SCIENTIFIC ABSTRACT KORSUNSKIY, M.I. - KORSUNSKIY, M.I.

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CIA-RDP86-00513R000825010010-4
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December 31, 1967
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SCIENTIFIC ABSTRACT
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oom for 0 oft Sep 04P 009 ago 00' 90* 0*1 00. ff. 0-9 -to"ll va"Isse poll maps p a #I a 4 a a I A-- lit 66~1- it t: 4 T pug m6" om~ po uniss" 9 21 MUIW no PO *s 'SWIM I supoxv ~R*nmv I"Vdo aq, 4-41 uma" q 11 Alma "qvp" lo uiolq MUS32P XPI'Volu V-'"&FfmM 0#1 -mv pits, 4try Its if 'XismIrl 'A -mem" WAAPGP ~me 'NVIIIIAM 'A 000 go C. 00 99 00 R00 00 00 go 00 ell" i.7 of so 141,4c) r V 11-1-1 4 A m T -H w -T-j U- I 0 0 099 0 KORSUNSKIJ' K. I. 104. Discharve tube for se v"olta ~ee up to .1700 000 V. A. -SINC-MAINN, SUNSKIYEk. So SUNSKIIF M, NEKRASO ~A. J. Techn. Phys. U.S.S.R., 9j 10s PP. 883-889, 1939. In Russian. - Using Lange and Brasch's idea of erecting a tube of discs the authors employed discs of micalex and steel alternately. By pasting the discs together with an insulating varnish it becomes possible to erect a monolithic tube of sufficiently good electric and vacuum-sealing qualities. It was shown that the sparking distance in air of a valve designed for a certain impulse voltage depends on the form of the electrodes. These latter being of a suitable size the length of the tube is only determined by the breakdown strength of the air. Thus a tube with 2 m. between electrodes of the Rogowski type will stand an impulse voltage of 2 700 000 V if there is no gas discharge within the tube., A gas discharge spoils the potential distribution in the tube and causes vurface leakages covering portions comprising several elements of the tube. F.B.K, log *****: :::::1 00 00000* Ill 0000000 a 0000000000*0 0:40 oe 00 0460000 c 0 ff C -4 x L Y- w I A A U a it 0 It U 0 0 * 41 U A) I f If Of AT IS I'l - , '!~~ - go I 0 0 o - *or 4101AWN411013 11414rdsill UNIA1111ILS. 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T. d uc heess f the jcwmtjoR of k)us comhtimus Is- "amiaw of Ptopongm that the to imim"m by Oka-" 'a a sm at "ct, - ties, P&tb 01 "W obet" is > dw didanco b"Is the okctinglow T1, 6 Qi t1w imic current on PCA-tiAl so tooltIA1. bmft nitincti. memo ed 00 - cat Nat is empikated: there The I a" ".m is poaible to Itat a m above Which it 0.3 o '3 19,01, mooWlIbmthood of thil tho MY wr 6" cugjmL Is the I very and". Thefts Jig an oarillatorv bcftmw bovem the alecoodes. With SufftIsfe an oil 0 * ~' t M 0 great that the is I r jow spogjaw per 46fttfm is > 1. A. J-M- 20.04 t - - U IS As PC 157, it slip "0000411 pilots 0 0 0 0 Is 0 * 0 0 0 0 0 0 0 0 0 0 0 0 010 0 * 0 0 0 * 0 0 0 0 0 0 0 a 4 N 0 1 OF f1 7 a 4 2 0 9 lie A I St 0 a 9 9 0 0 -00 -00 coo off roe at* 41 use 1 3 4 1 It I I I is 11 12 13 w is 16 to is 0 a 0 10 a jolt J)" up WMAIIIII IN 41 u 41 4d m 0 tax . m OA a . A OKI A-a _t_ _j -L L 4 k f I.- I A_J_ PlIKIIIIIIII &no Pseptollfs INCIfo Null. maj. k -00 C. A. 34, MN . 004 U-wo b u 0 AV SID All; 0 00 0 0 0 0 0 0 0 0 AD no age wee 1_4~kle 0 *0 e .9 w 0 AD 01 F 0 0 0 0 0 0 0 0 0 0 0 a 4 0 0 0 0 0 111 000 0 0 0 0 4 02 1 4 1 4 m 02 it it it w is ad it As to a it a n m a it n it A, r, it at if 1, is m 11 At " C 'I it of* A * I I V V , a "o 0 A T - 1 00 0 0 0 1 0 1 . 0 0 . - - . go f ftwartift 4d bw ink gime"Ift. 1. V. S. M. 1. KormaumiskV and F. F. LAW - ' S Pk U S R ) 10 . J. &P0. rhWillf. 1l h T A -00 0 0 . . . . yt. ( , e ma ut L-- U "I- -Qe . s w1opanewmetbodfarthepuffucti Th t k M on Ic Ms. on W r F nt the well. to c i -00 sea t ou ac a e n ey known fact that the lmiAiug pruptfty of clectrains depenik .00 fm the emrW and In cirrisin realont has art upthimin value. It It large IVO- 44 IFICCUOSIS rMill"Wifif thk knit ilukull VAILI-if -00 energy carrier a, covividirtable di-.tancr. fargir imi' %lumfulk 0 it v can be obtained. The lamnic fwainki obtai"A"I by fills anothurl we rstb*r brand, but can be foomd by olvaul lif 000 ion-oplic eyiKirmits, Larger Ionic currents ran 1w olplAit-eqI l A ice* er munounti t them to dw previnew wedoft. with tarmi of j valf'ray. For imimmusce. the Ionic current #4 ILI) Ina. tkvds :ice* 00 om~y to W. koksalmin a Gatuov zoo 00 -a 00 00 0 0 - 0 aso-ILA SETALLURCKALLITIRATL*ECLASIWKATtOm too _7 %t S.1,1411 .10 GINT off 4s, T-I- W-61 0-3 An 1 0 U 0 IT 0 IT to 0 0 0 * 0 : : 0 of 0000 * 0 0 0 0 0 0 0 6 09 0 0 0 01;0 0 0 00 0000000000* 0*91 ' N a 0 9 0 0 0 0 6 0 0 a r, 0 0 o 0 4 4 * 0 w ~ t o 4 1 1 to It U i is 0 3i ki is Jill units Ill?* a . 1atz. ~.4 1 i AIM. a - 41 Q a a 0 ~a 0 : p - *0 top pirojol o C 1*118, Z01 AllotoWd Value for MUCIOAC OnCitalit.ft tit Ill.. by 1 1011% I korsunskil. F. F. I.Anotir isiml V.S. lih mwl. I III R 5W W. U. N. S. S, 26, An invemigatille of as a function ill carrory tit rlm- produring x-ray%. with curvvit giving The inlrusili-, of %.Iavok n( I-WAI kv, Cut-roly a% a functwo N .4 Ilu. rortily tof 'wA."Ithult Ito 111C 111-1114 " 1 hol imil givillot Mv mlio thl"VY (Cf. 20, %-'ayl tit tatill kv., Showt-Al that NIN) kv. in not thr til". . Thi h i f N '. 't o% ollo 11111,114,14 valut. tit x-ray% rtivilot .N.. hold vulue litust be cutmidershly lowel. In'.1hillf). nem O*j IINX) kv. A, 11, KFAI'lit. emoo ', zoo go a moo of 00 goo 00 ago OOR ago (400 :moo i 390 Noo I.Y of %Igo~0 419 ag'# 0.1 1.00 , -_ .8 _ U I AV so L11; F 4 r Sam 4900000100000*0066060oooooooofo.% 00000000 14 : : : : : oil 0 0 0 so 0 0 0 0 0 4 0 0 0 0 IT 0 1 1 1 M rm R! F " ?~! ! -g w 1 as o On 41 4141 Waif'* " A . a-M.L.8 - A O . -1 . W-4- -1 A .1 1 , I. d .1 b . 4 1 4 1 1 , a I "I so A -011-1.19-01111011 '. 1. it- 1" " 14w ? '60 slil, "'Wra, ra, It III' L I y electronic impaict. go M L~-Kwbm"d, V. it. and .4. 1. lqpkill, d1bad Sasks S S . . . . 111"'itillatlVd tile IS-11VAI b 0 y mam""Mbe"of Approx. 1.0 fit. V. V, 0 Alice 41uwWS lor tile 00 mr atgtl~# -tsw -1--rdet by the ckv- ' 00 11 Itromi jimalit7gavictiptLertraw. G. N1. KUNA.IPUO oil 0 0o oo age 00 we* 11 "0 '1, it a i OF 0 0 0 0 0 0 0 9 0 6 0 16 1 a rw a 0 a I Or ~a a 0 16 0 a 0 0 0 e 0 NOO AD a 3 1 V 0 a 0 0 0 bumd= band im 41% bw dubw bw"L M 1: KW L v F G bo and S. 1. ZIPkin (Contd. read. Acad. ~icl.. ii4i. a 403-406).-Momochromatised electrons (-1-6 Me.V.) bons, two bils of to " cm,) separated by an Al plate (0-03 C_ 1. irb aw second In " Was 0 to r-rays on)), and the 4N 7.0711 11~10c~ i 4CIMUrs oxcitW in the wo foils was measured bv a jj~. ", 17.1h Counter. Irctrom excitation occurs, awl the cfkvtive ctowwcf~m Aw As @I hm Offect is -9 x I" 6q. Cm. W. R. A. Me - ~; KORSUNSKIY; M. 1. "Investigation of 'Bremsatrahlung' by means of the Indium Isomer," Zhur. Eksper. i Teoret. Fiz., 12, No. 1-2~ 1942. Physico-Tech. Inst., Acad. Sci., Kharkov, -1941-. Goo 0 6 a, 0 0 0 0 0 a a a It a a Sao 00 00000*0 of v 111junIA Fri# nx*11 I Didt- 11 1111IM-40 1:0 011 M V NOV 41, QJ - US a a I. IF M r A tr UP Ett , 1 4 0 r_I..& 00 so *6 00 As of by mass W Inscostl 00 SO [Milo M 1. Kurstaxiltif. k. K. Valtef A It is Ivarm, S. 1. Tsophin'-sed V. E. Clatteriko. J. pk,.- 00 11'. H. 8. R.) 7 120-W0110)(in YnOM); d. C. A. 37, ZIMI.-Io & lovesilp" of the Intautity of a 760 A norrvor spectral reginto of Orrmwitraltlung pratfuced by of tam dectrans, the yW cd the metastable nucll of In", was ussOl w 1 11 tor. The threshold roerp for the ex. 00 citotim of The vortoolable mote of InIll W 1417,0 & III) e. kv. This tbrvdwM em a, *equala the energy of the activation *a J!" level. The tes (AV - IMID - W C. iv.) for *0 So the W"Mankhood of decirms frum thick-leaf He mW tMM4stWj6:..9 me./:3. em.) 841 twpto were Investi. 00 pled In relplon Frorrgirt; between IA)4 and 1.5 m. It. v. Pw both pTkiRv of the Intensity tDc--- of f*ctftW agrees wen With the odiw.Heitkr I . The relative It for the purlowfluts no I quantum of 2-Mys in =d As ow"t mie so the upmes of the at. noit, 9. = teso I WM vu ur Fir the probability of emis" of r the thres"I &:=gs energy. and The Values for ve pri"bilitics fit 00 quanta hum fle &W Au targets am at variance with the so rMplo. of Collins OW Wishisn" MW also with Oath's too theory. (Cf. C. A. M, 27W, W780; M I 4MP; SS, 24121: 36,24711.) P. If. Rathinant, 00 A I w S L A OITALLUK~~AL U111114111111 CLASSIFMCA11004 Vz, _-.n so W.. -it -Q-T G., Ill -Aft- W_FW_ -0-4 -_ I V U I A 4 3 4 1 PIP tp to It at 4 a 4 11 9 4 4 0 11 09 IF I its 44 00 0 0 a 0 a 0 0 a 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 a 0 0 0 0 0 "0 0-000*0 goo 000-6 6 GCO609,90 $00064 goo soosio goose 0000000000000000000! 966196009060000.60*00.0000060 got sea a otr 90S 0 002 111" oil: I v x It Illill Ask VJ4 NIL; Of" de 45 A x I, S I L k 0 it cm Ay "DILINASS11) smity"Ill) 1C)II I S w a so 00 00 00 if-of 1 09 000 00. 046 Go- so. "(It in "mil -ip isiqiim pusniqoaq tsw llv!j 00 74 so ; : 413112will 34, oi joqn)lll pbtljjA allipt a4) III unfol wupap , 00 lilt in lumuol aplal 'I v )a qI41 qll.%% P. 440261113m% 00 I'll, , 0 till 111W 11VIN of C AT'S"l) 'Aj_,F#UV I .,Pd,r.r 'r 'AIIII.I.1 'I[ IsIfir llefil.131 "t off umxij -1~ 3: vauhtu --tiasmump! 43"%-A1 00 e0.' -Flog lpla IV 00 00 00 0 IV It 0 4 IF it It n n It Ot to pi it 111111t 11 tiff I M~009~009 0 0 00 go ; 0 0 1000e0000000000 I go 0 0 0 0 o 0 0 * 0 0 0 0 0, lot 10, K L It 'it it 4-2- 5 I.S.f 040141 - , - - 11, W! . --- .?. cn!lls -40 "cr PROCE110 -14141 "00 KInNuIlAil. J. A.Pti, -00 111"m.."ll-heyo. rMKIt 1 14 V 11141). CaIrn. ,( Iral(VIM" of r1rctrolls IIII'l .4 JWFI Jlj3jjt;Cjj-- 0 11, TWh 4 11, r4ph Al"W Ifull a resumm ImInctl by Itm lwmftt (4 COMIrtM4. the flivergelf v id wll~ -Ach vAn Im factis,"I in thi, way. i. 00 06 till! CA WALLURGIC&L LITINATWE CLAINFICATOW 110.1 tIVIN IVA- f.".4 it a~v Jal A 00 Ll all Kldl;Wl W u 9100609 0 0 0 0 0 0 0 -00 =00 coo off 400 see gee -00 -6--#l vii Blond 31 v AW I i it &i 0 KORSUNSKIY., M. I. IrFocusing Properties of the Axial Field Er--ar" and "On the Molecular Mass Spectro- graph," in Journal of Experimental and Theoretical Physics, Vol. XVI, No. 1, 10 Jul 44. (Identified with Phys-Tech. Inst., Acad. Sci., USSR, 14 Dec. 44. SO: CIG Documents Branch Translation No. 82, 3 Jul 47. 0 00 0 0 0 0 0 0 0 0 000 0-0-0-0 of 4 10 It 11 11 4 11 14 It It to 4 11 11 13 id Ins A v I A A A N r 0- A -3. on", Mit .0 Crf.t,.Ih lilt Ogo KQMWAW V Kel'umn few 2i Peti Ttcb'*Inw-.', Im;i. &i. M.I.J. &u I C.A. 30, .Vj 0o g0'3 00, Mao J'at'l A 14 - 5 L AOCT1144VINKIL LITEWIPIll CLASIVICAlfall It 0e"470 0 0 $6646#064949 *64- jolvil ilu ids 160 11114041 uglwi3 110 A A, no* fiild. r (Phys. ; 1 -00 .00 .200 API A t 0 fu 0 10 w I ff IN 5 do a I's ZOO Weft 'so* 01 0 0 0 a 0 00 0 00 0 00 0 m Is 16 11 if 11 A? 11~ J2 n m )) . -1. 9 -A 3 ,V-10 I I AA N-a'y *0 %1 A-0 -w- "DIPS Formill ..0 .60FINUO1 J'(11. , ! ! 0 0 a w I. v it is 41 m I) as a U p M 00 ,rcch. -est.,PA ain1wa SSW. J. Pkyi, go 9, 14-m(1915).-SLO c.,f, 39. 3-,2W. 00 so #0 00 A j o. I L Ao9TALLVRfK*1, LIMAYLOS CLASSIFiCATIO10 '14Z ;7- N AV 10 ISF. L 4 a if 0 13 a WT a, X, K o*1 Is In u It pr lp -it 0 ; :w -0 ; 6, ; *is 0 4 floe lee 0 .00 fee a,@* goo see too nfo I KORSUNSKIY, M. "Focusing Ptoperties of the Axial Field Epsilon sub r-ar," Zhur. Phys., 501, No. 6, Vol. IX, 1945. Phys. Tech. InBt., Acad. of Sci. of the Ukrainian SSR -1945, te i 1 0 A X 1 4 $ 6 1 0 0 fill It ti U w a0 C A I I A I I IL- L- *&eel haff into atim" I The I . com With Its (2) T is krow 00 the modur dbb 00 Pkft*"aW= 6#---Ibqpmb d, = d Ag capid ; . _ a h b dig t d ma w t e thin pkte. 4-i sr. an 190 symbodooo A~, 01.01141,11 wpto i~w am is tow. dit followin k at the pipe Is _1141-4 " Im Path Zc -mob. in the twi The equatkm aasjAp and dis. n-( w a gkn pkte in bub The am. of depnit kFC."PA- iff a$ COMPUW With so eftsion tbroV 0 " is & lee me* 900 00 460 400 400 400 400 100 too see ol *Fee* go *00000 0 Gov. A If, L-A_" a N I a L-It-f( F, a -A, - 1 -1. AA 00 90 U I I a a 1. W ...P.J.1, "OPPRI Kuwait" ait" a KUOGIN#h. Irk, "'T"4 1. V-S'.S.R. 16 K. timpoics the cumtructioll WeIrtWepli Word awl the IOM CAUS"I fly 411 5 C'I inhonagaranus Hialp"ic Aellif an the maignetic intiturett, of 11"It"d Shainal at tuals. ,kick a "'Ittv"ph w'"Im WiNfitate awl lawy wt. isottalwit, but *W) I..111m %%lilt VA111'. is tile Iralloit tillie-I a pLivral 1.401. It. 4.. havillig,filyrfvIll impaillm dill I Itilit lml~ 1411.1 diffi-tv"I V.-havilk-4 At the MW I so (11WUM6141, so 000 00" i 100 004 -r1-0 A) VA -09 zoo -1 Mg zoo U- 1710 ;~L 30* 0100 UOO -00 his it A 01TALLURGILAI. 1.1111164011 CLAIISPIC411006 woo a -at O-V ')It ist a II I In In T-i-11 -rw 4-0 1 IF am 0 a a 3 1 0 3 u K A. 'D is: It a x a a If x KW n a No ooo:o:iooeoo*oo*oooogooooo!oo,*****4booo*oooo ;T.40 Ali 411 a 0 a so@ dl 0 as 0 0 000 0 49 0 0 *10-0 0 -0-0- 0-6 - --* * 0 -0- O-e-0 0 KORSMI;SKIY, 1-1. 1. U-,-WrAdgsr-,.'InIIw Countwo X-nW& - *,sxuraienU )bv V46 nA stuc~7 of the opemtion or ciaiger-men or Counteve Umiw Intwwive Radiation ~Dpvpl an 1,,~,g)ujve SOITCeg" F9 ?'* JAWS Vo So Shpinells M6 I. K=Wmm)dyo 8 Pp, "Zhur EW i Tsor FLO Vol XVIO Ib 11 inmtip,suton or eombimd operation of an impulse set and of G~Igar-Mm*Uw couaftmg Whowing that undtr candItions of intswive iWulme x-ray radiution faIlLng on the counter the irotallation is capable of measurlm etprt-paviod activities an Im as S.W44- 2063 &K PA 13154 4.0 Ck ~-I-h. Awmil N-11~ _ t.,j f Al:,~ __ _ " .1 11 "0. adoll. K-11 , (.11(l T i~ 1 %0 KORSVNSKJ~-I Authort F'Oumi&u. is, I. Titlet The itaide =Imus, issue J2. (Atamwe isim. Lid. 2.) G:Ltyt YAscow PublLsbart State Printing Bowe of Teabacal and Theoretical Literatus Date 1. 2950 AvaiUblo s Library of Congmse source: Month3y List of Rusnian Amesgdonap Vol, 3p xo. no p. 75o rawoml, 168T103 P ..Capacitor (Condenser) "Detection of a ftlnular Bunch on the Basis of the Variation of a-Capacitor's Electricai Conductivity," M. I. Korsunski~,*L. I.. PiYovar, A. M. Mar~kus, Phys-,. icotech lust, Aca& SdI Ukrainian SSE. '-Zhur Eksper i Teoret Fiz*,Vol::XX, No 9, pp 860-861 Letter to editor reveals possibility of creating high-sensitivity detector of molecular rays, based on ..subject variation.by measuring deposition-J, from bean. under study, upon the Condenser. Shows that conduc- tivIty of vary-thli metal films- dgends. complexly on KORMINSKIII, '1. -1 - Korsunskii,M.I. The atomic nucleus I&d. 3., ispr. i dop. Moskva, Gos. izd-vo tekhnilco-teoret. lit-r-y. 1951. 347 p. (52-31219) Qc7?8.K6 1951 USWPbysics - Molecular Beam 51 MaWntic Field, Nonhow-, geneous "Focusing of a Molecular Beam by a Nonhomogen*ous X&Mtic Field," M. 1. Korsunskiy, Ya. M. Fogell,~ Pb~yeicotech Inst" Acad.Sci Ukrainian SSR "Mur Eksper i Teoret Fie Vol XXI, No 1, pp 25-37 Indicates various types of nonhomogeneous magnetic .fld Vhich permit one to realize double focusing of mol beam, and considers motion of mol in these fld takling into account action of gravitational force. TJSSR/Pbysico - Hole;-]- Boom (Contd) 1742t Jan 51 Shows that with aid of 2-dimensional nonhoso- geneous m6netic fld disclissed here one can realize lenses for mol beams. Submitted !&Aug,50. 44T61 T - The Committee on Stalin Prize& (of the Council of Ministers USSR) in the fields or science and inventions announces that the folloving scientific works, popdar scign- tific books, and textbooks have been-subsitted for competition for Stalin PrIzes for the yea" 1952 and 1953- (Savet!~M Kul vAmov, rio. 22-4o, 2o Feb - 3 Apr 1954) Home Title Of work r"Inated a "T110 Atomic Nuelcu"01 Fhrrlkov Polytechnic Korsungkiy, Institute Imcni V. I. Lenin r48 ICON wv;e6 db yo-q, 4ri - 3 -4,0 - 5- 1 4 ju S-3 j so: w-3o6o4,. 7 JulY 1954 K C) IR ~,-, 0 W ;~ K I Y) ~,-) - I . PHASE I TREASURE ISLAND BIBLIOGRAPHICAL REPORT AID 596 1 BOOK Call No.: ATIC 101536 D Author: KORSUNSKIY, M. I. Full Title: ATOMIC NUCLEUS. (4th ed., cor. and supp.) Transliterated Title: Atomnoye yadro. (Izd. 4-e, isp. I dopol.) PUBLISHING DATA Originating Agency: None Publishing House: State Publishing House or Technical and Theoretical Literature D Zate: 1952 No. pp.: 407 No. of copies: 50,000 Editorial Staff: None PURPOSE: Popular presentation of fundamentals of nuclear physics intended for students of advanced classes of pre-college sahoolso physics teachers, students in natural science, faculties and technical schoolso and also technical workers. TEXT DATA Coverage:' The book represents a general review in popular descriptive form of the major stages in the development of nuclear physicas be- gining with the discoveries of Curie and Becquerel up to the present study of chain reaction of uranium and neptunium, including work with Wilson chaniber, Betatron,-, Cyclotron, Varitron, etc. The fourth edition contains many corrections and additions on recent basic ac- complishments In the physics of the atomic nucleus. 1/2 L 1\4 S K I PV ATOM 11TOLEL 44 ki U16417W. . ISM-" G,~rtakhlxdal,1264. 327p. PRintan) (BooLondtaplay at C-Aava Coderadcol A raonography an theoretic tivestiptiovA and ened- inenW 4AA 4n isomeric imolol, their orlain gzA bobxfar. lave0g340al of the 4t"Cturo al MOM14 lk,4014t. A summary tAble of Isomeric nuolof ladicittlag #.~efxr propcotlem ad numtrous dlagams at isomeric, tr%adformaUa-as ara Oven /at the ettd o! the book. (pubIliber's natn) KORSUNSKIY,- 14. TO USSR/Nuclear Physics Nuclear Shells Jan 54 I'The Experiseiiial Foundations of the Model for Nuclear Shells M. I. Korsunskiy Usp Fiz Nauk, Vol 52, No 1, PP 3-82 A survey of the literature (1932-1953). Lists 82 references, 30 USSR and 52 Western. Refers to recent (1952-1950) works of: D. Ivanenko, N. Kole- snikov., A. Sokolov, L. V. Groshev, I. S. Shapiro, V. Rodichev, V. A. Kravtsov, B. S. Dzhelepov, L. N. Zyryanova, M. L. Chepelevetskiy, M. M. Venkov-, 276T92 1. A. Vaysman, M. A. Levitskaya. Treats: the magic numbers; binding energy of nucleons; distri- bution of the isotopes; quadrupole moment of nuclei vs magic numbers; classification of nuclear levels; nuclear spin; magnetic mownts of nuclei; beta- Opectra.and nuclear shelis; isomery of atomic nuclei; investigation of excited nuclear levels; angular distribution for (d,p) and (d,n). T-t -7 -77-- 17~ -7 777~ le'. -- - * '!',, I I ~Ieuil 1.0 -., i. ;_ - !". 4% - I t J) RUO rUr NA' Na" :a skiy,, Moscow, Gostekbizdat., 19506,, 428:pp-,5t ~e~ioniefieiar- This book is a popular presentation of problems of nuclear physics. it is intended for the use of upper classes in secondary schools, physics in-. structors, students of natural sciences and technical schools,, and engineer-, .lng and technical personnel. "Numerous changes and additions have been made in the fifth edition ..'-covering advances in the field of atomic physics since publication of the Iourth edition." The chapter headings and pages devoted to each chapter follow; activity (7-6o), Nuclear Model of the Atom (61-84), Mass of Atomic Nuclei ~,85-110) Splitting of Atomic Nuclei (111-141), Discovery of thL- Po itron 142-1641, Artificial Transformation of Atomic Nuclei (165-209), Art2r".Lai_ J,k.udioactivity- (210-231), Mesons* (232-268), The Neutrino (269-285), Structurt-:.- of Atomic Nuclei and Forces Acting Between Nuclear Particles (286-308), Xuclear Fission (309-337), Nuclear Chain Reactions (338-355)1 Peaceful Uses: to -394), 4 Pf-~A-;;ic:~Aw.gY- (356! -!379).,~;-ank T lear Heactions_(~8~ -ppendix (figdktz)' are' on jAges -- 395 (11) Category : USSR/MagnatiLl- Mqwimental methods Of Magidetism F-2 Abs Jour : Ref Zhur - Fizika, No 1, 195T N01389 Author :Korsunskin M.I., Fogel$, Y& M., Bykova, G.A., Livshits,L.I., Lozovskiy, N.S. -Cho-vnik, A.A. Title :Invostigation of the Thpography of the thhomogeneous Plane btgnetic Field f a Six-Pole Electrocagnet. Orig Pub :oh. tekhn. fiziki, ~956, 26, No 2, 122 .2-1232 Abstract :A procedure is described for t4,p.investigation of the topography of an inhomogeneous plane magnetic field of a six-pole electromagnet, used to focus Particles that have a -goetic moment. The cited measurement results show that the above fiild can be produced without substantial distortion in a circle 10 cm in radius. Card Category : USSRINuclear Physics Origin of Charged and neutral particles through 0-6 matter Aba Jour : Hof Zbmr - Mike.- No 1,, 1957,No 585 Author : I(brBunskiy, M.I., Imiantp Xh-L-, Plvovar-, L.I., 16t :-I5W9k-o-v-%Ty-te-c-I%aic lzzt.~, Title : Applicability of the Ratio ( 12 31023/72A3032) a 1, which Holds for Detailed Equilibrim, to a Been of loss with a Stationary Composition Orig Pub :Dbkl. All SSSR) 19560 10T) No 5) 664-~67 Abstract :An'analysis of the experimental data, obtained by various investiga- tors,'is'used to show that the following equality holds with an &a- curacy to within 5%: where NJ., N , etc is the ntwbor o ions in the beam having charges 1, * A 'is L the j, atc., a2 NJ, N I etc. mmbor of ions in the stationary case. Equation (I) is ogained if the rdationahip T (2) IL 1 J3 2a is valid i , cross sections that characterizethe charge exchange between 6. beam of fast ions and a substance at room temperature; Card 1/2 /V'Y /Z~-- /9?, AUTHORS: Korsunskiy, M.I., and Bazakutsa, V.A. 120-5-2/35 TITIE. An Electrostatic Analyser with a Non-uniform Field Produced by a System of Plate Electrodes (Blektrostatiche- skiy analizator s neodnorodnyr., polem obrazovannym sistemoy plastinchatykh elektrodov) PERIODICAL: Pribory i Tekhnika Bicsperimenta, 1957, Vo-5, pp. 11 - 17 (USSR). ABSTRACT: An electrostatic analyser of the differential type is described. It is designed to produce a non-uniform field which has the following components: Er i-. Ei/r - E2r1 Ez = 2E2z (1) (2) For such a field, the ion-optical properties depend on the coefficient of non-uniformity T1 given by: 2 2 2 - 2kr,/(l - kro) (3) Cardl/2 where r0 is the radius of the equilibrium trajectory and -U-LV1-CJ-'Y U-L Card2/2 -- ZMR~~- - - -- -- - IKORSUN4KIY. M.I., doktor fiziko-matematichookikh nauk, professor; LAGUNOTO Ass.# Gn~&kat tekhnichookikh nauk; BATTILI, L.P., kandidat tokhnichosirikh nauk; SINIII'MICOV, A.N., kandidat tekhnieheskikh nauk. 1~~;aior-':for- re-ginte'ring-*chmW-a'.In,cisarances in steam turoin*s. Inergomashinostroenie 3 no 5:26 My 157. (KM lot6) iStem turbines) AUTHM: RmWantsev, I.A. , Korsunskiy, M. I 4&10-IV20 TITUb The I&- and L -Lines in Cu- and Zn-Spectm (Linii L P6 ' Lt5 v rv spektrakh Cu. Anj PERIODICALi Isvestlys. AN SSSR Serlya Fisichaskaya, 1957, Vol. 21, Nr 10, Pp. 1435-1437 (USSR) ABSTRACT: The first results obtained by tests carried out in the L-series of Cu- and Zn X-ray spectra are described. This paper was intended to find out vðer in Ou and Zn in the solid state the Ln, ni-Ni transitions exist. The line LP6 corresponds to the Lill-Ni transi- tion and the line L to the LII-NI transition. The investipticas 0 of the spectra were carried out in a powerful vacum X-ray Mpectro- graph with bout mias, crystal and photorooording. The dependence of the appearance of Cu- and Zn spectra an the conditions of exci- tation me Investigated. It Is shown that the appearance of the L spectrum in the case of Cu and Zn depends to a considerable ex- tent an the conditions of the excitation of the spectzum. There- fore all data for the L-series of elements with an average atoodo Card 1/2 number (about 26 Fe to 35 Br) must be re-exudned. In the Cu- and The L 6- and L5-Lines in Cu- and Zn-Spectra 48-10- 15/20 U-spectre. LP6- ana Lj5-lines we" founa,whioh corresporA to the transitions from the Nrlevel to the Lljl- &M LII-levela respeo- tively. There are 5 figures, and 6 references, I of which is Slavic. ASSOCUTICE: WarOkov PolytectAnio Institute (KbarOkovskiy politekbnicheskiy institut) AMIABLE: Libmry of Congress Card 2/2 AUTHOR: Borevikova, G.P., Korsunskiy, M.I. 48-10-16/2.0 TITL19: X-Ray Speatruis of the Gertanium L-Series (Rentganovskiy spektr L-serii germnlya) PMODICA14 Izvestlya AN SSSR Serlya Fizicheakaya, 1957, Vol. 21, Nr 10, pp. 1438-1444. (USSR) ABSTRACTs The X-zvty spectrum of the gormnium-L-series was obtained 'by means of a tube or the Krasnikov type (Zavodalmya Laboratorlya, 1939s, 4-5). The investigation of Lp - and Lp ,-lines in -the germanium 3peotrum gave the following rea2ts: The 'horophotograph shows that the short- wave line Is more intense then the longwye line. An the Most in- tome with 9561X ma assumed as L N and that with the wavelength or 962o x an Lp (on the strength of published data). The ratio of intensities at i A and 11 L~4 is difficult to determine and to be obtained only by re-calculating the intensity of the Lp,-line. The ratio IL P3 . ILpI was found to be equal to 0-13. Herefrom it may be seen that the intensity of the L - and therefore also of the L 3 Card 1/ 3 line is very low. Furthermore, investigations were carried out I-Ray Speotn= of the Germanium L-Series 48-10- 16/20 in order to determine the presence of L III -NI, 1,II-NI and LIA -transitions in solid germanium. It(, 2and LN-recorftap II-Iii - . were made at different conditions of excitation and ex-posuree The miorophotograph shows that the double line is symmetric. It follows therefrom that the satellites are broader than the base lines. Such a strong intensity of It( and L& Justifies the statement that x these lines cannot be satellites but that they are diagram lines. It was found that the ratio between the intensities of the satellites and those of the base lines depends in a considerable degree upan. whether the sample was subjected to an eleatron, bombardment or not. On the strength of all factors determined it may be said with Just- Ifioation that the line 16(7. in the line LP6' and that the Lpi-Ilne is the Lr-line. As a result of the investigations carried out the 4.15 hypothesis is set up that the lacking of the LP6- and Lir.-lines Card 213 AUTHOR: KORSUNSKIT BAZAKUTSA, V.A. 20-5-23/67 TITLS: n 0 App=ioatlos of 'an Elootrostatib Field,of the Differential Type to the Spootrescopy of the Bundles of Charged Particle*. (Ob. I #pol I sovanit - elektrestaticheakego polya rasnestego, tips v spektrookepli saryashonnykh ahastits . Russian). PERIODICAL: Deklady kkadoxii Nauk SSSR, 1957, Vol 113, Nr 5, PP 1029 1031 (U.S.S.R.) ABSTRACT: First of all the present state of the above problem is briefly die- cussed and sevaral relevant preliminary papers are quoted. A special cassof the differential field is defined by a radial and an axial component of the form Er M (yr) - 12 a 2E2 2. Here 11 and N2 are certain constants which are in the following way connected with the inhomegeneity coefficient 1 and with the radius of the path-,.*f equilibrium: Z 2 12 2 2 (2 re (1 re 3 +01/ar)(r/31V r The differential field,f*ousees in radial and axial direction, and it in possible to apply the WEBER rule in its generalized form: the Card 1/3 source S. the ei.do of the effective sector angle and the pro- AUTHORSs Borovikova, G P., Korsunskiyq M. L 20-11j~_&j 5/54 --------------------------- TITLF,s The L6-and LP4-Linos in the Speotrta of Germaniua (Linii LN i, LP4 Y spektre ormaniyo) PERIODICALt Doklady kkadeall Sauk SSSR,1957vV*l*114qNr 6,pp.1192-1194(UBBR) ABSTRACTs The present paper shall find the lines which correspond to the transitions Lj_-vMjjI and.L,-I!,, , i_ e. the lines L(33 and LO . The wave lengths of these lines shall be measured and 4 their intensity estinted. The apparatus and.the metho& of investigationt The X-ray speo. trum of germanius was obtained by means of a Krasnikov type tube. In -the here described 0experiments the temperature of germanium remained below 50 C. The primary anode of the tube was covered by an aluminum plate. The main exciting radiation was the Kot .Ko(2-radiation of Al with the wave lengths 8321,3T and 8323,81 X. The entire focalspot participated in the.pro- duction of the spectrum. Card 1/2 Measuring multat The possible value of the wave length of t\6 AUTHORi Borovikoval G.P.# Korsunsklyq M.I. 20-1-19/54 TITLE The Satellites of 1he LaL.10 2 and Ifi Lines in the Spectrum of Germanium v spektre gerzaniya) (6 sputnikakh liniy LoL 11 2 1 LF1 PERIODICALi Doklady Akadsaii Nauk SSSRq 19579 Vol. 1150 Nr 19 PP- 75 - 77 (USSR) ABSTRACTs The. authors refer to a respective earlier worko They continue the study of the L-sories of the spectrum of germanium in order to determine the extstence oflines not observed hithertot especial- ly of the ~lines'l + N ) 9 L r5 (transition 46'(transition L ILI I L 4 N ) and L if (transition N The experi- mUtal Irrangs'-se Odiscribod'by G.P! Borihioil,and,X.I. Kor- sUnskly, Doklad* Akad- lauk SSSR, 1957, Vol- 114P Nr 6'is used. The obtained x-ray'spectra of the L-series of Go within the range of wavelength@ of from 10150 - 10400 1 (which contains the lines LoPL3 , (trans,ition L p, L I ) and If, (transition L N `dffftr:~roatly fAl the,15 otra known Lfrom literature. 9 the iYatures taken bj*the authors-brightlines were observed on the short-wavo-part next to the lines LoU 1 2 and LF,. A Card 1/2 picture of thi a spectral range as well as a odrresponding m1cro- M15 613-7 .K811 Korsunblciy, Moysey Israyllyevich 1958- The atomic nucleus. Moscow, foreign languages Publishing House 412 p. illus., diagrs., grap'ns, tables. Translated from the Russian: Atonnoye Yadro. KORSUNSKIY, M.I.; RUMYANTSLT. I.A. yC_J~nsm In copper and zinc spectra. Isal, po sharopro (MIRA 12:U) '(Copper--Spectra) (Zinc--Spectra) 82792 s/o58/6o/ooo/W) 4/t)08/'0 16 AOO,3/AOO 1 Translation from: Referativnyy zhurnal. Fizika, 1960, No. 4, p. 224, f 9169 AUTHORS: Bazakutsa, V,A .Korsunskiy, MJ, TITLE: Some Aberrations of a;n~IonnBeam When Passing Tbrough an Electric Field of the*Er .-Eor-1 (1-kr2) Type PERIODICAL: Tr. Khartkovsk. politekhn. in-ta 1958, vol. 14, pp. 83-ioi TEM. The motion of ions in an :electrical field of the difference type with the components Er = -Eor-l - (1-kr2)'-Ez--= -2kEoz, where E0 and k are parameters of the field, was considered in the 2nd approximation. The Ist approximation was discussed by M.I. Korsunskiy (Abstract f 9168),r In so far as ~he motion of the ions is considered near the equilibrium trajectory,the method of perturbations is applied to the solution of the problem. The calculation of the side shift of the ion beam from the equilibrium trajectory made it possible to establish its dependence on the inconstancy of the value of the ion energy (~), their angle of divergence ((P r) and the width of the input slit (Aro). The aberration coefficients have the highest value at and q) -3. The aberration r coefficients of a difference-type field were compared to the corresponding c0- card 1/2 S/'058/60jWO/t)04/0O9/t) 16 AOO3/AOOl Translation from: Referativnyy zhurnal, Fizika, 1960, No. 4, ppL. 224-225, # 9170 AUTHOR: Korsunskiy, M.1. TITLE: =lMo=ion of ~Ionln an Axial Magnetic Field of the Hz = Hlr2s-H2r Os+2 Type PERIODICAL: Tr,.Kharlkovsk. politekhn. in-ta 1958, Vol.. 14, PP, 103-110 T W e motion of ions in axial magnetic difference-type fields of the Hz = Hlr2s_H2rYS14-2 type was investigated in order to find magnetic fields with a high dispersion and resolution power. The components Hz and Hr of the difference- type field were determined. Conditions for focusing a diverging ion beam were established. At the focusing spot the beam Is decomposed into spectrum with a dispersion exceeding by one order the dispersion in a homogeneous magnetic field. A high degree of dispersion can be obtained for a difference-type field wity, various values of the s parameter. A differenoe-type field with parameters s-0 has a minimum aberration for ions moving outside of the plane z=O. Difference- type fields have the property of double focusing in direction (in z and in r). Card 1/2 C^ i P LO L/ 67983 SOV/81-59 12-41476 Translation fromt Referativnyy zhurnal. Khimiyaq 1959, *30- (USSR) P 35 AUTHORS: Pastushuk, N.S.. Litvinov, LeBo, Reznik, M.V., Korsunskiy, M.I, TITLE: ivit re Selenium~_With The Negative Photoconduct Arlof Thin LMe #Vof Admixtures of Tellurium PERIODICAL: Tr. Khar1kovsk** politekhni.in-ta, 1958, Vol 14, PP-111-115 ABSTRACT: The photoconductivity 6 of thin layers of amorphous Se with an ad- mixture of Te dusted in vacuum on glass backing at room tempera- ture has been investigated. The darkness conductivity(5`0 of.the studied layern is extremely low. It has been shown that the in- vestigated samples have a noticeable negative photoconductivity observed at very weak electric fields (10 2v/cm). The ratio of the dark current to the light current is 1.2-2. The time of es- tablishing the itationary value of C is equal to 15 - 20 minutes, and the time of relaxation of the "negative" 6' , determined from the moment of switching off the light to eatabYishing the equili- brium value, is 12 - 16 hours, It has been pointed out that there is no theory which can explain the described phenomena. Card 1/1 V. Ostroborodova AUTHORS: Korsunskiy, X. I., Bazakutes., V. A. soy57-28-7-24/35 TITLE: Investigation of Ion Optical Properties of a Sector Electro- static Field of a Difference Type (Iseledovaniye ionno-opti- cheakikh evoysty sektornogo elektTostaticheakogo polys, raznostnogo tipa) PERIODICAL; Zhurnal tokhaicheakoy fiziki, 1958, Vol. 28, Nr 72 PP-1510-1525 (USSR) ABSTRACT: The results of the investigation of ion optical properties of an electrostatic sector field of the difference type pro- duced by electrodes of the shape of equipotential planes are given. The authors discuss a special case of a difference fieldl viz. a simple superposition of the field of acylindric- al condenser and of an axial fieldp as described in Ref 17- First the focusing in the difference field is investigated and it is shown that a use of the difference fields can practically increase the resolving power also in those cases where the dimensions of the picture are mainly fixed by the Card 1/4 dimensions of the sources. An experimental determination of soy57-28-7-24/35 Investigation of Ion Optical Properties of a Sector Electrostatic Field of a Difference Type the ion-optical characteristics of an electrostatic sector field of the difference type and especially a determination of the aberration factors is carried out in order to solve the problem of the usefulness of an application of difference fields in the spectroscopy of beams of charged particles. This field was produced by condenser-type coatings to which the corresponding potentials were applied. It was found that such a field just as well as the field of a cylindrical con- denser is equivalent to a thick lens combined with a prism, and that in the case of good focusing it shows a consider- ably greater dispersion (by one order of magnitude). The ex- perimental determination of the values of the aberration factor coincidowell with those calculated theoretically. In the determination of the ion-optical characteristics of the differenee-seotor field the authors started from the applicability of the geometric parameterg q and p of the systems and from the parameters A r , Yr and 6 characteriz- ing the beam of charged particles. fien such a set of variable magnitudes is at hand the wanted characteristics Card 2/4 may be determined. - The description of the experimental :3OV/ 57--29-7-.24/35 Investigation of Ion Optical Properti9a of a Seotor Electrostatio Field of a DiffererQa Type apparatus follows. Based on the carried-out investigation the following is said; 1) The theoretical investigation of the ion-optical properties of a differenee-field of the sector type carried out proves the possibility to use it in the spectroscopy of the beams of charged particles. 2) This was proved by the experimental checking of the theoretical con- clusions. The experimental data obtained well agree with th'ose from theory. The dispersion of first order in the dif- ference analyzer amounts to the 12-fold of that in the ana- 1~zer with an electric field of a cylindrical condenser. 3 *The method worked out permits to determine experimentally the ion-optic-al system parameters- 4) By realizing the dif- ference fields by means of a heterogeneity factor which is as small as p,~~Hsible (where no focusing takes place yet) an important dispersion can be obtained- 5) The dispersion of 0 the energy field dependa on the magnitudes 6,A r and which demands an earlier calibration of the analyzer. 6) it is useful to use the electrostatic seetor field of the dif- Card 3/4 feron,~e typo for tho eons trdction of tho compact spectral sov/ 57.. 29-7-24/35 Investigation of lor, Optical Properties of a Seotor Electrostasic Field of a Difference Type apparatus with g--aat resolving power. 6 denotes the magaituds oharaoterizing the soatterirg accord- ing to ener&-. 6.r0 denotes the initlal dtqviatir~xi from the path of equi- ligrium. i~f aw. ion. kP denotes the initial angle of the inclination to the tra.- j6X ,Story of equAilibrium. q and p are the magnituda-,ir, the scheme of the generalized rule by N. F. Barber (Ref 22). There are lo figures, 3 tables, and 25 refarenoss, lo of which are Soviet, ASSOCIATION: Khar1kovskiy politekhnicheskiy instiltut imeni V. I. Lenina (Khar2kov Polytechnioal Institute imeni V. N. Lenin) SUBMITTED: may 3, 1957 1. Electric fields--Optical properties Card 4A 18M FUSN I DWI EXPLOITATION SOV/3355 Akadesiya naule SSSR. Inatitut "tallurgii. Kaucb=77,40vat PC problems abaroprochnftbi OVI&TOV zMalsdo'"anlys po zharoprochnys splayss. t. V (Studies an Reat-ri- St nt Alloys, val. 4). Xomcov, lzd-vo AN SSSR, 1959. 400 P. ta slip Inserted. 2,200 copies priza0d. ;= ad. at PublighlUg NOUN@: V. A. 911sov; Toch. 34.: A. F. Ouseva; WItarial-Oftards 1. F. Bard1n. Academician; 0. V. Kurdrumov, Academician, X. V. Agmyev-, Corresponding Member, USSR Academy or Sciences; 1. A. OdIng. 1. X. Pavlay, and 1. P. Zudln, Candidate of Technical sciences. JURPOSgt Thin book 18 Intended for notallurglStO eone*rned with . the structural metallurgy or alloys. COVIRAUXt This Is a collection of specialized studies of various groblem in the structural metallurgy of heat-reMiStAnt alloys. -Inciplea. @cuts with do al z o ti re c p 0" are concerned with the .riptions of now equipment and methods, others with propert Occurring under ve iried Conditions are studied and reported on. ftr details, c ?sbl* Of Contents. The articles are Accompsal-id by a num- " ber or references. both Soviet and non-Soviet. Studies (Ccot.) 1 SOV/3355 Act'-LOO.or a.if-dlffusion and the Debys Charxtris tic Tespersturs -of metal. 117 And X L*-r-' . Npendene~ or "IS lrfUAI*n Parvait erg on the Type of 6 on- tim P"Stact Of Small Adaixturss a Crystal lettlce Ax f & Second Com~ ponest . I . 123 x GortspIkon 3 0 &W A Study af Small During the Annealing Or iworw9d xickel 134 (M the L- iorlos P.. and X. L. mg%= ~ 3pactrum of Oarmajal 140 DavIdenkow x x and A 1. 3m irn," An Investigation or the lmik~- ~-#;runws:;~~' Ormed at Various Temperatures 147 D. Studies (Cone. 30"355 Investigation Of the Diffusion Or Cobalt and Uran Along tb4 Grain MOundarles 152 X-OkshtgYn. ~S. -2 j T I Oudkola. A. A. Zhuwhovitakiy, and , S xisiiiin' . . .. and Strain on the Dif- fusion Procoas 158 Sbinyay*v A Ta DirfuglOn C haracterlstIcs and Heat to light Component Xickel Alloys 16~ ArkftarQv_-W-X,-S-. X-JUntsman, ind A. X. Ttso oyov~ The - f Small feet0 -Uslatures an the C4ftlel.nt of D f fusion In PO1Y*rY8t4l12n* Mat6rL4kls ITO In the f,,Y*v,, &ndrl. P. Polrkar~pdva. Concerning Changes at n' V& lou& ~ Ad&lxtur*s at Different 3t&ggs of Aging at All ys 176 Xmtsrftl PrIction or run lkt&ls &W Alloys - Coro 6/12 24(,4) Akademiyx naux Ukv~&Ln.Aoy Z.,.jj. Clrlki Pb4oalaktrizbodkiya I qptj4r4.-dkLy~ ravionlya v poluprovadnikakhi tri4r p4rvaga vacanyu-.tiogo PO rOtf'v1~ktrI1h4skl;& I aptlaheaklm yavlenlyam v pol~~avNlnt"kh. 1c. Klyev, 20-26 0074ta"ra 1957 g (rhcto--1-4trL'c SUJ OptLuai rhan0m-.414 In SMU- conductors; Tranaaaclonts of tm~ First Conre~n4ft on rhatceleatric and Optical Phenm,,na In XlYev, 1959. 403 P. 4,000 copies print-d, M"tlonal SPonnorlns Agencyt na.k Aft-n . Prealdium. KomlsslYa Po poluprovocnikam. M. of Publishing Houses 1, V. Xzs--a; Teah. Ed.: A. A. R3tveychuk; Reap. S1.3 V. Ye. Lashkarav, A~--emlci4n_UkralnLaa SSRA Academy or 3alences. 1MWMKs eLis book In Intended rar scientists In the field or send- -conductor-PM 3pectro*Capy. and n=lCOAdUUtzr Will C, UZerul E6-j-4-V7& GOV1404. The nced ~etudentslh vAUv*rs1tlQs and Inatttutca or -11=~r'tachnical training specializing In the physics and technical application or Be"- Gonductors. COVIRAOSt fte collection contains --*P*rt3 and information bulletins (the latter ars indicated by asz*--Wv-'l read at the nrat All- Union Conference an OPtLc3l anti Z%or~alectrlc Phenomena In Uzi- conductors. A wide scope of prccl=3 In semiconductor physic and technology are considereds ;C'otoco.ductivity, phctc&IQ=O- motjv* forces. optical properti". phateelactric cells and photorealstors. the actions or r~rd and corpuscular radiations the propertlea of thin films and c~=pltx semiconductor systems: *to. 12he materials were prepare-* -Izr publication by E. 1. Reshboy, 0. V. SnLtko* X, D. TDIVYS*o A. F. Lubah=X0,And X. X. Sheynkman. ReCamncaa and dincu*stan rallow, each article. ycotoel.etrjo and optical FAvOoftefts (Coot-) 30v/-,140 4 M=ihs -dI-nS the M jerefelchev. V. G. # and 10 . o the Ab-Sorption SuIrimo AccoMLO 1 rhotocan=-rTM f Le - or x1crowaves 213 Base roculirities of the photoconductivity 1 . (Theaef) 229 pmporties of 3w&,_oc=doc tars In 1hic P1105 I I ., JL-L.-XL=&. a n- aki v u 1 - 2= nA an' Nazat rj4 --joTchov -aj;j~r;or SaTrnT=--TFG-A-f0d With rAer-cury 220 optical -AL-2i. 1 L1.2-t-A me Semiconductors ?F~ --- perrats or T=n Vilng Of 3 227 XjJLy&y, A~ A. 1MahzhSlI70v, 0- X ~ Allyev. and X. Salarov. In extigstion of the Optical fropertles of 3~16nium With Adsdx-~& of Iodine, Bromine, 05432 SO'1/120-59-3-3/46 AUTHORS: Korsunskiy, M. I., and Zashkvara, V. V TITLE- On~tii~`: ~6RTR~Yeduction of Aberration Coefficients in Non-uniform Field Analyzers (0 vozmozhnosti umen'sheniya aberratsionnykh koeffitsiyentov v analizatorakh s neodnorodnymi polyami) PERIODICAL: Pribory i tekhnika eksperimenta, 1959, Nr 3, pp 21-25 (USSR) ABSTRACT: Contemporary charged particle spectroscopy uses electro- static and magnetic analyzers with non-uniform 9 axially symmetric fields. The use of a non-uniform electro- static field which falls off along the radius more rapidly than the field in a cylindrical condenser and also of a non-uniform magnetic field, enables one to increase considerably the dispersion of analyzing devices (Refs 1 to 5). However, such fields have the disadvantage that they have relatively large aberration effects (Ref 3). The aim of the present paper is to investigate the possibility of removing or minimising these aberra- tion effects, which are due to the non-uniform fiold, Card 1/5 while preserving the large dispersion. It is shown that 0502 SOV/120-59-3-3/46 On the Possible Reduction of Aberration Coefficients in Non-uniform Field Analyzers this can be done by using a number of electrostatic or magnetic non-uaiform flelds,slightly different from each other. Such a multisector analyzer is analo-gous to a collection of lenses correcting the principal aberrations of an optical system. The particular set-up.considered is shown in Fig 1 and consists of a number of,-non-uniform electrostatic fields in series. ~In Fig 1 the sources on the left and the detector on the-right. The field components in the neighbourhood-of the main orbit (a circle of radius r.) may be represented as power aeries in the small uan t ties (r - r~)/r and z/ro (Eqs (1) and 2)). Expressions (1 ana (2) satisfy Maxwell-'s equations and the symmetry requirement with respect to the plane z = o. It is assuiAed that on the boundary between two neighbouring se re th re 2-1 a jump within the field from a value EM to EZn + ). At the input and output of the analyzer the field changes (liscontinuouzly from zero to the values given by Eqs (1) Card 2/3 and (2). The equations of motion of an ion with a mass m 05432 SOV/120-59-3-3/46 On the Possible Reduction of Aberration Coefficients in Non-uniform Field Analyzers and charge e in the nth sector are given by Eq (3). This equation is solved by the inethod of successive approximations and the first order focussing condition and energy dispersion are derived and are given by Eqs (10) and (11). Next, an analysis is given of the aberrations. It is shown that by suitable choice of the geometry the aberration coefficients may be reduced to zero. This analysis can be extended to magnetic fields, In particular, second order double focussing and high dispersion may be obtained by using a three- sector electrostatic analyzer in conjunction wi:th a sector producing a non-uniform magnetic field.. There are 4 figures and 6 references, 5 of which are Soviet and 1 German. ASSOCIATION: Kharlkovskiy politekhnicheskiy institut (:Kharlkov Polytechnical Institute) SUBMITTED: April 14, 1958 Card 3/3 - ~ BOROVIKOVA, G.Pq KORSUASKIY, N.I. L-sories spectrum of germanium. Isol.po sharoproplav. 4: 140-146 159. (MIRA 13:5) (Gormanium-Spectra) .27758 P/0-9p/61/000/007/062/086 aU.2%?.7.2 AOOI/A101 AUTHORS: Korsunskiy, M.I., Zashkvara, V.V., Bazakutsa, V.A. TITLEt On the joint action of electric and magnetic difference-type sector fields on an ion beam PERIODICAL: R-aferativnyy zhurnal. Fizika, no. 7, 1961, 299, abstract 7Zh4q (11Tt. Kiarl. kovak. politekhn. In-ta% 1959, v. 25, 61 - 71) TUT: I1; was established that a system of consecutively arranged electric and mWctic Cifference-type fields ensures double focusing of a divefgent ion beam, Moreover, in this system it is possible to bring about, by a correspond- ip,-1y selected shape of the magnetic field, &lso additional focusing along the z- .t~xis. Conditions are derived for automatic compensation of variation of one field by varying the other.,- which ensuries a high stability of the ion-optical sys- 44~ tem. As a result of theoretical investigation of th e ion motion, optimum valu- es of parameters were selected for obtaining high dispersion at small image widti-4 The ion-optical system studied can be utilized for designing a powerful mass- spectrograph with a high resolving power. There are 11 references. V. Bazakumea. [Abstracter's note: Complete translation] Card 1/1 YOF Say, RUIVAJ,Ts C Zn cyutelz- -6,ae Ul- t Zri in al.LOYJ 14-2) 'pectra 0. 7 no. 6:35C--35-9 D 159- -1.-Spactra) 24M BOV/48-23-5-6/31 AUTHORSt Borovikova, G. P.f Korsunskiy, M. 1. TITLE: Investigation of L-Series of Germanium (1, esledovaniye L,-serii germaniya). Influence of Impurities (Vlijaniye primes PERIODICALs Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, 1959P Vol 23t Er 5, pp 564 - 568 (USSR) ABSTRACTs The transition of matter into another physical or chemical state causes, an is known, a change of the electron state in thes6tomc , and-these changes are revealed in the structure of the X-ray spectral lines. The comparison of the spectra shows that the spectrum change occurring in.metallic germanium takes place, as if the samplG surface were oxidized. In the inves- tigations under review, the intefisity of the lines was measured with a microphotometer. The classical dispersion curve for- mula is then written down, and a diagram.shows.the measured intensities of the L-lines as well as their aplitting up into individual maxima. Table.1 slimmarizes the.half widths of the individual maxima, and table 2 the interval between the maxima (both in ev'). The intensity of all lines is computed with the Card 1/2 abovementioned formula. Germanium rectifiers are investigated Investigation of L-Series of Germanium. Intluence of BOV148-23-5-6131 impurities next, and their frontal and lateral spectra are shown in two diagrams. Finally, the influence of small iron impurities (0.002%-0-05%) on form and position of mfxima is investigated, and results are summarized in four tables. Special samples serving for these investigations were prepared by the Institut poluprovodnikov AN USSR (Institute of Semiconductors As Ukrin and gratitude is expressed to V. Ye. Lashkarev. There are figures, 10 tables, and 3 Soviet references. ASSOCIATIONt Khar1kovskil politekhnicheskiy institut im. V. I. Lenina (Khartkov 1?alytechnic Institute imeni V. I. Lenin) Card j/2 ,t,, PHASE I BOOK MUWZrATZON SOV/4347 Akademiya neuk Ukrainskoy SSR. Institut neta.Uokeramiki i spetsiallnykh splumv. Seminar po zharostoykim materialam Trudy., v-yp. no. 5 (Transactions of the Academy of Sciences, Ukrainian SSR, Institute of Metal Ceramics and Special Alloys, Seminar on Beat Resistant Materials, No. 5) Kiyev, Izd-vo AN Ukrainskoy SSR., 1960. 63 p. 2,000 copies printed. Ed. of PUblishing House: I.V. Kisina; Tech. Ed.: A.A. Xatveyebuk,- Editorial Board: G.V. Samsonov (Reap. Ed.), I.N. Frantsevich, V.7. Grigorlyeva, A.Z. Men'shikov.. and M.I. Korsunskiy. PURPOSE: Tha book is intended for engineers, scientific workers and students specializing in refractory metals and their compounds, powder metallurgy, electronics, machine building and physical wtallurgy in schools of higher technical education. COVERAW.6 This collection of papers, originally presented at, the Seminar on Beat Resistant Materials in Kiyev on June 13-June 17, 1958, Card 1/4 Transactions of the Academy of Sciences (cont.) SW/4347 discusses the physical properties and production technology of refractory metals and their metal-like compounds with boron., carbonj, nitrogenL, and silicon. The results of investigations of the absorption and emission spectra of niobium and chromium compounds., processes of joint diffusion of two elements in metals., and data on phenomenological studies of physical properties of metal-like phases are presented. Methods of processing rare metals and refractory compounds In making powders and various articles used in many fields of modern technology are analyzed in detail. Several articles discuss the particular problem of powder metallurgy of ordinary metals and alloys. The papers reflect work performed at the follovIng institutions: Inatitut metall keramiki I spetsiallnykh spl AN USSR (Institute of Metal Ceramics and Special Alloys,, Academy of Sciences UkrSSR), Gosudarstvennyy institut prikladnoy khimii (State Institute of Applied Chemistry) leningrad., Khartkovskiy politekhnicheak:iy institut (Kharlkov Poly- technic Institute),, Institut fizild.metallov AN SSSR (Institute of the Physics of Netalsj, Academy of Sciences U=)., Sverdlovskiy gosudarstvennyy universitet (Sverdlovsk State University),, VrM' TaNIMbEEWT., VNIrMhj, Institut metallurgil AN USSR (Institute of Metallurgy, Academy of Sciences Ukr8SR) VNIrm., RM.. Gorlkovsldy politekhnicbeakiy institut (Gor,kiy Poly-technic Institute)$ and Ytoskmrskiy elektrolampovyy zavod (Moscow Electric Bulb Plant). accompany individual articles. Card 2/4 Transactions of the Academy of Sciences (Cont.) SM/4347 TAMZ OF CMUMM: Introduction 3 Beshpor, V.S. Physical Properties of Metal-Like Compounds 5 and Ya. Ye. Genkin. Emission Bands L Korgunakiy,.M dL - t~ 02 an .1 of Niobium in IM, NW and MbB2 15 Questions and Ansvers 19 Discussions 20 ffenmono,7, S.A.y and A.Z. Men'shikov. KZ pectra of Chromium Absorption In Borides, Carbides, Nitrideo, and Some Other Compounds 21 Discussions 24 Frantsevichp X.N., and A.N. Pilyankevich. Comparative Brittleness of Refractox7 Compounds 28 Questions and Ansverp 36 Card 3/4 Tran actions of the Academy of Sciences (Cont.) SOV/4347 Arkharov., VJ.j. and V.N. Konev. Joint Diffusion of Two Elements in Hard Metal 37 Questions and Answers 40 Discussions 40 Samsonovo G.N'.p and N.N. Zhuravlev. Structure and Properties of Borides of Rare-Earth Metals 43 Questions and ansvers 51 KudiTartsev., V.1.2 and G.V.Sofronov. Precision Determination of Lattice Intervals of Boron Carbide of B a B ,,C Composition According to Roentgenograms Obtained in2Q Re on'6f Large Scattering Angles (0-0 900) 52 Questions and Ansvers 60 Discussions 61 AVAILAME: Library of Congress Card 4/4 TA/dvn/ mas 3.1-18-6o pill Fie IN 1 ~! ~e It lit ~14 t4 P 14 9 v ell a, ICU , , Ir VIP 11 VS J 82336 A9'T)-)00 S/139/60/000/03/Oi8/o45 a 14 r'>Z_V 0 Efi~'VE314 AUTHORS: Reznik, M.V._and Korsunskiy, t" TITLE: On the Diffusion of Mercury Atoms Into Selenium PERIODICAL: Izvestiya vysshikh uchebnylch zavedeniy, Fizika, 1960, Nr 3, pp 107 - Ill (USSR) ABSTRACT: The effect of mercury impurities on the conductivity of selenium is well imown (Refs 1, 2, 4). The mercury impurity increases the conductivity of selenium by millions of times.and alters its photo-conductivity. It has been found experimentally that the change in the photo-conductivity of selenium depends on its electrical conductivity and consequently on the amount of impurities introduced into the selenium. Depending on the concen- tration of the mercury-impurity atoms, the photo- conductivity of selenium can be either positive or negative. Henco,,:Ln order to obtain a definite concen- tration of mercury atoms in stlenium and consequently a given type of conductivity, it is important to have information about the diffusion of mercury into selenium. Published data on this subject are claimed to be not very Cardl/4 consistent. The present paper reports results of 82336 S/139/60/000/03/018/045 Eg3ef/en -14 On the Diffusion of Mercury Atoms Into um measurements of the rate of diffusion of mercury into thin (10-4 cm) films of amorphous and crystalline selenium. The selenium was deposited onto circular glass plates, 16 mm in dia, or rectangular glass plates, 14 x 26 mm, with grooves cut into them. Wire electrodes, 0.45 mm in dia, were fixed in these grooves and were covered with a layer of gold or silver. The selenium was then deposited on these discscind placed in a vacuum. The thickness of the selenium deposit was 10-4 _ 10-5 CM. The form of the discs and plates is illustrated in Figures I and 2. Depending on the tem erature of the base, the selenium was in an amorphous or crystalline state. The structure of the deposits was investigated by X-ray methods and also metallographically. The mercury atoms were introduced into the selenium with the aid of the apparatus illustrated in Figure 3. This simply consists of a perspex holder B into which the specimen ~ could be inserted and subjected to the effect of mercury vapour, Card2/4 the mercury being held in the adjustable reservoir A . kr 82336 s/i39/6o/ooO/O3/O18/o43 On the Diffusion of Mercury Atoms' -10PARlium While the selenium was in the mercury-vapour atmosphere, Its electrical conductivity was continuously measured. Mercury atoms entering the selenium increase conductivity. -After a.cert&In_tiizte *L-- after*the beginning.of the penetration of-mercury into the-s-elenium, a measurable conductivity could be observed. At toomtemperature 't = 10-20 min for amorphous selenium and 3-5 hours for crystalline selenium. The conductivity rapidly increases after this time and & typical graph of conductivity versus time is shown in Figure 4. When the specimen was removed from the mercurya-vapour atmosphere the resistance of the specimen Increased by a factor of 2 _~ 3 and then remained constant. It was found that ^& decreases with increasing-temperature ("r, = 10, 3.5 and I min when t =:36, 48 and 58 OC, respectively). The experiments -indicate that the diffusion of mercury into selenium takes place both 40. room and higher temperatures. The rate of diffusion in amorphous selenium is greater than in crystalline selenium. The rate of diffusion in crys?alline Card3/4 83362, 1/ /7 /7 S/139/60/000/oo4/020/033 E201/E591 0 0 AUTHORS: Korsunskiy, M.I., Pastushuk, N.� and Mokhov, G.D. TITLE: Photoconduc ivi inetics of Amorphous Seleniumh yers Treated with Mercury Vapour PERIODICAL:Izvestiya vysshikh uchebnykh zavedeniy, Fizika, 1960, No.4, pp.167-172 TEXT: The paper deals with photoconductivity of amorphous selenium layers treated with mercury vapour and exhibiting both positive and negative photoconductivity (positive means here enhancement of the electrical conductivity by illumination, negative means reduction of the electrical conductivity). Selenium layers were produced by vacuum deposit ton (at 10-5 mW Hg) on glass plates. The layers were from 2 x 10- to 3.5 x 10 cm thick. The electrode positions are shown in Fig.l. The experiments ext--anded over the ff7c,11owing wavelength ranges: 360-46o, 530-58o, 600-720, 740-1000 m-0- Figs. 2 and 3 give typical oscillo rams showing the dependence of the change in the crduct 2 inten N a) with time (t) under illumination with light of 10- W/cm sity. The oscillograms show that illumination raised the conductivity Card 1/3 83362 S/139/60/000/004/020/033 E201/E591 Photoconductivity Kinetics of Amorphous Selenium Layers Treated with Mercury Vapour irrespective of the polarity of the applied voltage. Initially the photoconductivity rose very sharply, reached a maximum (od a max and then decreased slowly reaching a steady-state value (j& a ) in 4-5 min. A family of oscillograms representing the depenaence a = ad + A a = y(t), where a d is the dark conductivity, is shown in Fig.4. Figs-5-10 show, as a function of the intensity of illumination, (ILO) (Figs. 5 and 6), AU (Figs-7 and 8), dt t -4 0 max 'AUc (Figs. 9 and 10). It was found that the photoconductivity kinetics of mercury-treated selenium layers depended strongly on the wavelength of illumination, on its intensity and on the polarity of the applied electric field.The negative photoconductivity was observed under illumination with short-wavelength light of sufficient intensity. The positive photoconductivity decay became less pronounced with increase of wavelength at a fixed illumination intensity. There are 10 figures and 5 references: 4 Soviet and 1 French. Card 2/3 833052 S/139/6o/ooo/oo4/020/033 E201/E591 Photoconductivity Kinetics of Amorphous Selenium Layers Treated with Mercury Vapour ASSOCIATION: Kharlkovskiy politekhnicheakiy institut imeni V. I. Lenina (Kharlkov Polytechnical Institute imeni V. I. Lenin) SUBMITTED: June 29, 1959 (initially) March 26, 1960 (after revision) Card 3/3 S', 2 2," foliS, Mpbf 12'73 23332 9/058/61/000/0096/017/063 AOOI/AIOI AUMHORS: Korsunskiy, M.T., Genkin, Ya. Ye. TITLE- NiobitLm emission banda I A2 and Ti in NbN, NbC and NbB2 i PL11:10DICAL: Referativny- no. 6, 1961, 151, abstract 6vii4 ("Tr. .; zhurnal. Fizika, Seminara po zharoatoykim materialam", (in-t metallokeramiki i spets- sPlavov AN UkrSSR, no. 5), Klyev, 1960, 15 - 20) The authors investigated the L-series of Nb In the compounds NbN, NbC and ?TbB2- it was found out that intensities and shapes of lines Lo~,, L 21 ~11 L ~.4, LA and others varied'insignifio3antly, whereas these of bands L~ 2'and T suffer only pa , shlrp changes. The bands L~ 2 and L,,,,,l of Nb In compounds are r . of ;the corresponding bands of pu e Nb. The"outting-off" of band parts Is a con- sequence of escaping of a part of electrons in the ffientioned compounds from d- state of Nb., The measurements performed are insufficiently accurate for reliable quantitative 2onclunionz, 'out in the NLB2 compound this phenomenon is more pro- nounced than in NbN and NbC. [Abstracter's ricte: Ccmplete translation] Card 1/1 S/115J60/000/05/25/034 B007/BO11 AUTEORS: Korsunekiy. M. 1,. Lagunovt Ae S., BaYvell, Lj_.E" 51neMIKOV9 A6 We TITLE: Use of Radioactive Isotopes for the Measurement of Vapor Moistness PERIODICAL: Izmeritelinaya takhnikap 1960, No- 5P PP 50-52 TEXT: A method of measuring vapor moistness is offered here. It bases on the determination of vapor density after absorption of 0-partioles. A radioactive sulfur isotope was used for the purpose. Investigations were first oonducted in the laboratory. Source activity and counter were selected, the optimum distance between isotope and counter as well as the absorption coefficient were determined. The experimental setup shown in Fig. 1 served for the investigations. The setup is briefly described along with the investigation course4 An aluminum vepoel pre- pared for the purpose and shown in Fig* 2 was used as source. Radiometer 5 -2 (B-2');$served as recording device. To determine the vapor density it was necessary to determine the mass absorption coefficient of Card 1/3. Use of Radioactive Isotopes for the S/11 60/000/05/25/034 Measurement of Vapor Koistness B007YBOII irrespective of the state and the drop also of the moistness contained in the vapor. There are 3 figures and I table. Card 3/3 IKORMNSKIT, M. I.;- GININ, Ya.Ye - Possible determination of electron distribution br their d and d5/2 states in relation to the intensity, of L-series line J~2 Sal. po zharopr. oplav.6:165-168 160. OGRA 13:9) (Ilectrons-3kission) (X-rayl3-Dif f raction) 29409 S/081/61/000/017/002/166 B102/B138 AUTHORS: Korsunskiy, M. 1.9 Genkin, Ya. Ye. TITLE: X-ray L spectra of niobium in the diboride, nitride and carbide, and the nature of the bond in these compounds FERIODICAL: Referativnyy zhurnal. Khimiyaq no. 171 1961, 11 - 12, abstract 17[;65 (Sb. "Issled. po zharoprochn. splavam", M.t AN SSSR, v. 6, 196o, 169 - 173) TEXT; X-ray fluorescenceL spectra of metallic Nb and of NbC, NbN and NbB2 (lines L 0t1, La2, L01 , LY1 , L02 , L,, and LP4 ) have been obtained. When passing from metallic Nb to compounds, the intensity and shape of the lines La1 , LPI, L03' LP4change very little, while in the L,2 and L Y1 lines the change is considerable. The first of these lines, which is of normal shape in metallic Nb, becomes a broad line with two peaks in NbB 2; the change consists in the "shearing" of part of the band. The same Card 1/2 Z' /Y 62550 S/181/60/002/007/030/042 19 0 0 B006/BO60 AUTHORS: Korsunskiy, M. I., Pastushuk,_N. S., Mokhov, G. D. TITLE: On the Photoconductivity of Sulfur yers Exposed to the Action of Mercury Vapor PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 7, pp. 1581-1583 TEXT: In a previous paper (Ref. 1) the authors had already found that layers of amorphous selenium treated with mercury vapor exhibited both positive and negative photoconductivity. The development of photoconduc- tion proved to ba complicated and very sluggish. In the present paper the authors examined sulfur layers. The samples were prepared by vacuum sput- tering of sull)Ar (jo-5 torr) onto a glass plate 18 mm im diameter. Gold electrodes were applied at intervals of 3 - 4 mm (Fig. 1). The sulfur layer had a thickness of (2-$.jo-4 om and a dark resistance of 1012 ohms. After it had been treated with mercury vaporg its resistance dropped to 106 ohms and less, depending on the durat ~on of treatment. At room tempera- ture the treatment took 4 - 5 days; at 70 C, 7 - 8 hours. The authors found a peculiar oatalytia action of sunlight: The treatment took no more than Card 1/3 82550 On the Photoconductivity of Sulfur Layers 5/181/60/002/007/030/042 aposed to the Action of Mercury Vapor B006/BO60 - 12 - 15 minutes with the use of sunlight~ It was further shown that photo- ac3ivity differed in various parts of the sample; the differences amounted to almost one order of magnitudeo The highest activity was exhibited by the layer at the points over an electrode. A loop oscilloscope with a d-c amplifier and a galvanometer was used for the measurement of photo.. r;onductiYity9 and a projection lamp (400 W) served as light source. Speed measurements were made on a monoohromator of the type Y11-2-(UM-2). Fig. 2 shows ~d - f(t) for a sample irradiated with X - 453 and 645 mg at room temperature. At X = 453 mp photoconductivity rises, passes through a maxi- mum, and drops (below the value of darkness) deeply into the negative range (nagati-fe photoconductivity). At A - 645 mp a rise is observable vith subsequent saturation (sluggish positive photoconductivity). Such a dif- farsnt behavior is also found if the conductivity of the sample whose photooonduotivity was effected by 453 and 645 mag respectivelyg is measured in the dark (Fig- 3). The dark conductivity is maintained for 2-5 hours in both oases. There are 3 figures and 4 references: 2 Soviet and I British, Card 2/3 86810 S/185/60/005/001/009/018 Z 7- Yj 12 7.3 A151/AO29 .20 Korsunslkyy, M.I.; Borovykova, H.P. The Effect of Very Small Admixtures of Antimony on the L-Series of ~,he X-Ray Spectrum of Germanium --'.OD.'-.CAL- .'ikrainslkyy Fizychnyy Zhurnal, 1960, Vol. 5, No, 1, pp. 88 - 93 M.T. In Ref. I the authors reported on the effect of small admixtures of Ivon, obalt and gallium on the L-series of the X-ray spectrum of a germanium single crystal. The aim of thIsInvestigation is to determine the relationship ~--tween the value of the displacement4EB6 -AI12 and the concentration of admix- r,ures in Ge. The four lines (emission bands) of the L-series of Ge Lcq'.2, LA5, 16,, aad T_-(5 (Ref. 1) were investigated with the aid of a high-vacuum X-ray spectro- S,aph fit ed with a bent crystal of mica, as well as by a mixed method of X-ray pe3t-im exciTation. The curvature radius of the mica crystal was 1 m. The ?-F~italls work surface was 10 x 40 mm. The X-ray tube and the spectrograph had 171in'',n Va~.IWJM. The speo Ifu-M. recording ~as effected by a photographic method ~-N .'Ilm Ag-L'a Isopan F - DIN.: The operation conditions of the tube- tension c~r, current 4 - 8 ma. 19he linear dispersion within the reflection angle range -1 32 Xmm , the energy dispersion was 3.68 ev - mm-1. The photometric measure- d 1./? A 86810 s/185/6o/0o5/ooi/oo9/oi8 A151/AO29 The Effect of Very Small Admixtures of Antimony on the L-Series of the.X-Ray Spec- trum of Germanium. ments of the spectrilm were oarried out on the ft-4 (MF-4) m1crophotometer with a magnification coefficient of I x B. Each speotrogram was photometered three U_r-*38 on a different height of the lines. Three spectrograms were made of eaca of germanium single crystals investigated. It is shown that an introduction of mony in the quantity of jo-3 _ 10-2 atomic percent into the Ge single crystal causes a displacement of the line L& in relation to the line W1.2, and a din- placement, of the line L15 In relation to the line LPj of Ge by the value I - 2 ev, The value of the displacement,& Ep6 -A 1.2 is proportion4l to the cubic root trom the concentration of the admixture atoms. A displacement of the lines 10(j.2 and Lh to -the short-wave direction was revealed which points to the displacement of the 1 vels Ml- P 7, V with regard to the levels LIIj and LII. This displaoement., how- ever, is considerably smaller than the displacement of the level N, with regard to M The width of the lines depends upon the concentration of admixture atowiv,it-he germanium single crystal. A linear relationship was established be- tween the increase in the width of the line and Y-F. There are 6 figures, I table and I Soviet reference. ASSOCIATION:.Kharkiv, Politekhnichnyy instytut im. V.I. Lenina (Kharkov, Polytech- i' Institute lenj V.I. Lenin). Card 2/2 9MTTED; July , 959 (-.-Xojj5Ujja&jjj_X._Lj LITVINOVAI L,B#; BOROVIKOVAq G.P. Influence of small amounts of gallium on the position of the I ' and L emission lines of germanium. Fiz. tvers tels. 3 no 1-M-283 ja & (NIRA 14:3) 1. Khartkovskiy politekbnicheskiy institut im.V*I.Lenina. (Germanium--Spectra) KORSUNSKIY, M.I.; PASIIJSHUK, H.S.; MOKHOV, G.D. Wainating the effect of nonphotoconducting layers in studting the photoconductivity of layers of amorphous selenium with meicury ad- mixture. Fiztveretela 3 no.5:1366-1370 W 161. (KmA 34:6) 1 I* Khartkovskiy politekhnichookiy inatitut, imeni V.I.Lenina, (Photoconductivity) (Selenium-Electric properties) IWA ct,*/77 /40'399 ), (" .'V* )_ I 28084 S/18 61/003/009/016/039 B102YB104 AUTHORS: Korsunskiy, M. I., Pastushuk, N. S., and Alokhov, G. D. TITLE: A new type of photoconductivity PERIODICAL~ Fizika tverdogo tela, v. 3,no. 9, 1961, 2667-266a TEXT: The authors discovered a new type of photoconductivity in mercury- doped selenium., They studied the dependence of this photoconductivity on wavelength andintensity of illumination. The specimens were irradiated with monochromatic light in a vacuum chamber (10- 6 mm Hg) and the photo- conductivity change was recorded by a loop oscilloscope. The curves a = f(t) for illumination wavelengths between 0.425-0.715P. were taken and dark conductivity was measured. It was found that upon illumination with A 0.535~1. conductivity did not change, at A > 0.535pit increasea and at A 0,535t.4 it decreased. The transient period of a steady conductivity is much shorter in illumination with short-wave light than in illumination with light of longer wavelengths. On illumination with any monochromatic light (except for X = 0-425~0 the photoconductivity of the specimen Card 1/4 28084 S/181/61/003/009/016/039 A- A new type of photoconductivity B102/B104 decreases during 2-3 min. This decrease is tile stronger, the longer the wavelengthq howeverg it never exceeds 5%. This new photoconductivity is termed quasisteady dark conductivity and may be regarded as a new effect. Observations made during 2 hr showed that it did not change. It was found by measurements that the strongest conductivity changes occur upon -4ff illumination with wavelengths between 0.610-0.490~t(intensity 10 /cm 2). In some specimens they were even of one order of magnitude. In the intensity range 1*10-4 _ 801,10-4 W/cm2 and in the range of the Arange 0,420-0-71* the amount of the quasisteady photocurrent was independent of the intensity. There are 2 figures, 1 table, and 1 Soviet reference. ASSOCIATION: Kharlkovskiy politekhnicheskiy institut im. V. I. Lenina (Kharikov Polytechnical Institute imeni V. I. Lenin) SUBMITTED: April 7, 1961 Card 2/4 ff 0 0 Odftj,~ //x wo) S/16IJ61/003/01*0/030/036 B1251BI02 AUTHORs Korsunskj".. i. TITLEs Nature of a new type of photoconductivity PERIODICALs Fizika. tverdogo tela, v. 3, no. 10, 1961, 3181 3186 TEXTs M. I. Korsunskiy,'N * S. Pastushuk, and G. D. Mokhov (FTT, UIP 90 1961) reported on a new type of photoconductivity in mercury doped selenium samples. The photo-response is independent of light intensity used but depends on its wavelength. The transient period of the photo- response will decrease with increasing light intensity. This paper tries to explain this phenomenon. This new type of photoconductivity will occur when all other- carri er-recombinat ion mechanisms are of such a small probability that the recombination induced by light plays the principal role* The photoconductivity is assumed to be of hole type. Then, the 0 concentration of free carriers is given by no a cxp/hVpj, where the rela- tion (dn/dt) excit 0 (dn/dt )recomb is valid. Eq. (4) yields the ex- pression ao a euno for the photoresponse, where u denotes the carrier 29700 S/181/61/003/010/030/036 Nature of a new type of photoconductivity B125/BI02 0 mobility, e the carrier charge, n the equilibrium concentration of ' . 9 1 electron traps, a the quantu m yield, ~ the absorption coefficient, y. the frequency of exciting light$ and r a coefficient dependent on the wave- length.The author investigated the type of photo-response obtained when changing from a monochromatic. light with a wavelength to such with a wavelength >-2 for the following two casest a) n 9~~n and b) n.. a no At the-inatant of changing the.,following expressions are valids cot (8a) 1301:=eu When'ohanging frop'l to 0 01 I d* T 7t TIR,, (Ooi am). I d Card 2/3 011;01~0 (0., KjR3UN3KIY, 11. 1., LOGUNJV, A. S., and BAYVIL, L. P. ------ IlThe Application of Radioactive Isotopes for the Control of Parameters -if Moving Wet Steam" paper prejented at the All-Union Seminar on Application of Radioactive Isotopes in k1easurements and Instrument Buildin6, Frunze (Kirgiz SSR), June 1961) So; Atormiaja Lnergiya, Vol 11, No 5, Nov 61, Pi) 468-470 B10481611025100610091009 B104/B202 AL.L~HORS: Korsunskiyt M. 1.t Genkin# Ya. Yo. TITLE: Device for correcting the shape of emission spectra PERIODICAL: Akademiya nauk SSSR. Izvestiya. Seriya fizicheskaya, v. 25, no. 8, 1961, 1013-1016 TEXT: The present paper was the subject of a lecture delivered at the 5th Conference on X-ray Spectroscopy at Khartkov, January 30 to FebruarY 4, 1961. The authors studied the scheme shown in Fig. 2 for taking account of the distortions of the emission spectra caused by the apparatus and the width of the inner levels. By means of these scheme fi relation f - !:E b F (i . 192# ... s), where 11b 11 is a certain i k=1 ik k ik transformation matrix and Fk the ordinate of the experimentally determined spectrum. The elements of the matrix 11bikIl are produced in the form of resistors rik consisting of manganin wire. The device consists of n the authors determine the rectified ordinate of the spectrum using the Card 1/7 3/048/61/025/008/009/009 Device for correcting the shape ... B104/B202 cells. Each k-th cell contains s resistors corresponding to the elements of the k-th column of the matrix and which are connected in series. Furthermore# each cell contains a d-o source, a tuning potentiometer, a load resistor, and a resistor having the same resistance as the instrument measuring the amperage in the cells. With the aid of the tuning potentio- meter an amperage is tuned in each cell which corresponds to the value of the ordinate at the k-th point. Thusp a voltage drop V ik ' rikik = ab ikFkoccurs in each cell where a is a constant of the instrument. Hence, the sum of the voltage drops in all i resistors of the cells is proportional to the value of the ordinate at the i-th point of the rectified curve; n Vi - kM.:1 vik - a fi- Fig. 2 shows the scheme of this device. As can be seen, each matrix element is connected with an immobile contact panel which sums the voltage drops at the matrix elements 11, 12, 13, .... f It23. I.e., the voltage drop proportional to fI is calculated. This voltage at the ends of the resistors 11 and 1,23 is applied to the mobile contact of the compensating Card 2/7 S110481611025'00610091009 Device for correcting the shape ... B1041B202 potentiometer and its central point. If the voltage drop at the potentiometer between the central point and the mobile contact is not equal to that at the ends of the elements 11 and 1923 the galvanometer needle is deflected to one side or the other. By means of a motor the mobile contact of the potentiometer is adjusted such that the galvanometer needle again indicates zero. In this case the voltage drop at the potentiometer is proportional to fl. The position of the mobile contact can be exactly read on a scale. After the determination of f, the mobile contact panel is adjusted to position 2, in which the summation of the voltage drops at the resistors 21, 22p 23P .,..p 2.23 is made. In this case the voltage at the ends of the resistors 21 and 2,23 is applied to the compensating potentiometer. This voltage is compensated according to the above scheme, with the value of the rectified coordinate being read at point 2 of the scale. A scheme representing a (11,23) matrix and serving for the direct correction of spectra from the microphotographB without transformation with respect to intensity was tested. Pig- 3 shows a comparison of a rectified curve with one calculated directly. The authors than% L. I. Lukashenko for valuable help and V. F. Balditsyn and Card 3/7 S1001611025100810091009 Device for correcting the shape ... B104/B202 I. A.-Belenko for the production of the device described here. There are 3 figures and 2 Soviet-bloc references. ASSOCIATION: Kharlkovskiy politekhnicheskiy institut im. V. I. Lenina (Khar1kov Polytechnic Institute imeni V. I. Lenin) Card 4/7 KORSOUNSKIY, M.I.; GENKIN, Ya.Ye. CorTected LA2 --emission band in pure niobium and its Compounds. Izv, AN BBSi,. Ser, fiz. 25 no.8:1028-1030 Ag 161 (MIRA 14:6 -.- . NJ obium--Spectra) %obium compounds-4pectra) ' KORSUNSKIY H.I.; GENKM.. la.Yee Botablinhing the Fermi boundaz7 from X-ray opectral eminoion bandso Isv. AN SSSR. Ser, fis. 25 no.8:1031-1037 Ag 161s (MIRA 3418) 1. Kafedra obshchey i skeperimentallnoy firsiki Kharskovskogo politekhnicheaka o inotituta ims Vil, laninat fl-ray opectroneopy) KORSUNSKUY9 Moieg lzrailevich; VERES, L.F., red.; MMCHKOVA, V.N., tekhn, red, (Optics, atomic structures and the atomic rrucleus] Optika, stroenie atomas atomnoe isdro. Moskva, Fizmatgiz, 1962. 516 p. (MIRA 15:6) (Optics) (Nuclear pbysics) ion-optical properties is described In fj_r_Fj_t_-ap"p`f`o-x-j`ffi`A 5 Ion UY --- UwV-rnwxx-- of linear distribution functions depending on two field factors and on the dimensions of the cylindrical torus. It is shown possible to Card 1/2