SCIENTIFIC ABSTRACT ROZENBERG, G. V. - ROZENBERG, G. V.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
• Document Release Date: July 13, 2001
• Sequence Number: 5
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

Collection of Articles (Cont.) 811
PART I. GENERAL PHYSICS
Andreyev, N.N., Member, Academy of Sciences. Comments on the Thermodynamic Theor-y-
of Electrostriction (January 1953) 5,
Arkad'yev, V K., Corresponding Member, Acadezirj of Sciences (Deceased). Simplest
Fom of Solid Bodies of Greater Than Limiting Volume (June 1953) 11
Botvinkin, O.K. On the Variability of Some Physical Constants in Industrial
Glass (May 1953) 27
Vartanyan, A.T. Photoelectric Phenomena in Pigments (January 1953) 30
Vershinskaya, V.F. Relationship Betwen the Height of a Mound of Loose Material
and Grav-1ty (June 1953) 51
Volarovich M P Investigation of the Uniformity of a Stress Field and Study,of
!-@e oce'ss of Formation of Cracks in Double-shearedSamples (January 1953) 57
Deryagin, B,V,, Corresponding Memiber@ Academy of Sciences, Karasev2 V.V.,
Card 2/6

Collection of Articles (Cont.) 811
Zorin, Z.M. Boundary Phases as a Particular State of Aggregation of Liquids
(June 1953) 65
Predvoditelev, A.S., Corresponding Member,' Academy of Sciences. On the Heat-
conductivity and Viscosity Coefficients of- Liquids and Compressed Gases
(June 1953) 84-
Rebinder, A., Member, Academy of Sciences. On the Nature of Plasticity and
Structural Formation in Distributed.systems (September 1953) 113
-Rosenberg,-.-G-V. On the Problem of Reflectivity of Tinted Turbid Media -
(July 1953) 132
T21inai, A.A., Rosenberg,,G.V. Experimental -Iavestigation of the Teflectivity
of Tinted Turbid Media (July 1953) 143
Tolstoy, D.M. Sliding of Liquids and Distributed Systems Along Solid Surfaces
(April 1953) 159
Shuleykin' V.V.,.Member, Academy of Sciences. Cause of the Bluish Tint of
the Sun and the Moon (July 1953) .222
Card 3/6

Collection of Articles (Cont.) 811
SECTION II. BIOPHYSICS AND PHYSIOLOGY
Aladzhalova., N.A., Maslov I N.M. immediate Changes in the Liver due to the Effects
of X-rays (February 1953) 227
Asratyan, E.A., Corresponding Member, Academy of Sciences. Effects of Transverse
Cutting of the Rear Hald of the Spinal Cord in Dogs (Contribution to the
Physiology of Spinal Shock) (July 1953) 236
Demirchoglyan., G.G. On the Initial Stages of -the Visual Process (July 1953) 254
Yefimov, V.V., Oltshanskaya., N.M. quantitative Determination of Elasticity of
Relaxed and Tensed Muscles and of Diseased Muscles While Bathing (on the Para-
doxical Relationship Betveen Relaxed and Tensed Muscles) (July 1953) .274
Kovalevskaya) L.A. The Pover of a Moving Fish (JulY 1953)
Kuzin, A.M., Sayenko, G.N. On the Effect of Fermentative Poisons on the Various,
Phases of Photosynthesis (June T95)) 287
'Card 4/6

AUTHOR: Rdzenberg, G.N. 48-11-2/13
TITLE: Some Aspects of the Problem of the Spectroscopic Analysis of
Light-Dispersing Media and the Reflection-Capacity of Dyed
Polydispersed Substances (Nekotoryye aspekty zadachi o spektrallnoa
anailze svetorasseivayushchikh sred i otrazhateltnaya sposobnost,
okrashennykh polidispersnykh veshchestv).
. . . PERIODICAL: Izvestiya AN SSSR Seriya.Fizicheskaya,,-1957., VoL 21, Nr 11,
ppe 1473-a484 (USSR)..
ABSTRACT: Thisreport deals with the ana@ysis,of.substances which are in a
dispersed-state and which,.according to.their nature,,.do not admit
the application Iof abs-orption'methods exclusively's The causes for
the-diff iculties arising are'el-arified in this--- report@and-the-ways
of'surmounting them are pointedout. Besides theresults of:the
attempt to-find a solution f.-)r-aome spectroscopic problem&) are
given* Witkxespect to the question.of'taking account of mu]Ltiple
dispersion, it'is shown.that@a separation'of'the coherent'and in=
coherent part of the redipr ocal.Iirradiation'bf the particles permits
to,'attribute the solutionof the'statistic problem t.o.the formula-
tion of the socalled'transport. equation.@The..coherent part is ta-
'Card 1/2 ken into consideration in the absorption- and dispersion phenomena,

.241(4) PHASE I BOOK EXPLOITATION SOV/1142
.Rozenberg, Georgiy.Vladimirovich
Optika tonkosloynykh pokrytiy (optics of@Thin Films) Moscow,
Fizmatgiz, 1958- 570 P. 4,000 copies printed.
Ed,.: Kuznetsova, Ye.B.; Tech. Ed.: Murashova, N-Ya.
PURPOSE: This book is intended for engineers, scientists postgrad-
uate students and students of advanced optics making and using
optical instruments.
COVJERAGE: This book gives a detailed. survey.of theoretical interpre-,
tations of interference phenomena in sin$le-layer,and multi-layer
films and explains theoptical properIties ofIvarious types of film
(metallic, dielectric and m6nomolecular)14 Their application in
the study of optics and the preparation of selectivespecula,
polarizers and optical instrumentsare described. Special attention
is given to the use of interferometers for solving practical prob-
lems .(with respect to interference light filters.,.Investi.gating
Card 1/1:3!

Optics of Thin Films SOV/1142
the micro-relief of-surfaces, determining optical constants, etc.).
Many of the considerations, conclusions and results arel'original@
and,are published here for the first-time. No personalities are
mentioned. There are 616 references of which 146 are Soviet,,
257 EnglishY 112 French, 76 German, Dutch and-17 Scandinavian.
''TABLE OF CONTENTS:
Foreword
PART I. OPTICAL PROPERTIES OF THIN FILMS
Ch. I. The Structure of Thin Film Coatings
1. Introduction
2. Formation and structure of thin metallic films 16
2.1. General p@cture of theformation of coating layers@ l6
2.2.* Theor of.the formation of a @18
@y granular coating
2.3. The dependency ofthe character of a coating on
the "nature" of.the metal 27
2.4. "Aging" processes., The.influence of temperature
and the undercoating 31
.Card 2Ak

AUT1HOR; Rozenbarg, Gy-, S.011/51-5-4-13/21
TITLE; _Opt@ical conditions Within a'Waakly Absorbing Scattering Medium and
Possibilities in Spectroscopy (Svetovoy rezhim, v,glubine
s labopogloshchayus hchey. ras s eivayus hchey a red yinakotoryye,
vozraozhnosti snelctroskopii)
PERIODICAL: Optika i Spektroskopiya, 1958, Vol 5, Nr 4, pp 4-2.0-449 kUSSR)
ADS MIGT: The author diocusses optical, conditions -within a "Weakly absorbing
-isotropic scattering dedium. His diecussioa applies both to,alectro-
magnetic waves and to spin particles. It is' shown that -with increasa
of specific absorption of the inedium the steady-state intensity
indicatrix becomes more extended in shape and consequently steady-stat&
polarization of emission ap9eare. Dependence of the emission intensity
on depth is- given by an exponential law with a decay constant which
is not equal to the coefficient. of extinctilon,butwhich is proportional
in the first approxim- tion to the square root of the product of ttlie
absorption and extinction coefficients. The constant of prop orti onal 1 ty
depends on the form of the scattering indicatrix. 'Spectroscopic
Ca rd 1/2

............
Optical Conditions Within a Weakly Absorbing Scattering Med ium and, Certain
Possibilities in Spectroscopy
applications of the fommlaa obviinod aro iridicatod. Thode
applications rofor' to measurdments of the absorption,and scattering
coefficients, amploying a technique similar to that of Timof eyeva
(Refs 1-3). There are 5 figures and 18 references, 15 of wtilch
are Soviet., 2 German and I knerican.
ASSOCIATIO17a Institut fiziki atmosfery, W1 SSSR (Institute of Physics of the
Atmosphere, Academy. of Sciences of the U.S.S,R.)
SUBM T-r:!,D January 6P 1958
Card 2/2 1. bptical materials--Effects of radiation 2. Spectroscopy
3@ Electromagnetic waves--Properties 4.;. Nuclear spins

SOV51-5-6-6/19
AUTHORS: Rozenberg, G.V. and Mikhaylin, 1 X.
TITIS Ellipticity of Folarization of Scattered Light (Elliptichnost,
polvarizatsii rasseyannogo sveta.)
nR!ODIQIL.- Optikq_ 1 Spektroskopiya, 1958, Vol 5, Hr 6, pp 671-681 (USSR)
ABSTRACT-- The paper describes experim-ts ox. the ellipticity of polarization of,
light scattered by the ground layers of atmosphere and on dependence
of this ellipticity on the scattering angle. A visual polarimeter Ifor
measurement of allpolarization characteristics of a light beam kdogres
of polarization, degree of ellipticity, position of the planeof
predominant polarization) vas constructed. This infftrument is@based
upon.the following theory. It is assumed that a light beam may be:
described by a Stokes vector-parameter S -with respect to a certain plane
of reference. A compensator is placed in the light beam; it introduces
a phase,shiftr and is rotated by an anglovf with respect to the
reference plane. Behind the compensator a polarizer, rotated by an
Card 1/li angle ky + -with respect to the reference plane, and an analyser

Ellipticity of rolariza-cion olf Scatterad Light
is rc,t-atbd by at, anglo + S w.r.t. the reference plane, are
placed. By sele@,ting varicus valuec of Y and 'k and by measurement ot
ttis) anf;Le TL which corresponds to the condition of equal brightness, of
,:m (which is used in the place of a polariter)
fields in a Wollaston pri-
one can fird tha deFree of polarization p, the degree of ellipticity q,
and, zhe anmlr@ of rctation of the major axis of the ellipso of
polarization with respoct to tho reCerenco plane V @ The polarimeter
11 0
was based on a theodolito with a diaphragn of 6 anGular diamet5r.
quarter-weve plate and a Woilaston. pri:.,m, which.could separate two
boams by 0 weeo pla(-ed behind t-no djaphrafga. The vertical plane
r was taken to be the
through the optical. axiz, of the theodolite
reterence n1ano, Bahina the Wailaston prism a polaroid and a long-,focus
eyepiece wore placed. The evelYie,:e nroduced a virtual image, of the''
h s was used to
:L SZS-Itj li@;ht Itor of 5 mrd thicicnes
diap ragn, . fi
TDonoctiromatize the fields of view to be compared. The error of a:
sin-le, determinatioa of TL Waounted to +0 . The error in determination
of the dec-ree of allipticity Vias 'Jass than �0.03. Measurements wore
made on moonlecs nirhts in the second half of SeDtember in mountairLs of
Card 2/4 Northern Caticasus (750.m above r@ea level). Atmospheric aerosols were

SOV/51-5-6-6/19
Ellipticity of Polarization of Scattered Light
present in very small quantities. Is. projector, wl th a., reflector of...
150 cai diameter and an arc of 1-1,15 IN power, waj k4fled as the source* of
light. The projector wan covered up cunplately except for an aperture
of 4-0 t.,91 d-ismoter, A polaroid of 40 cm diameter vian placod at st
distance of 1 m from the projector. A. largo acreen (5 x 5 m) with an
aoorture of 40 cm diame+-r wq.r rilaced at a distance of 8 m from tiie
Pro'j ector (along t h e b 9 a m ihia system produced a sharply defined
linearly polarizod beam cr liGnv at a height of 2 m above%the ground
level, The pclarimeter, vas placod at 12 w from the screen and 2 M away
frca.@i the light beam. The results are F,,iven inFigs 1-6. The ordinatea
give q, the degree of ellipticity of the scattered beam, ar, a functior-.,
(if the scattering angle 9, for vaz-iouls fixed angles S between the ulan'9L
of polarization ef the b;:@&m and the plaas of scattering. Fig I gives
q(4) for 1 +4Z@ in the at@,.ea,-:e of mi,@!t. Fir
r-, 2 and 3 show
of q(8) for +45 in a thiuk. haze with a rainbow (curves 1) and in
a slight haze kzurve:: 2, of
Card ;5/4 The maximum of q, which ia characteristiz@

SOV/ 61-0-6-b/ V)
Fllipti-7ity of Polari-.@L,tjon of Scatte.red LiK_ht
a rainbow, occurn also when no ham in pre.-@ont (Fir, 4)' protnbly dv,-,.)
to large drops of moisture prenent ii; the air. Omy-ven I and ;? of
Fig 5 woro obtained for -45 and +45" rospectively, Fig 6
shows r-3sult@- for 0 (01>3zi and b1pok doT--) and +90 @crossa3
and half-black- dots). There are 6 figures and I Soviat reference.
SUBMiTTED: January 6, 1958
Gard 4/%

AUTHOR: IR
enber@G.V@,. SOV/51-7-3 17/21
TITLE: Optical Conditions Inside a Medium with Rayleigh Scattering
FERIODICiALLt Op.ti"ka i spektroskopiya, Vol 7, Nr 3, pp 407-416 (USSR)
ABSTRACT: In an earlier paper (Ref 1) the author dealt -with the general optical
conditions inside a scattering medium with low absorptivity. The
general relationships were illustrated by,considering the special
case of a wedium with Rayleigh scattering. . The present paper considers
further the optical conditions in a medium with Rayleigh scatter in
these conditions are a function of the proparties of the medium,,.its
absorptivity end depolarization. Various calculation methods are
compared and errors due to neglectiou of the polarizatinn eff,3ats ar-,
.estimated. The possibility of use in a .pectroscopy.,of -.the rela tionships
establish ad hera ia discussed.. As before, the author usas -une
terminology and uathe=tical techniques employed, earlier to describe
the polarization stateof a light beam by means of a Stoker' vector-,
mrameter (Ref 2). The paper is entirely theoretical. There are 10,1
figures and 6 references, 5 of which are Soviet and, 1 French.
SUBIUMD: Dectmiber 2, 1958
Ca rd 1/1

2AW SOV/20-122-1-16/44
AU 'f@RS: Rozenberg, G. V,, Mikhaylin, I. M.
UTLE: 1he Expe-rime-F=1--Detection of the Ellipticity of the Polari-
zation of Scattered Light (Eksperimentallnoye obnaruzheniye
elliptichnosti polyarizatsii rasseyannogo sveta)
PERIODICAL: Doklady Akademii nauk SSSR, 1958, Vol 122, 11r 1, pp 62-64
(USSR)
ABSTRACT: The purpose of this paper is to find preliminary data con-
cernin- the degree of the ellipticity of light scattered by
the lowest layers of the earth atmosphere and concerning
the character of its dependence on the scattering angle.
A theodolite, in the focal plane of which a diaphragm.of
0
the anGular diameter 6 was placed.,vias used as a polari-
meter. The authors immediately measured.the angles-@ in
which tile brightness of both the photometric fields was
equal. YL denotes the angle of rotation with respect to,
the vertical direction. The degree of the ellipticity q of
the incident light was found by means of the relation

- cos 2 By. choosing other, values of, cer-
2
q = (co
Card 1/3 +
tain angles, it is possible to determine the degree of the

SOV/2o-122-1-16/44
L
The Experimental Detection of the Ellipticity of the Polarization of
ocaftered l,i,-ht
volarization of the light and the angle of the inclina-
0
tion of the plane of the principal polar ization with respect to
the vertical direction. Tile experiments were carried out
rJuring r.-ioonleSS nights in the second half of SepteLiber 1957
on-the foothills of thp Northern Caucasus. A projector wac
placed in a comparatively narrow valley,.its horizontal
liaht beam was directeL ilong the valley. The carrying out
of the experiment (places of the polarimeter etc.) are@dis-
cussed in short. Because of the comparative pureness of the
air, tile scattered air ms rather faint, and the.visual
methods took a long time and were not very precise. Accord-
ing to theoretical considerations an ellipticity of the
polarization of.the scattered light will be observed only
as a result of tile scattering on.an aerosol and it will
have a maximum for + 450, if the irradiating beam is
linearly polarized in a direction which includes the angle
f with, tiie.plane of scatteringr, The ellipticity distinctly
depends on the scattering an-le, approximately satisfying,
the relation. - cos 3 Q. In the e-xturema a - 0, 1 which is not ai:
Card 2/3 iow value* second diaL@ram shows the function a(@) for 2

SOV/20-122-1-16/44
The Experimental Detection of the Ellipticity of the Polarization of
Scattered Light
cases of more or less dense fog. A zone of irridescence
.(Q = 130 - 1400) (in which q -/ 0,5) and a change of the sign
of q in the region 9 - 40 - 900 were observed. Sometimes,
the irridescent re.-ion was observed also in cases without
an actual fog. This is an argument in favor of the presence
of an aerosol fraction consisting of large drops in the air.
The values of the degree of polarization were within the
limits o,6a - 0,76. From a theoretical pointof view, the
ellipticity of the polarization of the scattered light is
not a surprising phenomenon. There are 3 figures,and 1
Soviet reference.
PRESENTED; March 8, 1958: by V. V. Shuleykin, Academician
SUB',',! ITT ED March 21 1958,
Card 3/3

24M SOV/2o-122-2-13/42.
AUTHOR; Rozen.er-, G. V.
flITTLE: The Light Distribution Inside a Dispersing; i!edium and the,
Spectroscopy of Dispersed Substances (Svetovoy rezhim v
glubine rasseivayushchey sredy i spektroskopiya dispergiro-
vannykh veshchestv)
PERIODICAL: Doklady Akademii nauk SSSR, 1958, Vol 1222, Nr 2, pp 211-214
(USSR)
ABSTRACT: V. A. Timofeyeva found some empirical laws which may be im-
portant for the absorption spectroscopy of dispersed substances.
This paper deals with the theoretical explanation and with
the improvement of some of these laws S nce the polarization-
effects have to be taken into account, the author uses the
terminology and the calculation methods which are used for
the description of a polarized light beam by means of the
vector parameter of Stokes Stoks). The lower half-space
Z > 0 is assumed to be filled up with a homogeneous isotropic,
scattering medium and to be lighted from the upper half-space
Z < 0. in the case of an isotropic medium, the scatuering
Card 1/3 matrix must have certain integral-properties, the correspond-

SOV/2o-122-2-13/42
The Lisht Distribution inside a Dispersihg_ Mle'dium and the Spectroscopy of
Dispersed Substances
formulae are given by the author. The propagation of:the,
light (or of particles with spin 1/2) is described by a
@transfer equation . According to physical considerations, a
sheady distribution of light must exist inside the scattering
medium in-a sufficient distance from its boundary. The angular
distributions of the components S. of the vector parameter
I
of Stokes do not depend on the distance from the surface, on
the inclination angle, and on the polarization character of
the light flows fallin.-r -ipon the external boundary of the
medium. Simultaneously, "_-.e azimutal dependence of S. must
vanish. The author then step by step gives.the calculation
operations which correspond to the above-discussed considera-
tions. Inside the substance, S i(z) must be an exponential
function. The damping coefficient does not depend,on the direc-
tion of the beam. Then a formula is given for the radiation
flux through a horizontal cross section. Then the li-;ht dis-
tribution for the case I