SCIENTIFIC ABSTRACT TELKOV, N.A. - TELKSNIS, L.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001755210018-1
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: July 16, 2001
• Sequence Number: 18
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

f - - - - 21i 1 11
'T - -, I ~- - - - -
TIMY, N.JL., kandidat meditsinskikh natik (Novosibirsk)
-
Knife wound of the heart. Yest.khir.75 no.6:114-115 Jl '55.
(HEART-WOUNDS ABDINJURIMS) (MLRA 8:10)

TWZOV, N.A.,kandidat meditainakikh nank.
Technic of closing an intestinal stump using a gastrorrhaphiatome.
Vast. khir. 77 no-1:99-103 Ja 156 (WIaA 9:5)
1. Is Mirurgicheskogo otdalaniya (zav.-N.A. Telkov) 9-7
Havosibirskoy bolinitsy.
(DUM30M. surg.
closure of stump with gastrorrhaphiatome)
(SMGERY. appar. and instruments
gastrorrhaphiatome, use in closure of duodenal qtuxp)

Doc Med Sci (dies) -- "A comparative evaluation of various
methods of intestinal suture in reparing annatomosin under experimental OTYI
clinical conditions". Novosibirsk, 1958. 25 pp (Tnat of Surgor-j im A. V.
Vichnevokiy Acad wa Sci USM, and 11ovonibirsk Mod InBt), (KL, ITO 11 1959,

TZMV, N.A., kand. med. nauk
Wound-retractor and a slight variation of suture inexophagoenteric
anastomosis. Xhirurgiia 34 no.3.117-118 Mr 158. (KUA 12:1)
1. Iz kafedry gospitallnoy khirurgii (zav. - prof. I.L. Bregadze) Novosi-
birskogo maditsinakogo instituta na baze 9-y bollnitsy (glavrqy vrach
V.P. Tatar oentsev),
(GASTRWTOMY
with eaophageal-intestinal anastomosia; wound dilator &
suture variation (Ras))
(RSOPHAGUA, warg.
esophageal intestinal anaotomosis in gastrectomy, Vound
dilator & suture variation (Rae))
(INUSTINES, surge
same)

TELKOV. N.A.. kand.mod.nauk (Novosibirsk, lirovskiy r-n,ul.Stanislovskogo d.6,kv.7)
Comparative evaluation of various methods of intestinall;uturing
during anastomosis healing [with eummar7 in Inglish, ps 8-1591.
Vestakhire 80 nool:82-95 JS 158. (MIRA 11:4)
1. It gospitallnoy khirurgicheskojr kliniki (zav. - prof. 1.L.
Bregadze) Hovosibirekago meditsinakogo institute na base 9-y bollnitey
(glovrach - V.P.Tatorintsev)
(OASTRF,GTW
enterorrhaphy, tec7hnic (Rug))

TALKOV, N.A., kand.med.nauk
Repeated stomach surgery. Sov.med. 23 no.7:121-123 Jl '59.
(MIRA 12:11)
1. Ix khirurgichaskogo otdelenlys (zavo - N.A.Telkov) 9-7
Novosibirskoy gorodskoy bol'nitay, (glavW vrach V.P.Tatarintsev).
(STOMACH surgery)

TP~V, 1,T.A- (rovosibirsk, Kirovskoy r-n, ul. Stan i slavsk oco, d.6, kv.7)
Resection of the stomach in situs inversus viscerum. Vest.khir.
no.72122-123 161. (MIRA 15:1)
(STCMACH-SURGERY) (VISCERA-AMORMITIES A14D EEFOWITIES)

TELKOVI 1,.A -!,,, doktor med.nauk
Suturing of perforating gastroduodenal ulcers with a chain-like
seromuscular suture. Vest.khir. no.9:121-123 161.
r (MIRA 15:3)
1. 1z gospitallnoy khirurgicheskoy kliniki (zav. - prof. I.L.
Dregadze) Novosibirskogo medi-~minskogo instituta na baze 0/-7
bollnitsy (glavnyy vrach - B.P. Kanygin).
(PEPTIC ULCER) (Siumm)

TELKOV, N. A. (Novosibirsk, u1. Stanislavokogo, d. 6y kv* 7);
N. s.; somovi, G. s.
AutopInsty of the femoral artery with a venous transplant in
gunsh(-, injuries. Vast. khir. no.12:85-86 161.
(MIRA 15:2)
1. Iz '.ravmatologicheakogo otdeleniya 9-y Novosibirskoy klini-
obaskoy bollnitsy.
(FEMORAL ARTERY-SURGERY)
(VEINS-TRANSFLVITATION)
(GUNSHOT WOUNDS)

Y2 1
TELKOV, N.A.
T=oro of the mediantin= in children. Grud, khir. 3.no.2:115-116
161. (MIRA 1414)
(MEDIASTINUM-TUMORS)

mwzl qt-q N&Pmjg
R

TELKOV.. N.A.., doktor med.nauk
inadequacy of suture of the duodenal stuap and gastric resection for
the exclusion of ulcers. Sav. mod. 25 no.9:312-3-15 S I ~mim 15:1)
1, Is kafedry fakulltatskoy khirurgii lechabnogo pediatrichookogo
i sanitarno-gigiyenicheskogo fakullte%ov (zav. - doktor med.nauk
N.A.Telkov) Omakogo moditsingkogo instituta (dir. - prof. I.S.Novitakiy)
i Novosibirskoy 9-y Gorodakoy bol'altay (glavny7 vrach B.P.Konygin).
(STO&CH-SURGERY)

TET-KOVY N.A.
A n at unu' c a I and h'i t- tol ~p! ~tk 1. dE, Ii ch az I ng exr-2rimnta I
4,~, -64
.6- v3t,,- nal i)uture3. Eksper. kh'r. 1 7 n0.5;63
S-0 162. (MIRA 17;10)
1. 1z kafedry fakull tetslcoy kh,' rurgil prof. N.A. Tclkov)
Astrakhazmfkogo

Milli
TELKOV, N.A., prof. (Novosibirsk., 100 ul. StaniBlavskogo, d.60kv.7)
Use of the 8-shaped suture and hepatic clamp in resection
of the liver. Vest.khir. 90 no.304-58 Mr'63. (fMiA 16slO)
1. Iz fakulftetskoy khirurgicheskoy kliniki (zav. - prof. N.A.
Telkov) Astrakhanskogo meditainskogo instituta imeni A.V.
Lunacharsk-ogo (rektor - dotsent I.N.AloyMarov) i Novosibir-
skoy 9-y klinicheskoy bollaitay (glavnyy vrach - A.I.Fedorova).
(Livmt-~UWJEU) (SUIWM)

TELKOV N A prof. (Novosibirsk)
ltt~~s
Review of V.A. Malkhasian's Look "Technique of operations on
the stomach." Vest. khir. 93 no.11:133-.135 11 164.
04IRA 18: 6)

MZAYEV, A.P., dotsent (Leningrad); TELKOV, N.A., prof. (Novosibirsk)
Reviews. Vest. khir. 94 no.1:155-159 Ja 165. (MIRA 18:7)
il,

u
TElI,KOVY V.P.
Aa~xlysis of the ~a-~;nes of death of pat!en*.5 ;,nu have
c',-olecystltAs oreration3. Tmdy U-GiC- ?4:160-164 162. (MIM 1": .10)

ussR/Microbialotff - Microbes Patho-enic f:ir Man and Animals. F
0
Dacteria. tacteria of V2e Intestinal Group.
Abs Jour Ref Zhur Biol., No 22, 1956, 99356
Author
Inst
Title On the Problea of t~e Lab,)ratory Diatno6la of Somie
Dysentery.
OriG Pub Zodravookhr. Belorussii, 1958, No 4, 38-40
Abstract No abstract.
Card 1/1

. : 1 .1 . . . - I I- ~- , -~,- "" Lly - P-4
TELKOVAI K.A*, h!ed Oc! - (disb) "Clinical and laboratory
diagnosis of onneipVdysentery." 1zhevsk, 1959, 21 pp
(Izhevsk 3tate Med j~mt) 200 cot.-ics M, 33-59, 122)
- 74 -

TEZOVAO L.A.
New data on the mode of food intake in the flagellates of the
getius 117nchoxonair.. Mol zhur- 43 no.4t6O6-607 "64
(MIRA 170)
1. Sevastopol Biolrgical Station,, Academy of Sciences of
Ukrainian S.S.R.p Sevastopol.

TELKOVAt L.P.
27673 DRABKIKAI B.M. I TELKOVAs L.P* Zrolost' polovykh produktov
U samok kubsmkoy sevryugi I leykotaitarnaya formla krovi.
trudy laboratorii oanov rybovodstva,, T. 119 1949, a. 258-61.
Bibliogri 6 nazy.
SO: Knizhwa Letqpia., Vol, 1., 1955

TZLKOVA, L.P.
__ _Www"MAP",
Stimulating ovulation in fish. Vop.ikht. no,2:112-].13 154.
(KM 8:5)
lo Moskovskiy tekhnicheakiy institut rybuoy promyshlennosti i
khozyaystra Imeni A.I.Mikoyans, - Hoorvbvtuz,
(Ovulation) (Fishes-Physiology)

ACC NR; AP6014263
SOURCE CODE:
UR/0153/66/009/001/000'3/0064
AUMOR." Koz1ov, L. M.; Bmmistrov, V. I.; Tolkova.-.T. F
ORG.' Dezartment of Chemistry and Petroleum and Gas Technology,, Kazan Chemical Engin-,
oaring 1~stitute im. S. M. Kirov (Kafedra khimii i tekhnologii nefti i gaza, Xazanskriy
khimiko-takhnologichaskiy institut)
TIT12: Synthesis of Ditrga" esters of bgric acid
SOURCE: IVUZ. Khi=:Lya i khimicheskaya tekhnologiyat v. 9, no. 1,, 1966, 63-64
TOPIC TAGS: borate, boric Acid, alcoholy organic nitro compound
j'CSTRP.CT: The reaction of boric anhydride with a series of primary, secondary, and
tertiary nitro alcohols was studied for the first time. The alcohols used were 2-
nitroethanol, 2-nitro-l-propanol, 1-nitro-2-pro-Danol, 2-nitro-2-methyl-1-propanolo 2-1
nitro-3-butanol, 1-nitro-2-pentanolj, 2-nitro-2-'mothyl-3-butanol,.3-nitro-2-pentanol,
1-nitro-4-methyl-2-pentanol, and 1-nitromethyl-i-cyclohexanol. Primary alcohols re-
acted with boric anhydride more readily than secondary ones. 7he reaction of ter-
tiary alcohols was the most difficult. Under the same conditions, the yiold of nitr-
alkyl borates decreases with increasing molecular weight of tho nitro alcohol. The
tris-nit'roalkyl borates obtained are very sensitive to hydrolysis and hjdro3,,fze in
moist air, but are stable when heated to 200-2200C. Orig. art. has: 2 tables.
SUB COrZ.- 07/ SUM, DATE: 09Dec63/ ORIG RFF: 002
Card 1/1 UDC t 3!~' ?,~E

SADYKOVAp F.Nb.; MOROZOVSKAYAp, I.S.1 SEDOVA,, G.V.; TFaIOVA,_,Tej.__
Optimum size of strips used in determining tearing loads for
textile fabrics. Standartizateiia 25 n0-113"3 A 161.
(MIRA 34%3)
(textile fabrics-Testing)

SOBOLIP S.I.; NEUN'p I-M-; SPIRIDONOVA, V.I.; BMINp Z.L;
GORYACMUN, V,I.; TARAUNOV, B.M.; SHKRSKIY, V.D.; Prinimali
uchtatiye: FREYMAN,, A.K.,, inzh.; BRUK, B.H., inzh.;
CHEBOTKEVICH, G.V., inzh.; OSPIN, V.G., inzh.; ALEKSANDROVAp N.N.j
laborant; SALTYKOV, I.B.,, laborant;.-MLKOVA,, Yq.~Aj_laborantka;
TEMAKOV., TuAl laborant; GAVRILZUKO, A.P., slesarl;
KURGUZOV.. A.S.,, eaektrik; GAVRILOV,, I.T., elektrik
Pilot-plant testing of the State Institute of Nonferrous
%tals flow sheet for the autoclave retreatment of copper-
mo3,vbdonum intermediate products. Sbor. nauche trud. Gin-
tsvetmeta no.19:319-339 162. (MIRA :L6:7)
(Nonferrous metals-Metallurgy,)
(Leaching)

LIPKOV, I.A., kand.takhn.nauk; GRECIRWHINA, N.A., inzh.; TELKOVA, Ye.I.;--.,
SAVINA, V.N., tekhnik
Processing of the new types of synthetic fiber yarns (in mixtures
and as such) in the manufacture of krit goods. Nauch.-issl.trudy
VNIITP no.4:118-141 t63. (YdRA 17:4)

TELKOVA, L.P.
Conpletion rX 3pawning stocY of t-I'le RI'd 7:!an4'na7lFL:'
herring at the expens- cf the high-yiel! generat.,cn of 1950.
Trudy PINRO r-,-,.!4il41-149 162.
(!,ITR.A 17-10)

LIPKOV, I.A.; GRECHUKRINA, N.A.; TEMOVA, Ye. 1.
Developing the technology of knit outerwear production from
ImIked synthetio yarnz.Haueb.-issl. trud7 VNIITP no. 5t62-79
164 (MIRA 19il)
1k I
V

- - ~:4

Caiegory : USSIt/Photoeffect - Electron and Ion Imission H-2
Abtj Jour: Ref Zhur - Fizika, No 1, 1957,No 1653
Author : Tellkovskiy, V.G.
Atle : SecorMary EWRFF-on Emission from Metals Under the Influence of Ions and
Neutral Particles.
Orig Pub : Dokl. All SSSR, 1956, 108, No 3, 444-446
Abstract : An investigation was made of secondary electron emission of metals under
the influence of h-pdrogen, helium, nitrogen) neon, argon, molybdenum, and
neutral atoms of inert gases with energies from several to 120 kev. The
investigation was made with a mass spectrometer, and the pressure of the
residual gases in the target region did not exceed 3 x 10-8 mm mercury.
The target surfpce was purified by heating to 2500 -- 3000P K and its purity
Vas monitored dixr:Lng the measurement by checking whether the secor4ary elec-
tron emission coefficient t r ined independent of the density of the stream
of bombarding particles. The targets employed were made of Mo, Zr, Ni, Ta,
Cu and graphite. Fj rience has shown that r increases linearly up to parti-
-we
cle speeds of 2 x 10 cm/sec, followed by a gently-oloping maximum followed
in turn by a smooth decrease. In all cases, a threshold of secondary elec-
tron emission is observed in the 0.5 _- 2 x 107 cm/sec range. The investi-
gation has shown that the secondary electrons have a VAwellian velocity dis-
tribution. The average energy of the secondary electrons is independent of
Card 1/2

Caiegory : USSR/Photoeffect - Electron and Ion Rmispion
Abs. Jour : Ref Zhur - Fizika, No 1, 1957,140 1653
the energy of the incident particles. The proportionality of Y to the
number of particles contained in a molecular ion suggests that when the
ion approaches the surface it decomposes and interacts aa the sum of in-
dividual ions. The value of Y depends only on the energy of the incident
particles and not on their charge; consequently, the theory of the po-
tential breakaway of electrons does not agree with the fact.
111-2
Card : 2/2

[,r~ -1
T-raymysmay, V., moseaw
"The Electron Liberation From lttallic Targets by the Impact of
Positive Ions and Atons," a paper presentcd at the Third International
Conference on Ionization Phenomena in Gases, 11-15 Jwl 57, Venice.
~-k': B-347,498

AUTHOR TELIKOVSKIY V.G., PISTUNOVICH V.I. 20-5-25/6T
TITLE The Transiti on--of Ions of Different Gases Through a iian biiyer
Foil. (Prokhczhdeniye lonov ra2lichnykh gazov cherez ton'kuyu
serebryanuyu tollgu.- Russian)
PERIODICAL Doklady Akademii Nauk SSSR 1957, Vol 113, Nr 5, PP 1035-1038 (USSR)
ABSTRACT The authors of the paper under review developed a method with the
aid of which it is possible to obtain a thin silver foil (thinnoss
up to 40 millimicrons), and investigated the transition of ions
of He+, H+, C+, N+ and 0+ through the foils of a thickness of 40 to
60 millimiorons. The dimensions of the crystals must be oonsiderab-
ly smaller than the thickness of the foil. The manufacturing and
production of the foils are discussed in great detail. The investi-
gattons were carried out with the aid of a device of the type of a
large magnetic mass spectrometer of a length of approximately 5 m
and with a rotation of the bundle by 25 degrees. An arc discharge
in a longitudinal magnetic field served as ion source. The density
of the ion current in the neighbourhood of the slot of the gas dis-
charge chamber amounted up to 100 milliamp4res/om2, and it was
possible to continuously regulate it during the operation of the
device. The receiver is surrounded with a copper cover at the
temperature of liquid nitrogen. The energy lose of the ions at the
transition through the foil was determined by means of the method
CARD 1/2 of the retaining potential. The measurement errors remained below

20-5-25/6
The Transition of Ions of Different Gases Through a Thin Silver
Foil.
CARD 2/2 1 %. The principles of the construction of the receiver and the
measuring arrangement are clearly represented in a diagram,
The results of the measurements of the dependence of the energy
losses and of the velocity of the ions H+ and He.+ upon the mean
velocity of the ions are shown in two diagrams. A chart contains
the threshold values of the energies and of the velooities at
whioh a transition of different ions through a silver foil of
a thickness of 55 millimicrons is observed. If the velocities are
the same, the velocity losses are equal (within the limits of the
measurement errors) for all atomic ions investigated. The essential
element in the meohanism of the energy transmission is the velocity
of the ions going through the foil. Finally, the paper under review
gives an estimate of the number of the neutral particles leaving
the foil for H+ and He+ at 9 > 25 keV and of the remaining ions
at the threshold energies. This estimate, however, has only a
qualitative character. As far as the ions He+, C', N+ and 0+ are
concerned, the neutral atoms are predominant in the energy interval
investigated (approximately 70 to 80 % of the total number),
(3 reproductions, I chart)
ASSOCIATION: not given.
PRESENTED BY: L.A. Artsimovich, Member of the Academy, 14,12. 1956
SUBMITTED., 5-11- 1956
AVAILABLE: Library of Congress.

0.
88433
$10561601039100610221063
>1 B006/BO56
AUTHORSs Ioffe, M. S., Sobolev, R. I., Tellkovskiy, V. G.,
Yushmanov, Ye. Ye.
TITLEs Investigation of the Confinement of Plasma in a Trap With
Magnetic Plugs
PERIODICALi Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 39, No. 6(12), pp. 1602 - 1611
TEXTi A report is given on plasma confinement in a cylindrical magnetic
mirror which is some 10 cm in size. The experiments were carried out with
a hydrogen plasma having a mean density ofvl.1090M-3, at a minimum
pressure of the neutral gas of -,3-10-7mm Hg. The mean ion energy was
1 - 2 kev, the electron energy 10 ev; the magnetic field was 5 - 8 koe.
In this case, it is possible to reckon with adiabatic and quasineutral con-
ditions, i.e. the Larmor radius of tho ions is small compared with the trap
dimensions, and the Debye screening radius is small compared with the
region filled by the plasma. The greatest losses in fast ions occur as a
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88433
Investigation of the Confinement of Plasma in S105 60/039/006/022/063
a Trap With Magnetic Plugs Boo6yBO56
result of charge exchange with the neutral gas. The experimental arrange-
ment, in which the experiments were carried out, is shown in Fig.l. The
maximum field in the center of the trap (constant in time), was 8000 oes,
and in the plugs it was 12,400 oes, i.e. the plug ratio was 1.55. The mean
lifetime i of the fast ions in the trap was measured as a function of
pressure for different accelerating voltages, magnetic fields, and plug
ratios in the hydrogen pressure range of 3-10- 7 _ 2.10-5mm Hg. The ex-
perimentally determined I/T-values are, as shown, indeed linear functions
of pressure, as must be expected also of charge exchange processes. Also
the flux of fast neutral particles and therefore also the current of
secondary electrons in the range of 2.10-7 _ 3-10-6mm Hg is a linear
function of pressure. If pressure is reduced, the neutral-particle flux
tends toward zero (and not toward a constant value). Amonj the+processel
developing in the plasma, there may also be the process H + H 2-9,H + 2H
which fact has been pointed out by G. I. Budker. However, it was found
that the ion escape from the trap takes place much more quickly than would
be expected, if only charge exchange and scattering processes are taken
Card 2/4

88433
Investigation of the Confinement of Plasma S10561601039100610221063
in a Trap With blagnatic Plugs B006/B056
into account. Thus, additional losses of fast ions must be assumed, whose
time dependence was investigated. It was found that the losses not
connected with charge exchange decrease with time until eventually they
vanish completely. Such anomalous losses of ions are due to the presence
of plasma in the trap. If the density of the charged partJole is so low
that the Debys range is of the same order as the trap dimensions, the
losses are equal to zero. The authors thank Academician L.A.Artsim6vich
and B. B. Kadomtsev for their interest, advice, and discussions,
V. M. Petrov, E. N. Braverman, and Yu. T. Bayborodov for their technical
collaboration. There are 9 figures, 2 tables, and 11 referenoest
7 Soviet, 1 Swiss, and 2 US .
SUBMITTED: July 20, 1960
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88433
s/0'56/60/039/006/022/063
BOo6l.BO56
!z7
!+7 7 j 6
7 7 6
r z
Text,to Fig.Is 1) Coils for generatingothe magnetic field.. 2) Vacuum
chambe'r. 3) Titanium vaporizer. 4) Diaphragms. 5) Plasma 'source.
6) Receiving electrode. 7) Top fixture.
Card 4/4

T L / - i-I 0 *.~-,"--',I'!'" ~ Y-L-'-~
----TOL,KOVSKY) V. G. and GOTT Yu. B. and IQ-f,?E) N. S.
"Sorpe new results on the confinement of wgnetic traps"
Report presented at the Conference on Plasma Physics and Controlled
Nuclear Fusion, Salzburg, Austria, 4 8 Sep 6l.

22208
S/168/61/000/001/003/009
BIOS/B209
AUTHORS: Molchanov, V. A., Ttllkovskiy, V. G.
TITLE: A mass monochromator with double focusing in a sectorial
magnetic field
PERIODICAL: Vestnik Moskovskogo universiteta. Seriya 3, fizika,
astronomiya, no. 1, 1961, 22-28
TEXTs In the laboratoriya kafedry atomnoy fiziki Moskovskogo universiteta
(Laboratory of the Department of Atomic Physics of Moscow University), a
mass spectrometer has been designed which delivers an ion current of a few
milliamperes at an accelerating voltage of up to 35 kv. In this paper,
a similar device is described, intended for ion-beam experiments as well
as for the separation of small quantities of Isotopes. In work with high
ion-current densities, ion sources of an aperture of a few millimeters
must be used and, consequently, a dispersion of 1 cm for a relative mass
difference of 1% was chosen. The weight of the magnet which should not
exceed 2 tons sets a limit for the power of the sourca. The magnet of the
device under consideration was designed in the form of a sector with a
Card 1/6

21208
S11861611000100110031009
A mass monochromator with ... B108/B209
central angle of 670- In order to attain high current density and dis-
persion, an axially symmetric magnetic field with horizontal and vertical
focusing was used. In the calculation of the monochromator, the authors
employed Kalov's method (Ref. 4s Baranov S. A., Kalov A. F.,
Shlyagin K. N. PTE9 no. 1, 3, 1956). The edges of the field change the
angle through which the ion beam entire the sector, and shift the beam
sidevard, but both effects cannot be determined accurately. Therefore,
the authors used a field which is propo.~tional to r1/2 (r denotes the
radius of the sectorial magnet) in the center of the sector, since such
a field can accomplish double focusing for any r without astigmatism, so
that a lateral displacement of the beam is insignificant. The magnet
(except for the profile of the pole ends) was calculated in linear
approximation. The initial quantities were the dispersion, the maximum
energy (35 kev) of the single-charged ions (mass 200 absolute units), and
the angular divergence of the beam. The magnet is made of Armco iron.
Its windings are copper pipes through which water is conducted; the
current density in these windings reaches 6 a/mm2. The magnet is fed by
d-c of 100 a and 200 V, stabilized to 0.01%. The vacuum system (Fig. 1)
Card 2/6

21208
5/188/61/000/001/003/009
A mass monochromator with ... B108/B209
essentially consists of three sections, viz., the chamber with the ion
source, the monochromator plus ion ducts, and the fission chamber; each of
these sections is evacuated to 10-6 - 10 7 mm Hg by an H-2T (N-2T) pump
(2000 l/sec). The ion-source chamber is made of brass, and all the other
parts of copper. The ion-source chamber, the ion ducts, and the mono-
chromator are cooled by running water. The diaphragms 6 are made of
stainless steel. A special jacket in the fission chamber provides
nitrogen temperatures. By this vacuum system, a pressure drop by about
100 times could be attained between ion-source chamber and fission
chamber. The ion source consists of a water-cooled discharge cylinder
with a tungsten cathode which is heated by electron bombardment from an
incandescent wire. The electrons emitted from the tungsten cathode into
the discharge cylinder oscillate in the longitudinal magnetic field which
is applied between cathode and first lens, thus causing strong ionization
of any gas or vapor conducted into the cylinder. The ion beam is focused
by two lenses, the first of which has a negative potential with respect
to earth, and the second has earth potential. The high voltage was
stabilized to 0.01%. Such an ion source delivers a current of 50 - 70 ma
with a divergence of not more than 50. In essential, this source is
Card 3/6

212W
W188/61/000/001/003/0019
A mass monochromator with... BIOS/B209
analogous to that designed by L.A. Artsimovich (Ref- 71 "Atomnaya
energiya", 111, 483, 1957) et al. Since the exact deflection of the ion
beam could not be calculated, a stainless steel siphon (Fig. 1, no. 8)
was inserted between the monochromator and the second ion duct. Optimum
focusing was attained at an angle of 85 ; the distance between source and
magnetic pole end was 1400 mm. Ro)adings are taken from an aluminum screen
on which the focused ions leave clear marks. For a qualitative determina-
tion of the resolution of this derice, a mass spectrogram of Xe was taken.
The principal characteristic of tais device is the fact that dispersion
does not depend on the angle of deflection of the beam since the distance
between magnet and focus is diminished by_narrowin� down the angle. At a
voltage of 35 kv, a current density of 2 3 ma/cm may be attained at the
target. The high resolution and good dispersion permit preparing isotopic
targets of almost any element. The authors thank Academician
L. A. Artsimovich for interest, L. F. Malov for help in the calculation
of the magnet, and V. M. Kellman and D. L. Kaminskiy for valuable advice.
There are 3 figures, 1 table, and 7 referencess 6 Soviet-bloc and
1 non-Soviet-bloo.
Card 4/6

..........
S/18 61/000/001/003/009
A mass monochromator with ... B108%209
iki (Scientific Research Institute
ASSOCIATIONs NIIYaF kafedra atomn)y fiz
of Nuclear Physics, -Department of Atomic Physics)
SUBMITTEDs July 18, 1960
Card 5/6

212r-q
1/1 61/000/001/003/009
B108YB209
A mass monoohromator with... 8
Legond to Fig, 11 1 - chamber
-with ion source, 2 - coil
generating the longitudinal
magnetic field in the die-
charge cylinder, 3 - N-2T
pumps, 4 - window, 5 - ion
ducts, 6 - diaphragms,
7 - mass monochromator,
8 - siphon, 9 - fission
chamber.
Card 6/6

DUSHKOV, I.I.; MOLCHANGV, V,;A.,- TELIKOISKU V.G.- CHICHLROV, V.M.
3,
Some angular relationships in -.athode sputtering. Zhar.tekh.fiz.
31 no.8tIO12 Ag ,61.' (IMU 14:8)
(Sputtering (Pb7nica))

27168
S/057J61/031/009/308/019
B104/B102
AUTHORS: Gott, Yu. V., and Telikovskiy, V. G.
TITLE: Determination of the ionic energy in a high-temperature
plasma by means of thin foils
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 31, no. 9, 1961, 1061-1065
TEXT: The method of measuring the ionic energies and the energies of
neutral particles by means of thin foils is based on the fact that after
the passage of a ray through several atomic layers, the fractions of
charged and neutral particles within the foil do not depend on their
original charge. The main difficulty of this method lies in the
production of thin homogeneoug foils. The authors produced films by
sputtering silver at jo,5-jo- mm Hg on an aluminum foi.1 (2-3 p thick).
The silver was evaporated. The temperature of the L! base layer exerted
a great effect on the quality of foils. In the tests described the Al
base layer was kept at nitrogen temperature. After production of the
silver foil, the aluminum was removed with caustic soda. Then, the
silver foil was taken out from the solution with a very fine copper net.
Card 1/3

27168
S/05 61/031/009/008/019
Determination of the ionic energy in... B104YB102
TI--2 resulting foils had thicknesses of 100-2000 and a size of
2
10-20 cm . Their inhomogeneity was less than 4 After the ion beam
has passed through the foil with an energy below 20 kev it contained many
neutral particles. Behind the foil, an insulated collector was installed
in front of which a grid was arranged with a potential of +40 v against
the collector. Thus, both the ions and the neutral particles (due to
secondary electron emission) could be recorded. Since every foil is
porous, a certain current always reaches the collector at any velocity
of ions. The current to the collector increases considerably from the
ionic energy at which the ions begin to pass through the foil. This
energy is called threshold energy. Measuremento with hydrogen,
deuterium, and helium ions showed this threshold energy to 9 proportional
to the foil thick ese up to a foil thickness of about 1300 ~. At a foil
thickness of 100 1, the energy of hydrogen and deuterium ions can be
measured from 500 ev, that of helium ions from 2000 ev. The effect of
ion scattering was eliminated by use of a semiepherical collector,. Thus,
it was shown that the current to the collector may be well described by
Card 2/3

27168
S/05 61/031/009/008/019
Determination of the ionic energy in... B104YB102
Icoll aa (E - Ethresh),o; a . A/dn . d is the thickness of the foill A is a
constant mainly dependent on the coefficient of secondary electron
emission; n -0-85 for H+, 0.42 for D , and 0.2 for He o The following is
obtained for the determination of the integral spectrum:
E
max I(E)dE d (z 1 dI Coll
f a2 'oll dEthresh d'thresh'
Ethreah
The authors thank Academician L. A. Artsimovich for valuable advice.
There are 3 figures, 1 table, and 9 references: 7 Soviet and 2 non-
Soviet. The reference to the English-language publication reads as
follows: I. A. Phillipst Phys. Rev.9 21, 2, 404, 1955-
SUBMITTED: October 17, 1960
Card 3/3

AUTHORS:
TITLE:
PERIODICAL:
89202
8/056/61/040/001/007/037
B102/B204
Ioffe, M, Be, Sobolevp R. I.p Tellkovakiy, V. 06~p
Yushmanov, Yo. Ye.
Escape of plasma from a magnetic mirror trap
Zhurnal eksperimentalinoy i teoretioheskoy fiziki, v- 40,
no,, it 19611 40-48 1
TEXT: This paper is a continuation of an earlier paper (Ref - 1 in which
th� authors studied the retaining of a hydrogen plasma with a thickness of
10 Qm-3j which concieted 'of fast ions (1-2 kev) and slow electrons (-10 ev~
Anomalously fast escape of ions from the magnetic mirror trap could be foun4
which wan caused not alone by the charge-exchange losses. In order to got
to the bottom of this additional leakage, experiments were undertaken for
the purpose of a direct-meacurement of the fast ions leaving the magnetic
trap. The losses which occurred through the end walls, and which occurred
through the lateral walls were studied separately. For the purpose of meas-
uring the quantity of ions leaving the trap through the end walls (in the
direction of the magnetic fields) a sector-shaped metal electrode (1/6 of
Card 1/8
~.I'_ *,"JM

Escape of plasma
89202
3/056/61/0"0/001/007/07,7
B102/13204
the end-wall area), to which the -20 v were applied for the purpoue of pre-
venting an impinging of plusma eloctron3, was ueod. By moano of tho 31Pnalfi
omitted from the sootort tho charges conveyed to tho sector by ions were
measured. Fig. I shows the lateral and front view of the electrodes, as
well as the comb-like arranged 6-plate electrodes, by means of which the
quantity of ions (thus only that of the fast ions) could be determined ad-
ditionally and independently. From the recordings of sector electrode and
comb electrodes, the following quantities of fast ions
a 1.33 1-55 2.0 1 2-35
107 qseotj coult 3-3 8-7 12.8 10.8
107 (,tot coul. 46 125 200 200
and the following quantities of slow ions
Card 2/8

Escape of plasma ...
89202
8/056J61/040/001/007/037
B102/B204
1-8 3 3
8
10 coul. 5-5 19.0
Sect'
108 Qcombf ooul* 2.4 1 7.6
Qalow/Qfast' 5 1 ,v 15
could be found to exist. a -Hmax/Ho, qtot is the total charge inoiding
upon the two end wallej due to the additional escape mchanism. The quantity
of fast ions-inciding upon the lateral walls (perpendicular to the H-field)
was measured by means of an arrangement shown in Fig. 2. The electrodes had
a size of 298 OM2 and had a distance of 10 mm from the chamber wall. To the
measu.ting electrode a -20 v was again applied. The measurements yielded the
following results:-
Card 3/8

I-; ylg~ j! -'~' iI ".Awl ~Zr'~ '?q
11/056
/M /040/001/007/037
Escape of plasma B102/B204
a 1-33 1-55 2.0 2-35
106 Qside 0'-03 1-8 444 5-8
106 Qtot 1.9 5-3 16.3 23.2
qwall % 43 34 27 25
~tot again denotes the total charge of fast ions inciding upon the lateral
walls due to the mechanism of additional losses, q wall is the ratio of these
charges. Thus, up to 40% of the fast ions, leaving the trap in consequence
of the mechanism responsible for the additional losses, may do so through
the lateral walls. Fig- 3 shows a typical oscillogram of the current from
the comb electrodes (a) and from the side wall (b). The results of these
studies confirm the conclusions drawn in Ref. I with respect to the anoma-
louely high fast ion losses, The major part of these losoes, no less than
Card 4/8
V

PMOM
3/056J61/040/001/007/037
Escape of plasma B102/B204
80P,'is due to an escape to the aide wallst and only about 20%, to an escape
to the end walls of the trap.' The escape is nonst4ady, the ions are thrown
out from rddions not connedted with one another, whoae dimensions - perpen-
dicular to the magnetic'field - are small compared to the trap diameter,
whichp hoVevery, extend throughout the entire length of the trap along the
maUnetid field. There are 5 figurest 3 tables# and 2 Soviet-bloc refereneft
SUBIAITTED: July.20, 1960
Card 5/8
MI

Espape of plasma
31056
/61/040/001/007/037
B102/B204
Legend to,Fig. 1: 1 measuring elec-
trode (comb)l II fastening, III - dia-
phragm, IV - nectorp V - shield,
VI - isolatorl 1) cross section,
fl front view, 3) comb, 4) sector,
5 the comb-like arrangement of the
electrodes.
Card.6/8

3/056/61/040/001/007/037
Escape of plasma
Legend to Fig."' 2: 1) em'ergenoy eleotrodel
2) central arose section through the-trap;
6 diaphragm.
. ,meas-uringelootrodes;4
3
X-0 Im.1 #,vt
2 NX
Card 7/8 1"4 JLJ Q Jim
vl~

I
I
A
h
. I
. 8

S102 61/136/004/009/026
B019YB056
AUTHORSs Molchanov, V. A. and Tellkovskiy, V. G.
TITLEs Change in the Coefficient of Cathode Sputtering as a Function
of the Angle of Incidence of Ions Upon the Target
PERIODICALt Doklady Akademii nauk SSSR, 1961, Vol. '156, No. 4,
pp. eOl - 602
TFXT: The aut".ors priisent the results of a a-.udy of ti-a cathode
sputtering of polycry3tall'ine Cu specimena by argQn ions having an energy
of 27 key. The ions incided. at an angle of 0 - 84"'. Some of the Cu
specimens had a minimum of impurities, while others were produced from
commercial copper. The apurification of the surface was carried out by
annealing at 750 - 800 C, whereby the grain sJze increased somewhat. The
experiments were carried out with a device similar to a mass spectrograph
with double focusing of the io~ beam in a magnetic field. The ion beam had
a current density of 1-2 ma/cm , and the target was heated to nitrogen
temperature, the pressure round the target amounting to 1-2-10-7 MM Hg.
Fig.1 shows the coefficient of cathode sputtering for a perpendicular ion
Card 1/3

Change in the Coefficient of Cathode Sputter- 510201611136100410091026
ing as a Function of the Angle of Incidence B019/BO56
of Ions Upon the Target
incidence; Fig.2 shows the coefficient as a function of the angle of
incidence (curve 1). In addition, this figure shown the product of the
coefficient with the cosine of the angle of incidence (curve02). Thorough
investigations showed that up to an angle of incidence of 70 , up to which
the cosine law is satisfied (curve 2), the energy loss caused by particle
reflection vanishes within the accuracy of measurement. The increasing
energy lose above 70 0, caused by particle reflection, corresponds to the
decrease of the cathode-sputtering coefficient. The energy loss was
measured with a special electrode, to which a thermo,;ouple had been
fastened. Furthermore, it was found that apart from the energy loss caused
by particle reflection, also other factors must be taken into account for
the reduction of the cathode-sputtering coefficient. There are 2 figures
and 8 referencess 2 Soviet, 3 US, 1 German, 1 Italian, and 1 Dutch.
ASSOCIATIONs Moskovskiy gosudarstvennyy universitet im. M.V.Lomonosova
(Moscow State University imeni M. V. Lomonosov)
PRESENTED: August 17, 1960, by L. A. Artaimovioh, Academician
SUBMITTED: July 25, 1960
Card 2/3

S/020/61/136/004/009/026
10 B019/BO56
i~4
P"C. 1 43
0 80
PRC. 2 [f,'S
Legend to Fig.11 Cathode-sputtering coefficient for perpendicular F
incidence of commercial copper (curve 1) and chemically pure copper
(curve 2).
Legend to Fig.2s S uttering coefficient an a function of the angle of
incidence (curve 15 and the product of this coefficient with-the cosine of!
the angle of incidencenas a function of this angle.
Card

S10201611137100110101021
B104/B209
AUTHORS: Molchanov, V. A., Tellkovskiy_l_V. G., and Chicherov, V. IA.
TITLE: Anisotropy of cathode sputtering of single crystals
PERIODICAL: Doklady Akademii nauk SSSR, v. 137, no. 1, 1961, 58-59
TEXT: This article presents the results of measurements concerning the
dependence of the sputtering coefficient of the (100) face of nickel and
copper single crystals on the angle of incidence of ions. The experimental
setup has been described in an earlier paper (Ref. 3: V. A. Molchanov,
V. G. Teltkovskiy, Vestn. Moskovsk. univ., V. 1 (1956)). Sputtering
was done with singly-ionized 27-kev argon ions; curr,,nt density was
1-2 ma/CM2. The single crystals were polished and then annealed for some
time in a vacuum furnace at about 8000C. After this, they were slowly
cooled down to room temperature, and their surfaces were chemically etched.
Surface condition and orientation of the c rystals were examined by X-ray
structural analysis. The sputtering coefficients (atoms/ion) are plotted
versus the angle of incidence in Figs@ 1 and 2. Curve 1 in Fig. 2 was
taken at a Cu single crystal, curve 2 in Fig. 2 at polycrystalline copper.
Card 1/3

Anisotropy of cathode... S/020/61/137/001/010/021
B104/B209
The results of analogous measurements with a nickel single crystal are
shown in Fig. 3. The results found with these two single crystals are
very complicated. The position of the minima is the same for both
single crystals and corresponds to the angles of incidence of the ion
beam which coincide with the crystallographic axes (100), (111), and
(112~. The authors note the non-monotonic dependence of secondary-elec-
tron emission on the angle of incidence which differ8 for coper by more
than twice the amount at an angle of incidence of 36 and 48 . The
single crystals used in the experiments described here were grown at the
Institut kristallografii AN SSSR (Institute of Crystallography AS USSR)
under the supervision of V. A. Timofeyeva, who is thanked by the authort;.
Moreover, the authors thank Ye. V. Kolontsova, I. V. Telegina, and N. A.
Khatanova for having determined the orientation of the single crystals,
as well as I. I. Dushkov for assistance. There are 3 figures and
4 references: 3 Soviet-bloc and 1 non-Soviet-bloc.
ASSOCIATION: Nauchno-isaledovatellskiy institut yadernoy fiziki Moskovsko-
go gosudarstvenrogo universiteta im. M. V. Lomonosova
(Scientific Research Institute of Nuclear Physics of Moscow
Card 2/3 State University imeni M. V. Lomonosov)

Anisotropy of cathode... S/020/61/137/001/010/021
B104/B209
PRESENTED: December 171 1960, by L. A. Artsimovich. Academician
17MIUM
SUBMITTED: December 10, 1960 r
I Om
Card 3/3
25

3 24-09 /138/004/009/023
4, r).10 0 B'l 04./B203
AUTHORs Molchanov, V. A., Tellkovskiy, V. G., and Chicherov, V. M.
TITLEs Angular dictribution of oputtored particles in irradiation
of a single crystal by an Ion beam
PERIODICALs Akademiya nauk SSSR. Doklady, v. 138, no- 4, 1961,
824 - 825
TEXTa The experiments reported here were made with an experlmental
arrangement described in one of the authors! previous papers (Vestn.
Mosk. univ., no* 1t (1961)) and schematically shown in Fig. 1. The ion
beam I passes a diaphragm 2 and hits the crystal 3. As a collector
served the base of the X-ray film which was attached either to a plane
(4ft) or a curved (0) copper plateo Fig* 2 shows a photograph of the
deposits on the collector, obtained in the irradiation of the (100)
plane of a copper single crystal witb an argon beam of the energy of
27 '--ev. The four symmetric patterns correspond to the crystallographic
axes[1103, and the fifth in the center to the [1001 axis. The arrows
give the directions in which the deposits were photometrically deter-
mined. Figs. 3 and 4 show the results. The different curves correspond
Card 116

O/C28/1~138/004/009/023
Angular distributions ... B104/B203
to different Rv d (d - diameter of the ionic beam on the crystal), and
angles of incidence a of the ionic beam. As can be seen, a considerable
part of the atoms leaving the target lie within narrow cones whose axes
ooinqide with the orysta~lographic prinnipal axes of the target. The
angular half-width is 20 . The authors state that the "intensity" of
the Wehner patterns greatly depends on the angles between the crystallo-
graphic principal axes and the sectional plane of the crystal. If the
sectional plane of the crystal is none of the crystallographic principal
planes, then the more intensive patterns lie in the directions forming
smaller angles with the normal of the sectional plane. The authors
thank I. A. Shakh-Melikova for assistance in the experiments. There
are 4 figures and 9 references& 6 Soviet-bloc and 3 non-Soviet-bloo.
The 2 references to English-langua e publications read as follows& G. K.
Wehner, Phys. Rev., 102, 690 (19561; G. K. Wehner, G. S. Anderson, J. Appl.
Phys., 319 2305 (1960).
Card 2/6

2 L, 0 419
S/020/61/138/004/009/023
Angular distributions ... B104/B203
ASSOCIATIONs Nauchno-isaledovateliskiy institut yadernoy fiziki
Moskovskogo gosudarstvennogo upiversiteta im. M. V.
,Lomonosova ( Scientific Research Institute of Nuclear
Physics of Moscow State University imeni M. V. Lomonosov)
PRESENTED: March 49 1961, by L. A. Artsimovich, Academician
SUBMITTED: February 28, 1961
Card 3/6
--H
N;

42728
S/109/62/007/011/007/012
L ~ 61) D295/D308
~j f Lt -,0
AUTHORSt Gott, Yu.V. and T k i y- ~V. G
TITLE: Deceleration of light ions in thin
metal foils
PERIODICALs Radiotekhnika i elektronika, v. 7,
no. 11, 1962, 1956 - 1901
TEXTt The passage of ions with less than 20keV
energy through metal foils has been little studied. The small
ion velocity makes both Bohr's and Fermi-Teller's formulas in-
applicable. In the described experimental investigation a hydro-
gen, deuterium or helium ion beam from.a high-frequency source
with 1-5 - 15 keV energy is deviated by 900 by a sectorial mag-
netic field with double focussing and passes through 100-500 A
thick foils of Ag, Ti and Ge. The output-beam energy distribution
is measured by means of an electrostatic analyzer. The epeoific
energy losses ( -dE:/dx, where E is the ion energy and x is
the transverse coordinate of the foil obtained for several foils
Card 1/2

S/10 62/007/Oli/007/012
Deceleration of light ions ... D295YD308
of various thickness are plotted as a function of the mean beam
velocit and exhibit a linear relationship for velocities greater
than 109 cm/sec. Departures from linearity below this velocity are
interpreted as due to a reduction of the effective charge owing to
electron capture. The linearity coefficients are independent of*
the ion mass and of the properties of the atoms of the target and
are determined mainly by the inter-atomic distances of the crystal
lattice of the target. Calculations based on a simplified model
for the lose mechanism# in which the target is assimilated to a
very dense plasma, are in good agreement with experiment and suggest
that, for the velocity interval investigated, energy loss is due
mainly to collisons with free electrons. The results of similar
experiments with molecular ions ( III, and H* ) confirm this view.
These ions are dissociated at a ema distange ( 10 - 20 A ) rrom
the target input surface and the energy-lose calculations are to
be carried out for the dissociation products separately; The most
important English-language reference lot J,R~ Young, J#Appl. Phys.,
v. 27, 1956, 1. There are 6 figures and 1 table.
SUBMITTEDs March 19, 1962
Card 2/2

GOTT, YU.J.j TF.LIKOVSKIY- V.G.
Deceleration of light ions in thin metal foils. Radiotekh.
i elektron. 7 no.21:1956-1961 N 162. (MIRA 15:11)
(Metal foils)
(Ions)

4] -1
S/040/62/026/oll/005/021
B125/B102
AUTHORS: Molchanov, V. As, and Tollkovokiyt V. G.
TITLE: Angular characteristics of the destruction of metals by ion
beams
PERIODICAL: Akadomiya nauk SSSR. Izventiya. Soriya fizichookaya,
v. 26, no. 11, 1962, 1359-1365
TEXT: The Kafedra atomnoy fiziki Moskovskogo universiteta (Department
of Atomic Physics of Moscow University), which has been investigating the
angular dependence of the destruction of metals by ion beams since a
number of years, pays special attention to thp case when the ion beam
falls at very small angles upon the metal.surface. The results of these
studies are of great technical importance, ouch as in the design and'
con'struction of thermonuclear reactors. The experimental arrangement
consisted of a large mass spectrometer with a doubly focused ion beam in
a sectorial magnetic field. The angular convergence of the ion beam is
small, and the pressure of the background gas near the focus of the device
is low. Although previous investigations were carried out with great
Card 1/3

S/048/62/026/011/005/021
Angular characteristics of B125/B102
care, their results differed greatly. The influence of the roughness
(degree of destruction) of the irradiated surface may be seen from the
fact that the sputtering coeffi'cient of a single crystal is independent of
the duratiun of bombardment and of the degree of surface contamination.
The sputtering coefficients of "Bmoothn and "destroyed" polycryetalline
surfaces differ considerably; for example, in the case of commercial
copper they differ by 25%. At present, it is not yet possible to infer
the mechanism of destruction from experimental results. The sputtering
coefficient increases in inverse proportion to the cosine of the angle a
at which the ions strike the target. Deviations from this cosine law,
occurring at large angles of incidence, are neither due to the reduced
transfer of ion energy to the target nor to the effect of the microrelief
of the specimen. The sputtering coefficient is a non-monotonic function
of a, but drops sharply when the direction of the ion beam approaches the
crystallographic axes of the target. For this reason, grains with
properly directed major axes are not destroyed on the sputtered surface.
The density of the deposition on a spherical collector with its center
in the middle of the irradiated specimen is proportional to the angular
distribution of the sputtered particles. In the neighborhood of the
Card 2/3

S/04 62/026/011/005/021
Angular characteristics of ... B125%102
t I
1110" axis, the density of the deposited particles shows a Gaussian
r 0
distribution with a half-width of 20. The radiative mechanism proposed
for the destruction of metals is almost indubitably correct. The
problem under consideration was suggested by L.-A. Artsimovich.
Card 3/3

21 74
S/05 62/032/005/022/022
B104YB102
;L(~00
AUTHORS: blolchanov, V. A., Tellkovskiy, V. G., and Shakh-Melikov*a,i.k.
TITLE: Effect of the target temperature on the angular distribution
of sputtered particles on irradiation of a single crystal by
an ion beam
PERIODICAL: Zhurnal tekhnicheskoy fiziki, v. 1.2, no. 5, 1962, 647-648
TEXT: The effect of radiation damage of a single-crystal lattice on the
angular di8tribution of particles emitted from the crystal on irradiation
with ions-is explained. It is assumed that when lattice imperfections are
present the spot of an X-ray diffraction pattern contracts on increasing
the target temperature. The deposits of the sputtered substance are
photometered. The width of the spots alters very little for target
temperatures between 1,50 and 7000K. A flat minimum of the spot widths lies
approxim.ately in the middle of the temperature range, i.e., at- - 1-50+700 o..
2 2 2
For ion current densities of 1 ma/cM and radiation doses of 2-3ma-hr/CM
there is no marked brof dening of the angular distribution due to radiation
Card 1/2

S/05 62/032/005/02~/022
Effec-,' of the target temperature... B104YB102
damage of the lattice if the temperature in not too low. There io 1 figure..",r
SUBMITTED: July 3, 1961

3/057/62/032/008/014/015
B104/BI02
AUTHORSs Yendzheyets, G., Molchanov, V. A., TelIkovskiy, V. G., and
-Paruk, M. A.
TITLEs Angular distribution of evaporated particles in the irradia-
tion of single crystals with an ion beam
PERIODICALs Zhurnal tekhnicheakoy fiziki, v. 3i, no. 8, 1962, 1032 - 1035
TEXTs The angular distribution of the particles produced when the (100)
faces of copper and nickel single crystals were irradiated with argon and
neon ions was measure4, The diameter of the single crystal surface
irradiated was smaller than 8 mm, the distance between target and collector
95 ram- The target temperature was lower than 1000C, the angle of
incidence of the ions 20OW:'. After irradiation five Wehner spots became
visible on the oollectori four at the corners corresponding to the
(110) axis, and one in the center which corresponded to the (100 axio.
The density of the spots was determined photometrically. (Fig. 1~. The
angular distribution of particles and that of the sputtering coefficient
do not depend on.mass and energy of the ions, There are 3 figures.
Card 1/2

5/057/62/032/000/014/015
Angular distribution of..; BIOVD102
ASSOCIATIONs MG~
SUBMITTEDs Ootober 24, 1961
Fig. 1
4v 40 0
Card 2/2

GOTT, Yu,V.; TELIKUVSKIY, V.G.
Determining the lifetime of a high-qtemprature plaama on the basis of
the duration of neutron emission. Zhur. ekop. i teor. fiz. 43 no-3s
831-834 162. (MIRA 15:10)
(Plasma (Ionized gases)) (Neutrons)

h2 103
S1020162114-1100210091021
B184/B102
AUTHOAS: Balarin, M., Molchanov, V. A., Tellkovskiy, V.
TITLE: Anisotropy of the cathode sputtering coefficient and the
focused collisions in monocryetals.
PERIODICAL: Akademiya nauk SSSR. *Doklady, v. 147, no. 2, 1962,- 331-333
TEXT: The angular dependence and the anisotropy of the sputtering
coefficient was investigated under the same experimental.~conditions as
used by V. A. Molchanov and V. G. Tellkovskiy (DANO 136, 801, 1961) by
rotating zinc monocrystals about their