SCIENTIFIC ABSTRACT SOTSKAYA, KH.N. - SOTSKIY, B.A.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
• Document Page Count: 51
• Document Creation Date: November 2, 2016
• Document Release Date: August 23, 2000
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SOURCE CODM. U4
AUTHOR: Sots, Kh. N.; Fedorov, F. 1.
ORG: none
TITIZ: Singular points of the cross section curves of the surfaces of elastic W'M
In crystals
SOURCE: AN BSSR. WSW
SMY& Mika-matemtrebiwkh naruk,, no. 3p 15"p 30T-3616 I
TOPIC TAM: elastic mve,, elastic wdulus,, crystal lattice structures =75tal NYW
metry
ABSTRACT: The authors obtain equations for the sections of the wave surfaces by the
MYMWtrY Planes for rhOMbiC.. hexagoM1j, tetragona,, add cubic crystals in a parametric
form., and for arbitrary crystals in an impucit form,' and investigate the singular
points of these sections. All the calculations are based on the fact that the sec-
tions of purely transverse vaves by the symmetry'planes are ellipseso-and the equap.-
tions for *the di:,Yerent symmitries are obtained by substituting the proper moduli of
elasticity and other constants. The investigation of the sir4gular points, which has
not been carried out by anyone before, is based on eliminating the angle variable
from the parametric equations by =man of a coordinate transformation. It is shownp.
In aaeamez* vith earlier results by one of the authors (Fedorovj, Teoriya upurgM
voln Y kristallakh (Theory of M^xtic Waves in Crystals]., AvAmp x. 3X5) that the
equation for the section of the wave surface by the symmtry V2AW in any crystal has

. 1. 1. . .... I " . I ~ I .;~,~
QW 2121' . 1, 1 .~ I '. i : ,
:1

SOTSKAYA. M.N.
----------
Heating of penduline tit in southern Mr,scaw Prcvince. Ornitologlia
no.7s488 065. (MIRA 18-:X")

SCITSKAYA, V.P.; SMIRNOV, V.A.
Chemical changes of starch due to cooking in the distilling industry.
Izv. vys. ucheb. zav.; pishch. tekh. no.4:2-S-34 161. (MIRA 14:8)
1. Leningradskiy tekhnologicheskiy instit-ut, pishchevoy promyshlennosti,
kafedra tekhnologii spirta.
(Starch) (Distillation)

SOTSKAYk, V.P.; SNIRNCYV, V.A.
Effect of the pH during the thermal processing of grains on the
losses of fermented carbohydrates and the Aeld of aleohol. Izv,
vys. v~cheb. zav.; pishch. tekh, -no,2:93--~98 163.
(NIRA 16:5)
1. Ieningradskiy mezhotraslevoy nauchtio-issledovatellskiy I
institut pishchevoy promyshleimosti, laboratoriya tekhnologi-I
spirta.
(Distillation)

SOTSKAYA, V.P.; SMIRNOV, V.A.; TIKHOMIROVAY, L.Ya.
Effect of pH on alcohol yield in the thermal treatment Of
crushed raw materials. Izv. vys. ucheb. zav.; pishch. tekh.
no.6:67-69 163. (MIRA 17:3)
1. laningradakiy nezhotrasisvoy nauchno-issledovatellskiy -.
institut pishchevoy promyshlennosti, laboratoriya. tekhnologli
spirta.

V. L. Sannitsiva " arDitln-7.nykhi DVtyt,riy-v 1, Nosityelyey. llrachyeb
kh
No S'D 317-11c
L~~Tlld~!S TIC. '113

S~' TSKA'YA, Z. it.
SOT-ISKICYlt, Z. A.: "The stimlating (-,f fect of -.old on certain functions
of mcrobes producing antibiotics." Odesqa St-te Medical Inst
imeni N. 7. Pirogov. Odes!~a, 1956. (Dissertation for the Degree
of Doctor in Medical Sciences.)
Source: Kriizhnaya le-top-is'- ,To LO 1956 Moscow

SOTSKAYA, Z.A.,,, Doc Med Sci -- (diss) "Concerning t-le
-~ - W, In certain functions of
stimulating a of cold
611-V
microbes of antibiotics." Kharikov,
T'
1958, 16 up. (Kharikov State Nei, nst) 230 copies
(KL, 39-58, 111)
59

GROKOV, A.S., prof., doktor med.nauk, otv.red.,, 130TZMA Z.A., dotsent,
red.; GORITSIAYA, V.I., dotsent, red.; K~ I., neuchnyy
aotrudnik, red.; BADAYKV, D.A., tekhn.red.
[Problefas in the im-imology, microbiology, and epidemiology of
intestinal infections] Voprosy Immmologii, mikrobio'logii i
epidemiologii kishechnykh infektail. Dneprope~~ovskq 2959.
256 p. (KiRA 14:z).
1. Dnepropetrovskly nauchno-inaledovatellskiy institut epidenio-
logii, mikrobiologii i gigiyeny Im. N.F.Gamaiaya. .2. Dire"or
Dnepropetrovskogo neuchno-iseledovatellskogo inntituta epidemlo-
logii, mikrobiologii i gigiyany im. N.F.Gamaleya (for Gromov).
(INTESTINES-DISMSM)

GORGIYEV~ T.B.; SOTSKJIDII.-Z.A.,
14icrobe forms resistant to antibiotics. Vrach. dolo no, 3:125 Mr 161.
(MIRA 14:4)
1. Dnepropetrovskiy institut epidemiologiiv mikrobiologii i
gigiyeny.
(STAPHYLOCOCCUS) (ANTIBIOTICS)

E-11RICUM"~INIJ), S.S. iz;ll.; YESIKOV, A.S., in?A-i.; SUIP~~EIY, A.11, Y-izh
'li.Y
il. 31MUTH, A.A. , inzh.; VESELOll, Yu.A-.--
Deepeni ng the shaft of the Kc-nintern iline. halclit. stroi.
I
0 no.7:20-2-4 Jl 162. (1,MU 15-7)
upravlenip No.2 tnasta `-' ::'~szshaklita-
proldiodIr'. (for flikolayr-riko), 2. Yxivorozhski-.r ftili-
m-uchno-isoledovatellskago i-nstituta or-anizatsi-i
z;,-;al-"itnoj;o stroitellstva (for YesIlcov, Sotshly.,
voselov).
(Krivoy Rog Basin-413haft sinking)

YES`KOV~ Anat--'iy sp-menovich- MAKSIMCHUK Aleksey Arssentlyevich;
KAZAKETICH Eduard Veniardnrjvich; _�g:TS~IY. Ananiv
,~~14~94qvich- TREGUBOV, Vitaliy Anatol sye,.rich; SOUIN,
Mikhail Samcy-'1-jvi.,:h,, FEW-R'OV, S.A.9 prof.;, dcktor tekhn.
nau-Kr retserzent
[Short haDlbcok -,n shaft, deepening) Kratkii spravochnik po
uly.11jUe stvo!~~v shakh-t. Vaskva, Nedrr., 1965. 1,75,p.
(MIRA 18:8)

SOMISKIYY B. A.: Master Ph.lrn-Math Sci (diss) -- "Th" molecular theory of the
--l. -- - - -
Complete reflection of light". NUnnk, 1958. 1? pp (Bel.OXIISB 9tate Tj Im V. T.
Lenin) (IM, 1-10 5, 1959, 143)

55-1- 4 13/ 3C
AUTIJ ORS: LS--ot-skiy, and Fe-dorciv, F.I.
TITD~: ole~aar Theox-y of Reflection and Refrac.-tion of Light.
I. Light Tn,-.idenju- from Vacuitm or-to an Isotropic Mediua.
(K mc..'-eIa----1yar-r.L;--Y te(--:ri-i otrazheniya i prelom'Leniya
s-jeta. I. Padeniye, s-,im'Va 1z -7aI-xLma na 4:_zctropulayu
sred,,. )
PBAIODICAL: Opt.ika I Spekctrosl~'I-ol:dya, 2.958, Vci.IVv 'Nr-3,
pp. .36-'3--3?2 (USSR).
ABS-2EkCT Molecular theory of and refraction of light
in isotropic. inedia was developed b'7 Ewald, Esmarch,
Oseen, Lundblad and cjtliar~~ (Refs 1-1-18). This the o----y
is based on the foilnwim- assumptions, Und--r the
action cf an eler;troluagnetic incident ficm vacuum
-r'.,-J the r~,--ecliuL- mi~].~;cula.-, d4c.Ds are ex,;ited into a
- .7
state. of vibTaticr-,~-- :,:ind emit secondavy wa-ves.
D:,,'th the in,-,idlent and Se3u:dary waAres obey 1-iiamvell's
eqa a t I o n Sl)-pe--T-csitior- cf all the
via-',es and ~-I-f the Tvvave gives t-he
-efr-a --ed '---va-vre the and the --:-If:flected
1--i-, MT cul --i- --,ecry has a niumber
lh-j,s
Card 11-A

-3-13/1-; 0
Lolecular T; ecry z~f Re 'Ie cn and lief r*a (-,t or- c, f LJ
lormulae fc;.r tiie L;er-er-ai case c,f ln,:,idence a3.e
c~btained- en2j in. a --u by using the method
pproximate f c
of Oseen and Lundblad (Ref .10-12). In none 3f the
papers an the molecular theory cf reflection and
refraction is the case of total refle,tion of light
dealt with. The pTesent paper is an attempt to
develop a more compIete and exaot molecular theory o:,.'
reflection and refractioni including in pa:rticular-t'ie
case of total reflection. All the main relationshi::)s
(such as the relationship between the iefractive indl.*IX
and polarizability, -the q:-.en-,~hing theory off, Oseen,
Frcsnel~s formnlae) are obtained exa-'tly and in a
comparatively simple, way. The present authors also
generalize Oseen's -.1heory ie-c-) the oase of non-homogen-3cus
wave s . The paper is enti-rely U:Leoistioal. There are
2 fi6ures and 21 ieferences., of whicI 14 are German,
4 Soviet, 2 Englisb and 1 a translatlL~-.-n of Born's
"Optics" 111t0 Russian.
ASSOC IAT-1 ON-. Be'.ooussiari State University (Be--1.-1rL:.sski-.7
Card 2/3 6osudarst-v--unyy ujai--.Tersi:tet.)

5-1-- 4 -3-13/1;-o
Molecular Theory of 11-Reflection and Refracticr- of Light. J--
SUB~JTTED; May 4, 195"?.
1. Light-fteflection-Theory 2. Light-Rt~fraction--Theery
3. Light-FropWtiv;;i-Thsory
Card '.V*;
. I

-kTJ TH ORS Sotiflciy, B.A. and Fedorov, F.I. 0/
On the Lolecular Theory of Reflectlion and Refra~-Ion- of light.
IT
(K molokulyarnoy teorii otrazhenlya i prelomien-iya svota)
II, Light Incident on the Boundary 3etwean an Isatroplu- Kedilum
and Vacuwa or Another Isotropic Medium. Total Refle..-tion.
(II. Padeniye sveta na granits-a izotropnoy srody a vaLcuum"T Ili
s drugoy izotropnoy sredoy. Polnoye otrazhe,-iye)
Q
PERIODICAL: Optika i Spektroskopiya, 1956, Vol 5, Nr 1, pp 5.7-65 (USSR)
ABITPACT: In the preceding part of this woric (Ref 1) the authcra c3asiderad
the caas of an infinite plane monochromatic electromagnetic wave
incident from vacuum on to an iaotropic medium. The present paper
gives the molecular lk'--ory of reflec-~ion and refraction of light
at the boundary of two media, of vhich the first consistas cf
molecular dipoles and the second is vacuum or consists of dipoles
of another type. The molecular theory of total refleution is given.
Card 1/2 It is found that, under certain conditions, the vaovwn .-;ave vihi ch

SOV/51-5-1-10/19
On the Molecular Theory of Reflectica a-.4 Refraotion of Light. 11. UiS4t
Incident on the Boundary Between an Isotropic Mediem and Vacuum or Another
Isotrooic Medium, Total Reflecticn.
appears as the result of superposition of primary waves produced by
vibrations of dipoles, may be damped in spite of the faab that the
dipole vibraticns are undamped. This is the convei7se of the -base
discussed in Part I -(Ref 1) 'where a damped dipole wave produced an
undamped va=-am vave. There are 3 fikpires and 5 referen;-,as , 2 of
vihich are Soviet, 1 translation of a Wastern. work- Into Russian,
1 German and I Engliqh-
ASSOCIAT ION -Beloruaskly Scsudarstvennyy univeraitot ( Belorusalan State
University)
SUEUTTED: Auguat 1-9, 1957
(;a rd 2/2 1. Light - Reflection 21. Light - Refraction 3. Light -
Pblecular theory

SOTS~Iyj P,
A~
Molecular theory of the refraction of light in cryst4ils-
Opt. i spektr. 11 no.2!229-236 Ig 161. (K= 14:8)
Molecular theory)
ft"tal optics)
i

GONCHAREINKO. AAM.; SOTSKIY, B.A.
Condition of self-excitation in a plane-parallel layer. DokI.
All BSSR 6 no-4.223-225 Ap 162, (NDU 15.4)
1. Institut fiziki Ali ESSR. Predstavleno akademikom AN BSSR
B.I.Stepanovyrq.
(Optics., Physical)

0 S/250/62/006/005/003/OD7
1024/1224
AUTHORS: ~ki -P. AAnd Goncharenko, A. M.
TITLE: Electromagnetic field of a plane-parralet layer in conditions of self-excitation
PERIODICAL; Akademiya nauk Belaruskay SSR. Doklady, v. 6. no. 5, 1962, 297-300
TEXT: This paper is a continuation of: A. M. G(,ncharenko and B. A. Sotskiy, DAN USSR, 6, no 4, 1962,
A system of equations is written for the normal and parellel components of electromagnetic fields, propaga-
ting inside and outside an active plane-parallel layer. These equations contain the refraction angle and di--
electric constants. Expressions are given for the electric and magnetic fields inside the layer and also for the
time and phase averaged energy density and Poynting vector. For the lait two a definite dependence of the
dielectric constant on the radiation density is assumed. An agreement is claimed between numerical values
characterizing the system of rings actually observed on a screen (T. H. Maiman and otheirs, Phys. Rev 123.
1151, 1961) and those predicted by the present paper. There is one figure.
ASSOCIATION: Institute fiziki AN BSSR (Institute of Physics AS BSSR)
SUBMITTED: March 14, 1962
Card 1/1

KHAFALYUK, A.P.; STEMOV, B.I.; SOTSKIY., B.A.
Electromagnetic field in a plane-parallel lepr w3der self-
excitation. Opt.i spektr. 13 no.2&282-285 Ag 162.
(KIRA 15:11)
(Optics, Physical)

GCVGHARENKO, A.M.; SOTSKIY, B.A.; FEDOROV, F.I.
Self-excitation of a plane-parallel anisotropic layer. Kristallo-
grafiia 8 no.l.-47-50 Ta-F'63 (MIRA 17M
1. Institut fiziki AN Beloruaskoy SSR.

AID Lr. 9-93-3 7-9 June
SE T07
LF-EXCITATA \T COINDITIONS FOR A PL-~NE-PARALLB,L CAYSTAL-
LINTE PT TE (USSR)
A
Sotskiy 33- ard. A. M. Goncharenko. Kri's tallografi3ra,: Vs no, 2
17%~.LaApr 7 2 1 3 0. S/070/63/008/0'02/01 /oil
The " 'Yn--m ic ecufllibri~m of monochromatic phLne waves inside and outside
a pl-----lo-parallel anisotropic plate bou-nded by an opaque metallic -iay'er on
one su---face a serni- er is consi
transparent layer on the oth 'dered in; the
absence of exterral incident radiation. Such equilibrilim can be established
only in n1Z t-~s wil:h a neaalive, absorption coefficient. For fhfe genei~*al case,...
eight waves described by eight equations, each having its ovrn, absorption
Caxd ~/2

'D
~3-3 19 June
S E L_-- - E ]K'C _1T-3 _NTCONDITITONS (Cont.) s/070/63/008/00~/012/61:7
However: thio 'specific
factor and -ref-"active index,r-nust be consilde're,d.
ca~; --.n- is reduced to two Independent sets of fdui-- eqti4tions: each'
desc_-ihin~;- generation of ordinary and extraordinary wave's i t*i, zi;~ I ate
cu-~ fronaa--nonaxial crystal of mean syngoi Iiy,perpen6icula'Pf~ to th6 optical
a_xlz~ 11ach set of _-quations is considered separately, and.0scillAtion condi.'
tions are cl e-rived by setting the determinant of each set equ~al to zero. - Con'4
d-t4on'-s fcr the existerice of non-zero solutions yield the osd'illation:: conditions
04' e-raordinarv %Ajaves. It is noted that emi8sion in.differ~nt dir;e`ctions with-
(BB]
P. thu plaic: roust be polari,_,ed differ ently.

(1)/BDS/EEC(b) -2-AF.'VTr,/ASD/
L 9879-63 EWT
ESD-3/SSD--GG/IJP(C)
ACCESSION NR: "3000786 S/0070/63/PW/003/0471/0473
AUTHOR: Petrov, N. S.; Goncharer-ko, A. M.; Sotskly, B. A*
q
layer in the presence of;
TITLE- Oscillation of a plare parallel anisotrapic
total reflection
SOURCE: Yxistallogra-fiya., v- 8, 3, 1903, 41,473
TOPIC TAGS: o3cillatian, plane -paxallel laye;r ,aniso-6iopic ~nledium, 1
coefftclent of absorption
ABSrMAG-T; Oscillation ixi a plw,~e -Parallel mnisci-txopi~.- `,-*~je lj~~vhich
elec-L-amagnetic vaves are propagated. obliqUely 4~ ,the:] er!i sur
ZX faces i's
a
na
"yzed withiz, the framewcirk of linear optics. Two cases are.' considered:
1) osaillation in- the presence of total reflect-
ic)n, rather th-4m oscillation.
Ln a layer wlith r-etal coatings oz,-, both sides, and 2) osnillAtidn with total,
reflection taking place at a simg~e inte-rface an. It is sh6m.that :Ln the.
ly.
case a stable oscillatian regime cannot be attairied fbil either The
ordinary or the extraordinaxy wwres without resorting in, bigh.'en;erar densities-
Card 1/2
- - - - - - - - - -

5/051/63/014/001/018/031
E032/9514
AUTHOR: Sotskiy., B.A.
TITLE: Oseen$s extinction theorem'for metals and Optically-`
active isotropic media
1,- 1963,- 112-116
no,
PERIODICAL: Optilca i spektroskopiya, v.14*
TEXT: The propagation of ~electromagnetic waves. in 'the4 'free`:'
'electron gas in a metal is considered*assuming that 1) each
electron executes a simple harmoni6-o9cillation-under the ac.tion~,
of the field, 2) the waves are - transverse, and 3) tfi Ose'en
c
theorem holds for the system (Ann'. Phys., 48, 7, 1915).. Subj ti-
to these assumptions it in shown that by it'dnaidering the intor:c't 115n,
of the electromagnetic wave with the Xreo-electron gas,'.itis
possible to obtain the usual, Fr-esnel reflection form*u'lAe Sok a
metal. The analysis holds for wavelengths in excess of V.cm.
and in the region of the normal skin effect.-The analysis isl-
then applied to the case of an optijpaliy-a4flye isotropic m6dium-.-,
in a vacuum and expressions are deriveckitor"Itherrefracted atid
reflected waves. 'The restilts-are identical with the usual
phenomenological.expressions,.i.e..macroscopic solutions of,
Card 1/2
%

Oseen's extinction theore"rd ... S/951/61/014/001/018/0311~
P
E032/E514 .2.
Maxwe I 1s equations,so tfidt the,present anslysis in effect
provides a"wolecularfoundation'for these re's'ults. The Oseen
extinction theorem is thi~x found to, have a very.; wide range -of,.---'-f'..-~--,_
applicability and it is concluded that it may*bi regarded
the fundamental and univer~sal result determ'lnin! the behaviour.
of an electromagnetic wa,~e~ at the boundary Oietwien two arbiiialry'.1
media.
SUBMITTED: November 4 '1961
N
Card 2/2

45079-
s/o5i/63/014/001/019)(031:
2 Z032/B514
U,
AUTHORS: Bokut B. V. alwd Sotskiy, .8.,A.
TITLE: Transinission'of light through an,dptically active
absorbing.plate
PERIODICAL: Optika i spelctroskopiya, y. 114, no.1, 1963, 117-120
TEXT: The radiation is-assumed. to be at normal inci'derice
~on a plane-parallel optically-isotropic active 'Abnorbing plate
of thickness d placed in-an isotropic medi!4m.witfi a
index n. Tjie reflectio.tis from both surfaces' are taken into,
account. It is shown that the reflected and transmitted field:
are in general elliptically polarized.If the incident wave is'
circularly polarized, then double refractio'n will be absent Bin
a
11 the waves will have the same polarization as the incident
wave. if the-ine'ident.wave is plane polarized,, then the
transmitted wave will also be linearly polarized but'Its pjane
of polarization will be rotated through an-angle 1/2 k daL
where Ic is the wave number in vacuum andt~- is the optical;
activity coefficiento=fl;,4~.The reflected 'wav~'*will be elliptich4lyt~
polarized with the ratio of the. semi-axe's given by'
Card 1/2

Transmission of light through ... s/o5i/63/014/001/019/0311,
E032/E514
np 2)
n M
b c;
a 2 2 2
n 11
0
where n' and x are tbe, refractive index 'and'absor:ption
0
coefficient of the plate,,,respectively.' and Ip .= kcx.'. These
-tax-s-re I DI aequation~;`subject to
results are obtaineel'by solving
the appropriate boundary qonditions.. The-paper coricludes with
a molecular interpretation ofthese results in~tekms of the
C. W. Oseen theorem (Ann. Phys., 48, 7, 1915). . The~molecular
treatment yields the same results a- the .11macros.-copic solution"
of the Maxwell equations~
SUBMITTED: November-30, ig6i
Card,2/2

STEPANOV., B.I.; GONCHARENKO, A.M.; IVANOV, A.P.; SAWON, A.M.;
SOTSKIYP B.A.; KHAPALYR, A.P.
Generation of radiation from an infinite plane-j*ranei layer,
Izv.AN SSSR.Ser.fiz, 4 no.4s460-465 Ap 163. (MA 16:4)
(Masers) (Electric resonators)

ACCESSION NR: Ap4o44254 S/0250/64/008/007/0438/0440
AUTHOR: Sotskly, B. A.; Goncharenko, A. M.
T;TLE: Diffraction of partially coherent light
SOURCE: AN BSSR. Doklady,*, v. 8, no- 7, 1964, 438-44o
TOPIC TAGS: physical optics, dielectric resonator, light dIffraction, partlally~
coherent light
ABSTRACT: An attempt has previously been made to calculate the diffraction of
partially coherent light at a narrow slit, given an exponentially decreasing co-
herence function. Since the implicit assumption that the latter satisfies the
wave equation is not satisfied, the results obtained are doubtful. in tile presents
paper, the calculation is made for a coherence function of the form (sin X)LX
where cc is the coherence interval. The diffracted intensity found does rlot giffer,;
greatly from that for monochromatic light when Zalct Is small, where 2a Is the
width
_of the slit. When this ratio Is large, the divergence of the-radiation is
I.A /211ct, independent of the slit width, as confirmed by experiment. For dielectri * C'
resonators this angle will be several tens of minutes. It Is not known how well i
he coherence function fits the case of a dielectric resonator; however, It satls-'~
Lt.i.qs,~~e wave equation, decreases with Increasing distance between,the points cone's
7

ACCESSION NR: Ap4o44254
sidered and probably does not give results differing greatly from those given by
other functions satisfying these criteria. "The author acknowledges the Interest
of Prof. 0. 1. Stepanov and 8. Bo Boyko In his work." OrIg. art. has: 1 flqure
and 9 formulas.
;ASSOCIATION: Institut fizIkI AN BSSR (Physics Institute, All OSSR)
SUBMITTED: 28Feb64 -ENCL:: 00
JSUB CODE: OP NO REF SOV: 001 OTHER: 006
Card _2/2

~A,
!j
-WFOP _,Izt
L 23062-65 EWG(J)/EWA(k)/FBD/W(i~)/EiIT(i)/EtC(k~)-2/*(t~/ /&C(b)
RWA
EWATM 2TE (h Pf44/Pi-4/?1-4/ft,,4i/Pn-4/Pa-4/Pa~t1 1W
ACCESSION HR: AP5003373 I./oz~ 4
F, o-
AUTHOR: Goncharanko, A, Hs; fliotski B.; Ao
TITLE: Oscillation of 4 cylinder vi:th a circulor crbvs sectio'n s6d i-
sphere
SOURCE., AN HSSR,, Doklady, V4 as noq~ 11V 1964,
TOPIC TAGS: oscillation, generation:, tss ser.$ lasiar *(:~t~on osci It otiam',.
mode, oscillation condition
AbSTRACT: A theoretical analysis.is', conduc,ted ~aii: 13tim;ulated e MI 13 on
of a cylinder with a circular cross section and: A spiie~!A: SLh~e ihL
problem is actually equivalent to lia,dLng mo'des; F-pr ~gl~ Ly e'n caL4 L ~Y~ .
.resonators, the authors use general solutio'1139 ofil,vax4e-11 s eq~itidas
t i IF
for the cylinder and the sphere. Under ~~the: assui~p an;! tha t ~ tfi~, ir 'd
of the cylinder and the sphere are finite !Isymptotid' Oessel aid Hank4i-
functions are used in the solutions. The tif'o daces dereCar~
ohsi
those for which the mode number is low an: -the m6de wi4abeis &Z.4 of 'th-i
order of the absolute value of the wave num4er times jt6e; iadI4~ of, th--.14;
Card 1 / 2

ACCESSION HR: AP5003373
sphere or the cylinder. It is shown' thit the q4flactbri,is higher kor~
igher modes. Therefore, for the:gi'ven -g'eometr#1 ti
h ~m`lated eM~Lssjon
of higher modes should be observed, 1 In-Casi of ithlighd-r~ mode eml~ a s L on
the index of refraction of the activd-medium Ld ~~"'e n
gr ate;t "ths, t6at of
the surrounding medium. Therefore, both in the 'idAse !al ~the spo.ere a ri
to the ~n:4 o waves
the cylinder an effect analogous scatteri i *- nea~r
the critical angle takes place and the energy ii~ radiaie:d. primirkly in~.
the direction tangential to the surf ace,lz- This eff,ectica'us6s a~dftt
energy losses and a decrease off the Q-fa6tor. tt.:; isiipo` Lnted out ;that~
such losses are absent in gaseous lasers 'and alio'An !t~e~ presence :6 f
a dielectric along the sides of the 6ylLhder witl~an liddex of ~ ie fiaC-
adium, Oria": ;k 0-~
tion higher than that of the active' m art' Ji' st 0

........ .. .
AC=31CM
810521WO161003103131OW
AMCR: fttzws, No go; Ae Xe; SOMIdyp S. A;.;!
T=: Concerning In a plane-parallal s3L*b In the ynm~ ar
total reflectIca
SM=: OpUkL I spekbrookoplya,, v. 16, no. 3, 19S4, 53.3-516
TOM %W: 1wer, ]=or cscdLIUtAcnO stimxIatea gmeraticn, self-miftacu'p
laser slab,, plme-para.Uel slAb., reflectica,, laser slab reflection
ABSOUT: Under the usual coaditims of SeneratIm (laser oscIllatbicn) in a p2mp.,
p=-allel s2nba, energy Is mItted throuGh =& or both faces (Sivem a suMeUnt
tbickmess of the metallic coating on the other); that is,, uaer ecadIticam In
,&ich Dart cC the emerMr Is lost due to absoz7bicae This can be mrodded IbV Wari&
Ins for ccmplets reflect.1cm by bevelllnZ at least cme of Ue and faces to the
Angle of total reflectica. Thus,, the stI=LU:te& mission froa a. sSbariwa speci.
mcm 6baerved by C. Be Garxet, W, raiser, and W. L. Bcmd (Bzyzftvv124,v2WTp -_ )
may lba- expladned by Increase cC the reflectica coe=cImt &+, now -total refur..
Cwd,

ACCEWION NR: A4020966
Of electromagnotiia waves In a plane-parallel slab under conditions of total refloc-'
tion. The approach is solution of the Maxwell equations with the appropriate boun-
'dary conditions; an analogous problem was solved earlier by two of the authors (A.
M.Goncharanko and B.A.Sotskiy,DAN BSSR,6,223,297,1962), and the expressions for'the.
condition necessary for self-excitation are taken from thaw papexa, By separation of
Ithe real and imaginary parts and introduction of the Presnel reflection coakficled%,
the conditions for self-excitatica in a plane-parallel slab are derived In
the case of total reflection from both facas. Analysis ct the expressions shown thst?f
~
:self-excitation is impossible if the imaginary component of the dielectric constant'
.(i.e.,the negative absorption) Is smaller than zero, that is, in the region of Un-:
ear optics; however, the energy density in the layer may build up to the point vbm,
in the limit the medium becomes transparent and self-excitation becomms possible
(but, of course, no radiation can be extracted without violating the condition for
total reflection). The equations are also extended to the case of a slab with total:
reflection only at one face; in this case self-excitation (laser oscillation) be-
!comes possible in the region of linear optics. The condition for generation Is af-
fected primarily by the value of the ordinary Presnel reflection coafficlent. "ne
authors are grateful to F.I.Pedorov and B.v.solatte for their Interest ja the work."
Orig.art.has: 2l.formulas and 2 figures.
2/$

emu
I ACCESSION NR: AP40107 3/0020/64/154/
57
AUTHORS: Sotskiyp B. A.; Goncharenkop A. Me
TITLE: On the condition of electromagnetic waves generation In a
d6uble-layer crystal
SOURCE: AN
SSSR. Do%lady*9 v. 154P no- lo 19"P 91-93
TOPIC TAGS: photon generator, electromagnetic waft, crystal# uni-
axial crystal, crystal self-excitatift, laser, double-layer crystal
ABSTPRACT: The previous work of the authors (Kristallograxlys. S.
47 1963) which dealt with an ideal homogeneous crystal Layer Is ex-
tended to a parallel plans cry3tallins plate consisting of two
layers of equal thickness of uniaxial crystals with an arbitrarily
oriented optical axis. This represents the simplest'model of an
actual Crystal which has a nonuniformity of the refractive index
and of the absorption coefficient. For the derivation of the condi-
tions for generation (self-excitation), In the absence of external
radiation, the Maxwell equations are saved with'the boundary can.
1ditions at the three separation planes. The results ohmathat Wn
Card 1/2

ACCESSION NR: AP4010757'-"'
conditions of generation In a double layer are considenkbly ljore
complex than those in a uniform layer. Small deviationa from'Val-
formity have very little effect on the generation of the ordinary
wave. The extraordinary wave Is affected more.
"The authors are grateful to Prof. F. 1. FedorOT for a useful
discussion of the results.
i Orig. art. has: 1 FIg=v and 12 Equations.
ASSOCIATION: Institut fisiki AkadeMli n&Uk SM Phiflaa
Academy-of ScIencessnW.
I SUBMITTED: OlApr63 DATS ACQs 10F064 INCL: 00
SUB CODE: PH MR PJW 307t 003.; t 0102
Card 2/2

7-:
-L 45567-61.5-- - EWA(k)A_,
,w/EwG(j)/EwT(-j-)/ -
g0A Ak(k
F_ WA (m F-2TE- WA (h) PM-4/Pn-4/Po-4/Pf-4/Pt-7/P* P 'S
P1
ACCESSION MR: 061
AP5031
J
Croncharenlw,, A, K Sotgklr~, 16. AO
-AUTHOR.
th itA;
TITLE: Contribution to1he~~ e(
MT a a And ikii*-'', T6
J
SOME t M MRe Dokl&T~rx v. 99 no 41, lq%sl 0241.0
TOPIC TAGS: laser arwityp dielectric "vi fiber '"VityV (We 1w rea
loss
the-
out first that ni4aect:of 1-0-ft
ABSTRACT: The authors point n Sidi
-too
gee 6t e the cb~.-
vmUs of laser cavities is not Suotfied i -ee
!to th
served distribution of radiation intensItk1n.'dielegirl,
5V _X9 1 .
-distribution 6btai
ned-4a -optical-- fiber cavitle thir-themk
fairly well. developed. They therefore extend.the resultic obt Abers io
derive some information on the properties af 11idite 4W."i-atridi'lia :i&ri, ciaxltbis
without solvi.M the baund=7 value problem. It lit ohmm: t fi6n~ infinite
cylinder,, the field inside a finite cylinder cad; be. msed!ln W%x 6*f A at'
position of cylindrical vaws traveling In beft4ir!ctic" &41 th6 4ilmer
axis. the ezt fleIA-zazu-be, datqwvihx~; AM-4 t

AS WIN Do

SUM o4Aj;rA

NO M 5": 003.-
A7;

7- 7-- 7~ i?:-
i --- -- -
II

F

L 1983-66 E7v/T(1)/3dA(h)
F1 -ME-9 MSI 0 NNR: AP5017693
UR/0250/65/009/006,,0360/03t.3".
AUTHORS: Goncharenko, Sotskly, B. A.
TITLE: Contribution to the theory of a dielectri,c,circular resonator.~,,.,-,I~
~SOURCE: AN BSSR, Doklady, v. 9, no. 6 1966, 36o~-363
!TOPIC TAGS: resonator, dielectric material, laser*: opti''
laser,
pumping
7
:ABSTRACT: This is a continuation of an earlier P o
ap r DAN. BSSWY
9
-no. 4, 1964), In which generalTorm-0as were deriVe'd fan'the ene~r
,of
a finite resonator and for the energy losses. The pr6sent pap:
ideals in greater detail with the properties of dielectri.16 circula(r.,
;resonators in the case when the critical resonancelcondift6ri cah~be' I
'satisfied for cylinders of finite length, and wheni~the~16:*sses thitougffi
:the resonator ends are replenished (negatIve absorptlon' or amplifica-
.tion). It Is shown that with Increaoing radial propagation conatant 1
;the total energy and the energy flux through the resonator ends. d6-~
It Card 1/2

L 1981,-66
jACCESSION NR: AP5017693
~crease rapidly, so that nonaxial modes begin to pre,dominate.. This
,explains, In particular, the occurrence of divergence In laser beams
.It Is deduced from the analysis that at minimum pump energy, th re 8
'hold) only lower axial modes should appear, and that.an4ncrease:In
:the pump energy Is accompanied by the appearance of'nionaxial modes,
which must be suppressed to limit the beam divergence. ',The authors
,thank Professor B. 1. Ste,-)ationcLitor a discussion of the results.' This'
~report was presented by B. I. Stepanov. Orlg,,art.~fias:, 6 formulasi;
MSOCIATION; Institut fIzIk1 AN B88R (Physics InstituteAN jBSSR) i 1)
ODEs up
~:SUBMITTED: 05Jun64 ENCL: 00 S1 0
M REP SOVtV 003 OTHER: 005.
!Card 2)t2
T 7

a
L 6189?-65 AT(d)/D-FD(1)/T/EE
P
Ij
ACCESS 7--uk/061/001066 01306*i4d:
ION NR: AP5017906
5 3 5 .1112 . 0 6;1!;. 1.
AUTHM SotBkly, B. A.
On the possibility of determining the .-oher6iace -~f 4ncti
TITLE, 0
'observations of diffraction
ptil-d- i spektraskoplya vj --1:9
,SOURCE: 0
t lar'.
TOPIC Ti%GS., coherence function, opticai diffractitup:0 d
ern, cobearence, diffraction
.patt
!G10TMW`i', Tri vj-,~w of the. great di.ffictilties 11'nt6ilp-d in an,
tion. of the coherence function, the author
a
Prp ~ . - ,
t1he diffraction patternOt- o this: end- I
1V
A
17ir the intensity distribution in the foceLl plane- of a 1~ms pUtcad-:Q d- n'd the';4lit'.1.
ille validity o.--' this approach is demonstrate(I by an analyaii~6f t foiwula for tliej,
interisity of light having a specified coherence i'unction awl:!~rliffriic;te4 by a;,Aitj`i i
which i-s a Fredholm integral equation of the first kin& relat:lve coherence
function. An analytic solution for the coheren: ce -functioni ~-(~~itain~d,~ fkcm thts~ dn-
fu-d
tegral equation, is preserrLed, and it is shown'that to deteil~.ne tbe, coherence a
tion it is sufficient to measure the values of the ligttt itxt~isitylitni iL discrerte J-i
set of equidistant points. "The author thanks B -L Stvoa-n6~-,i B. ;b.j&ykQ A.1
andh Khamal~i& for a useful discusaicin. ort1r. 1~9 for- 1
nu I a
[;02
Curd 1 2

T 7 -717--7-F,
L 61897-65
------ -
ACCESSION NR: AP50179o6 ...... p!7.

:-ASSOCIATION: none

SUB1111TED 2lDec64
E[ICL:: 00

ODE:t
SI
op
;NO MF SOV: 002
01M, "R 003
PRES
4W~9
ATP

it

Card 2/2
7~

E
L 8106-66 E IVIA (k )/FqP/
4M~ k SCMAJ
'ACCESSION NR: AP5027672 UR/0051/651619/065 810791;
621-
-Y15-9:535-000
:AUTHOR-. Sotskiyl B. A.11 0oncharenko, A, M.4y
TITLE: Connection between the coherence of radiatiori and the nuiber.of modes ."I
jquantiLm generator
ISOURCE: Optika i spektroakopiya, v. 19, no. 5, 1965, 788-791
23
iTOPY. TAGS: L A5 rR AADnIrldo
.quantum generator, laser
theory
ABSTRACT: On the basis of the classical theory of coheren~~:(ik. i6 and E. Wolf,
rn
"Principles of Optics#', NY, 1959), the degree of coherencelof radiation in a quan-
I
~tum generator is evaluatedand its connection'with the number of:generated modes
tis determined. It is assumed that the radiation field of th~a quant
um,generator
iconsists of N planar harmonic modes having different frequelicies.and directions of
'propagation but identical (unit) amplitudes; also the eledtfomagnetio field is
~considered in a scalar approximation. It is found thab under stationary conditi6nal
;the radiation is entirely coherent, when only one mode is generate'd.*** Both spatial-.
!and time coherences rapidly deteriorate as the number of gefieratedmodes increases#
iUnder nonstationary conditionsp the radiation field of a lader is partially d0he, t
;the degree of 'coherence again depending on N. IfThe airLhorB wish toUank
Card 1/2