SCIENTIFIC ABSTRACT ZAKHAROV, M.P. - ZAKHAROV, V.P.

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CIA-RDP86-00513R002203720010-4
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December 31, 1967
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SCIENTIFIC ABSTRACT
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212 008 UNCLASSIF~IED PROCESSING DATE--11SEP70 C-IRC ACCESS ION- NO--AP0106845 .--A~STRAC.T/EXTRACT--(U) GP-0- ABSTRACT* LEATHER WAS CHROME TANNEOp 0a6PERCNET CR, SU~12 0 SUB3 13Y WT. OF HIDF BEING USED,~WITH SULFITE PULO EXT.,ADDEO TO THE TANNING BATH., THE LEATHER WAS TREATED WITH 28PERCENT BY WT, OF HIDFS OF SPS AND FB-2 SYNTANS IN A 4:1~RATrO. SIX HR ACTER THE BEGINNIiNG OF SYNTAN TREATMENT 7.4PEqCE.NIT K ALUM WAS Af.)L)ED TO T14E TANNING BATH. THE PROGRESS OF TANNING WAS ESTIKATED BY DETN. 13F THE RVELDING TEMP," c' N (A MEASURE Of: THE CHE14.1 AFr-It4jTY.,0F T,'(E TANNING A E T TO -COLLAGEN) AND THE EXTN OF CR SBU2 0 SQB3,FRQM THE LEAmER BY SYNTANS WAS DETD, - AN-INKREASE IN WELDING TEMP. FROM, SIMILARJO 55 TO.86Dr- G.REES.. OCCURRED MAINLY DURING CHRDMINGo DURING SYNTAN TREATMENTt ST.-"IIL4R TO 25DEGREES, OF THE CR SUB2 0 SU83'W4S EXTD. FROM THE LEATHER. A SIMILAR OF CR SUB2 0 SUB3 OCCURRED DURING TANNING UP CHq.OMED LEATHEq 'WITH TANNIDES; THE DEGREE-OF EXTN. INCREASED WITH~INCKEASING AMT. OF.CR SUB2 0 SUB3 IN THE LEATHER. 9URjt4G SYNTAN TREATMENT, THE FXTN. OF CR SU82 0 SUB3 WAS COMPENSATED FOR BY IfITRODUCTION.OF AL C014PDSO' INTD THE LEATHER. LINCLASSIF.IED OF M. 112 027 UNCL`SSIFIED PROCESSING DATc"--230CT70 -,TITLE--STUDY OF THE TERNARY DIAGRAM COPPERv IRONw iTITANIUM -U- ,.AUTHUR-(03)-KHANv M.G., ZAKHARQV#:A.M.f' ZAKHAROVP. 14.V. '~~:COUNTRY OF INFO--USSR -SOURCE--ISVETNAIA METALLURGIIA9 VOL. 13 NO 1 1970 P 10tt-109 :jATE PUBLISHED ------- 70 AREAS--MATERIALS --COPPER ALLOY, IRON ALLOY,, TITANIUM ALLQY, BIBLIOGRAPHY, 1 QPI C TAGS -.-THERMAL ANALYSISt INTERMETALLIC:,COt4POUND#.:ELECTRIlC RESISTANCE? SOLUBILITY, TERNARY ALLOY, CARBON:- _:'CONTROL MARKING--NO RESTRICTIONS DOCUMENT CLASS--UNCLASSIFTED PROXY REEL/FRAME--lq98/0444 STEP '40--UR/0149/70/013/001/0104/0109 ,.~.CIRC ACCIESSION 1160--AP0121118 2/2 027 UNCLASSIFIED PROCESSING DATE--230CT70 CIRC ACCESSION NO--AP0121118 ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. STUDY OF THE TERNARY SYSTEM CU.-FE-TJ CONTAINING TO 5PERCENT FE ANY TO, 5PERGENT T I USING ANALYSES MEASUREAENTS' OF 111CROHARONESS %IICROSCOPICe X RAY, AND THERMAL I ' 14AL SECT I ONS OF AN40 ELECTRICAL RESISTIVITY, AND MAGNETOMETRY. [SOTHER THIS.SYSTEM ARE CONSTRUCTED FOR 650,.850t 'AND 900DEGC; THE QUASI BINARY SYSTEM CU-TIFE2 IS ALSO STUDIEO. THE'SOLVUS LINE10F THE INTERMETALLIC COMPOUND IN COPPER IS DETERMINED. ITIIS FOUND THAT THE MAXIMUM ,.SOLUBILITY OF TIFE2 IN COPPER.AT!1095DEG C IS ABOUT 2PERCENT AND J-,.~--DECR,EASES TO 0-.4PERCENT AT 650BEGCO FACILITY: MOSKOVSKEI NST ITUT. STAL II SPLAVOV, MOSCOW,,., USSR* i F -.7, -7 1fl-1j, ~-r-l v- m m ................... .. 048 UINCLASSIFIE0 Plk'OCESSING 0ATE--Z7NUV70 T-I TL.E- -P R INIC I P L ES OF ALLOYINIG HeAT RESItTAM ELECTRIC.4,LLY, CONDUCT ING COPPER:A'10 ALUMIMItlill ALLOYS _u__ AUTHOR--ZAKHAROV f M.V. tGUNTRY OF INFO--USSR ,'d SOURCE-IZVEST. V.U.Z. TSVETN.AYA ME T, p070o Mr 1"l-119 D AT EPUBL I SHED ------- 70 UBJECT AREAS--MATERIALS Erj;~TC (:C~tl Djj(j-rr I, I N J I _.,p -1 .1likOUM PHASE TOP tK T, S-f: L CoppFR ALLOY, ALW DIAGRAM,, BOR074, DUCTILITY: SURFACE ACTtVE AGEmTv H. If i1"EMPERATU'RE ALLOY TROL MARKING--,'40 RESTRICTIONS 0 0 C UM E N TCLASS--U4CLASSIFIE0 .:PROXY REEL/FRAMF -30031149o srp,fl 7 6 io 0 0002 f 0 111 f 01 L 1 1) W ACCESSION N0-4'10130419, A UNCLASSI IED F E--27MOV70 212 PROCESS ING DAT ,,:~-CJRC ACCESSION NO-AT013040 ABSTRACTIEXTRAICT-M GP-0- 415STRACT. THE PMNICIPLES U-1 ~RLYINC, THE PREPAR, ATI-ON OF H! 13H TEMP , CU AND AL ALLOYS f:JR EUECTRICAL CO-NOUCTIORS -BARE DE SCRIBED A-140 DISCUSSED* A,LUIYS~LYING ON 09 ME QUASI MiNARY c HZE DIAGR~ S' rEND 'TO 6E THE -ECTIONS OF~ THE CORRESPONDING MULTI PLE- P , I L BEST IN THIS RESPECT. ALLOYENG ~ADDITIOMALLY W[T+f SU-~)-ACE ACT[VE SUCH AS B SUBSTANTIALLY~ iNCREASES THE tiult;TILITY AS WELL AS THE ~-ELECTRICAL CONDUCTIVITY WITHIN A LIMITED,~JEMP- RANIGE. T',IqD NEW GROUPS OF CGN0UCTI-%'G, MIGH TEMP~, ALLOYS HA'JE DEVELOPED ON THE ~E 5 S OF Tli~SE~ GENERAL PUNCIPL UDIC 548452 USSR Y, V. R. BP-R=EMVA, G. V., TSV9rKOVA, I. N', ROZI[ANSZ and XORYWIMN, ffl6I9Ng~MI'3'PYV!t- clademy of Sciences USSR V. T., Institute of "GMWW Mechanisms of AIN Whiskers" MOSCOW, Kristallografiya, Vol 16, No 5i.Sep-Oct 71, pp 978-981 Abstract: The article describes, results of a study of AIN whisker growth 'under isothermal conditions during the~reduction of al=inun, ~ oxide with si4mul- taneous nitration. The whiskersvere grown in a horizontal graphite furnace in a- flow of commerclal nitrogen from an Al 03 Q rge~at 1950719800 C. The 2 ha resultant specinens were studied in a scanning and a transraission electron nicroscope aund their brittle strength neasuriad a,", room tenpematura. The re- sults indicate both top growth from the'Atapor pl=e an4 bottor. Mwth from the idelt. In neither ca-se is the presence of an,axialscrev dislocation a necessar- y corAition for crystallization in whisker fori.n. The aiticle dis- cusses possible growth mechanisms. L fe 009 UNCL AS S I F rl.ED IROCESSiNG )ATE-1~60CT70 TITLE-l-EFFECT OF THE TRANSITION LAYER' AT' THE RUBdEf~ RUMIE!Z !1JERFACE. ON `F 'UL-CANIZA-ES THE COHESIVE ENERGY DENSITY ANL):A ON BETiiEEIN -- ;ADKI N, B.A. 'AUTHOP~(04)-~IREKHOV, S.V., ZAKHARWY N*D.v ~KULEZNEV14 V,N~ 0-1 ......... (PIDUNT RY OF INFO -USSR Z" RrE--,KQLL0 IDNYY ZHUqfNAL 11970#: VOL 32vl:liqR 21. PP'245 Z50 ;dATE PUR IS HEO----- 70 .-'SUSJECT AREAS--MATER I.ALS To..1C.TAGS-VULCANIZATE, ADHESION ELASTOMER~COHESIQAI C13NTROL ~MAAKING-NO RESTRICTIONS DOCUMENT CLASS--UNCL4SSIFIED -PROXY REEL/FRAMC'--1993/0397 STEP NO--UR/0069/70/ 10321'002/0245/0250 C.IRC.ACCESSION NG--AP0113315 UNCLASSIFIED .212 009 UNCLASSIFIED;; tNG DATE--- I. &OCT11 0 C:lq(: Ar~zss7o% A-?!j 3 3 l 5 :ABSTRACT!c_X'R,A-k_T--llJ) -UP-0- ABSTRACT. ADHES 10-N 1, E I EE% RM ii E R 5 N A S A E E N Z A N U M -A E R 0 F RUB B 1E P S . A 0 S I ON 8 Ic T E E L D U R U 6 ~, EgR S STUDIED LZ Pi E P E ItZ S 01-1-t THE P-ATIO OF rHEjR 00LAR COHESIVE ElN;EMrl_ES A'iD ""A-l'i 5ERVE 4S A QuAk LITAlIVE' 13F TK,~ THIC-KNESS 0-F I'Hz`~ T~,ANSITIJN L AYER RY aLE ~~' Y14G UP 17 1 - ' 0? -E:0 N D' 1 N G C LIF RUB6,c_:_~sl 1,.iE 3 E T w'E -N F V'J L Z A T E L -*Y S OF P T;: D 1~p R UaEERS HAS tlEEN, OEJE~4'k'i%E' -31 STATIC, AND 0 YNIA M I C M T J S TINE D Y rvA ll? I C TF.ST RESULTS ARE TN i"UAWATIVE AGRE-ZMEM WITH THE -.";'ATA F.-N ADHE-SION Of- ONCURE-0 POLY,-iERS A,'ll 0 CAN 6E OSED TO ASSESS -l' LAYE HE EFFECT OF THE TRA% 3 1 T 1 ,~P, ONN CU Y'JL C kt% i zA.r I &N 1 oF RUMI FR S. T H e. 'T -SIVE ENE; C, Y DENSITY AND 11" i_~, MPONEN I S "SH I P R A C U _1 RFLATIG% 4'~EN THE Pi R 4 T 10. , i) E.- T I E 0 F fi- i A '4J M, BE ~,-% Of , 8 L E 14 0 P E i~ 10 & ON THE TmANSITION LAYER Teilr_~,'iESS A~ I OF NU 0." THE UIFFERENCE- I P.- COHESIVE. fli ERG I F.S THE .,BLENDEO RU66ERS. UNCI 1. AS S I F I E D "'M Wo 7 7 NC ft, U -c A sl 'D R.OUSSINN5 D4TE--160CT70 BREAKOUN OF R UBBER-11M SUPEkHEATED WER VAP01 AT -u- f~ERIC PKESSUR E tfflip -(Q5)-MAKAAGVt V.M., EPSHTEY.N, V.Gt ZAKHAROV-t N.O. , MAKAROV, m A LQ A UA t-,WNIRY -OF--- INFU"USSR ~'SOURCE- 'KAUCH REZINA 1970, 29(2).t. 25-7 -AT SuBjECT A.REA S-MATER I ALS JOPTIC TAGS-THERMAL DECOMPOSITIOU, STYRENE, WEAR RESISTANCE, SYNTHETIC STYRENE RU13BER -CONTROL MARKING-NO RESTRICTIONS -DOCUMENT CLASS-UNCLASSIFIED ST.;:P C I'P. CAkCrIESSIG!4 Plil-APD113305 U-NCLASSIPIED Mal 11 MEMO 02 3 U. C L A S S I F I 1!7 - PAGCESSPNG ~)ATC---160`CT70i A-3STRACT, FH 5 Tz A! N L ;(,i r i D 7 Ej P. AI . s MED RU6 OzR S i; 1~ T I G .- c C L A 1 T 6 2 I ZE G 1", E E scc w I L I-S A ~-L) E D F T L) L E I, l L T ING CIF S S L Ny, I , I i- I ;= R I i 4 ~ ~, A l 'J'ES 1 J 3 ti 4~l I THOOT k~ . T THI S T I 43 D ;I I N, E: 6 y - , T T S T 81 L I TY, N, -z AFs RE:S a' t-Nli) PAT IGti k ECC L I. I r1 E c E KHNOL N S T Y -A R 0 S L A V L , USSR F-AC I L I T Y.- y AR OS LA V 028 UNCLASStFf.Eo~ ~OROCESSING OATE--23OCT70 ? 'OROPRENE RUBBERS AND -ITLE--QUANTITATIVE STUDY OF CRYSTALLIZATION lN cHL. -IZATES -U- VULC AIN ~'4UTHGR l(I.31-KOSTRYKINA,. G.[.- N.D.t EPSHTEYNi V.G4 ..COUNTRY OF INFO--USSR ?~~SOURCE-ZAVOD. LAB. 1970, 36(2)r 179-80 'D ------- 70 DATE PUBLISHE UBJ ECT AREAS--MATERIALS ~_":_TOPIC TAGS--CRYSTALLIZATIONt CHLOROPRENE, SYNTHETIC-RUBBER, VULCANIZATE, IR SPECTRUM,. ELONIGATION NAkKING--NO RESTRICTIONS :00CURENT CLASS--UNCL4551FIED PROXY REEL/PRAM;_--I"5/1472 STEP NQ--,UR/0032/'7t,~/o3ti.-*Dt)210179?~OiciO lp c ACCESS103.1 UNrLASSIFIED _1 R -1 T1.1 .2/2 028 UINCLASSIFtED, 'PROCESSING DATE--230CT70 CIRC. ACCESSION NO--AP0116909 ABSTRACTIEXTRACT-W) GP-0- ABSTRACT* THE CRYSTo BANDS IN THE IR SPECTRUM AT 955 AND 755 CM PRIME NEGATIVEI WERE USED TO DET. THE -CRYSTALL11*11TY OF POLYCHLOROPRENE (1) FILMS, AND THE METHOD WAS CHECKED -AGAINSTTHE DILATOMETPIC PROCEDURE AND REPORTED-DATA. THE RATE AND MAGNITUDE OF I ELONGATION AFFECT ITS CRYSTALLINITY; E.G., I PREHEATED TO 80DEGREES AOD T.HEN ELONGATED AT ROOM TEMP.: AT 1200 Mm PER MIN HAD TWICE -VAT 200,MM PER MIN. THE CRYSTALLINITY OF I ELONGATE FACILITY: 7; 'YAROSLAV. TEK14NOL. INST.t YAROSLAVI-t USSR# UNCLASSIFIED USSR C: 8.74 UD K N I WOV M "Cmeerning the Problem of Organizing Normative Data Blocks on Magnetic Tape" V sb. Vychisl. mashipy i pro-Eragair. (Computers end Pxogramrdng--collection Of works), Moscmr, 1971, pp 198-20T(froi,a. M-Kibernetika 110 6, Jun 72, Abstract No 6V516) Translation: The follow-ing basic -requirements are formulated for ortaniz- ing data blocks. 1) the necessity, for selecting an effectiie systeri of coding no-_uative data; 2) the necessity for wUnimizing. the -volurne of re- duadant date; 3) the necessity for optimizing the distribution of data blocks among the stages of the raemary devices to minimize the ~juanl(-Aty of normative data in the process of retrieval and alteration; 4) the possibility of re- cording and conposing normatives of data blocks of any volumes (both from punched tape and from punched caxds); 5) ;the possibilit~r of checking all operations of organizing the data blocks en ma6met-ia tar'es; 6) the possi- bility of correcting normnative data blocks recorded on ragnetic tape. The ~general principles of constructing data blocks, are defined in accordance with these requixre=nts. A method. irp de.s,cribed for tramsir.erring normative data.from punched carLlni of normativL. managenetit. to mapl."tic tape. It io 1/2 MaMROV, R. I., achjsl. mashiny i proalammir., Moscon, 1971, PP 198-204 noted that in organizing data blocks of normtive inforinat Acn, it is es- pecially important to provide for timely introduction of all chenges which arise in the process of improv C I ing technology and prrdu tion technique. in this regard, the following changes are possible in rormcitive data blocks: correction of outdated requisites of record; insertion of a new record; removal of an outdated record. It is concluded that effective organization of normative information on magnetic tapes and insertion of changes appre- ciably reduces expenditures of vork and timed. in utilizing automated produc- tion management systems. 48 UDC: USSR 5'.C)7/.08+53-001.5 -GLO ASITIN, V. In. V KOVALM05, V.-V., 1, B VINaculatiwS the Ga a Radiation Dose Rate of aCar~- O"et Fro-ptigating in thes Gro~ad Layer of the Atmosphere" -V sb~ -VoDr.- doz-ir-etrii i zashchitir ot izluch. (Problei=-, of Dosinot-nr and Tadiation- Sbielcliing collection, of works') . vy-p. 12, Mo3cow, Ator!izdat, 1971, pp.94-97 (from 41~ kor 72 Abstrm~t 11o li,%6961) The ga=--a s calciilat -~d Tj!~.LaUon radiation.dose rhte of a gas jet iz usi g 1dalta on distribution of the cozeentration of ai-tiviy iti t-c rrowld 1wer of. the atmosphere. The results of the computation z~r,:. nre,-c-nted -in a.,. Oil of '. Jot the! form,of the reduced dose rate:c-eated by.the gzlrrxp- I*a,!-l eacap! -from a source with a: rate of c ng I uric/s Lt U VA-11d -'MUcd of I ittht; f ix long-lived isotope Vith K. - I ramz/hr, curie. 'Une reduced dose rate or ~y deq*new vealy oant tb-e g&mma radiation enerf, -. in the ~qv:rfj -,w-,j:,,r, Z, y I O.-l'-t6,2.5 it 6anrcs by i-3-0% from the vajie tit E= I Accowiting for the radioactive decay of isotloyes Ndth T~,'~20 min givc-,-- it correction to the close rate calculated for long-lived isotopes of' azo rorc- than 8/j. The position of the maximum for the ground-layer dose ritte in thc case of 1/2 V, 0. V. do metr4 i i zashchi ty 0t i ZIUCIII. K"10. PzSccv, At"mizda:t, 2972, -up 94-9T a solarce raised alcve the sunfa2:~e do--s not -coinclidie wi-~h ll--ie of the =--7frm= for t~he Erc.;z-d-2ayeer cczecAratiol). of a:l Jsot'c-~I-' for all i n- vestigated, g-amrza radilaticzn ener~des aad~ metcorologi-cal Tll~ttv 4 for 'r Joc!i'ed nuuh 4111-- thler from the souxce thwl the maximum f~r the grotaid-level ilose rate. A. A. 2/2 -ft IN 017 UNCLASSIFIED PROCESSING DATE--30OCT70 .TITLE--SY, DISSOCIATIOW %1THE-SIS AiNO EQUILI&RIUM DURING THE OF SOLID ~ULUTIGNS 3F IRON AND MANGANESE ORTHOTHANATES -U- AUTHOR-104)-SHCHEPETKIN, A.A.t ANTONOVt V.K.v LAKHAROV, R.G., CHUFAROV, ~~CGUNTRY OF 1NFO--USSR ,.-.--SOURCE- I ZV. -AKAD. NAIJK SSSR, METALo 1970.? 12),~144-6 ---DATE- PUBLISHED ------ 70 ~.S:UBJECT AREAS--CHEMISTRY, MATERIALS -,-TOPIC TAGS--CHElliiCAL--SYNTHESlS, SOLID SOLUTION, CHE141CAL REDUCTIUN, _''SPINEL, CRYSTAL LATTICE STRUCTUREo TITANATE, G NESE COMPOUND .. tCNTROL 1111ARKING--NO RESTRICTIONS 0 0C_UJ14 E N TCLA55--UINCLASSIFTED 199 V I U -P NO-U, PROXY REEL/fRA, STL 't 0j r 0/ t 0 1000 100 0 14 40l6 tlRC A Ct. F S S I ON f4fj--APolZt64&-' UNC' LjkS S i F I ID ~:~'2/3 017 UNCLASSIFIED PROCESSING DATE--30OCT70 ACCESSION:NO-AP0121682 -ASTR ACTZEXTRACT*-(U) GP-0- ABSTRACT. THE FORMATION OF SOLID SOLNS. OF -SU,84 AND MN SUa2, T:10:SUB4 'AND THE PHASE EQUIL. PROCESSES DURING THE REON. OF SOL10-SOLNSAWERE STUDIED. SYNTHETIC FE SU134 AND MN SU82 T I U, SU84 WERE PRESSED INTO TABLETS AND HEATED ,`~-'-FOR, 10_HR,--AT-ll00DEGkEES UNDER AN ATM. OF~88 VOL.PErzCENT CO AND 12 PERCENT GO SUBZ. THE SAMPLE~ THEN WERE TEMPERED IN WATER AND -A ALYZED BY:USING AN X RAY METHOD.~ FE~SU82 TIO SUB4 AND MN SU82 TIO -':SUS4 ARE~.PERFECTLY MISCIBLE, FORMIN G A*CONTINUOUS SERIES OF SOLID SOLNS. CRYSTAL LATTICE OF SPINEL STPUCTORE.- TH&PERI D OF THE LATTICE 0 :INCREASES 'WITH INCREASI NG CONCN.- OF ~ MN li SUBZ TIO SUB4 IN THE SOL ID SOLN. BAND RANGES WITHI_%, THOSE OF PUkE fE. SU32 TIO SUB4 ANO KN SLli3Z TIO SU64 i535-8.679 ANGSTROM). THE STUDY OF THE EQUIL. CONPN. OF THE SAMPLES AS, - AFU-NCTION OF THE AMT. OF 0 PRESENT-WAS PERFORMED BY HEATING THE :SAMPLES AT 1000DEGREES UNDER AN ATM. OF. H,AN0 H SU82 0. THE AMT. OF 0 -SAMPLE (EXPRESSED IN PERCENT: bF THE TOTAL AMT. OF 0 PRESENT IN THE PRESENT) WAS:CONTROLLEO aY CHANGING THE.PARTIAL PA~SSURE OF H IN THE REDUCING ATM. ON REMOVAL OF 0-25PERCENT Ot SPINELLs, RHOMBOHEORAL, AND -METALLIC FE PHASES ARE IN EQUIL* THE SPINEL PHASE CUNSISTS OF A SOLID 1. -SOLN. OF MIN SU82 TIO SUd4 AND FE SU82 TIO SUB4. THE kHOMBOHEORAL PHASE CONSISTS OF SOLID SOLN. OF ILMENITE ANlYPYROPHANITE" ON INCREASING OF THE AMT. OF 0 REMOVE09 THE CONCN, OF FE SU82 TI-0 SU84 IN THE SPINEL PHASE DECREASES AND THE CONCN. OF PYR-OPHANIlE fN THE RHO-4110HEDRAL PHASE INCREASES. AT 25-35PERCENT 0 REMOVAL, A RHOMBOOEDRAL PHASE EXISTS IN EQUIL. WITH A TIO SUB2 PHASE AND A~METALLIC FE PHASC-. UNCLASS IFIED OATE--SOUCT70 AMT* OF 'USSR UDC. 533.9... 16 BASOV, 11. G., ZP-RITSKIY, A. R., ZAKHAROV, S. D., KRYUKOV, P. G. , RAT- V=1S, Yu. A., SENATSKIY, Yu. V. , FEDOSIMOV, A. I., XHEEKALIN, S. V. "Producing High-Power Light Pulses on Wavelengths of.1.06 and 0.53 Pm and Using Them to Heat a Plasma. Il. ANeodymium Glass Laser With Con- version of Emission to the Second Harmonic".'~ Moscow, Kvant. elektronika--sbornik (Quantum Electronics--collection of works), "Sov. radio", 1972, pp 50-55 (from PZh-Fiz-;ka,, No 6, Jun 73, abstract No 6G375) Translation: Investigations of processes of heating by means of laser sources -with different wavelengths are,of considerableiimportance for explaining mechanisms of energy transfer in.laser heating of a plasma. This paper tells of the development of a.high-power light source for heating experiments with emission on, .two wavelengths: the wavelength of a neodymium laser (1.06 )jm) and ltr, second harmonic (0.53 pm). An ef- ficiency of greater than 501a in convel-ting IX6-wn emis'sion io the second hea"monic is achieved in a KDP crystal. The emission enera on the 0-53-5m Vavelength is 10 j with a pulse duration of 1.0 ns. Part I, see R7,hFiz, 1973, 5G239. 1/1 46 USSR UDC:~~ '621,378.9:533.9.02 ZARITSKIY, A. R.,- ZAKIIAROV. S, KRYUKOV, P. G., FEDOSIMOV, A, I. 11M easuring L -he Polarization of Back-scattered RaOiation Accom- panyinl- Laser Heating of.a Plasma" Moscow, Kvantovaya Elelctronika, Sbornik Statey, No 2(8), 1-072, PP 89-90 Abstract: h1hen a plasma is heated: by powerful laser emnission with the use of solid targets, the laser light is strongly back-scattered. Polarization ineasurements are made oil a wave- length of 530 nj-..i using polaroid films; the de I.C-(! Of I)CIar4 1) - 1) 14 og rZi r,]-- - tion of the reflected emission comes to 90-95T. L _k of three titles. US19R ULO ~~--J - + BASOV, A.R., Zid'.11f, ROV'k, yu, 1~.. S.D.?_lJ,-fUZC'kf, F. 'Y SMAT-SK1117, W.V., FEDC'SlYcv, 'ix, sa. "Achievemont Of Poverful L--E- _se-_- At A v _,ht n~ 1 alem~- h ~G' I CkS And Their Uou For Plr,,.lma flestiMc-. IT--" -Glar~r- Lanc-er VNIh Conv6r.,;ion 01 Raci-l- ;yd ation To The Second ;larnionic" Kvantovayn elchtronil~,_ (q~uantum Vu 6(1'-).. 1572, un `0-55 Abstrzict; Thi, cornt)-ok;tion iE deo~~ribed. ami th, c O-P a rill It iat e h2-rJ:a,_v liz~!-er. Tote arsombl- ccr,;Diztr~ iAf' '100 Act've elezentu of CLS-1 reodr-,JL',J;n D T41:11 jCng lr"tjj C.O.A. lit n Bre-asterian jingle; 2) Pet;onator mirror; C.(jl,lrj wlth nlwurin! of lonf-ALW",,wl brIni'le, and o A dirirlrE, atir: i 11 c, t c, rP se r3 E, t! a c c c rn,7 t G- -Vf~C ~CJICULIO CU'. G0L;i'll;itGr ',itll st~ cf, ~_mrv.olj a.,- t'nf, "Jource ol ~.,,hart 11HU in device. The lanELh o4' thr-, 02cillator reson6t or, f orm~-d by ta o r r o f JeC4 n c j ~ nt c C,' jr 2C? pr,-rcant, artounU to 6 in. "e" ncil.- linc~r abcarber -- Ei r, ct I -u o P c 'L 110. U, e in nitrohuer,;~~,,,!t!(-,, wi~,rc 4-n e~ on trac' with an onaque mirror. Iwo s-glec, Ors Cif f Orl!~ f"r USSIR N.C,,, et al, Vvantmi-rIva e I ekt !.'oa c o wMn (S(!2), pp incl-ired 17, brv-'Ferot erc-r~~, d f'or nLrrcw:,,u- ci t,,r~ spectnnaf:. W'ith t-he uid of '~'-P-se itatr-rferon,eturm th;-- nerz-,I, i (~,rl narrowu~d toevO.05 P, rend ir, sa daing the pulm~,i by, oi c I o r v; oxnarded to 1 In tLr; VDIP. cryst-,',I thi-. -A the nu'i)~,zt -& ccn- verteC, into a occord with en efficicncy ',0 percent. The radibtlen enerry rA o- microu wavelcn;~th Ei-mtA.-mts- tQ IC; 'cule. Ti~,-,- thonk 1-!.F. Steil~a]7'h I.S. A.T.Yovrifrin , arid .1or cry -!tccdved by in cciiduc~,.L , experli-ftents wilth 1"JO I i, ill. 16, --c--' R, ed It ors, 25 c)----' I S;-('l - 70 USSR UDG' 54~.46 + 621. ~'75----25 B. D 1-*, R% H 13;-~ O.N., RM"1011, 1~.G. msov, ZARITSIM, A.R., ZAKHAROV, MATVM-~M, Y1J.A., BRNTAT,ci~IY, ITUN., FEDOSDOV, A.I. Of Powerful Light Paleee At 1.06 And Nic-ron Wt:velen,~trw j,,.nd cnievemen" u U Their Use For Plasma ficating. I. Experimental 54- Wdy Thu OP ion Reflection Durinz Laser Heating Of Plunrw At T w u I E;- x1gii I i I` oul e, 0, Kvanto ~~ya elaktron'Ma (Q-~.,antum. Elpatronice) 901),197-2, pp 6;~-V Abstract: Th.-. experil-nantal resulte ar'e Prei3-anted o-. in i ;---at in m eu, s, 1 r e m e i it u of ra d j F- t i o n r eIc t oils snectra I and Polar k which is heuted by nitlosen-ond laser pulses Wit'- a wav31C;nrf,1-, or 1. Co micron with fluxes at targets of vi~riouq IrrmLeviil~i 110- 11, L r The reoulto dipc~asnecl reo-enenll t~e first ckttwipt to stud-1,11 jt~em.,-r lieAin,~ of plagma whl.ch is prodwo-ed at solid targo, -, in ti On C.-I, th- t r he It is f Oond t1int plao!".-A abso-r-ption 01, the Ilea at ti 0- langth in throu 1,1!noo gre-ILC-~r 1,1wil et. it I 106 na-lcron wav(-;Iura~,h. Th~~ exproco thuir approciation to V.B. Rozanov for dli3cun-,tlq~i of -t~he re,.-Li'Lcz of' 11,o, L viork. f i g. 19 reC. c c, i v c dby_ edl Pre, - 2~ P,~ L19'114.a USSR ZARITSKIY, A. R., Z KRYUKOV, P. G.0 V4TV=S, YU. A., and FEWSIVIOV, A. I*f nstituto imeni. P. H. Lebedev, A.cademy of Sciences USSR "Vaxiations in-Back-Scattered Radiation Spectrum DurIng Iaser Heating of Plasma" Hoscw, Fisma v Zhurnal Emperimentallnoy i Teoretielitskoy Fizikl, Vol 150 No 4, 20 Feb 72, pp 184-186 Abstracts It is known that strong back-seatterln6 of laser light oc-Mrs during the high-power laser radiation heating of a plasma with the uso of solid targets. The authors meassured the spectrum of the latier light reflected by the plasma* The targets used itere, I&Dj ~ap-2)n, hea~vy ico, Al. The radia- tion source was a self-node-locking Nd lazer:consistin'(g, of a riaster oscillator and a six-stage amplifier. The plasma. heating and spectral mi)asurements were ca=ied out on the fmdamental frequency ( /N*- 1.06 miin.,ons), ws vell as on the second harmonic frequency 0. 53 zicron). The- measurements were 1/2 USSR ZMTSKIY, A. R. ot al. Pis Ima v Zhuimal. Rk-sperimeatallnoy I Teoraticheskoy Fiziki# Vol 139 No 4p 20 Feb 72s pp 184-186 made on a grating spectrograph u-ith f 130 cm. The tack-sGatterod radiation apectrum was found to have a large number of equidistouLt lines, situated gen- erally both in the Stokes and -the anti-oStokes part of the spectrum. Ttds is due to the presence at the line of Incident radiation::rrom weak sat:ollites, the distance between which equals the interval between the lines of reflected light. 7he observed process is of a stimulated chax meter. Its explanation may be related to the phase modulation of high-power.light pulses in the plas- na layer. USSR UDC 662.215.2 ZAKMAROV~ -D, LIKHOV, G. M. MIZYAKIN, S. D. , Mos -'6w I'Determination of Dynamic Compressibility of Soi Ion ~the Busis of I'arancters of Flat Explosive Waves" Zhurnal Prikladnoy Mekhani'd i Tekhnicheskoy Fiziki, No 1, 1972, pp 137-140. Abstract; The d),namic compressibility,of soil has been determined on the basis of wq)erimental values of the parameters of flat, cylindrical and spherical explosive israv,cs at stresses generally~not exceeding 80-100, some- times 250 kg/crii2. This articl-:- n",gents results of e-xperim-zntal studics of flat waves at stresses of up Lo 1,000 kglcj112. These data are used to construct a stress-strain diagrant corresponding to shock coirpression at the leading edge of the wave. The degree of:compacting of the soil is deterillined. It is demonstrated that deformations continue to incmasc behind the leadin- edge of the wave. The residual deformations are grootor than those fliat occur at the leading edge. This. indicates a, signific. pit inf of viscous wid plastic p.-Operti-es of soils on the wave7process. 775 UDC 621.376.9:533.9.02 USSR ZAKHARQV,~~S. --D.,--MOKHI1T, 0. R., MYUKOV, P, G., SDIATSKIY, Yu. V., BASOV, It. 1YUR111, Ye. EkkV, A. I.- CHIEKALIN, S. V., Sh'CHELEV, 14. Ya, "Stud les of a Plasma Formed by Ultrashort La-ser Pulses Moscow, Kvaantovaya M-ektronika, No. 1, 101, pp 11-28, C t Experiment-a'. studies'of procelssc-s Occurring in 1~1,je heating of a plasma by focusing ultrashort laser rad tion an thO Surface oF uteride are described. Studies of.,plasma heating ,;it*,'l jas~lr ral iation lithium de n 10-11-10-12 sec were begun in .19~8 at the Laboratory of Quajj-,:Lin Padio- of duratio physics of the Physics Institute imeni P. 11. Lebedev. ~Fast neuti,ans were recorde-~ -F thlun upon focusin-- these pulses oil the surface r- ---4 11 deuteride tavZet, Indicat- ing the rise of conditions for a thermonuclear db-reaQt4,on z1nd fox, obtaining a blasm,a of high temperature and density. Subs'equent reso-~arch raic-Qd the -foliowin-- questions: how does absorpti-on of energy by a solid occur if, tile Jasev radiiitio~i is concentrated in a pulse with a duration of sevellal plcoseconris? How is tile sstt~ng reflection of laser radiation from the target expiiainej? What are the possibilities of raising ion temperature, and consequenOY 11"I'tron yield, in A o G e t a I Kva n t ktr6nikd: Ito i I pp 4-26 BASOV heating a plasmna with ultrashort pulses? Shadow photographs of the plasm-i with illtmiination by ultrashort pulses and the recording of plasma dispersion with th~~ aid of ai, electron-optical converter are described. The same ele--tron-opt-Ica! converter was used to studv the chanae in the reflection of laser vilises w`th' time, and x-ray mea-sursments were niade of the electroa tempz!rature of the Plasma, A review of the'basic experimental data indicates that the results are from laser pulses consisting not of one, but of several subpulses. Experiments show that the interaction of each suhtpulse Drith the target is rot the. s:ime but a 11"urct-lan of the previous history and repetitlon -E.ime of the subpuise relative to the beginnLing olf the process. Heatinr7r of the p, asma occurs as follows;: one r--,f the 1 first subpulses incident on the targ~et ionizes it to a.~dejpth appPcj>:iwatQ1,, cQual to- the wavelength of the laser radiation,. When the vall.ue n-J: n becomics pSit of the SUbpUlSe is rerjeC4_ to the value of n cr the rrjpainin L the plasma to a tc-mparatura of _czevi~raj. electrbin-volts Occurs sxmultaneoL_-~Iy with ionization. As a result, the plas-mrin- formed is slowly disper5ed. All suhpLilscs incident on the target at this stage will be reflected until the particle densit,; drops as a result of dispea-sion,to value correspording to n At this tire cr" high-temperature heating of the plasma is possible. It is thus e!-,tablish,:!d that reflection of ultrasonic pulses arises in, plasma regionz7, wlere thc, electron den- ical. Other subjects discussed j-~I, -1,,c: ticle i., IT - p-. sity ~is cl-ose to cr .1 8F radiation and heat coaductiVity, the ;ffect of laser radiation Pressure, ar-A elec- n-jon relaxation in a pla-sma formcd by,a powerful ultrash-~~'t laf:er tro, Z12 61 ov 'USSR TjDC: 62-1 385: 530-1115-6:53 BASOV, N. G. , ZAP KROKHIN, 0.. No KRYMCOV P. (1. SMATSM, Yu. V. , CIMKALIN, S. V. FEDOSIMV, A. I., SHOMLEV, Y. iYa. "Investigation of Heating of a Plasma Formed by Ultrashort Laser Pulses" Kratk. soobshch. po fiz. (Brief Reports on Physics), 1970, no 8, pp 48-52 (from RZ -Radilotekhnika, No 12, Dee 70, Abstract Ito 12D464) - Translation: In order to form a plasma, ultrashort pulses of emission from aneodymium glass laser operating umder conditions of' sl~lf-synchronization of modes on a wavelength of 1.06 P vere focused on a target of LiD in a vacuum The period between pulses was 15 insec. Me individuitl laser pulze is not simple, but rather consists of a series of peaksli tube Interval betWeen them and the number of peaks varying from flash -to flash. The overall pulse duration reaches 10 nsec, the duration of tw individual peak being in the range of 10-11-10-12 s. 5he output_energy is -0.1 J. The diameter of the focal spot on the target is.2*10 2 cm. Oleatling of the plazma -was studied by the methods of shadcr4 photography ahd schlieren photography. A. K. 102 OW, USSR UDC 532.71:66.066.6 DYVERSKII, YU. I., ZAKHAROV. S. L., Moscow Chemical Technology Institute im6ni D. 1. Mendeleeva u "Additivity of the Process of Separation of Two Aq eolis Solutions of Salts by Reverse Osmosis" Leningrad, Russian, Zhurnal Prikladnoi Khimii, vol 46, No 7, July 73, pp 1455- Abstract: Experimental data obtained with cellulose acetate membranes and K, Ha, and Ca chlorides and nitrates in aqueous solution showed that the selec- tivity of the membrane for each salt in a mixture is the samit as for the indi- vidual salts alone. The constant porosity of -the mettvane was shown by de- termination, before each ezperifrient, of. Its penetrability to pure water. The selectivity and lower poni,~Crability of the mi,4mbvano tt~ ,iti. rig a Od C) ly hydr, t:. W~~ ion thiin co z~iolut:lon8 containing the weakly~hydrated 14.1-f and K'~ ions can be explained by ,a capillary model. The additivity off pvocosseL~5 for separating chlorides and nitrates by mwer5e osmosis makes it possible -to calculate the expected separation from data on individup-1 salts. USSR UI)C: None BASOV, N. G., BOYNO, V. A., "LD-ROV, S. M. -IaOll~alnl' 0. -'1., ah LI MIMPLY-011, Yu. A., SKLIZKOV,~ G. V" d FRPOTQVq &J. I. "Mechanisms of Nieutron Geaeration in a Laser 21asmall Moscow, PisIma v ZhETF, vol 18, No 5, 5 September 1973, PP 314-317 Abstract: This letter gives the results of. experiments Derformcd to investigate the mechanisms Which give rise to neutrons in laser plasmas. The experiments here described proved that, depending on the experimental conditions, both hot and cold neutrons are pro- duced. The mea'~urementz involved were conaucted in a vnr.4,-.nt of the sharp focusing of a sinCle-channel,laser on'a massive C*'2 tal'- get, as well as in spherically symmetrical irradiation of CD2 particles measuring about 100 /A.in diameter by the output of a multichannel laser. Both methods ia,ere discussed in earlier 13a-ners by the first-named author above, ot al. .(Pis lm'~ it Z1113'4~'I'l 13, 1971, p 691; L5, 1972, P 589; ZhETF, jL4, 1972, p 205T. He:~uits of both types of measurement are separately exaninod. Some Of theoe cast doubt on the assertion of previous researchorsthat the appearance of-fast ions is comie.-ted with acceleration in the cril"'ical den- sity region. IA' USSR BASOV, N. G., BOYKO, V. A. t GRIBKOVv V. A. r S.M.o KROKHIN, 0. N., anct SKMKOV , G. V. Physics Institute J Academy of Sciences -USSR ling!' "Gas Dynamics of a laser Plasma in the Process of He;i Hoscow, Zhurnal Eksperimentallnoy i Tedreticheskoy Miki,:Vol 61, 110 Iffl, Jul 71, Vp 154-161 Abstracti ,Ono of the two well-known approaches to tba problem of heating plasm to thermonuclear temperatures by-irradiating. it with a laser is the method in which a substantial portion of the energy cT the laser is convexted Into the energy of directed, 6-as-dynamic movement. in the present a--ticle, an attempt is made for the first time to neasure the'distribution of the density and speed of movement of the plasma, to evaluate the pressure of the plasma during the process of heating. A taultimode Q-switahed laser and a carbon target were usedg, amd measurements were made ty slit scanning of an interferogram on an image converter, It ms foum that the naximam rxessure (10 atmospheres) and temperature occur at the beginning of -the laser pulse. At later times, the profile of the density:is elevate6o and the area of the 1/2 USSR BASOV, N. G., et al., Zhurnal Eksperimentallnoy I Tooreticheskoy Fiziki, voi 61, xo 1 (7), Jul ?1, pp 154-161 plasma In which absorption take,5 place dxaws back fxom the taxget and increases, The mass of the gas heated dixectly by, thelaser beam also increases. The temperature in the hot portion dropsi and:an incra-Laingly greater part of the radiation energy is converted directly into the kinellic energy of the disintegrating substance. In this manner, by varying the dependence of the dispersion of the radiation on time, it ispossible to shift the naximun ..Pressure and to achieve optimal.utLUzation of the,la6er's energy when heating plasma under real conditionSO 2/2 7.7 ,-fit; USSR UDC 533.916 1;,.,:~~__:_-.`_:..~ i~sov. VN. G., Academician, BOYKO, V. A., DROMBIN, Yu. A., KROKHIN, 0. N., SKLIZKOV, G. V.j and YAKOVLEV, Y..A., Physics Institute imeni P.-:N., Lebedev of the Academy of Sciences USSR, Moscow t -Dynamic Dispersion of a Laser Inves igation. of the Initial Stage of the Gas Jet-Plasma" Mosc&f Doklady Akademii Nauk SSSR, Vol 192, No 6, -1 Jun 70, pp 1248-1250 Abstract: Since previous experiments study the radiation spectra and gas-dynamic parameters of a plasma In large time. intervals oxcoi!ding the len8th of the laser pul.se -in and the kfnc~tics of the present study covers the dynamics of the moLk ionization processes in a laser plasma with a high time resolution. It ts noted that the gas-dynamic motion of a plasma accompanying the high-temperature heating of-condensed material with focused laser radiation has beun investigated because of the-importance of the possible use of a laser.plasma for thermonuclear fusion, as a-source of multicharged ions for spectroscopic studies of astrophysical in- terest, for accelerator technology, etc. The study of the diapersion of n 1)103sma during the action of a laser pulse and at distances r fton the- surface of the rable with the diameter d of the focusing spot of the laser radia- target compa tion made it possible to trace different phases of the motion of the material, Z4 IA 44 USSR BASOVI N. G., et al, Doklady Akademii Nauk SSSR, Vol 192, It 'a 6, 21 Jun 70, pp 1248-1250 including the initial stage of heating and the "freezing" of the -Ionization state of the plasma. The radiation of a neodymium laser with an:energy of 10 j and a half-length of 15 nsec was focused with a 5-cm lens on the surface of a carbon -6 torr, and the structure of the dispersing plasma was target in a vacuum of 10 investigated on the basis of its luminosity, Space-time diagrams of ion dis- persion were obtained from analysis of the data (see Fig.):; for r 4 1 mm the plasma emits a continuous spectrum in the visible region (lines are observed only at distances r > I mm). As the distance increases to 10 Twn, a break is observed in the luminosity of ions CVI and CAI from the target. The regions occupied by ions of different charges partially intersect, although there tire no discontinuities in the density of material in the plasma. The following model of the gas-dynamic motion of the heated matter is constructed from an analysis of the experimental data: The plasma moves frora the region of heating (r < d), where the electron temperazure Tenjl20:ev on the. basis of measurements of the recombination x-rgdiatioa, into the~vacuum perpendicular to the surface With a velocity u -v 6,10 cm/sec. In this.region the vejocity of tile plasma .is close to the speed of sound and the ion temperature cOrreep6nding to this 2/4 USSR BASOV, N. G., et al, Doklady Akademii Nauk SSSR, Vol 192, No 6, 21 Jun 70, pp 1248-1250 velocity is rul25 ev. A considerable acceleration of tile plasma is observed at distances r :5 1 mm. The velocity here is several times greater than the Initial. -ir-2 along the The effect of "freezing" is obtained, since the density arops as u trajectory of the ion and the.recombination time becomes much greater than the characteristic.dispersion time. In one process the freezing of the maximum degree of ionization occurs several.nanoseconds after the beginning of the motion of the "elementary volume" of the plasma. This.freezing process also occurs for the remaining ions. The laminar structure of the jet which is ob- served in photographs is explained-on this basis. The~energv;lost by the plasma contained in the region r 4 d to radiation in.the range120-160 over a time of 40 usec is estimated to be about 0.5 joult. 3/4 1/2 023 UNCLASSIFIED PROCESSING DATE-30OCT70 OF TEST CONDITIONS ION A COMPARATIVE EVALOATION OF THE WEAR RESISTANCE OF TIRES -U- A.UTHOR-!--!-04J-GENlNIKH# M.E.v GUSLIT SERI R*L. ZAKHARbV, -S.P., MISHNEV, G.V. __jr .ARCH-- ACCESSI-ON- NO-AP01 24503- - , --- -- - -- - -- -- - - --- - - - - - - - - I - - - : , i , ii . . . . . . . . . . . . USSA UDC 620.179.14 ZAKHAROV., V. A., MMEYEV, M. N., FRANTSEVICH,:V. M. "Design of a Ferroprobe Coercitimeterlwith,an Attached Electromagnet and ~Coi~pensation Winding" Defektoskopiya, No 4, 1971, pp 21-31.~ Abstract: Results are presented from a study of the'dependence of the ampere turns of demagnetization and compensation~on the parameters of the magnetic circuit of a ferroprobe coercitimeter with an attached electromagnet and compensation winding, as well,as certain experimental. results. Simplified formulas are given for calculation of the ampere turns, as well as an example of calculation and a schematic diagram of the semiautomatic ferroprobe coer- citimeter for testing the quality.of heat treatment of products. MisceUaneous USSR UDC 669.15-196:669-974 ZAKWOV V LAWEVA, N. K.,, and CRICHAGOVA, N. P., GorIkiy Automobile Plant IAustenite-Stability in Alloyed Cast Iron at Low Temperatureq" bloscoi-i, Metallovedeniye i Termicheskaya Obr4botka I'lletallov, No 12, 1970, pp -49-v5o Abstract: Nickel-copper-chromium cast irons have an austenite structure at room temperature. At below-zero temperatures, however, the austenite in these cast irons turns to martensite, vAich is followed by volumetric changes, an increase in hardness, a nd a decrease-in metal plasticity. This paper discusses the effect of chromium, nickel, manganese, and copper contenbs on austenite stability. The study involved 20 melts pro 0. It is noted in conclusion, -that tht:! pro_hl(%m of thC- asymptotic behavior of- the cross section when exchange of inassless particles is possible is not limited to the scope of weak interactions for which neu tr i n o exchange is essential. It also has a direct relationship -to electrWlagnetic interaction caused bv photon exchange. For the case of massless PaX"_ ticles many theorems of quantum field theory aro inapplicable in -th(_- forrq in which they are ordinarily formulated. This is attrlbate~d to the fact that they assume the presence of an energy slit between the vacuun and the sT)ectruir. of physical states. It is suggested that it would be of interest to obtain a more detailed description c- the asymptotic behavior of amplitudes on the basis of the,-;e ideas aiid to understzmd better their relationship with the basic Principles (-"-r f-1(-.1d theory, 2/2 USSR UDc: 621.3-71-34 ZAKTAFOV, V. I. ItMeasurement of Distributed Reflections With the Aid of 1-lide-Band Frequency I Modulation' DoPl. "Ises. nauchno-t~!kiiri. konP~rentsii po radlotakhn. iznaLcni =i. T. 2 (Re- ''Ports ot the All-Uttion O'clentific and:TachnicaL -Con fe!rerictt~ on lludLo Eiigincter- Ing Measurements. Vol. 2 Novosibirsk, 1970, PP 139-143 Cfrom BZi-Radiotekh- ni~ka, No 12, Dec 70, Abstract No 12A389) Trmislatioa: It is noinPeel aut that in contrast to classical -nethods (mea- surement linefi, bridges,,(:tc.), radar method,.i at.* appli;z!tl to prol)ing a f -.1-ranspLission lines and extundc.,d 8,HP lbaths make, it pal,-oibloj to (Ie-tf~,~rnjine not only th-e distribution of extreiriely small discrete rnfluctions oJovig, the -nderice of anV.zpfcJfic reflf~c- channel, but also the pretilt,_~ frequency dtqw tion, over a wide frequency rnn[!j_,. , A ~brief deticription in :givfx~ of a mea- t device in which a continuously radiatvd sipaL wiUi lirtear frequi!ncy surement, modulation. is used, together with a description. of the extraction of neces- sary information, processing of these data,: which is done sby the methods of low-frequency.technology, permitting.increased measurement precision. Gon- sideration is given to the effect of a number of factors (modulation non- ~7' USSR UDO 621.382.3 V.M., SHCHIGOLI, F.A., NAUMMWO V. GP P SHICHEM-HIOV, B.I., XOZLOV, TLJ. G., MHAROV. V.I. "Silicon Planar n-p-nn+ y Transiotor Obtuined By T h oMathod Of Ion Implantation V Bb. Fadiatsion. fiz. nem-ot. Irriatallov (Radiation Physiall Of Nonmetal Cryatals- Collection Of WorkBF, mlnsk, Nauka i teldui., 1070, pp 155-1~_;'8 (f rom RZh-Elektronika i yeye primenoniye, No 1, January 1971, Abstract No IB221) Translation: 'fno mathod of ion im3lantation in conjunction. with planar I-echnology ;i~kou it possibla to obtuin n-p-nn rlicrowavo: tranoistors with a critical freq- usney of amplificutlon with reepect to the curront of f,,,. - 2) Giliz. Spocimons viero obtained and investi-Eated with a diffuaion bape and an ion-implantation emitter, .-:and dovicea in whien both the collector and emittor junctioiia wero produced by -.,::the method of ion implantation. Banic otaticiand frequency paramoters of the .-devices.are presented and aleo the depohdencos V ct: f(ia)" Stumary. 11- !H i I j I I I I. I 111 '1 -1:111 USSR UDD 621.*5821621.1 117-799 -ZAKHAROV, V.I. "148BBurement Of The Scattering Parameters Of High-Frequency Traneistors" Tr. Moak. eleRtroteRhn. in-ta avyazi (Sorke Of The Moscow.'GlectrAcal Engineering Institute Of Oomminics one), 1970..No.[Not shown], PP 74-79 (from M-Elektroniks iyeye primeneniyo, No 12# December 197Q9 Abstract Nq 12W441.8) Translation& A method is proposed for measurement of the aoattering parameters (S) characteristic of the operation of microwave transistor amplifiers. Measurement of the scattering parameters Is conducted with * resistance connectod at the input and output of the transistor being investigated,. which aBomrav a: regime close tc the operating conditions of an omplif Ler. A bloc*K diagram -of the unit is presented no wall no the principal alroult for binning tho tranolator mnd %hm roe-oltis of measurements of the scattering parameters of,wior,owava lot#-;P9iofo~dirfjsod tranalo- ~tors connected in a circuit with a common olittor and, a CmIzon bilse. ill. 6 tef. ----------- ffimnumi USSR OKUNI L. B. DOLGOV, A. D., DOLGOLENKO, A. G., ZAIUIAMr. V. 1. Institute -of Theoretical and Expiii-n MUITYt cs, State Com- mission on Utilization of Nuclear'P6w'er "KL -2p Decay and the Possibility.of Existence of a Light Vec- tor Meson" Moscow Yadernaya Fizika, Vol 16 Aug 72, pp 376-383 Abstract: The authors discuss the hypothesis which holds that the existence of a liaht vector meson X0 is responsible for the failure of experiments set up to detect 1%'L,,4-, decay. The analysis shows that existence of a X-meson with the properties necessary for compensating the two-photon contribution to Im F (KI -* 2 v) contradicts experiment. This and other diffi- culties seem to rule out the existence of such a particle. If the hypothetical X-meson does exist, it w6tild have to decay into new light neutral particles or undergo interaction both unlikely possibilities. The authors thank V. V. Barmin, 17. S. Demidov, A. G. Meshkovshy', N. N.~ Nikolayov and V. A. She- banov for constructive criticism. M i T 1-iff9 USSR BOGOMOLINYY, YE. B., DOLGOV, A. D., ZAKHAROV. V. I., 0KMN L~ B., T SHIFMI, M. A. SPIALAI fKOV, M. ZH. t = u t e~�r M"retical and Experi- mental Physics of the State Committee for* the Use of Ato,"nic Energy "K0 p'~'jj~ and tche Anomalous Interaction,of Muons With Hadrons" L Moscow, Yadernaya Fizika, Vol. 16, No. 1, Jul 72, pp 129~~142 Abstract: The possible cont-ribution of the 3n-intermediate state in the imaginary part of the amplitude of litp- decay and tl~e possibility of AL the existence of anomalous muon-pion interaction which c6uld balance the imaginary part of the amplitude of KO vtp- decay arisipg through the L 2y-intermediate state are discussed. it is noted that tl~e existence of an anomalously strong pio-i-nuon interaction cculd resolve the contradiction betveen the experimental results of -Clark,: Field, et al and the theory, but it is shown that the anoralous, tpteraction~s Tro - 211 and 3t, -- 2p do not contradict existing experimental data On elastic and:inelastic scatter- ing of a maon by. a nucleon, on the generation of muon pairs by pions, and by data on (g 2) for the mion. it is noted that in thJ,8 aprp~oach scrie, Ov) difficulties arise which are associated with the very large value of Re j, 1/2 KL I MI I a .1il UIPI'l, ;1:1-111F; __!A IPAI' PFI.T: IA USSR BOGOMOLINYY, iE. B., et al., Yadernaya Fizika, Vol 16, 'No 1, Jul 72, pp 129-1~2 2P and with'the necessity for compensating for it with a high degree of accuracy. Experimental observation of the anomal ous muon-pion I was complicated-by two circumstances. the smallness of-the ancmalcus (_,() 34 cm2) cross section and the large ~value of the dross sections for background processes which exceed thelanopalous pracesses~bv a factor of 10-1000. Elastic backscattering of the P-meson~by a.proton at an energy of 1v1 Gev, measurement of (g - 2) of the P-meson, and a ~s.-tlidy ofithe VP -), )1PTT 0 process at E,, > 10 Gev are recoliTil ended as.tbe nost sensitive methods for observing this interact-1 .11~,1(2y) on. It. is" proposed itat T is X-2p compensated not by the contribution of the 3Ti'intcmediatl~e state but by the contribution of other intermediate states arising in KO p+11-: decay, such L as 21ry. A discussion of the consequences of possible 27T~_- 2ji-anomalous interaction will be the subject of a.later,paper. 78 .91 lull -17- USSR TJDC 539.12.01 -`DOLGOV. A. D., ZATU&ROV, V. I.? and.OM', L. B*.~ IlKi~ 2~A Decay" Moscow, Uspekhi FiZicheskikh Nsuk, Vol 107, No 4* 1972, pi) 537-557 Abstract: This paper is in the~nature of a review of the vexatious problem of the decay of the XT meson. There has been a great deal of contradictory experimental and.theoretical data concerning this problem, and the authors review the experimenta1and theoretical evidence thorouChly, questioning it as they Co. They que.-,tion the reliability of the experimental findings -- some. of -Which have led to the negative result that no decay wasc detected -- and apply equally radical examination to the re-liability of tho various theories. 1, -fter this introductory discussion,,the authors examine a mathematical exDression of the decay,..as found'from a hiZh-ly ac- curate exreriment, and consider its conrequences. Then, to plot an exact path through this confusion of doubtful facts and erratic U theory, they carefully analyze the ne~. interactiens of Imown par- ticles arising from the decay, the new particles~and particularly the new light particles that have been found, and the theory of conservation as applied to the decay,in addition~to apparent vio- lations of the theory. In discussing this last, the authors touch 112 HAMM .7 VSSR 4 ~DOLGOV, A D et al, UsDekhi -Fizicheskikh: Nauk, vol 107, No 24, -:AM pp 537-557 on the unitarity condition, through which a limitation on the probability of the KI, --). pc~ decay,is obtained. t,,ith re-ard to the question of the existence of new decay particles, they review the basic limiting conditions such new particles must satisfy. .-Finally, in their efforts to vprify the apparent contradictions to classical physics theory, they:reconsider the mathematical decay expression. already mentioned for an eiamination of the 'theoretical -principles on which it is based. They conclude by thanking Ye. B. BoigomalInyy, G. V. Grigoryan, 11. N. Nikolayev, M. V. Terentlyev, M. A..Shifman, and M. Zh. Shmatikov, colleagues who helped clarify y problems as well as V. B. Berestetskiy, B. _,J. Ioffe, I. Yu. an or Kobzarev M. S. Marinov, S. G. Natinyan, B. 14. Pontelcorvo, I. V. 'he ~Chuvilo I S Shapiro, and Ye. P. Shabalin for having read review: and for the ir useful comments on it. In an appendix, they mathematically develop the contribution of the -two-photon state to .-the.- absorptive part of the K2.---~214- decay amplitude, and the uni- ity-~condition as applied to XL meson decays. 2/ 93 11 1 ET!.::A iE N; PLi lmll 1! Ul 111134 flill i WIM'NA Mli P. Ill I 1110 liJI i I I MP9; I A tilt vA 113u t I Mlmt Il-If I Jim- USSR uDc 541.671547-341 ZArURROV, V. I.. BELOV. YU. V., IONIN, B. I., and PETROY A. A., LeninZrad Imeni Lensovat "Study of the Spin-Apin Coupling in Fluoroanhydrides of Phosphoric Acids by the Method of Double and Triple Nualtar Magnetic Resonanoo Moscow, Doklady Akademil. flauk SSSR, Val 209, No 6, Apr 73, pp 1343-1346 Abstracti Analysis of double and triple resonance spectra tras carried out by the method of subspectras selective exposure,to a high frequency field H2 of one of the subspectra In the resonance of the nucleus X leads to the merging of resonance lines of other nuclei in the same subapeotrwi, For e=ple, in the spectxvm of the difluoroanhydrlide ofmothanephosphonio acido when the low frequency subspectrun p3l in expoobd to high fr6quency fieldj the high frequency lines of the 1 1 Wplets H morget and ponverselyl:when the high frequency subspectrum. P-P- Is exposed, the low f:requency H~,tripjet lines become serged. It follows from this that the constants H-,F and F-P have the opposite aigns, tho conatant Wing ponitiveo To perform sWlar analy sis In case of the 2-chloro-X-propene-1-phosphonic aeld di-Cluoride, it is neceseary *,to solva the spin-spin coupling of the ethylone proton with the protons of the methyl group# that is under conditions of triple resonance. USSR UDO 666.266-52 DOTSENKO, A. V. and ZAKHAROV, V. K., and TSEKIIONOYIY, V. A., Candidate of Sciences "Determination of the Constants of the Relaxation Process in Photochrome Glass" Leningrad, Optiko-14ekhanicheskaya Promyshlonnost', No li, Nov 73, pp 2-9-31 Abstract: There is conducted a brief critical discussion of vorks dealinrr 0 with investigation of the relaxation mechanisms in photochrome glass, that is to say,.parameters of the relaxation process, the values of' which do not depend upon the conditions of exposure, but are functions.only of the conposi- tion of the glass and of the temperature at which decolarizat-ion takes place. An expression is proposed, which describe& the process oX destruction of the color centers. The constants of the relaxation procesa 6.re found, and an investigation is made of the relationship of the relaxation canstants to the wave length of the control beam. 1 figurei 4 tables. 7 references. -~5(47) USSR ubc 629 ?P1. o14t 5 BALAYFV, N. F., GROD.-OVSKIY. G. L. , DANILOV, Yu. 1. V KRAVTISEV, N. F., KIRIMMI, R. N., MAROV, fil. Ya., MORO NIKITINO V. Ye., PHROV, S. P, PETUNI14, A. N., UTKIN, V. PO., and SHVIDKOVSKIY, Ye. G. "Scientific Data on the Flight of Automatic Ionospheric "Yantar" Laboratories" Uch. zap. Tsentr. Aerogidrodinam., in-ta (Scientific Notes of the Central Aerohydrodynaric. Institute),19'?l. Vol 2, No 2, T)P 56-65 (from Referqtivnyy Zhurnal Raketdstroyeniye, 'No 11, Nov ?1, Abstract 11.4-1.87 Resune): Atstract: Launches of automatic ionosnheric "Yantar' laboratories with gaseous plasna--4cnic enpines ua to.100-400 kn altitudss i,,,ere conducted with the ai~ of geophysicn~l rockets, for the purpose of studying prospect-s of controlled fli!!~ht, in v-Pper layers of the atTrosphere.Performance of gaseous plasma-Ionic enFlnes under iono- soheric conditions was studied. Parameters ch-iracterisinp- thp ion jet-ionosoheric T)Iq.sna interaction, Ps wO.1, ris P?-I-Im-ters of neutral atmosnhere were r9ensurpd, Scientific on conducted ex- Bros -Re iment-~s is presentpd. P flrures:, I t~able, 11 r-iflerences. USSR UDC 619.611.9-022.6 4- 636.1+ 636.24- 636.44- 636-52/.58 WIMFRIYEV, V. XF D 'UD N, I YK OV, A . IIMAMV, V. K.;, 'STIVETSOV.. YIX, _ F-. ;C.IIMTAYEV, Yu. V.; KRAVCHENIKO, V. M.; ~'R I. A.; NIKITIN, A. Y. "Diatelic imnunization of Cows with Foot-and-Mouth Disease and ~Prospects for Obtaining L-m-aune 11ilk" Iou'h Disease Val 1 -- Vladuiir, V sb. Yazhchur. T. 1 (Foot-and-M Collection of 'JoTk~s, 1~970, ~P-D 160-172 (from RE)i-56. -hivotno- vodstvo i Nlo Apr 71, Abstract~ No 1~. "i" I 0-~7-3) Translation: Diatelic imnunization of cows ijith f oot-and-mouth U -'h a disease anuibodies zirovides lactoserm and Lmmunolac tone wit high concentration of foot-and-mouth disease.antibodies. q--'he foot-and-nouth disease -* unolactone, has pronounced ureventive properties in research -,rith baby nice, guinea. :pigs, bull calves, and suckling pigs. Polyvalent foot" and-mou th disease im-mu-no- -one has a more prorouriced.virtis-neutralizing aotivity wit act l respect to heterologous strains.of f6ot-and-mouth disease virus 112 - --- 92 IN MINOT MUTIM-974M MINFIMM MORM ril mm MIMIM-31M INIVI'm M-MOU SMI'm 4 USSR ONUFRIYEIRV, V. P,; nt al, V sb. Yashchur. T. -1, ~1970, pp 160-172 than the monovalent one, The high specific activity of the foot-and-mouth disease lactona, obt ined under biological -pro- ai duction. conditions by immunization of cows with inactivated foot-and-mouth diSease virus, indicates a promising use of the diatelic immunization method under industrial.conditions. 2 12 T -? IJSSR UDC 536.46+662.311 ZAMWOV V. f1,, and KLYACIIKO, L. A. "C'n ernin the Combustion Rate of a Model Gunpowder Mixture" 0 c 9 Novosibirsk, Fizika Goreniya i Vzryva, No 1, 1972, pp 15 26 Abstract- This paper deals with the combustion 5cheme of a model 2-component. gunpowder mixture, consisting of finely divided potassiuia nitrate and charcoal. it is found that the position of the concentration limits of the combustion of a model gunpm-7der mixture is detennined by the temperatu're equality of the combustion products within the zone of influence of the J.Pnition temperature a of the mixture, namely the temperature of the transition of pot, ssium nitrate into nitrite (Tf 111,000 K). Increased pressure, increase.:; the combustion rate, as does also an Increase of the initial gunpow(lar temperiature, An opinion is given with regard to the heratofore uneyplained influenc(-,~of thc-~ addition of sulfur upon the combustion rate of smoke powders. The combustion raLe is said to increase due to the formation of.K2S.in~the combusLioa:products, instead of K20,, thus releasing approximately A0% more~heat and,liberating. more oxygen for oxidation of the charcoal. 5 figures, 18 references. USSR UM 669-157:669.15-194-56 GOLIDSHTMT M.-I.9 DEINISOVAI, I. K., ZAKHAROVJ'~ V* P_4- p and KOPYLOVA, VO, A.,, Ural Polytechnic Institute imeni S. 14. Kirov "Change of the Fine Structure of Heat-Resistant Austenitic Steel During Aging" Sverdlovsk, Fizika Metallov i Metallovedeniyeg Vol 369 No 4, ~~.Oct 731, pp 742-746 Abstract: An experimental s"Cudy was made of fine structure changes of three melts ft - containing Mo,, V, and Nbj 2 - not containing 11o and Nb, band 3 - not containing Yo, V,, and Nb) of E1481 austenitic heat-resistant.steel in the pro- cess of aging. The results are discussed by reference to dia- ams showing the changes in vridth of-the interferential line U F3 )cK, of. the austenite, the blocks and micro di,9t ortion s 9'he density of dislocations, and of the lattice parameter. The fine austenitic structure of.steel alloyed with Mo. V, and Nb (melt 1) -41 ds -rili- W I ~Jll ill HdP;OHIJAM~ i"PI19 13 It lo I it it I ~,kl im ivil imi ~,mioy im:m MIME 111r, USSR GOLTSHTEYNt M. I., et al., Fizika hatallov IMotallovedeniye, Vol 36, No 4, Oct 73v pp 742-746 and alloyed with only V (melt 2) were foun'd to undergo conside- rable, changes during ar ushing of. blocks ,aid a gro-aing ging, a cr of microdistortions and of the density of dislocations take place These changes in the structure of the matrix are accom- paniea by a considerable enlargement of interforential lines and by a Change of the lattice parameter. The discussed changesof the fine structure of 'he matrix together with the.influence of U the very dispersion particles resul t in a considerable strength- eningof steel in the process of dispersion hardening. Five figu- res, one table, ten biblio aphic refe-rences.~ 9r It r9 Jig 14.11FYI SPIN USSR, UDC 577.4 ZAKHAROV, V. N. "A Method for Minimizing Se~uential Descriptions of Automatons" Yloscow,V sb. Ekon.-mat. metody i programmir. plan.-ekon. zadach (Economic-l-lathematical Methods and Plan-Economy: Programming--- collection of works) 1972, pp 103-113 (.from RZh-Hatematika, Ho 12, 1972, Abstract No 12V245) Translation: A finite automaton in the form of sequences is con- sidered in RZhMat, 1972, SV440. In-its;.simplest case, the sequence has the Corm xtst ~- st+lt where xt is Ithe i put',symbol at the-mo- in ment t, and st and st are states at laoments.tiand t+1. A method for the. maximum posside reduction in ;the- niimbber.of sequences spe- cifying the automaton is described.~~.V..Shevyak6v =Ups USSR UDC: 681.2.063:531-767 913:531-766 BARBAS, I. G., ZP N. . ITIN. 14. Ye. , KRUTIKOV, I. A. "Use of Semiconductor Strain Gauges.for Measuring Accelerations" Materialy Yubilen~ nauchno-tekhn. konferentsii DneRro-j1.ei!tr. in-ta inzh. Zh.-d. transp. (Materi'als of the juJbilee Scientific and 'Technical Conference of the Dnepropetrovsk inst-L rs U.*tute of Railway Transport atio n En-inee ), Dzepropetrovsk, 1970, p 266 (from RM-Metroloaiya i lzmeritellnaya Teklinika, No 11, Nov 70, Abstract 11 o 11.32.448) Translation: The authors present the design and cons truction of an accel- eration pickup in which semconductor strain-gauge resistors were used as -'~~e sensing elements. The pickup canbe used to measure the acceleration of processes with frequencies ranging from 0 toi2OO amplLtudec of up to 50 g (g is the acceleration due*to gravity). Conl3i 4~eration Is givc-n to the possibility of introducing critical danTing of the elastic element of the pickup by various =Qthods, as well-as using electrical damping in the am-pli- fl-cation che-nnels. The suitability of the: given pickup' for neasurJ ng accel- erations of the various elements of rollifig, stock was checked ou-, on test runa. USSR UDC 577.4 V- 19. "A Procedure for Minimizing a Sequential Desc.ription of' Autdriata" V sb. Ekon.-mat. metody i programmir. plan.-ekon. zadach (Mathematical Economic Mfos- Methods and Progran=ing Economic Planning Problems-collection of works), 1 cow, 1972, pp 103-113 (from RZh-Kiberneti ka, V lo 12, Dec:72, Abstract No 12V245) Translation: The assignment of a finite automaton in the form of sequences is investigated, for example, in M-111atemat ika- 197Z, MO. In the simplest case.the sequence has the form xts 1-.3 +,,WVLere xt is thc input symbol at the time t, St and st+l are the states at the times t and t,:+ 1. The procedure for maximum.possible decrease in the number of iv4ng the automaton sequences g is described.. Thin Filst6 USSR UDC: 539,.216.2:536.42 ZAKHAROV, V. P., ZALIVA, V. 1. "Phase Transition from Amorphous State to Polyerystal in '11iin Films of C, Si. Ge, GeSe and GeTe and its Influence on~Conductivity and Optical Density" Moscow, Neorganicheskiye Materialy, Vol 9, No B. Aug 73, pp 132S-1329. Abstract; This work studies certain regularities of the phase transition from the amorphous state to the polycrystalline state in thin films of C, Si, Ge, GeSe and GeTe and the influence of this transition on conductivity and optical occurs underthe experimental conditions properties. The phase tr, (films 10-5 cm thick, prepared by vacuum sputtering onto unheated glass sub- strates and transferred to capron holders,.transition StiMLIlated by the power- ful light pulse of a gas discharge tube) inisuch a way as to indicate the qual- itative.identity of the conversion in all.of the substances tested. The threshold energy required to stimulate the transition indicates that the amorphous state is relatively stable in these compounds.. The transition changes the conductivity, optical reflection spectra, transmission spectra and.integral optical density of the films. 1/1 x USSR UDC 535.44:621.378 BEIVICRINITSKIY, N. S., GNATOVSKIY, A. V., D TILEYKO, N. V., ZAIMROV, V. P., and SHPAK, M. T. "Holographic Recording of Information on Amorphous Semiconductor Films" Leningrad, Doklady Akademii Nauk SSSR, Vol 209, No 2, 1973, pp 330-332 Abstract: This paper is a report on the:application of local variations in the structural and optical characteristics of InSb, InSe, InTe, GaTe, GeTe, and Te for holographic information recording. In an earlier paper (N. S. Belokrinitskiy, et al, Pis'ma v METF, 15~ No 4, 1972, p, 198) it was found that in GeTe films under strong light pulece a growth of crystallites was observed, accompanied by changes in the physical and optical characteristics of the compound. Similar characteristics, including tlie transmission and absorption spectra, were explored in thepresent paper for the compounds listed above. The equipment used for the holographic recording is shown in schprAtic form. Records of objects measuring 2X2 mmz to 15X15 mm2 were made by illuminating them directly with neodymium and ruby lasers. Samples of the images obtained are shown. The authors thank V. N. Pavlyuk for running the experiment. USSR ZAKRALROV V. P. GMMIMENKO, V. S. KUCIWE ENKO, L. P~ "Optical Phonons in Amorphous Arsenic Chalcogenide Films" Leningrad, Fizika Tverdogo Tela, Vol 14, No 8, Aug 723 pp 2466-2h68 Abstract: An investigation is made of the vibrational spectrum of binary mixtures of arsenic chalcogenides of various:compositions in the form of amorphous thin films produced by-thermaldeposition in a vacuum. A study of the infrared transmission spectra of AspS3 and AS2SEi3 showed the ab- sorption bands typical of.these substances:in the crystal state for AS2S3 and-in the vitreous state for AS2Se3. No,absorption band was observed in the 400-33 cm-1 frequency interval in the IR-spectrum.bf thin films of AS2Te~. An examination of the transmission spectra of mixtures of As2(SxSel-X)3 and A52(SxTel-x)3 deposited from suspensions of various compositions showed that the presence of atoms of heavier c~alcogenides in the mixture changes the relative intensity of the bands of the As7S3 opectrum. When selenium is introduced into the. films,;the nofit notice- We chELnga in observed for the lov-.frequoncylarid, ane4 the.center of gravity of the entire absorption band for As 3 is displaced toward the 27S 1/2 IT, ",l USSR ZAKHAROV, V. P., Fizika Tverdogo Tela, Vol 14, No.8, Alig 72, pp 2466-2468 high-frequency region, occupying a position defined by two stable bands in the As2S3 spectrum. The relative intensity of the ks2Se3 absorption band. increases with an increase in its content in the film, md a slight displacement is observed in the position.of the band makimum toward the low-frequency region of the spectrum. It is concluded that the solubility of As2S3 and As2Se3 in chalcogenide mixtures is higher than that of AS2Te3- 2/2 IM mom 'MMOMWE" H USSR UDC: 621-315-592 ZALIVA, V. I. and ZAjqL&RQy, V. P. "Physical Nature of the Switching Effects in Amorphous Semicon- ductors" Leningrad, Fizika i tekhnika poluprovodnikov, No 7, 1972, pp 1252-1255 Abstract: This paper describes comparative experiments in the in- vestigation of kinetics of the phase transition from the amorphous state to the polycrystal Paid of the switching effects and "memory" in amorphous GeTe films. The purpose of these experinents is to clarify the physical nature of.thereversible switching effect. Such effects were observed in films of such materials as Ge-Si-As- Te compounds and in stoichiometric GeTe,.all of.them amorphous. Also.investigated was the thermally stimulated crys a.1lization of amorphous GeTe with an electric field of up to 4. '0 V/cm in in- tensity applied to the substance.. The effect of this experiment was negative, with the applied electric field having no influence in the kinetics of crystallization. :The authorr, find that the physical nature of phaae trannformatione ia univorsal, and that tl4ey are connected with the f ormatiorl of I'memory". irl simorphous J/ "), - USSR ZALIVA, V. I., et al, Fizika i tekhnika.poluprovodnikov, No 7, 1972, pp 1252-1255 GeTe and with its crystallization under the action of rapid heating by powerful light pulsep. They find:also.that the growth of crys- tals measuring 10-'+-10-" cm. and taking the form of threads causes the.memory effect and occurs in a time of the order of 10-~ to corresponding to the experimentally determined time m for the formation of the me ory. 2/2 13 6 &-77-3- XVI-S. VIFNAT (24 OP nit: FILM SITEWTURE OF CLR'IAIN SF.'fI=d)UCTU1S IN ThL CASL OF L&SL)k Ut.PXr;,ItC*i (IF SPECIMENS lArticle by Yu. r. roizavtacv, v. P. znkk~^rov, I. t .,:rqtzu;, 1,Aclr. th~ulhlrjj~., 'at ii Pox ov I Plenok, Kusotan. 12-1) June' Ti7i.--j-2i? I hljFlk v4por pfitsouraw freijurntly.c"~illt ~"A za of, t.1chl-aceld tfl"691tion. beflnite rrvr.T"* booo be#n euda in chill direction In the presence, of laser 41, po%itAon of tile 940--Afs. Owl GlIttleate ." W..d. f tfle role of rhn~=ltcv of;b- _vano :=oA tile Interstomir iliter- ral4tt,,na Wt-h this tyP4 oU dapn4ttlon for the process nf fomati" of n-r- rhous film qtructurl,4 an A Ftlass substrate. Ille research subjects ere Sc.1- cond ,tors of the AilIEV and Y.03VI *typ" The molecular compatition of t1te vapor was ln~patjjatcd "a-ope0tro"trl,c4t%v; the structure of the deorphu,.. fil" W" InveatialAt .ed ily the me tfi6d'ofAiiterra1 analysis oVithe-olectran acnt- torinr. tntrtvott~ cur--*. 1 It Is established that the C&M varor contAl". tonized and neutral co~ 'Plates co"risins atolex of the name and difrvcent typss. and the strutture of v wolldsc~rLbed by tit.nnael of the net of 41.ar,-r".d the amorrho crj%r4jq, In C-ty-.0 t. to thin. in car Vapor emepleres of.iftoffla (,( lifferent tye. sr~ cn"J~.t-jy absent, Iand In tht&jorrhows filo.t.nicture In addition to in# "c rvatal - Ilkp." rep tons there ere rorkens containing StO161 of ot%t- t~pq with the structure of, amailihouu, itall1u, rz,r A&,S3. AxjSe3 end AnSt, tho ~Iec-jlAr coapoultion of the vnror turned ntst to be 4l.tlAf .11fteAll the &tructure of thr amorphoun fil- WA, dirferent. I'liun. for exAmle, In Off A* l r filcia the wilue of tile radLoy of Z 3 the fLrot coor4loation xphere and the Laordination numbers are tile onme as in tile crystal, And in the A.- 2 Se3 filbo they are appreciably less. Tile result* obtained have permitted evaluatLan Of tht effect of tile molecular vapor composition on the processes f the formation of the fLI structures of tbe inveatigated substances. A destrirtlon in given for th~ probable, kinetics for 9 he formation of cke file istcucturd. 1.31 - MIR 2 UDC 54- 544/661 . . T. OV, A R t o if.,-or c:` Tashkent, Kh-i-Inl~-,% Priro -14 p Abstract: A Pei: I z 1*1,:V~:_'.,Y~:~,-:~! f,c)", of Ll"'iVAIL11 lmabasi .~ :~-z-"._ i c ex" rac- u r, or fa !:T, -JIjO n,- L; by convc--~Ld~- ','I. c: L_ for y-ro- 4i J, lz ~3111 P . 1 to cb-AF.~-Icrabl c o' the ~t 1 k - I - - , " - ; .: r o. i 21:0Of t Ilita i~se c by SK '0, M. BEIDIMINITS, IY, H. S., CITATOVSXIY, A. V. DANILEYI, 'KOZWVI A. Yt, and SHFAK, H. T., Physics lnltituto, Academy of Seim, cas _._Uktainlaz SSR necording of'Optical Information on Amorphous Filins of Slerdeonducting Com- ds. 11V H6scowpTisIma. v Zhurnal Eksperimentallnoy i Teoreticheskoy ftzikl, Vol 15, i19 -200 Be' 20 FW72, pp~ 8 Abstracts The article descrites a nev optical inf -oxmtion method based on local variations. in structural and~optical. characteristics of some- somiconduct- ing comipoufi6: uader the action oft laser: radlation. Thlo opens up the possibil- -4 of creating.caarriers sritJi a high. recording speed (10 -.10-L) Sec) and high spatW -resolution. without the. need for: subaequwit pMeeasing. Am- )Thour, GeTa .1nSb filmal vacuu.-ii-evaporated. on glass and NaCI w3lx3trati3s, wero uscd by the-authors an cu c, Sipal x1ern for opti al ar alat on by a -recoxdIng. L er ra i vamit.ranspaxent mirror wan soparated into tito bews approxinitely equa.1 An intensity.and directed at the samplo.at.,a Convergence.0gla of 55 for G.-_Te 313 USSR BEWMNIVSKIY, N. S., et al., Pisima v Zhurnal Nksperimental'noy I Teoreti- 5, No 4, 20 Fe 72, PP-198-200 cheskoy Fiziki, Vol I b and 250 for InSb, The interforeence holograia grating of thn radi,ation field was recorded on the film. Samples vere exTosed to radSation pulses of a free- rtmning ruby ( A = 0.69 micron) and neodymiwn ( A - 1.06 nica-cals) laser, Given a sufficiently hornogeneous laser field amplitude distrIbution, interference gratings with a spatial frequency of, up to 1000 lines/im wcm-vs obtained, repre- senting alternating segments itith different spectral ancl structuxal pivperties. There was found. to be a relation betweon:the sample piv,-pu-ation conditions and the rAximiLm attainable spatial frequency$ There are optilaal, radiation oner- gies . for the pulse-mode recoiding of gratings (e.g., - 0. 1 j/sq mm for record- ing on Wre ftlnz Ath pulsed noodymium laser, radiation~ - 500 ricroseconds in duration). The authors observed two forms of film ztructural changes accompany- ing the information recordingo dependirg.on the density,of the reco,_-dod grating. ~,S of ~ 1 W-200 lines/lrura, the In Lthe recording of grating Ath a spatial frequency lines represent bands of polycrystallinepaterialp fllmu,in an Waorphous state divided in segmentse In the recording of. gratings with! a spatial frequency of 2/3 Uj W USSR BEWKMIITSKIY, N. S., et al. Pissina vZhuxral I~tsperiinentallnoy i Teoreti- cheskoy Fizi U-, Vol 15, Ho 4, 20 Feb 72, pp 198-200 -1000 lines/r-112 grain enlargment is observel over the entire area of -"he film segment being treatcd vith lizzin.ous radiation, but the optical density of the interference grating lines differs, making it possible to obtain a grating with sufficient efficiency in this case as -well. e- Wor"k, is continuing on the fixther kinetic atudy of Thai anorphou-9 stat polycrystal phaze t =,sition of the above-indAcated imtorials and a number of others, as well as. the study of their- use as 'carriers for rer*-rding Info-tma- tion in the visible and 1R region of the zpectrumo The authors thank V. So SAMOYLOV for,useful disaim;siow of the results. 3/3 Naomi UDC 621. 378. 335 P. PROTAS ZAMIPOV V. I M. TIJ V 1111ass-Spectrometric Study of the Evaporation of Type A" B Semiconductor Compounds by Laser Emission" Leningrad, Zhurnal Telhniclieskoy Fiziki, Vol XLII, No 3, 1972, pp 670-672 Abstract: Mass-spectrometric studies of vapor composition were performed dur- evaporation of single GaAs and Gall, crystals by ruby laser emission. The qualitative composition of the vapor in both cases was similar (the Ga , ~s and As ions for GaAs predominate, and the Ga+, P :P, for GaP) ; however, 2 the relative intensity distribution between them io nal: retained. The pre- dominant composition of the. part of the vapor hot ionii:ed by the Ifiser emission was established by using additional ionization of the vapor:by a high frequency spark. The causes of the quantitative differences in the vapor during e-vapora- tion of single GnAs and GaP crystals, by xuby lasar emissioa were discussed. The results were co--,.q)ared with analogous rn~ults for therinal evancration. In the case of additional ionization of the plasma, the A; As an(.' Ga. 11 ratios found from the mass spectra approach stoichiometric. Thus, the devree of ionization of Ga during evaporation by laser. eiiiission is appreciably hi~,Iier than for thermal evaporation, and the part of the vapor ionized by the liglat 112 , - .Midlil I ~ I Eli; 1 i ~' " I k' i 16' 1 L ~ ~ ~ ~' ' . ~ - ' ' i -- , -- - , , ' , L ~ , ~, 4;, .4 R; ;;irml I , , !I ,1 ~ , - " - I ~Q I ~ i~ 1~ .:-:,~ ~ ~, ~ . .: ', j-L- I . j ~-- I a ~.- ~ 1 7 1. ~ ~t --j~ .. - ~ -1 . i I!-- , I ~ 7j i - ; t i " !~, 11 .4 1 j:1 -I ij : I-, I- . . i~ I i 11 , , ~4 ~ F I I 1~ 6 1 ; e ; -A I t,i !; z: ! . i I I . ;!. I I ~ . .j 1 :1 ' i .~ ~ ~ ; j , , ; j , ~ , , , : ~ , j ', . ~j . , L' . . 11 ~ -, , . ' -' ~ i I j, , 4 , - Z .; L. ~ ~, . ~j, , , , ., UMF548 5,2 1 USSR, POLTAVTSEV, Yu. G, ZAKIIAROV V. P., CHUGAYEV, V. N.: "Structural Studies of Graphitization of Tliin,Carbon Films Under the Influence ~6f-Powerful Light Pulses" Moscow, Kristallografiya, Vol. 16, No. 2, 1971, pp 41S-419. t1stract: Changes in near order structure upon graphitization of carbon films under the influence of powerful light pulses are studied:. Amorphous carbon films were irradiated with light pulses of various energies, the process of graphitization being continued to various.stages. The intensities of scatter- ing of electrons by the irradiated films were -measured, and tLe curves of t,;i-- radial distribution of atoms were calculated, :The near order parameters were determined for various stages of graphitization. A probable kinetics is suggested for the transition of amorphous carbon to gra hite upon irradiation P of the initial films with light pulses of very high enorgy. It is suggested that a double C C bond is produced;betwben'some of thet ~atoips in addition tolthe single. C C bond in the graphitiz.ed films. US3R UDG~539-216-2:535.211 ZAKHAROV,_YA_P., POT ISKIY, M M.,, and CHUGAYEV, V. N. (Kiev) "Kinetics of Structural Changes in Thin Films, of Germanium and Carbon During Their Interaction With Laser Radiat;ionll Moscow, Fizika i Khimiya Obrabotki Materialov, No 5, Sep--Oct 70, pp 55-60 'Abstract: The article describes results of a study of the process of crystal growth in thin germanium films.during their interaction with laser radiation. An FLU-31 photymultiplier was used as tne recording deviceo The germanium films were obtained by evaporation in a vacuum of the. Order Of 5-.10-6,mm HF, on cold glass substrates. Tne interaction of tain gdrmaniumi films with focused laser radiation results imthe growth of single crystals within individual cells of the supporting grid on w;iich the film was Placed, I'he crystals reacned' 15-20 inicroas in length. Os-- cillograms disclosed a difference in,the duration Uf Ctlaflt;e3 in the optical density of the films. wnen- thoy we:re irradiatod. with laser radiation in air or.in a vacuum. Since.charkeies in the -1/3 69 USSR ZAKHAROV, V. P., et al., Fizika i Khimiya Obrabotki Materialov, N o5, Sep-Oct 70, PP 55-60 optical density of germanium film~in a vacuum ber-in following ~on, it m*ay be considered the completion of the laserpulse -act that the single crystals.grow in the film as it cools off The temperature for the start of-single-crystal gr(:w_-h:is strictly determined. In air the appearance:of significant temperature er rate of sinirle- gradients determines a aigh crystal growth in the films r-nan under vacuum conditions. Crystal g owth within diflCerent cells Lakes place sequentially as them film crystalli- d du-in coolinr. c. The. use of the temperature is reac~fte 9 photomultiplier makes it possible to estimate~mcan crystal growth rates. For 15-20-micron singlecrystalz the mean rate of JOL their growth in the film is of.the order of :_M/sec. The same metnod was used to study t~,e t1n, e characteris- tics of the graphitiza~wion of carbon film in its interaction with a laser pulse. Unlike germanium f ilms, where- ordering of the microstructure occurs during their coolingp~.caroon films are V.