SCIENTIFIC ABSTRACT MAK, A.A. - MAKAI, A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001031420006-4
• Release Decision: RIFPUB
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: January 4, 2017
• Sequence Number: 6
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

ACC Hilt AT6001396

fairly ~andc~ but strong increase in brtghtnes~ was observed at the instant o~ maxi-
mum radiation ~n the region of the positive elect~xle In the ceae off the spark dis-
cha~ge taking place in helium and nitrogen. The authors express their deep apprecia-
tion to S. I. Levikov ~ho p~epared the hydrogen ~nd deutevim are la~ps, and to
H. N. ~l"~-~--~o them. O~lg. ~t. has: q figures, ! table.
calibrated
SU~ CODE:' ".~ ~7 SU~S V&~: CO/

ORX'G HEF.' OOX/ OTH REF: 000

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AUTHOR: ~~ (Candidate of phvslco-mathematieal sciences.
A.; Yegorova, V.~A.A. ), aktionova

ORCr. none

TITLE: Radiation from spark discharges in gas mixtures

SOURCE: A~___~N SSSR. Komissiya po nanc~~afii i kinematografii. Uspokh! nauchnoy

TOPIC TAGS: gas discharge plasma, gas discharge, xenon, helium

ABSTRACT: Earlier s~udies of ~he gh~ness of spark discharges showed that while in the
case of light gases such discharges produce high temPerab~e channels but achieve the limit-
ing brightness only with strong discharges and at high pressures, heavy Inert gases exhibit
low limiting brightness, but this limit can be reached under soft discharge conditions and at
low pressures. In the present note the authors investigate experimen~dly and theoretically
a mixture of a light (basic) and heavy (admixture) gas which would allow the formation of very
bright channels under soft discharge conditions and low pressures. Calculations of the ratio
of energy losses due to the admixture to those of the basle gas And of the ratio of the respec-
tive coefficients of absorption showed that the most promisfng seem to be mixtures of g~_es
of very different atomic weights (e. g. ~ He + Xe). Experimental results are summarized in
Fig. 1.

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, ,
ACC: NR, AT~001399

W

Card ~ ~.

Fig. 1. Spectral brightness density as a function
of Xe admixture in helium base gas

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ACC NR, AT6001399 ~

The brightness increase found in He + Xe mixtures did not materialize in teste using He + Ar
mixtures, Ori6. art. l~m: 2 figure~.

SUB CODE: 20 / SUBM DATE: none / ORIG REF: 003

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/~CCXSSIC~! ~.m: AP~'~Oll~;99 S/0051/~/016/001/015)/0155

AUTOKOn: O-~lnJ~iono~a, N.M.; '~..Ls.k, A.A.
TiTLE: Spectral-time characteristics of the rad/ation of tubular xenon flash tubes

SODRCE: O~ika i spu]~roskopiy% v. 16, no.1, 196~, 15~-155

TOPIC TADS: flash tube, xenon tube, laser, laser source, discharge tube, xenon
spectrum, flash tube efficiency

ikBSTPJ%CT: In view of the importance of xenon filled flash tubes in lascr research
~ud operation, tubes of this type have been investigated to ~ctcminc the c;~c-
sion spectrt~ and energy output as ~ f~nction o� ~hc tube parameters ~nd the dis-
charge conditions. The test procedure, %fnich entailed the use of a D~.LR-4 monochro-
~tor and a ph~oclectric record/ng attac!%ment, has been described earlier (~4.P.
Vanyukov, A.A.]4ak,and N. V.Parazinsl'~ya, Opt.i spewer.,1956). The set-up was
calibrated with reference to a ribbon filament l~mp. Values of the peak spectral
density su~d brightness tempera%ute for differen~'a for tubes 3 mm in diamet~r ani
40 mn long (1) o.nd 7.5 ~m in diameter and 60 mm long (2) are ~abulated (discharge
cond/tions: V : 1000 v, C : 30~;af, L = 0); auothcr ~able gives the energy yields

C'nrd

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ACC. NR: AP401~99

in percent for different wavelength intervals for tubes of type (1).
Soectral distribution and intensity versus voltage curves are given in figures.
~,o e.xyerL~.ental results indicate th~b under the discharge conditions employed the
s:-,e�'~ral luminous density does not depend on the dimensions of the tube and corres-
ponds to ~he radiation from an absolute black body at l?000~-lS00�K except in the
ultr;~violet, where ~,e brig~'~tness tempe~-atu~e is somewhat lower, and in .the regions
of some Ze lines where the ~empera~ure is about~ 20OO�K. Orig. ar~. has: 2 tables

ASSOCIATION: none
SUBMITTED: O4Apr63 DATE ACQ: 04Apr63 w..~CL: 00

S~M CODE: PH NR SOV REF: 004 CTHER: 0OO

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ACCESSION NRt AP403S&8&

'-'~AUTHORI Anan"yev, Yu. A.~ GaXakcionova,'~. Sedov, B,
T~TLEI The emtsoton spectrum of a samar�um 2+ doped ca~ctum

SOURCE~ Opu�ka
TOPIC TAGS~ emissLon ,pec=rum. calcium fluor�de laser~ samartum 2+
doped laser, laser os��11a=�on specurum~ laser
ABSTRACT~ The expe=�men~al ~nves~t~a~ton off ~he emission spec=rum
of a samarium 2+ doped fluor�de laser (emiuu�u~ ac 0.708 ~) was
performed =o es=abl�sh ~he rela=�onsh�p beu~een =he =empe=a=ure of
crys=a! and
uhau wh~ie au smal~ pump~n$ energies ~he number of Bodes ~S ~ndepen-
den= of =he

SlOO~II6410~6100~IOg~IIO~&

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ACCESSION NR; AP4035484
16 when the crystal �s heated to 6OK, Theoretical and exper�menCal
eatine, due Co Stokes losses, of a crystal
results ind�cace chat.the h_ ..._~ de~.when the ~ump�n~ energy
-~ --- lono at 2SK ts Less than ~ f ~ ---~n~ the oscillation puim~
22 Joules and 1~20 ~eg ~t .__L ..... bu O,09~, while the distance
the wavelen 'h e c, mooeli 'iil;iL, a, O.08Sl.
between adjacent moses reda ' s-ec~ral shift of the laser was
hea~ing of the crystal,_tne tota~__p -eatin- rate was ~O.02~fdegree~. �
ted during oscillation from 0.035~
~0.6~, and thus the shift versus
wld~h of spegCral ~ode~ var._ hat the.various modes are
(start) ~o u,u~-~ � ..... Splitting of spectral
independent ~f each other only at the star~.
modes into 2 components was observed at the start of oscillation;
l~ amounted to ~0.03S~. ~he reason for this remains unknown, Orig,
ar~, hast 1 formut& end $

ASSOCIATIOHI none
5U~MZTTEDs ~6Au$63 DA~K AC~I 22May64
~0 R~F sort 00~
SUB COD~I P~
._cor~' } / 2

gHCLt~ 00
OTRERt

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ACCESSIO~ :IR: AP4039712

S/0051/64/016/006/1065/1068

,\UTiiOR:

TITLE:
d~rin~

Anan'yev, Yu. A,; Mak, A. A,

...... ' -tion of resonator characteristic$ in an optical laser
..~fa~ion process

0?tLka � spektroskopiya, v. 16, no. 6, 1964. 1065-1068

i,-~TiC i','..CS: ;optical laser, solid state laser, fluorite laser,
sam;.rium uoped laser, ia:~cr resonator

,\BSTRACT: 'The Stokes losses and nonun�form pumping of a sol�d-state
laser can lead to ~he deformation of the crystal rod and the parallel-
ola:c system. Experiments w�ti~ a dLvaicnt samarium-doped fluorite
laser were carried out ~o lnves~�gate the variation of resonatoc
characteristics in the generation process. A crystal rod 8 mm in
diameter and 33 mm long with flat ends was used. Dielectr�c coating
aboun ~.76~ ~ thick was applied to make the ends reflective. The
crystal was pumped by aquare-wav~ 700-aa~c pula~a by a flash lamp

Cord

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ACCESSION NR: AP4039712

in an elliptical reflector. In order to Investigate deformation due
to pumping, t~o identical crystals ,~ere placed separately in each
arm of the Mach-Ysender tnterferometer and only one crystal was
excited. Comparative photographs of tntt:rferograms si~ow that the
t;~cr;:;al deform., :on of crystal is a rune'lion of the initial
temperature of the crystal. This [s due to an increase
coe:flc[cnt of ti~ermal expansion of fiuorite with [ncrea~it.,s
tcmpct*,lgure. The difference tn the optlc,,i path at
t,,,~ ,~.~ ~e of th,~ rod is 1.5 bands at .'~ Init ial temperature of
..... � i:;~p[n,i-o:lui'Ky .ci~riity of 3~,) J /cra) o~ t~,u cry:;~al. At a~l in,rial
t ,',~,: :Lure o: 5OK, the avcra~Ic tem;~erature inc;*cas~' du,' io pumping
,...~ iii,.. '/iio ;lature of crystal deformation is independent o~ ge~lera-
t ion i;; a ct'yatal. Ti~e density of abaorbed excitation ener~%v
35; hi::her alon~{ the crystal axis tlian the average density Iii the
tryst.ti. Additional deformation ocnur8 In the form of cry~tai
i,~:,;~c:,caln%. This lead~ co a change in the wavelen~ th of ~tlmulated
e~,lsr;ion, ockg. art. haul i formula ar.d 3 liguria.,

ASS OCiATiO;;: none

;.,., i/3 -

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y~ B. A.; ~ A. V~ ~, A. A., ~~, D.
0~: ,one ~1
T~: ~se gene~ti~ with CaFm:U~ c~

(~i~h~), v. ~, ,o. e, ~% ~-~ ~
~C ~: solid ~te ~s~ ~ser ~tions, ~ser �
i, � .o,k
~ ~hich e~i~ of mon~se gene
~53s ~5) ~ -~.~ v. ~. ~ese~ ~er the a~hors r~ at~e~ of
with C~:~ ~s repo~ .......... - - -
~no se g~m~ion with C~:~ a~s ~t ~vele~hs ~.~ ~ ~.~1
e~~ s~ ~ w~ch the c~s ~e cooled to 80~X ~ e ~ off ~tr~en
g~ ~t~ ~ the li~id p~se (~. 1). A s~tr~s~t c~ti~ with re~ee.
tion c~cie~:,R = O.~ � 0.6 was d~sited on one e~ of the c~st~. ~e catty
switcM~ ~ ~ me~s of a r~eti~ t~ ~er~-re~e~i~ prism. ~e
i~tion ~s ~o~zed ~th a ph~oele~ric ~ c~led to the ~ism r~ati~
mt 1--2 x~ ~. ~e c~st~s used were ~~ ~ ~~ ~d ~ ~ lo~.
~e ~iati~ reeeiv~ ~s a Ge :Au ph~oresi~es ~ the generated ener~ ~s me~
~ed~tha~l~- ~e ~n~e ~s~ ~t ~ = 2.~ p.~ of the
t~e (~. 2a)~ ~th ~ssi~ ~er~O.1 x ~' J, c~~ to a ~se ~er of

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ACC N,. At~028019

! S,ynoh~onJzm&~'' :~

.~Jg. 1.!~ Experimental setup

'Rotor

i. Forelaeuu.
� Cool. aye.'

~ x l0s W. In several crystals monopulae b-level generation (~ - 2.~1 p) was ob-
tained, appareatl~, because of the high co~ce~tratio~ of the activator i~ these crys-
tals. ~he shape of the ~u~,se ~nss the same as ia Fig. 2a. The maximum laser enere~
in the monopulse ~e 10' J in this case (lmlse l~wer '-~ x 104 ~). At sms~ler ~isn

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speech, s-everal laser gulses were obtained rather than one (Fig. 2b).
has: 2 f~gures.
~ .
SUB CODE: EC/ SUBM DAi~E: 31Au~65/ 0RIG REF: 002/ ATD PRESS:

Fig. 2, M~nOln~se oscillo6rems

Orig. ar~.

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L 5026595 SOURCE CODE: UR/0056/65/0~9/0o4/lo68/lo~i
AUTHOR: G~tionov% N. M.; Ye orova v. e-., M~ A. A.

TITLE: The effec% of ~om~ous disper~ion on %he e%lmula%ed emi.sion
c~stals
80~: Zh~ eksperimental'noy i teoreticheskoy fiziki, v. hg, no. ~, 1965,
TOPIC TA~: solid s~age lau~~ s~im~a~ed e~ssion, ~sperston, ~om~ous ~sper-
8ion, ~peegroseopy, ~sprosi~ ion, ur~i~ ion
~ST~CT: A s~u~ was ~de of ~he sti~a~ed e~ssion spec%fa o~ CaF2:~2+
~ x = 2.36 u, ma c~2:u~+ e~u~ ~ ~ = 2.22 u (eec Fig. 1). ~e e~%~ ~em-
pera~e w~ varied in ~he 30~lOOK r~ge. ~e dependence of ~he l~neseenee line-
width on ~e~era~e was e~ablisnea for ~o~n e~%~u. Spectroscopic inves%iga~ionu
earrie~ oug by me~ of pho~oelee~rie e~pmen~ wi~h a Fab~-Perog e~on
= -- 0 ~ ~howea ghe~ in ghe above %e~e.~e r~ge ~he C~z:U3+
,L ~. 10 p_~_~. ~..- ~~ ~h~'~.~z* d"~~:~a~]- which is in~cative
hibited m ~ren~z ixne ~u~p~, ~- ~. -
-- 2+ sfas. M~til~er ~electric
~of a non~ifo~ line broadening in the CaF2:~ c~
.~rs ~th a 98% .reflection coefficient (at I = 2.B6 ~) were ~ed. Spect~ sc~ing
� was carried out ~th the etlon inside a v~iable-press~e b~ic ch~ber. ~e ~s-
placement of mo~es (up to 0.1 ~) due to te~rat~e instability w~

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L 2082-66

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ACC NR, AP5026595
The number of displacements for CaF2:DY2+ was from 1 to 3, depending on the crystal
temperature, excess threshold energy, and mirror transmissivity. The decrease in

Fig. 1. Stimulated emission spectra

a - Pulsed mode, L = hO.5 mm, T = 9?/{; b - pulsed
mode, confocal resonator, L = 36.5 mm, T = 9hK;
C - continuous mode, L = h0.5 mm, T = 80K.
temperature and the corresponding narrowing of the luminescence line caused a de-
crease in bt (difference in wavelength of two adjacent axial modes) and, in the case
of CaF2:DY2+ disturbed the mode equidistance. The. averaged experimental data are
presented in'Table 1, The data indicate that the effect of anomalous dispersion of

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Table 1. Averaged experimental data

C~st e/ r,, ~ Mirror Operation
sl~ty e % ~deo ~tio
C~2:~2+ 2~ 20 Continuous, threshold ~80 1
Conttn~ ~ euper-
threshold-3 ~0 2 0.~7 1:0.07 0.~
C~tinuous, super-
threshold.] ~ ] O.~t 0.~ 0.5~0.5~1 0.$3~ 0.62
7b 2 0.~ 0.83
~ ~ O.k~ 0.93
lOO 2 o. ~8 1.o
C0~-
~6 ~ 0.2 t~0,? o.~

eq~diet

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ACC NR, APSOP6595 0
the stimulated emission speetz~',m of crystals, which leads to mode tightening, can
be considerable. When no thermal effects are assumed, mode tightening is independ-
ent of pumping. A fully quantitative interpretation of the data would require con-
sideration of effects associated with the field distribution in a resonator and
other effects (H. Haken, H. Sauermann, Zs. Phys., 173, 261, 196B; 176 bT, 196B).
Orig. art. has: 1 table and 3 figures. '
SUB CODE: .~$y OP/ SUBMDATE: 21May65/ ORIG REF: 006/ o~ REF: 0os/ A~S:

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~ HR AP60i5~33 "
-- '~ ~- ~ S0URC~ C0D~; U-------~O~o5/o~nxn,.,.'
0RC: ~ne .....

C~A-RDP86-00513R001031420006-4

TiTL~;: L~inescence and ett~.ulated emission spectvu~ of CaF2.U3+ c~stal8

SO~: Opt~ka ~ spekt~op~ya~ v. 20, no. 5, [966, 890-897

~OPlC TAGS: ~s~t~on spect==, excitation spectv=, Z~nescence ~ec~,
phosphor, fluo~te~ co[o~ cente=,

~ST~: Data a~ g~v~ ~m a dens,zed anaZys~s of the ~so~t~on, Z~nescence)
~d st/m~ated ~iss~on spectra of fluorite =yst~s activated by tPivalent u~ani~
ions at ~.2--300OK. A vacu~ monoch~a:ol~ w~:h a ~solution of 1.~3 ~ a~
w~ used fo~ taking the ~so~ti~. . .
wi~h a ~ungs~en fllamen~ w~-~e~ _and l~l~escence spectra. An in A=2.5
fo~ ~c~tln~ l~ine ........ candescent lamn
Ph�~�multlplie~d' &'c~d lead ~u~ide ~sistop were used as detectors. The ~eco~-
� -u=flue ~ the c~stal.
~& ~sTem ~s ~de ~ of ~ ~plifie~ a~nous detector, ~a. PSI-~ electronic
potentiomete~. It was found that ~he ~so~tion spectra of these cPystals
a~ least fou~ types of colo~ cent
the first being lilac :- - - ~.. T~ ~eclmen,
~- co~om ~ the se~nd--~d, w~e divided ~o ~o c~sses,
~e~is~i~ ~ ~so~t~, l~inescenc% ~d excitation ~ch ~ype has its distinct c~ac.
~ec~pa. C~stals containi~ ~th
1/3
~C: 621.375.9 : 535

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types of centers (mixed type) show Bore comp]ex spectra. The difference between c~ys.
:als of :he first and ~econd type is most pronounced in the absorption and lumines-
cence spectra in the near infrared region. The spectrum for crystals of the first
type is rather simple in the 2.1--2.6 ~ region. Absorption resonance lines are ob-
served at 2.15 and 2.223 ~ and an additional line is observed in the luminescence
spectrum at 2.~3 M which disappears at helium temperatures as well as a line at 2.512
M which is observed at low temperatures. Luminescence excitation in crystals of the
first type is due chiefly to absorption in the 0.q-O.6 ~ region of the spectrum. The
spectrum for crystals of the second type is more complex with six resonance lines at
2.15, 2.252, 2.2q6~ 2.237t 2.22~ and 2.221 ~ which may he due to transitions between
the ground level and splitting components of the ~ll/2 state. 5uminesce~ce excita-
tion for crystals of the second type takes place chiefly in the 0.7--1,2 ~ spectral re-
gion due to wide absorption hands. Experimental data were used for constructing the
diagrams of lower levels for crystals of both t �
served between centers ~ ~ ......... ?es.. Considerable interaction is ob-
the first type sho~ of th~ ..~a~ ~u seCOnu type An mixed crystals. Crystals of
stimulated emission in three spectral hands: 2.512' ~, 2.~35 ~,
and 2.223 M. The POsitions of the emission peak with respect to time for the 2.512
and 2.223 P hands show a considerable degree of correlation.
~ne hand corresponds :o :he m~n~mum ~n the --~-~ ~ _. the e~.ission maximum in
nave a common initial unmer leve' ....... x~icates that these
second tyne in :~ , ~-~-~ ^ ~' ~:x~u~at~.emxssion is observed - -~
-~ -o uue oaszcazAy to absorption band~ a+ , ~---~-~ ~,~a~on ~n crystals of this
'Card 2/3 ' . ....... a,~ u.u ~. ~xe~ crystals show simul-~-

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t~-~eous emission /n the 2.5Z2, 2.5Z8 and 2.518 ~ bands. The Interaction between cen-
ters of the first and second type in these c~ystaZs is discussed.
?lfig'urea.. O~ig. a~t. hae: .'
[~}
SUB CODE: 20/ SUBM DATg: 22Jun6~/ ORIG Rt~F= 005/ OTH REF: 003/

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T. 44076�66
;--~AC~ NR~ ~'�O'~OTZ3" SOU~C~ CO~: 'U~/O36'8/'6~/oos/oo~/uZ~T/O~TZ
AU~OR: ~to~hina~ Ye. N.; Kozlov~ N. A. ~ H~, A. A.; Stepanov A. ~ Prile

~ORG: none
considered. The efficiency of eiii~t~.~- ~d ~iruu~r-~-/i~naer rez'ie~tars ~:~.a z:.e

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-- ~cc -r4~ .... ~g~-:~i~ '- -

diameter for which the ef'f".::i,,n.".; [.. ': ~;u~:~ ~tcrmpt~ when the mirror (~ - 150
was exposed to radiation for 30--40 sec. Orig. art. has: 5 figures.
SUB CODE: 20/ 5UBH DATE: 31Mar66/ ORiG REFt 007/ O~H ~F: 007/
ATD P~SS: 5108

Card 3/3

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ACC NR, A1~OO4139 SOURCE CODE:

AUTHOR: Oalaktionova, N.

OEG: non e
TITLE: Spectroscopic investigation of CaF2:DY crystals
SOURCE: Optika i spektroskopiya, v. ;;, no. 1, 1967, 68-73
TOPIC TAGS: calcium fluoride, actOrs'ed cry.~tal, luminescence spectrum,
~/ectrnlm, lane width, lAne broad,2nin~',
ABS~, \CT: The authors used hi6h-r~?,oluti~m a]q.r~ra!,us, consistinf{~ o. a diffrqct~on-
Krating monoc~omator and of a ?'ab~,'-Fcr.+t inteferomcter combined
mator, to inves~,igate the l~n[nesce~~e ~:-..~ ~b~o~-i~i:>n spectra of Ca -~:~.,

the production of other cente:'s in t~'

line widths were fo~d to be quite

Card 1/2

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ACC NR: A ~0041}?

weak t~.m, perature dependence. The br,~u:..:;,inl; is
chemical reduction results in a iow,,~' ~/~ ion co~, ,];~.,,~.ti~n
[.y ~n the c~ystai~ than reduction i:~ c,]icium vapor
quenchi~ of the l~nescence is n.~g~glb].e. An
the lower l~els of ~ in the CaFe. ~)r~g. a~. has:

stm coDE: 2o/ su~4 ~0ATE: 2~)~65/ 0~],~ mC?: OO2/
ATD PRESS: 5115

Card 2/2

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ACC NR:

AU'fHCR: A:-.an'yev, Yu. A.; :,lake ,',. :'..1 2,,-�',', -. :-'..

OEO: none

~:;b'f~'.": To de%ermine the inf!~:e:'.ce ~_-" ~' ...... -~' ~' .... -: ~a"~.. .... ~� ~T/.'~z-'-"i-'r~ ........... ... - ':'",-.~-=','c'~._..~
of a solid state laser, and to asce:'tai:', t?,u d~:rce ~c.. ',.'hlch la:.cr -:.r..e _ ~l,-;~llcr. i.~
affected bi,' the connectlo:', bctwe~:n %:.e arest, an~ F~tor-ial boaru memb,. "Gep~artas--
technolm~ia."

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Jozsef

Application
'61o

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BA!.!.0, R~dolf, profo, dr.; 5t4XADI, Jozsef; MOLNAR, Imre; SIPOS, Jozsef

Contributions to the data of strength of plastics. I. Plastics rein-
forced ~r! fibres and fibre bundles. I. Acta chimica Hung 29 no.4:
463-47Z~ ' 61.

1o Department for Plastics and Rubber Industry, Technical University,
~ud~pesto

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BALLO, Rudolf, prof., dr. (Budapest, XI., Muegyetem); P~jDUC?iEY, u. !.".rs
(Budapest,)il., Mue~yetem);~!-b\K~.D._I~ ..J_ozsef (Budapest, ].ii.,
Budafoki ut 32/e); MOM4AR, .~mre (Budapest, XI., Muegyetem~

Contributic.' to t!e data on strength of plastics. !'t.1.
Acta chimica ',' ' 129-1~ '63.
~.~.~ ~9 ho.l:

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KERTAY, Nandor, dr.; DOLOZSELEK, Gyula, dr.; MAKADI, Margit, dr.

Epidemiological and clinical importance of bovine tuberculosis in
children. Tuberkulozis lB no.12 : 362-365 D '60.

1. Az Orszagos Koranyi TBC Intezet (igazgato-foorvos: Boszormenyi
Miklos dr. kandidatus, tudomanyos lgazgato: Foldes Istvan dr. kandi-
datus) Mikrobiologiai osztalyanak es a Szabadsaghegyt Allami Gyermek-
szanatorium (igazgato foorvos: Szederkenyi Janos dr., tudomanyos
igazgato: Gorgenyt Gottche Oszkar dr., az orvostudomanyok doktora)
ko zlemenye o

(TUBERCULOSIS BOVINE in inf & child)

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~UU~_..~.L..I.,~. kandicl~t tekhnicheekikh nm~k; I~TSKIY, I.B., ~i~t

~etic time rely ~th~t con.ts. ~Y ~I no.l~:~3~ '~.
(Elec~ic rela~) (~ 8:7)

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MAYBURADZEs Z.N.; GABUNIYA, D.S.; LEGRAN, N.E.$ MAKADZE,
MAKHATADZE, N.K.; SARKISOVA, Ye.G.;
TSIBADZE, D.S.

Microvascular system of the cerebral cortex in dogs. Soob.
AN Gruz. SSR 26 no.4:469-476 Ap '61. (MIRA 14:8)

1. Tbiltsskiy gosudarstvennyy meditsinskiy institut.
Predstavleno akademikom A.D. Zurabashvili.
(CEREBRAL CORTEXmBLOOD VESSELS)

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M~U{AEL'YAN, T.S., red.; SAYTA~;IDI, L.D., tekhn, red.

[Growing hemp and ~::'ocessing retted hemp straw]�yra�hchlva~.ie
konopli i ~rerabotka tresty. Mosk~a, I~-vo M-va sei'.k~:oz.
[~FS[~, 1962. 107 p. (MIRA 15:lO)
(Hen:p)

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TESLENEO; I4AE.AQ.0N, ~. I.
~~ ~:;'
� ~ttachement to the C-225 and C-202 threed-cuttin~ machines for
the cutting of a taper thread on gas pipes. Vod.i san.tekh.
no.9:31 S '~7. (MIRA 10:11)
(Gas pipes) (Pipe fitting)

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_. MAKAGON ..Mt, .
ImprovlnE conveyer performance. Ma~t.ugl. 5 no.10:22 0 '56.
( RLI~A 9:12)

1o Nekhanik uchastka shakhtoupravlentya no.8-9 tresta Krasno-
gvardeyskugol ' .
(Moscow Basin-.-Convey~lng machinery)

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MAKAGONC5', POP,; SOLO~YEV,

Calculation of the correction for the effect of relief durir~
observations by a gravlmeter. Izv. rye. ucheb, zav.; geol. i
razv. 6 no.5:122-127 My t65. (MIHA 18:10)

1. MoskovskJy geo!ogorazvedochnyy inet!tut imeni Ordzhonlkidze.

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In the article~ "Experimental phexmacotherapy of Hypertonia and
Coronary Insufficiency in Simians With He: