SCIENTIFIC ABSTRACT SKLEAREVICI, I.A. - SHKLYAREVSKIY, I.N.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SnE,~'IE-qTICI) I.A. [Shkl-yarevich, I,Ao]
Application of high vacuun for the intensification of
agglomeration process. Analele metalurgie 16 no.3:15-18 ii-S
162,

SHKLYARE-VICH I.A.
"Equipment of sintering plants for ferrous metallurgy" by A.E.Seleznev.
Reviewed by I.A. Shkliarevich. Stall 22 no.10.-889-890 0162.
(MIRA15:10)
1. Vsesoyuznyy nauchno-issledovateilskiy i proyektnyy institat
;nakhanicheskoy obrabotki poleznykh iskopayamykh.
(Sintering-'quipm(3nt and supplies)
(Selezne, A.E.)

SHKLYAREVICH, I.A.
Intensifying the 8intering process. Met. i gornorud. prom. no.2:
16-18 Mx-Ap 165. (MIRA 18: 5)

SHKLY~%.1;LVSKIY, r.l~.; !.1jjj-SU-.VSj,7jy, V.K.; GOLOY:~POVA, V.I.
4 11 ~
1,1ide-aperture interference of light. Opt. i spektr. 17 no-5:
765-770 t,,, 64. (IMIRA 17:12)

SHKLYAB-P,lIr,)T- M., assistent
Malignant theco-follienloma. Zdrav.Belor. 4 no-3:63 Mr 158.
(KIRA 13:7)
1. Iz akushersko-ginekologichaskoy kliniki (zaveduyushchiy
Icafedroy - doteent I.S. Legenchenko) Minskogo instituta uso-
vershenstvovaniya vrachey.
(GRAERATIVE ORGANS, FWLU3--TUMORS)

BCDIJLM', V.P., prof.-. SHIMALREVSKAYA, Ye.V., kand. mied. nauk; YERCf4MH1V1T,,
G.A.,
Topical diagnosis of pulmt~narv. echinococc;osis. Uch. 2ap. Stavr.
goo. wed. Inst. M77-187 16.1 (MUFA 17,-7)
1. Kafedra cb-zh~theq khimir~gli ZaV. v7J. 3--dti!"n) 51.av-
Is' viediu:inzi:ogn -jizstiti~~,-~ zt:51uzhanrryy dey-a-
-c)gc, T
ropc- A
tell nauki. pro". V.G. BUdylin).

USb/Geophysics - Irrigation Jun 52
Specialists
"Chronicles: Conference on the Problem Con-
cA cerning Methods for Irrigation of Agricul-
A. 1. Shklyarevskiy
tural Cultivation"
"Gidrotekh i Melio" No 6) PP 75-80,
During 12 - 14 Mar 52, in Moscow, the Hydro-
technics and Amelioration See of the All-Union
Acad of Ngri Sci imeni Lenin held a plenum,
with participation of agricultural and hydro-
logical administrators, directors, arid main
Aff,r ~nomi~qts of MTS (machine-tractor stations),
besides presidents of kolkhozs in irrigated
districts of Kuybyshev.and Saratov Oblasts.
Discussed were problems of,utilizing irri-
gated lands under conditions met beyond the
Volga and in other new regions being irrigated.
Reports were beard from 22 lecturers: "I.A.
K~iRkemich, substitute f or .. Minister of
USSR; Prof V.A. Shaumyan, substitute for the
d13~6ct-df_d:F_ -c-i ent ific part of All-Union Sci
Rep-Inst of Hydrotechnics and
'I.P. r a " " yshev Oblast Water..
y, hea , Kuyb
yle
i-con;-I.A. Isakoy, Chief Agronomist, Georgiyev
Tq_i Dorokhiqj ;` L: res,
~haritjonQv,' Chief Agronomist, Saratov Oblast
j!.a '6hief A---- ---
~dAd~ktxi;-Prokhorov",, gronomist, Saratov
A-INIQQ+. T~fps: PC~Eh_&i~3-~,~,pres "Komsomolets"
Kolkbo YershovV Pres, UXbYi ~M_0_4~jAst E!?~ec
Comltt~~e~; je._C`~etrov, Cand Agr Sci, -All-Union
Rg
Insj_ _Hydx~tjchnics and Ame~l~63~tion;
Yegorshilov, En9r; N.P. Samsonov, Sr Sci Assoc.,
A1 I _-jJnj on Se~ f HY-drotechi.cs, and
Amelioration;, Nesteroy,,, Pr "Zar.)ra" Kolkhoz;
V.G. Kornev; _-_ es,
Sr Sci Assoc of
Ukrainian Exptl Sta;.etc.,

ASTAPOV, Sergey Vasillyevich, professor; SPENGLNR, Valentina Vasillyevna.
SEKLYAREVSKIY.-A.I., redaktor; MRSYPKINA, Z.D., tekhnicheskiy
- -
eVM-T,- dr-,---,RTMXNSOVA, S.L., takhnicheskiy redaktor
[Prevention and control of salinity and sqamping in irrigated lands)
Preduprezhdenie i bor'ba s zasoleaiem. i zabolachivaniem oroshaemykh
zemell . Koslcva, Gos. izd-vo salkhoz. lit-ry, 1956. 158 p. (KMA 9:12)
(Salinity) (swamps)

t
OFFEUGENDEN, Samuil Rafailovich,kandLt tekbnicheskikh nauk; PANADIADI,
A.D., kandidat sellskokhozya3rstvennyk:h nank; TROMBACREV, S.Po,inzhener,
Edeceasedj; YARUSHIN, M.I., inzhener; KUKEIN"PSKlY , H-D-kandidat
sellskokhozyaystvennykh nauk; KAGAN, G.S., inzhener; NIKOLAYEV,I.G.,
inzhener; TRUBACHEVA, Ye.G., kullturt,ekhnik; ~~' AUT A.I.
redaktor; FEDOTOVA, A.F., tekhnichosl:iy- redaktor -A~
LOperation of irrl,~:ation and drainagn s7stemal Ekspluatataiia gidro-
meliorativnykh sistem. Pod red.S.R. Offengendena. Moskva, Gos.izd-
vo sellkhoz.lit-ry, 1956. 535 P. (Ml--RA 10-6)
(Irrigation) (Drainaze)

AUT, HOP: Q /-I
I., Eng-neer "~V/99-59-1-8/13
TITLE: The KbtEtyksk~yaIrrJ-ation SyStem is in Operation (Kotaykskaya
0
skaya orositeltnaya sistema vstupila v stroy dey-
stvuyushchikh)
PERIODICAL: Gidrotekhnika i melioratsiya, 1959, Nr 1, pp 33-37
(USSR)
ABSTRACT: The author describes how, under very difficult con-
ditions, Armenian workers in a short time built the
Kotaykskaya irrigation system. This system will
irrigate 7,500 hectares, serviced by 116 km of per-
manent canals. A total of 23,000 cu m of concrete
and 700 tons of metal structure were used in the
construction. In November 1958, the Arzni-Shamiramskaya
irrigation system with EL 17 km long canal was put
into operation. There are 8 photographs.
Card 1/11

30(i) sov/99-59-7-10/10
AUTHORS: L_a;)`doks'=iYs -K.L'. , and -3h`:-1lyarevS`:1-__J-,-, A. _7. , E'ngineers

TITLE, In the 3cientific and Technical Council of the Ministry
of Agriculture of the USSR (V nauchno-tekhnicheskom
sovete ministerstva sel'Skoro SSSR)
PERIODICAL: Gidrotekhnika i meliorats-iya, 1Q,19, Nr -64
pp 60
(USSR)
ABSTRACT: The article is concerned with a meeting of the Scien-
tific and Technical Council of the Ministry of Agri-
culture of the USSR held_ during the period 12 - 15
January 1959. and devoted to full mechenization of
Cotton cultivation and harvesting. The reetin- was
attended b-- specialists -in cotton g-r-oviing of Uzbe-
histan, Turl=eniya, Aze:-baydzhan, Kazakhstan, and
Tadzhikistan, by research ~:,,.,o-rkers of 'he co'-ton-produ-
cinc-, republics, bir reprasentatives of the -olants
mak~n- cotton-tillins machinery, by scientific workers
~ ~'
I
O.L the Vsesoyuznaya akademiya sellsko'l~-hozyaystvennykh
Card 1/5 nauk imeni Lenina (All-Union Academy of A-gricultural

SOV/99-59-3-10/10
In the Scienrific and Technical. Council of -,,he L,~-Jn~~ry of Agri-
cult-.ure of the -U'SSR
imonj- Lcz!in), and b,,/ specialists of the or-
economy, hydraulic
Th,,,- was -ilso attended by
i,epre sent a tiveo, of the Crosudarstve,iiiyy nol-ichno-tekh-
nicheskiy komitot 6oveta L-Iiiii-4strov SSSR ~State Scienti-
fi.1- ,--nd Te~,hni~,al Commill-tee of the Elinisters! Council
o.--P the USSR), t~iose of the Uzbek and Kirgiz SSR; the
Gosplan USSM, t;he Minist-erstllvo sellskogo khozyaystva
SSSR (lainistry of Agric-liture of the USSR), and the
ministries of agriculture and water economy of the
r:ott.on--Droducing repullic~s. The meet-ing was opened
by G.A. Bor-kcv, Deputy 111inister of Agriculture of the
'USSR, vihose s',- 'ort' speech was followed by reports made
by tl~e 'folloviing perso-val-ities: 1) T.G. Zinin, Deputy
Di--ector of the U7,be'L~-s~:.-,Tnauch-Tio-i-ssledovatel'skiy
insti-tut mekhanizats-ii -i e1ek-L:ri'Likatsii sel'skogo
1,hozyaystva (Uzbek ReSE~arCll Institute for the Lllecha-
rjLzation and Electrificat-ion oF' Agriculture); 2) V.A.
Card 2/5 Tyup.',:o,. of the Srednea-,-,iatuskaya EIS (Central Asian

SOY199-59-3-10110
-P A crri-
i ri i e n t 1' --- i c -n n r: Ti e c !in- i cI ^- f tu", ein-i-t Y Of
culture of the USSR
LI.Y3, Topada. Chief Engineer of the Pakhta-
Aral sovkhoz; 4) IT,,, 3iekirov, of the "Bayaut Nr 4"
sovkhoz. Tashkent Oblast TIelesh'Ko , Director
of the Z)redneaziatskaya mashino--spytatellna a stan-
L
4
ts~ya Central Asian N"ach-1-ne Testing Station
6) B.Ye. Arkhangel'skd.-y-- Chief Designer of the Li-
pet-sIr-'-1y traktuorny-j zavod (Lipetsk Tractor Plant);
7) Ye-A. Sarkisyants, Chief Designer of the Vladi-
mirsk.iy traktorny-y zavod ~Vladmimir Tractor Plant);
8) N.I. Popov, Ciiief .3pecialist of the Nauchno-
tekhnicheskiy komitet Soveta ministrov Uzbekskoy SSR
(Scientific and Techn2-cal Committee of the Ministers'
Counci-I of the Uzbek SSR); 9) Ye.V. Radkevich, Chief
Designer of the SKB for Cotton of the Tashl--ent Sov-
narkhoz); 10) B,P, Firsov, Deputy Chief inspector for
Cotton of the 1,.'SKh SSSR; i1) -A.N. Askochenskiy, Aca-
de.riician and Secretar,y of the Otdeleniye -I-idrotekhni-
k---' i melioratsii VASK--il-TIL (Hydraulic En-ineerin- and
Mielioration Departmen,- of VASKhTNIL -~ K. P:. -S'
Card 3/4 J., 12 hub-

59- 3 - 10/10
In then Scierit-i 'Lic- and Tec'hnical Cour-c il of uhe ;,`Lni.~- ry of A-ri-
culture of the USSR
ladze.. Deputy Cl-ief of G1avvod-'k:ho-- 1IS-7-h USSR; 13)
N. 11, T-~ul~o~,, 3enior :.1) C 4enti 'i c V-Jorker of VITIIGilliiii
14) L.D. S-Ionov, 1,71IUill'~. 25) M.F. Euldkov,, Fer-ans-
,,i stantslya Fer a Testing Stiation)i
kaya opytna-7 an-
3- c Go!3pla--. 3SSR, 17) N.I. Fershtat,
Depui~.y -of Agriculture of the Uzbek SSR;
18) A~A. Troits-lkiy, De-j--v Minister of Agricultu:,~'e of
the Tadzhik SSR, 110) Tv,.A. M 'atvoyev, GosNIIGVF-, 20)
N.I. Kostyuk, r.!SKh of r..'ate Kirgiz SSR; 21) S.ra. Shakh-
muryadyan, VIM; 22i LT. Khalilov, MSKh of the Azer-
baydzhan SSR4 2-.3) K.A. Gularyan, ArmTNjIIZ; 24) A.A.
Karimov, GNTTk of the Sovet TTinistrov Uzbekskoy SSR
11111inisters Col-uncil of the Uzbek SSR); 25) N.I. Depta,
Tashkent sovrarkhoz; 26) M.N. Anan;yev, Giprovodkhoz;
27) I.P. Panow, Tashsel'mash, 28) Ivanov, GOSNITI;
and 29) V,A. Kaufman, G-11avnoye upra-uleniye melechani-
z--tsii i elek-trofika;1--ii t'SKh SSSR ( Central Adr-ini-
stra-cion of the Lieclianization and Electrofication
Card 4/5 of the i,!SKh USSP)~ Aroorip, the organizations only

so~jqq.. r.-9-3-10/10
In the Scientific and Technical Council of the ?,,in-. -~-U:-ry of Agri-
cultiure of the USSR
mentioned in the above reports yet not listed above
are the following: 1) Vs,,esoyuznyy nauchr-o-issledo-
vatel'skiy institut gidrotekhniki i melioratsii
imeni A.N. Kostyakova (All-Union Research Institute
of Hydraulic Engineering and Lielioration. imeni A.N.
Kostyakov) ; 2) Gidroproyekt; and 3) VNIIStroydormash.
Card 5/5

SHKLYAREVSM, A.I., inzh.
Kotalksk irrigation system went into operation. Gidr. i mel. 11
no.1:33-37 da '59. (MIRA 12:1)
(Armenia-Irrigation)

SHKLYAREVSKIYI A,I._
Plenum of the Section for Hydraulic Engineering and Soil Improve-
ment at ehe Lenin All-Union Acadeqf of Agrucultural Sciences.
Gidr. i mel. 14 no.4:57-63 Ap 162. (~IIRA 15:5)
(Irrigation) (Drainage)

BODULIN, V.P., prof.; SIMLYARETSKAYA, Ye.V., kand. med. nauk
Topical diagnosis of hydatids of the lungs. Uch. zap. Stavr.
gos. med. inst. 12:~05 163. (MIRA 17:9)
1. Kafedra obshchey khirurgii (zav. prof. Yu.S. Gilevich)
Stavropol'skogo gosudarstvennogo meditsinskogo instituta.

24(5)121(7)
AUTHOR: Shklyarevskiy, G. M. SOV/556-36-5_29/76
TITLE: Single-Particle Mechanism in Photonuclear Reactions
(Odnochasticbnyy mekhanizm v fotoyadernykh reaktsiyakh)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 5, PP 1492-1496 (usn)
ABSTRACT: In the introduction the problem as well as a number of earlier
papers are discussed in short. It is pointed out that there
exist experimental facts which do not fit into the framework
of the two-particle model (the existence of photoprotons with
energies that are nearly equal to the maximum energy 4-n the
'r-spectrum, shifting of the m,-zimum of angular distribution.
towards the angular range of 20-500, and direct obser,;-ation of
( y-p)- and ( rn)-reactions at high photon energies). Therefore,
the direct single-particle mechanism, especially in the range
of gigantic resonance, is'of g::eat interest. To investi,,rate it
for nuclear photo-reactio-as athigh enerEies of the emitted
nucleons ( 3`1120 Mev) on the baais of the shell model is the ain
to be achieved by the present paper. Satisfying the momentum
conservation law warrants also consideration of the momentum of
Card 1/3 the nucleon bound in the nucleus, and, at the same timej

Single-Particle Mechanism In Photonuclear Reactions sov/56-36-5-29/76
makes it possible to explain.the forward shift of the angular
distribution like in the case of the,atomic photoeffect. The
author bases uDon the following assumptions: The nucleus in the
ground state is assumed to consist of nucleons moving independ-
ently in a centrally-symmetric potential field; the state of
p
each.nucleon is asslamed to be characterized by the orbital
momehtum 1, its projection m, and the binding energy El
SP:En and magnetic moment of the nucleon ara neglected, which
amounts to a neglect of spin-orbit splitting. In consequence
of the neglect of nuc','.-(,,n intezaction, only "hole" excitations
of the residual nucleus are possible; the energy of these
excitations is contained. in thE binding ene:rgj of the nucleon.
The description of the interadt.-;ons in the final state is
carried out by means of the optical nuclear model. Calculations
are carried out in momentum appro-CImation. Basing or. the
operator of the interactionbe-;ween nucleus and electro-
magnetic field, expressions are derived for the matrix eleT_-.~rt
21r 2
in the reaction cross sect4on. formula dd =-3r- IMI ~ (E)
Card 2/3 Theoretical and experimental results are compared.

Single-Particle Mlechanism in Photonuclear Reactions SOV/56-36-5-29/76
it is shown that interaction in the final state can be de-
scribed by the optical model and that 2 effects, above all,
occur: 1.) The existence of.an imaginary part in the potential
leads to a reduction of the cross section of the direct photo
process at the expense of the development of intranuclear
cascades and (or) the occurrence of' excited states of the type
of a compound nucleus. 2.) The nucleon after photon absorption
is elastically scattered on the real part of the potential,
which leads to a certain "smearing-Iout" of the angular
distribution. The author finally thanks Professor L.A.,Sliv
and Professor I. M. Shmushkevich for their valuable comments.
There are 1 figure and 13 references, 2 of which are Soviet.
ASSOCIATION: Fiziko-tekhnicheskiy institut Akademii nauk SS.SR
(Physico-Technical Institute of the Academy of Sciences, USSR)
SUBMITTED: November 20,. 1958
Card 313

8 1., 4 0 "7
S/056/60/039/004/0251/048
BOO6/B063
AUTHOR; Shklyarevskiy-,-G. M. 19
TITLE,~ Theory of Photonuclear Reactions of Light Nuclei With
Emission of Deuterons
FERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 39, No. 400), PP. 1031 - 1038
TEXT: In the present paper, the author gives a theory of thewd-reaction
of light nuclei within the framework of the independent-pair model in
small-correlator approximation. This model takes into account both the
general self-consistent field and the pair interaction leading to
nucleonic motion correlations. The wave function in this model is
formulated as follows: T = 1~a 1( i )1,2(2) .. .. ~, n(n)j(1 +Q,j). where
~?ai(i=192..n) is the single-particle wave function, andl,,j the
correlators. At distance of the order of the mean nucleon distances in the
nucleus, holds in t!7- TI-e mechanism
Card I/A
I

8hh07
Theory of Photonuclear Reactions of Light S1056160103910041025,1046
Nuclei With Emission of Deuterons B006/BO63
excitation of the product nucleus as a result of quick variation of the
self-consistent field of the nucleus during em'-ssion of a pair of
nucleons is considered, and the excitation probability in the region of
the continuous spectrum is calculated for the case of independent
particles. It is shown that correct values for the ~-d cross sections of
light nuclei and also for the shapes of energy spectra and angular
distributions can be obtained by employing published values of the para-
meters involved in the theory, The results obtained are compared with
experimental data on C 12 and Be9 nuclei. Data on the a rdIcy ~,p ratio were
given by V. P. Chizhov and L. A. Kullchitskiy.-The experimental data are
graphically compared with various theoretical curves. Fig. I shows
dcl/d-Q= f(E d) calculated for transitions without a change of the nuclear
configuration (Curve 1), for transitions taking account of single-particl~
excitations (Curve 2) and two-particle excitations (Curve 3) for C 12 with
'&~C 12 ) = 15.2 Mev,4w(B 10 ) = 17.0 Mev, and E ;~Mjx = 80 Mev; Fig. 2 shows
the same for Be9 withkw(Be9) - !6.2 Mev,Aw(Li ) = 18.9 Mev, end
Card 2/3

Alto?
Theory of Photonuclear S/056/60/039/004/025/048
Nuclei With Emission of Deuteroiis B006/BO63
E~,max - 90 Mev. Fig. 3 shows a comparison between the experimental and
theoretical angular distributions of the reactions C 12 (7,d) and Be'(~d)
normalized for 0 = 60'~ R = 1,5A1/3.10-13cm was assumed for all the
calculations. The author thanks S, V. Maleyev. A. D. Piliya, and Professor
L. A. Sliv for discussions and comments, and also V. P. Chizhov for a
discussion of experimental data. Migdal, L. E. Pargamanik, and
V. V. Ullyanov are mentioned, There are 3 figures and 16 references:
4 Soviet, 6 US, 2 British, 1 Swiss, and 3 German.
ASSOCIATION: Leningradskiy fiziko-tekhnichesl:iy institut Akademii nauk
SSSR (Leningrad Institute of Ph,sics and Technology of the
Academy of Sciences, USSR)
SUBMITTED: April 30, 1960
Card 3/3

SHKLYAREVSKIY. G.M.
Nucleon correlations and photonucle&r reactions. Part 1: Photo-
disintegration of He/+. Zhur.eksp.i teor.fiz. 41 no.1:234-238 JI
161. (MERA 14:7)
1. Leningradskiy fiziko-tekhnicheakiy institut All SSSR.
(Photonuclear reactions) (Nucleonsj (Helium-Isotopes)

SHUY-AREVSKil, G. M.
Dissertntion defenied for the legree of Candliate of Physicomathematical
Sciences i~~t the Physics imeni ?. H. Lebedev in 1962:
"Correlations of N,tcleons, and Slimple Photonuclear Reactions."
Vest. ALal. Nnuk SSSR. No. 4, Moscov.,, 19~'53, p--i-es 119-146

ACCESSION NR:' AP4019238 S/0056/64/046/002/0690/0694
AUTHOR: Shklyarevskiy, G. M.
TITLE: Inelastic scattering of photons by a Coulomb field accom-
panied by electron-positrOn pair production
-SOURCE: Zhurnal eksper. i teor. fiz., %r. 46, no. 2, 1964, 690-694
TOPIC TAGS: Compton effect, inelastic photon scattering, scatter-
ing by Coulomb field, electron positron pair production, Weizsacker-
Williams method, proton polarizability, proton polarizability c.or-
rection
ABSTRACT: in this investigation the
tons are assumed much larger than tha
losses are assumed to be small. The
by the Ileizsacker-William method in
by Gribov et al. (ZhETF v. 41, 1839,
Card 1/3
energies of the incident pbo-
electron mass and the energy
analysis of the scattering is
its invariant formulation given,
1961). This scattering process

ACCESSION NR: AP4019238
has not been treated in the literature before. It is shown that
this process occurs in a lower order off perturbation theory than
other processes involving the Compton effect on protons or other
nuclei, and that at small angles it appreciably exceeds the correc-
tion-to the Compton effect on a proton due to the polarizability
of the nucleus. Furthermore, it exerts a decisive effect on the
background which interferes with the measurement of the Conq.~ton-
effect cross section in the small-angle region. The results are
compared with some experimental data. The cross section of the dis-
integration of a photon into two photons by interaction with the
Coulomb field of the
proton is two orders of magnitude smaller at
all angles (except the largest ones) than the cross section of the
investigated process. "I am grateful to 1. M.'Sbmushkovich and
V. M. Shekhter for a discussion of tho work and for critical re-
marks." Orig. art. hass 17 formulas, 1 figure# and I table.
ASSOCIATION: Piziko-tekbnicheskiy inatitut im. A. P. loffe AN SSSR
Card 2/3

ACCESSION NR: AP4019238
(Phksicotechnical Institute AN SSSR)
SUBMITTED: 15JU163 DATE ACQ: 27Mar64
SUB CODE: PH NO REP SOVt 005
Card 3/3
ENCL.- 00
OTHM: 001

SHKLY,'J6,VSEI'Y
Py-r.31T,icc Do!-s-rization of protons in ho -- I
ydraTed- paramaLmetic salts by the
method o~ miltiple rapid adiabatlc crcsslng of the forbidden line. Fiz.
-1 (MTRA 1815)
,ver. tela 7 no.5il'031-1334 My 165.
1. Fi7iko-tekhnic'neskiy institut Imeni loffe AN SS.",R, Leningrad.

_Y4
RP

-Ph&" R&UGni at
(2); 33
j R.usdanI..-(I) The ms&W fide mad. azid of the
phase dL-poatintlity which tikis pl~wd j;b~a'Ughtja reAected

fi)om - 9, dkk-ctzicjindt&l inlet ' bbtalned by selera::~-,: -
an
e
'UtL
inde
endent method
U
of th
h
f thm
t
*
s
-:4- j

ns
,
c
e
a
ze
o
x
.q=
p
Measuie. -
givan in the literatute u* shown to ba wrong,
ments m given of the aperdea af pb&,w discedidnuity
obtafiA when 4ht & raffeited from i~ airjA&-'lnj46j4M-
(3) An indmedvo fornuft is dettv
thlanan of thin fit= by an Lnwferel
Intedemcce method Ls given far doti~
18 r, F. m
2 2
:7

L 15986-60' EVIT (1) 1 SWT W/TIMP (e) IJP(a) WH
ACC NR: AP6005475 SOURCE CODF: UR/0368/66/004/001/0065/0067
AUTHOR: Shklyarevskiy, I. Korneyeva, T. I.; Ryazanov, A. N.
ORG: none
TITLE: An interferometer method for determining the refractive indices of mica
SOURCE: Zhurnal prikladnoy spektroskopii, v. 4, no. 1, 1966, 65-67
TOPIC TAGS: refractive index, mica, interferometer, spectrum
ABSTRACT: A method is proposed for determining the dispersion of birefringence in
silvered mica From a single Laterference pattern by measuring the wavelengths of the
interference lines. The procedure is a modificat';on of a previously proposed method
(I. N. Shklyarevskiy, Opt. i spektr., 6, 780, 1959), and may be used for measuring
the dispersion of refractive indices 1j, and V~ of mica in the visible region of the
spectrum. Equations are derived for determining -these indices and dispersion curves
for the indices of refraction are given. The results agree satisfactorily with the
tabulated values for the indices of refraction of Ural muscovite. Orig. art. has:
4 figures, 5 formulas.
SUB CODE: 20/ SUBM DATE: 19.Apr65/ ORIG REF: 004/ OTH REF: 002
Card UDC; 535..417

1. 31535.-66 -3,4TO-) FQQ fTJ
SOURCEt /2789/6 5-/-06-6/6G6/-607*3/oo8o7
ACC NRI A;F6005154 CODE: UR
AUTINOR: KorobOv. M G - Shk_ My, V. G.
eVB
ORG: Central Aeroloiftal ObservqqTy (Tsentrallnaya aerologicheBkaya obdc~~vbioriya)
Y
udines by the st~~op
TITLE: A study of the topography of the upper boundary of clo
metric method
V/
SOURCE: Tsentrallnaya aerologicheskaya observatoriya. Trudy, no. 66, 1965. Aerosinopti-
chesldye i aerologicheskiye issledovaniya (Aerosynoptic and aerological research), 73-80
TOPIC TAGS: stereophotography, aerial photography, atmospheric cloud
ABSTRACT, The stereophotog-rammetric method applied in geodesy is employed for the
topo!~raphic study of the upper surface of clouds, using aerial photography. Disregarding the
physicall f-uctors in the origin of the nonuniformities on the cloud surfaces, the method makes
it possiiolc to determine tht'2 altitude of the clouds with sufficient accuracy. It is feasible to
measure the height of cloud elements over other cloud elements by means of aerial photography:.
Knowlc of the scale of the photographs makes it possible to determine the lengdb of the cloud.
waves a-,~ well. Th(-- calculations performed in the article show that the correction device
of the stereometer may satisfactorily serve only sme.11-scale aerial photographs. In conclusiori'
an evaluation is made of the accuracv of the determination of the excesses of the cloud elements.
obtained by the stereophoto.vrrammet~ic method. Orig. art6 has:'4 figures and 14 formulas. L
SUB CODE: 04, 14 //SUBM DATE: none / ORIG REG: 004 / OTH REF: 001
Card 1/ 1

TrI.-
of
I f R~-
it -

SOV/137-58-12-24qio
T ranolation from. Referativnyy zhurnal MetallUrglya, 1958, Nr 12, p 128 (USSR)
AUTHORS Vintsel , G . Shklyarinsk.is, D.
T,TLE On the Preparation of High-grade Manganese Plating by Electrolysis
(K voprosu polucheniya kachesTvenrvkh pokryiiy pri elektroosazhdenil
iiiargantsa)
PERIOMCAL. Uch zap VO nyussk 1_111-1. Ser maten-i. , fiz, 1 khim n., 1957;
Vol 7, pp 133- 137
A,BSTR.t~CT The electrolytic deposit-ion of Mn from -A sulfate electrolyte (El was
Investigated A study was made of the effect of the ca!hode cd. the
ternperature. pH of the solution, concent ration of Mnzi~ and additives
on the current efficiency expressed in terms of the yield of metal
and the quality of the coating (C'. A glass membrane was used in
the electrolysis; Cu was used for the anode and graphite for the
cathode. The optimum composition of the E and the parameters of
the electrolysis were established The catholyte was (in g/literl:
'IvInSO4 2
I 4H20 250, (NH4)2SO4 I DO; the anolyte was (NH41-SO4
100; pH3 2 - 8 8; the E was stirred. High- grade C are produced
Card I /Z within a narrow range of the cathode-cdIremperature curve 0,vithin

SOV/137-58-12-24910
On the Preparation of High-grade Manganese Plating by Electrolysis
the range of cathode cd = 8 - 23 amp/dm2 and 0. 5 - 200C); at any given temperature
the corresponding cathode cd sho,ild be selected. A deviation in either sense re-
sults in a sharp deterioration of the quality of C. The current efficiency increases
with the increase in the cathode cd. The pH of the solution rises with the progress
of electrolysis; at pH > 8-8 the quality of the deposits deteriorates and E should
be acidulated with H2S04. A decrease in the concentration of Mn?-+ ions and Mn
ions of a different valence exercises a negative effect on the quality of C and cur-
rent efficiency. At 180 and cathode cd = 20 amp/dm?- the current efficiency is 21%
when the concentration of MnS04 - 4H20 is 83 g/liter and 33.3% when it is 250 g/
liter Dendrites form on the edges and corners of the cathode as the growth in
thickness of the deposit progresses. Addition of glycerol ( '40-50 g/liter) improves
the quality of C, whereas addition of joiner's cyl--ie lowers it.
A, L.
Card ?_/Z

SHKLYARNIX, V..mladshiy serzhant
Training device for shooting from a tank. Voen-vest. 38 no.11:
80-82 X 158. (MIRA 11:12)
(Tank warfare)

N
GALKIN, 0,; SHKLYAREVS.'Kly, I*W-
~*-kww&4*-,-Y,-W,.~.mw~~ .
Change in thn optical constants of 'tin during transition into a state
of superconductivity. Dep.All UM uo.6:445-447 #54. (YI-RA 9:9)
I.Fizike-tekhnichniy- imstitut AN UMM i Kharkivslkiy derzha-vniy uni-
veraitat. Predstaviv diysniy chlen MN MM K.D.Simellnikov.
(Tix--Optical properties)

J.N.
An interference method of daterrahing the refraction of
~Uuld and solid bodies. 1. N. Shkiyarevskil and V. Ic
oslavskil. Zhur. Tekh. Fis. 24 1387-91(1054),-
semitransparent mirror reflects the jight of a point light
source on a set of interferometric plates consisting of glass
p;ates coated with Al. The plates are- held by a micrometer
arrangement In such a way th:tt the spaces form wedges that
are filled with the llq~ld to betestc~, Thereflectedli t.
Is measured with& spectroscope. nzanbedetd.tothe4th
of
ddmal., Curves are presented showing x as a function
the wave leugth for ZnS (Wedge eva;d. an the glass plate
and aluminized), lodomethylene, ard a 2% s~ln. of an
traphioxine-fuchsin dyed S. P.~'
s
a

USSR / Optics K
Abs J=% Referat. &%ur-Fizika, 1957, NO L, 10340
Author ERtnel'nikov, K.D.,.Shk1yarel(skiy., I.N.,, Skarobogatov, B.S.
Inst Not Given
Title Determiration of the OptiC31 of 3,~Ymartur;.
Orig Pub: Uch. zap. Kharkovsk. un-ta, 1955, 6~, 13--.-i4o
Abstract: The index of refractior.,At of thin Sezmanium filn~ -vas me~_Sured Ily
the germanium =wedge method, coated in WLCUM OL gla55 Or On 5il-er.
The average value , in the given region Df tYe ze-Jg,~ thickness vas
,4 A /: ' - - -
I I k,- ) -where
o-,tained from the equation,,7Z = ~ "k mi~:. -4!-k max,
,-k min and tkmax a--e the thicknesses of the vedge in th,-
locations of the Mth imt-' rference min-kTrim aad maxi-mum f:)_r a giv~-._q
wavelength. For A 590 r~A, the value 3f,- r, is inlezendent of
all the way ip to t the order of 4 x 1C%-- cm. a:2~1 eauals 3.6
This shows that the st:nuctur-e of the fiLms In-=H Y.,ot _-hanwe wilh
is 4.? and.
'hiclkne:~s . For X, = 690 ar~(~ 550 I.-he of
Card l/ 21

z
Category USSP/~-ptics Physical Optics
Abs Jour Ref Zhur - Fizika, No 2~ 1957, No 4938
K-5
Author Shklyarevskly, .1,N., MJ.I~slavskiy, V.X.,Fakhomova, O.S., Ryazanov, A.N.
Title interrerometric Method for Determining the Dispersion of Liquids in the
Ultraviolet Region
Orig Pub Uch. zap. Ehar'kcvsk. un-ta, 1955, 6, 147-150
Abstract The Iceviously described (Referat Zh. Fizika, 1955, 23123) interfero-
metric method for determining the dijpersion of liquids and solids, based
on the application of the lines of equal chromatic order, has been
expanded to determine the dispersion of liquids in the ultraviolet region.
The investigated liquid is introduced into a gap between aluminized quartz
plates, which are attached to the slit of an ISP-22 quartz spectrograph.
The thickness of the gap is regulated by means of screws. The resultant
spectrogram is used to determine the wavelengths of many interference
lines.-to determine their interference order, and knowing the thickness
of the gap, to calculate the index of refraction for many wavelengths.
The crder of the interference is determined by filling the gap half with
card 1/2

VMKIN, B.I.;MILINER, A.S.; Rf)ZFMSVEYG, L.N.; Y.AYNJUWr, YA.B.,- EfOUBVICH,
V.I.; SHKLY.AR7,VSKIY, I.N.
Sections of Experimental, Theoretical, Faid General Physics at the
Department of Physics and Mathematiesp 1.930-1955. Uch.zAp.XHGU
60:63-79 155. (MIRA 10:1)
(Kharkov University-History)
(Physics)

"- /. t' t /k ~
SIMINIKOV.-K.D.; SED&AUTSKil), I.H.; KM, E. A.
173"" awwoomwFAW~
Interference of light in thin silver, foils. Uch.zap. KHGU.
64 no.6:127-134 '55. (NM A 10: 7)
(Interference (Light)) (Metallic films--Optical properties)

SIIIM'NIKOV, K.D.; SIIKLYAREVSKIY, I.N.; SKOROBOGATOV, B.S.
Determination of the optical constaats of gormqnium. Uch.zap.
KHGU 64 no.6:135-14o '55. (MLRA 10:7)
(Germvinium-Optical properties)

USSR/Optics Physical Optics. K-5
Abs Jour Referat Zhur - Fizilca, No 3, 15,57, 7698
Author S-inel'nikov, K.D., Shklyarewskiy, T-N., Lupashk.o, Ye~A.
Title Optical Properties of Intermetallic ComDoLuids. Z*nc-
Antimony CompoiLnd.
Orig Pub Uch. zap. Khar'kovsk. tui-ta, 1.955, 64, i4i-144
Abstract The antimonoid of zinc (1) was obtained with S.A.
Vek-shinskiy's metho-1 by simultaneous sXblimation of zinc
and antimony on class in vacLnuii. A portion of the com-
plex film corresponding to I was obtained by measixing
the specific conduclivaty, which for I is 2.5 x lo-3
ohm-l cm 1. such Qortions have an increased transuaren-
cy T and at thicknesses t ;~;;' 1,000 A they have a brown
hue in transmitted light. The dependence of T on /\\
was measured with the SF-4 zDectroDhotometer in the 350
-- 110r) m ~e rnziI-ler of f-ilins of diffe-
,,t, in a larr
rent t, and the absurD+_L:_--n c-Deffici.ent, t, X was calcula-
ted
Card 1/2 28

Abs jczu7

the

- (T, /To) L (+
1
se
'
f
A
13 t
'
o
~

'U
P
S
i L'C) 11ka -
-
,
nc t
ie

ta -,;he. Lj
'
.
h

+
'
"Y
-- - -- ~. t_
_
cl: t-h
f'
the rail-7Q
l'on
20 e tet-jper,,~~tt,,
.
I -
i
Card 2,i2

USSR/Optics PhyBical-Optics,' K-5
Abst Journalt Referat Zhur - Fjzjka, No 12, 1956, 35731
Author: Sinel'nikov, K. D., ShkIlyarevsk-ly, I. N.. Vlaaenk. N. A.
ins titution: None
Tftle: Optical Characteristics of Complex Yaterferenz-e
Original
Periodical: Zh. tekbn. ftziki, 1956, 26~ i1o 1, 96-1o1
Abstract: For the green region of the spectinm, complex interfer-anc~! ligh-J,
filters were prepared, consisting of 3 reflecting layers and. 2 d-J-
electric layers between them. The d-ielectric used was bar--'=
fluorideY and the reflecting layers were silver. in some cases
the third reflecting layer was a multilayer dielectric coating.
The optical characteristics of 4qoh light filters were investigated
using a matching method previously proposed (Uch. zap. Kh&r-kovsk.
gos. un-ta., Tr. fiz. otd., 1955~, 6; 147). The. transmission band
was recorded with a DFSJ~ spectrometer w-Lth a di�ffraction g-rating,
having 600 lines/mm. it was shown that the-transmi-ssion band rf
Card 11/2

USSR/Optics K-9
Abst JouzrDal: Referat Zhur - Fizika, No 12, 1956, 35731
Abstract: complex light 11*Ilters 1.3 5-10 times narrower than in sfmPle I-n+.-r-
ference filters (30-100 A instead of 2oo.-.400 A and -the IIMMS-
parency j_9 1.5-2 times better (30-6o% instead of 20-30%). The-use
of a miiLtilayer dielectric coatin,3 instead cf a silver
layer -Irdproves the quality of the filt-e,rs. P_ixthex impr-~-Ment
the ovrft.cai characteristics lies al,~ng the path of re~pla--'jcg -,f all
the s~.Iver lay-ars with multiple,-Iayi~Ir
Car-I 2/2

SHKLYAREVSKIY, I.N.
~,, ,
Phase correlations on the dielectric-metal boundary. Zhar.tekh.
fiz. 26 no.2:333-342 F 156. (MLRA 9:6)
(Dielectrics--Optical properties)(14atals--Optical properties)

5,7~
T OF-M
URBJ;=
awl
.
OF TM LAYERS OF MC LTIrdM -AMCRYOEM
SU 9
and
n tekh rtz.,' V61, 26, Md. 656
SchiLIZ ird lichegmer (Absti.
Contrary to the fir-dIngs
1762/io5t), ttie autbars have fourd thzt the ~re t v e jader.-
of

a (as used in mult layer ciaangB) Is
thin ZAS fum

qual
r$j2. - I - . ' %
to Uat of Zr.9 to bulk, whereas, the refraaive; tnetex arc
Zte IUM depeads cn their tWOmess. rhe "fWIn&I.If4Ctor of
-
(porous) cryata (Ums, whoa a go re o. have'3-temilUe d wittt
t
+r"

"At tow f0
inacimPt ve
a, m the:refmcti'v6
PS its a I (ts';
-
-
sub tmc~ in its Fares M-Petuvely,
Cryolfte 2'
'
Whus % IU *e cryaWe an4 -
;d are th~ ira(:W
-
pores (q, + ih
Ims b4c i
n fdur4ia J"1664li
w
expeftment, Otfs flud .proves, 14 turni alit the UqW44
used (glycerol,- pkraffin 60, z4)
Poo l; W~
d-

51-4-20/25
AUTHORS: Sinellnikov, K.D.,.Shkiyarevskiy, I.N. and Vlasenko, N.A.
TITLE: Complex interference O*ptical -fjlt-~~-rs with improved charac-
teristics. (Slo&1rmyW interferentsicnMye svetofilltry s
uluchshennymi kharaKteristikam:L).
PERIODICAL:110ptika i SDektroskoDiyall (Optics and Spectroscopy)
Vol.2) No.4, pp-534-536 (U.S.S.R.)
ABSTRACT: This note describes construction of several types of
optical filters and is the continuation of earlier work by
Sinellnikov et al. (Uchenye ze.piski Kharkovskogo gosudarst-
,o otdeleniya, Vol.6,
vennogo Universiteta, Trudy fizicheskog
147, 1955; Zh. tekh. Fiz., Vol.26, 96, 1956). MlD1M2D2M3
filters (Mls are reflecting layers and D's dielectric layers)
were prepared as follows: to an MlD1142filter (Dl of barium .
fluoride) an M3 layer in the form of a glass plate was attach-
ed and D2 was a wedge-shaped layer of air between M2 and M3-
The filter was made "consistent" by illumination with white
light,observation of-the resuLlting interference pattern via
a spectroscope and appropriate adjustment of D2. No numerical
values of the characteristics are given. M1DlM2D2M2D114l
filters., with Dl of barium fluoride and D a layer of air,
similar to those of A.Hermanaen (Nature,-i74, 216, 1954)
Card 1/2 were prepared. With reflection coefficients Rl 83% and
51-4-20/25
Complex interference optical filters with improved charic-
teristics. (cont.)
R2 :-- 93% for M1 and M2 respectively, an overall transmis.sion
of 30% was obtained with a pasts band,(centred on 5000,R) of
only 45 A and "Contrast" of about 10-2. A method of prepar-
ation Of-filtersp similar to that for Fabry-Perot etalons,
is also described. Two high-quality glass flats were covered
with the usual layers (silver Euld barium fluoride) by vacuum
evaporation; they were the MlDjy2 systems. A wedge-shaped
layer of air D2 was left between the two plates. Light from
a monochromator (of wavelength of the maximum of the filter
pass-band) was made parallel bit means of a lens focussed on
the exit slit of the monochromator. This light was directed
on to the filter. Iffinen 1) was wedge-shaped hundreds of inter-
ference lines were visibie. When the two surfaces M2 became
parallel the lines disappeared and the illumination became
uniform. Then) keeping the plates parallel, they were adjusted
by screws to give maximum uniform illumination
state). There are 1 table and 6 references (4 0 ("consistent
Slavic.) f which are
ASSOCIATION: Kharkov State University.(Khar'kovskiy Gosudarstvennyy
Universitet.
1'"'k SUBMITTED: September 15, 1956.
ird 2Y2 AVAILABLE.- Idbrary of congress

Dispersion of the Phase Change of Thin Aluminium Layers. 51-5-15/26
ively, and were obtained for a sample shown in Fig.la. The
upper diffuse lines are due to Al-ZnS-air; the lower lines
are due to Al-ZnS-Al, with iron lines (for calibration)
superimposed on them. These lines are displaced towards
short wavelengths by a value which. represents a negative
phase change at the boundary ZnS-Al. The phase changeg
denoted by *(ZnS-Al), is plotted against wavelength, X , in
Fig.4 (the continuous curve represents the present authors'
results, the broken curve- the results calculated from
optical constants of Al measured by O'Bryan, Ref.5). III and
IV in Fig-3 were obtained for a sample shown in Fig.lb,,
The upper lines are due to Al-ZiiS-,,U (thin layer:-195 71).
They are displaced towards longer wavelength which indicates
that the phase change on reflection at a thin Al layer is
less than at a thick layer. Fi,g.3, V was obtained for an
even thinner Al layer (50 ISQ and the phase change was found
to be still less than in III and,IV. On decrease of layer
thickness to 50-80 A the displacement of the equal-
chromatic-order lines was greater than in the absence of
such layers. Presence of such layers on ZnS deterioriates
Uard 2/3 the sharpness of these lines. With decrease of the layer

Dispersion of the Phase Change of Thin .~,.luminium Layers. 51-5-15/26
thickness the phase change beco-.11es negative (Fig.5, where
numbers at each curve denote layer thickness in angstroms).
Fig.6, I, shows dependence of the phase change * on thick-
ness t (in 11) for X = 5500 1. Curve II in Fig.6 is
calculated from the optical constants for bulk Al given by
01 Bryan (5). At the top right-hand corner of Fig.6 two
parallel dashes denote the value of * for bulk Al. The
results in Fig.6 are taken by tile authors as an indication
that the optical constants of thin Al films vary with thick-
ness. This conclusion forms the basis of the authors'
e�planation of the observed behaviour of Al films. The
authors thank Prof. K.D. Sinell.nikov for ad-vice. There are
7 figures, 13 references, 8 of which are Slavic.
I
ASSOCIATION: Kharkov State University. (Kharlkovskiy Gosudarstvennyy
Universitet)
SUBMITTED: October 15, 1956.
AVAILABLE:Librai7y of Congress.
uard 3/3

Doiible refraction of fluoride films. 51-5-16/26
The absolute size of the particles, so long Pas it is smaller
,th, is not important. For many substances
than light wavelenp
the dimensions of microcrystallites and the distances be-
tween them tLre considerably smaIler than visible light wave-
length, and therefore in that region one would expect
anisotropy of the film. Double refraction was, in fact,
found by the authors in films of CaFo, BaF2, LiF, PbS9 V205
and other substances obtained b- deposition on a glass
Y
base in vacuum.On introducing such a film between two
crossed nicols one can observe fairly strong transmission
in the field of vision. This transmission is at maximum
when the glass with film on it is so oriented that the dir-
ection given by the cross section of the plane of the base
,.-tith the plane of incidence of the evaporated molecular
beam is at an angle of 450 to the direction of polarisation
of the -nicols. Wetting of the film by liquids of various
refractive indices decreases the intensity of the transmitted
light. The transmission becomes zero on wetting with a
liquid whose refractive index is equal to the refractive
index A, of the bulk substailce. Double refraction of
the fluorlde films may be also studied by an interferometric
method. On a glass plate a semi-transparent silver layer is
Card 2/3 deposited. On silver a calcium fluoride layer in a form of a

Double refraction of fluoride films. 51-5-16/26
symmetrical hill is deposited which is then covered by
another semitransparent silver layer . In monochromatic
light a system of double rings is observed (Fig.2)'. The
equal chromatic order lines are split in a similar way.
(Fig-3). The results show that ":he fluoride layers possess
biaxial double refraction and that the -plane of the optical
axes'coincides with the -plane of incidence of the molecular
beam. The orientation of the refractive index ellipsoid
relative to the layer of the filia depends on the angle of
incidence of the molecular beams on to the base in the pro-
cess of the deposition of the film. The magnitude of the
double refraction also depends oil this angle of incidence.
The results are shovm in Figs.6 - 10. There are 10 figures,
and 11 references, of which 8 are Slavic.
ASSOCLA,TION: Kha~kov State University (Zhar1kovskiy Gosudarstvennyy
Universitet)
SUBMITTED: October 15, 1956.
AVAILABLE: Library of Congre'ss
Card 3/3

51-5-1?/26
A
Measurement of the Optical Constants of Tin by an Inter"erometric
Method.
and mica were used. ZnS was deposited in vacuum at
5 x 10-5mm I~g. Thin leaves of mica were all obtained
from the same samnle. The sample was fixed in front of a
Tolansky (Ae~.4)spectrograph.The interference fringes were
photographed in reflected light. As a result of the phase-
charge differences at the boundaries dielectric-silver and
dielectric-studied metal, the interference bands due to
the system Ag-D-M are displaced with respect to the bands
due to the system Ag-D-Ag. The interferometric method
C,
described here is applicable o-nl- to those metals for
which the refractive index jAA- and the absorption co-
efficients )ULX are of the same orcLer when the reflection
coef-ficient of the metal is not less than 50 t0'6,0%. At
small coefficients of reflection the interference lines
were recorded immediately after -he preparation of samples.
Figs.2, 3 show interference for one of the sampies. Fig.2
corresponds to wavelengths 6500-4800 1 and Fig.3 to 5000 to
4100 The upper lines correspond to the Ag-ZnSAg part of
the sample and t1ae lower lines to the -,kg-ZnS-Sn system. For
Card 2/4

51-5-17/26
Measurement of the Optical Constants of Tin by an Interferometric
Method.
,7here
7L = wavelength in IAA... T~ie results are given in the
adjoining table and they yield a value of 2.5 conduction
electrons per atom. Students L.Sukhacheva and E.Pavlova
carried out the experimental work. The authors thank
Prof. K.D. Sinelnikov for valuable advice and interest.
There are 5 figures and 7 references, 4 of which are Slavic.
ASSOCLA.TION: Kharkov Statue University (khjx&kovs1z7iy Gosudarstvennyy
Universitet)
SUBMITTED: October 15, 1956.
AVAIL,~BLE: Library of Congress.
Card 4/4

61-4-11/26
A New Modification of the Polarization Method of Measurement of the
Optical Constants of Metals.
for the refractive index PL and the absorption
coefficient,im in terms of measurable quantities:
angle of In ce 9D , azimuth of reduced (relative)
polarization I and ph~ise difference between the
p and s components after one reflection L . The
apparatus used is shown in Fig.l. A monochromatic,
parallel, linearly polarized tby poiarizer P, at an
angle of 450 to the pL:.ne of incidence) beam falls on
plates (1) and (2) wit-A mirrors of the studied metal
deposited on them. Tha two plates are attached to a
goniometer table; one of them is fixed and the other
can be moved parallel ti) it. 'The light, reflected
three times by the meta 'lie surfaces, falls on an
analyser, A, whose angh! of rotation can be read down
to 2 minutes of arc. r is a receiver of radiation.
leirst the second plate --s in the position 21. Its
displacement to positi(':i 2 makes it possible to obtain
quintuplet reflection "' necessary. in the visible
region the source of l-_,,ht is the exit slit k0-) of a
Card 2/7 monochromator 'YM-2. r" -an prisms serve as the

61-4-11/26
A hew Modification of' the Polarization Method of Measurement of the
Ootical Constants of Metals.
Cara 4/7
the receiver. This an6le of' incidence was measured
several 'times, and a mean value was taken. bjear. values
of V wei-e also obtained. linowing Lf $ W and A
= - 600, the optical con6tants of the metal could be
calculated from Eqs. 6 arric, 7. Mleasurementsof the optical
constants of metals for lii~.-ht fallin8 from the glass side
(Fig.2) did not differ in principle from measurements
using liGht fallinE~ from ~~Iae air side. The authors
applied the method to meaL~i%urement of' the optical constants
of aluminium in the vis,*IbJ:;a re6ion. These constants
--aere Measured earlier by ')'Bryan (Ref.l), in vacuo
because a layer of oxida i'~, always present on aluminium
in air. To exclude the el"fect of oxide the present
authors used the apparatus -.)f' Fi6.2- Aluminium layers
.,ere deposited on the slz-I~Loet. AAI and CC' at b x 10-0
mm. lig. To avoid any contai~,,Lnation, for the first few
moments aluminium was evapor,.,ted on a special screen and
only then on the surfaae of t'I.ie prism of Fig.2. Table 1
Gives the results of measurem-,nts thus obtained (triple
reflection with 600)-~j This table gives (in

61-4-11/26
A New Modification of the Folarization Method of Measurement of the
Optical Constants of Metals.
This shows the great influence of the oxide layers in
measurement of the optical constants from the air side.
The highest values of the optical constants were obtained
from the glass side. O'Bryan's results are lower;
results for samples measured on the air 3ide after 6
hoi-.rs are still lower, an~L the results for samples meas-
ured 50 days after deposition are the lowest of all.
Thb authors concluded that aluminium surfaces used by
O'bryan, altho%h r~repared and measured in vacua, viere
covored by an oxide layer about 26 R thick. Samples
measured in ,.ir after 6 hours and those imeasured after
b0 days F.re (.ztii-mtted to have had oxide layers 74 and
97 R thi-(,k respuctively. Tile oxide thickrfews estimated
by the p-csent authorz ror freshly prepared .4amples
(6 hours aft----r deposition) -were several tinies hii~her than
those calculated by Hass (6hef.10) - This is tecause Hass
did not ta&c into account thu oxide la-er formed in vacua.
The autho--,s thank Professor K.D. Sinellnikov for valuable
(Ascusslons and hiE inter,~st- There are 2 figures,
Card 6/7 2 tables and 10 i,e fevence s, 4 of -.jh--',ch are Slavic.

AL.
51-6-13/25
AUTHOR: Shklyarevskiy, I. N.
TITIE: A New Interferometric Method for Determination of
the Optical Constants of 1.1etals. (Novyy inter-
ferometricheskiy metod op-Dadeleniya opticheskikh
postoyannykh metallov.)
P.EidQDICAL: Optika i SpektroskoFi-ya, 1957, Vol. III, Nr. 6,
i
pp. 638-611-0. (Ussi)
ABSTRACT: This paper describes a new interferometric method
for determination of the optical constants of metals,
based on the measurement of the difference of phase-
shifts of the p- and s-components of polarized light
at two anGles of incidence onto a surface of the
metal studied (deposited on interferometer plates).
On oblique incidence of light on the interferometer
plates a splitting of the equal-chromatic-order lines
is observed (Refs.3,4). The magnitude of this
splittinS depends on the angle of incidence 9.
increasing with increase of that angle. The long-
wavelength components obtained on splitting are found
Card 1/3 to be polarized in the plane of incidence, and the

51-6-13/25
A New Interferometric blethod for Determination of the Optical
Constants of hietals.
short-wave length ones - perpendicularly to the plane
of incidence. Splitting of the interference lines
is due to the difference of the phase-shifts of the
p- and s-components, which are produced on reflection
froiff the metal. Splitting of the equal-chromatic-
order lines can be used to find A , the difference
between the phase-shifts of the p- and s-components,
for any angle of incidence T. From two pairs of
values of A and (P the refractive index ~L and
the absorption coefficient ~LX may be found at any
given wavelength using the well-knowm equation relating
A , (p, p and ~Lx (Eq.6 on p.639). This equation
is valid for bulk metal, while the layers on the
interferometer plates are thin and semitransparent.
To avoid errors due to the thinness of the inter-
ferometer layers the following method was adopted.
Measurements were made on two identical semitrans-
Card 2/3 parent silver films at two angles of incidence.

I SOV/51-4-6--13/24
AUTHORS: Shklyarevskiy, I.N., Staranov, N.G. and Padalka, V.G.
TITLE: Measurewent of Optical Constants of Silver in the Infrared Spectral
Region kl2mareniye optichaskikh postoyannykh serebra v Infrakrasnoy
oblasti spektra)
FERIODICLL; Optika I Spelctroskopiya, 1958, Vol IV, Nr 6, pp 792-795 kUSSR)
ABSTRACT: Optical constants of metals are of great interest in the electron theory
of metals if they are measured in the frequency region-which
satisfies the inequality given by Eq. 1 on p. 792: 2 4
Vo J.4102
00
-where 'V0 is the frequency of electron collisions with the crystal
lattice and 4 is the frequency corresponding to the upper limit of
the internal photoeffect. This frequency region lies usually in the
infrared part of the spectrum. The present paper reports measurementa
of optical constants of silver in the 1-12 j& region using the methods
described earlier ~Refs 1, 2). In the first of these methcds (Ref 1)
the phase difference A = d - d between the p- and a- components Is
made equal to -1800 by multiplasreflection of light by two identical
samples. The apparatus used is shown in Fir, 1. Here 8 is the exit
Card 1/4 slit of a monochromator aMR-2; Z1, Z2) Z3 and Z4: are aluminized

SOV/51-,1-6-13/24:
Measurement of optical Constants of Silver in the Infrared Spectral Region
mirrors; F and A are a polarizer e.nd an analyser, respectively, msde
of piles of six selenium plates which are placed at an angle of the order
of 700 to the light-beam; M, and M2 are the samples of the studied
metal; B is a receiver. A parallel beam of mono-_-hromati4~ light papses
through a polarizer, which is positioned at an angle of 450 to the plane
of incidence, and falls at an anglo ? on to samples M, and M2. The
angle of incidence is chosen to make mA -1801, where m is the
number of reflections from metal ssanplas Under these conditions the
light reflected from metal samples may be extinguished by the analy-ser,
Position of the aaalyser gives the value Y1 , -which is related to the
azimuth of restored polarization T by the relationship tan Y ;Z ~ . ~77 -
Knowing the angle of incidence AP, the phase difference L and the
a:&irwath I the optical constants car,. be easily calm-ilated. The secon-'
method of "rotating analyser" (Rof 2) is based on a conversion of
eMptically polarized into circularly polarized light. The apparatus
is the same as in Fig 1. By a suitable choice of the angle of inciden-ce TO,
for a given wavelength, the condit"Lon mh = -900 is satisfied aad the
amplitudes of the p- and s-components are made equal by a suitable
Gard 2/4 rotation of the polarizer. Then the light reflected frcm metal Eurfacez

SOV/51-11-6-13/24
Measuraaent of Optical Constants of Silver in -the Infrared Spectral Region
is circularly polarized. The modulated component -which has paised
through the rotating analyser disappears and the recording instrument
shows only a constant signal. The azimuth of the restored polari-Lation
is obtained as in the first method, but i:f now represe=ta the angle
between the chief direction of the polariser and the plane of incidence
of light. From measured values of 9, & and V the optical constants F-
(refractive index) and ~Lj (absorption coefficient) are obtained. The
optical constants of silver layers produced by evaporation in va=um
viere measured by both these methods. The results are shown in the
table on p. 795 -whose columns give respectively the wavelength (in
the anrles of incidence 9, the m,.mber of reflection m, the phase
differences -h, the azimuth Y, the refractive Indices ~L and the
absorption coefficients AN - Fig 2 compares the values of the
refractive index and the absorption coefficient kcarves 1 and 2
respectively) obtained by the pres,ent authors kshown by open circles)
with those of Forstarling and PreWericksvz (Ref 7, shown by black dots)
and those of Motulevich and Shubin (Ref 6 shown by half -black dots).
All these values are shown as a function of -wavelength and they agree
Card 34/44 well with each other, except for values of the refractive index in

SOV/51-4-6-13/24
Measurement of Optical Constants of Silver in the Infrared Spectral Region
the 3'5-6 region reported in RE)f 6. in the spectral region vihare
the inequarity given by Eq. I on 1). 792 is satisfied the conduction
electron density N is independent of the wavelength If N 1!5
constant it follovs that (e
V - fk'~,-2) which should be a
straight line. Such a atraigtit line is shovin in Fig 3. In the regior.
5-12 V, the slope of this line gives the conduction electron de-Vqity
as 7.4 x 1022cm-3. The experiMerLtal points in Fig 3 in the regii=L
1-6 ~& also lie on a straight line -whose slope gives the cond--- ~~.,ticn
electron density as 5.Z x 1022=--',, vhich is the same as the numbe:~
of atoms of silver in 1 cm3- The authors thank K.D. Sinallniko-T fu:r
his interest and advice. There are 3 fiSures, 1 table and 8 referen:~A.;~,
4: of -which are Soviet, 2 English, 1 Gennan and 1 American~
ASSOCIATION Kharlk vskiy gosudar8tvennyy univer,3itet Ln. A.M. Gor*-'kogo
(KharCv State University imeni A.~A. Gorlkiy)
SUEa-TTED: November 15, 1957
Card 4/4

'a.lj r, lc'i-.- 3 h SOV/51-5-5-19/23
~'IT 11-7 On -.Lu Frobleu Cf of Thic~cLaL;,~ of Thin Lavers Usin--
Equal Chrnzj:~Li1c Ord ~r Linor. (K vopresu ob izm5renii .-ol5hchir-
tonkikh Flen-ok i pmxshchlyu liniy cavkio-o klir"..atic~asko-o por
yal a~
PSUCIDIC4L: Op!-Iiim i Spa:."roskopiya, 1938, Vol 5, Nr 5, pp 617-619 (USSR)
AUS 7: In 1945 Tolansky applied equal chrozz-a--;ic order lines lo ths st-ady of
of t plaue surfaces, usinG 1"hite li6ht. Lutier
Sin-311nilcwr and Rapp (Ref 2) applied Tolansky's mathod to measureuiew"
of t -,in fil,~ls lliopmeed in va-cu c'
or glass plates. A scratch is iaada
across such a filLa. The filia is i;hon covered (by vacuum daposi-.,ion)
by aa opaqua lay3r of silver which repeats the scratch contours fonnia-
a Six-3,11 Ste-0. Tha height of this step is equal to the orivinal film
"hic~aiqeis second glass plate is covered by a seui-trars parent
layer of silver. The two pla-las aru pressed to6ethar and ara placed
in front of a apectQrograph slit in such a -v.,ay as "m place the step,
referred to above, at right anglea, to the slit. The---e platas are
ilhaLlir,ated .~.,ith a par,,~;11-31 beac; of white lic-Int, da-:ails of the
Card 113 a 9 p-a I-;..:us !~~r-3 7iver, in Refs 3, 4. An aahra.-.'~tic lens is used to foms
Q

SOV/51-5-5-19/23
0:1 Probla:,t of of Thic~mez;s of Thin La-,,-,ars Using Eclal Jhroma-:ic
Ord ~~r Lin-~i-
Card 213
rap bj'~lv:aett i;he -lass plates on to a spectro -raph slid_
-'!he fo~:~il pla_ne of the sp3e-'rogra-,311 caiAera objective tvro s~-,Stafus of
equal chrcr_~_,Iic order lines are observed (Fig 1). The sea,_ral-ion
ba'~-i,f~cn the ".,, system-F, of lines is a fazction of the ori-irjil film
-~hickmess . Wavelengths cf borh svstems of lines vare ~.ie~_suriA in
~ho spac~ral reion 5000-6500 1. 'For auen of the systems a gmsph of
fal-ctioll nl)~z is construc~ad. Have Li = ic - 1, where k is
+ho iii-Irfaceaco ordor of a particular line. Fig 3 shows such functicnE
obtained fro.-i ~is interfero~~ram of F-10-c- 1. The difference be-1-aeL,
cr,_4ira`t)s of the tvo st.raight linDs s_~icvn in Fig 3 is aq:ual t-o t1ne
cri inal film tLickma-ss t (in the prel-ant c --- s e i -1 .7a s 2 6 0-rh- a U
t~-ickriess is of craar of sevaral wavelengths -he air gap
"he int-4rferance platei is chosen to i_-ake the m-th line of one sy t-3r_1
_i 7-oln2ide with 'the r.--h line of +he a' er systam, ar. shown in Fig 2e
~h
Then -c = Aj(fa - r)12,-vIhara b ia the original filrd thickness and Xi i~
---a ravelergth a-: -.-,hijh 'he m-th and a-th linet; of the two sys-e~l.,--

SOV/51-5-5-19/23
On the Problew of :-,aL~zurerwit of Yhi6niass of Thin Layers Using Equal Ghromatic
'Order Linas
coincide. For tha case given in Fig 2 Al = 6176 R, m. - n = 4 and
t = 1.225 The author thanks K.D. Sinellnikov for his advice.
There are 3 figures and 5 references, I of which _zra Soviet and
1 English.
SUBLaT_'ED ;April 29, 1958
1. Thin fil=--0'ePLP4rement, 2. Thin films--Testing equipment
Card 313 3. Spectrophotometers--Performance 4. Mathematics 5. Silver
--Applications

67212
sov/58 -16118.1.
P~ 0 C) -59-Y
Translation froin., Referativnyy Zhurnal Fizika, 1959, Nr 7, p 259 (USSR)
AUTHOR- Shklyarevskly, I.N.
TITLE-.~ Measuring the Optical Constants of Metals, In the Infrared Region of the
Spectrum Using the "Rotating Analyzer" Method
PERIODICAL-, Uch. zap. Khar'kovsk. un-t, 1958, Vol 98, Tr. Fiz. otd. fiz.-matem. fak.,
Vol 7, PP 325 - 328
ABSTRACT: In order to deteinine the optical constants of metals in the infrared
region, the author used the rotating polarizer method of Konn (Russ.
spelling) and Eaton (RZhFiz, 1956, Nr 2, 14657) in conjunction with the
repeated reflection of light from two identical surfaces of the metal
to be investigated, Light from the monochxomator passes through the
polarizer (a selenium pile), is reflected from the two parallel samples,
and passes through the slowly rotating analyzer and on to the radiation
receiver. By gradually varying the angle of incidence of the light
on the samples, an angle of incidence is found at which the reflected
light is circularly polarized, i.e., the signal at the analyzer is
Card 1/2 constant. Then the optical constants are calculated from the known

SHKLYA.REVJKIY, I. N. Doc Phys-Ilath Sci -- (diss) "C,-,rtain problems of metalloopties."
r,-hsrlkov, 19h9. 22 -or) (Min of Higher end Specialized Secondary Education McSSR.
Khsrlkov Order of' Labor Red B8nner State Univ im A. IA. Gorlkiy), 150 copies. Lis'.
of author's works at end of text (26 titles) (KL, 44-59, 125)
-1-

.- ..' 51-6-i-13/30
.-LIUTHOCtS Shklyar$73k-y. I.N~ and FadalL-R..
TITLE Yea~,-,reme--it cf the Gr.tical. -'ctr-.tantz sf Co-joar, Gold and Nickel in
the Infrared L~$giOP, 01: tne Spec-tr'lm (Izineraniya optichaskikh
postoya.nnyk---d madi., zclota i nib-,31ya v infrakrasnoy oblasti spektra)
PBRIWICAL: Opti~~ 1 Spaktrcakopiya, 19,19., Vol E., Nr 1, pp 78-34 (USSR)
ABSTRACT: The optical con-it-ints cf %oppar, gold and nickal were measured in the
reg~cn --~f 1-1-2 u !--y means, of the method described by Shiclyarevskiy at al
(Ro:P,n- -1, r5" .YwAittyrorzent.; were mado on a nixaber of pairs of samples
an~ c-t' tv,-) refractive index IL and -L-i46
ab,~vrpti-.n index c.. were obtaine,~ The results of measuremeata are
giver. in Table2 The saver- columns of each table give the
-wavelen~,t!.. %., th-a angle of in-;1don,~a of ttie li&t ip, the number of
7, t~ia phaa-, sti'Aft &, the azztm-oth V, the refractive index ji
and the abtcrptlon- indw-, 1,~X. The cptical conetants were calculated from
the UGL,a--, .-ro-.mula* (S,:~s 5 and ev Ythich give )i and in term of
and A. Thi,:!k layara oi copgar were prepared by vacuum deposlon on
glass platoe. b159-surements of the optical constants of copper war*
made within five daya. Control measarements carried out on freshly-,.,,
Card 1/3 prepared stunplaq yielde, the same optical constants as the measurements

SOV/51-6-1-13/30
Measurduant c.' tria 0,~tlcal Cojw~tant-7 cf Copper, C,ole. and Eickel in the Infrared
Region of the Spe:ttr---j-,
C-Tt aft,!- f-,ve 1%o e-f1*Fj--;t: of a layer of copper oxide
a--:ur-.;imfr 1-1-0 fisdrpicn (Rof 6) su~,h a layer should not
afft-ct -Iti,3 ~ptj,-al mic.-i than a few par cent. The results
kcr ~cpner era glv-.~n i-c-. Ta(,1,5 I and the derived optical constants
are Ln Fi- 1, w)-tP.,4 tha represent the authors'
dc-t:- re,-)~,a~ent thv3ts of M-3tarling and
F r 0 64- a r-J R a f La yard of go' , A; 1. 1,L thi,-k were d apos ited on
a
-,Ia~5s plate? by va--.-tam
I- Ns differenzea -were found between
c-rt;--al n--natant3 derived frcv. measuraments made seven days after
aLc' ontill-al dariy5d from weasuraments carried out
ons after rrazaraticrin of ths sampi-su . rho results are given in
Talbl,t ., aui~ the, a6fived cptir--al ;.c-n3tantz are shown in Fig 2. Again
open :-irclea denote the present author;., results and the black dots
th~ae ~:P FZ:r~atarling ana Freedzrichez (R"ef- 7). Thin layers of nickel
ware de-no:31to-d by vanram deposition cn glass plates. The results obtainod
are given in Tabla 3 and the derived optical constants in Fig 3?
where oDea circles denote the present author.:i I values, and triangles
sh-W th U
- a optlcal r~-mtants obtainad by Inc-ersoll ~Ref 8) at A= 2 IL.
Card 2/3

Measlir amen-% -~f T-h-5 C-coner, Oola arji flj;~kai
in tho Infraxed
+
t~ f-r,!,3 OILO-ArOI13 ill MatalS the
raaxation tiines and
d ~I f~.O sillrar. They are
wi-,~n "roo llod-5,-mt-s and
Beatt":~ ;jn;i w;.-r~: (.Rof~ 10,1. Fr~oi tho' 1:1.cwn -values of 11
and" -.4 it If of t1w absorption
whers R I'F te~a rof'.Q-ti%,-n oC tine matal. Dapendenca of
tha a'-,-Forrtl~,.a A wav!3langth is given for copper, silver,
A 12-'L J`Iiq -7)rd;rtAt,j aXj.S copper, gold
i ap'-111-9s to
alij t. P~-:~knoriledgmenta are made
to Pr C;'-~-X S for hi ad s . There are 7 f i gures , 4 tabLw.
and %f whIA ar-~ Scr,',3-t, 3 Engliah 2 German I Dutch and
SWi.~ITT3U-
C I r'! 6"',

24(4); ;,4k'6) SOV/51-6-4-19/29
'0. -iy, 'vdeyen~-o, ~~..A. and Padalka, V.G.
ITI, RS - Sh~clyarevu
X
IITLS; i~laasuramant of t?,,j Cotil-ai --',onj-canth of Antimony in tile Infrared S-Cectral
Hegion at -T-V-1~,--~ratizras of 2PO and llooK. (Imereniye optichaskikh
postoyanny'kh sur'ray v infrakrasucy oLlasti spektra, or-3 temoerature
290 i 1100K)
Optik-a i 10~--9, Vo, G, Nr 5,28-532 (USSR)
ix BS MICT: The optical constants cf antimony were ma-~sured at the wavelengths
of 1-12 Ii and at temperatures of 290 and 1100K, using the technique
described by ;--vary (Ref 3) v,.rhich is ess~~ntuially a measurement of
o2 = Rp/RG ,
at two angles of inciderxe (0 (RD and Rs are the coefficients of
reflection for li,~ht polarized in tho olane of incidence and at
rightangles to it).
Z~vury obt~ii:iad the rafractive (Ii) and
absorntion (1,1,j Indices from a systew of t,.-;o equations
2
fi i~?jj and (jL, 14, LP2)-
This method of caletilation is laborious and the authors used the
method of intersectinr, circles (Rof t). The procedure described here
1// 4 is applicable to tha optical constants of inetals for which Ii A:$
the optical. c-on,stant~'. of antimony satisfy thi-3 condition. The

SOV//61-b --i-19/29
~.'easuremwt of the O~tical ~Ion~-tants of Antimony in th,3 Infrared Spectral RaZiroa at
Temperatures of 290 and 1100K
ao-)aratus used for measuremwit of the optical constants of metals
in the infrarad ra;ion was described ~Rrlier (Ref I). ""he aonaratus
used in vaidio,- of antimony differed from that described earlier
(Raf 1.) in one rprti,~iilar. instead of t-xo samples on the gonomater
table a cryostat was usdd nith one sEuanla in it. Fiv 1 showa the
external viow, of the a--,oaratus. Th,3 i'ollowin- details are. marked in
Fix 1: the slit (S) of ft monoch.,cmator ZITR-2, a pollarizar F and an
analys ar -A , the. cryostat i, and a race' ver B (a ohotores istor or a
bolometer). The polarizar aud analyaer consisted each of a uils of
selenium plates which had to uza r-:3-placed every 3-4 month-S . Detaile of
the cryostat are rshoiqn s(thematically in Fiv 2. Leasurements were made
at 290 and 1100'K, (usiriE liquid oxygen in the jacket of the cryostat).
The a,.)paratur, had to b-3 adjusted very carefully in ordar to avoid
serious errors: first the selenium piles %are adjusted and then the
sample. !~easuremants ware made on four samnles: the values of the
optical constants of tha individual ssinple differed by no worc- thar.
5-81%. Controi !,;easureniant,,-i'carried out using other methods (i~6f 5j.
gave similar resulta. Fig 3 show-,~ the refractive (curves aj and
absorption (curves d', indices of antimony aa a function of -wavalr-ngtl-,
card between 1 and 12 Ii at temperatures of 290 (curves la, it) and 1100K

SOV/51-6-4-19/29
hja~,.s u 1~eaieiit5 of' the Optical- ""011574-Itzi 01' -ntimony in the Infrared Spectral Regicn at
of' 2,110 and 11OOK
2,a, i'd). Vito ~;,,Lwo f1rure contains thu vuluou of JL and
of' antimony, obta-inod at room tL~niporature and 2.45 p wavelength, by
DoinansKiy and Noskov (Ref 6); these are shown as ooints 3a and
From the meaii values of the oDtical constants the authors constructed
the -oavelength dependence of' the real 2 and imaginary
11L
[21ioi%)] components of comolex permittivity; this is shown in Fig 4.
Fig 5 shows the waveleng-th depandence of the absorption coefficient
A calculated from
A = 4,1/[(,, + 1)2 + (111)2]
Tha A = f(;L) curves exhibitclwirmaudma which are due to interband
transitions. From tha positions of -,he maxima on the A curves the
intarband energy gap was calculated. It vias found to be 0.18 eV at
room temparature and 0.15 aV at 1101K.. 'This compares well with the
Ca rd 3/4

SOV51-6-4-19/29
Leasurements of the Optical Constants of Antimony in the Infrared Spectral He-ion at
Temperatures of 290 and 1100K
values of O.o5 to 0.20 eV at room temperature reported by Smith (Rof 7".
Aciuiowledgineat is alude to K.D. Sinellnikov for his advice. There
are 5 figures and 7 references, _5 of -.%hich are Soviet and 2 Engl-~h.
SUBMITTED: May 19, 19E-3
-lard 4/4

24(4) SOV51-6-5-19/34
UnioRs S hklya revs lciy, I.N. and Avdayanko,
"
I
TI TiB Reduction of -Reflection of Metallic Coatings (Prosvetle-niye
matallicheskikh pokrytiy)
PERIODICAL. Oritika i Spektroskoriya, 1959, Vol 6, Nr 5, pp 678-684 (UssR)
ABS'rRA.CT:
A 1/2
It is very desirable to reduce reflection at the glass-metal boundary
in The Fabry-Perot interferometer plates. koe-Ang the reflectivity at
the air-metal boundary unchanged. This would improve transmission of
the olates and consequently increase -choir speed, contrast and resolving
power. Such a reduction can be achie-ved "ry evaporating a thIn film
(100-150 1) of silver on a glass plate heated to 300-4DOOC and then
depositing the main aluminium layer. Tramsmission of semi-transparent
aluminium coatings on glass pre-treated in this my is increased by a
factor of 2 to 4 in the wavelength region WO-1100 m1i (Fig 5).
Transmission of semi -trans parent coatings of silver can be imoroved
by a factor of 1.5 to 2.8 -when these coatings are deposited on glass
plates previously covered with 100-11E-13 X silver films (deposited at
300-4000C) or top of vihich very thir. alufainium layers -,are evaporated
(Fig 7). Reduction of reflection of interferometer plates proauces
a revorsal of interference 14-nen, kFi~; V.). --vine iutansitiez of the
ravors,3 line:. are hivhor thazi tkie inta_'.~Atius of linas reversed by
o

Reduction of Reflection of Metallic Coatings ~OV/51-6-5-;9/34
cutting out the "zerc-ordar" line.S. Th"S Makes it oossible to use
reflection interfarometers with a opa(Tue coatinu, in studies of
hyperfine structure. One section of tha uaoer deals witn trie optical
Pro-)3rties of tnin silver filrns dencsitod on glass plates heated to 1W,
LOO, 300 and 4rjCo;;. The optica.L constalats of such films ware found to
be similar to the constants recorded eariier for thick silver layers
d3posited on hot subctrat,,~s. These films are, granular in structL,.-e as
shorr in Fig 2. A6:nuwIed0srt 16 made to Y.X. Sinel~nikov for his
ad vi ca. There are 9 fi6ures and 13 reforane6a, 6 of -which are Soviet,
3 Ger,=--n, 1 6nglisi-- aLY-1 1 tr-n-;Iaticn frcmi EnSlish into Pussian.
a r-i
,ara

241(4), 24(3" 51-6-6-9/34
1 5 Ov/
"MHORS Shklyarevskiy, 1.17. Padalka, V.G.
TITLE: Tiio Anomalous Sk_jn-;7_ff'ect and the Optical Constants of Co:)Der, Silver,
.3old and I,-, tho infrared Region (Annmaltnyy slcin-effelcb i
o-pticheskiye postoyawiyye inedi, serebra, zolota I nilcelya v
infr-tkrasnoy oblasti SDektra)
F-ERIODIGAL; Optika I spektroskopiya. 1950, Val 6, Nr 6, pp 776-779 (USSR)
ABST,tACT: Recently the authors ;aoasured the optica). constants of copper, silver,
--old and nicicf;l at iafrarad wavelaugths and interpreted their results
in term.-5 of the class!::Rl frea-alectron theory of Drude (Refs 1, 2).
From thes,3 optical constants the authors had deduced, inter alia, the
d.c. elec-cri~7al eolld u eti, Vi ties of these metals. These conductivities
,aere foliuo to be :considerably s~rialler than the values obtained directly
on massive samoles - The reason for this discrecancy lies in the use
of disaarsion fonaulaa of Drude which are valid only for the normal
s kin-af fact, ,,jhsn the inequality Is satisfied is the mean free
,vith of electrons and 6 is the death of the "skin" layer). For good
conductor,~ at roorr, temperature the Plean free path of electrons may be of
the order of the cleptn of the sir-in layer, and at low temperatures this
?7Lth may be ~onsidaraLly larger than 4' , i.e. anomalous skin-effect

S OV/51 -6 -66 -9/34
The i'~,ncmalous SIKin--Effect a11!4 the Optical Constants Of Copoer. Silver, Gold and
"ickal in the Infrared -Rasion
conditions apply. Dingle (Refs 4-6.1 gave the theory of the anomalous
sicirl affect and derived the d:s-oarsion formulae for the optical constants
of ire-cals in-the infrared region'. Dingle allovied for the f-act that
electrons can be reflected from the ms-b-l 3urface both specularly and
diffusely. His theory involves a coefficient of spacul~rity p;
2, - 1 for specular reflection and r) = 0 for diffuse reflection. in real
raotals p lies between I. and 0. Thtj authors used Dingle's theory and the
v~i_-aas of the wpzieal nonstants of copper, silver, gold and nickel,
deteriainad earliar, ~Refs 1. 2), to calculate the conduction electron
densities IT, the relaxation tiirivq -6 and the values of (1 - p,Iv for these
metals khera v is the electron velocity at the Fermi surface). -%11 these
on p 779, cols 5, 6 and 8 respectively.
-juantities are listed in the tabl,
Thaue calculations aere --L-.de an the assi'lliantion that the electrical
conductivity of thick metal fiLas depcsited in vacuo is equal to the
conduezivity of wassive sarples. Acknoviledg7pent is made to K.D. Sinellnikov,
for his advice, There arr. 3 figures, 1 table and 8 references, 4 of which
are Soviet, 3 Engli~;h and 1 translation from English into Russian.
0
SMil'TTED: "o,,ember 26, 1958
Card 2/

24(4) SO','/ 51 -6-G-10/34
~~jTHOR: -I'mclyarev-skiy, IS.
TITLE. iiev: Interferometrit: Method of haasurinr Disnersion of Liquids
(Iicv-yy into rf a rorrietri. -has ki y :ietod dispersii zhid~'-osteyj
F:,~R_LOJICAL: Outim i Gpel,-troskopiya, 1959, V31 6, IT r 6, pp 780--e-3 (U~_"SR)
R T
-lard 1/3
I
The author at al had already described itn interfaromatric of
metsurin,r disoersion of liquids and sol,"ids tfil;-as) in the visible ~Ref 1)
and ultraviolet (Ref 21.) region5. it Y:a5 *hown kRefs 1-3) that,althaagh
the !aethod has the advantap-a of high soead comnared with the method
Q
described 1,y 0breJ_'mo,7 (Pef 4.1, it vns not very accurate because the phase
shift at the dielectric-uletal boundary was neglected. Tile present paper
describes a modified method which dces not have this disadvantare. The
effect of dispersion of the phase shif-~ is --illomled for in the saneway .;:s
in measurement of thickness of thin films kRef 5". One of the inter-
farometer ol;ates is nolished in such ;a vav as to form. a steo of 2-3
thickness ~FiG la). The second plate is In optical flat. T-he inte~w7...;
surfaces of tho two plates are covered by semi -trans Da rent layers of
silver or alumini-,ua ~tha latter is used for i!iaasuramants in the ultra-
violet region). The metal coating on the plate with the step is ruled in
several olaces (Yig 1d). The scratchos F so fonaed are used later as
a

A New Interferometric .-,ethod of Dis,,arrsion of SOV/51-6-6-1-0/34
1: - Liq~airls
the dat7,ua marics. The two plates are pressed against each Othe.- and
placed in front of a spectrograph slit, as shown in F-iog 2. In the focal
plane of the objoi-tivn of' tne s r)o:,*tro grit ph c-uiiara two syqtoiai; of equal-
chro:aatic order lives are obsorved; they are due to the two different
thickntisa"-.1, of the air ~-Aps. tj Und tA, stown in Fir, la. The plates are
Placed oil in object tablo and are itioved In a horizontal direction
parallei to th~3 --~laxie of tho coactroZraph slit. 'Xilen one of the scratches
P is foo-ised on the slit,the interference pattern disappear!3. '71"len tills
hapoens the reading of the drum of the mi::rcraeter screw of the object
table is noted aDd in this way two or thrae oositlons cf the scratch qiarks-
a-e recorded. The height of the step is determined exactly at several
places between the scratelles. This height is deduced fr=
t
-.-ibere ;k is the -.,nvalength at which two interference lines of ox4er M and n
(one f::-am each systm) coincide (Ref 7). Since the wavelength can be
found to within 0.1 X, the stop height may be also de'..3rmined -.-;ith the
same accuracy. To find dispersion of a li(Tuid it is Dlaced in the ggap
between the interferer2s olates, and the interference pattern is recorded
for one of the ;places -share the stop height t --s L-nown exactly. T h --t
refractive index of the liquid is deduced from the difference between
rd 2/3

A rem Interforoyaotric Lethod of Y"eaSurin& Oirror3ion of Li-z2-zids
the ordinates of the follo,~;inF, tao curves: m~/Zt = f(X1 anei
2t = tp(X). Such a ~-,rocedure excludes the effect of the dispersion
-111/
of the phase shift at the dielertric-metal boundary. The order of
interference is determined as follo,,.,s. Lei; Xo and )Ll be the wa-velengths
t~
of t7wo neighbouring lines. If the (.-orresponding refr-i,:tj.vg indices of
the liquid jLo and ~Ll do not differ too rrich, then
m = Al/O~,, - X;), -
The value of m shculd be rourAed out to the nearest integer. The true
order of interference -.-- equal to (m - 1j, -.s sho,.-;n in Ref 34 -rhe
method described abovc- is suitable also for measurements in the ultraviolet
region. In this case the source inay be an iron arc or spark. The
axoariraental tachnique for this case has a'-read,,, been described (Ref 2,;.
G.Y. folyakova and S.T. V,9r,';1,cvtseva tooic xirt in experiments designed
to trv out the mothod descrIbed above. Aci:rowledgment. is made to
.K.D. Sinellnikov for his ,.idvica. There ara 3 figures and 6 Soviet
ref orancez; -
SUBKITTED: Deceiaber 26, 195~3-
-a
rd 3/6

SOV/51-7-4-23/32
'UTMt~;: \,_. L~ hklyu revs kiy, 1,111., Vurkhovtsova, E.T. and Polyakova, G.N.
TITLE: On the "Vernier Effect" Obviarved when the Thickness of Thick Layers
is -'-aasured Usino an Intarferomatric Ilethod.
0
PMUOD-101.~L: Optika i spektroskopiya, 1959, Vol 7, Nr 4, pp 566-5C,8 (U~~4RJ
-0ZTR.CT: in a preceding; paper Shklyarevskiy (Ref 1)' described an interferometric
wethod of measuring thickness of thin and tj-dck films. Two plates
were used, distance t, apart. A layer of thickness t deposited on, say,
one half of one of the Plates, reduced the ai; gap locally to t2,
i-8- t = ti - t2- If these plates rare DLaced in front of a
spectrograph slit and illuminated with a parallel beam,of white
light, then two syst&as of equal-chrowatic-order lines were observed
in the focal plane of the spectrograph camera. By selecting the air
gaps t1 and t2 it was possible to make one line of m-th order of one
system to coincide with ann-th order line of the second system. The
wavelength No of the coincident lines and their inzerference orclers
determine the layer thickness;
t = (m - n)),0/2.
Th's formula is indeuendant of the phase shifts (Ref 1). A new
Ca rd 1/3
I coincidence betweeL lines of the aqual-chrcozatic-order systems should

SOV/51-7-4-N/32
Ort tne "Veraier Effect" Observed when the Thickness of 'Nicir Layers is ~:eeisurod
Using an Interferometric !~:fathod
occur after k lines of one system and (k + 1; lines of the second
system, i.e. the so-called vernier effect 3hould be observed . The authors
show that tne eyact vernier affect would be .' jossiDie only ii: tne
dispersion of the phase shift wds absent. If such disparsiou occurs
exact coincidence of 2iore than one pair of 1~_ne5 is impossible. "."han
not even one _ttir of lines is coincident on an interfarogram, the
film thickness can be calculated using
M)o ax0l
t = t1 - t2 7
2 2
0, th a t-no
v4bere n and La arg the orders andX N, are the T:~.velengths o~
lines which abaost coincide. Yaglact- of the chase shiiTai in :;q "10)
leads to an error in the fifth olaeo. 2his is uni-aporthnt in measureLlenT,
of thicKnesses of rho order of several microns as shown by the practical
exam-ple of a ZnS layer whose into rf -3 rogram is givan in a fi--.ure on p 568.
THa wa,.alar:-ths and the interf-3rence orders of tna almost coircidoat lines
Card 2/3

SOV/51-7-L--251/32
on the "Vernier Effect" Observed -when the Thickness of ThicL- Layers is Yfeasured
Using an Interfarcmetric Ilethod
shown in the fizure, are listed in a table on p 568. The mean thickness
of the ZnS layer, calculated using Eq (10) -was 49998-45 1, -which differs
only slightl I om 50 000.2 1 calculated using Bq (1) for the
A = 5263.18 Acknowledgment is made to K.D. Sinalinikov for his
advice. There ara 1 figure, 1 table and 5 roferances, 2 of which are
Soviet, 2 English and 1 translation from English into Russian.
SUBLaTTED: Karch 27, 1959
C;ard 3/3

yt
-Imz
of
7 no.
GPV
on L;.L.7

68889
s/o5l/Woo8/o2/016/036
ni
E201~~3A-I.
AUTH01"_: ShklyArevskiy, I.N. and Sharano 0 11
TITLE~ of Measuring Optical Constants of
Metals
PERIODICAL: Optika i spektroskopiya, 196o, Vol 8, Nr 2,
pp 239 - 242 (USSR)
ABST%1kC*_-`: The paper describes a photographic method of measuring
optical constants of metals in the visible and ultra-
violet regions. This method is a modification (in
experimental technique and in calculations) of the
Shkiyarevskiy et al polarization method of measuring
optical constants of metals in the visiole (Ref 1)
and infrared (Refs 2,3) regions, based on the use of
multiple reflection of light from two parallel identical
samples. Th;e apparatus used is shown schematically in
Figure 1. Whie light from a source 0 proceeds via an
achromatic lens L 1 and a polarizer P to reach a
sample (2) from which it is reflected to another
sample (1) Several such reflections occur between
the-Wo samples and then the light proceeds via an analy

68889
S/05l/6o/oo8/oz/ol6/036
F_2yl_~E~2_jant,
A Photographic Method of Measuring Optica a of Metals
A , another achromatic lens L 2 to a spectrograph
slit S . By suitable selection of the angle of
incidence on the samples q)l one can find a certain
wavelength At for which the phase difference _mA 0
after m reflections from the samp, Los will be 180 C.
The wavelength X1 is extinguished by a suitable rotation
of the analyser and the value of X1 is found by
comparing the extinguished band (line) with a
calibration spectrum. The procedure is repeated for a
different angle of incidence W'' and a corresponding
wavelength %''- is found. In this way we can construct
a curve representing y = f 1 (k) f or -AI = -600 (triple
reflection, m = 3) Similarly, a curve representing
(P = f2W can be constructed for five-fold reflection,
when A2 = -36' Using these two curves we can find,
Card2/5 for any given wavelength, two pairs of values:

68889
S/051Ao/006/02/016A36
EjOl Y3~lnstants of Metals
A Photu,;L,aphic Method of Measuring Op ic 0
'Pi" 'i ~ - 600 and y., 48 2 = -360 The refractive
index IL and the absorption index Ii are given by:
2 2 2 1 2 2 2 2 2 2 2
IL (a b + sin (P) -V(a - b + sin (p) +.- 4 a b
=~2 2
(a 2_b2+sin 2Y) +. (a 2 b2 + sin 2T)2 + 4a 2b 2 1/2
II)C 2 2 V
wh ere
b tg Altg A2(s'n (P it g2(Pl sin (P,tg 2(P2)
2(tg A 2sin y 1tg yl - tg Alsin Y2,tg Y2)
C a r d'j./-:-)

V18211,
S/051/60/00 0 016/036
E281/Eg2j ConstiLntS of Metals
A Photographic Method oif Measuring ptl
and
2
a =Vsin'Tlt g YJ - b2 2b.ctg A s in (p1 tg (P1 (5)
2 (6)
sin (p - (sin yl + sin ~P.)
2
If sin 2~O It:Z:: s i n2Y2