SCIENTIFIC ABSTRACT FR:MAGONE, J. TO:MAGOMEDOV, G.K.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001031400039-6
• Release Decision: RIF
• Original Classification: U
• Document Page Count: 99
• Document Creation Date: November 2, 2016
• Sequence Number: 39
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTR

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L X1225-66,
~cc x~: X3821
different mechanisms ~~
duc~ox$, (electronic ana phonon] of thermal c~anducti
melts A ~ ~ the thermal conductivity by a factor vit~r in $e~icon-
~ ~, and a ~wnp in the electric conduotivit s>f two is observed during
heating in the Liquid Mate ~~ aeenm,ied ~ ~ a feed-ar of ~. .
pity and thermal oanductivit . ~ ah increase in the~eleCtr.~rthe~
~eonductiyity c~tinues to rise ~e latter reaches a ~ at conductiv
the meta~ixatian of the bonds betweeneasing t 9~5K. The electric
emPerature and is connected with
aluded that gal,l.ium antimanide is a s he elements of the crnrrpound. It is conb
melting reg~.an, and has emi.canductor in the $~~lici state and in the
the ahQrt_xa a metallic properties in the liquid estate.
conductivit ,~ order during melting influent�~ The variation of
Y Orig. ~. ha,s; 2 fi 81l the cotsponents of the thermal
8ure$ and 1, foxmula.
$UB-CODE: 2a~ $~ ~p~; 2oFeb6s/ ORIa
REFS 019/ 0TH REF; 002
2/2
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b,..~,~25, b6 EW~'(q~)~L~I~iP (t) IJP (c;) JD
ACC NR : rA~003821
AUTHOR. SOURCE CODE: ~j,/018I,/~~p08~~1,/029p p ~
Am3,khanav ~
.._.~....~.. ~ LL I � ; owed 1 ~~
Comes Institute of ...,.. Ya~,~.
sine estan Branch .~
tansltogo fil~,ala AN SSSR ~ SSSR ~~
-.~..~.,..~-.~....~......~.,~....~v,~ Makhach~~,la
2'IT.LE; T,h,c~,~,l conductivit --~--.. (Institut fiziki
SOi1RCE: Y of allium an,~,.t~monide in valid
FYx;tka tverdogo tela v~..~ ~ snd liquid sta ,.~/
TOPIC ' , Sao. l tee
TAGS ; ~al~iurq all ~ 19~, .292 ,-::
electric conductivit �~''~ therms,l conduction ~
Y, heat c ~ ordered a1X
A8S1'RACT: a of states melts aY, semiconductor a
The puz-po,~e of the imresti ~' te~erature dependence u~'
' therms.3, conductivity and, the effe ~atian was to clari
The thexynal ~anductivit et of shox-t_ra ~'' the mechanism of the
mal canditidne Y wa$ measured ~8e order on its component
~atmospheret us' as described elsewhere ~' absolute method Parts.
3 ~ x lOi� R�a,Ycryst; (Izv. AN AzSSR v. 4 under '~tatianary then.
~- ~ a]a.ine samples of ~ 3, 1946) in an
!lisped res The ds'ta obtained at ro p`tYP@ Ga.Sb with carrier densitygon
'P~denee o the their is cZa om temperature
imed to be the first info agree we11, with the pub-
si;ates. The result~l conductivit rmation on tide to
~'e interpreted of GaSb at high t~Peratu~;+es mperature de-
;` fx'om the po~xt of v3 and in the
~ thst liquid
,Card ],/2 there are $eirexal
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r
t
i27R.~8-b-2~2;
.~� ~
Ai;,,HORo Uzbeltov t;i~R~, c,nd 1~i~,~~;oinedc~v~ a~G~, ueologists
TI7'laL� ~.Cl~e .~tan~:;cr l.rcln Ore i)e}~o,i,t�s i.rr It~.zakhatan (Atansaa�sls~.t3 are ,situated on the south-western
kc~hetay Oblast
K
h
�
a
2
o
e
share of Lake AtaY15G r ; i n t
were
but
discavared in 193 s
zakr~ytan~ The deposita wf:re
lored uri i l ~ 95.3 ~ ~++hen magnetometric pro-
ex
ll
d
p
y
not fu
The ore bodies are foame
spec ting shc~~ved their importance
nd amphbolic-
by layers r.f m~agnJtii%e', garnet ~rnagnetites a
f iron reaching in some
magne~:ite scarns~ the c.ontants o
I~iany other ore deposits are known in. this
`J
~�
places 53 ~ >
c anomalies observed here permit the
magnet?
n
d
_
y
ma
reg~or~; an
n of the available deposits of the 5tepnyaksko-
ti
o
estima
o be 5~U"S~~ million tons In future the
"t
,
Ate,n~~or area
n could sere-e as a second ore base for the
i
a
Atansor reg
Karagandinskzy met~~ll~lx~g~.cheskiy zavod (Karaganda ~etal-
lurgi:~al Plan~cl
Card l~2 There is 1, map and 2 graphs.
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a~~a~~_a_~~~~~ti~~
~.
AGCESSZO~t NR~: Ap5pig2~2 ~'
the wave equation. The
;finding the invariant ~,.placian, and solving
nitesima~. operators of U are then. determined as linear differ-
' 3.nf~. 3
gyrators and their matrix e~.ements are ce.~.CU1as~faedninnterms
~ential ope
Ib~,trary representation. ~e supermultiplets areTheainfiniteaimal
jof r ctangular etiagrams in the (~S, 2T) piane.
stare ~ -are ir~troduaed as linear differential Qresentatignd thThe
ope
matr~.x ele:nte are eomps~et~?~i~ aT.~Xu I~ob arev� ~d I~. ,B. ,.Okun,~~~,
authors thank ~'. _. B. Here ,~ -~" - f o~~~~s ~.
fug. di`~cu~sori~-`:~~~ __o~~~rrt. ~"Inas: 35~
;far he ~.p
ASSOC~AT~ON;t None
FNC~s o0
SU8 CODES
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sv~cT~Ens 03Feb~5
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card 2/? -~` ~ -.......~.:
a~~R: 405

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AUTHORS' ~agomedov, M. R.; Sudakov ~V.M V. ~.r,r ,;~'
Realization of the three dimensional. unitary group by ;~:.,
TITLE. ~,,,~:
e spher9.ca1 functions! ,~:~ g
~SOURG~� 2hurn~l eksperimental~noy i teoreticheskoy fiziki, v. ~9,
no. 1, 1~~~, 27~-rt2~1
~pp~C TAGS group theory, matrix function, mathematic operator
{ABSTRACT: 'fhe authors develop the mathematical formalism of the
three-dimensional unitary group U~ on the basis of a parametrization
means of special spherical. functions
Land realization of this group by
Which, fir certain purpose, have definite adv~ tihodsofvreali~ation
~stract-operator approach used by others. The
;is first ~.llustrated by applying it to a three dimensional rotation
'igroup. In th~.s aaae the method reduces to the invariantzrnetric~f a
~aaxiifold of unit vectors, determination of th
l~
(.Card . _. , _ .
~.
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o.------
- QQ
J ACCESSION NR: AT54Z228a
~~ Ori .art. has: 5 figures and 35 f ormula.s.
S
~p�~~r valuable c�mme~nts, � iapol' zovaniy
' irstitut goskomiteta p _,_
ASSOCxATTON: ~Magomedov~ Fizieheski.y State Catrnni.ttee an the Use
Ph aica inetitue$~�~:~.,,~,~g ~ti~~'~naY`.`.~~~-ki..
en~rgii SSSR., Yerevan (_.
Y at~.tute of The�zet'~,~ca't r
. at��w'oy ner '.:~.~'dalso.~�xnsti.tut te�ret~~Y ...~..... ,
energii SSSR t n.._..~..,._ ,.,~,...._,...,.,
of At~c ~,`~o ~~po~.' zovaniyu atofianoy am3~c ~.~~-
~ 4skomiteta p ttee, ot1 the� U e ~.~..~--~- ,;
and4 Ex,.,~e~im~eritial Pt-~t,~.,- '
CL. 00 _ S1SS LADE: ~i ~
S~jTTED. ,
d`~ER: 005 ~.
N0 REE` SOV; Ofl3
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AUTHaR� ~a~ont~dav, M. R.; ~udakovV,,,~ �V �..
,.{,,.
TITLE:: geelxation of athree-dimensional
functions"
un3,tar.~!'_.gr~lcp ~ "spherical
f~
komitet pa ispol'xovaniyu atomnoy energii.
SOURGE; USSR� Gosudarstvennyy t no. 311, 196G.
Institut ~eareticheskoy ~. eksperiwexital nob ex~icheskimilfundtsiy~uni, i-.3i ~~
Real.izatsi.ya trekhmernay unitarnoy gruppy f
article interaction, wave function
j TQPxG TA~GS� group theory, p
~ A convenient parameCrixation of the three-dimensional U3 group is `
ABSTRACT: ++ herical functions,,, which is
used tv x'epresent this grroup in the foam of C~-o eratoa: approach� The method
preferable ~~r certain puxposes�to the aa~am~tr#.~atian of the set of unit
consists of t~.e follawi.ng stePe� {1} p derivation o.E the
1 vectors , {2} detezminati.on of the i.mrar~.ant imetrices~tian� The supermu'itiplets
! ' solutiail of the wave q
. ~.nvaxi.ant X,aplaci.an, end {4}
classified in the form of square diagrams on the plane �S, 2T}� Infinitesi- i
are
ors sacs introduced in the fcrs- of linear diffexentiaioaoper~~ors,
mal group operet
. s 8nd Chelt' az~-Cr~.~ e~,ements aze computed for an arbitrary acepresenta
Bereetetsk~.y, I~ Yu~ Kab~_axev,_..ansl, L_�..._B.� .~,~ w,
conclus~o~i, tt~e authors xhank V� ~� _.~...,...,~..~w, :...~M .~_:
..~...Card..l/2~,. --
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ACG NR~ A~C~~+~73 '~~
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AUTHOR: ~ia~o~nodav ISh. A. ~ ~S.aiynulch~nadov, 'Yue Sv,s ; ~~lc?f t,u~.~ , ~i ._~'_P I
_, /
OIL ~~Tn~itut~ ai' Cry~ta7.lo~ra~~~y Aii S~i~ (Xn~si,:ituv kz�isi,al~.ut r~;'~.~. ~~;~ ~>.):~c~I
'~ITLF: Znfl.u�nc~ p~C d�ping on tha growth r~a'ta and moz�phalo _~t,~.r~.l ~._.,__~.__
~' ~,
~,~;~nic~o f i.lms ,
~~
SQURCE~ ~itristeLl.lograf~,ya, v. 11, no. ~, ~;.~6~>= 67;~..6aO
ibPIC TAGS G~-~tuli ursar~ida~, satll~.canzlUCLii1{; f~.1.m~ a~~-~,a~~.'~~, i;ro~r~.n~~ a`";,~c~~r+ductox
impurity, stoichiomotry, i;winnin~
r
c'~ t11U s.n~~l. C; E1 UL .liii c`~11C) CJ.~ C~t~IiLl.'=1 ~i;;G vl+ %l;' _: ~,J
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'I'~lo authors ~.n~ra., iiatc~ uorl ,
1ir;STi~~G ~ � ~ `
accap~ors an ~4hQ i;zowth rr~t;f~ acid sLrur.t;zr~~ ai: ~~t}~ta~;.~i.~:L ~'~.11n., ;~'c,,.%rl :,~ .r~+~ ~, ,
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Uar~.3.o~� cotlc:iusions ~~.�awn k~y~ kh4 au~.szo l'.~ (k~1�`LS~;~;.~. ~ ~ ., , ;
r. o ara~i n~ tkaa of f ~lc~t of ~toiciiioniQ~~z`y o k ~~,h~s ~.~:z11Rx~nc~rli;;~ r,~' t?lzl ~:,.r;iz~; ~z~^cb c,~; :., :'. ,;~,,; ~--
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at a given point, It is also established that in contrae~ a:o a ci,rrespandin~ twa-
dimensional scheme, the order of difference approximations is reduced to the first
order in the purely three-dimensional, case. Difference equations are derived, and
~~the parameters of the desired point are obtained fram two correlations along stream-
].ines and two along bicharacteristics. Four elementary problems are considered:
d~term~.nat~on v~ ~oi.nte inside the flow, on the surface of the body, on a shock wave,
and. end on a free surfe~ce~ The method described hems i~ su'bstant~.ated ~iy nu~merica~.
calculation oae hypexsonic flows peat a sphericuJ.ly blunted cane with semi apex ang~.es
of `~+�53' ~d 9�30' at M~,'= 6 and. at an `angle of attack p, = 5�. The author fi.hanke
V. 4'. Lunev for eanstant interest in the work. Orig. art. has: 3 figures end
'~5 formulas . ~~ ~
5~3B COIaE : 20/ SUBM DATE : l~Mar65/ ORIG :REF: 4O6/ 0TH REF: OO7/ ATD ~'RESS :
. ~~~~,

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Acc Na: S URCE CODE: UR 024 ~06"~o2To~i3T~25
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AU`T'HOR: Maga~nedav, K. M. (Moscow) ~
nom` ,1'X~ j'~
ORG: none
TITLE: A method of characteristics for numerical. calculation of three-dimensional
flaws
SOURCE: Zhurnal vychislitel'noy matematiki i matematicheskoy fi~iki, v. 6, no. 2,
1966, 313-~~5
TOPIC -TAGS: sup~:rsaniG seradynamica, eupersan~.c flaw, three: dzmcnsian~~l. fl.~aw, steady
flow, shock wave, flow analysis
i ~ '~,~ 1
ABSTRACT: A number~f methods of characteristics for numerical calculation of
three--dimensional su~xsonic floxs or unsteady two--dimensional. problems of ;as
dynamics ors evaluated and their complexcity stre:~aed. Anew approach is outlined
by which relat,~,ve s~.mp~.ici`ty and uni.i'orm~.ty axc attnined. ~'he equatit~ns at' a steady
three-diu~rasiansl supexsax~l.c f1c~w ttrc ~;rr~~sf~a~�mc~cl tc~ an e~,ui~alcr~fi, ~�~i~~,x~acte~l~;t~,~
form which is not the only possible one. Therefore, a general farm of cha.ractci~zstzc
correlations (aampatibility conditions } i5 car~sidered slang asingle-parameter family
�f bieharacteristics passing through a given paint It is demonstrated that an equa-
tian cl~seribing supersonic- steady flow can be reduced by equivalent tranafarmati.or,s to
a system containing variables only slang strea~nl.ines and bicharacteri:rf:~c d9.rec~is~r~s
Card.
U17C: ~17.9~533.7
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L 12773.66
ACC 6VR> A.p60a3369 ~~ ~
son of experime a1 weight loss measurement data Faith calculated data served as a I
cxiterian of a ui~.ibrium. Tt was shoFm that the near equil~,brium conditions ~'ar
GaAs thin filml eposition were:l000C at the GaAs source, 640C at the substrate,
2.26 x 10- m I.ar iodine concentrat3.on in the Hz + Iz mixture, and 5cm/sec space vel-
o~ity duet the ~o~rGe. Supersaturation in the d osz~ti.an region increased from 2 to j
xhen temperature was decreased. from 850 to 600C.~ thalpy AH was also calculated #'ro~
the experimental data both for the reaction at the saizrce: 2GaAsC;~)+ Tz(g = 2GaI(gl ..
-x.1/2 As4~ and ~vr the above given reaction in the deposition region. the AH~IOOK
of the ~ir~~ reaction waa found lower than the value calculated from literature data,
and AHlppng of the second reaction We,s nearly the setae as the value based on litera-
tu2~e date. Orig. art. has: 5 figures, 1 table, and 22 ~ormu~.as. [JKJ
SUB C01~E: 07, 20/ BUBM DATE: 03May65/ ORIG REF:- 002/ 0TH REF: 006/ ATD PRESS:
~i~~/
f
Car
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AUTHOR: t~~~cm~dov, Kh. A.
ARG: Inst~:tute t~P G etal.ln
Akademii I~auk SSSR
~ _.M.- 1~._-_t .,.--. .__..._.~.~.._ .~_
t~
_. ~.~
ay i Academy of Sciences SSSR (xn:~titut kri.sts,11 ~~ afi t~
TITLE: Equilibrium conditions and supersaturation in the GaAs-Tz-N2 system
SOURCE: AN S$SR. Izvestiya. Neorganicheskiye materialy, v. 2, no. 1, 196b, 11.7-123
TOFIC TAGS: crystal growth, epitaxial growing, palli.wi~ arsenide, thin film, chemical;
transport ruction, reaction meehan9.srn
ABSTRACT: 5upersaturation of the vapor phase in the ~taAg deposition re~;ic~r7 t~is been
caleul.ated as a function of crystall.izsti� ,~temperat~.~re in thh GnG~---i~~:i C range i.n the
open flog system of a~u~~arseni.d~~i.oc3i.n~hydra~ez~~~ This researci~ work was prompt-~
ed by the lack of data an supersatura.tion which is a very important ~ar�r~meter of crys-
tallization, ,and determination of which helps to understr-end the mect~a.ni.sm of crystal
growth by chemical transport reaGtians. The known farmulw for isobaric--iso~thermic
pgtentia~. was used fc~r calculating supersaturation an the basis raf the experimental i
equi~:ibr~um data which were obtained .far the reaction: 2GaAs(s + GaI3(g) ~ 3GaT(g) +~
I/2 As4(g) in the deposition region of the open flow system. The open f~.aw apparatus
was a v~rtica7. tube in which hydrogen saturated with iodine vapors was flowing at ~
atmo$pheric pressure and in a temperature gre~dient thrau$h a layer of GaAs. Campari� ,
U.L1C: 541.123.3--546.6$l'191-546.15-546.11
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~cz ~~:APSOO~2~ ~.~ sov~~E col~i~: ~1R/Q363/65/001/Q12/2ii3/2119 ~,- f
AUTHaR; ~a . l'~hF A. , Stint', N. N. ~,
~~
O~t~: Instfb~ttie of stall~a Y Academy of Sciences SSSR (Institut Iarietaltografi! Akac
. nauk SSSR~ ~"`
~~
T1TLEe Mechanism of growth and defects of epitaxial gallium arsenide films
SOURCE; AN &SBR, l~xve~~iya. Neorganicheekiye mate~rialy, v. 1, no, 12, 1886. 2113-2118
TOPIC ~AGBs epitaxial growing, gallium arsenide, crystal defect
ABS'1'RACT: 7t'!~ effect of mainly two factors, the crystallization temperature in they 554 -
850C temperature ran~+e and partial pressure of iodine in the p.8 - 8 mm Hg pressure range,
on the perfeat~an of GaAs elaitaxtal .films wan investigated. At 940 -~ 650C packing defects
in ~ form .af equflatexal triangles, isosceles trapezoids, and :single lines are faxaied on
surface A (111. So~rt~-ttme~ ~xowth pits atsu appeax. At hfgh~r temperatures of the deposi-
tign zone (7~p, -- 8500), only growth pits in the faxm of trigonal, ditrigonal, xagonal true-
" sated, and complete pyramids are- formed. The formation of stacldn faaxlts growth pits
is due to. the presence of oxide islets of ~-~s on the ~eubstra'~': ""~"~o gr'i~wth pits cnr stacking
.fasts axe formed ~ auurfaaa B (ixi~, Ibut penebratic~ twins appear at low temparaturea~ (84UG~
. and truncated complete ppgaxn~c~e are forn~d at 70q ~ 78gC. tN~n th~i~4~ ~-ouurtxa is at
1~O~C and the i~uhst~a~e at 9400, the Iodine pawl p~ssure !s 2. ~8 x 1a mm Ng aa~ the
UDC;. 546, 88 ~' 1,91
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. .M1 Ate-1'HOR. 11~ : edcyv;w . At ; ~ha~', N'. N, , ~` ~ "` -~
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1 . �3~CG; ~ nom . ~ ~ ~ , ,.~
. ~f,TLI~; A{~~~= ~ epltax~al ~1~um ar~en~de fi~~a.: (Papex presented at tbc~ i~,
~~ C~i~'+ereirtcu ati : stal4Cixo ~~~ in~ ow prom .18 to ~5 ~tavem-ber 24~63.1.~-r,-~ '
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~~t#tu~,krisi~al~og~sf'4~, Rost kratalic~v, v. ~, 1965, 388-392 _
_ _
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~~~`.; .'~~~ ~TA~~:;� ~'~,:; ~"~~ giul~ ar~et~d8
~~.. ..
~'he�article describes- the apparatus and method developed for preparing
t ~ AASTRACT: In this method, a
�;~',~ ~:. epitaxial ga~~iu~ arsenide films by the open; hydrogen-iodide method.
,, stream. of hydrogen carries #odine vapor, which encounters gallium arsenide in the high-
u4 __ ~: _ . :._ - -
:. ` temperature zone and reacts as follows: 2GaAs -}- J,= 2Ga7 -}- 2 Asp, _._.
~~ ~'
;.The ~~e~~on;proilucts are carried to a,cdoler zone, where the second reaction occurs on
.,._...
s tie surface a~f a substrate: .~,.~. _ __.:... _ __ _-
~ ~ ' 2GaAs ~ GaJ, '3GaJ -~- As,,
{
:st .1~.;1~ 1Saie.-/14.s~ _.i:._ ;C. .. u.' >~ ':~r.