SCIENTIFIC ABSTRACT ABROSIMOV, V.V. - ABRUKINA, R. Y.

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• Collection: Scientific Abstracts
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• Document Creation Date: November 2, 2016
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• Sequence Number: 6
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

Nuclear Energy and tho Navy (Goat.) SOV/6261
5. k,__R_j-ojoy Ziginoor Commander (Navy). Primary
Penetrating
Radiation 58
,ndr2vL Engineer Lieutenant Colonel, and Q,_NqAtay,
6. A, A
Majo:7 Engineer. The "Foot Wave" and Its Damaging Eff
.,,act 66
7. 1. Frolov. Ionizing Contamination 70
8. P
a4)Captain (Navy), and 0
L-Jaier Bhginoer
cot Protecting a Ship AAga st Nuclear Weapons T8
9. G. FIigirenl1co, Captain (Navy), Professor, Doctor of
Engineer-
ing. rroteorxng~a Ship Against E:xplosions 86
10. P. Abolishin Captain (Navy). Means of Protection
Against ,
Nue:1ear weapons in Foreign Navies .93
11. P, 1[hq,%hlny, Engineer Captain (Navy), Candidate of
Tech-
nimil Sciences. Nuclear Protection of Light-Class Ships 100
Card
- r1

KOLESANOVp P.F.; KOJIAREVA, A.S.; Prinimali uchastip,:
ABROSIMOV, V.V., inzh.;
GAIRINp E.G., inzh,; SUYETINA, G.F., laborantjf~ ~GV,
B.I.p
lalwant; PANOV, O.V., laborant,
Pelletizing Ufaley deposit nickel ores with subsequent
roasting. [Sbor. true.) Nauch.-issl..Lnst.met.
no.4:54-6,1
161.. (MIRA 15:11)
(Ufaley Range-Nickel ores)
(ore dressing)

SHCHMMOV,, V.A.; kIMIMOVI_Yf~.V.; STULIPIN,, Ye.A.;
GOROKHOV, I.S.
Mechanism 6f slag formation during the melting period
in high
capacity open-hearth furna-cese Izvev7soucheMave;
chern*mets
5 no.11:48-56 162. (MIRA 15:12)
1. Hoskovskiy institut stali i splavov,
(Open-hearth process) (slag)

ABROSKIN, G.I., inzh.; KUDASHO~, A.V., inzh.;
POTAFENIKO, B.T., inzli.
Construction of the Golovnoy hydroelectric
development on -the
Vakhsh River. Gidr. stroi. 32 no.8:7-10 Ag 162. (MIRA
15:9)
(Golovnaya Hydroelectric Power Station)

/ 4 1-" ;-. V . fl . I-
, 2~ 11 1 . I II I
ABAOVP N.A. (Hoskva)
;'
Curriculum of elementary mathematics in podagcgical
institutes.
Mt. v shkole no,Z-.17-20 Mr-Ap 158. (MIRA 11:2)
(Mathematics-Study and teaching)

ABROYAN, I.A.
4
Emission from an oxide cathode bombarded bv positive
ions. F12.
tver.tela 1 no.12:1854-1856 D '59. (MIRA 13:5)
1. PolitekhnichesHy in-stitut im. M.I.Kalinina,
Leningrad.
(Cathodes)

.Z1 ~- a2O 14
A)THOR:
TITLE:
2 9 7 55'
S/19li/61/000/006/030/077
D201/D302
,%broyan, I.A.
The effect of ion bombardment on emission of an
oxide coated cathode
PERIODICAL: Referativnyy z1hurnal. Avtamatika i
radioQ1ektro-ilika,
no. 6. 1961, 2, abstract 6 G16 (Nauchno teldin. in-
form. byul. Leningr. politelvdin. iTi-t, 1960, no. 3,
33-45)
TEXT: The effect of positive 1-iydrc(-,cii and potassium
ions on the
emission of oxide coated cathodes was studied. The invgr, t
igati oils
were carried out at the rcsidual gas pressures < 1.10- min
lig.,
a device consisting of an ion source 600 maun. analyzer aild
a
measuring section. Hydrogen was let in through a palladiiiin
capil-
lary. The energy of hydrogen io-as was 10 - 70 keV,
Potassium ions
were obtained by calcination of a mixture of potassium
carbonate
with aluminum and silicon o.-ddes. An intensitvc surface
ioniza-
Card 1/2

2)7515
S/191V61/000/006/030/077
The effect of ion bombardment... D201/D302
tion of potassium thus occurred due to chemical reaction at
temp-
eratures 900 - 10000C. The energy of potassium ions in the
ex-peri-
ment was I - 10 keV. The ion current falling on the oxi.(Ic
coated
cathode was 10-8 - 10-7 amp. The aiming, of the ion boxi at
the
oxide coated cathode caused an increase in the clectron
current
from th,! cathode in all cases. Every bombarding ion releases
2FOOO - 5,000 additional electrons. The ratic of the
variation of
the cathode emission current to the ion current causingr this
varia-
tion depends on the emitter temperature, the cuergy of
bomoarclin,T
ions, the intensity of the beni-ii and also on the
miaguiti-i(Ic of elec-
tric field at the cathode surface. 7 rcfcrenccs. Abstracter's
note: Complete translation-7
Card 2/2

ABROYAN, I.A.; MOVNIN, S.M.
Emission of an oxide cathode bombarded by charged
particles. Fiz.
.L
L,vr. tela 3 no.2:567-574 F 161~ (MIRA 14:6)
1. Leningradskiy politekhnicheskiy institut im. M. 1.
Kalinina,
Leningrad.
(Secondary electron emission)

3 / 20 e'~Kd
AUTHOV
" 9
11"~Oj //3F, 11q3) S/1 6-1 ~601'_)003/002/037/050
B1 02/B2011
Ab~yanj
TITLE: Electron emission from germanium induced by cesium- ,
potassiurry
lit'Aium-, and hydrogen ions
PERIODICAL: Fizika tverdogo tela, v. 3, no.. 2.. 1961, 588-594
TEXT: The ion-induced electron emission from dielectrics and
semiconductors
has heretofore not been systematically studied; on the other
hand, this
study is necessary in order to get an insight into the
mechanism and under-
lying rules. Studies in this respect were ti.,erefore conducted
on r.-type
germanium single crystals (resistivity 37 ohla-cm), and results
are described
Jn the present paper. The disk-shaped Ge crystals (6-7 mm in
diameter) were
ground, etched with CP-4 (9R-4), and washed in distilled waters
Subse-
ontly, they ivere introduced (M) into the oxperimental setup
(Fig, 1)~ The
apparatus had a residual gas pressure of not over 5''0-8 mm
119; ovacuation
took place with a mercury diffusion pump, The positive ions
were emitted
from the hot source (0) which was coated with a paste made of
Al 203 + Sio2
Card 1 /~

20139
S/18 61/003/002/037/050
Electron emission from B102YB201,
I
alkali carbonate. The ion beam was focused by a s,,stem of
Ni electrodes
(41 9-42) , monitored, and caused to hit the target (M)
w1nich was arrangee in
the center of two collector semispheres (50 ,nm in diameter)
The target
temperature ranged between 700 and 8000C during the (static)
measurements,
and the primary ion beam had an ampera(~e of 5,10-6 a The
e'lectron-emission
coefficient y was measured as a function of the ion energy;
the results tire
illustrated by Fig. 2. y grows linearly with E for Cs, K,
and Li; the in-
clination of the y straight lines is the same as in the
bombardment of
metals; for all alkali ions there is a threshold energy
(1000 ev for Cs,
about 500 ev for K and Li), above which the kine t4C
ejecting of ions be-
comes considerable. Mass-spectroscopic studies showed that
the ion beams
used were by 98~o ions of the same type, The curve obtained
for IU -, ions
(at 5000C target temperature) shows that field-induced
electron er':ission
from germanium takes place with `;ydrogen bcmbardment, ),
shows no dependence
on the target temperature (in the range investit;ated). but
),(E) exhibits a
shift to the left, if the tarE~et is exposed to heat
treatment Drior to the
bombardment. The maximum energy of secondary, elec:r=s Js
al--ut 20 ev, and
the volt-ampere characteristics reveal that sa-uration is
noi-~;omyletely
Card 2/y

;~U-'-35;
S/181/61/0.03/002/037/050
Electron emission from ... B102/B201
ato,m to txcite an electron to an enczG~r sufficient to permit
its eaca,pe
into the vacuum, n is the number of collisions per ,iniL
length, and a is a
pro,,porticnalit~ factor takine the primary electron
distribution into accouqt
G. G. illina, G. 1,,r. Batanov, and A. G. Llorozov are thanked
for their
cooperation. There are 3 fiCures, I table, anc~ 1'r
references: 10 Soviet-
bloc and 3 non-Soviet-bloc.
ASSOCIATION: Politekhnicheskiy institut im. "I. I. Kalinina G.
Leningrad
(Pol,ytechric institute imeni T. Kalinin, Lonincrand)
SUB:-,,1ITTED: Jcne 24, 1960
Card

20135
C/131,20
~'PW3 1
S/'181/61/'003/002/033/0'zO
B102/B201
AUTHORS: Abroyan, I. A. and :,11ovnin, S.
TITLE: Emission of an oxide cathode bombard:!d by charged
particles
PERIODICAL: Fizika tverdogo tela, v. 3, no. 2, 1961, 567-574
TEXT: Abroyan has shown in two previous papers that a beam
of potassium
or hydrogen ions incident upon the surface of an emitting
oxide cathode
gives rise to an increase of the anode current, with A = 6
Ia/I 1
attaining up to 5000 electrons per ion ( 61 a, change of
electron current
of the cathode, I,, intensity of ion current at the
cathode). Further
studies have been made of the effect of different positive
ions upon the
thermionic emission and the mechanisms of the change of the
thermionic
cathode current. The measurements were made on an apparatus
described
earlier at 1-2.10-7 mm Hg. The primary pulse currents had a
duration of
10-200 psec and a frequency of 2-2000 cps. The primary and
the secondary
pulse currents were recorded by a linear amplifier with
resistors
Card 1

S/181/61/003/002/033/050
Emission of an oxide cathode ... B102/B201
ensuring the conservation of the pulse shape. The pulse
heights were
measured with an C~4-1 (SI-1) or 25-W(25-I) synchroscope, Oxide
cathodes with coatings of (Ba,Sr)O and (Ba,SroCa)O were
utilized, and
the effects of ion bombardment were found to be "'airly equal
for both
types. The typical dependence of L\ on the energy of
bombarding ions
is repreqented in Pig. 1 for 6.5 v at the hot cathode, and an
anode
current of 1.2 ma; (for eieotrons (I), hydrogen j,ons (2),
helium ions
(3), and argon ions W, as well as. in the case of U. ath ~ 5.5
v and
Ia= 1.4 ma, potassium ions (5)), Experiments with K; were,
however,
conducted with another cathode, so that the results are not
comparable.
The monotonic decrease of L~ kfrom 2.5 to 10) observed in
electron
bombardments of the cathode fits ob!;ervations made by
Pomerantz.
L\ as a function of the plate voltage Ua first exhibits an
exponential
rise -ap to about 60 v, and, with a further increase of Ua the
rise is
slow and practically linear (on a bc-mtardment by 2.rj-kev
potassium ions,
voltage of filament battery U 5.25 v), I (U ) exhibits a
similar
Wh a a)
Card 2/45-

20135
S/184 '61'003100210331050
Emission of an oxide cathode B102~0011
course, a property which is conserved also on a bombardment
with electrons
or other ions. a as a function of the voltage of filament
battery goes
through a maximum at U I =, 6 v, has a very low value at 4
and 8 v, and
cath
at 9 v, Z3 ~~-O. The electron current additionally emitted
by the cathode
rises and drope with time after an exponential law (1-e-
t/v , e- t/rI
respectively). Por hydrogen and helium ions, Z c- 20 psec,
for argon and
potassium ions, -10 liseoo The results show that the change
of the
emission of an oxide cathode bombarded with positive ions
cannot be
explained by the slowing down of ions, The safest
assumption seems to
be that so-called "displacement defects" are formed in the
surface layer
of the oxide coating, i.e., defects caused by a
displacement of ions
from their positions of equilibrium in internodal
positions~ This
assumption is above all supported by theoretical
considerations. The
following formulas are obtained for the penetration depth 6
of ions of
the energy E and the atomic number z 1:
Card 3 /5

20135)
S/181/61/003/002/033/050
Emission of an oxide cathode ... B102/B201
A t A
A > A o.6 2 1 2 j.i"E cm
1 2 1z2 Al - d
0.7 z2/3 z213') 1/2 A2 E
A 1< A 2; -772) z z A + A cm;
70--S~) V - 1 2 1 2
A 1is the mass of the bombarding ion, A2 the mass of' atarget
atom of the
, 3
atomic number z 2j d the density of matter in jig/cm,t.P, the
scattering
angle of the ion in the laboratcry system, ~ ~ T-nT:t,', ~E2
, the mean
logarithmic decrement. At E kev, 1500 A was obtained for 1-,1+
2t
750 A for He+, and 50 A for Ar+ and K4, The mechanism of the
increase of thermionic emission of the oxide cathode
bombarded with fast
ions is governed by the following rules; 1) increase of ts
with E,
2) independence of 2~ of the intensity of the ion beam, 3)
the inertial
change of the thermlionic current (the primary square pulses
of
Card 4/~-

20135
S/181/61/bO3/002/033/050
Emission of an oxide cathode B102/B201
-7
1-10 3.10 a gave ri-~e to secondary pulse j1ags with rising
and
dropping times of 15-30 psec), 4) the similarity of !~s and
I as
a
functions of the electrode potential difference, 5) the
existence of a
peak of the Z~(T) curve, and,6) the ratio of the !~a values
for different
ions (L rises with the atomic number of the bombarding ions)-
Professor D1. A. Yeremeyev is thanked for having supervised
the 1%ork, and
G. G. Il!ina for her measurements. Kozlyakovskaya is
mentioned. There
are 5 figures, 1 table, and 6 references: 4 Soviet-bloc and
2 non-Soviet-
bloc.
ASSOCIATION: Leningradskiy politekhnicheskiy institut im. M.
I. Kalinina
Leningrad (Leningrad Polytechnic Institute imeni 114. 1.
Kalinin, Leningrad)
SUBINUTTED: June 15, 1960
Card 5/5

AUTHORs Abroyan, I. A.
S/181/62/004/010/011/063
BiOB/BI04
TITLEt Conductivity induced in germanium by bombardment with
potassium ions
PERIODICALt Fizika tyerdogo tela.t v. 4# no. lot 1962, 2719 -
2726
TEXTs The additional conductivity of n-type Ge i6duced by
bombardment
with a pulsed beam of potassium ions (100 - 10,000 ev) was
studied with
an arrangement similar to the usual.secondary-emission
apparatus (FTTI 31
2, 588, 1961), comprising a spherical collector, an
antidynatron grid, and
the Ge target. The samples had previously been heated to about
8000C in
vacuo. Bombarding the Ge targets gave rize to an ad,'..'tional
conductivity
pulse during each pulse of incident ions. The rise ind fall of
these con-
ductivity pulses (due to excitation of electron-holc pairs,
defects) is
exponential. The additional conductivity increases with
increasing energy
of the incident ions. However, there in a threshold energy of
300 - 400 ev
below which no additional conductivity is excited. The number
of electron-
hole pairs excited by one incident ion is a monotonic function
of the ion
energy E, amounting to about 900 - 1000 pairs at E - 10 kev.
The fraction
Card 1/2
M

Conductivity induced in... S/1'8 YB 62/004/010/011/063
B108 104
3
of excited electrons going into the vacuum is 2 - 2-5-10
throughout the
energy range of 1 - 10 kev. The mean energy consumed in the
excitation
of one pair is shown in Fig- 5 as a function of E; (kev).
There are 5 fig-
ures*
ASSOCIATIONs Politekhnicheskiy institut im. M. I.'
Kalinina, Leni,l;;rad
(Polytechnic Institute imeni M. 1. Kalinin, Leningill)
SUBMITTEDj May 7# 1962
E
Figo 5 40-
20-

h3127
S/181/62/004/011/028/049
B125/B186
AUTHORS: Abroyan, I. A., and Lavrov, V. P.
------------------
TITLE: Secondary emission of dielectrics and semiconductors
resulting '11rom potassium ion bombardment
PERIODICAL: Fizika tverdogo tela, v. 4, no. 11, 1962,
3254-3259
TEXT: Ion induced electron and ion emission from LiF, NaF,
NaCl, KBr, C8C1
and silicon monocrystals was investigated. The crystals were
bombarded with
potassium ions of 40-7000 ev using the pulse method of G. M.
Batanov (FrT,
z
J, 2, 558, 1961; 3, 2, 642, 1961).A triple-electrode system
was used com-
prisir.E- a spherical Crid, an antidynatron I-rid and the
target to be
investiLated. The. pressure of the residual. gas* was 3-10-7
mm Hg. The K ion
beam was square-pulse modulated with repetition frequencies
of 0.5-50 cps,
amplitudes of 0.2-0.8 i,a and a duration of 8 to 16 jLsec.
Electron emission
was obs.-rved only at energies of the K ions between 100 and
300 ev. The
.coefficient w of the ion-induced electron emission was
found to increase
with growing ion energies, up to -12 kev sharply, and then
slow.y. KBr
crystals had the highest and LiF crystals had the lowest
values z,!' f. The
Card 1/3

3/181/162/004/011/028/049
Secondary emission of dielect,rics... B120186
coefficients K of ion-induc6d ion emission of all
alkali-halides were
similar and similar,y dependent on the energy of primary
ions. The
coefficients K became largerwith increasing energies
(starting with
threshold energies of AOD-500 ev) of the primary ions and
reached saturation
values of 15~~ at E-1.5 kev at'most. The positive secondary
particles
consisted of knocked-out particles of the bombarded crystal
and reflected
ions of the primary beam. On increasinE the temperature from
room tempera-
ture to ANO-4000C, K+ and-K- remain practically unchanged.
The decrease of
j is attributed to the scattering of excited electrons from
phonons. The
temperature dependence of ? and the shifts in the spectra of
the secondary
electrons may be qualitatively explained by the enerC~r
looses of the
excited electrons. The coefficient i of silicon
monocr7;stals showed almost
a linear increase with Erowing energies of the bombarding
ions. This
increase was less at elevated temperatures, i.e. when the
specimens were
heated from EVOO-13000C. The coefficients K+ o*f etched
silicon monocrystal
samples and of trose heated to 13000C showed a sharp
increr.~n with growing
energies of the primary particles up to - 1.7 kev followe(l
-er and
Card 2/3

.,. 112(.-
S/02 62/144/003/011/030
B178YB104
AIJT'MS: Abroyan, I. A., and Zborovskiy, V. A.
T ~-~'xcitation of electrons in germanium by potassium ions
-HOD-CA"; Akademiya nauk SSSR. Doklady, v. 144, no. 3, 1962,
531-534
TIXT: A study was made of the chan-a in conductivity of n-type
Germanium
U
s~n-le crystais bombarded with potassium ions of 400-10,000 ev
energy,
0
which is due to the excitation of valence electrons. The slowin&
down of
these particles at a velocity v< v 0 (VO - 2.2-10 6 cm/sec) cai,
-..- determined
from an investiEation of the lonLgitudinal conductivity. A.1
-~Iectric field
was created on the germanium plate onto which a potassium i--~
beam of
0-1-50 t,-- stren[;th, modulated by square pulses of 10-50,itE!;-,
duration, was
ocused. "Non-equi"'ibrium, carriers produced by 'he potassirm ions
induce
an additional measurable current. it is possible to record the
variation
of 16'-e conduction current. The time constant -5 of the pulses is
3-5-~-kSec
if the specimen is not heated, and 10-20 ,,see if the target is
vacuum-Ineated
to SOJOC. The lower the rate of cooling, I the greater the mean
lifetime, z ,
Card 1/3

S/020/62//144/0071/01 1/0.310
Excitation of electrons in germanium ... B178/B!04
of non-equilibrium carriers. The lower values of /I' area
attributed
0 1
to the increase in concentration of thermal acceptors by rapid
cooling
w um carriers.
..hich reduces the lifetime and mobility of non-equilibri
The current of the induced conductivity is a linear function of
the field
strength a. It is found that (_,ai /I+e)Kt where
0 1
1, and 0-5 kev,
f(E). equals 0.135' 0.114, 0.071, and 0.032 for 6, 3,
respectively. The relationship between the ionization cross
section and
elastic collisions with lattice atoms at v< v. can probably be
obtained
from a study of the conductivity of semiconductors ~nd
dielectrics. A
comparison between the coefficient of ion-electron emission and
the number
of excited electrons makes it possible to predict the
production probability
of secondary particles in vacuo. "here are 4 figuros.
ASSOCIATION: Leningradskiy politekhnicheskiy institut, im. I.
1(alinina
(Leningrad Polytechnic Institute imeni M,. I. Kalinin)
Card 2/3

AMOYAN. I.A.
------ ----
Induced conductivity in germanium under bombaOrdment
with
potassium ions. Fiz.tver.tela 4 n3.1022719,-2726 0
162.
(MA 151l2)
1. Politekhnicheakiy institut Imeni M.I.Kalinina,
Leningrad.
(Semiconductors--Effect of radiation on ion beams)
(Potassium)

ABROYAN, I.A.; LAVRGVI V.P.
Secondary emission from dielectrics and semiconductors
under
bombardment with potassium ions. Fize tver, tela 4
no,11:3234-3259
'N 162. (MIRA 15:12)
1. Politekhnicheskiy institut imeni M.I. Kalinina,,
Leningrad.
(Secondary electron emission)
(Alkali metal halide crystals)

~V~~o r 0 LAot

SAMOLYTEt M.; DUBICKASp V., spets.red.; ABROMAITIENE,
H._,_ red.;
KINDIAKOVAt 0., red.; PILKAUSKAS, K., tekhn. red.
(Use of synthetic materli%l-& in tthe light industry;
bibliogmphy3
Sintetiniu medziagu panaudojimas lengvojeje
pramoneje; biblio-
grafine rodykle. Primenanie sintetichaskikh
matorialov v legkoi
promyshlennosti; bibliograficheskii ukazatell.
Vilnius,, 1962.
69 P. (MIRA 16:2)
1. Lithuanian 5,3.RLlaudies ukio taryba. Centrine
moksline-
technine biblio*;eka, Vilna,
(Bibliograpby-Synthetic products)

SIMONAVICHENE, K.(Simonavicienep K.1; FMTSLrWS,
A.[Kancleris, A.],
otv. za vypusk; ERIS, A., inzh., opets. red..;
ABROMATIYT1?E,Kh,
[Abromaitiene, H.), red.; YEFII,,CVA, F., red.;
PILKAUSUS,-
tekhn. red.
(Heohmisation and ai.tomation of production processes in
the wood-
working industries; Libliographical index] Medzio
apdirbimo pramones
gamybos procesu mechan-I.Pavimas ir automatizavinas;
bibliografine
rodykle. Vilnius, 1961. 1.17 p. (MIRA 15%4)
1, Lithuanian S.S.R. Liaudies
technine biblioteka, Vilna,
(Bibliograpby-Woodworking
(Bibliograpby-Automatic
ukio taryba. Centrine mok:31ine-
industries)
control)

ZHILEVICH I.I.j red.; KMOVICH, N., red.;
A~~9MAYTENE, G.
[Abromaitiene, G.1, red.; LABKAUSKAS, S. red.;
URBONAS, A., tekhn. red.
[Electrophotography and magnetography;
transactions of the
Scientific wid Technical Conference on Problems of
Electro-
graphy held in Vilnius on December 16-19, 19581
Elektrofo-
tografiia i magnitografiia; trudy. Pod red.
I.I.Zhilevicha.
Villnius, Respublikanskii in-t nauchno-tekhn.
informatsii i
propagandy, 1959. 390 P. (MIRA 17:3)
1. Nauchno-tekhnicheskaya konferentsiya po
voprosam elektro-
grafii, Villna, 1958. 2. Nauchno-issledovatellskiy
instAut
elektrografii, Villnius (for Zhilevich).

O"ogitnic sub;dgmtts. 9. AbIposovki wrl llwknvia Cumi.
c0aw in ll:sol, ntltj nvtral dpv!i of 1110t, ppt. Fie with
NJ 1,011, filtm %vath: (14imlyeppf In IvIiel,wil, reduce
i$ C,, A.
,Lfb S!iCl,, nnd tltj-ufe ul!b tit

Ft VK I V. _V
AUTHORS Lbrosenkova,V.F.tLogginoy,G.I.t~"Ilidw~k ,P.A.,?,
-k-ember of the Academy
TITLE Binding of Lime Into Calcium Hydrosilicate Under Normal
Condit,-,.aa.
(Syyazyyaniye iZTesti v gidrosilika'u, kalltsiya pri normallnykh
usloviyakh - Russian)
PERIODICAL Doklady Akademii Nauk SSSR,1957,Vol 115,Nr 3,PP
509-5110.3.5.*.~.,
ABSTRACT It is usually said that the formatiou of calcium
hydrosilicate
on the occasion of the interaction between limestone with ailica
in the water medium by hardening of the binding oaloareous-sili-
cious building materials can only take place by hydrothermal
treatment in autoclayes at temperatures of an or.der of magnitude
of 1700.At normal temperatures this process is assumed not to ta-
ke place i.e.it is not expressod in a noticeable increase of
strength of the formedprpduotion. Some building productions,as
e.g. wall blocks,whioh are used more and more in low buildings,
do not need the strength obtainable in autoclayes. On the other
hand,the papers of the authors confirm the assumption that,be-
sides a hydration hardening of the caloareous-arenaoeous
bindin;,-
substanoe,the binding of the calcium hydroxide gradually devclopa
in the surface strata of the sand grains.The better this surface
Was developed and the more it was activated in the common break-
ing process,the greater is the quantity of limestone bound into
calcium hydrosilicate.By means of the radioactive isotope Ca45
Card 1/2 (as Ca45(OH)2) it was determined that the bound
quantity of cal-

Binding of Lime Into Calcium Hydrosilicate Under 20-3-2.4/59
Normal Conditions.
cium is proportional on ooarse-dispersed sands of the specific
surface of the sand.In the first stage the chalk binding has a
charao;er of the irreversible adsorption nhanging into a chemical
surfafe reaotion.In the present paper the kinetics of the
constant
oaloivn binding by the sand with better daveloped surfaces (up
to 2,9 m2/g) from a saturated solution was studied by the same
method.In the case of the introduction of fine-pulverized sand
which.was activated by simultaneous grinding with limestone the
strength of the productions(with a reground sand filler)was
increa-
ead -nre and more in the course of time.The strengthening isjun-
der i.,%tural oonditions,cau8ed by two simultaneoua
prooesseetchalk
bindingtl)into calcium hydrosilicate by silica and 2)by C02 into
calcium oarbonate.Both processes take place very slOwly and are
ba-
Bed upon a diffusion process.There are enough reasons for the as-
sumption that the chalk carbonization takes place much more
slowly
than its silicatization.Thi8 is especially confirmed by the
radio-
structural analysis.The line of the calcium monohydrosilicate ap-
pears after two years whereas the lines of the calcium carbonate
are still lack,There are 2 figures,2 tables,5 Slavic references.
ASSOCIATION Institute for Fhysioal Chemistry of the Academy of
Sciencesof the
(Institut fizicheakoy khimii Akademii nauk SSSE) V331
AVAILABLE Library of Congress.
Card 2/2

55(4)
SOV169-21-4-12122
AUTHCRt Lo,,.,Ginov, G.I.# Rebinder.P.A. and Abrosenhova,
V.P.
TITLEi The Interaction at Ordinary Temperatures of Calcium
liydroxide
,"ith Sand of Various Degroes of Disperoity
PERIODICAL: Kolloidnyy zhurnalt 1959, Vol XXIr 1Tr 4, pp
442-448 (USSR)
0:1MACT: This is a study of the interaction of calcium
hydroxide with
sand in aqueous solution. The experiments i%rere carried out
with the aid of isotope Ca45, used in the form of Ce (011)2'
The binding kinetics of the lime were studied with the chemi-
',
C
al methoL; employed for the determination of free CaO. Object
of the investigation was sand (quartz sand) of the Vol'sk de-
posit of different disper s'ty2 (specific surface 3 ). The
dis-
persity varied from S 0.11 m Ig (natural state) 10 S values
2/g(finely ground). 1
equal to 0.621 0-95; .06 and 15.4 m The
eyperiments, which continued for 6 months, were carried out
at
a temperature of 17 0 + 10 C. Figure I (jraph) illustrates
the
bindin,~ kinetics of calcium ions from a saturated Ca (0H)2
Card 114 solution with sand of the above-mentioned Sl
values. The

JO-."/!~19-2' 4-1
The interaction at Ordinary Temperatures of Calcium Aydroxide
'~1th Sand
of Various Degrees of Disperoity
curves show that independently of the disperAty of the sand,
the binding process always consists of two stages: 1)
chemisor-
ptiong .-,,hich ends i,,,ithin one hour after the start of
the inter-
action, and 2) a very long period of chemical binding of CaO
at constant rates. The second processp evidently, is connected
with the formation of calcium hydrosilicate, the lattcr being
a new pliase crystallized from the 6rradually formed
supersatu-
rated solution. According to 11"rasill,nikov, this process
will finally result in the full binding of OaC in the hydro-
silicate, ivhf.ch correoponds to a final concentration
ofe-,10.006
U/1, i.e. to a hydrolytic eqDilibrium of the calcium Iilicate
in the oolut--;on. In the case of concentra'ed suspensions,
this
process results in the development of a solid crystalline
hydro-
silicate structure fil eference 11 -71 as is shown by tile
aut!~,orsl
e-'Periment-~ vith small solid blocks of lime-simd binder. The
Card 2/4 specific surface of finely ground sand ivas
determined on the
basis of adsorption at low temperature. The medium values for

SOV/69-21-4-12/22
The ~n 1' oraction at Ordinary Temperatures of Calcium
Hydroxide "lith Sand
of Variouz Degrees of D,spersity.
each diopersity served for the calculation of the space occu-
piod by a CaO moleculo (table, 1) The modium value (So) of
this space was found tb bo 10.2 On the basis of the medium
value S , and the value of CaO sorption, the authors also
calculayed the values S 1 of coarsely-dispersed sanI, which
cannot be detcriained on the basis of nitro6en adsorption. Both
methodsli.e. the method of investigating the CaO binding
proceso-
with the aid of isotope Ca4 and the method of determining the
active specific surface of sand through chemisorption of the
zame isotope, permit determination of the surface of sands of
any dispc.ooity. Low- tempo rat uro idoorption of nitrocon
only for the deteriniination of the surface of highly-dispersed
sands (.). 1 M2/6). The remaining part of the study can be
summar-
ized as follows. The dopcndonce of the rate of CaO bindint; on
tI,
dispersity of sand i.,; oubject to the equation of the
s~micubi_
Card 3/4 cal parabola (fit-,ire 2). The I,ardening of
lime-silica binders

;-"OV/69-21-4-12/22
The Interaction at Ordinary Temperatures of Calcium
Hydroxide *'~'Iith Sand
of Various Degrees of Dispersity.
can be intensified (by 505,) ly activation processes, i.e.
by passing the limesilica binder through a vibromill. The
discovery of tne mcchanism of CaO binding opens new techno-
logical possibilities to increase the strength of lime-
silica products by adding substances, which increase the rate
of dissolving of silica in water. In addition to the above-
mentioned scientist, the authors mention D.S.Sominskiy and
G.S. Khodakov. There are 4 tables, 3 graphs Lind 16
referenceso
14 of which are Soviet and 2 English.
ASSOCIATION: Institut fizicheskoy khimii Ali SSSR9 1,1oskva
(Institute of Physical Chemistry of the AS jSSR, Moscow)
~AJBMJTTEDi 15 November, 195B
Card 4/4

LOGGINOV, G.I.; REBINDER, P.A.;A4ROSENKOVA
I _Y.F. - . - -- .
Interaction botwaea calcium hydroxide and eand of
various degrees
of dispersity at ordinary temperatures. Koll.zhur. 21
ao.4:
442-448 Jl-Ag '59. (MIRA 11:8)
1. Inatitut fizicheskoy khimii AN Sba, Moskva.
(Calcium hydroxide) kSilica)

ABROSIMOVp A.
Standardization in the motorcycle Industry. Za
rul. 21 no.2:
3-4 F 163. (MIRA 16W
1. Rkspert Gosudarstvennogo komiteta Sovets,
Ministrov SSSR
po avtomatizatsii I mashinostroy-eniyu.
(Motorcycle industry-Standards)

ABROSIMOV, I.I., red.; KHAVIN, T.N., red.izd-va;
WDVEDEV, L.Ys.,
KORNBMAP V.I., tekhn.red.
(Production standards on planning and surveying
operations
paid for by the piece rate system; automobile roads
and city
transport] Normy vyrabotki na proaktnys i
izyskatellskie
raboty, oplachivaemye sdellno. Woskva, Gos.izd-vo
lit-ry po
stroit., aelchit. i stroit.materialam. Pt-23-
[Automobile
roads, city transportation] Avtomobiltnye dorogi,
gorodskoi.
transport. 1958. 29 p. (MIRA 12:9)
1. Russia (1923- U.S.S.R.) Glavnoye upravleniye po
stroitell-
stvu avtomobilinykh dorog.
(Highway engineering)

.g~pSKV, n!# _Ajq~j~ey _TARBOV, Aleksandr
Alekseyevich;
__L _qy _qy~q~j
PETROVSKAYA, Ye.K., red.; MANINA, M.P., tekhn.
red.
[K-750, M-62 motorcycles] Mototsikly K-750,
m-61, M-62.
Moskva, Izd-vo "Fizkulltura i sport," 1962. 204
p.
(MIRA 16:7)
(Motorcycles)

GINTSBURGY M.G.; ABROSIMOV, A.A., Inzh., red.;
VASIT
red.izd-va; DEPRINA, N.F., tekhn. red. IIIYEVA,
I.A..,
(Construction and operation of motorcycles]
Ustroistvo i
obsluzhivanie mototsiklov. Izd.2., perer. Moskva,
Mashgiz,
1963. 316 P. (MIRA 16:10)
(Motorcycles)

ii-'~ D. i. /f4 --I f-7i TjP( If, /F!~ T,
T IC) 11 11 F lk i!7 J 11
n. i
Ai,% Lri %r q-
06 L -
!Lrl
IS,
+
c c,
c :-ear
jong. 7he nwriner o-- sucil DaIr ~zxcltl--,l ~,,V 10%, TO L116
comolet-9 cessation o1, tjj,~ Drocess, j,,.cre-.,ec iniziaL
tlu-ee ttmes the nurrber o f electron-nole pairs Tria,,, electrc,~.., a,.,d
w~,ttl tile s ame
Card 1/2

ACCaESSION IIR- AF)~-03'1655
initial ener7,. il-rcl,:,n,-,e,-
ASSDOIATIO13%, Loningradsk.~y poljtekhniehon~jy jwtitut im. yl. 1.
Kalinina
(Leningrad Polytechrdc?-l Inttitute)
-M~D~ 2LDec63
VEMR 1 005
(C. 2/2

ILL _ _9rP,-_ 7_46 PP
, f~
')
j
f
kv ono;
F!.OLJRCE: Fizika tverdogo tela~ v. -i. no. f, -L'JDJ, ICVIII-4-
D i V-
e x e 'i sin s )n P.
re w
me n t 'I de vC C C- G
of these contained a source of a-kaline ions while the other
contained the single
crystal tarot, I w,-Iy that thc electric
A. Thp target was oriented in s~jch j
-'t- q,-imT I p wa.--, 7parnllel to tke 'he angle of incidence
C.,d 1 /2

A~'
-N 0
Ac- ion f the whpr the -V~~nt wz~ I thp Airnppn W,-IS
cnI-; wt,,~Ie the pullse of conlu~-tivi-l and PISO
I U 11 - - . - , ,
z wt,. i r h p v,:i ,r a Tr m rh
tl~e varfa-- -17 f r-!?,
w
en in
7 'e
c 'Inst i tute
D. rM
SOrMiTTLE); 29Lvc64
,NO PLT SOV! 003 OTHER: 005
21

L 5409-66 El-.'T(1)/EWT(m)~T/EliP(t)/FdIP(b)/DIA (c) LJP(c) jD I
ACC NR: AP5027306 SOURCE CODE: UR/0181/65/007/011/3159/3162
AUTHOR: Abroyan, 1. A.; Lavrov, V. P.; Titov, A. I.
ORG: Leningrad Polytechn[c Institute (Leningradskiy
politekhnicheskly institut/K6
r,
im. M. I. Kalinina)
TITLE: Secondary emission of germanium bombarded along various
cyrstallographic
axes by potassium ions
SOURCE: Fizika tverdogo tela, v. 7, no. 11, 1965, 3159-3162
TOPIC TAGS: semiconductor single crystal, single crystal,
secondary emission,
_germanium si 1e crystal
!5~' q I '." -I
ABSTRACT: The ion-electron emission of germanium
sing.;Le_.EU.Etaj~ is studied to
determine the effect which the crystal structure of the target
ha5 on secondary
emission. Germanium specimens were bombarded with potassium ions
at energies up
to 7 kev, and secondary emission was measured as a function of
the angle of inci-
dence. It was found that the coefficient 60.1 (the ratio of the
number of ions
reflected from the target at energies greater than 0.1 kev to the
total number of
Card 1/2
C) r?,,n,

L 5409-66 E%'T(1)/LWT(m)/T/W (t)/E'd'JP (b)/EMA (c) DF(c) JD
ACC NR: AP5027386 SOURCE CODE: UR/0191/65/007/011/3159/3162
AUTHOR: Abroyan, 1. A.; Lavrov, V. P.; Titov, A. 1.
S
ORG: Leningrad Po hnic Instity
lytec tp (Leningradskiy politekhnicheskiy Institut
im. M. I. Kai-inina) 4 )
TITLE: Secondary emission of germanium bombarded along various
cyrstallographic
axes by potassium ions
SOURCE: Mika tverdogo tela, v. 7, no. 11, 1965, 3159-3162
TOPIC TAGS: semiconductor single crystal, single crystal,
secondary emission,
ge ~aniu~m shingle crystal
ABSTRACT: The ion-electron emission of germanium singj~
~c~!tals is studied to
determine the effect which the crystal structure of the target
has on secondary
emission. Germanium specimens were bombarded with potassium
ions at energies up
to 7 kev, and secondary emission was measured as a function of
the angle of inci-
dence. It vas found that the coefficient 60.1 (the ratio of
the number of ions
reflected from the target at energies greater than 0.1 kev to
the total number of
Card 1/2

L 14131-66 EWT (1)/t1-JT W )I'TIMTP(t')/_EWP(b) Jjp(~ JDIAT
ACC NR; AP6000877 SOURCE CODE., UR 0181/65/007/012/366Q/3662
0
AUTHORS: Aby-oyan, I. A.; Lavrov,, V. P.. Fedorova, I. G.
ORG: J~!jinarad Polytechnic Institute Im. M. I. Kalinin
'(Leningradskiy politelchnicbeskly i-n-s-FIT~TET
TITLE: Angular dependence of the secondary-emission coefficients
of
single crystal KBr bombarded with potassium lons
SOURCE: Fizika tverdogo tela, v. 7, no. 12, 196,5, 3660-3662
TOPIC TAGS: potassium bromide, single crystal, ion bombardment,
~secondary emission, angular distribution
:ABSTRACT: This is a companion pa er to similar work b the
authors
F
on semiconductor single crystals ~FTT v. 7, 375_9, 196- The
pFesent
,investigation is devoted to the difiectric K_Bt tingle
crystals,Pwbose~
.p
(100) face was bombarded with Ou KeefRassium ion beam witb
energy;
~l -- 6 kev. Tffe- axis of rotation of the crystal coincide with
the
(1001 direction and made a right angle to the primary beam, the
di-
vergence of which did not exceed 2.50. During the measurements
the
CarJ 1/2

L 111131-66
.ACC NR: AP6000877
.target was heated to a temperature at which no surface charging by
LD
.the ion beam was produced (200 -- 300C). The results yielded non-
:monotonic variations of the secondary-emission coefficient and of the
positive and negative ion-ion emission-coefficients on the angle of
incidence. In view of the increasing dependence of the secondary
remission coefficient on the incident-ion energy, it is deduced that
at still higher energies the increase of the coefficient with the
angle will be steeper. This points out the advantage ol' using alkali-
halide compounds as cathodes for multipliers used to register ions
and neutral atomic particles. The positive ion-ion emission coeffi-
cient was found to be larger by a factor 4 -- 5 than the negative
coefficient. This is attributed to the fact that the reflected ions
of the primary beam contribute to the coefficient of positive ion-ion
emission. Authors thank M. -A. Yeremeyev and N. N. Petrov f or
interest
in the work and useful advice. Orig. art. has: 2 figures.
~SUB CODE: 20/ SUBM DATE: OlJul69/ ORIG REF: 0031 OTH REP: 001
~Card.___ 2/2

L 36322-66 EWT(1)/EWT(m)/T/EWF(t)/ETI IT(c) GU'/AT/JD/JG
ACC NRi APGO15792 SOURCE CODE: UiVO043166103010051083410839
AUMOR: '."Jroyan, I. A.; Yeremeyev, M. A.; Petro,, N. N.
OIX: lo-ni i-rad Polytechnic Institute im I.I. I. N., linin
kiy ilrititlit)
~z
(LeninCrnds1.iy poh t; lzntiichr-~i-
TI- I*": Irduced conductivity and secondary emission of
semiconductors aW dielectrics
uilioi- osi,Ave ion boiabardment TReport, Twelfth 1.11-Union
Conference on the Physical
Mi.,; -')f Cathode Electronics he-ld in O-c-tober--19G5/
ACU."CE. AN SSSR. Izvestiyn. Scriya fizichesknyn, v. 30, no. 5,
19G6, 884-889
TOPIC TAGS: nlkili linlide, s in[;le crystal, germt-nium,
secondary electron emission,
eleci-ric condiictivity, ion bombardment
'riie atitliors review the restilts of invcstigations conducted
in the Ion
-Pj-oce'sses Lnbovrt~i )I-Y 01 the Electronics Departiaeut of
the Leningrid Poly clinic Tnsti-
)1 1. nd germanium
LnLe cc 1(;,~ jIvectron cinission under ion bombii-dmcn4
oi~nlkalj
c
2nium ion bombard
in"Ic
rystnls tand condtictivity indLICed dryst. by ment.
1-r fixed energy of incident atoinic ions the SeCGiidary
emission coefficient of an
:iliz,-ili halide crystal decreased with increasing Ion mass;
the coefficient foi, 0.6 keV
1s+ ions incident on the (100) face of an NnCl cry-.3-tal wns 2,
and for 0.6 IcoV Ar+ ion3
thc ,;ccoiidary emission coefficient was 0.7. The 3ccondnry
emission coefficients at
U.6 hev incident ion energy for 11+, 112 and 11, Lons were
approximately equal, but
zL C.ard_1/2___

L 363 22-66
ACC NR- AlIG015792
at 10 kev tile necondnry emission coefficients for hydrogen
molcculnr ion.-, were greater
than for protons, and the datn were not. comptitibl-3 with the
hypothesis thrit the mole-
cular ion dissociates in tile first collision. Th-:i secondary
emission coefficient de-
creased with increasing tLempcrature of the crystal; this is
ascribed to scattering of
electrons oil their way to the crystal surface by )honons.
Monsurements were made at
incident ion cacrt;ier. down to 10 cV. Different iann behaved
very differently at very
l(,w Onergics; for some ions (110+ and Ne+ oil alkali halide
crystals) the secondary
emission cocffic~.cnt remained finite at the very lowest
onervics, whereas for other
ions their wasn threshold energy bel(Av which seccidnry emis3ion
did not occur. The
condtictivity induced in germanitm crysOls by n vait flux of
bombarding ions incrensed
with increasing ions energy nnd decreased with ir-creasing ion
mass. rrom a comj~arison
of the conductivity induced by ion bombardment with that
indticed by electron bombard-
mciiL it was estimated that n 100 eV K+ inon incic;ant oil
gcniinniiun given rise to about
6 electron-hole pairs. When the incident ion envrgy wns equal to
the threshold value
of F.Scitz (Disc. Faraday Soc. , 5, 271 (1949)) , , t least 30
'j'0 of the energy of inciden
I& ions and 5 % of the energy of I& ions was expc-nded in
inelastic collisions. The in
duced conductivity was maximum and the secondary emission
coefficient was minimum when
the ions were incident in one of the "transparent" directions
[116 , L-111] , and [112] .
Fr(xn a comparison of the induced conductivity and secondary
emission coefficients of
germanitun for electron and K+ ion bombardment, it was estimated
that only one in sever
al thousand of excited electrons escapes from thc crystal. Orig.
art. has: 1 formula,
7 figures , and I table.
SUB CCDE: 20/ SUIN DATE: 00/ ORIG REF: 105/ CFn1 REF: 001
Card

L 10066,~-67- (-I)/ W(n. )/T/ Elm ~t) /".,I - - Wulko) JIDIMIG
ACC NRi AP6015786
n, SOU11CH INDE: UR/0048/66/030/005/0865/0867
AUTHOR: ..Abroyan, I. A.; Titov~-A- I.-
ORO: Leni!!grad Polytechnic Institute im. M.I.Kal.~Min
(Imeningradskiy p6lU4~dlnIiche y
instA-ut)
TITLEt Changes in radiation conductivity under i.)-nbombardment
Atoport, Twouth All--
.Union Conferenco on the Physical Bases of Cnthodo Blectronicp
hold in Loningrad 22-26,
rl-1- IntTrz
SOURCE: AN SSSR. Izvestiyn. Seriya fizicheskaya, v. 30, no. 5,
1966, 865-867
TOPIC TAGS: germanium, single crystal, ion bombardment, lattice
defect, electric
conductivity, radiation effect
!
AMTRICT: The effect of bombililime t ith 3 keV K+ ions oil the
coefficient of radintlon
I
induced conductivity (r.-~t~o of tlizueed conductivity to the
inducing radiation flux)
iniumV'6 a
of a 35 Ohm cm gormr Entnl\ as been investigated by a technique
that is described
ielsewhere by tho authors (Fiz. tverdogo tela, 7, 2007 (1965)).
The surfnce of the tar-
.[,ct was perpendicular to the 1113 axis nnd the bombarding ionn
were incident ill tile
[100] direction. A dose of 10R4 ions/CM2 was found to reduce the
radiation-induced
iconductivity coefficient by an order-oi magnitude. -The
radinthn-induced conductivity--
:coefficient, as n function of the incidence angle of the
inducing radiation, showed a
!pronounced jrnximum at an incidence angle of 350, corresponding
to incidence in the
i

A 015786
N
N
[1101(liNection. Although increasing the dose of 3 kcV h+ ions from
zero to 3 x 1014
lions/ce' greitly reduced the radiation conductivity coefficient, it
did not affect the
position and relative height of this maximum. The number of pairs of
Frenkel defects
due to the ion bombardment was estimated by dividing the energy dose
by half the thresh
14 ions/cm2
iold energy for producing a pair of defects. For the 3 x 10 does this
cnlcu-
lation gave a defect density of 1.8 x 1016 cm-2, corresponding to
about 20 interstitial
germanium atoms in each channel in the (110)direction. The authors
argue that so high
in density of defects should alter the dependence of the radiation
conductivity coeffic-
lient on the incidence angle, and conclude that the defect density
was not actually so
high as calculated. Two possible reasons for the discrepancy are
suggested: either
there may have been a partial anneal of interstitinl atom - vacancy
pairs , or a par-
ticle moving In the LIQ direction in a germanium crystal may expend
considerably more
than half its energy in collisions in which the energy transfer is
below the threshold
-for defect production. Orig. art. has: I formula and 2 figures.
3U13 r-CDE: 20/ SUEN DATE: 00/ ORIG REF: 004/ Cq11 REP: 002
LCard _vIr

8/0 62/013/006/019/027
B102 SW
kUTHORSi G. T. and U. R.
TITLE# Hauohnaya konforenteiya Mookovakogo inthenerno-fiziaheakogo
institute (Scientific Conference of the MoscowtEnginetring
Physics Inatitilts) 1962
PERIODICALi Atoxnays, snorgiya, v'. 13, no. 6, 1962, 603 - 6o6
TEXTs The annual conference took place in Uay 1962 with more than
400
delegates participating. A review is given of these lectures that
or*
assumed to be of Interest for the readers of Atomnaya onargila.
They are
followingo L. 1. Loypunskiy, future of fast re&otorel A. A.
Vaoil'yov,
design of accelerators for superhigh oziergios'l 1. Ya.
Pomeranohuk,
analytic'Ityp unitarity, and aoymptotio behavior of strong
interactions at
high energies; A. B. Migdols phenomenological theory for the
aany-body
probl I Yu.'D. Fiveyokiy# deceleration of medium-energy
antiprotons in
matte., Y-7y.-goian, Ya. A. loollovskiyj theory of the MOsobsuer
offectl
M. 16 Ryasanov, theory of ionization looses In nonhomogeneous
madiual
Yu. B. Ivenovo A. A. Rukhadsof h-f oonduotivitl of-suboritioal
plasmal
Card 1/4

S/0' 62/013/006/019/027
Nauchnaya konforentsiya ... Bio2YB186
design of 30-Hey slootron linear scoolerstorl To, 6e Pystnovo Lo A.
Glaskov#
Y. 0. Lointol A. 1. Finogenov, G. N. Skepokiy, V. D. Seleaney,
sxperimental
characteriatica of low-enorgy el-otron linear aoceleratoral 0. A.
Zeytleak,
V. M. Levin, B. 1. Piskunov, V. L. Smirnov, V. K. Khokhlov,
radiooirouit
parameters of JIO(LUE)-type soooleratoral 0. A. Tyagunov, 0. L. Val
Idner
B. M. Ookhborg, S. 1. Korshunov, V. l.'Kotov, To. M. Moroz,
accelerator
classification and torminologyj 0. S. Miloyanov, V. B. Varakeiff,
P. R.
Zeakevicht theoretical analysis of magnetron operationj A. 0.
Tragovt
P. R. Zonk8vich, calculation of attenuation in a diaphragmated
raveguidel
Yu. P. Lazarenko, A. V. Ryabtsev, optimum attenuation length for
linear
acoeleratorl A. A. Zhigarev, R. To. Yelineyev.1 review on
trajeotographol
X" .-Uorosov," 0. A. Tyagunoy, review on more than 500 ion bourosel
Ut A. Abroyan,/V. L. Komarov, duoplasuatron-fyp* souros; V. S.
Kusnetwovo
A.-T-.-S-61-ny-ishkov, calculation and production of intense ion
boamal
V. U. Rybin (Ye. Y. Armenekly), inductive current transmitters of
high
sonsitivityl V. 1. Koroza, 0. A. Tyaganoyl kinetic desoriptionof
linear
acceleration of relativistic eieotronst A. D. Ylasov, phase
oscillations
in linear aoooleratoral E.'L. Burbhtsyn, 0. V. Voskrosenakiyp b4;&M
field
-effect# in the WaTtguide of an electron linear acceleratorl R. B.
Bobovikovp
Card 3A.

SOLNVSMVp A. 1. J KMROVp V- P.; XUZn-=Vo V. S.1 AMOTANO M. Aq
MNOVp N. F.
ZMU2??IKOV, F. G.; TOM# I. M-1 ZAEWTSKATA,, 0. IATMANISOVA, 0.
m.
and GERASIMOV, V. Fe
Current Injector for a Strong Focuased Linac.
report presented at the Intl* Conf. on High Energy
Accelerstore, Dubnav August 1963.

ACCESSION NRt AT4035115 6/3092/63/000/001/0119/0133
AUTHOM :Abroyan, M. A.1 Komarovo V., L.
TITLEt Pulsed large-current ion source
SOURCE: Moscow. Nauchno-isaledovatellskiy institut elektrofiziches-
koy apparatury*. Elektrofizicheskaya apparatura; sbornik statey,
no. 1, 1963, 119-113, and chart B facing away-from p.204
TOPIC TAGS: ionized plasma, plasma jet, plasma sourcet proton syn-
chrotron, plasma injection, ion beam, ion source
ABSTRACT: In view of the lack of published data on ion sources
with beam currents on the order of 1 ampe're and above, the authors
report an investigation of a pulsed ion source of the dual plasma-
tron type, intended for pre-injection in a.,proton synchrotron. The
present dual-plasmatron output limit, approximately 530 milliamperes,
has been increased by modifyin the geometry in the ion selection
19
Card

ACCESSION NR: AT4035115
region and by operating at a forced discharge mode. In addition to
attaining large current it was necessary to impart to the beam
definite optical characteristics to match it to the optical system
of the acceleratoritube. The plasma generation principle is the
same
as proposed by Ardenne (Tabellen der Elektronenphysik,
Ionenphysik und
Uebermikroskopie,-Veb Deutsch. Verlag der Wissenschaften, Berlin,
1956). The pulsed current reaches 1.5 amperes, and a focused ion
,abeam with a current of approximately 170 milliamperes can be
obtained,
with a minimum diameter of 10 nun at 70 keV. Experiments show that
:if an immersion lens with larger potentials and compensatiop is
used, a much larger,ion current can be focused in this diameter.
present value of the beam current is limited by the limits of
plasma flow through the emission aperture in the selection region,
and by the slight divergence of the plasma as it diffuses through
a
small aperture. Further increase in the ion cu--rent can be
attained
,by increasing the.aource dimensions and source parameters. A con-
tinuous current of.1 ampere can be attained by Inproving the
cooling
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ACCESSION NR: AT4035115
of the anode and of the grid in the drawing electrode. Multi-jet
-plasma sources, which produce a dense plasma with large surface in
the selection region, will contribute to the production of larger
ion beams. The authors thank 1. P. Maly*shev for interestlin the
work, F. G. Zheleznikov and A. 1. Solny*shkov for a useful discus-
sion, and V. S. Fok,"06n, V. A.i,Grinevich, and 1. 9. Dorofeyev for
help with the work. Orig. art. has: 12 figures.
ASSOCIATION: None
r
SUBMITTED: 00 DATE ACQ.- 07May64 ENM: 02
SUB CODE% ME, NP NR REF SOV: 006 OTHER: 003
Card 3/5

1,CCZSSIOII NRt AT4035115
ENCLOSUU:01
Construction of ion source
gasket, 2 - coil, 3 - a=or,
4 cathode , 6 - cathod current
-lead, 6 - gas supply, 7 -'iziiemed-
iate anOd8 . 8 - cooling unit j 9 -
Pvincipal anode, 10 - drawing electrode
with grid, n - water
Card 4/5

Principal diagram of test stand
vacuum containert 2 -- &wAliary
container in which the tour