SCIENTIFIC ABSTRACT BASOV, N. G. - BASOV, N. G.
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S
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100
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December 31, 1967
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0. (Basov, N. G.]; KMXHI-N, N. [Krokhin, 0. K.];
POPOV,
YU.
Pl4eparation of states with-rAgative temperature at
p-n trans-
itionf 6f degenerated semiconductors. Acta phys Hung
14 no,2 3:
2~~= IQ.
4 P* 19,10bedeu Institut fur Physik der Akademis der
Wis"up.-
-sobaften W$Rj, Moskayj U=,, Yorgelogt von G.
Szigeti (wigy
azigetil
RASOW2 1. G. EBwov, N. 0.1; CSIPOW, B. D. Epoipmj,
B.P.11 HWOSCHTSCHZWI
--r 40
, 1,41hoshobavp A.
Aeccubingtion luq~waoenoe of indium antimonide in strong
eleatrio field. Acta, pbya Hung 14 no*2 3;245-46 162.
1, P, N, Labodew Institut fur Physik der Akademie der
Wissen-
schexten UM, m6s,kau.. UW. Vorgelegt von 0. Szijeti
[.Gyorgy
4zigetil
W01- N-G.; KROHINO O.N. [Krokhin,, O.N.]; ORAEVSKI,, AX
[Orsyevekiy, A,N,J;
STRAHOVSKI, G.M. (StraMovskiy.0 G.M.11 CIHADILT,, B.M.
[Chikhaohovt S.M.]
Possibility of studying relativistic effectswith the aid
of the molecular and atomio standards of frequency.
Amaele
oft 16 no.203-146 Ap-Je 162.
BASOV, S. Go; IRDEM, 0. 1.; POPOV, J. M* [POPOV.,
yu. M-1
f
Negative aboorptibn ooefficient at indireot
transitions in
.oemiconductora, 4t&-Pbyw Hung 14 no,2 3t231-240
t62.
i
1. P' It cademy of Soisnoes
%,14bedev Phys-ical-Institutd of the A
uw: Moscow, USSR. Presented by Go Ozigeti [Gyorgy
Szigeiij
38861
9/056/62/042/006/0,18/041,
B104/BIO2
A1JTHORS: Basov, N. G., Orayevskiyj A. N.
TITLE; Emission of molecules in a mixed energy state
PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fiziki, v. 42,
no. 6, 1962,-1529r.1535
TEXT: A double resonator molecule generator is investigated. It is sh..~
that a molecular cultrent polarized by a monochromatic emission excites
a Al.
monochromatic oscillation in a resonator on which it is incident* The
frequency of this oscillation coincides with the frequency of the
polarized
emission. A change in the eigenfrequency of the resonator affects only
the amplitude and phase of the excited oscillation, not its frequency.
The emission-with frequencies different from that of the polarized field
is incoherent. Therefore it is not necessary to take the effect of
coherence into account while calculating the noise produced in quantum
generators and amplifiers by spontaneous emission. If the polarized
emission is not monochromatic the response of the resonator is also not:,
monochromatic for small intensities. The spectrum of the response affects
Card
BASOV, NX.; ZUYEV, V.S.; KRYMV, P.G.
Increasing the power of a ru~~type quantum pulse
optical maser
by resonator Q-factor modulations Zhur* ekspe i teor.
fiz. 43
no.l.-353-355 J1 162. (MIRA 15:9)
1. Fizichookiy inatitut im. P.N. Lebedeva AN SSSR.
(masers)
S/056/62/043/003/058/063
B104/B102
AUTHORS: Basov, N. G., Karkin, Ye. P., Mash, D. 1.
TITLE: of neon-helium' quantum generator
FFRIODICA;,; Zhurnal eksperimentallnoy i toorstiohaskoy fiziki, 'v.
43,
nz~. 3(g), 1962, 1116-1117
TEXT: The quantum generator shown in the figure is described. This
operates on the principle of A. Javan (Phys. Rev. Lett., 3, 87,
10,59, 6,
106, 1961). Thie discharge in the ias mixture is excited by-a 10-Mc
generator by -.-.-ay of external electrodes. Interference mirrors
with a high
coefficient of reflection are used. They consist of 13 quarter:-wave
ZnS
films and cryolite. The mirror backings were optical fused quartz
with a
transmi*5'sion factor of ab8ut 1 % for 11,530 9ft waves. Power ~nd
angular
deDendence of the 11,530 h emission were measured. The beam
divergence was
about one. angular minute and the power about 8.2 m-..-. The latter
remained
4 virtually constant throughout the-range of the neon-to-helium
partial
pressure.ratios of 1:10-1:4 but decreased when the neon partial
pressure Tas
further increased. There is I figure.
Al. Z:
8/2504/63/021/000/0176/0199
ACCESSION NR.- AT3012118
AUTHORS: Basovs N. 6.1 Zuyev, V. S.; Svidzinskiy,, K. K.
TITLE: Manor using a beam of Nr~ molecules
SOURCEs AN SSSR. Fizichaskiy institut. Trudy*, v. 21, 1963, 176-199,
TOPIC TAGSz ND maser, maser power output, maser frequency stabil-
ity, maser absoiute stability$ microwave band maser, signal to noisei
ratio
ABSTRACT: The purpose of the investigation was to ascertain the
feasibility of a maber using the inversion transitions in a beam of
heavy-bydrogen ammonia ND # and resulted in the construction of an
3
-11 W
operating-model of-sudh a maser generating approximately
at
10
1656.18 Me (line J 6* X 6 of the ND3 inversion spectrum). The
9
absolute frequency stability.is of thworder of 10 The calcula-
Curd 1/3
01;
ACCESSION NR: AT3012118
tions nd include
proving the feasibility of the maser are presented a
proof that self-excitation can be attained with sensible maser pari
meters and a calculation of the hyperfine structure of the inversion:
spectrum of ND 3* in addition to estimating the absolute stability
for the (6, 6) line, the possibilities of increasing the absolute
stability of the maser by-choosing other lines (3, 2 and 5,S) or by
14 15
replacingN with N are also considered. The measurement-results
agree well with the calculated data. The power yield of the ND3
maser is approximately one-hundredth that of the maser, but the
NH3
sensitivity of microwave receivers at 1600 Mc is much higher than
that at 24,000 Mc, so'that detection of an ND maser signal entails
3
no more difficulty tban.that of an N maser. The signal/noise rati07"-
-12 H3
exceeded 100 at 10
W. The resonator used bad a diameter of 14 cm.
and a beam length 1.2-1.5 meters, compared with 1 and 20-30 cm
2/3
ACCESSION NR: AT3012118
respectively for the maser. The entire apparatus (without dif-
NH3
~fusion pump) measured 1,5 x 0.5 x 0.5 meters and weighed 150 kg,
"but further reduction in size and weight is expected. "In conclu-'.
sion the authors thank A. X. Prokhorov for a useful discussion.
:Orig. art. has: 17 figures, 14 formulas, and 2 tables.
ASSOCIATION; rizicheskiy4natitut im. P* N. Dibedeva- AN SSSR (Phy-;
sics Institute, AN SSSR),
SUBMITTEDs 00 DATE ACQs 29JU163
ENCL: 00
SUB CODE:, PH NO -REP -SOVt 010 OTHERs. 015
Card 3/3
-2
L(k)/BEWP (1~ JPP1,74;1EEC(b) ftA t
L 1497-2-42 EW _ ,-- . - - . - --- '; I ~
- - ,-
66 _d
F
i'
4 A
-OZ-01-
WL
IJF(
AFM/A3P/ESD-3/F=/AFGC/A1
C)
TA
/
A=sIoN jiR: Ap3oo5363 S/0181/63/005 2 /2
/008 2384J 386
A=OR: Ways No. Of MMkh1Uj
'
!ranotcrmation-or'strons -i-Aromatic:
"radiation into~ electric
corrent
P
I SOMM.. FIZIka, tverdogo~telap~~V* I P
TOPIC TAOS t oitmicondiwtor. lwer$' r:..,
t-t6-alectrIalty converslci,.'llsbt-to-a
trails ade-e- r- lase r
detector
ABSMACT:
It is showA that strong radiation can bi'c:onve'rted:~
Into electric currentAn an
r, 7-77F.M. *w p-1-n semiconduictorvith strongly
degenerate p end n regions,
merent monoebromatic rad4ation is focused
on the semiconftctor, prod~xcing
-.771Mron-bole Odra, In this case the chemical
th,
potential in the electron region of Yie serd'eonauctoi (C.) wil.1 coincide vi
the
FQrmi quasi-level of -? r.T47 the i region (11.) j, and the chemical POW
tential
In the hole regi.on QI]CEMoincide vith the Fend quasi-level of the.
hole# In the
i region _; - =77. tion current can be made small if
Card 1/3,
f
0C
ACCESSION NR: AP4003988" S/0109/0-Y60810121208412086
AUTHOR: Basov N. G.; ~jArkin, Ye. P.; gikitin, V. V.
TITLE: Some charactcristi~ .s of the No and He laser ior A - 3.39 V
SOURCE: Radiotekhnika i'alektronika, v. 8, no. 12' 1-963, 2084-2086
TOPIC TAGS: laser, gasUlaser, pumping power, neonuhdlium laser
ABSTRACT: The Physics Institute AN SSSR has investigated the relation-
ship between the output of the neon-helium laser and its various
parameters, i.e., the dAameter and form 'of discharee~tubesii discharge
duration, mixture pressurl,,pumping power, and transmission coefficient
of the mirrors with metil c and dieleceric coatini ior the most in-
tensive spectrum line (Ne3S2-3P4,X - 3.39 V). GrapWs!of output power
Cin millivolts across the measuring photoconductive cell) as a func-
tion of pumping power were plotted for various pressures in the dis-
charge-tube. The discharge.length was 0.9 m. Maximum output power
was obtained with a pumping power of 1001w and a pressure of roughly
1-2 mm HS. The diameter.-of';the generatedtlight spot was equal to that
of, the discharge tube. Variation in Ne*.and He mixture pressure in
2~-
Crd
U
AICCESSION NR: AP4003988
the tube from 0.3 to 6 mm ft did not disturb the stable operation of
the generator. Generation cutoff occurred at a pressure of about
&,mm Rg. The optimum diameter of the tube was found to be 12 mm at
3.39 v. Output power depended only slightly on the change of
pressure within the range 0.9-1.4 mm H& and increased linearly with
the length of the discharge. Output power oscillations were de'Eicted
during nonalignment of the mirrors. Some 100 maxima were observed
during shifts of the mirror i10. The relationship between output
power and mirror transmigsion coefficient was investigated for co-
efficients of 2, 30, and 50%. The highes.t power was observed at 30Z.,
Afier the addition of *some spectrally pure Xe to the Ne-He mixturei
simultaneous generation at wavelengths of 1.52, 2.02, 2-.60, 3.10,
3.36,
3.39,and 3.50 is was obsir,~ed. With the Xe-He mixture, the following
14avelengths were obtained: 2.02, 2.60, 3.10, 3.36,and 3.50 p. Orig.
art. has% 2 figures.
ASSOCIATION: Fizicheskiy institut,im. P. N. Lebedeva AN SSSR (Physics
Institute, AN SSSR)
card 2/A
BAS071 N.G.; MARKIN, Ye.P.; NIKITIN, V.V.
'.
Output power of a noon-helium laser as a fimotion of
various
parameters. Opt. i spektr. 15 no.3t436-438 8 163.
(MIRA 160-10)
BASOV, N.G.j, B=ANMICH, O.V.
--- ~ I
1080A -*a of ,
Recombination Wr . I AiOA and Go following exc4tation by
fast
electrons, Zhur. i _. toor, fis. 44 no.311115-1.116 Mr
163.
(MIRA 16 W
31 Fisicheakiy institut imeni P.N.Lebedeva AN SSSR,
(Gal*um arsenide) (Germanium) (Quantum electronics)
_P~4wv -N.G.; ORAYEVSKIY, A.N.; STRAKHOVSKIY; TATAREIIKOV, V.M.
Molecular generator vith resonators connected in series. Zhur.
eksp. i teor. fiz. 45 no.6:1768-1777 D 163. (MIRA 17:2)
1. Fizicheskiy institut imeni Lebedeva AN SSSR.
191915 ej cl, A).
AZ Nr. 971-27 20 MW
EXCITATION OF RECOMBINATION. EMISSION BY MEANS OF A LAS1kR
(USSR)
Ba6ov, N. G. , L. M. Lisitsyn, and B. D. Osipov. IN: Akademiya nauk
SSSR.
5o-k-lady, v. 149, no. 3, 21 Mar 1963, 561-562.
S/020/63/149/003/009/028
experimental study of recombination emission in germanium, silicqn,
and
gallium arsenide at various temperatures employs a ruby laser (6934
A) to ob-
tain high excitation levels. Samples of n-type germanium with a
resistivity of
40 ohm-cm and a diffusion length of 1. 5 mm in the shape of a
')Yeierstrass
sphere" 8 mm in diameter were excited by light pulses with a
duration of
200psec and a density of 106w/cm~. Aspectrometer with a 1-ead sulfide
indicator (100 tL see time constant) was used to analyze the
recombination emis-
sion pulses. The signal was amplified by a broadband amplifier and
registered
by a dual-beam oscillograph. Laser output was monitored by a
photomultiplier.
Card .1/2
AID Nr. 971-27 2D )by
UCITATION OF MCOMBIrATION (Cont'd] 0/020/63/149/OD3/009/028
7be results show that the Intensity of r~~ombiiii~i~n_ emission
at the tempera-
ture of liquid nitrogen is "two orders" greater than at room
temperature, and
at the temperature of liquid helium 2 to 3 times greater than
at the temperature
of liquid. nitrogen. *Analogous results were obtained for
silicon'and gallium
arsenide. it is proposed that laser pulses of 10-7 sec be used
for further in-
vestigations of recombination processes. (Bbl,
Card 2/2
-- BASOV, N. G. ; BOGDANKEMCH, 0. V. ; 1104-j.11TOV, A. UG.
"Excitation of the semiconducting quantum oscillator by a beam
of fast electrons."
paper presented at the Symp on Radiative Recombination in
Semiconductors, Paris
27-28 jul 64. 'L~Intl Conf on Semiconductor Phyz~ics)
Of(.'~Y 1.V,-;, ~Y , 1AkoE,:,,-vw!:; V li J.), C-tv.
1'01.;
t~. - a- -.0 4
B~AYIJJI.Inll V.G.,, ret%
[Molecular generatt- ' IfolokuliarrVe generziton,. Nc-
skva~ Nauka, 1964. 2014 P- (MIRA 18:1)
1. Chlen-korrespondent AUN S~k,-~R (for Bnsov).
T P sl~~, F74- "k'."7-Vi-! ~L-? J'Y/-
7-rt
t5
Art S-z'."H. Vestnik, no. 196.4, ',9-33
TOPIC TAGSi sEniconductor, quantum generator
ABSTRk"T: This Is a nunm-ry of the development and uoev of such
generators.
'3r)-cla! is Piaced an the arifiliclation to o;D=uniGatwn.ltTnfOj-jp
-q- a-tion MEjy
now trrn!;r.Ittft~d to distances of tens of lir~ht years. The high
directivity
wn,! the ablitty- to lr):--,--i-, b('~!AS ~'.T(' ~,Dint(,d cut. Thc
r~iithnr the advwltages
vtlch 0 f
n. -:e c-,~' h !li,q,
--77.1
~;i em, 4; Z-3
th plprtr~nz; c)r h by I n t - --x3 u c7 t j --,i f -3.r, e r- 1, 1
ty a t-7, 07'hw very low
time Lag at fr-fl jufl,L-i- L"61'aLit.-
quen cy .Senicond,,ictor --uterials that have proved wiccessful as
quantum generators
liste-1 wi'h thei, rqfliation wu-7---!Pnrthii and -vith their
operating temperatures.
Card
L 858D-65
ACCFSSIGN VP AP,1046'~B~
Spenial emphasic in placed on the work accomplished at the Fizicheakiy
Institut in.
P. N. Lebedeva cai Institute ayid the Fiziko-tekhnichteskiy 4natitut im. A.
F.
T-M-e-r-Physical and Technical Insti-tutp). The author discusses a new type
of sD-M~-L--
conductor quant= generator developed at, the fir3t of these biatitutf~s
(curing the
A rf,n,~r~itor excitod by a benum of' hit~-h-spee~ Plect.rDT111. This
C'-F?Vr1Upzv-ns oi powerful and very efficient quantum generatore. Is it
otill neces-
san, t,) macihinlng or ib,? ?--att-rials? in it atill necesalLu Ln uGe
ent, as for erl
-m IV, ror tranomittnr evierry? May it rot b-e slm-,Ier, Rt leLtz'.
t
EWT A lip(
D J A F~vI,.4,SD ( aC ( n~ Sc D,
~ACCESSIOR NE': AP4045491 8/0109/64/009too9/1680/1686-!
'AUTHOR: Basov, N. G.; Gracyuk, A. Z.; Orayevskiy, A. D.
TITLE: Some special features of information transmission and recep- 1
tion ib-y-Asaus b-11P -1 .. 111'410'rbr and amplifters
SOURCE: Ruaiotekhtika Kolek-tronika, v. 9, no. 9, 1964, 166o-1686
ITOPIC TAGS: laser, multichannel communication line. laser bean,
traveling vave laser, Image amplifier
ABSTRACT: Some basic properties of multichannel communication lines
using the time afid space coherence of the radio emission of a laser
!
I
ioscillator concurrently %-,e studied. The information is transmitted
1by irradiating an object of variatle transparency with a laser beam.
~The authors demonstrated that the transmission capacity of such a
To ^I -------- I-- --tuds,
at using "reatu*rati I :C *rs - s- a so-- eea
,Card 1/2
-7
ACCESSION NH: APhOh5h91
The authors note that"" for the purpose of sinplifying the receiver
of a multichannel cozmunication line, It in possible to utilIze space
quantization of transparency functions vtth limited diffraction
bpectra. Orig. art. has: 7 figures and 8 fzrvulas-
ASSOCIATION: Fizicheskiy institut im. P. N. Lebeaeva As sosp
Mysics 7nstitute,AX SSSR)
SURM17TRO: 25Apr 63 ATD PRESS: 3112 ENCL: 00
F Z T V HE F.
BASOV;'N.G.
Semloonducwr lasers, Vest. AN SSSR 34 no,91l9-33 S 164o
(MIRA 17SIO)
1. Chlen-korrespeindent AN SSSR.
BASOV9 N IG,; KROKHIN, O.N.
Conditions for heating up a plasma by radiation from
an optical
manor. Zhur. eksper, i teor. fiz. 46 no.1:171-175
Ja'64.
(KM 17t2)
1. Fizicheskiy institut imeni Lebedeva AN SSSR.
%cc=imf m.- IF4031193
810056
/a/046/004/130/isio
AUMCF-6 333 jov.,-N.-Go; 1(roldlins 0- H-
seideoncluctors
mm Optical excitation of
Zh. alm-pore Iteor* C:Lzo.P Ve 46, no. 4, 19a, 1508-333.0
semiamftator lasor monochromstle radiation coherent
TOPIc VM: laser,
roagatich recodbinatica ridiation.. optical ymping.. optical
excitatica.0
resmant cavity
Excitation of semicoaductors by Monochromatic radiatica with a fri-
AWZWT;
s3
vency _j&tly bighor than that of the edge of the intrinsic
abscm"Ttic'm band
id investigatea theoretically. A battery or independent P-n Junctica
3=8n
is suMested as the excitation source of incchei4mt monodhmmatio
radiation.
high the SUQ
it Is pointed out.that Vhen.the Intensity Of Incident mdlaticu Is
quasi-levels for electrons and holes anromobes the OnerjOr
MP cc Pd=i cc
1nci4oMv:ihotms-&,e For sme frequency band, such thatlW4#6 +
ppoopilatim
Inversica Is achieved and osollUtim may boaam possible. An enjUDI.Ca
for
C.,d 1/2
AC=ICU NR.- A1403U93
the miuimu4 Intensity of Incident radiation Jidu necessary to reaeb
the
th--mshold for + PP a spoading to the oscilUtiou threshold is
derived.
It is shown thdt vhdn oscillation OCCIMM 14e + remains constant for
a vide
ran,,,,,e cl J )o Jidne At a very M& i~6~sltv Wi-saution (a.*.Tmln)j
.-&4p con-
siderabla biDating ot electron-lho3A (;as takes places the system
becomes.& War
efficient converter of incoherent Into cd=4mt raaiatica, vith
efficiency
ASSOOZMCK: Piz:Ldmlrtv Anstltub In. P# So Ubedevu USIONU Aal* SM
(Pbysica lualtituto,, Acadevor of &dences,5M)
SUN-=TtD: 7FO*: DAM AOQ' O7Mw% MEL: 00
NO MW SOV.; 005
SUL CCDH: M t 002.
-4/Peb/f1_4/P14 AS.D(d)/SSD/
t V
)/RaW UP
ACCM11D.2 BRz APhID47929 afir, 8/0056/64 047/004Y1.58W1590
BORA
wmat teorottJ
beekoy flilki, v. 47,
.Mo.
TaPlIC TAGS-. laser. sealconductor lazer~cadmlun sulfide, reconbina-
t1am radiatlazt, coherent light
!A2MA-CT-. -The present paper is an expanded version of an earlier
G., 0. V. Bojtdankei_i9_k1A___G,.
iamer-by's rawt~'elimtron beda, AN-SSOR- Dbklady
li*. k, 1964W T83) whIch reported successful devel;pnent of
t1ke ftrat ele-etrors-beampamped semiconductor loser. The following
additloma data were provided in this paper: The 2 x 1.5 m=2 faces
af the 3-c=, loza aazple were made parallel and carefully polished.
The duratiaa~ af the electron beam pulse from an electron gun was 2.5
ij
W71A mai- Z&a w&* *vvKrrtc* is the earlier paper. The electron beam
vs.&- energles an the or6er of 200 kev In.s. cylindrical
Car* 119
I'A=3WS=1W 3R-. AP40479"
-ftan-Fe-ti- 11 , im-mv iILA MR ex"Visests i. ft's, recombination
radiation
~*Vectrwm ==Ixted or a sunber or wide bands Vith transition etergiee
a=w1ler than the width o:r the forbidden band. Three narrov lines at
imvelengths of 5035, 4966 and 4891 R vere observed at high current
d-v=aitiea. The Intensity variation cof the emission line at 4966 9
vith the eurrent density Is sbown in FAg. i or the Enclosure and a
simu,ltaneauz n&rrowing of the spectral line from 35 to 7 A is shovn
in
Fig. 2. Orig. art. has: 2 figures.
kSSOCTAIIION: Fisleheskly Institut im. P. N. iAkbedeva Akademil. nauk
MR
(FItysics InstIture, Aca" of Sellences SSSR)
SUMaTTED: OBFeb6]6 ENCL: 02 SUB CODE; EC, NP
90 REY SGV: 003
OTHERs- 002
Card 2/4
E
_J)/ O/Mb -k)v
WG( (m)/EEC( W/T/
ESC'(b) P(k /EPFA (m) -2~ EWA (h )/Pn-4/Po.-~/Pf -4/PI -4/P1 -4/Peb
IJP(,.)'/SSD/AFfIL/
AFETR//~B_--I;D EN~a')/ASD(a)*-5/ASD ESD(qs)/tSD(t) WG/WH
ACCESSIO, NP,* AP4047933 S/0056/641/0471004/1595/1597
AUTHOR: Ba bartsumyan. R. V. ; Zuyev, V. S. ; Kryukov,
P. G.; Stoylov, Yu. fu.
TITLEs Q-switched laser
~SOURCEs Zhurnal oksperimentaVuey i tearetichask" fixtki, v, 47
;no. 4, 1964, 1595-1597
;'TOPIC TAG t uby laser$
8 laser amplLfierl, Q switch, Q switching
Is er, r
:laser
-and produced a 7 00-usec pulse.
:erglzed- y an 8-kv, 366-uf-powersupply
~The Kerr cell was energized by a 0.5o-usec pulse, whose rise time was
5 nanoseconds, 500 iisec after ignition of the flash lamp. The laser
then emitted.a single pulse with an enerp;y of 1.8 joules. The addi-
tion of a second ruby laser as an amplifier produced an output pulse
of 8 Joules having a steeper fo=. Orig. art. has: 2 figures.
iCard 1/2
-BASOVP N.G.; GRASYUK, A.Z.; CRAYEVSKIY, A.N.
Some special features of transmiesion and ref-eptaon of
information
using masers and lasers. Radiotekh, I elektron, 9
no.9:1680-1686 B
164. WRA 17:10)
1. Fizichaskly institut im. P.N.Lebedeva AN SSSR.
L 23061-65 E74A(k)/EiN?(I)/&W(k)-2/T"FM~b)-2/W(k)/g-IA(m)-2.'
Pf4j/Pi4i/P1-L/
pov-L TJPW JM-- M
ACCFZS10B NR; AF5001858 8/0056/64/047/006/2314/2316-
U
AMHOR: Basov,--&-Q.; Vjld~tAn,_At. 1,; Str~ oyA G.M.; spenski3r. A.
V.
TITLE: The possibility of detervdning ~~j~azationriates by means 0i
a hy&ogen
atom beam maser
SM-RU: Zhurnal eksperimental'noy i teoreticheskoy fiziki, v. 47, no.
6, lg&-),
2314-2316
TOPIC TAGS: maser, hydrogen beam maser, relaxation rate
ABSTRACT: The authors present sme. characteristics obtained at FIAN
with's
hydrogen atom beam maser (A a 21 cm) and &bow how a study of these
characteristics
can be used to deduce the relaxation rates of various processes that
lead to the
lots of active atoms (escape of active particles from the vessel,
!.,all lossel,
r e 1 a x a t i o n due to majwnetic field inhomogeneities, and spin
re-
orientation upon colliston or two hyttrogen An oscii-Logram of the
time
dependence of the pover of stimulated emission of an underexcited
m3ser
under the Influence of * 11 Sht pulse yielded for the FIAN equipment
a
relaxation rate Y 3oec-l* Irformationonthe relaxiationyate-wees
MA)P.~-
0
L M61-65
ACCESSION NR: AP5001656
by DlottinA the output power of an operating maser astainst the i
ntensLy of th6 active-eh=
beam. This yields the constant characterizing the relaxation due to
collision
of two hyidrofea atoms with spin exchange. The value obtained was in
the range
(1-6) x 10-10 cm3/sec/particle, which Weed with published data. A
value of
sec-1, obtained for 'Y() by plotting the resonance curve of the
cavity and
using a formula for the frequency pulling of the maser by the gener-
atoris ingood agreement with the value obtained from the
stimulated-emi!95ion
oscillogram. Orig. art. has: 3 figures and 1 for=aa. 102]
ASSOCU-TI'Mis. - Fj d cheskiy- 4 Akadeal- no" SM -(PiLsics
Institute, A6atdeny of Sciepices,SSSR).
SUMITM: 1WUI& ENCL t 00 - - SUB CODEt EC, EM
NO REF SOVt 000 OTHERs 003 ATD PRESSt 3173
'2/2
ard
C
ACCESSION NR, A?4030780 8/0020/64/155/004/0783/0783;
AUTHORS JLaLQYj M., asponding Member# AN BSSR); BogdanUsvic
j6_jCoTT hvl
Oo Vol Devyatkov-.Ar-G.
TITLE$ Zxcitsition of a semiconductor laser by a fast electron UG&M
SOURCEt AN SSS.X# Doklady*t v. 155, no. 4, 1964, 783
TOPIC TAGS: laserl semiconductor laserg junction laser, electron
beam laser, cadmium sulfide laser
ABSTRACTs This article reports the first successful results of
experiments in which stimulated emission of radiation was achieved
from CdS monocrystals in pulsed operation,by means of an electron
beam* Intense radiation In the green part of the spectrum (A-49661).
was observed during irradiation of CdS monocrystal, placed in a
*helium cryostat. by a beam of %200 Kev electrons. The Luton icy of
fluorescence increased sharply with current density. A thra:-fold
Increase of the current density above the threshold resulted in
a two-order increase in the intensity of radiation and a
simultaneous'-
Card 1/2
ACCZSSION - Ni.- AP4030780'
nvrrowing of the emission line-from 35 to 7 1. The threshold current
was observed to depend strongly on the quality of the crystals used*.
The duration of the current pulses was 2 Usec and the rep6tition
frequency was several t&ns of eppi At sm411 current densities, the
duration of emission after the and of the pulse was 2 useco At the
maximum current densities, the light pulse was synchronous with the
pulse.
ASSOCIATIONS none
SUBMITTEDs 12Feb64 DATE-ACQ: 30Apr64 ENCLs 00
SUB CODES. PR No REP SM 002 -OTHERS 900
cowd 212
_7777=_A~--L
L 8723-65 V.Wn(J)/EWA(k)/VBD/EWf
EWA (h) -4/Po-h/Pf 4, !PAb/Pi -4/P1-4
IJP(C)/,RSD/BSE~/RAEN(t)/AFETk!ASD(d)/RAEM(a)/
ESD(gs)/PSD(a)-5/ESD(t)/AFW1;-
ACCESSION NR: AP4043832 S/0020/64/157/005/1084/1087
AUTHOR: Basov N, G. (Corresponding member AN SSSR); Cxasyuk. A. Z,,;'
Zub a re v,
TITLE$ Regenerati-se Jaser J
SOURCE: AN SSSR. Doklady*,- v. 1370* no. 5, 1964, 1084-1687
TOPIC TAGS: laser,, ruby laser,, regenerative laser, laser amplifier,
unidtrectionot laser., traveling wave lasero laser gain
ABSTRAM An optical amplifying By3t6M is presented, consisting of
a Q-switching ruby laser driving a unidirectional amplifier laser
The Q-switch of the signal source was provided to determine properly
the shape. length, power, and time reference of the driving pulse,
The unidirectional feature of the driven laser, achieved by a third
mirror taking the return path outside the ruby rod, renders the
threshold adjustment of the system loss critical and makes it
easier
to 'reach stable gain. Furthermore, the unidirectional system allows
cord I / 2
L 8723-65
ACCESSION NR3 AP4043832
for the employment of several amplifying lasers in series without
Interstage isolators. In the experiment, the overall power gain was
measured as a function of alngle-pass gain. An overall gain in the
vicinity of 10 was recorded against a single-pass gain of 6 and the
ref lection coef f itient of the semitransparent mirror v= etpal to
0.1
In order to aeasure the sensitivity of the amplifier, Lhe photomul-
tiplier va3 placed as far from it as possible to reduce luminescence
effects and a fl&sh lamp quenching device was used to eliminate the
pump background. The measurements showed that the 3yaten is &ensl-
tive to signal power of the same order of vagnituds a-a the
thooratical
va'ue, Sivem a signal-ta-solat ratio close to unity. The pass baud-
Vidtb was 5 eu-1 for overall power gain of 25. "The authors extend
their thanks to V. S. zuyev. P. G. xr-yukov' and V. 1, sverg-jl:'~ for
tn !:b-1- hz'o! t figurag ztuO tx ttqr-~,Pti-.n_
ASSOCIATIONt none
SUBMITTED: z8peb64 ATC PRFSS-. 3113 ENCL. 00
SUB CODEt EC NO REF 50vt 004 OTHER: 002
Card 2/2
azov N r as yuk 7 u Iei r e YEAtujill, "ir.
-ij 'noy j '~-Dret chesk.~.,y 1 r.1 &- v ];~z
_i r n
Prllozhenlve, v. 1, no. 4, 19')5, 29-33)
TIOPI C TAGS : gall ium am;enide, optical piurping, ne-)dymimn
glass laser, norl-I i rlear
effel-t, t-,,rrD photon absorption, Rwr=n scatteriug~ secuud
ha-imanic generatif-in.
P,iIS'J RACf A neodymium-ch,-)r3ad ~Iass
T
jf !-,-t r
2~y
The in a x r:2-
n vj- r-
T~,
was ~,.I,tached to a ma-s-1ve heat. s ink v a- e,! r) i n; lar,
E'-S at ~-rvsta-)- '~~dg~es t -'y! ...
)y
other two edges, orthogona-I to edge 4, were polished accurately to
form E~. I Lm C.
.resohator , Light 5 from one side of the resonator, was directed
at the I I-'I ? - -1 i
card 1/4
ACCESSION NR: AP501 L21-16
Ispectrograph 7. where it waz photographed; the light from the
other side was
directed at a screen 3, where it was aloo photograpt-;f-d.
r_,,fe:_t -if tht- A~!is"y
~Lrl n t e ri
V A K atu-l _i ri lad'y MI, SSSB' ,i.
W)
large volume of the semiconductor taken- part in the generation.
The eff-icien-y of
the generation, expres=ed as P. ratio of yir-ld t- T,~ Lrp W El-s
~]Ll
Fest-arrh is -urren+ly ~---in; 1 ~i i'm :~IV-I' -Li "x Ln
g Px[,
- -1 N
ut
F-, irce '-;~~renna, -96'i~) knave nz"~ yet vie-Ir.:: pjt~0-~-Vt-
F"r-, ,as 2' f g u re s . L, f K
ASSOCIATION: Fizicheskiy institut im. P. N, L-ebedeva Akademii
nn,,,,.k SSSR (Physics
Instit~ite, Aca-rle-?V r~f -Iciences,SSSR)
aamjwu: 16Apr65 ENCL: 02 SUB CODE: EC
:NO REP SOV: 001 MAER: 001 ATD PRESS; 4015
10ard
L 5358i-65
ENCLOSUM, 01
314
Fig. 1.4
Schematic of the irist-&II.ation
'L _535A445
I ACCIMSION NR., ki~-5-ol4n6
ENCLOSURE: 02
Fig. 2. Spectral line of GaAs for
various values of pumping pcywer.
-se-ale-along the' or nate axis
dI
differs for various curves: the
maximum at curve 3 is much greater
that at curve 1.
AW Aw im $W
Card--- 4/4
791t t A 1fX-W/zAUArJfz"4A &;/&Wr~e it
DIMM / - -WP
FitCESSION N : AP5018842
R WGM uR/o368/65/003. 0011bg 70031
535-89
"Z
AUTHOR: Basov, N. G.., Grasyuk, A. Z.; ZRbarev, 1. G. 2
*Mae'
TIM: The response of 06 (;ti:1ii;kum. lass aser amp er-
SOURCE:. Zhurnal prikjradncy spektroskopii, v. 3, no. 1, 1965, 26--u
TOPIC TAGS: laser amplifier, neodymium glass amplifier, traveling
wave amplifiers'
neodymium glass laser, amplifier response
ABSTRACT:_ Data-are--p"sen'teG-on-.the--eiperimental~-investigation
-of -a neodymium.;.glasd
laser amplifier. The block disgraMLof a setup.used for the
measurement of the am-
plifier response is shown in Fig. 1 of the Enclosure. A
neodymium-glass laser with~
Q-switching was used as an exciter. The laser output was transmitted
through the :
Itheodolite T, where it was focused and subpequently converged on an
object with var..'
liable transparency. After passage, through #r_-theodolite the
angular divergence of the
ibeam was smaller than the angular diffraction at the input and
output apertures of
Ithe amplifier. The beam from the theodolite was attenuated by
neutral filters which
were precalibrated to the laser wavelength (1.06 mv). After passage
through an
object, one-half of the beam was separated by a 50%.mirror and
photographed. The
!
other half was *passed through a neodymium-glass amplifier and was
also photographed~~
CWd
7-1 __1
-58925-65
AcassioN NR. Ap5ol8842
The roci isC
ographs--sh(nr--tbat-,.-unlike-the-ruby7'a3~pllner-,,-the-necfd~mi
W- r-1-
-7 amplifier i-s- capable of - 11f.- VOUP-lification of the image of
alaser-illuminated object.
IThe amplifier response was computed theoretically and measured
experimentally by
imeans of a two-beam oscillograph, as a function of the area of the
amplifier output
,aperture and the magnitude of the solid angle of the recorder. The
experimental
Ivalue of the response of a neodymium-glass amplifier was 1.7 x 10-6
v. This value is
Iclose to the theoretical LWt of 1.2 x 10-6 v for a transmission
band of 6 x 1012 cps.
'Orig. sit. has: 4 figures and 12 formulas. [YKI
!ASSOCIATION: nono
ISUBMITTED- oftpr65
.NO REF SOV: 001
ENCL: 01 SUB CODE: EC
OTHER: 003 ATD PRESS: Ao5l
M-2 P F
T PIT
n
'DO
Y1
LCOrd-3h.,_
Fig. 1. Blook-diagram of the setup for the measurempnt
of a=plifier response
AKT - Autocollizator; OKG - laser witb modulated Q;
T - theodolite; P - precalibrated, filterB; D, Do - dia-
phragms; P - plane-parallel glass layer; OKU - laser
amplifier; L, and L - confocal lens (F 6 cm);
FEU-1 - control pbao;ulZiplier; FEU-2 recorderl
DO tvo-beem oncillograph.
_EWG J)/EWA(Jc)/"D/SW-(J)/_ESC(k_)_ t)/T
L-4! 2 6 - 1 2 SXC~ -/EEC
370(h) - Pn-4/Po_4/Pf-4/Peb/Pi-4/P1-4 IJP(c) wo
ACCESSION NRt AP5003477-
AUTHORi Basov, No Gel Belenov,
TITLE: Synchronization of osctllations
several p-n junctions
SOURCEt Fiaika tvardogo tel&,
8/0181/65/007/001/0337/0339.~
Es Mel Lstokhov, Ve S,
in a semiconductor laser vith~'_'_
v. 7, no. It 1965p 337-339
TOPIC TACSs laser, semiconductor laser,, p n junction, stimulated
emission, laser action, mode, resonator cavity& cavity resonator,
standing mode
ABSTRACT: A theoretical analysis is conducted of the mode of'operation
of an injection laser consisting of an array of p-n junctions In which
oscillations are synchronized in order to obtain larger power output
and better directionality of laser emission. An slectrodynamic model
of a p-n junction as a dielettrI4 waveguide with a low critical fre-
quency In which there are only the lowest order standing waves E.,
and Hoc is used in deriving & formula for the internal coupling of the
junction due to the penetration of the fields An eipresslon Is also
derived for the external diffraction coupling coefficient by a mothod
1/2
L 2 6
?2
ACCOi0i HRI AP5003477
developed by N. G. Basov at &I uhich is described in a paper yet to be
publ.ished. External diffraction coupling of p-n junctious is obtained
by making a hole In the face of the semiconductor and using an
external
mirror. The criteria for stability of the synchronized mode of oper-
tion are obtained by analyzing the oscillation equations of a system
similar to that of two interacting lasers. Numerical estimates for a
typical p-n junction show that synchronization of oscillations is more
favorable In the case of external coupling* Orig. art. hass 5 form-
ulas and 2 figures. ICS)
ASSOCIATIONs FixichaskLy institut iment. P. N, Lebedev (Physics
Institute)
SUBHITTCDa 02Nov64 ENCL: 00 SUB CODEs ECIGS
NO REY SOVs 002 OTHERt OOZ ATD PRESS$ 3172
CO-d 2 2
Pt R-4 P1
P(OVP b XWMA1(.'f-_2 4 ft-
tlAwp( (h)
IJPI,c WG/JD/JG
AL71HIDR: Ba ~L.N. G.; Yeliseyev, P. G.; Nikitin, V. V.; Lishina, A.
V.; Maslov,
V. N.; nashel'skiy, A. Ya.
ITITIS: A semiconductor G&As,_,P, junction laser Ik:)
SOMICE: Fiziks tverdogo tela V. 7, no. 6 1965, 1902-1904
TOPIC TAGS: laser, semiconductor laser, junction laser, injection
laser, stim-
ulated emission, gallium arsenide, gallium phosphide
'.1
ABSTRACT. A G&Aso.8 5P0:15 pulsed injection laser operating at 7TK
is described.
Thq monocrystalline solid solution of GaAs 0.85P0.15 was prepared by
epitaxial grovth
(5aadwicb method). The p-n junction was formed at a deptn _~f