SCIENTIFIC ABSTRACT BASOV, N. G. - BASOV, N. G.

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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