SCIENTIFIC ABSTRACT KITSENKO, A.B. - KITULESCU, I.

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CIA-RDP86-00513R000722920011-7
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S
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100
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November 2, 2016
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September 18, 2001
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December 31, 1967
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SCIENTIFIC ABSTRACT
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7 3/057J61/031/002/902)O15 The': ex6i tat dn of,olodii6iijois ib"464 112 B2W t 4/ A, -4 4 #wow(, '4` yj k o' f 4*0 a IMP d N 4160 e 77 44,t q - - IL to Ale Ql@ &)As its `isiriTOLTS 12 and Coo' j OA -density 44"Mriuin a tion of, a distribution.of the p and _Iun tb a t 'e" kind t('#, The, f unotions r depend :Tj. and IN (T.L@ &n&.Tj, are t1j# n ii of,; parti, andioulwand a /or p &1101 t mpone t ale 'trelb oitfivhich- or porp in.@ (2 out over all kinds of beam particles -J@J@;'Tho- summation n C 43 31/002/002/015 @/057/60 -4 W20204 Tie.: jxCitstion, ce"Olsitromaottio-", V A q,; Q.3 KI Volk Oc by -the plu", The f or' E: (Obtsin4d, th be obtaizia!,61* -when'."! Sy n the. form ten lot D, f ranov) @j denotes t tonsor f the d At. where by t are AVOW 2 the," 01 .0netint of'. 4X 94N 1,@ IA X- d: tbi sence 'nA t-ThO BUMMand F,4'4 is the arift-,1-7- ho at i 'k 0, k tj-swik,.@ 00 11 .10 partiales uged not be take j!m&1- motion of the @b the the '1*10city of the _Goa S, IsocounU@ where t IftC -.Car 444@LTF- /662/01 V010311002 BI 24) B204,, tan of-. Old ihoA 4 titt ho te&W@ @J Igo rowsp partiole did 2 T k4 0 3 2 2,w A (21T) f j* ore 8 wbere th4 ji, Nn A 4 , f Q 57@ Car& jW _ /000i ib3 2 ' Y 2 0 4 @D B1 24 to= 2 (2 T T jj@, IL N w, AW U2 gel ! e f Vs i S/057/61/031/002/002/0115 The excitation of sloatromapotto B124/3204 where' 1. 1,1(p.) is a modified B18801 funationt ISO 418/*j -sOj*j4)/yQk vh am W(s is the probability integral, In the further course of the work# equations are derived for the electron longitu4inal oscillations# the quasi longitudinal propagation "well as the Lou-oyolotron and magnotohydrodyna- mia waves. Vention is *ads of As 1. Akhiveserg V. V. Zholosayak*vq Ya, Bo ronborg# and Vs P, Dokuchayov, A, 1. Akhiyossr and T.;?.Alaksin are thanked for discussion and valuable advias, There are 12 references$ 10 Sovietobloo and 2 non-Soviet-bloo, ASSOCIATIONs Pisiko-takhaiabookiy institut AN USSR, Kharlkov. (Institute, of Physics and Toohnoloa AS UkrSSR, XMr1kov) SUBMITTSDI Vay 91 1960 Card 9/9 8/057161/051/602/00 3020/3067 i%5@04 in i@@4s 'and Stopanor 10, NO A iMMU&I t' kh6l Cho skoy fisikip vo 31y.no, 2gI It"it knowa 'that the anisotropy of the equilibriua diet butloh, &as& 0 a trons and ions with respect to velocity may lead Win o 9 paper deals %@.4th the Instability of an unbounded PlA sixi In h, goneous Magnetic field a Ir Ions with an equilibrium distriWti Olk @-ifuno iQ3% of 'the fogs (1) k occur- In-- the, plismat vh*ro n the dinsity of the Ions$ vj. and T" -"'the 0 -'perpondiou t and'pars, 1191 aomponentel respectively# of the ion - vol6cli The lons Wi h'the distributi a on Nmotion (1) have the same Larmor radlu r rob @@,"Whsre Q *Vc/Ma and X the mass of the Ions It is dws"Wolast 'Y 'C rd I p'- A 8925, 6/057J61/031/00 clotron instability in'r on& 3020/BO67 CY "it'h that disturbanass of a wavelength of the order of ro and frequencies- i are equal to or a multiple of the ey"frequenoy IJ are unstable (01010"nk, Instability) . The order of a tudo of the growth Increment, is ror for an 14-::1'.:th* first harmonics. It sAy U expected that the results obtained b r ba a Apo~ un ounded plasim vill be qualitatively also correct fo adia ti tr ?irst I the o at is studied vhere the thermal scattering of ion velocities' parallel to A can be neglected* goncet it may be assumed that 0 Wr(Y11). The Unnor o@f tho Aieleatrio constant In this *&#* has form (2) Ae N J, A,; 411031100210031015:1 8/057 cyclotion, Instability -4i 3026/2r;67 Ott 4-11-1@4.@ 9 - Sig=~ Pe - *NJF) z. 22 it SON ? @4@4' "@j' X -its &A 07. W "Jr 2 IA :'vhore 147 jl@vm A ion f 0 the,,.angle, t be us" the'. Wave @rsctor k and I k;, koded k@ -@'k*inQj kiro;. I iw3 ;Ja) 24 r 'On denotes, the diffe tiation with,rospoot to A4 (0+ Jr is. the oo4lox frequency.- Tho@ axis 03 Is parallel axis ot,A44 in the P1 '"a oi:t:@Ic--vio'*ors.k,&Ad 2 @If the slectr6no have Card:Ve'.' 89 00 /057 61vowooil. Vol 1DO20 B067 rF 4 060i @ek I '0 then solut Ong, U o vayes litAr" 120 Ot ii t; ILI 41 1411 d the ImabOT, Of the @h&ruPio# Abo@:Aov an are 1. 11 ion' for in equat this @-fsat-.l A I it too (is) '61051JOV031100 4@ Ton inotabl 3020/BO67 itheri @4` y If -it appears C/v 4, "1 U11 4 This* Is 62@ffi froj ,j ts-tho @when th fir" t,"i nd nd -oiitignd a' greater than the 8400 F j A sb@Js-,dea w ereAM thermal motion of the ions is C Finallly the .6 It ko simplioity Awation @ro (Vit) 10 SAamed to i of Xazt 7F, A @c* -+/-=exP 777r7 2 Ott rd 5/8 A. "T": S- azz, 8"57 61 031 c Al 162 2 Aa- cyclo roll, 444uition Gassi @4?.)-- di iYo -,,tv 112, .0i tjj;@% @,- Sol 1-14 00 is I 71 AUTHORs Aitseak9j- A. B- TITLIs Character of the instability in the interactiori of a be" with plasma in an outer magnetic field )61 1270 - PERIODICALs Zhurbal tokhniobeskoy fisiki, v. it, no. 10, 1< 0 127? TEXTs A convective instability can only be eliminated if Jis zharaotor is known. This article deals with tht excitation of h-f long;.tud1nal:#lootro13. oscillations during the passage of a charged particlo boam thr4ugh plasma in an outer magnetic field. Tbe resulting instability 110 :onv&q)t1vv in the absence of a magnetic field (Ref- @. eve btlow). A sizilar Instabillty occurs in an outer magastie field duo to cyolotron vxcitati6z on th# basis of the anomalous Doppler effect* This instaoility to Investigated.in tht following. Integrals of Vbo form a(k) o dZ dev:rlte the electric and the magnotio field atr ngth and ean be used to dlotlmguloh between the absolute and the *OnVSOtiVG instability If this into Val % tends to zero for any constant rwith t 4 the inatabiAlIty Will be convective, and it it tend$ to infinity, it will be abPolute, "the IzOgrAV Card 1/5 Character of the Instability in the may also be written as ng of .fa[k(Wfl lei *hero C -the m,%pp) dt the real axis of the k-plane on the p'l ti n oThe va.'9@. mis t, which dWdk 0. are found from tht dispersion equation 0 tv 2 2 0 M 06(1 J@7 11)2 - 4,jos 0 2 _Q,2 WH where 0,, is the electron cyclotrOn fr4@-q.;,roniyj -a theq2ngmuir frequencies of plasma And boaml 9jis the arg.- bf.@Wi?ell a ], - a it and 'I. The dispersion equation show4 that C cuts vhdi :vag,car/ Ixld 0 only in 4- 0* The contour C can be deformed such that it '.@Oz in.z@tv lower somiplano 0, 1 1 a. . that the in togral f or t-#, - %&Ldo to 2*t ro N. Stapanov, R. V. Pol6vin, and V. a. tihapiro hre that-kel f@-r d-19cae sione. There,are 5 rof*roncest 3 SovIet and 2 non-Jovi*t 9*40 Ya. B. Paynberg st.al, ZhTIP. U,6530, 1961. The tw,. rolfvrrn@;** to English-language publioations read as followst Ref, Is F@ A, Szurrock,,. Phys. Rev.0 j_Ijj 14881 19561 Rof. 21 P. A. Sturca,:k, Phys. Rev_ Card 2/3 S*We'2606 7" A 8/056J61/040/006/027/031 312@[B@02 @409, 17L4 AUTHORS: Akhiyetert A4 I.j Kitsenko# A. Do, 4tePnoVo Ko 9. TITLE: Interaction between charged partial* currents and low-frequenoy,plasma oscillations PERIODICAlt Zhurnal skeporimentalinoy I tooretiobeskoy tizikip v- 46; no* 6p i0i, ie66-im TEM., The-authore deal with the interaction between a compensated be of charged particles and the low-froqueney oscillations of a plasm (mainly with the magnsto-scoustic waves and the Alfvln waves) In a t of constant field in Wallel direction to the basis and In the absence collisions. It the plasms, is rarefied to such an *xtent*that the frequency W of the oscillations is such higher than.th# frequency Ift the collisionotthe plasms, oscillations must be des@kbod on the basls-.@@f the kinetic equation With wt