiting ourselves to the
initial terms of the expansion* After performing the necessary arithmetica
operations we obtains
(&r)2 4 G (9)
sin 2 a
In order to determine the order of the magnitude of the rotation of the
Card 5/8

22025
S/I 5Y61/000/002/00 1/0
On the rotation of the plane of polarization ... D051 D113 01
plane of polarization# we rearrange equation (9) in the following wayt
sin2 (10)
4
Converting radian measure into angular we obtain:
2
A sin2 r)
4 ?"
Let us assume that the refraction index of the air changes along the path
of the beam not steadily, as is actually the case, but suddenly at one par-
ticular point of the beam. Let us also assume that A r . 10811 (see above)
and sin 2 0=1. In that case
1. 17 -, 10 10- 0"*015.
4 4 2
In this way an analysis of tjie order of the magnitude ofAO shows that the
rotation of the plane of polarization in an air layer near the Earth's
Card 6/8

-1 1 ~
4A)I
9115 1 000/00,2/001/001
476
On the rotation of the plane of polarization .00 D051/"DI13
surface can be neglected. This also follows from an analysis of formula
Mo The study pernits the following conclucions to be drawnt *
lo The assumption that a plane-polarized '.)eavi travelling in an atmospheric
layer near the Earth's surface over distances up to 20 km is not exposed to
rotation of the plane of polerization, is gractically fully justified.
2o Porraula %I
shows that with the rotation of the plane of polarization
the distortion of the been can be determined and a correction for refraction
obtained.' It must be noted that the available devices for measuring the
angle of rotation of a plane of Dolarization are not sufficiently acourateo
2he best of them permit this angle to be deter:.-.ined only with an accuracy of
some tens of seoonds.. fAbstraoter's note: essentially complete trenslationlo
There are 2 figures and-1 Soviet-bloc reference. .j
A'~'SOCIATIOIT: *41avosibirskiy institut inzhenerov geodeziiq aerofotos"yemki i
kartagrafii (11ovosibirsk Institute of Lngineers of Geodesy,
Aerial Photography and Cartography),
~)UBI',ITTED: October 6, 1060
Card 7/8

N`,'i F 0 V F.".1 ... a~3'4 16 t#Ln-'-
(MITRA

MOSKOVO F.P.
Using the method of comparisons in measuring distances with the
SW-1 goodimeter. Geod. i kart. no.8:13-16 Ag 163., (KMA 16:9)
(aeodimeter)

ROSKOT. r.S.
SWficancs Of COUJanctlyal InfGatiou Of guinea pigs In the Identi-
fication of dye3ntery bacilli. Zhmr.mlk~oblol.epid.l I==. 30 n0.7:
124-125 J1 159. (KEn 12: 11)
(MIGV.L&)

Nosmo, F.S.
Ifis of Perfl2cay-Cmbe eapil2aries for the ster-UrAf -tion of
Aicrobe sups=ionx. ro. delo [7) na+41-43 Ap 161.
(KIFA 1493)
(UGT&UOU)Gr-TljcHNIQm)

GULYLMKIY,, R.A.; KOSKOV, F.S.
Possibility of using s=e nitrofuran preparations for emrgency pre~-
vention and treatmento of agpecisUy.dangerow infectiome Report
90.1t Effect of nitrefuran preparationo on the. vacaLml, straia,
F.pestis 116.1, ~7. Zhur.mikrobiol., apid., i 4=1 . 32 no,laiza~-
25 0 061. (HIRL 14CIO)
(FU~dfi) (PA.STEURUU, PESTIS)

BMWs F694
Nicrobe motility In plane-Varellel capillaries. Mrobiologiia,
31 no.6*IM2-1093 R-0 t62. WFA 16'3)
I., Tayokava)w ah&W 14,09743.
(UGTMIOr=-TEGHnqax) (UGTMI&-4WIIITT)

~UOSKOV. F.S.; BOLDASOV9 V.K.; GOLIDIN, R.B,; YM&KOV, N.V.; VOLKOVA, L.A.,
Contrast method of fmmu ofluoreacent dincovery of adanoviru4see
In the kidney cell culture of guinea pigs. Vop. virus. 10
no.5t6l3-614 8-0 165, (KUU 18M)
1. VWnno-meditsinakaya ordena lanina akadeniya imeni. S.M,
Kirova, Leningrad.

L -27116-66 MTM/T JX
ACC NRt AP6 04/005/0613/0614
004869 0) SOURCE CODE: UR/0402/65/0
AUTHOR: NoskQV-, Boldasov,_V, Xo; Gol I din Be Be; -yormkup
"IF "50
N. ve; Vol ON 0 Ls Ao 33
ORG: ftlit2a Medical Academy im. S. Me Kirov, Order of Lenin,
Leniu-rad (Voyennomeditsinskaya ardena Lenina.skademi
TITLE: Contrast medium for immunofluorescent detectio- of adenoviruses.
in c 11% of guinea p-17g,-Vi-dneys
a I oulturet
SOURCE: Voprosy virusologii, no, 5, 1965, 613-614
TOPIC TAGS., virus disease, animal diseaeo, experiment animal,, boat
ABSTRACT: Bovine serum albumin labeled with sulforbodamine B fluoride
was tested as a contrast mediun for adeovirus t-YPe 4 infected guinea
piE kidney cells stained with I'luorescein. The infected cells wera
exposed to the specific rabbit imm-une globulin, then added with
fl~orescein isotbiocyanate at eil rate of.10 mg fluorocbrome per 1 g
protein. The phosphate buffered serum albumin was first-conjugated
with freably synthesized sulforboderine B fluoride in an alkaline
medium, then purified, Th.e fixated adenovirus preparations were treated

L27116-66
ACC NRi AP6004869
with the mixture of conjugates J'or 20 minutesp than studied under the
luminescent microscope, *Normal cells were brick red., the protoplasm
lighter than the nucleus; the infected nuclei bad a specific green
color with bright green sparkliug enclosures$ Upcn single step
processing of the preparations,'tbe specific interaction of virus
antigen-antibody was not inbibil',ed by the presence of the labeled
albumin, The pbysicochemical absorption of labeled albumin on cells
led to nonspecific staining of ;be backgroud (cells containing' no virus
antibodies) wbicb did not depret3s specific fluorescence Tb',.s method
.al.so permits the detection of single infected cells, Ns use is
recommended. "The sulforbodamine B fluoride was placed at our disposal
I
by Prof, 1, S. loffe whom we wish to thank for his courtesytlo Orig,
iart. has: none* .
SUB CODE: 06/ SUBM DATE: 26Ncv64/ OTH REF: 006
-4 2/2

NOSKOVP G.A.
I ~ -a ~- -: ~, ,. I
Use of decoy birds in ornithological f-,eld studies. Vezt. Uj-
20 no.3:14"t-150 165. (:,lI*.-,It IP:2)

ROOM, ,-.
ftse.1bilitios for the ImproTiment of contraligod control.
Ilske sta, 30 ne.3:49-51 Kr 159. (MM 22 c 5)
(IlectrIc power-plants)

KOSK070 G.S.; CHERKYAKOV' G.S.
9
Raise road design to the I#vel of modern problems. Avt.dor. 26
no.4slo-3 Ap 163. (Etoad"esign) II (KlR)L'l6t4)

HOSKOV9 I,g podpolkovnik
Lomder of a taak gtw. Voen, snan. 40 no.6t13 JT6 064.
(MIRA 1717)

MOSKOVO I., podpolkovnik
------
Succosses don't come aaay. Komm. Vooruzh. Sil 46 no,4:66-70
F 165. (MIRA 18: 5)

__-ff! podpolkovnik
The gas scout. Voen. zman. 41 no.4:11 Ap
O"TRA, -?: 3

110SKOV T rod- -,1kov-r
Jk
, 1. ,
Seeing, but, unseen. Voen- znan. 41 no.9:12-13 S '65. (KIRA 18: 10)
I
I
I
I
N,

- NOSKOVI I.0 podpolkovnik
Without a miss. Vaen.-znan. 41 no.32:12-13 D 165.
(MIRA 18:12)

1,'OSKOVP I.s podpolkovnik
Tankmen conduct accurate fire. Kom. Vooruzh. Sil 46
no.20:53-55 0 165. (MIRA 18:12)

AUTHOR: Hookov, I. A.. Engineer 105-58-6-9/33
TITLEi On the Determination of Torques of Turbine Generators
During Nonsynchronous 4eration (K opredeleniyu velichiny
momentov pri nesinkhronnom vklyuchenii turbogeneratorov)
PERIODICLLs Elektrichestvo; 1958, Nr 6, PP. 36-38 (USSR)
ABSTRLCTs With asynchronous connecting of the generator, the maximum
instantaneous value of the electromagnetic moment will de-
pend on a series of factors. It is attempted here to ob-
tain a simple formula for the moment which takes account
of all these factors, or at least of those which do not
introduce any essential error. Such a formula can be ob-
tained with sufficient accuracy from equation (1) expres-
sed in relative unities. The amount of the moment with
asynchronous connection - formula (2) can be obtained by
taking account of all factors enumerated here (initial
phase-angle-error, - difference between the EMK of the
generator 3 and the line voltage U, amount of the effec-
tive resistances in the stator-circuit and the amount of
Card 1/4 the initial slip), - as well as of the attenuation of the

On thaL.Determ1nation of Torqaes of Tuxtine Generators 105 -58-6 -9/33
DuAng Sonsynchronoug; Operation
aperiodical stator-current component. Formula (2) does not
take account of the rotor-asymmetry. The analysis of the
formula for the moment with asynchronous connecting which
takes account of the rotor-asyametry shows that even with
the minimum admissible external reaotancea, the error does
not exceed 5% in case of not taking account of the rotor-
-asymmetry. The investigation of the influence of indivi-
dual factors on the maximum value of the moment shows that
in the practically interesting cases where the amount of
slip is within the range of from zero to lo%, the influence
of the slip must not be taken into consideration. Formula
(2) is simplified by this to formula (3). The amount of the
effective resistances in the otator-eircuit or the value
of the angle 9 exercizes an essential influence. Inventi.-
gating (2), the angle corresponding to the maximum-valu,!-
of the moment can bo found. It is pointed out that a change
of the generator-EMK influences the amount of the monent
much more than the change of the line-voltage. The analysis
Card 2/4 of (2) and (3) for the power delivered b,-, the generator

On the Detemination of Tortues of Turbine Generators 105-564 -9/303
DvxIng 11onsydochronous Operation
under different syi..,,motric asynchronous connections and
the comparison of the same with the formulae (2) and (8)
from reference IC, ohow the following: 1) The maximum
occurs at an initial phase-angle-error of 8oc - 12o to 1350-
2) The amount of admissible amperage with asynchronous
connecting determined from the condition of the extreme
moment in comparison with the nominal amounts to from
6 9 to 6, 4. The amount of the minimum admissible exter-
nal reactances ie within the range of (19 58 to i, 6e)X"
dg
in dependence on the impedance-angle. 3) Disregarding of
the values a (alip), T (angle of the full resistance) and
k (ratio of the line-voltage-values to the generator-e.m.f.)
in the formulae for the moment leads in the most unfavorable
case to an error of from 15 to 2o% in direction of the un-
derrated calculation-value. 4) Disregarding of the attenua-
tion of the aperiodic stator-current component leads to an
error of the same order in direction of an overrating of
Card 314 the moment- 5) The formulae recommended in reference 1,

On the Determination of T orques Turbine Oenemtore 105-56-6-9/33
During Nonsluchronous Operation
ASSOCILTIONt
SUBMITTED:
which takes account of the asymmetry of both the longitu-
dinal- and transversal axis according to the machine is
inadequate with turbogenerators on account of the compli-
cated calculation-formulae. 6) formula (3) is recommended
for technical calculations of the moment with asynchronous
connecting of the turbogenerators- 7) The simplified for-
mulae by Kir3hbaum-Luter can be recommended for the appro-
rimated calculation (Reference 1).
There are 3 figures and 2 references, 1 of which is Soviet.
Llvovskiy politekhnicheakiy institut
(Lfvov Polytechnics! Institute)
July 5, 1957
1. Generators--Performance 2. Torquq-'-Measurenent 3. Mathe-
matics
Card 4/4

NCSF,GV, 1. 0'-'%
Noskov, I. G. "A case of Asiatic lacusts flying to the Kzyl-KuL-a sands," Doklandy
A-kad. nauk UzSb-R,, 1948, No. 12, P. 34-35
SO: U-3566jaViarch 53 (Letopis 'Zhurnal Inykh "tatey, No. 14, 1949).

USPENSKIY, F.H., kind. biol. nauk; SOKOV, I.A.; RUMINOV,, A.Ks,
kand. sellkhoz.-nauk; IVILKOV, nauk;
VASILIYEVp I.A.9 kx4d. sellkhoz. nauk;-SOWV'1ZVAO A.I.P
kand. sellkhos, nauk; ZAPROMMV, N.G.-, doktor sellkboz.
nauk; YAKMNMV,.V.V., doktor biol nauk; KMSTIMA, R.I.;
STROM, M.G.;,POLZVSHCHIKOVA, V.N.; kand. ~~"llkhoz. nauk;
KARIMVt N.A.,, daktar biol. naukkf"7 TIG, kand. sell-
khoz. nauk; KHODZHALM, A.M.; ALF-1KV,_B.Z._;-,Tca_nd. sallkhoz.
nauk; YAKHORTOV,, V.V., doktor biol. n&uk;.STZPLKOV, F.A.;
LYUEETSKIY, Kh.Z.j, kind. med. nauki GUMVICH, B.E.;
KONDRATIYF,Vv V.I.; SUDARS, L.P.; KOSTMG, I.R., zaal. agr.
Usbekskoy SSR; GORELIK, I.M., red.; RAMIYAROV, A., tekhn.
red.
[V_nnual on controlling the pests, diseases and weeds of cot-
ton, earn, and legumes] Spravochnlk po, bo~lbe a vreditaUktd
i bolesniani khlopchataika, kukuruzy L bobovykh kulstur, Mz~2*p
parer. I dop. Tashkent, Gos.lzd-vo UzMp 1963. 325 P.
(MIRA 16:5)
(Field crops-Diseases dad pests)
(Weed control)

NOSKOV I G inzh
Sialne #looms for electrode covering. Swar. pralar. w.g.-27
Ag 162. (KERA 15M)
1. Urallskiy savod khimicneakago mashinostroyeaiya.
(Electrodes)

xomv~, I.G.
Eully pulverlsed C.Pl. ejuays an hard facing zatarWs. jvton. ayar.
16 no,4:71-72 Ap -*&j. WA 16-4)
lo Urallskly savod khImIcheakogo mashinastroysaiya,
(Ketal powders) (Flux (Notallur"D

NCSKOVO I.G.
Using complex alloys in electrode coatings in place of iroa powdtr
Lvtom. avar. 17 no.3:76-79 Kr 164. (MIRA 17:11)
1. Urallskiy savod tyushelogo khImichaskogo mashinastroyeniya.

kandaellskokhozn=k' (Tashkent); PONOMARENKO, O.Yao;
ZMIVIDGROU, S.P.; ZAKEUVIDOROGA, Z.S.; LIPSITS, D.T.;
LIEUBOVSKAYA, P.I.; POLOTAft. V.A.; TARAMOVSKIT, X.L.;
FASTOVSKIYp V.L.
14tters to the editor. Zeshch. rast. ot vred. I bol. 6
no*8:10 Ag 161. (KIRA 15t12)
lo I/sesoymaya otaatsiya po raku kartofelya Vsesoyuznogo
iwtituta zashchity rasteniy i Chernovitakiy meditainakiy
institut.
(Plants, Protection of)
(Synchytrima--Toxicology)

110icallovo V6 Ff
2. U9SR (600)
4. Arctic Regions - Forests eM Forestry
7. More complete utilization of timber resourses of the arctic regions. Les. khoz. 6,
no* 19 1947.
9. 'Monthly List of Russian Accessions. LibrM of Congress. -1953. Unclassified.

% M11, 1. P.; YOLM"A4"OV, 7- F.
ME
Foro~~ts and Foror;rj - Arcl'~-'c Ii--I!xis
NO. 1
yor-:3 co:npjeto ut-Mizalt,ion of re'.jurcr,.i of ',* - L,.-;. :L .;Z. 6, 1.
1953-
9. Konthly List of Russian Accessions* Library of Congress, :ay .1953. Unclassified.

YMKOVR L.
Use the example of beat practice to train. Sov. profmoiuzy 19 MQ.7:
20 AP 163- (MPA 16--4)
1. Starshiy instruktor organizatsionnogo otdela Bryanskogo oblastnogo
soveta professionallnykh soyuzov,
(Bryanak-Trade unions)

ACC Wo
-4 SOU
INVE14TOR: Sheynin I. S.; Kaskov, L.
ORC: none
TITLE: A method r determining the
and concrete In b11 Idifig structures..
ul
Izobreteniya,
C UM
D.
breaking'of the bond between reinforcement
Class 42, No. 188744
promyshlennyye obraztey, tovarn"e zaaki, no. 22, 1966, 118
SOURCE:
TOPIC TAGS: reinf d concrete, concrete, structurai engineering,,structure
',~rce
stabilit adlv w(; Afcav&lry
Y
"STRACT: An Author Certificate has been issued for a me;hod for determining the
breaking of the bold between reinforcement and concrete in building structures by
using seas'qrs t gister the acoustic impulse originating in the broken-bond area
between the rel caw=4' and concrete. To determine the location of this area,
the difference in he son'Ic-wave travel of the acoustic impulse to pickups located
I
on'opposite aid" the test structure Is measureds
SUB 00M 136 14/ LK D=t 11 BepW
Gwd I/L VDGt 666,9M693,554:62O.M.2-666.6

Nosko' V, L. N.
"Contact-free magnetic re-gristration and rarwoduction." Ilin
C6mmunications USSR. Yoscow :Uectrical Enfjne-2ring I~~st of C6mmunications.
I scow, 1956. (Dissertation for the Dc~ree of Candidate in
Technical Sciences)
KnizL~&-a letopis,
No. 25, 1956. Poscow

1. au=m, G.; MOSKOV, M.
2, IISM (600)
4- Gottou Growing
7. Chief tasks of cotton workers.
Khlopkovodstvo no. 9, 1952
9. Konthly List of Russian Accessions, Library of Congress, -JuuArT 1953. Unclassified.

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when
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act&
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Cr
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Z== CIO
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t
tram pec cc. The rtee decfx-
10-Pew-aud
ko-P, LO 0,
tim at rwo acd

Age,
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*
1
moo
ASS.&LA 419TALLONSCAL LITC94TWW CLASWCAtWO
No $1"ECATO gas
141462 NAP Ong 404 4 ass A Ido -- 4.0 's,-
6 N, t I t . I . r . * " I- - ir a 9 a d- j -4-79
It It PC K a
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Nature 131, 725s 1933

__ . - _==_ - - - oi,
1~ 16 1' U K AL It It It p 40
L4 M Ow it 1 40
-40
A moroor pk*Uwf*ct* t1roct ilk
am* Ko-
L.4u acki
LUJI-A thin pUtc 44 CuLgo
In "tgro, w4, pli~l 1~1 ww" I foo,
00 j-1, s t4 an ckwittastagnct APAJ One %kh 4(jUfU(UAtC4l, I 11T
Ap.d. wits 6wit4f wah mad-
toe ficki 1-"t alwnt withut lbe fi.M. ATkI at-cut at
fwfm trouts. Only Uilht atwxlwd toy Ifw CUA) was cece.
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HOSKOVO M. m.
Thermoelectric and Galvanomagnetic Properties of Semiconductors.
Leningrad Physica-Technical Institute,, 1936.
SO: U-18379 24 April 52.

N()SKOVV H. M.
Frall's Effect in Nickel ffigher than Curiefs Point. Sow. E*s- SP, is, 1936.

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into It", ~vv
jDaLAU11f) Mad. &S. U.Abk., Wit, U.
60)--4Eu Ell lish.) Films of cellu&)go, Pakt-jito, or liquid oil somo tenths of
& , ttdck stpplied tolhe surfse" of nickel, Permaltov, or iron tpecimwx multi-
,I'd th" Magnet(. wip. Jreq Woe or 1-3 ti - The incteam d-lj,-ndcd
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NOSKOV, K.M.
USSi 7505.
"On the Iafluence of Thin Films upoa the Magne-to-optical Kerr Effect" published in
Comptes Rendits (Doklady) Vol. LIII, No. 5, dtd 1946.
SO: INOW-B-2293, 17 March 1948 446581
'Awleft FHES

NOTA)ea IqkT
FerrccagaatiA~m
Kagmetic Yields
**gaeto-Optio Methods of Studving Forrawgastic
Ancqe,w X. X. Nookor, lust ftjs of VAtaas, Vral Br,
Ana& Sal UM,
rly Ak~A Nauk SMj Ser Fie Vol XII No 6
DI"OuSfes Laluence of magastic fIeIA m distribu-
tiam of II&t In substan a.
=86

9f cocnim..
Effect of the thickhen and the 0 1 sun V of
thin dieleC(9 LIM ort the ft Wit .,r q, P
L. M- Al- Nb4U_j-. Zhur. "Itil. 1-forel. Fox. L7. IRK-K
(10-ur---We tLtlge Of rotd(fort ,r of the plane of ofariza-
b tibn on refice(ion 9 filtered polarized light lue. C en~
Yellow. PtA red) from a ferromagnetle surfa (St c . Ni
or CO) i!q altered by thin films of stot, Ca 1. " . f:I
C":O, I fgS, Nfc6r, PbS, and TlOt, rodu by c a tt.,
ot hy filtni of the oxides of the meta , FctOr. NiCP, CoO
Lgw With I=
tirmlactA by gnmrficfat - ox wig reasin~
thiclkne-S of the Wtute-4haptli tum, the relative M/as
angle without fitttt) varies Periodical1r, PaSsinc from
an lCmay: (cctas > 1) (a a detemse (mlet < 11. and (ftcd
j inctcasing again. The shape of the curve of a giv(:n di-
ek-tric varies with; the color. In contrast to transparcrit
filins, ab-orbing oxides give rise, at a certain thicktic,%.
to a revl~rsat of the rotation (alas < 01. The normal
cffcct t1king place with a tramparent film is safisfacturily
zwcountrd for by the theory of Frrnkel (C.A. 3T. 42834).
which attributes it tos Interfem-n-t-e-W-Mri the film. and
givcs, f(w the total angle of rotation. cE - att(t - r"181
r, - 2r Cos 2ka). where r - -(it - 1)1(tc + 1) (tc
raractive index). k - 2r/k. a - thicirnm. and all i- the
change of the angle of rotation between the frcmt and the
back Of Me filat (film/mew boundaryh due (a the mac-
netiratiott of the metal. Absorption within the film
r(Linces the ratio of amptitudesq - A IB of the ellintic
P40yarit-70101. At $mall OU, the (Utal 2nille of rotition in
Me 'presence of absorptloet Is a w an(L + I cos &VRI +
11 Cos 6), + (iv sin &)Ili :where the phase diffiselacc A
2k.2 - V, with jo - phase Jump an reflection at the metal/-
filin lxluttdary. Net. values of tv arise If v > I. and cm & i
-1. This point of view Is bcKneouttryexpts. in which 1
a stmi Fample with an oxide layer, and a sawgly rict.
citect, shavred the TIOC"Tal MS. dt1d periodic M When CoVer,!(l
-bytnacfdnl.wedite-ifttpetiSiO~fitfft. 0a the other hand.
with a steel + SiO~ film sample, with a norsnAl pos. a,
ClkltinC With an addrd. At film pive rtse to the anomalous
ticir. effect. In, the Ist vaic. the addlat. fill, tesutted itt
n - i I
it 4ricrrase of V, in the 2n,1 cAie, fit I(% decrrav. Tlh"#-
Phenotnena con-ititute a not commonly cousidercd in-
stance of itittdcrence of 2 way" with M(arita ion ftAnes
slightly rotatcd relative to each othex. Ir. it H.
Noikov and A. V. Sokolov.
Md. Nq-75.-The fore-
going concfu%7_n_s_r"eZTi_v=o e effect of nb$MptiOn Within
the. film on a/as. are e0ablished rigo~ousfy by nuth.
aualysir, m-Aulting in a general formula, that extends
Frcnkei*s original thcory for tmn4partnt fitntc. and criates
cc with it. k, a, and the absorption coe(r. c. For films of
celluloid. SW4. or ZnS ott Ocel. of ZnS an Ni. and of cart
OR Co. the calLd. a/a* at the mzx. and at the wiff. ate irt.~
fair agreement with the cxptt. values. For af*orhinr
is a satisfactpcy qu;.t. agreement.
N. Thon

:105i:07, !.,,. z.
"Magnetooptical Properties of FerroaxWnetic ~!atnls and heir Modification Under the
Influence of Nonmetallic Films." Thesis for degree of Dr. Physiconathematical Sci.
Sub 28 Jun 49, Physicq Inst Iment P. It. Lebwlev, Ac.-id Scl USSR.
Summry 82, 18 Dee 52, Dj,4nArttgHnr,- Preqnnted ?nr DpgrfZpa 4n SniF%nrp. jnj ErginApring in
Magname in 1242. From Ver-harryayr. L'acloca, Jan-Dee 1949.

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to 4 bmIdiscartim of the c9ft4ma b"d "em k8 Ac.
S. Pti'swer

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AA AA
A-
v -V-~
TRUDY IMTI=A rIZIXI- METALLOV AM. NAUX. URAIZFII;FTLIAL, 195h, 170- 15 ~j
C-n the relation botiraer. 6e Intonafty of mgmetisatio.n-4nd magnet -op ical ro lAtion
.1 - -' ' Y-~I N o
.,~,~rr -effect) in nickel and ita a1113 -a with cop~~e7r'%) iikov P. 67-59) -
The effetto of t re variation (00 - 4000ZI)-aj)d compogiti6i; (100 to 73.7% Ni)
nn flin miffn4flirIn nf fha Vorr Pffect are experimental1v investirnted. The reaulta

I I ___ I--- _aU A ^1 -4 1 n#nrn t,+i nrt rind a ~_prn"n P12
V_ Yonno-ValLit 4M A. V,;--WSQlOV
USSR/Physics Metallurgy
Card 1/1 Pub. 43 - Z1/97
Authors 'I Noskov, M. IA., and Skornyakov, G. P.
Title .1 About certain characteristics of an arc discharge cloud
Izv. AN SSSR. Ser. fiz. 18/2, page 257, Mar-Apr 1954
The effect of a falso electrode on the relative line intensity of a basic arc
electrode material and upon the sensitivity and accuracy of a spectral
analysis was investigated. The intensity distribution of individual lines was
investigated along an arc cloud in the case of uniform Cu eloctrodes and in
cases where one of the electrodes was made of C, Al, Mg, Zn, Fe, Me, Ni
and W. It was found that in the case where the arc bi;~rns between Cu-
electrodes there is a'distinctly expressed near-electrode int ensili cation of
the Cu line and a less distinctly expressed intensification of other Unes. In
the case where on(, of the above mentioned elements serves as'an anode,
the emission of Cu (cathode) is concentrated mostly at the Cu electrode
which also serves an a cathode. No Cu emission was seen near the anode.
Institution Academy of Sciences USSR, iJral Branch, Physics of Metals Institute
Submitted ............

AIPARSITZTA. L.A.; NOSMY. K.K.; CHMVAMY. T',I-
.................
A new xistfud, aperipheral lzteraectlW , for optical coxxtaat determination
la metals. Iris.inst. I netalloved. 1 soe3:566 155. (Kou 9:6)
I.Urallskly getudaretvannyr ualversitat imeal AA.GorIkoge.
(Ketals-Optical properties) (Optical measurements)

!V I-,- -1 1 T- I
Category ; USSR/Wacs - fty~.tica:. (Ptlea K-5
Abs Jour :Ref Zhur - Flzika, W. 1, 1957 1j,:. 23o4
Author :Domonskiy, E.I., N.,ek-,v H.M.
inst :Urall State
Title :Determinatloa of the Opt-*cal of Metals, Usizg the Autocollimation
Metho4
Orig Pub Fiz. metall,7,v I metalloveler-1ye., 1955, 1, No 3, 567
Abstract The autocolli tion fftethl (O'Bryar~ H.M., J. Opt. Scc. America *, i9.36, 26, 122)
is used in the ir~fraxel regioL.. Idght Is reflected from the specimer. twice in
the forward path azA 1y. the retura path, and passes twice through the same Se
polarizer, which is sirwly rztated by a.:~. electric motor. A recording infrared
spectrometer automatically reccrIs the intensity, the mil.im';M 4eviatlon of
which is used tc fill the prir-cipa I az!jwath 'k 0 ar-A the py.-Vicipal aQ:1a of in-
cidence f with a probable error of -~- 35' fcr P, and * as 151 for ~O 0 in
each indiv?dual measurement. The opt*fcal constla-a?s of Fmirroro obtaIndd by
evaggration of 3b, Cu, Ag, Al, and ZrA In vacuum were measured for ,\ 2.4c;
Card 1/1

UOSKOT.H.K.
Relation between
nickel aad in its
57-59 '55.
(Nickel-copper
magnstizability and magnstooptteal rotation in
copper alloys. Trudy last. f1c. net. no-152
OCRL 8: 6)
alloys-41agnetto properties)

FD-3190
USSR/Physics Interferometry
Card 1/1 Pub'. i53-20/21
Authors : Noskov,, 14. A. and Yasinetskiy, A. 1.
Title : Measurement of striction phenomena with the aid of a three-alit interfero-
meter
Periodical: Zhur. tekh. fiz., 25, No 8 (August)v 1955, 1518-1519
Abstract : The authors discuss the measurement of the dimensions of solid bodies during
magnetic and electric striction,, during thermal expansion, elastic deforma-
tion and when subjected to a load. They outline existing methods of measure-
ment aad describe a new three-slit interferometer which is specifically de-
signed to permit accurate measurements in the most difficult range, na 1y
from 30 Angstrom units to 1 micron. The physical and optical characteristics
of the new interferameter are outlined in detail.
Submitted : January 4, 1955

Category : USSR/Optics - Physical optics K-5
Abe JO~r :Ref Zhur - Fizika, 11-D 1, 1957, lk- 2303
Author :Afawslyevap L.A., lt.~skov, M.M., Cherepa"mov, V.I.
last :Ural' State University, USSR
Title :New "intersectiag-Circle" Meth~d f~%r the Determination of the Optical con-
stants of Metals
Orig Pub :Piz. metallov i meta.11ovedenlye, 1956,, 1, No 3,, 566
Abstract :Description of a variaat of a method of measuring the optical constants of
metals using the reflectioa of pdarlted Infrared 11ght. A recording nono-
chr,omator is used to determine the value of F (the ratio of the ability of the
specimerr to reflect light para-II&I to the plane of Incidence to the reflecting
ability for the perpendicularly-polaxized light), at least for two jangles of
incidence. To'ftml the optical constants, tha authors propose an aRproxInate
method based on a graphic solution of the system (x xi)2 +. y2 . R hi
sults from the-Fresnel equations for metal. Here w ch re-
(xV
andf I is the aagle of inciderace (I - 1, 2). The abscissas of the intersection
points of two circles vith radii Ri and R2 yield the Yalu 8 of the index of
refraction n, and the ordinates yield-the absorption coeflicient k. The method
was tested with B1, Sb, and their alloys in the range of A frod,2 to' 1~1* -
Caxd 1/1

LUMV, A.S.; NDSKOIT, .
Magentooptical Xerr effect and the structure of surface layer
of mechanically polished metal. 1xv. vys. ucheb. zam.; fit,
w.3'.76-81 158. (ERA 11t9)
1. Urallskir gasuniversitst im"d A.M. Gor'kago.
(Yetallography) (ftnatooptles)

,SEMMTMV. Tu.A.; MOSKOV, 9.K.
Photoelectric method for registering the contours of spectrun
lines In a d.c. arc, IrIzeabor. no.4:1&9-190 158.
(klEtk 12:5)
1. Ural'skiy gosudarstvennyy universitet Iment A.M.Gorlkogo.
(41metrophotometry)

51- 4 -~-15/30
AUTHORS: -,-d 110skoy, LIX.
TITLE: h1agneto-Opt'i,.'al Rctation in Alloys of Nickel with
Pal'-'a d1lira. (MaU~Ptoopticheskoje vrashcheniye v
spla-;akh nikzr~ly,,~. s palladiyeu.)
Vol.T'V, r.
PERIODICAL: Optika i Spektroskopi37a, 1958,
pp -3?8-38-1 (USSR)
ABSTRACT: The present paper reports measurements on the magneto-
optical Kerr effect (rotation of the plane of polariz-
atior, o-P li0it on i:-aflertion by ferzomagnet-'cs). This
effect is dug to a diffferer.,-.e in the degreee of damping
:Lnside. a uagnLettz,~d ferroma[~metic of electrowtgnetic
wave2 polarizcd in two mutually perpgndicular directions.
Nicke 1--palladium alloys were. studied. These two metals
fom a ;ontiv~rjs Oeries -.-)f solid solutio-.=: in which the
mean Oistance bet-ween atoms :. uniftrmly with
in,reavF~ Pd . T,Le Llawpies were fn the form
r,f d1ska vr-th from 0 tc 50 %%t- c m i -,. c,-,, c f Pd. Uniformity
of the. .9anpleq was by X-rqZ~ anal f31.~i of their
St lu ~~t U 1xi F-;~.rr.-,iLagnetic Chirte point;o Mg,3) of the
4-0
samples were found to ds;,-,-vease Morow ni,-,-a-lly with
Card 1 A In,irease of Pd, --~r-teLt. Nl-~rr-r ~3-a~rfa-~es on i~amples

51- '; -./--5/30
Magneto-Optical Rotation iL Alloys 2f Ni,:~kel with Palladian.
were prepared by mechani-,al pz)lish~n-. Llie apparatus
used is shovr-. in Y;P,.l~ An I-eland spar -_rystal was
used to separate the T9flectod light int-- twr. mutually
perpendJc-alarly polarj.zed beams. .ha 1-1~1.ti_,_~ of the
relative intensities of these two beams altered by
the Kerr effect had ite original value re-established by
a rotation of the plane of pclarization by means of a
cell filled with distilled water and placed inside a
solenoid. Current- in the solencid. was proportional.
to the measured Kerr rotation. Re-estlablishment of
the oriGinal va-lue of the intenalt .), ratio Wao observed
by balancing a photoele,tri3 bridge with a quadrant
electrometer as a null indicat-or. A me=ury lamp
was used as the sour,_-e. The results cf photoelectric
measureaents were. partly -1hecked visnall-y. All
measurements were made at- r:cm temperature. The
cpti--al eonstants of gamplee were deten2ined by B.Ya.
Silant I e-.r. Measurements of the depender-ce Cf the Kerr
effect = the alloy ocaposizion (FiS.2) were made in
a magnetise fl .eld of 8000 oe-r-cted iT, whi.-:I-L, in all cases,
Card 2/4 magneti- saturation. was xea,~hed az)d a value of

-0
V
;
jj U,
Magneto-Optiral Rotation in A113ys of I'lickc , P 1
vith al adi. a.
the angle of rotation a was obtained. At. 50-65,'~
Pd the Kerr effect -~,,arleg slowly with -~he alloy"
composition, but on both sides of this mgiou the Kerr
effect depends strongly on the aaount of Pd in the alloy.
Vailae.3 of the saturation magnet izat ion I., ar-,4 given
in Fig..3. These MD-ies wer-3 used tc, ;alt"ulate the Kerr
constant R = cL /I The dashed cur~7e in Fig-3 gives
the -raluee of I which is the sat-uration magneti-
!301
zation, iedu,ed t-I the absolute zero of temperature.
The third riix-ve in Fig.3 gives the dependence of the
Curie point on the 'a C ontent. Fig.4 shows the
dependenre of the cpt!.,:a1 constants of NJ---Pd alloys
C.OMp'._, 84 ton.
on their The
strong depender.._-e of the
magneto..7~pti-.a] K~-rr effect on the Pd -;oncent ration
seems t,) th- ,',:mstar.--_-.y ;I,f the ac, omi-;
magnetj.,~i moment and c~f Optic.91 --c.-istaut'a cf !II-.Pd
alloy_q when the Pd The-
_Dtf-~Iit is t he or-y
GL,!r~n :Lu Ref.1 d,-,A.,3 xi~', Scl*ie this pr,--bably
becallse (,f rissi)mption2 (~n %i?h--'-h tids theory
Card 3/4 is baL3ed. "4,.-.
th,---3 thno- i-s appli -able to

L !a gn,.- t o - Op t i - a 1 Ro t a t 'A. o n in A-' .1. o y F o f I T i ~; ko, I lu i t, h P1 a
pure raeta'-.zi and :~-ot allcy3. A tentative
exDlanation of tho, dep~~ndence o-11' th,~ K,,,ri, conotant R
Onthe Fd ccnt,:-n.t 4n Nj-Pd , i; in the
alloya is zough
dependence of R on the reiati,.ra '~: ion
Y = whi~3h 'Lails with ir-3re-ise of Pd in the
alloy2. In a separate experizent t'-qf,- authors folmd
that annealing in all- atuc,3phere of hydrorem (both
Ni and Pd c-= absorb large qjuan~tities of hydrogen)
at 7000C affested 3trongI7 the Kerr ancle of rctation
in Ni-Pd alloys with 20, 50 and 57 af,omic "'. of Pd
(Fig-5). The effe-44- of hydrj,-,-,,n is re-,ersible;
0- ~
annealinr,, in -vacuum at 9C )C re-establ-i3hed -,he original
values of the Karr ar-~~la of roltation. 2,-iere are. 5
fJL-mares and 7 reforence-s, of which 4 are '--'-Vviet, 1 German,
-1 French and I AnerlIcan.
ASW-CTATIOIT: Ural State Uni-,,-orFity,
(Urallskiy Gos%tdu::,stvennyy uzilversit,,,t, G. Sverdlovsk.)
SUBUIT'L,'D: June 3, 1957.
Card 4/4
1. Nickel-p*Uadium allM--Refleatlys zffeat.4 2. Magnete-optic
rotation

SOV/137-59-3-6548
Translation from: Referativnyy zhurnal. Metallurgiya, 1959, Nr 3, p 229 'USSR)
AUTHOR: Nookov, M. M.
----------
TITLE: Substitutes for Nonferrous Metals (Zameniteli tsvetnykh metallov)
PERIODICAL: Zhrd. ~ transport, 1958, Nr 6, pp 87-88
ABSTRACT- The T9AM9- I.S alloy consisting of Zn with 8- 1014 A], 1-211o Cu: and
0.03-0.0616 Mg,'has a low melting point 0950C), exhibits good
plastic characteristics, lends itself readily to machining, rolling, or
press forming, and possesses antifrictional properties comparable
to those of bronzes and babbitts. Performance tests on floating bush-
ings manufactured of the T9AM9- 1-1) alloy are progressing satisfac-
torily under actual operational conditions in locomotives of the
series L, SO, FD, and IS. For purposes of increasing their
fatigue strength, the threp-layer floating bushings have a steel
casing.
Card 1/1

ZIL. gooo 65707
sov/139-59-2-6/30
AUTHORSt Zverers LePas Moskovg K.M. and Shur, M.Ya.
TITLEt The Effects of an Ele.ctric rield on the Spectral Response
Curve for Photoconductivity in Cuprous Oxide
PERIODICAL.- Izvestiya vyxshikh uchebnykh zavedenty, Fizika, 19391,
Kr 2. pp 3~42 (USSR)
ABSTRACT: Polycrystalline Cu2O is,used at 710X in this work.
The
spectral response is examined at high dispersion
(6 /mm) with a grating spectrograph. and the absorption
,
spectra are also recorded. Only two field stran~ths
(300 and 6000 V/cm) are used. Fig I shows spectral
response curves (uncorrected 'for the energy distribution
in the exciting spectrum); the wavelength scale is in atik;
rig 2 shows a small region at higher resolution. Fig 3
shows the effect of the field for one specimen; curve I
relates to 300 Y/cm and curve 11 to 6000 Ylcm. The first
exciton line occurs in absorption at 612-53 mg but it can
be detected only in thick specimens; it is not seen in
Fig 4b. (Fig 4a is merely rig 5 on a larger scale.)
Figure 4c is at the top right and relates to 6000 V/cm;
Fig 4b is at the bottom right (300 V/cm)~ The 3econd and
Card 1/2 third exciton lines lie at 579.2 and 575.6 mo respectively
C

67 731
00 L;0V/12C"-7-3-40/44
AUTHORS: Zhuravloya, L. I and Noskov., Lt. M.
TITLE: On the Method of Measuring Qptical Constants of 1,11etals
(K metodike izmereniya opticheskikh konstant metallcv)
PERIODICAL: Fizika metallov i metallovedeniyel 1,959, Vol 7. Nr 3,
pp 475-476 (USSR)
ABSTRACT: A high-precision variant of the polarimetric method of
measurin optical constants of metals was described
earlier Nef 1). Later this variant was improved and
used to study invisible surface layers on metals. The
latter application is described in the present paper.
A monochromatic lidat beam passed through two mechanically
coupled polaroids. The polaroids were replaced by
selenium polarizers for measurements in the infrared
region. Four mirrcrs made of the metal investigated mre
placed between the polaroido in suoh a way that light
was reflected from each of th~, mirrors a8 the same
angle, whose value was between 45 and 80 . To determine
the reduced polarization azimuth V and the phase difference
A between the polarized components (* and A are necessary
to calculate the optical constants), it is sufficient to
Card 1/3 carry out measurements at one'value of this reflection

IJ
S)OY/ L 2E,-7-3-4044
I
On the Method of Wasuring Optical Constants of ~ietals
angle. When the coupled polaxe-ids are imiformly rotated
about the optical axis the intanS4 ty at the entr.V slit
of a light receiver (a photoelectric photometer) varies
with the angle of rotation a accordine to
y = A + 2B sin 2 m + 0 sin 1~a
Between zero and 90 0 three extrema of 3- are observed
(they are a, b and c)~ The relatic~nsh-ips Lwt-aeer, V and
and the -ialues a, b and c. are g]-VS11 by
tg (a/c) 1/8 cos 4 b c - b)
Here a < c (i.e < 450) and
presence of f ilms on the untal
values V1 and A is obtained;
V and 6, make it possible to
Card 2/3 and the refractive index of the
00 A < 900. In the
Eiurface another pair of
these, together with
calculate the thickness
surface layer (Ref 2).

67732
SOV/126-7-3-40/44
On the Method of Measuring Optical Constants of Metals
If the number of mirrors is less than four, the missing
samples are rep-Laced by standard mirrors, e.g. of gold
deposited on glass for which the value 10 and -4 0
are measured separately. Yhe method can be used to
detect and m sure thicknesses of very thin film of the
order of 10 r. In vacuo the method can be used to study
adsorption of 6ases on metals. Since no phase
compensators are employed the method can be used also
to measure the optical constants of metals in the
ultraviolet and infrared regions.
There are 2 Soviet references.
ASWCIATI(XI: Ural'skiy gosudarstvennyy universitet imeni AX.Gorlkogo
(Ural State University imeni A.M.Gorlkiy) tw~
SUBLITTED: January 89 1959
Card 3/3

84619
7 700
AUTHORS:,
00 Y-3 /93
S/181/60/002/010/049/051
B019/BO56
TITLE:
Zverevp L. P., Hoskov, M. M., and Sbur, M. Y&.
On the Contour of the Exciton Absorption Bands in Cuprous
Oxide
PERIODICAL: Fivika tverdogo tela, 1960, Vol. 2, No. 10, pp. 2643- 2646
TEXT: In the introduction the results'obtained by investigations of the
optical propertfei of crystals, especially of the absorption spectra,
are discussed. Among others, E. 1. Rashba, L. S. Davyclov, and Ye.. F.
Gross are mentioned. The authors of the present paper experimentally
investigated the contour of the second band of the yellow series of sx-X
citon absorpti.on bands and of thin'cuprous oxide single crystals at
temperatures of from 4.2 - 1900K. The measurements were carried out on
a diffraction spectograph of the type AfC-4 (AFS-4) with high dispersion
and photoelectric i-edording. The three sanplee investigated had a thick-
ness of 9, 30, and 110 p, respectively, and were produced from thin
copper foils by oxidation In air at 1030 OC. The contours of the exciton
Card I / 3

84619
On the Contour of the Exciton Lbsorption B/lal/60/002/010/049/051
Bands in'Cuprous Oxide B0191BO56
abaor~tion bands (n 2) in all three samples investigated showed good
agreemeit. The maximum absorption coefficient was measured at 77-30K as
amounting roughly to ISO OIL-1. The temperature dependence of the exciton
absorption line width Lagraphically repreaented in f1g, 1p and from the
Contour of the absorption liaeshowed in Fig. 2 the goo& agreement of
the measured result& with those obtained from the formula (1) given by
Toyozara. (Rif-3) for the absorption coefficient.may be recognized. Thus,
the opinion expressed by Toyozawa that the broadening of the exciton
absorption bands is caused by the excitom-phonon interactioal is con-
firmed. Furthermore, it is also confirmed that the lifetime of the
photoexcitona at temperatures below 550K is principally determine& by
zero-Tibrations of the lattice. From the good agreement between the
experimental data with the theory, the conclusion may be drawn that
only the acoustic branch of the lattice-ribration spectrum plays an es-
sential part in excito4-phonon interaction. The authors thank
IT- T. YoUgnshteya for his assistance in the experiments and G. 0.
Taluts for discussing the results obtained. There are 2 figures and 10
references: 5 Soviet, 4 US, and I German.
Card 2/3

67899
S/226/6O/O1O/OO3/oo6/oo9/xx
603200 (also nov-) E201/E391
AUTHOR: Noskov, N.M.
TITLE: A Reflecting Phase Compensator for optical
Measurements on Metals
PERIODICAL: Fizika metallov i metallovedeniyl 196o, vol. lo,
No. 3, PP. 467 - 486
TEXTj The optical constants of a metal may be found by
measuring'the rotation of the plane of polarization on
reflection of plane-polarised light by a metal mirror. The
authoir describes phase compensators suitable for such
daterm*inations of the optical constants of metals at iqfrared
frequencies. The compensators are mirrors of Cr, Nb, Ta and
Pt, which have low conductivities and are stable in air, The
optical constants of the compensator mirrors must be
measured accurately in the required range of wavelengths.
The optical constants of the compensators are used to find
the values of the phase difference introduced on reflection
and of the ratio of reflection coefficient for two components
Card 1/2

67699
s/l26/6o/olo/oo3/oa6/oo9/xx
E201/E391
A Reflecting Phase Compensator for optical Measurements on
Metals
of light polarized at rightangles to each other. The author
concludes with a cakulation illustrating the case of plane-
polarized light reflected once from a test sample and once
from a compensator.
ASSOCIATION: Ural*skiy gosudarstvennyy universitet
imeni A.M. Gor,kogo (Ural State University
imeni A.M. Gorlkiy)
SUBMITTED: June 6, 1960
Card 2/2

30808
3/181/61/003/011/056/056
B109/BIO2
AUTHORS: Zverev, L. P., Noakov, M. M., and Shur, M. Ya.
TITLE: Photomagnetoelectric effect and band structure in cuprous
oxide
PERIODICAL: Fizika tverdogo tela, v. 3, no. 11, 1961, 3556-3558
TEXT: Owing to the lack of an appropriate monochromatic light source the
spectral behavior of the photomagnetoelectric effect (PME) could so far not
be sufficiently studied. These difficulties could be overcome by using
aA -3 (D-3) lamp with strong monochromators(paos band 15 to- 40R). The
measurements were made with 150-300-micron thick cuprous oxide platelets
at 77 0K in 25-koe fields between 4000 and 7000 X. In this case the dark
conductivity was much lower than photoconductivity. Fig. I shows the
measurement results which clearly indicate three spectral ranges: (1) NO
PME occurs above 5600 R. This can be explained by the fact that electronst
are produced in the polaron state. As compared to the free electrons ty
their mobility is lower and their diffusion length is shorter. (2)
Card 1 1
X'3

006
S/lBY61/003/011/056/056
Photomagnetoelectric effect and band ... B109 B 102
Between 5800 and 4900 R the PHE is due to the production of free carriers.
Its monotonic rise is determined by the dispersion of the absorption
coefficient and the quantum yield of the internal photoeffect. (3) Below
4900 9 the behavior of the PHE corresponds to the wavelength dependence
of the PME near the fundamental absorption edge, which is typical of
semiconductors. This phenomenon is connected with the abrupt increase of
the diffusion length, in this case determined by the electron parameters,
and suggests the existence of a new band-to-band transition in which
electrons with other diffusion characteristics are produced. The
conduction band splitting in Cu20 was suspected already by S. A.
Moskalenko (FTT, 1, 1755, 1960). Also the data by I. Fastrnyak, P. A.
Titov (FTTt It 8619 1961), 1. Pastrnyak (FTT, Lt 971f 1959), A. L.
Rvaohev (ZhTFf 289 45o 1958),and N. B. Gornyy (ZhETF, at 261, 195P) spoak
in favor of this assumption. The authors thank I. J(a Taidillkovskiy for
discussions. There are 1 figure and 9 references: 7 Soviet and 2 non-
Soviet. The two references to English-language publications read a5
follows: 1. Kikoni, ;4. Noskov. Nature, 131, 725, 1933i1r. Gartner. Phys.
Rev., jO
823, 1957
Card

''J1 17,003/011/95~/056
Photomagnetoeleatrio effect and band bl,,)~gBI402
A850CIATION: Urallskiy gosudarstvennyy universitet'im. A. M. Gorlkoga
Sverdlovsk (Ural L;tate University Imeni A. M. Gorlkiy,
Sverdlovsk)
SUBMITTO: August 259 1961
Fig. 1. Spectral dependence of the photoconductivity and of the
'short-circuit current of the PRE (CV,e) for Cu2O.
Legend: (1) 1 short-circuit current; 6'., photoconductivity in
ac P
arbitraty units; Cis the f irst part of curve a on an edlarged ac4le.,
Zaid

SoM. DoUair BelCmIc-e AlaUjj !:z-A. Vol 14. '.'o 6. 1151 Cam-
:rr"!&,,*i w,.,Lh a rc..t cf xzAys.- z. iuke*os afd z.
BAST M-1 trclia-l With ~-Lry)z rp
of
AI (1.1
24. -Wyr.4% ('Alto t
"Atts" k-l-h--
WMA
2". of Cl. Aldll;.-L-',`-~ 'XI"'... cr L.M.iil
cn ~,tt. 1r.! -1--U .

BLAGONRAVOVv S.I.; BMK, 3.14.4~BYAKOV, P.T.; VIKTOROV, V.S.; VAGANOV,
V.I.; GUSEV, S.A.; GLEEOVE V,V.; GL?,Ilzv, A,M.; DAIIIWV# G.D-;
ZAV9YAWV,, V.G.; IOMj Ye.F.; IM, MV, G.H.; KOMMvp S.A.;
r,ULIGM,,, 'A.S.; USATKIN, A.P.; DZIETSOV, N.I.; LEBEDE:V,, A.I.;
W4FERTq Ye.N.; 101MEEVICH, Ya.l.; KAYZEWj, M.A. ; MITYAKCIV, V.S.;
UOSKOV.-M.; RYABCHIKOV, 1I.Ya.; 4TSKUI, R.I.; TVOROGOV, 14.K.;
UGOWNIKOVP V.Ya.; KHAROKOV, G.I.; CUMV, S.L.
Lev Hillevich Hatvcev; obituary. Torf. pr=. 38 no.4:38 161.
(MIRA 14:9)
(Hatveov,, Lav Millevicht 1914-1961)

"192 71
S/126/62/013/005/030/031
E073/E535
AUTHORS: Kirillova, M.2"I. . ~~~~nd Charikov, B.A.
TITLE: Influence of heat treatment on the optical properties
of metallic layers
PLIZIODICAL; Fizika metall.ov i metallovedeniye, v.131 no.5, 1962,
798-799
TLXT: The effect of heat treatment was investigated for
0.23-0-35 11 thick filivs of c?ld I COP9 er, silver and cadinium
deposited at a vacuum of 10- to 10- mm Hg onto a glass base at
room temperature. The annealing was in vacuum at 110-120*C and
in some casea up to 200*C. Before and after aunealing. the
following were determined: donsity (by measuring the thickness
and weight), resistivity atid the optical constants n and k,
which were measured according to the method of J. A. Beattie
(Phil. Mag., 1955, 46, 235) at the wavelengths 0.423, 0.542 and
0.550 U in several points between 2 and 9 IL. Measurements-
have shown that.,
1) Freshly deposited non-transparent layers of Ag, Au and Cu an
-lass have a density 5 to 101a' r6yer than that of the cast metal.
Card 1/4

Influence of heat treatment ... s/126/62/013/005/030/031
E073/E535
The density increases after vacuum annealing for 10 to 15 hours
at 110-1200C to the values given in the table. The metal with
the lowest inelting point, cadmium, did not show any change. in
density after annealing.
'_'L7
Density. g-cm Resistivity 10, CGSIE
Initial Annealed Massive Initia 1 Anneal ed Massive
state state
Gold 18.3 19.1- 19.3 2.2 3.5 4.o6
CopT)er 8.65 8.90 8.95 2.1 5.0 5.35
Silver 9.50. lo../* 10.5 2.65 5.1 5.6o
2) The refractive index -n 'of gold and copper shows hardly any
chan.-e,after annealing,for short-wave radiation (% = 0.423 -4)
but drops by a factor of 1.5,to 2 times in the long-wave part
of the visible spectrum and in the infrared range. The
attenuation index k increases approximately-by 2014 in the same
range in which n decreases. The optical constants of cadmium
Card 2/4

7'-)
,14~.
Influence of heat treatment ... 5/126/62/013/005/030/031
E073/E535
change only insignificantly after annealing.
3) The clian46es in the optical constants correspond to a decrease
by about 1.5 to 2 times in the absorption capacity A = I '- R.
The changes in the optic . constants with annealing are virtually
tori'Anated after 2 to 3 J Aours but,for obtaining stable values of
density and resistivity,the annealing had to be continued for
10 to 15 hours. Then, it can be assumed that the structure of
the metal in the optical layer in the neighbourhood of the
surface is satisfactorily normalised.
T'.'Ie nomialising effect of the heat treatment is particularly
noticeable on metals with a relatively high melting point, whilst
metals with low ;-aeltin.- points .,rill deposit in vacuum at a
sufficient initial density and the effect of heat treatment is
negligible. Annealing has also little effect on the optical
constantsof gold and copper in the short-wave range of the visible
spectrum in whicii lattice defects are not of great importance
due to the quantum nature of the excitation of the electrons by
light. Calculation of the classical depth of penetration 6=k2TY k
from the values of k yields the following values: 6 = 0.0335 11
for X = 0.55 It and 6 = 0-0283 1A for X = 7 IL (0-35 1L thick annealed
Card 3/4

Influence of heat treatment ... s/126/62/013/003/030/031
2073/E535
6old). Since in the range -2-9 ji , Ic is almost proportional to
the wavelongth, the depth of penetration will be prnctically
indenendent of the wavelength. In the near-infrared range the
optical properties of gold can be approximately expressed by the
formulae of Drudo-Ziner and therefore, for an approximate
estimation of the collision frequency, the relation ,
y = 2nk w/1 - n2 + k2 can be applied, from which we obtain
0.8-10 14. Prior to annealing, y is about twice as high and
6 is about-20'/j higher than in the normalised annealed state.
There is 1 table.
ASSOCIATION: Institut fiziki metallov AN SSSR
(Institute of Physics of Metals AS USSR)
SUBMITTED: January 17, 1962
cac-1 4/4

39j%- 6/62/013/oo6/002/018
67. 5 3 '7 0 9202/E492
AUTHORS: Bolotin, G.A,, Voloshinskiy, A.N.j Kirilloya, M.M.,
Noskov, MtM._,_Sokolov, A.V., Charikov, B.A.
TITLE: Optical properties of titanium and vanadium in the
infrared spectral region
PERIODICAL: Fizika'metallov I metallovodeniye, v,13, no.6, 1962,
823-831
TEXT: Experimental data of the magnitude and frequency
dependence of the real and imaginary componentap of the complex
permittivity C' for titanium, vansdLum and gold were studied in
the region of Z to 10,1&, and room tomp*ra-ture. The changes in
the state or polarization occurring during reflections from the
surfaces of the metals were measured. Mirrors were prepared
from 99.99% pure vanadium and titanium Iodide by mechanical
polishing In an acidic medium. Measurements of stati*c electro-
cond4ativity at room and liquid nitrogen temperatures confirmed
the high purity of the samples used. Gold mirror was prepared byl
vacuum deposition and was used Car comparisons Parallel beam of
polarized Infrared Light was reflected in tgrn from four metallic
Card 1/4

s/i.26/62/013/oo6/002/0-18
Optical properties of ... E202/E492
t
mirror aurfacei and the ratio of the parallel and perpendicular
Intensities and phase differences of the polarized component were
evaluated. Emerging from the analyxer, the beam was focused on
the alit of the infrared spectrometer type WKC -12 (IKS-12).
The ellipticity components were evaluated by the method of
parallel polarizers. Almost complete data of n, k. and the
real e1 and imaginary C2 , component dependency on frequency
was tabulated at 0.51& Intervals for Ti, Va and Au. Plats of*
reflectivity and dispersive power versus wavelength were also
included. The above experiaen~iiL data were used in a detailed
theoretical analysis of relations existing between the dielectric
permittivity and wavelength$ using the elaborate method of
approximating polynaKialas Polynowlats satisfying the
experimental data gave the miowing vatues for tho respective
coafficientol
Titaniums cl w6a4ho(b + WK00 ma + 4.60 o.at9406
92 43,941-1 + 11.16A + 0,2oh3i (6)
Card 2/4