SCIENTIFIC ABSTRACT AYUKHARNOV, A. K. - AYURZANAYN, B. A.

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• Collection: Scientific Abstracts
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• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 6, 2000
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

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AUTHORS1 Ar-..fov, U. A., Ayukhanov, A.U., Starodubts,qv, S. V.,
56-4-3/54
TITLE: On the Coefficient of ffusion of lono as a iunction of the Ra-
tio of the Masses of C61liding Particles (0 zavisimosti koeffit-
siyenta rasseyaniya ionov ot sclotnosheniya mass stalkivayushchi-
kh:iya chastits)
PERIODICAL% Zhurnal Eksperim i Teoret. Fiz-..ki, 1957, Vol- 33, Nr 4,
Pp. 845-
-8,50, (USSR)
ABSTRACTt By means of the method of doubLe modulation the secondary
emission
of ions wqs investigated for Vie case that the masses of the bom-
barding ions are larger than tae atom masBes of the target. The
following conclusions may be drawn.
1) Positive Cs-ions enter into interaction with nickel atoms ac-
ocrding to the condition Vi m2:
a) Neither in the case (if a cToldm~3ooOK) tor of a hot nickel sur-
face (13500K) may there be detected any sE!condary ion-electron
emission
b) The secondary ion em.-'LS8ion from a pure nickel surface ( at high
temperature) contains only thE vaporized ions which formed on the
sx;irface of the target after a diffusion process.
2) Positive Ba-ions enter int(raction with molybdenum atoms accor-
dJ_n8 to the condition Vi 9, H,j m2l
a) Feither in the case of a cold (300'K) nor of a warm molybdenum
Card 1/2 surface (13ooOK) may there be detected an.,i secondary
ion-electron

ARIMV, U.A.-,, MKIWOV, A.Kb.; STAPODUBTS11r. S.Y.
Secondary emission of negative partilcles duri-ng
-the bombardment
of foreign films on pure metals witli alkali mstal
iona. Izv. AN
Uz.SSR. Ser. fis.-mat. nauk n0-2:1107-115 '58- (MIRA
11:10)
1. Fizi'ro-tekhnicbaskiy institut AN UzSSR.
(Ion beams) (Alluili metals)

ARDPOV, UoJ,.o; ATUEHUOV# kplhe; SWRODUBTUVe Soy- I
ERWZH'ML'U'A=l Oyo lh*Uo
... ... -,
Met,hode for investigating seconda-ry process(le Osn~Od
by tons at
hj(~, target temperatures during Viiermoele6tPOMO
emission. Izv.
AN Uz.$M.Ser.ftz.-mat-nauk: no.5:15-22 '511- (YaRk 1l:
12)
1, liziko-takhnicbeskiy institut J%N USSSR-
(Illectron emissio,n)

.1
901
SOV/20-124-1-16/69
AU~kORSI
ArJ.fov, U. A., Academici&n, A;i
Uzbekskaya SSR, Ayakhanov,.. A, Kht 0

Staxodubtsev, 461. V.,
Academic:'.an, AS UzlDekskaya SSR, Khadzhimukha-

medov, Kh. Kh.
TITLE:
On a Method of Investigating -.he Secondary
Processes-Which Are

Catised by Iono at High Temperutures of the
Target in the Case of

a Thermoeleotranic Emission 0 metodike
issledovaniya vtoriehnykh

protseseov, vyssyvayemykii ionami pri
VYBDkikh temperaturakh misheney

v prioutstvii 1;ermoelektronnoj
emisaii)
PERIODICALz
Dol:lady AkademJ~i nauk SSSRv V599 Vol
.124, Nr 1, pp 60-62 (USSR)
ABSTR)iCT:
It was interesting to
perfect the methol of double modulation -used

for the
invest:Lgation of secondary ion processes at high temper*6

u
tU3.'eS (at which a flux of the't,mal electrons exists). The
apparqi

used was similar to one that ':Las already been
described (Ref 2)

with the exception that an ell)ctrically
heated filament was sub-

stituted for the plane target. A
schematical drawing shows the

principles of the electric wiring
diagraJ2. Target temperature was

determAned from the heating
o!.irrent and fxom the diameter of the

filament; the 'Nork
function wis determined. by the method of

Richardson straight
lines, tarting a correction for the 'Schottky
Card 1/3
effect
into amant. Tbm primary and secondary ion fluxes and also

SOV20-124-1-16/69
On a Method of Investigating the Secondary -"rocesses Which
Are Caused by ions
at High Temperatures of the Target in the Cuse of a
T;heruoelectronic Emission
the current iiitensity of* the ~,hermal oleotxons were
determined
from the' coordinates of 'oncill.ograms. 131 t:aO 06B0 under
investiga-
tion the application of the mthod of double modulation is
reduced
to the following: thq primary ion beam accelerated by the
field is
modulated with respect to int(insity by a generator for
rectilinear
pulses with a frequency of 500 - 1000 0701,98 (first
modulation)
and direationedl on to the tarilet. The flux of the secondary
emission
from the target is then colleoted by a collector and is
transmitted
to the imput of' the vertical amplifier of an oscillograph. The
horizontal development of thin oscillog:rap12 is synchronized
with
the generator of the saw-tootli pulses. Thriae oacillograme of
a
filament-like W-target (which was bomba:rdell with 840 ev
K4*-iona)
are added at 16000 K. Secondary ion emitision consists of 3
components.
On the basis of' the here disatissed examplea it is possible
to de-
fine the coefficient of the soccadary ion (~misaion as the
ratio of
the sum of components of the ijecondary :Lon fluxes to the
primary
ion flux. The amount of this noefficient dopends in a
complicated
camner on the aftergy, the ioniuation potontial, the mass of
ions,
the temperature, the work funution, and thin mass of the ions
con-
Card '4V3 tained in the larget. It.ia tbus possible, by the
here discussed

SOV/20-124-1-16/69
On a Method of Investigating the Secondary Processes; Which
Are Caused by Ions
at Righ Tetaporatures of the Target 'Lit the Caue of a
The-rmoelectronic Emission
improved methDd of double modulation, separately to
investigate
the individual compononts of secondary emission, vizz the
amperages
of the scattexed, evaporated, and diffteeid ions, as well as
the
thermoelectro,me occurr.'Lng in the bomberdnient of pure
metal targets
by Positive iDne (at high temperature in the presence of
consider-
able-thermoelBotronic omiesion).'~There are 2 figures and 3
Soviet
references.
ASSOCIATIONt Fiziko-tekhnioheBkiy institut
(Physico-Techaical Inw;itute
SSR)
Akademii. nEkuk UzSSR
of the Academy of Sciences, Uzbekskaya
SUBMITTEDt August 29,,1958
Card 3/3

4-1 x
'71 3
AUTHORS:
TITLE:
PERIODICAL:
J17~
s/0110 0 C24/06/15/017
B01CI/B067
Arifovj U9 A,, Ayukhanovq Ji.. Kh., Gruich, D. D.
On the Problem of Scattering of Slow Alkali Ions From a
Metal Surface
Izvestiya Akademii naialk SSSIL. Seriya fis;icheskaya,
1960, Vol. 24, No. 6, ?P. 7`10-714
TEXT: 'This is "the reproduotion of a lecturti delivered tit
the-9th All-
Union Conference on Cathode Electronio.9 fronOotober 21 to 28,
1959 in
Moscow. For the experiments desoribed here tho authors used the
experimen-
tal arrangement described by Arifanov et al. (Refs. 4, !i, and
6) in
p,,revious papers with minor moll if ioatioi:isa '.q-..ge. 1p 2
and 3 show the de-
pendences of the egpttering ooefficient on %he energy of Na+
and K+ ions
in the bombardmentjbf a pure -tungsten aurface, on the, energy
of Cs+-ions
in the gombardmint of a well urified Ni-eurface and a less well
purified
Ni-surfaoep and the dependence of I on the energy of Na" and K+
ions in
the bGubardment of a pure tungsten au:rface. ~ denoteei the
ratio of the
limiti.~g energy of' scattered ions and the energies of'
primary ions. ok~
Card 112

82170
On the Problem of Scattering of Slow Alkali Ions
S/04,8/60/024/06/15/017
From a Motal Swaface B0150067
Furtherimoret the voltampere oharacteriatice of secondary
ion emissions
are shown in Fins. 4 and 5. In the diocusaicins of the
results it is pointed
out that the soattering coefficient attaine its maximum
value when the
energy of primw,%y ions attains the value of the bonding
energy of atoms
in the target. For this maximum value, 45 aud 43 ev are
given for pure
tungsten, and 42 ev for pure Ni. In tho further discussion
of the results
the dependence of 71 on the onergy of primary ions (Fig.
3) is explained
by the influenoo exercised by the bonding energy of
tarj:ot atoms.
There are 5 figures and 8 references: 7 Soviet and I
German.
Ix
Card 2/2

v,

5/04 87~1610')624/06/16/01 7
X)

:BO1q/BO67
AUTHORS:
_AFukhanov
, A*
Kh., Lolchako'f,
G. I.

TITLE;
Uiie of Mass �2eotrometisrs ol

the
Dynamio Typo to Investigate

Socondary
Processes

PERIODICAL:
Ijivestiya
Akademii nauk SSSR.
Seriya fiziohookaya,

i!i6o, Vol
. 2,10
No. 6, J)P. 715
-722
TEXT: This is ilia reproduction of a lecture delivered at the
79th Aall~
Union Conferenoe on Cathode Electronl!-(is from Ootober 21 to 28,
1959 in
Moscow. In the introduction to the present paper, the authors
dqmonstrate
that now mothode must be developed to study secondaiZ_omission)4f
oon-
taminated surfacce; whioh make it posvible to 9ru_d_y__1;ne'
`aeo-1775-n component
and the oompononi of negative ions of' secor4ary amicsion. The
investigation
of secondary enission by meane of ordinary magnetic matte
spectrometers is
impossible, and the authors tried to study secondary emission of
surfaces
of different states in their bombardment with ions. This was done
by using
a magnetic maefi spectrometer in which the energies of the ions
were mo-
dulated and multiplier was used to record the ions. The device
with vhich
Card 1/2 - &W

8217:1
Use of Mass Spectrometers of the Dynamic Type to S/011
60/024/06/16/017
Investigate Secondary Processes Boi%o67
the BOCDndary particles were analyzed is discussed with the aid
of Fig. 1.
A rectangular j,,,onerator is used to modulate the pria,ary
ions. The study
of the secondary effects on rapid change ir the state of the
bombarded
surface is regr.rded as the main problem. This was achieved by
applying
various films of alkali metals and of alkali halide salts. The
experimental
results shown in Figs. 2 to 6 are discussed in detailq and the
energy
distribution of' secondary ions (Pigs. 7, 8) :Ls discussed. It
was found
that on the application of an alkali motal film to a,
Tit-surface very strong
changes in the ion component of secondary emission ciocur. Above
all, al-
ready a small mount of alkali atoms ohowed an intensive
sputtering of
adsorbed gases in the form of negative ione on the curface. ,n
general,
a sputtisring of' atoms in the form of negative ions could only
be observed
when tho formation of chemical compounds ort the bombarded
surface was
possible and when it was accompanied by a dissociation of
molecules.
In conclusion, the difficulties in detormiriing secondary ion
emission
for negative ions are pointed out. There are 8 figures and 6
references:
4 Soviet, 1 Gemanp and I American.
ASSOCIATION: Irtntitut yadernoy fiziki Akademii nauk SSSR
(Institute
Card 2/,'! of' Nuclear Physics of the Academy of Sciences, US~Hj

3LL 062
S/166/'61/000/006/003/010
~;29 6. ~'? 13U BI 02/11138
AUTHORs Aril'ov, U. A., Academician AS U2bekskaya SSR,
Ayukhanov, A.Kh.
TITLED The nature of 8econdary emissior ariaing whou alkaline
coatings of metals are bombarded with alkaline ions
PERIODICALs Akaden.iya nauk Uzbekskoy SSR, Jzvestiya. Seriya
fiziko-
mateme-ticheskikh nauk, no. 6, 1961, 34 - 39
1
TEM The charj--e and composition of secondary emission from
tantalum
and tungaten bombarded with alkaline ions were studied in
dependence
on.the steadlily increasing alkaline conting, its
compoi;ition, and the
rate of deposition. Standard experimental 1.echni-.1ue wao
used, The
electrons were eeparated from the negative long b.,i a
maiMetic field of
400 oe. The pressure in the apparatus was 10- mm Hg.
Measurements at low
rates of deposiiion showed that the negative component of the
secondary
emission was relatively high and increased vith the d.enoity
of the film.
At highe:r rates (-20 monatomic layers per see) the secondary
emission of
negative ions increased rapidly with density, reaching ft
maximum after
about 2 Bee, then falling, almost to the initial ralv,.e.
Ion-induced
Card. 1/2

S/166/61/000/006/003/010
The nature of secondary emission... B102/E.138
electron emission is almost independent of layer densit~r. The
coeff-*,-
cient of negativa secondary ion emission depends on the method
of target
treatment. If ion bombardment is carried out immediatel.y
after high
temperature treatment (25000K) the peak can be lowered. At
higher
densities the nature of the backing had almost no effect on
the secondary
emission, The presence of negative ions in the seconda3-y
emission is
attributed to the lowering of the work function of Ta or W
surfaces by,
alkaline ion bombardment, possibly to a. value below the,-. of
electron
affinity for certain gases, especially oxygen, which aro
adsorbed and
ejected again by the bombardment as negative ions. Thia is a
source of
error which must be taken into account in meisurements of
ion-induced
electron emission. There are 3 figurefj and 10 references: 8
Soviet bLnd 2
non-Soviet. The reference to the English-laaguage publication
reads as
followT:: P. D. Moon, Proo. Cambr. Phi,, Boo. 1931, 27t 570-
ASSOCIATION~ Ak%demJya nauk UzSSR (ActLdemy :)f Sciences
Uzbekskaya SSR)
SUBMITTE'D AuF;ust 21, 1961
Card 21~_)

31066
S/166/61/'000/006/007/010
C~2 6. .~?'3 /'q B102/B1 38
AUTHOR5. Arifov, U. A.9 Academician AS Uzbekskaya SSR, Iyukhanov,
A.
Aliyev, A. A,
TITLE: The? angular distribution of alkaline ions scattered from a
metal surface
PERIODICALt Akademiya nauk Uzbeksko,y SSR. Izvestiya. Seriya
fiziko-
matematicheskikh nauk, no. 6, 1961, 57-64
TEXT: After ar introductory discussion of the results of own and
other
pre,.rJous paperEj, the authors give a aetailed description of the
apparatus
and procedure. The electrical measurements were based on an
oscilloscopic
method with double modulation. The primary ion bearr, modulated in
E,qu&re pulses, was focusad on the target, a 0.02 mm thick Ta or
Mo plate.vi
The target was encompassed by a cylindrical collector nhielded
against
parasitic currents.. Between target and collector we,11 a mo-ble
probe was
installed, for neasuring the secondary-ion inten3ities. The
targets were
purified by ral-Ld heating up to 2400 OK, the measureuieni;s were
made at
Card

310t~ 166)'61 /000100610071010
The angular distribution of alkaline B102/11136
'3500K and a piessure of (2-3)10- 6 mm Hg. The targett was
bombarded by Na
ions %ith enerFaes between 300 and 1700 ev. The nualber of
scattered ions
was found to be inversely proportional to the ion eriergy,
and the angular
distritution was independent of energy~ Angular
distr:Lbutions of the
intensity of scattered ions did not depend on target;
temperature
(300 - 15000K)~ Angular distribution wa3 Eilso almost
:Lndependent of the
angle of incidence of the primary ion beam, The coeff:icient
of secondary
emission incree:.sed with the angle of incidence G. If *.he
mass m2 of the
bombarding ion ie less than that (ml) of tYe target atom, the
angular VIK
distribution of' the scattered ions will be almost a
cot3ine-e curve. The
cosine-0 shape6 distribution is independent of the etng:.e of
incidence.
M, A. Yoremeyev end M. V. Zubchaninov (ZhEIF, 1942, No. 12,
358) are
mentiored, There are 6 figures and 16 referencest 6 Soviet
and 10 non-
Soviet,. The fcur most recent references tc English-language
publications
read ae followt: Langacre A. Phys. Rev, 19,4, 46, 407; Massey
H. S..,
S,,ni,r,h G. Proc,, Rcy. Soc, , 1933, 16, 5701 Rcuse 0. Phys
, Rev, , 19,47, 52,
'238; Amdur J., Pe,drelman, J. Chem, phys, 1W, 8, 7-, 1943,
11~ 57.
Card 21j- ~,/z --r--Tec-

145133
S/166/62i'000/006/008/oi6
B104/Bi8f;
AUTHORS: Sharipov, N. A
"khaXLvY_"._., Kh,
TITLE: The correlation betwibn thevmionic emission and
secondery
electron -emisnion from some typea-of oxide-ooated cathode$.
on ajotivation
PERIODICAL: Al:ademiya nauk Uzbekekoy SSF.. Izvestiya. Seriya
fisiko-
maAematicheskikh nauk, no.',(-, 19620 66-70
Tur; The obange in the thermionic emission density i and the
secondary
electron emission.ooefficient a during activation of the
cathodes of
6117 (6N7) and.6',e (6N8) tubes and of the carbonate-coated
(BaCO 50%, SrC0 50%, BaCO i00%) cathodes in-glasirentelopes
3 3
at 1*10-7 mm Hg were measured by an inertia-free double
modulation method.:
Results: With the double modulation methaS the thermionie
emission and the
secondary electron emission could bo meaaared sithultaneously
and for the
same state of the oxide-coated cathode when the voltage of the
heated
ciithode was 2-7 V, the energy E0 of' the peimary electrons
was in the
Card 1/2

S/166/62/01)0/006/008/016
The correlation between thermionic ... B104/B186
region of 1200 ev and the collector voltage was 65 v.. 6 increases
rapidly
in the initial stages of the activation and somewhat more slowly
later-,
it is practically the same for (Ballsr)0 and (BaSrC&)0 at current
densities
of (. -6 2
1-55)110 a/cm 9 and somewhat higher than for acAivation energy. 'The
form of a(E ),remains Practically unchanged. There axe 6 figures,
0
ASSOCIATION: Institut yadernoylfiziki AN UzSSR
(Institute of Nuclear Physiiis AS UzSSR)
SUBMITTED: September 15, 1962

S11 09/62/007/009/013/018
D409/D30-1
AUTHORS:
4 ,:,A..,~ukhanov, A.Kh.v Vos"rilova, N.V., iuid Shustrov, V.A.
TITLE: Evapora:tion of oxide-oathole components during its
operation
PERIODI t'.10AL: Radi tekhn
'.A
15980 1Vor" 411., 1elektronikaj vq'i 79 no. 9, 1962p
TEXT: The evaporation of the components of bariura-strontium
oxide
conting:3 of various composition was studied by thes method of
radio-
active isotopes. Earlier studies of the temperature dependence of
the r.~ta of evaporation ol" the components were qostly of a
co.-,'Ipara-
tive nature; t.'.11e dependence of the rate of evaporation on
the compo-
sition'of the .',%oating was not ascertained and the dynamics of
eva-
poration were not studied. The method u3ed in the present
investiga-,'~/
tion made it possible to obtain quantitative resu:'.ts and to
study
the evaDoration over sufficiently small time-inte3. vals; in
addition
it also permitted to perform a large nunber of various operations
with th~.- same !-.athode specimen unelor tha same vacuum
conditions.
The experimental lamp wds continuously evacuated by two nercury
Card 1/4

S/109/62/007/009/013/018
Byaporation of oxide-cathode ... D40q/D!.;O1
coating. UVapOrELtion at-increased temperatures of the
activated ca-
thode, is apparently related to th(: fornation of a solid
solution
(Ba, Sr)O and the appearance (in the laiter) of free Ba and
Sr. The
change in the r,fLl;e of evaporation of Ba as a function of
time, was
studied over a temperature range of 10OC'-15000K, A figure
shows the
chance in rate of evaporation from ooatJngs-ivhich contain 30
% and-
100 a Ba., respectively. Anotlier filriare -hows the
dependence of the
mean rate of non-equilibrium. evapo,..,atior. of Ba Emd Sr, on
the com-
position. of the, coating. These curves are characterized by a
maxi-
mum for coatinEs which contain 70 5D of 1he
respective:carbonate.
Hence the presence of the maximum is nol a property o ,f the
solid
solution (Bag 'Sr)o, and tho obtained curves are rela t� d to
the be-
havior of the free metal in the cr3r,3talline lattice. . n the
process
of.heating the cathodev depletion of the Ba-layer sets in at a
cep-
tain temperature. This leads to the parE.doxical conclusion
that
(from a certain. temperature oil) the rate of evaporation
sl'ows down.
It is concluded that evaporation of Ba end Sr was practically
not
observed during the decomposition of the enrbonates.
Evaporation
becoutes'significant only during the activntion process, at
tempera-
tures above 10000K* At that staget '~he Evaporation is related
to
Card 3/4

S/04 8/6 2/02 6/011/001/021
BI 02/B1 66
AUTHORS: Mo-ro:ts L. P-* and Ayukhanov, A. Kh.
.............
TITLE; On a possibility of determining the offactive depth of ion-
indui:ed yield of secondary eleotrons from dioleatrics
PERIODICAL: AkAdemiya nauk SSSR. -Izvostiya. Seriya fizicheskayap
v. 26, no, 11, 196?, 1322-1327
TEXT: The coef:irlcient y of ion-induced eleotron emiasion plotted
versus
the thickness of an all-Lali-halide lay-ar on it metal backing,
nhows
saturation. Tho depth from which the soconcary elecLrotio are
emitted can
be dotermined fn)m thio saturation. Ideaeuromexits wexe made with
NaCl
films dE.-posited on molybdenum sheets. Theso were bombarded by
ions of
energieD ranging from 0.2 to 2-5 kev. A sp(!cial method of ener8y
mod'ula-
tion waci applied so that the dependence of the coeffLciento y of
.secondary emies-on on the film thickness could be measured
simultaneously
for two different energies of the incilent %ons. Tho target was
exposed
to square pulseo of the ion current; the froquency was varied
between 50
and 100 opup tho awplitude between 0 and 701) v. The curves I/Ysat
n f(t)
Card 1/

S/048/62/026/oi 1/014/021
Some p:ropertieti of the ion B 1 ' 25/31102
particles leav.-Jig the surface of target 1 could reach target
2. The
existence of end-point energies of th,D .9cattered iorj.s
.*,ndicate an
individual elatitic collision of the iaciderA ion with an atom
of the
target UnaCCOM-ALnied by charge exchange. ]`or a part of the
elastic
collisions of ";he primary ion with target i4toms, an elactron
is captured
and the ion is neutralized. When thia neutral beam, hJ.ts
target 2, it
causes surface ionization and secondavy emission. 1he high
energy of
particles knocl;cd-out from target 2 'Dj neutral atomc can be
explained only
in the followinE, ways: The neutral ,.omponent of the-
socondary emission
contains scattored neutral atoms. The neutral acome, hitting
target 2 leave
it as positive ions and retain a conoiderable part of thoir
energy.
During the bombardment of target 1 by 100-ev Na + ions,
secondary ions of
77 ev ILre emitted. If neutral atoms of EMEX , 77 ev hit target
2 the
end-point eneriy- of the secondary ioni; from target 2 amounts
to 59 ev,
The delay curvo for bombardment by secondai-y ions is similar
tc the delay
curve for bombivdment. by secondary noutral atoms. Tho fast
neutral atoms
are alao elastically scattered if ta:~get 1 is at other
temperatures.
The intensity of the neutral componen-, remcinB almost constant
up to
f'.irl 213

S/04 0/6 2 / D26/011/001 /021
On a possibility of determining ... B102/B186
were compared fo.r several pairs of ion onorgy. E.g. , fDr Na+
ion energies
of 450 Lnd 920 wi two curves are obtained: oaturation is reached
first
(1.0. GA a SMO,110:7 film thickness) with the lower ion onergy.
With ion
energies of 1360 and 1640 ev a single uurve is obtained, i.e.
saturation in
independent of t;ae time t of NaCl deposition. Since t-.Id, it is
independent of tho film thickneso. These measurements ahow that,
if the
lower energy Ea i:"I of the two ion energiea io below a critical
value E orit'
the coofficient 5:' ion-induced electron emission will coaae to
depend on
the film thicknesn as soon as a certa.in thickness d sat is
reached. doat
decreases with denreasing ion energy. Fo r 2, mid, Ecr'Lt y
reachcj
saturation at eqlaal film thickness, not depending on the ion
energy. For
No+ ions, Eer is of the order of 1000 ev. Tho curve:3 -//Y,,t
-f(t) are
compared with Ahe curves (I/Cr sat - f(t), where 6 is Vie
coefficient of
electron-inducid electron emission. At primary-electron energioR
%>25C1 ev, 6(1) xeaches saturation at cquvA film thl.ckness
independently
of Ee. This tI,ic,,.ness corresponds to the d.epth from which
the secondary
Card 2/3

S/0,18/62/026/011/014/021
Some propertii!s of the ion ... B125/13102
T"110000K. The current increase that attends furth-~r
temperature rise is
due to thermal. ions. The secondary neutred emission and the
secondary
ion component apparently contain the same groups of socondary
particles.
The SCILtterini,: mechanism of primary ions from a metallic
surface in the 01
form of neutriJ atoms is essentially similar to that of the
scattering I-
of positive ions. There are 5 figures-
Card 3/3

)41)112 ~11
S104EV6,?1026101110201021
B1 2 5/ B1 02
AUTHORS: Arifov, U. A., Ayukhanov, A. Kh., and Allyevp A. A.
TITLE: krigular distribution of scattered secandary ions when
heavy
ions bombard light targets
PERIODICAL: hkademiya nauk SSSR.. Izvesti.ya. Seriya
fizicheskaya,
v., 26, no. 11, 1962, 1440-141.5
TEXT: Hot molybdenum (14000K) and nickel 11000K) targets were
bombarded
with fast Cs+ lons (500-1200 ev) and the a:-tgular
distribution of the
scattered ions was measured. Apparatus anil~ measuring methods
have been
described by Arifov et al. (Izv. AN UzSSR, Ser. fiZ-.-MILt.
nauks 6, 571
(1961)). In order to retain evaporated ions irom tbe
c,ollector, a voltage
of 1 v was applied between target and collia,ctor. The
currents of
scattered ions were measured with a movablo probe. Fox angles
of
.incidence betw,?4)n 00 (normal) and a certain limiting angle
the currents
measured were xoak and the dietribution wa* coeine-Uhaped. At
angles of
incidence ~ lirk:er than the limiting angl* (scattering angle)
Gin-1(m JIM2) the conditions are complel;ely chanj:ed, the
weak probe
Card 1/3-

3~5'~4
sA~20 162/42/006/006/019
BlC47,1108
AUTHORS: Arifov, U. A., Academician AS Uzbekskaya SSR,
Flyants, N. N.,
E,nd Ayukh_an2z,.&- _K111.
TITLE: Some properties of secondarl ionic-neutral emission
P E-RIO DI CAL: Akademiya nauk SSSR. Doklaliy, v. 142, rio. 6,
19b2,
1265-1267
TEXT; Two Ta targets, each surrounded by a collector and a
protective
cylinder, wer(i placed in a T-shaped glass container. Target
no. 1
(30 b:f 7 by O.,C15 mm) was bombarded with ions generat(!d by
surface
ionization of an alkali halide. All charied particles between
the two
targets were ileflected by the field of a oapacitor so that
only the neutral
particles emL '.tod from the surface of tarj:ut no. I coudd
regch tarCet
no. 2. Pressure during measurement was butween 1 and 3,10- mm
Hg.
Prior to each -measuring series the tareeto were heated to
2,5000K for
6-8 hours. The naximum energy of the neu,;ral atoms striking
target no. 2
by bombarding target no. 1 can be calcula*;ed from the relation
Card '112
P

ACCESSION NOr AP30DO223 3/01661(63/000/002/0065/0069
AITTHORSt 13hustrov, Y, Ati Poltoratskiyj Vs lei 4mkhanov, ke 11,
TITM- On the role of barrier formation in the wthode sputtering
process
SOURCL'i W 'UzSSR. Izve Seriya fiziko-matem, 7iaxiOno. 2'j 1901
65-69
TOPIC TAG!;r contin-aouo sputtering, tungsten targ(itt ion nourotiq
surface ionization$
p4l,tative ion
:ABSTRACT: An experLment has been performed -to coupare
qualitatively' two processes:
continuous sputtering of material and knocking-out target naterial
forming a
chemical ccqnpound wLth the adsorbed substances. 1he experiment was
done in a jo-7
mm Hg vaeuvia, using a heated tungsten target. and an Na and K icn
source of I to
1OjA a/cm2 density. The latter was obtained by means of surface
ionization over an
incandescent tungston wire. The sputtering product was accumulatsd
*n a collector
nade 04' 0-5 mm nickol plates. Experiments ivere dcne in three
i9teps. First the
tungsten target was kept cool and the sodium ion beam was turned on
at 1600 ev
energies with the collector potential V at stero value. Next V was
set at -140 v,
followed by raising the target temperature to 116CK. A graph of
%thode sputtering
Cara

iACCESSION NOi AP30)O223
.coefficient versus ~)olleotor potential shows that the greater jart
of thi Imocked-
out negativa ione puisesses an energy of 20 ev. For V f: -140 N' the
collector
contains only neutral particles. Under potassium Ion bombardment, a
noticeable
amount of negative tungs ten- containing compounds Is observed ix.
the oputtering
,products. Orig. art. has' 4 figures and 2 formulas.
-ASSOCIATIONt Fizikt)-tekhnicheakiy inatitutKI UzSSR
(Phyaical-Tedmical Institute
AN UzSSR)
ISUBMITTED: OBJan63 DnE Acq: 1:?,run63 MICL: 00
SUB CODE% M NO REP SM 006 OTHER 1 004
Cwd 2/2

SAW 63/0 OZ!/002/01(5/028
D3,08
Arniona: nyants :;.N.N. ArUoiri U.A. axid
-TITLE,:: Transient- secondal-
-y ai4ission processes during ~o
bardmentlof.filmli n
o 1~etals by fast neutral atoms
of anotIvir elem6rd:
PER101 ICAL: it
ejCj
adi ckfinika 3. ohika v. 8, no. 2 3.963
311-3L5
-Althoughiin the at;udy~': of the int-pra tion 0" atomic
part#les ima solid surfii6es it icj.of;~value tc; k4ve tigate bombard
ment 4y neutral atoms as.,~woll as t~r ions, this h.~s been neglected
because of tiie difficulties of obt,
-air~xg suitable fast atot,~i beams
and wiasuring their secoz, ary efftcts;~~ the exper'iments that have
been- done, r, ach as by Chaudry and Khau, have an!, rmation
y givc!n info
on sc4:iond electron eml'.saion. The outhors havit. m&cqcurcd the soc-
ondax-i' CMIMOU of positive and iiegat.i've ions from, 'a' Ta target
both
in th(.,i clean! state and dti':ring deposition of a Ila film,
boutbarded
xdth either LOns or neuti,al atoms of- fia and K of energier, i~p to
Card 112.

S/1010/di~/POO/002/010/028
J.,
ros
dind An*h MOV A.Ith
ij)n the
atj IMt'V?eeu 1rhe -negatjv~ _Jon and electron ';7
0
COMPoneUte of tbm sec.4indary extissiou from jqaCj f ilms,
bombar0d_ by Na-0-1 Rb+* land 08+ 'jvrm
PEA%
ODICAL., Radiotel4mikA i "lik miorditai v. no. 2,
J 322-327
W
. -Several workers bave itudied the!negatlive.accoindixy I
t
GmistlOn f r01:' &I U-1i himilde MM bomt~ardqd by i(')ns, but have
not."
~:distihgluished between the.nogative_iot~ and
on cj~mponents, which
~,Car- 9;ive mis%aading results. The. auttiors have moasurod these
compt)n__
ent s in the 4 m4 a sion'from K40 I f L Ime a m No or Ta undo I,-
bombardn, ent
by No.+ and 011+ ions in.the enermy ranp 150 - 2100 ev and Rb+ ions
in thm range ~200 - 1600 Im, 4urb.-ig dep6sition of 'the NaCl. ' The
chcr_~
Acteristic ol! the negative.ion e1nigsiott agreed CIOSOTIP i-rith
that of
the PositiVa-'ion cmissiono risinj sharply to satuxration at a thick-
ness porresponding to a 11~10n-atomfo 14ytr and beir~g oubstantially
n-
I'Card 1.
A

1~

AID-Nr. 981-1 3June
AlEASIMING SECONDARY ION AND ELE CTRON EMISSION ~DURING FILM
DEPOSItION ON METALS (USSR)
zl=and S.- V. Starodubstev. Radfotekhnika
Arifov, 'U. A.. Aygkha
i elektroidka, v. .8. no. 4, Apr, 1963, 669-674.
3/109/63/000004f017/030
I A vacuur, fi-tube Inj Itrument is described which P(irmits
improved observation
of high4peed dep)'sition of Na or Mg on a Ta siI-bstrate. The device
can
sec hdary em'sslon from the target
measure imultan6ously the coefficients of 0 1
surface caused, by' either bombardment byparti(iles of two evergy
levels or by
alternate' bombartment of electrons and ions. 1,4his electriclil
circuit differs
from the usual double modulation circuit. in thati the borqbardtng
particles are
1 energized both wiih a d-c poteirti-J, RIO, and a e'quare-wa- e
~generator, whose
i wave forrii is in turn modulated b, ;~~i
y a sinun I dal i ioltage Ea sin wt. Thus a
current of secondExy particles, changing r~eriod;,cally per I ti
I(Fd + Irusinwt),
I
card 2/.'!

- ------- --
-----AID- Nr Juae-----
MASMIN31 SECONMjjr 101f (Cont #d
S/1%1/6,1008/004/oi
7/030
appears tit the colj(j~ior, -This 6urrentis fed 61the
verti(',,af!~`deflection ampli-
t
fier ofac:athode-.~;.iyoscillogr~K:Ph. Mie Oodulkion of the; pi,kimary
ion (or elec-
tron) current by Oki modulated rebtangular puls,.is makes
it'p~.Ossible to obtain
the zeroline automatically and to measur-6 secotdary curvents caused
by the
maximurri-energy (:E,I') + Ea' ) a'
nd minimum-ener'.[y (Eb -E,,,) lirimary particles.
The resuits of bovibardment. with electrons shoV that the dependence
of the.
secondary emission of negative particles on filni thickness, 'while
differing
quantitatiyely for J~ifferent bombarding-ion ener,~ies, are Uentical
qualitatively
and that the coeffic,. lents of the aecondary~iimiss;bn of negatiye
particles,due
to both ioa and electi-on bombardment undii.rgo
~i:talltativelyioimilar changes
with an iricrease i n, Vilm thickness. It is - iioncl' ~ed that tho
method de.~cribad
u
makes it Possible to obtain reliable. eValuations Tor a numb~Nxj of
basic secondary
emission icharacteri6tics. (DW
Card
2/21

'targets:
Is
V Nam "of L
and
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ON Prit.
Q'-
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Ao

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6,65
0.61

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-.':'A' S ON' .'AV
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of 00M 7
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-YV.72 7E0.77-T 5 17 70 ~,. ~TTu7-K-,"~~31V
IJ, ~~4`
-7 7~7.
aI

~ACCRSSION N.R: AP4022711
S/0020/64/19'5/002/0306/0308
AUTHOR: Arifoir, U. A. (Academicipai); Ayukhanov, A. Kh.;
Sustrov, V. A.;
Khas,mov, R. M.; Poltoratskiy, V. 1.
TITLE: Cathode sputtering of tungsten by potassium ions
$OURCE! AN i!' )SR, Doklady*, v. 155, no. 2, 1964, 306-308
TOPIC TAGS: cathode sputtering, tungsten sputtering, tungsten
surface purifica--
tion, tungsten, potassium ion, 74W 184 , potassium 0
ABSTRACT: The authors investigated the sg,ittering of tungsten
in a form of
chemical compounds and also sWdied the conditions for
obtaining a pure tungsten
surface. Radioactive tracers were used for determination of
the amount of
sputtered mate:ri.al. Polycrystalline tungsten targets with
induced activity,
(74W 184) were bo:-,abarded;wi:th potassium ions. The
stinsitivity of detection was
10-9 gm. The experimental details were given in auth(-,irls
paper M. AN UzSSR.
No. 2, 1963). It was found, by using retardkig or accelerating
potentials, that
Card 1/2:

ACCEESSION NR: AP4022711
the spattered particles were negativedons to *i. considerable
extent. This is
attributed to the adsorption of residual gases by tungstela
ato~ns. Heating the
target reduces the number of negative ion's.' At T>1600K, the
spattering is
temperature independent, which indicates that the tungsten
compounds'are pract-
ically absent, alid that the spattering Is 6.haracteristic of a
pure surface. Orig.
art. has.- 4 figuz-es.
ASSOCIATION: Fiziko-tekiu; icheakiy inatitut Akademii nauk UzSSR
(Physics-
Engineering Institute, AN/UzSSR)
SUBMI'.'C'TED: 21Sep63 DATE ACQ: 08Apr64 ENCL: 00
SUB CODE: PH 110 REF SOV: 003 OTH, ER- 002
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AILT;12V, U..'.; ALL'YEV, A.A.; AYUKHANOV, A.hh.
Ani-.tlir dependence of f,~.e energy spectra of
secondary Jona
I.
f
c. -oAng the bombardment of metals with positive ions.
Izv.
P,"' Uz,,SSR.Ser.fiz.-mat.nauk 8 no./+-.20-26 164.
(MJRA 18.03)
I
. FLUko-tekhricheskiLy institut AN lJz,.SR.

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L oqoq~_6r,'. E34T (1)/EWP(-m) ---.--AT
ACC NRi AJ?7002336
AUTHORI Arifovt_q~_A.; AI.iyoyj_A!
Ayukt~~A. 11.
SOURCE CODE: Ult/01,66/66/000/003/0041/0048
ORG: PhYsicotachnical Institute% Academy of Scioncas Uzbolk S3,R
(Fiziko-takhnichaskiv.
institut AN UZSSR)
TITIX: taigular dependence of the energy spectra of secondary Ions
at vario"u*s angles
of eihission
SOURM AN UZSSR. Izventiyao Serlyn fizitv-mat4maticheakikh naukq
no. 3, 1966f
41-48
TOPIC TAGSt ion bombardment, particle spectrum
ABSTRACT: Earlier airticles by the authors described the uttie by
them of an
,electrostatic analyrer to study the angular dependence of the
energy spectra of
.secondary tons during the'bombardment of metals by positive
10ns." Or. the basis
.of the resulting data the authors concluded that during the
bombardment of
'metals by ions in an energy range of 1-3 kev scattering is
explained by paired*
:collisiona - single and multiple. The earlier articles dencribed
the results of
the energy analysin of the secondary ions emitted at a certain
angle ( - 500) in-
.relation to an angle: of Incidence of 100-80P. As a result of the
design of the
Instrument it was possible, by changing the. target positioit
vi.s-li-vis the ana4
~Yzer,_tojitudy thn dependence of the energy spectra of tho
secondary tons on
1/2

L 09093-07
ACd NR, Al-7-002336
& 'an'gle of inciftice at variou's emission Iiingie values. The
present article
I
.1i'gives the results of these investigations, in particular,
oficillograms showing
-ithe energy dist~ributicn and the angular dependenct of the energy
6pectra at
Ivart6us angles of emlission'for secondary ioi:is whe!i a .Ho target
heated to 1800, K:
A-is.bombarded by positive potassium or ceslun tons with energy Eo -
1000 ev. The
-~authors discuss some of the results and-conclude that they can be
explained from
the viewpoint of valred coll_isions of the bDmbarding.lons with a
system of freal
atoms.,.-' Orig. art. hast 3 formulas and 4 figures-, �PRSi: 18.166]__
SUB CODEt 20 SUERDAIM non* ORIG REFg 010 OTH REII 001
C,,d 2 /2

L237 L11=6
AT
CC,, SOURCE'C
A
XR: AP6CO8549 ODE: UR/0166/66~000/001/0057/0061
AUTHOR: -Arifily H
A.; Rhadzhimukbamedoy h. 1(h.; AgkJAEgL
AWh
ORG: )Physics re,%bnical Institute, AN Uz ISR (Fitiko-telthnicheakiy
institut AN UzSSR)
TITLE: The coefficient of surface Ionizat
ion of fi ist seco, !My -~A~p.6
~L secon,
SOURCE: AN L'zSSR. luestlya. Soriya fiviko-mittematioheskAh nauk, no.
1, 1966,
57-01
TOPIC TAGS: fast particle, secondary eixtisslon, Ion bombardment, ion
emission,
surface ionization~
ABS71tACT: A.'te'r. a brief review'of the literatura', the authoro'note
that there is no
clarfly in the q6e,stion on the charge state of fasli;particles emitted
from a surface and on
the application )J'Ihe law of surface ionization to these particlev,
The present authors
togedier with S, V.' Starodubtsev showed earlier OWN SSSR, 124,, 1959,
60) that there
are slow (evapcrai;ed and diffutied) as well. as fast (scattered) ions
in the seeondarlylon
emisi5ion. Exp~riinental work on the charge statn of emitted Nat
particles had been
conducted withcut separating the secondary ions Lito the indi
vidual compqnents. There-
fore, The purposo Df the present work is the expe-rimental study- of
the charge state of
Card 1/2

L 23756-66
ACC X.R: AP6048549
surfa(io-emitted fast particles depending ori'the laaftation enorgir
and potential of
bombarding jon.,i. On the basis of the cxpei,~imentta data obtained in
the present work
and that of other authors (Flyants, N. N. , Arif ov, U. A. ,
AyWffisnov, A. Kh.
"Radioteklmika :i,~,Dlcktronika, " 1963, no. 81 34; Zandberg, E, Ya.
ZhTF, 25, 19515,
1386; Arifov, U.A., 10adzhimukhwnedov, Hh. IQ. "Izv. AN'S8511," scria
fizich., 24,
1960, 705) it is concluded that the scattler1rig in th~ form Of
J)DSil,ive ions depends not on
the charge state.of the primary particle, but on the ionization
potential of the bombarding
particle. This process, however, only quoitativoly agrees with the
mechanisms of
surfaco ionization. This should have beer), expectod, since socondary
scattered ions
have im entire energy spectrum, from thermal to limiting, dotei,*mtned
by single Rad
multiple elastic collisions of the bombarding particle with tho a'tDMS
of the metal.
A better agreement of the results with the ourface ionization
moohnnism may be
obtained, appar,nitly, only for the group of slow ions with enorgles
below 10 ev.
Orig. axt. has: 1 figure and 3 formulas.
SUB CODE: 20 SUBM DATE: 1OMar65. ORD REF: 0:115 OTHREF: 001
Card 2/2 U

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1.4
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00
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WOO-0 WME1

AUTHOR: S a, _h n Lc o v 133-158-3-5/29
ki
TITIE: Rer.,.,.rl,,s on tho Pap~~r of A.S AIRYUI'ZOV 'Ichal.~;e
Distr"butor of
a N.~w Deaif.~r_" (Otk'Iik n~-.SLuET77T_I_.3. `2,v '-.-.,r-~dc
lite 1
s
n'RICDICAL; Stail, 3, 20'~ (USSR)
AB$T-RACT-.
ASSOCIATION:
AVA11-ABIE.: Library of ConE,.,ress
Card I./l

AX11KOT, A,14~1,~7
J:q
.ti
f, 4 -et
tt- j
WV tip !1i
j:J
IPPIR
jK
MOM
tab
aiwWo
1A
ti,
pit 6-wrow
L 7
. .. . ....
ti
It

2AYTSEV, Y,'.T,; AM-KOV DDIMATOV, V,A.
Blest fiwnace trial operation with raw Ltavu
are. Stall 21
nool2tl059-1062 D 161. (14IRA 14:12)
lo Karagindinokiy metallurgichesIdy zaipod.
(Blast furnaces)
(Atasu region-Iron ores)

lim
I
AYUKOVV A.S.
Local hxaing of blast furnace tuyeze..Metallurg: 8 no.lslO-3.1
A 163. (KMA l6d)
1. Ka-raj:andinskly metallurgicheakiy zavod.
(Blast furnaces-Desigr and construction)
Cm

STARSHINOVP B,N.; OSTROUKHOV, M.Yao; KOCHI;TEVt
70*Yo; 11'ritd=31 unhastiyet
TARLSOV, D.A.1 SOROKAs F.F,; KARACWTSEV, M.D.;
OSIKIN, V.T.;
KOUEVP V.K.; POPOV, Yu.A.; DOtHATOV, V#A.j ATIMOV,
A.S.
Blowirq-in of large blast furnams., Sbor.trud. UNTIM
no.11t;17-32 165, (MIRA 18111)

STARSHINOV, B.N.; SINITSKIv, V.D.; S)EN'KO' G.Ye.;
GULYGA, D.V.; BABIY, A.A.;
KHOMJZHIYp A.G.; Prinimali uchasti.ye: OSTROUYJIOV,
M.Ya.; SAVELOV,
N.I.; PLISKANOVSE~Hp S.T.; IIOISEYIV, Yu.G.; WIRENTIYEV,
M.L.;
TARAISIOV, F.P.; ZAGREBA, A.V..; KAMENEV, R.D.;
TKACHENKO, A.A.;
FRETDIN, L.M.; WKIN, P.G.; POPOV, Yu.A.; MISHIN, P.P.;
I(ARACRENTSEV,
M.D..; DOU4ATOV, V.A.; V.P.; VYAZOVSKIY, YU.V.;
SOJJ)DKIY, Yu.A.; KONAREVA, N.V.; SAPRONOV, Yu.V.;
SINITSKAYA, S.K.;
SAPRONOV, B.V.; LEKAREV, V.L.; STCLYAR, V.V.;
FROhTORENK01 7.A.;
BANDMA, Ye.ye.
Resul'ts of the first year of operation of large capacity
blast
furimces. Sbor. trud. UNIIM no.11:34-46 165.
(MIRA 18: 11)

ATUNTS. Zh.A.
km"Ow mmek
Signifia.ance of Aaorpha fruticova L, in the Silvia
greenbelt (in
Armerivi with sumom7 in Rusul.&Al. Isy.AIT AmAM.3191ol
sellkhos.
nauki 8 no.5:87-88 My '55. (NLVA 9:8)
(Irivan-Axorpl^)

AYUPOV, Arif; AVAZOV, liak.=atulla; KODIROUl R.J.
red.
vowft"i & .,- ~
(Large crops in (-.Iry farming') Lalpi-Aorlikda
nul khosil;
Sirdare oblasti, Zhizzakh lohlab chikarlsh
boslikar-inasi-
dafi IlUdamik" sovkhozi gaLlakorlarinin?
tw3hr:Lbalaridwi.
To r.likent, Uzdavrmshr, P-16.14. 2 7 j),. (MIRA
-17:2.21)

AYUPOV, A.A., l,nzh. distaritaii (atanteiya Chalkqr)
.'~Wmaipzlant has become obsolete, i
0, Put' I put. kboz. no. 8:44
~~OIR I Ag 158. (MIRA 11:8)
(Railroade-Squipatant and tiuppliae) I
f

AYUPOV, ?,.M., kapiItan
Ife are reducing the time needed to train firot- and
second-class
operators. Vest.protivovozd.ob;)r. no.2:54-57 F '61.
(KIRA 14t2)
(Radarp Milltary)

ATUPOV, Kb.
Rolco of the budget in the developmont of the
economy and
culture of the Tatar A.S.S.R., lin..SSSR 21
no-7:15-18
Jl '60. (MIBA 13--7)
1. Hinistr finanBov 2ktarskoy ASSR~
(Matar A. S. S. R. --Budge t. 11
(Tatar A.S.S.R.-Mconoml.c conditions.)

MUM, Kh,14,
Results achieved by the Swuwkand station for visual
optical
oboorvation of articicial satellit?s. Trudy Uzflu
no.117:
99-;-132 862. (MIRA 16:7)
(Samarkand-.Artificial satellites-Optical.
observations)

AY[TOV, Kh. and MEMASOV, A.
"The Tecbni.que of the Veterinax7 ProcestAng of Animals) 11 Ufa,
Bashgoslzdat.,
1951. 72 pages. In Bashkir language. A bool:let for veterinary
assistants.
Veterinariya, Julr 1952. Translation #155, L., Lulich

AYUFOVj Kh.
"Holminthiagis of INrlinanto wid the
Control I:ur.,.mrvo"
Ufa, *~asld:ir House, 1953

w-.er, Of n ! hi, Al
Pm'-.1-11'Llilt~3 Of CIO Of U10 lt-~: C---nd V-A
3c!, All-U,Aon In!it. of I Oo-ji~ iol v :o
31L-a. Allo. 704' 2 I'lov -)5 31u-v(,~y ol 3cl.I.-~jt3
7'.j
lJOM' A

USSR/Diseases of Farm Animals - Diseases (.auBed By
Hej_-gLjnths,, R.
Ab B Jour Ref Zhur - Biol.
I , No 6o 1910., 263ig
Author Ayupov; Rh N.
Inst Kazan' Scientific Research Institute.
Title Therapeitic Value of' Hemaclilorethane (EChE)
in Sheep
Fascioliasis (Raport of tbck Author).
Orig Pul~ : Byul. nauchno-techn. inform. Kazansk.
n.-i. in-ta,
1957, NO 1) 30-31
Abstract : It was shown that the mosi stable
suapension of HChE
is obtained when one part of HChE is mixed with two
parts of fat (sunflowarsmd oil or cod-liver oil)
and with two parts of a me-porcent solution of sodium
oleate or a five-nercent ijolution of corn
sourdouGft.
Experiments with ZR34 shoe,,) irhich vea,e vick with
fascioli-
asio.. have shown that a wispenslon or iiaz in
loosa(;es
Card 1/2

USSR/Diseanes of Farm Anirmls - Disciases ,'aused
by Helminths. R .
Abs Jour : Ref Zhur - Dioll, No 6, 1958, 26330
Author , Ayupov, fal. V.
Inst, -
Title : Apparatus for 'Idministerinj, Liquid
Anthelmintics to
Sheep and Goats.
Drig Pub : Voterinariya, 1957, vo 6, 36-37
Abstract : No abstract.
Card 1/1

AYUPOV,--Xh.Vt,, kand. veter. nauk; IVANOVS-KIY,
S.A.,, kan(I. veter. naak;
SATI.TULLINI G-K.j VALIULLIN, S.M., vaterinarnrr
vrach;
UPOPNIKOV, M.V., veterinarryy vrach; FROLOV,
:Bootokhnik
Veterinax7 heiminthologica.3. evaluation of the
year-round
pen system of keeping sheep. Veterinari-ia 40
no.6:49-52
Je 163. (MIRA 17:1)
1. Bashkirskav-& nauchn roizvodetvennaya,
vetA)rinarnaya
0-5
laboratoriya. for Frolov . 2. Direktor Miyakinskogo
sovkhoza
Ba3hkirskoy AFSR (for SafivIlin),

kKCHURIN, B.S., kand. vet. nauk, oty, red.1 AYUPOV,
Kh.V., zaln.
ot v. red. ; ALAROV, D. A. , - kand. I
16-177=r,-ii~d. ;
BOLDYREV, V.M., nau8hn. sotr., red.; SATTAROV, A.S.,
nauchn. sotr., red.; BUTIKOVA, S.N., nauclon. notr.,
red
TRASUNOVA, Ye.T., tekhn. rod.
(Paptra of the Bashkir ScientifIci Research
Imititute of Agri-
culture] Uchenye zapiski Bnahkirckogo
nauchnc-.issledovatell-
sUogo instituta sellskogo khoziali.stva. Ufa, 1963.
312 p.
,MIRA 16:10)
1. Bksbkirskiy nauchno-iseledovai;ellskiy institut
sellskogo
khoz;raystva. 2. Zaveduyushchiy oWelom
infektaionnykh bo-
le,zn,gy Bashkirskogo nauchno-isslodovatel'skopp
inatituta sell-
skog) khozyaystva (for Sattarov)_
(Bashkiria-Veterinary medicine)

X.flipov I Kharrit Vallyevichj D911DOV, Ni~olny
ViilaJA t~ru-;J :1,;
dotB.
IL-.-.ver holmintbinees cf fnrm arilpials]
Yochonochnyo gell-
mintozy sell okokhoziaistvennykh zhivotriykii. Ufa,
Bagh-
ki:-okoe )cnizhnoe Izd-vo, 1963. 49 P. (MIAA 18:7)
1. Bashkirskiy jobvdarstvennyy urivernitat (fc,r
Bayancv).

Arirov, M.A.
wa~wawwwwmw ,,,
lxpeAeace adjusting the automatic protective device
of a high
presslure PV-150 economizer; exchango of experience.
lxerg.biU.
no.4,1-4 AP 157. (Bollers) (RIBA 10:3)

'AYM
YL Kirsa ____
(Trade unions of Uzbekistan in th~ straWle to build
comunism)
Profsoiuzy Usbekietems v bo:r'be n3 postroenie
konn=izma.
Tatihkent, Gosisdat UsSSR, 11*?59. *117 P. (NM 14:3)
(Uzbekistan--Trade uniol2s)

GOLOVINOV, M,Y.; A)ROY'l_~.qj_ KAGAN, L.S.; LESWEVIC11p
G.G.; KURBATOV, V.I.;
KAL11GIN, A.A.
Exta-usion of pipe of varying cross sections. TSvet.
met. 36
no.E472-75 A 163. (MIRA 160)
~Rxtrusion (Metals)) (Pipep Aluminum)

4i
if
0, A WV(k
AWA 4 1 1 i
41
IF
';'EWPb WD/
1 0
lit
pov- R
777---7;
obim :JDf db,~,Al- rest$;O
0
te
veek -1", --
Ida' 0 edovik Anat tvit ~Ocvi* AWTrw
rib oo,~bm. 0b
ayov Orill
pip
'61
Wu *a
07
f Yi 116
pr
.3, 1
fit" th nd 'wt
t ~drl
P100,-', tb:l
L, v Vat I)
N Mi
_epee eq
811C m
so
tecb~h~~u-ej the Indost sh(ilm so kllrdpvibq.~ tor: the lm,v"BaLk
Lnte M, 1"ficit 0 is 4qajmR` -Mb gi Pin -of ~VAVIIS
of td,,03. lath ma thid k1j" (104,
Ye
orbdB nectiorm :whieh ub int[,K4,PAI ~ Ph* 66*tfl~ ~ im, Ue
'thlokitbd.ll
pultfs t1w tij - has' 'a spoiloW shap* b, dati 1;~gned ~Prevsiaeof
thi6kened
:0. ager: or.;
'*sonAesigned-for the'-pipm: with -axtmrnal- t4okening's aW'th6:n&ifij
t
-.n Ton-the
a
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-do a
na p 'B~L=~#4owu~
rkis
20 M4104,
Sly
ik~q A V;:(t 520G,
-P res
Vag
OMP81 10 .6gou t told's on 0
Ai
6d~ t~, n figuz
;Icon
A83W
4,jr
ifia.: 'bW: W'.-b t mili
Sao&
GOIX
2J
i~x
Y;I, .1
Ir

.0 i
i,zm 0~~ijo4t-u w-r J,~ 4."o-a-
401dejr;:, 7-. jodlag bush
-

UTW7
.,~

M700

Y2
Drying cf
tilt, Y
OLY,tv
I
It

NOVOPLYANSKAYA, R.; BRIK, A.0t, metodist- JIXUPOVA K.V.,,
prepodavatell;
p
SOXOLOV.j B.M., uchitel" geog-rafii-, SYEii~,-'V.G,,, uchitell
geogrE,fiij-HAGOMED, M., khalimanov, uchitell geografti;
AZIMON', D.B.
Editor's mail. Geog. v shkole 26 no.6:51-M N.-D. 163,
04IRA 17: 1)
1. Melitopollakiy pedagogicbeskiy institut (for Novoplyanakaya).
2. Lipetakiy institut. uso4efohenatmovaniya itchJ.teley (for
Brik).
3. PeeiagojjiohQrBkoya g, Kansk, Krasipyarskiy kray (for
irjtdn~,a shkola Novosibiriika (for Sokolov).
Ayupoi,a). - 4. 29-ya 1
5. Lyublinsk ""'fa'-inte;m'at Nc).2 Kharikovsl:oy oblasti (for
"Y 0' 1
Sychev). -6e Ul;mkaya shkola Gunibskogo rayona Dagestanskoy
ASSR (for khalimianov). 7. Plikrokiiktiya odin~adt'Mtiletnyaya
shkola
Akhtyriskolgo rayona Dagostanskoy 9SR (for Azirnav).

AYUPOVA,-&),,. I DUBIVKO, S.A.
Morl hology of the pulp of milk tocilh at the qtaf~c of
root
reocrption and duvb4,, anomalies in secondary dentition.
hlauch. trudy Kaz. gos. red. inst. 114-351-352 16.1j.
(MMN ls:9)
1. XaPedru ort.oFedichevlroy stomatologil (zav. - prof.
I.",I.Oksman)
Razaru,kogo meditoinskogo 1notituta.

ZMJKOVY V.D.; YAKOVIEV, V.I.; TOTAPOVA, V.I-;
AXU_PP.YA,J_9.._Q*;
RUDLYA11DER, I.N., rukovo,11tel' raboty
Tochnology of production wid the properties or
semifinished
prodacts from the highly resista-it B92 alloy.
Alium, spla
nc).3192-104 164. (MIRA 17:

AYURZAN.T.
-, "I 1~ ~.
Economin role of the Mongolian cimel. Trudy Mong.
kom. nq.66;
72-84 154. (KI2A 8:6)
(Kongolia--cameltt)

571
40261
S/200/62/uoo/006/001/003
D214/D307
AUTHORS: Vlasciv, A.Ya., and ~Y_U~_Z~~Jrn, B.A.
T I TU; Th..- dependence of magnetootriction and the coefficient
of linear expansion of Blin*;rar alloy on temp6,ature
PERIODICAL: Akademiya nauk 63SR. Izvestl.ya. Sibirskoye
otdcleniye'
no. 6, 1962t 99 - 102
TEXT: The aim of this -,-iork is -uo explain the volumetric and
elas-
tic properties of Blinvar alloys in termli of ferro-magnetism.
The
relationship between magnetrostriction (-Q and temperature was
cttu-
died. All',work was done on annealed spec.l.mens of.one Elihvar
alloy
(37 /, Ni, 7.56 1% Cr, 54-44 Of, Pe) in the 1;emperature range
from -196
to 3500C. Magne-tostriction curves constricted for various
tempera-,
tures showed that in strong magnetic: felds (11) the relationship
~ if u
between A and the field strength in liij,-,.!ar and the gradient
increa-
ses at temperatures approaching the CurJl.~! point. This
gradient de--
creases,and the curves deviate from line;:irity when the Curie
tcrrpe-~
r&ture in exceeded. Extrapolation of' theoe straight portions to
H'= 0 show that A, of technical salturut:!.on, is linearly
related to
Card 1/2

S/200/62/000/006/001/003
The dependence of magnetrostriction ... D214/D307
the temperature up to the Curie range, at various field strength3.
The coefficient of linear expansion (a) -;ias constant between
-196
ana 100001. Above this temperature a rapi:lly increased linearly
with
temperature. A theoretical equation relnl;ing o, to A,hps been
worked
out and lax-oerim~.,-ntal results closely agr'?e with the
theoretical,
This confirms tAtit the anom4lies of the i',hermal expansion of
R1in7
var are connectod with the ferromagnetisi!12 of the alloy. There
a;,c
4 figures.
ASSOCIATION: In.3titut fiziki sibirskogo otdeleniya AN SSISX,
Kr~.c-w
ya::,sl: (Institu,te Of ?hN-BiCS, Siberian Branch of thQ
AS USSR, Krasnoyarsk)
SUBMITTED: Jtuie 24, 1961
Card 2/2

114
'114175
S/04,3/6 2/026/002/024/03 2
Bi 17,'BI 38
AUTHORS; Vlasov, A, Ya , Lapt~-v, D A , Ayurzanajn, B. A ar~
Smelin, R P
TITLE- Temperature dependence of tho magnetic properties of
PERIODTCAL: Alcademiya nauk SSSR- Izvesti..Ya. Se.--,.ya
f_Jz,_chPskaya4 v. 21,
no. 2, !Q,62.~ 287-290
TEXT: This pap4~r was presented at a 'Ionfe.:,ence on
magnet3.:57,,. and an"-.tferr:,-
m3j.-netlism.. The aut!'.ors s-uli~-I :he depend,?nce of
ciagret,.--
- T, r, r The sturIl es A orr.,
tion, miarnt~tic hysterc,~is, and fcrcfi
,;%irried out on '.wo test arrangements at th:! sam,~- time.
Magre t JA' -,It :1 orl P!",'
:oer~.,i~re force vere measured continuo,.isly with a
vertital astatic
maEnet::,meter (Ref, 7, Drok0i, A !,., Illylishenko, V A I
ZY- eksperim
teorc fiz', 2 no 6, 339 '19.55)). MaCne,,ostriction was
meaq,.:re~i ty
trans.m..tting strain gauges in th.- temperature range from
-19~O to '310"C;
and in magneti.., fields of up to 5800 oe. flaenetic
hysteresis was stud*,
.in the. A-cycle (20-300-200C and 20-400-20c'(,) in externa!
mae-net--c
(0 - 30 oe) , kinealed (vacuum 0-4 mm Hg, '1000C. 2 hr') and
,-anann~,a!,:,d
Card 1/2

3).X 5
S/048/6,1/02 6/002/024/0 3 2
Temperature dodenden~e of the. BI i7/'BI!18
specimens of the following compositton, were used: '117 $, Ni
, 7, r)7 % Cr..
11
0 ~ 5 2 % Idn, 0, 2 1) ~ S i, C. , 0 5 ~'~ C, 0 0P, remainder;
Fe, Vo I)
magnetostr-,oti(in .'n Fure fcI'm was Observed in lr~olds
alove 900 c.e TI 6;
temperature dnpentien,;e of 3hows t~o "saddl.?" ~haractririeT-,
of znva.r ali,~:i,w.,,Vi F- peak at 11)1~'~C Dae to.
,nufnk!o,!f~-k'T10n,
at tech,-,ilcal ~i,tjzratjr)n X this doronden~-.t 1,i
norliiiear Parupz% . ~ ; s
magneto5tricllcr, X p IS stable and tot deperdent oti tie
pre--rious treatm~-.1
of tha 5peimer. llnjike mot3t f--~rromagretic:.,; there are a
number ~i
i~n the Temperature d-,pendenoe of magne;ization anJ ccEjr i
vi,
C-~-ri~~ pe,4nt ,in unannea~ed spt,-,-Imens no I'ELnoma'Ie--,"
ol,served- Thq sand bolds for the Temporat,.;i,7e dependonce
of niagnetl~:
wh-,,~!-i I's in annouled s.?e-Impris. T,~;~ va--? ~,i
qagne,.:~ hystere.~:..-: I.z, highe..it ,n unannealeA
spPcinigns, and the
der-endence of ,L),?rcive furce harj a m;Hmum :it 11,01C~ T h
e an,- al a IS ob ~ e
in the ,-Durse ~f AT) and H T.) cui bE, at*ri.buted zk
tho fa-,t tha-, Eliriva---
has gro,~tps of ;-,iajyriet,-c phase,-~ w:,th J-.Iferen~,
C~;-ip pc-y':4~ Tt%e-,e a~-i
fig..ArEs anl Soviet referenc-es
ASSOCIA71011~ T-istitut ,Piz-,k,, Sibi-skog,~ Akademii ra.A
SSSF
.-,f Friyo-.. of S~bc.r, .-j
USSR)
Card 212

, ATLUtZANAYN, II.A.
Law cT approach to magnetostrl~ctioi saturation Of
elinvar alloys
and the determination of magnotostAction caiatants.
Izv. AN SSSR.
Ser. fiz. 28 no.1:202-205 Ja lt.'~4.
Magnetization and niagnetostriction saturation in
elinvar alloys
subjected to plastic deformation. Ibid.:;:?O&.210 (MIRA
17:1)
1. Institut fiziki Sibirakogo otdo',eniya AN SSSR.

VLASDV, A.U. ; AYURZANAN, B.A.
Tomyernture relatlaiship of mpetostrictim and the
coef-
ficlcm~*, of linear empansion OL' olly.var. Isv.
Sib. otd. AN
SSSF.no.6v?9-102 IQ (MIRA 17t7)
1. Insi-Atut fizlki Sibirskogo Weleniyu AN SSSR,
Krasno7arsk.

ACC N
R' AP7005130
SOURCE CODE: UR/0126A6/022/004/0551/0555
AUTHOR: Xbromov, D. P.; Ayurzanayn, B. A.
ORG: Kra snoyars% Polytechnic Institute (Krasnoyar.-i-Riy
politeldmicheskiy institut)
TITLE: Susceptibitity of the para-process in elinvar alloys
SOURCE: Fizika molallov I metallovedeniye, v. 22, no. 4, 1966,
551-555
TOPIC TAGM magnetization, elinvar alloy, iron nickel alloy,
chromium, magne-tic
susceptibility, magnetic anisotropy
ABSTRAMN Elinvzar alloys display a number of anomalies:
considerable magnctostriction of
the para-process; a relatively low coefficient ofthermal
expansion, and a complex tempera-
ture dependence of these properties. The nature of these
anomalies is associated with ferro-
magnetism, and hence their elucidation should be furthered by
investigating the magnetic pro-
perties of -these alloys. In this connection, polycrysta! 'line
cylindrica specimens of Ni-Cr-Fo
elinvar allDYS (32% Ni, 6-12% Cr, with Fe as the reir Etinder)
were subjected to measurements
of differential susceptibility In various magnetic fieldii. of
up to 3000 oe with the aid ofa pro.-
viously described expnirnental setup (Khromovo B. P, Izv.
vuzov, Fizika, 1960, no. 1, 171).
Card 1/2; UDC: 538.214:538.221

ACC NR% AP70051.2.0
P indings: for these elhivar alloys magnetization in fie Ids Of
MOro thmn 300 00 occurs owing tt)
the para-process. Tho depondenco of para-process su
sceptibility on field intensity Is in good
agreement with the theoretical conclusions Of HDlstein and
Primakoff (Phys. Rev., 1940, 58,
1098). In laboratory fields -- several thousand oersteds -- the
para-process susceptibility of
elinvar alloys exceeds 'hy one or two orders of magnit, ido the
suscele3bility of nickel and iron.
The dependonce of 1xii-a-process susceptibility on floU
intensity is stronger for the alloys with
the higher contents of Cr. It is to ba expected that the
magnetic anisotropy constant of elinvar
Ooys should be much !owe-.r than for nickel anti iron. For the
eUnv&r alloy containing 12% Cr
room temperature, liositive susceptibility can be expected to
diminish to zero and, in fields
Df several tens of thousands of oersteds, acquire nega:Ave
values; it; would be interesting to ex-'
perimenta:ay verify ithia assumption, for which no theoretical
explanation is yet available.
Orig. art.. has: 3 figures, 1 table, 1 formula.
SUB CODE: ti.1 20/ SUBM DATE: 27De&65/ ORIG REP: 005/ OTH REF:
006