SCIENTIFIC ABSTRACT NASLEDOV, D.N. - NASLEDOV, D.N.

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CIA-RDP86-00513R001136110018-9
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December 31, 1967
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SCIENTIFIC ABSTRACT
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densit-ki ',the tivit 3r 5 r: ~dc evql P(&7.- -,Ovam IJAW at im, Ong I,&* -~ni'6f 4.q XvIddZif 0 (AiAis, -Phya. POICILIca, Cu3A to ss witb'intrinsio Z, ~29 6' foams was atabulatid -flar, Oree.. sampp Jui - - , -,, - *. d 1 1010 or olts 4 ~ -A ~ . - ibr.:2.4:x 101 and- 1 w4 4i; &"A ii +1i .'i*l .1ian - elcig 3 re of holes j- -10 -_,t6-10 --~o t4ined by -zone melting.- ihe fipecimens,- used were.-.- 6 -x 1, 5 x- 0'. ---,T6 ne rium j..cu e a clatermi i~he --lifetime of ~nonequilib xrent carri r 6to~tion~a'r~y-,,t~nd,noiistat'ion'a-ry h t c- t'xi duc t 1 -4 ty In -me"Ur p 0 jand.-nois es, -were _ meas ured. inj~ statioiia 'specinled vas illuminated, vith a modulated A.- _eted_~ a-1-14YJ7 brum- f rom 1. 5 to 2.5 p In mea _~neql VI 97- &~Tm _Wf't' -r as:- fvw #e7- or:- Ses d ft7 SoUrte oxgUlki --light p was, use. I~e. , on::o (x - i~ -10-9, it'a-) ~d de~ e :of 1 66ndikivit . -'Hall coefficient on temw I epen e ectro yalid. --e ~ -of nUtionary phot vity-,on temperatureo and .apeIv r 4,41i$ it~:: O-V, dotment noiOu'. in- -9 -tre from 2:x U al queAcy- 4ah 162.to 2 x 105 C;c J ~ekIMIF"Wo-M MOIL w6HI m %M W- -IT kid"-A 7 Man ......... IF 16 qb ~7~. -1.4~ A7 93*~,~."i, 7n VORONKOVA, N.M.; NASUDOV, F.N. Fffect of trarping levels in Gabs rhotoconductivity. Fiz. tver. tela 7 no.8:2542-2543 Ag 065. (MIPA -18:9) 1. FIzIko-tekhnIcheskiy institut iment "offe A3 SSSR, Leningrad. IMENKOV, A.N.; KOGO, L.M.; KOZLOV, M.M.; MESKIN., S.S.; NASLFDOV, D.N.; TS ARENKOV, B. V. Effect of impurities on the recombination radiation spectra of gallium arsenide. Fiz. tver. tela 7 no.100115-3118 0 165. (MIRA lgill) 1. Fiziko-tekhnicheskiy institut imeni loffe AN SSSR, Leningrad. - ll--~'- - - , , j~ , - ~Z.C- ~i r.,. -7 , ~.r, .4'. :..", . - I-A Tr~ klo em at "80 *h&-"20K '*tb- ti-n-vaerat ure Wand .51- ammol W. I-A AWL im~ of Yon Agat, ZIA I-F TITIE;- Me. scatterimg nie.chanisni of current -carriers of tellurium doped gallium - t WIMM-a-M Bantam" - 9 CESSION NRj, ~7 Figare: 3, Temperature-madependence of electrah . . A i- mobility f6r-.samples 2n.and 10n. V. er n e scatt I oalculated mobility for th a Va a -lattice-r.oscillittiong on pol r calculated mobility for the scatterb on acou tic-lattice oscillations S jut M - AV -Q~ 777 77: Card-:1/2 - -7 . '. ~. - 1. n_ -, 4-90URU - 9 t 6-~ U.I--- -, - _w r, )AINIKIMMAW ALP j :98 1 MW -AW-17" , jam voltap "J'A ',wnuw of rO. At am v almoww" WW_ FIVEN nZ NASLEDOV, D.N., prof. Symposillm on semiconductors held in Warsaw. Vest. AN SSSP 35 no.2: 87 F 165. IP:3, m~torlali to over fossetich of '444W. riv valad OD 0~' 300 wA)' And -tbwAw"ntjj*~go*ffjcjen~t of t1w :41 'A' 11001,111irt'". 4W it, ~~777 7 gm 08 at vw for only am of iod a ta"ra. the of ams W. 1- 0"r,w wide tm"rw astaule SM lost4mom L 2967 ZWT(d)/c1,P(k)/8WPQ) JKT 'v ACCESSION M: AP3WfiYN UR/0l05/64/WO/OO9/0M/OO9b AMMt QnVtWvv~V. K.- Y- a.; . Sat s",Pp-S.; Tii~rlin. 4. D.; Alokseyev. A. Yo.g 7561~indits 14,- YP -,- Berger. A. Ta.; Tavorskly. V. W.1 ~sslodoyl D. NO: 1~ S- 71 TITLE: Mikolay Wikolayevich-loAtsertkaj (Obituary) SOURCE: glektrichostvo. no. 9. 1964, 93-0 TOPIC TAGSs electric onginse.-ing persomwl ABSTRACT: Doctor of 24achnical Balance*, Uajor General In the Technical Engineering Service. Professor 1. 9. lutsanko died In MW of this year after a ImM and serious 111afts. He gradmated from the Wassm, HI&or Technical AaadwW to 1924 and vu closely associated with his spoeialty .of electrical engineering Ull Ww end of his Zito. No speat %b9 first years of his prootleal aot1v11W at the AoadsW workift In to alostriGal engin9oriag laboratory of It. A. Ibmag. After that be be" his career In the Soviet ArW am a 1swU laboratory assistant In she nkdl*WWnlml laborato3w ~* werin& hu war vp sm turv 7"" is be hema of the card I/ a L 2967-Z6 ACCFSSION NR t AP5026357 Dopertniont of i9leatrioal and 11111tary hngIji*arIag. No wrote several boolm, -Alternating Carrents.n "The Theory of Alternating Correct&." "Course In 'Gamoral Sloctrioal UnClasering." *Radio Enower1W mt. topther vdtb his -a*-worlasro. problen Isocks on *A Course In Alternating Carressts" arA "The Yooloal Friw1plee of Jasoltrical Englaserl".0 No set up a musiber of speaW courses (military s"21cation of *!*atria power. mill" portablo ol"tric pmr stationot electric equipment for armies. electrification of military sagineerl" wafts. eta.) and also participat" In now engineer- ive projects with the Soviet Am. No has written MW textbooks. mosso- graphs and articles on Sbe theoretical end aWled diviolesiss of military electrical sisonsorive. Theso Include "22ootrio Circuits" am& wyandspeo;Ws for Use Doellp mad namalag of Hobtle Mootrie statlaw.0 low of 2. N. IMSSOWW'S students an Orklag Is MUOM of thlb SOW161 AnW, 18 11411MUtte ismusatee ssisd is Genoese. MA Is 1114114"s Ike" OWASSU we 64SUM114 /* OW WON of falelt $"Off, as fam"r of owm oweary 01"tridel "00"r- INS. no "Solve& big lp In It" Ma Isla deetwase in 19490 so ba P"61"A so 0* Ift ftaw d so out SW* MO EM 11"W0, OrM6 mt@ bass I flgwee go ID W Cod 2/1 16065-0 - 77 Udw 44 so to or cw somw lAto the obm~ in the AAw All mpm lau L 33250-" WLSIA-Wo/m Tj C) a V-J-G ACC N& A0026231 SOURCE CODZ: UR/0058765/000/01VED6579175 I 1*dov D- -741 AUTHOR: PA"Isho Z. z TITINs Scatterlag of electrons by impurity atoms in Sallium arsenide SOUR=: Rot. ah. Pftika, Abe. 11Z509 MW SOURM Sb* Fiziks. Dokl- k XXnI Nauchn. konferentaii Tan' inzh. -stroit. in-ta. L., X96% 21-26 TAGSs Ke'llu- arsenide, electron scattering, imWity scattering, temperature vibration , N&U constant, actIvation energy, electron mobIlIty, crystal lattice ABSTWT: The authors investigated the temperature dependences (85 - 750K) of the Hall coefficient mid of the electric conductivity of GaAs crystals with electron den-; X 1018 cjj-3 at sity 1.1 x 2013 - 2.8 300K. The results offer evidence of the pre- sence of donors with activation energy 0.14 1 0.03 ev, whose concentration in the in-I vestigated crystals does not exceed 3 x IDIS cm-3. Me obtained values of the mobili.W.; ty agree with the calculated ones when account is taken of the scattering of electronj by the following: a) lattice vibrations, b) impurity ions, c) neutral atoms of im- purity with donor level 0.14 ev. The large contribution of scattering by neutral atam at T < 4WK is noted. Ye. Movehan. [Translation of abstract) SUB CODE: 20 Card 1/ 1 ---x A zom, 47 74-1 -".Wdr, 0 0., W -ou =I ~jl)AWTW 047wpt 1 la Intel L -NOW WSM399, saimm, owl uRrd .7 Z L:3928-667-- 3C AP f E D " . ; 1. EG fl KS KTTL , ii . v . ; ~cA m i rrS A 14 , 7 . ' . ; ';-~ . .. -- -- - tl'. ~ .. r 11 . a -,r;CoLriu C, t I V, ty 08 r ! 12 a t -., '* n Ggap. ?---. z . ,.-.- M 3671-3673 D 165 ..1 1 I . P, z i-k o-t ekhn I c he sk iy ins t i t ii t i Hi er. i 1 ri f f t-;;# - ~, ?:, d i :ris t. i tu t p r i k ', i An oy f i z i k I AN Mo I dliv 6 K c y f -.'7, , -. i ... 1, I.., -. BP,TKEI.IYF,V, A.D.; GAIAVANOV, V.V.; hIASLED( :'-11?1-.D.N~.. Rffect of a deep acceptor level cri the eleatric Properties of p-Tri5b. FIz. tver. tela 7 no. 120685-36e9 D 165 (Ml."A 190.) 1. Flziko-tekimicheskiy Institut imeni Taffe AN OSSIR, IAnlngrad. .-91A35-66- -R~.rrft) /EVJIP t) -.IJPI(C) JQ/J,--/AT- "02048--~-:.- -So /,00301#510 u KC 12/002/KO93/a9S act .1140 JA 110t,*_'J'_,~: kv"4L*"* i 1 411 *16918 104 ~40fffofj_ -Aca4euT of Selemess- SOVICte Ip -","Al totes soiLIA1 '120. *OIL* 20 196s .0 1.9 3 T,'O 5 tit A 44"it"40-, it, a I i t 6 0 04 f f ".1" VkOrmoolectric powelf, :~:Oz OT__r, to - 0own TA 4 he affective sees M* of t t L# NX&C A tee 41i ctl7-tl- av the is ~ made , -a' eswurenests of the Hall ;C--Jit 06- of. seuleoudv~cters tberjoele~Ciirie po**; agatlili 'effect. zu all t q4tal MK,,Plmw,~,~!W~_ Pz, _,(0I_,*L. -4K 19--4 3) were -Ai-___4i~_-jfI4i4 led ondest (42). _7 4` Op ~ajd of 'the f Mejk&~ 21435-66 -AC C? NL- AP6002046 -.-a f 6- c t I ve An 87.2 mo~:O- t" be ton of. tb yet. a - deviation. 8-10 tivo n&$is- of Samples alp at the bottom of 4640- Ok-tilili-SCOY 'other motbode Re,#. 1249 samples Lupur t7. - an The- ~authev -.iat44674titailued "at varleue~.- I table, elm on, Mrs - "I- 44ty tbal V"i4 -~IJPCQ) AT- AM06831 SOURC E cour.: MtQIRI/66100,8/002/0475/0477 il TIP. lao N~w IUW"' W''-- 14 'Irv 7,1 _F -tram 7 7 ant it ~,o :Aro. "site, &**lost* spri 'TO- I" ebta two time metal", 406164i.. too P&I pig _"m -Mrs Gee IT, cr 'M 4-1 n~t ~gn in f, 'A _i!ij ~7 '41'ZI, MS" _72 ,I " ~i: '~r ~-f ~ . -'. - ,-, - . . _j "kt- NA" k' 1, if q~ A, m li~ i 4 J_ ;rfr~~M' ~_e 4-W 7qJ i Jig '1' r A! AC; --------- - In ism GGI/JE) /1-rD __2 ~13C~~.7 ACC NA& A160IM70 Aid CON: UIV0182/66/6WO04/MV .-MMORt. Nealedurs Do No: RUM Do 0. rAmicatia __~Itute In. A. F, loffe, AN 8682, Leni3W (Fisiko- UffinIchoWdy lartItut AN 2IM: jjCM" of &tjMgtM -g np the electric proportion of p-JOILat Im tem- fts1ka kv tela, V. 8, no. 4, xQ66, liw-iu4 TAGS: crystal -lattice structure, prystal defect,, Indium campoundp antimonidej, band structure,, temweraftre dependence,, electric propertyp Hall effectp con&wtiv:Lty ABSTRACT: 2b check an the IWpothesis that Ir5b contains msiltipIy charged defects 'Ibleb we responsible for the recombizabSca of non-equillbrius carriers in It,, and to "certain the lonmace of Mich dafacts an the tampasto ~ dependence of the Hall coefficient in on h%Uy comWamted Bowles, the SUM=@ seamed In the texpa's- ture mega 4-]MK the ~ togmmmture dependence of the Hall constant and of the dark and th ho dew illuminated electric -conductivItisaj, using p-L30b samp),es vi Is ity .1-2 x 1021 cmr3 (at 7710 * In preparation of the samples and the cryostat in vhich the measure- Q6 -vents v= me& Awe In an earlier pqW (PM Y. 3,9 3031p X 3). The low natic neMused4i-the wasmveedta vas close to 3000 Oe. 2a Impurity levolx vow& 3.vift at 0.220 0.033,, and 0.008 ev Above the valene* berd. Analysis obsevvi4. card L 29958-66 i ACC NRs A P601 ~~81 SOURCr., CODE: Uli/ol8l/66/008/004/1176/1181 AUTHORS; Kesamanly- F. P.; Malltsev, Yu. V.; Nasledov, D. N.; lUkhanov, Yu. I.; Filipchenko, A. S. 'ORG: Physicotechnical Institute im. A. F.-Ioffe AN SSSR, Leningrad I(Fiziko-tekhnicheakiy institut AN SSSR) TITLE: Magnetooptical Investigations of the conduction band of InSb SOURCE: Fizlka tverdogo tela, v. 8, no. 4, 1966, 1176-101 !TOPIC TAGS: indium compound, antimonide, magnetooptic effect, conduc- Ition band, Faraday effect, light reflection, dielectric constant ABSTRACT: The authors investigated the optical reflection, transparency and locat'on of the plane of polarization (Faraday effect) In the wave- length ir,erval from 2 to 25 4 at temperatures from 130 to 550K and ~ 19 -3 electron densities from intrinsle to 1.2 x 10 cm , with an aim at ;checking the validit of the theory proposed by E. 0. Kane (Phys. Chem. ;Sol. v. 1, 249, 1957~. The apparatus used for the measurements was :described by the authors earlier (Izv. AN SSSR ser. fiz. v. 28, 989, i1964 and ~--arlier papers). InSb single crystals doped with Se were drawn from the melt by the Czochralski method. The reflection coefficient Card .1/2 L 29958-66 ACC NFI, AP6012481 exhibited a slow decrease with increasing wavelength, a sharp rainimum in! .ithe range between 10 and 17 4 (depending on the electron density), and ' ia steep increase. The value obtained for the lattice dielectric constantl jis 16.0 + 0.1, which is in good agreement with published data. The ef- I Ifective Zass of the electrons was found to be 0.071, 0-053, aad 0.033 i !times the free electron mass (m.) at electron concentrations 12, 6, and i 18 -3 12.6 x 10 cm when calculated from the plasma reflection and 0.018, 0.021, 0.027, 0.038, and 0.054 m for electron densities 2.5, 4# 7*5j, i 10 -3 0 1 26o, and 6oo x lo cm by using the Faraday effect. The experimental dependence of the energy on the wave number agreed with Kanels calcula- 19 -3 Itions up to electron densities 1.2 x 10 cm Some deviations from :L8 -3 Kanels theory are observed at densities greater than 5 x 10 cm and. ,call for a special analysis. Orig. art. has: 5 figures and 6 formulas I :SUB CODE: 20/ SUBM DATE: 13Sep65/ ORIG REF: 003/ OTH REF: Oll EEG(k)-,2/KWP(k)/EWr(1 (Fdr(m) -Wp(t)/Erj lip(c) wlin ,FM)/T/h .AP6024502 SOURCE ODDE: UR/0181/66/008/007/2251/2253 AUTHOR: Gol'dberg, Yu. A.; Nasledov, D. N.; Tsareakov, B. V. ORG: PUsicotechnical Institute in. A. F. lof fe, M SSSR, Leningrad (Fiziko- takhnichookly Institut M SSSR) .21 -1 TITIZ: Dependence of electroluminescent parameters of 11" lasers on the angle between the p-n junction plane and the resonator mirrors 7,1 SOURCE: Mike twerdogo tale. v. 8, no. 7, 1966, 2251-2253 TOPIC TAGS: semIcCWductor laser, gallium arsenide laser, diode laser, laser output., JUL". sq__Gpa~& TRAM Um threshold current density and the output of diode laaer~ were inves- tigated experimentally as a function of the angle (4 - 90* 29) he-tween the p-n junction plane (100) and the resonator mirrors placed in the (110) plans. It was shown that: 1) the threshold current density decreased with an Increase In the distance between mirrors I (Fig. 1), and with a decrease in the angle when I z coast (Fig. 2); and 2) quantum yield Increased with a decrease In 0 (Fit. 2). The maxi- sun angle Gmaz - d (where d - width of active madlum) for which the rermflected T L 37687-& 0 Fig. 1. Dependence of threshold current density on the distance bebmen mirrors '00.0~_ _. V 0 W W W mIn Fig. 2. Dependence of threshold current density (curve 1) (for I - 0.7 am) and quantum yield (curve 2) on the angle between the p-n junction plane and reso- nator mirrors L 37687-66 F-Acc -NR. Ai beam wl 11 travel the entire length of the active medium was estimated roughly at W-18', for d = 2-3 pand I Z' 0.5-0.7 mm. Orig. art. has: 2 figure; and 2 formulas. JYKJ SUB CON: 20/ SUBM DATE: 26jan66/ 07H RZF: 002/ ATD PRESS:,570 1// 61, "-i J01, Cw4 3/3 L .11' - 56 F-,'/T(I)/P T(m),/T,,"'-'JP(t)/ETI IJ:',c) AT,/JD/J- ACC NNe AP6026705 SOURCE CODS: UR/0181/66/008/008/2462/2465 AUTHOR: Danilova, T. N.; Kogan, L. M.; Meakin, S. S.; Masledov, D. X.; Teareakov, N.V. ORG: 1~hyC4S!!-nS - F. loffe, AN SSSR, Leningrad (Finiko- _M~WiKUW Institute In. A tekhnicbeskly Institut AN SW R-) TITLE: Comparative investigation of the recombination radiation 0 junc- tions with and without a Fabry-Ferot resonator SOURCE: Mika tvordogo, tels, v. 8, no. 8, 1966, 2462-2465 TOPIC TAGS: TabrymOminhLresonator, recombination radiation, pn d6eds, gaflium arsenide ) ABSTRACT: The published literature contains information on the investigation of spon-1 taneous, stimulated, and coherent radiation of GaAs p-n junctions pertaining to t e characteristic radiation parameters as a function of the current for diodes with or ,without resonators. The purpose of the present article is to compare the dependences of the maximum energy hvM and the half-width 6 of the fundamental radiation band on the current density through a single p-n junction with and without a Fabry-Perot reso- nator. The authors studied diodes In which the p-n junctions were V~talned Iby dif- fusion of zinc in To-alloyed n-CaAs with electron concentration 7-IOl-3-10 hcm-3; the area of the p-n junction =10-3cm. The current through the diode and the spectral, distribution of radiation Intensity were measured. It was found that bv,, starting L ACC NR- AP6026705 from the lowest current densities a/cm2), increases with increasing current and then becn is practically independent of the current. The dependence of 6 on current density is given for small current densities (5--70 a/cm2). It is concluded from the results presented that the primary narrowing of the spectrum occurs as a result of population inversion at the rarefied states which are responsible for the secondary narrowing of the spectrum, i.e., beyond the conventional stimulated and coherent ra- diation with maximmis energy -1.47 ev. The "tails" in the forbidden zone are probably the rarefied states responsible for the primary narrowing of the spectrum. The authors thank 0. V. Konstantinov. V. 1. Pavel', and A. L. gfroa for discussing the results of thLi7;or'i.__4Wig. -art. i~:2__figures. 1261 SUB COBB: 20/ SUM DATE: 26Jan66/ ORIG REF: 001/ OTH RIF: 001/ ATD PRESS- 6-06~ e L 44602-66 EViT(1)/EVIT(m)/EEG(k)-2/T/EViP(k)/EtVP(t)/EtI Ijp(c) --iCIjDljr ACC Nit, AP6030977 SOURCE CODE: UR/0181166/0081009/2789/2791 AUTHOR: Kogan, L. M.; Libov, L. D.; Nasledov, D. N.; Nikitina, T. Strakhovs Tzarenkov, B. V. GRG: PUsicatechnical Institute im. A. F. Ioffe&AN SSSR, Leningrad (Fiziko- cekhnfc-heskiy institut AN SSSR); Physics Institute im. P. N. Lebedev AN SSSR, Moscow (Fizicheakiy institut AN SSSR) IV TITLE: Certain properties of GaAs laser diodes with an epitaxial p-n junction at room temperature SOURCE: Fizika tverdogo tela, v. 8, no. 9, 1966, 2789-2791 TOPIC TAGS: solid state laser, semiconductor laser, gallium arsenidellaser, epitaxial diode, infrared laser$ A- a Ae 0 "Jim.) ~W -.rvAlerlo / I ABSTRACT: In an experimental investigation of epitaxial p-n GaAs junctions,telluriuu-! doped n-type and zinc-do~ed p-type GaAs was used. The electron concentration in the n-type GaAs was 5.5 x 10 7-2.4 x 1018 cm-3; the hole concentration in the p-type GaAs was 1.5 x 1018-2.4 x 1019 cm-3. The specimens were oriented along the (100) plane and the epitaxial p-n junction was prepared from the liquid phase by a method descrRed elsewhere (H. Nelson, RCA Rev., 24, 603, 1963). The dislocation density near the p-n junction in the epitaxial layers did not exceed that in the wafer and was 104 cm"2. The Fabry-Perot cavity was formed by the cleaved (110) surfaces,and the electrical L 44602-66 ACC NR. AP6030977 contacts were made of indium. The residual resistance of a diode with an area of 10-3 CM2 was less than 0.1 ohm. Laser action at room temperature was achieved with 30-nanosec current pulses. An FEU-22 photomultiplier recorded the optical output. The threshold currents were determined from the dependence of intensity on current. The p-type GaAs specimens with hole concentrations of 2.4 x 1019 cm-3 and a mobility of 50 cmz/v-sec lased at 90001 at threshold currents of 1.5 x 105 amp/CE2. Investi- gachns sere also made cfspecimens in which the epitaxial layer, doped with zinc and partly compensated by lead, wa grown on a tellurium-doped GaAs substrate with an electron concentration of 9.5 : 1017 cm-3and a mobility of 2400 cm2/v.sec. 7hese lased at room temperature at 9010 X at currents of 3.8 x 105 amp/CM2 and at 8910 at currents of 4.7 x 105 Mp/cm2 and up. The power per pass of p-CAAs lasers was 30 watts with 700-amp currents and 18-nanosec pulses; that of n-GaAs lasers was 10 watts with 300-aup currents and 30-nanosec pulses. Orig. art. has: 1 figure. JYKJ SUB CODE: 20/ SUBM DATE: 2SMar66/ ORIG REF: 001/ OTH RE?: 003/ ATD PRESS: 5078 ri-106-06~29- SOURCE AUTBOR: Xogan, L. M.; M~skin, S. S.; Nasledov, D. N.; Trushina, V. Ye.; Tsarenkov,BA' CRG: P~nlco-Technical Institute im. A. F. Ioffe.AN SSSR (Fiziko-tekhnicheskly insfitut AN SSSR) (2() TITIZ: Electron-photoAaAsVI ? transistor SOURCE: Radiotekhnika I alektronika, v. 11, no. 9, 1966, 1645-1650 TOPIC TAGS: transiBtor, electron photon transistor, gallium arsenide transistor I ABSTRACT: The results of an experimental investigation of GaAs electron-photon transistors(R. Rediker et al., Proc. 1763, 51, 1, 218) at 77 and 293K are reported. The transistors were made from Tjjdoped n-GaAs. Source meterial parameters:. electron concentration, 7 x 1O17 - 5 x 10 per am3; mobility, 1800-3200 cr&2/v seell dislocation density, 10000 per cm2; p-n-p structure was produced by Zn diffusion; plate thickness, 300 u ; base thickness, 100-200 w ; p-region thickness, 50-100 u Collector current vs. collector voltage characteristics (for 0-100 amp/cm2 ezrdtter current) and collector current vs. emitter current characteristics are shown. The emitter-collector current transfer ratio was found to increase from 0-05 to 0.075 with the collector voltage increasing from 0 to 8 v, at 77K. At room temperature, th,.j transfer ratio amounts to 1/20-th of the liquid-nitrogen ratio. When the emitter Card 112 UDC: 539-293-011-43 ACC NR. AP6031029 current increases from 0.1 to 0.5 amP, the power gain decreases from 12 to 4 and the voltage gain, from 350 to 60 (at 77K). The estimated total quantum yield of photons Is 0.1 at 77K. Desirability is noted and ways are indicated for making the electron-photon transistor a practical amplifier. Orig. art. has: 4 figures and I formula. (031 SUB CODE: 09 / SUM DATE: 29Mar65 I ORID REF.- 003 / OTH REF: 006 / ATD PRESS: 5089 Card 2/ 2 afs ACC NR1 06030161 SOURCE CODE: UR/0120/66/000/00410214/0215 AMOR: Belawyat A. A.1 Nazledov, D. N.1 Sres a 00 me ORG: Lvico-Te6nical batitute AN SSSR, Lenirwad (nziko-t*Wudah&sk~r institut AN SSSR) TITLE: Thermostable Hall zeneratore SOURCE: Pribory i tekhnika eksperimenta, no. 4, 1966, 214-215 TOPIC TAGS: Hall generator, Hall effect ABSTRACT: Xateria.1a in the manufacture of Hall generators and characteristics of the latter are devaribed. Source material: GaLs having a concentration of (3.-8)10116 per cz0 and a mobility of 3000 cmg/v see. Sides ratio: 2 to 3; plate thickness, 0.12--W =; nonrectitying contacts. Characteristics: temperature coefficient, 0.01--G .030 per IC within 0-300C. Voltage sensitivity, 10-50 WY/06.= Kots of output voltage vs. magnetic-field strength and output voltage v9. temperature (0-300C) are shown. Orig. art. has: 2 figures. [031 SUB CONS 09 / SUM AtT31 13Jul65 / Ono REFt 000 / ATD PRESS: 5087 1 pb UDC: 621. 'J ACC W Ap6012468 AUTHOR: Koichanova. N. )h. 2 SOURCE CODE: uR/oi8iJ66/oo8/oo4/1097/uo4 // GG: ical Institute In. A. F. Ioffe. M MR. -08skly Institut AN 680R) 2XIM: TiMperetwo depoWence of the :iarrier lifetime In r-Ap&%, MI'M PUIM tvadw tout To 8P Doe 4P 1966, WqT-L104 5.7 20PZC TW6: gLWun aroosidep semiconductor carrierp carrier lifetimes photoconduc- I tivity., pbotangnotle offset, photo eaf, temperature dependence, forbidden band ABSTRACT: In view of the interest In the pbotoelectric propm lee of GeAs as a sidt- able light-source material, the authors investigated the temperature dependence of the photocondUctivity and the photomognetic effect# and the spectral distribution of the photo-ont aM Its texpersture variation, In the temperature interval 80-300K. The tesperstar dependence of the carrier lifetime was determined then from these e3werl so The amwed. GaAs single crystals were of the n-type and vere obtained by zone meltIng without special "Be The electric prqperties of the Mstals were determined In earlier wqm"'me-nts M V. 3, 198, 2961). The surface finishing of the crystals prior to the measurement of the photoelectric properties was by a method described PrwlouQY (F= v- 5, 3259, 1963) - The light was either monocbromat ic JTW ra) or in a spectrus., ranging from 6oo-&)o nn. With decreasing teMWature I startin at tempersture)t the lifetime or the majority carriers first increasedl "it th dependent of the temperature, followed by a second increase at the Cmd 1/2 -1 0222"2 EWT(I)IF.WT(M)/EWP(w)/T/EWP(t)/ETI 1JP(C) JD A%X; NMI JIM13DT2 SOURCE COIDE: uW66*996-6-676-16/k7002M AUTHOR: X"emnly,, y. p.; ]W.; age', ft. V. TITW: TranapIort ZaGe"a crystals SOURCE: Ref. sh, jPJzIkj4 Abs. j0Z%q il W SOURCE: Sb. FISAIL. DoU. k M(III NELuchn. k-onf-ereft-si-i- LeniW in-ta. L.,, l96% 5j--W-- TOPIC TAGS: electric C00ductivity, Hall coefficient, thermal enf, temperature do- Pendences transPort Propertra carrier scatterine, bw~A-Wec_14- I "vA~.' AB67WT: The &Utbor* Wasured the tw*er4ture dependence or the 61"tLectric conductlyl. ty (a)# the ULU cawtant, the differential thermal emf (cL),, and the transverse Nernst-Ettlagabowen Offftt (X) of ZnGeAs.. In the teveraturs interval 100-550K. The character of the tuqpnture dependence jf &11 th~'transport affect is for P-ZnSnJ42a* It VW found that a and m increase with the temperature,, X < 0 in the entire teNTOPStUre Iftervalp and that the W1.1 -.iobillty increases like up to 400K, after Which It decreases. At low tengwratures the scattering Is by the Impuri- tY ionsp mid with I=ws"Ing temperature, also by the lattice vIbrations. [Transia- tion Of abstract) SUB CODE: 2D AMOR: r A. S. Do *; fifidinews To a.; 036: jotft nwico-Tedwimi Instituto. Awdemy of m*Jm. Ladvorad TITLCs On the second conduction band In Isdium antimmide, 809=: nplea atstas solidt, w. III, no. 2, 11669 KI95-IM99 TWIC TAGS: hWm ampound, antimoulde, conduction bend, Hall effiect, Fermi lowel, OISCUM `tVISM&ItIGR ABSTRWT: OM we pinsented to sbow the exLeteme of a condwtion bwA In In8b loc4 ed about 0.5 ev, ihom the bottom of the main conduction bend (000). The vi" In the Hall coefficigpt witb tmpn*we was measured In 14 IMIm antimmide samples dop~4 wift nlmlvnftr teLlarium. The hypoftesis Oat We rise Le dm to alectran trmel- tions -toe second conduction we tested and the value of the gap deteralmd. WIS. art. bes, 31 Ub"t 4 formul". m 0=1 20/ SM DATC: O9NwGG/ - ORIC Mrs 004/ OrN KF: 005 cd vab 04791-61 EWT ( 1) IEWT (m~l ERE-',L~LETLi TP CC) dW A F AP6024462 SOURCE WLE: UR/0181/66/008/007/20(44/201#7 AWHOR: QOinq A. 'A.; ftanwovq E. M. ;MWWlova , M. ORG: ~hMiootedinical Institute im. A. F. loffe, AN (Fisiko- tekhraRrmway Innitut AN SSM MU: Photosewitivity spectm of p-n junctions in InAs in the photon energy range 0.9 - 5 ev I SOURCE: Fizika tverdogo tela, v. 8, no. 7, 1966, 2044-2047 TOPIC TAGS: pn junction, photosensitivity, internal photoeffect, indium, owpound optic material, arsenide, spectral distribution, absorption ooefficient, quantum yi~ldl ABSTAACT: 7his is a continuation of earlier work (Frr v. 8, 712, 1966), where it was obser%*ed that the spectral distribution of the quontum yield of the internal pbotoef-~-l fect in the short-range region is connected with singularities of the band str`ucturle of GaAs. The present work extends the investigation to InAs. The InAs p-n junctions were obtained by diffusion of Cd in n-type material with electron dei-isity (0.5 - 1) X 1017 cnr3 and were produced at a depth of several microns. The hole concentration in the illuminated surface of the swple was approximately 1010 cnr3. Several p-n junctions illuminated ficim the n-side were also tested. 7he long-wave part of the spectral character-istic of the jurwtion was plotted with the aid of a ZMR-2 mono- chrmator, and the measurements at higher energies were by the procedure described in the ewlier paper. 7he measurements showed a narrcw long-save photosensitivity peak, C,Wd 1/2 L, 04791-67 ACC NR' AP6024462 connected with the change of the absorption coefficient near the edge of the ground- state band, followed by a mgion of weak variation, a faster grmoth at %0.7 - 1 ev photon enerV, a rieversal followed by minimun near 3.2 ev, and a renewed gmwth at higher energies. Mm results am shown to be connected with the variation of the quantum yield of the internal photoeffect as a result of secondary icniwticn. 7he threshold mmW of the photon, starting with shich the quantum yield begins to gmwt is found to be 0.7 - 0.8 ev at 293K and 0.9 - 1 ev at 100K, in agremant with theo- retioal cala-lations by others. 7he various secticna of the spectruin axe interpreted m this basis, so it is indicated in the conclusion tat the actual quantm yield may not be as lmqp as what foLlam f:rom theoretical acmiduutions, since account must be taken of the priol~ty mtios; of the difftrint electsude UUNSWAM. MIX authom thm* M. P. Yeaina and N. N. Sainum for pxmpmz6q Un bft " juncticm. orig. at. SUB OME: 20/ SM D=s 03Dmc65/ ONG MF: 002/ OSH W: 006 2/2 afs L 04785-67 EWT(m)/EWP(t1/ETI I*c) ACC NR1 AP6024467 JD SOLMM OOIE: tMtOI81/66/008/007/2074/2076 AUDIDR: ZDtan, M. V. ; lebedayt A. A. ; Nasl*dDv . D. M. 41? ORG: Mmiffnn!!!~- Institute im6 A. F. L-offe, M SSSR. Lmnittomd Criziko- UI9CI%VM M -MSU-