SCIENTIFIC ABSTRACT BORSYAK, P. G. - BOSANCIC, M.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000206610009-7
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 9, 2000
• Sequence Number: 9
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

8/181,/60/002/01/09/035
AUTHORS: Bors3rak. P. G.v Fedorovich, R. D.
MENOW
TITLE: Intrinsic Optic Absorption in Amorphous and Crystalline
Germanium
PERIODICAL: JPixika tver&ogo tela, 1960, Vol. 2, No. 1, pp. 45 - 47
TEXT: For cosparisonp the authors studied the amorphous and the
crys-
talline germanium within the rang* of strong absorption. The
absorption
coefficients were determined on the strength of measurement results
of
the passage of light through and its reflection from thin foils on
quartz base. A certain shrinkage was always found to occur with the
crystallization of amorphous foils. This reduction in thickness by
5-9% in indicative of a transition to a denser packing of the atoms.
The optical proportion of the foils were measured in the airg as
soon
as possible after their removal from vacuuma The authors detected
some
ualitative characteristics of the optical properties of amorphous
Zoolid lines) and crystalline (broken lines) germanium (Fig. 1). The
reduced absorption coefficients k(X) for calculated values of the
Card 1/2

Intrinsic Optic Absorption in Amorphous and S/181160/002/01/09/035
CrytbMine Germanium B008/Boll
spectral characteristics are shown in Fig. 2. It may be stated that
amorphous and crystalline germanium resemble each other as to their
optical properties. They have the same range of intrinsic absorptiong
whose general course and Intensity do not exhibit any great
differences,
although there are son* distinctly marked qualitative differences.
These
are caused by differences in the long-rang* order. The authors thank
L. Apkerp R. R. Philippq and E. A. Taft for communicating their in-
vestigation results in advance of publication. There are 2 figures
and
7 non-Soviet references.
ASSOCIATION: Institut fisiki AN JJSSR Kiyev (Institute of Physics
of the AS UkrSSRa Kiyevs
SUMITTED. May 49 1959
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?1 3 'Z_ 0
81777
5/181/60/0'0~/02/21/033
B006/BO67
AUTHORS: - Borzys'k, P. G.j, Marchuk, P. M., Sarbey, 0. G.
TITLE: Current-voltage Characteristics of the Photoelectron
Emission of Germanium
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 2, pp. 306-313
TEM The authors report on investigations of the current-voltage
characteristics of photoelectron emission of germanium layers
with a low
work function. P. I. Lukirskiy (Ref. 1) has already shown that
these
characteristics can be obtained in the field of a spherical
condenser
when the diameter of the emitter is small compared with the
diameter-of
the collector. For the investigations germanium was vaporized on
a metal
disk in vacuum. With strongly reduced work function of the
electrons
from the germanium surface, the contact potential difference
between the
front, the emitting, and the back layers of the disk forms a
barrier
field for the photoelectrons, as is shown by model experiments in
the
electrolytical tank of Fig. 1. For investigating the
current-voltage
characteristics of germanium of three-electrode device was used
whose
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817717
Current-voltage Characteristics of the S/181160/002/02/21/033
Photoelectron Emission of Germanium Boo6/Bc)67
schematical drawing is shown in Fig. 2. Its construction is
described
in detail. The results which are shown in diagrams are discussed
after
a detailed description of the experiments. Fig, 3 shows the
oharacteria-
ties which were recorded at an irradiation wavelength of 240,
254, 280,
313, 365, 435, and 546 mu. A quartz monochromator with a "K-4
(PRK-4)
lamp served as light source. The energy distribution of the
emitted
electrons is discussed in the following. Fig. 4 shows dI/dV -
f(V) for
the first six X-values. The first of these curves (largest hr)
shows
linear course, the following linear rise, a peak,and steep
decline.
With increasing 7L the curves become more symmetrical, the curve
for
435 m,),&,Shows a steep exponential rise, a peak with a
horizontal peak
line and a decline corresponding to the rise. The
characteristics shown
in Fig. 3 are then referred to the lines X a 313 mpand the lines
on the
left side are, according to Einstein's lawn referred to the
quantities
(hr - hw)le and those on the right side to (Rv--hv )/e.
The.results
313 313
are shown in Fig- 5 and discussed in the following. There are 5
figures
and 8 referencest 7 Soviet and 1 American.
ff

O-L777 - - - --- -- --- - -
Current-voltage Characteristics of the S/18Y60/002/02/21/033
rhotoelectron Emission of Germanium BOo6 B067
ASSOCIATION: Institut fiziki AN USSR Kiyev (Institute of
Physics of the
AS UkrSSR Kiyev)
SUBMITTED: April 20, 1959
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81778
B/181/60/002/02/22/033
X3/ B006/BO67
AUTHORSt Borzyakp P. G.9 Miroshnichenko, L. S., Sarbey, 0. G.
oyl ),I Y1
TITLE: Photoelectronic Emission of Germanium and Silicon in the
Amorphous and Crystalline Siates
PERIODICALt Fizika tverdogo tela, 1960, Vol. 2, No. 2, Pp.
314-318
TEXT: The germanium and silicon samples examined by the authors
were
produced by vaporizing films onto metallic backings. The
germanium films
were sputtered onto tungsten backings, cold as well as at T =
4500C.
Electron diffraction studies showed that the films sputtered at
room
temperature were amorphous, and crystalline at increased
temperature.
An investigation of the contact potential differences between the
amorphous and crystalline films produced under otherwise equal
conditions
showed that the thermoelectronic work function of the latter was
some
ton electronvolts smaller than that of the former. Fig. I shows
the change
of the work function 64(t) with time of simultaneously sputtered
BaO for
crystalline (Curve 1) and amorphous (Curve 2) films. The values
of the
primary photoelectronic work function of crystalline germanium
films are
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81,778
Photoelectronic Emission of Germanium and Sili-
B/181/6()/002/02/22/033
con in the Amorphous and Crystalline States BOo6/Bo67
lower than those of amorphous ones. Experiments were also
made with
monocrystalline p- and n-type germanium samples. The
preparation of
these samples is described; the pure surfaces of the
single-crystal
samples were obtained in such an evacuated tube as shown in
Fig. 2.
Fig- 3 shows the spectral characteristics of the
photoelectronic emis-
sion of three crystalline germanium samples with reduced
work function.
Curve 1 refers to high-resistance single-crystal germanium,
Jurve 2 to
n-type Go single crystals with 3 ohm.cm, and-Curve 3 to a
crystalline
film, Fig. 4 gives a comparison of the spectral
characteristics of
amorphous and crystalline germanium. Similar investigations
were also
made with silicon. The amorphous films were obtained by
sputtering onto
* backing at room temperature, the crystalline ones were
obtained from
* p-type single crystal in high vacuum. The spectral
characteristics of
these samples are also shown in Fig- 4- For comparison, this
diagram also
shows the characteristics of the spectral sensitivity of W -
BsO
photocathodes and two Cs 3Sb samples. In contrast to
amorphous germanium,
crystalline germanium shows a weak minimum in the short-wave
region, which
corresponds to the maximum of the spectral characteristic of
the optical
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81718
Photoelectronic Emission of Germanium and Sili- 5/181/60/002/02/22/033
con in the Amorphous and Crystalline States B006/BO67
reflection of crystalline germenium. Amorphous samples do not even have
this maximum. Since optical absorption In silicon is weaker than in
germaniumv the photoelectronic sensitivity of silicon is also lower.
Such a parallel cannot be observed in a comparison of germanium and
Cs-Sb. In conclusiont the authors,thank Professor D. N. Nasledov for
the
pr2paration of the Si single crystals, Ye. G. Miselyuk and A. N.
Kvasnitskaya for the supply of the germanium sing e crystafe, and R. M.
Mykina fo the conduction of the electron diffraction studies "here
are 4 figures and 4 referencess 3 Soviet and 1 American. r
ASSOCIATION: Institut fiziki AN USSR Kiyev (Institute of Physics of the
------ AS UkrSSR KiZev)
SUBMITTEDi April 20, 1959
rlard 3/3

87906
43 00 S/181/60/002/012/006/018
b Z q-"~- B006/BO63
AUTHORS: Borzy and Fedorovich, R. D.
TITLE: Optical Properties and Photoelectron Emission of Amorphous
and Crystalline Germanium Films
PERIODICAL; Fizika tverdogo tela, 1960, Vol. 2, No. 12, pp.
3020-3025
TEXT: The optical properties of germanium films within the range of
intrinsic absorption have been studied many times. The types of
filmsp
however, were not named. Following a previous paper (Ref. 2) in
which
the spectral characteristics of transmissivity, reflection, and
absorp-
tion, of amorphous and crystalline germanium films were studied,
the
authors have now analyzed the results obtained and determined the
influence
of the type of film upon these characteristics. The experiments
were
repeated with an improved method, and more exact results were
obtained
since various corrections (eg., for the spectral dependence of the
refractive index) were taken into account. The device used for the
purpose is illustrated in Fig. 1 and described in detail. The
authors
studied the spectral characteristics of the reflection and
transmission
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879o6
Optical Properties and Photoelectron Emission
S/181/60/002/012/006/018
of Amorphous and Crystalline Germanium Films B006/BO63
coefficients, and determined the influence of the atmosphere (air,
vacuum).
The spectral characteristics of absorption coefficient k(A),
refractive
m De
index n(A), and reflection coefficient R(A) a be represented by I
(I-R)(i-R')exP(-4 nkd/A) and n - 1+R + 14-R 2 - (1-k) 2. Fig- 4 shows
0 1-R - (1-R)2
k(A) and n(A) for amorphous (continuous lines) and crystalline
germanium
(broken lines) which were applied in vacuo. The dotted lines
obtained by
Philipp and Taft (Ref. 5) show k(A) and n(A) for single crystals of
germanium, without taking account of the oxide film on the surface.
The
effect of optical peculiarities of the films Upon the
characteristics of
photoelectron emission was studied with the same device. There are 6
figures and 6 references: 4 Soviet and 2 US.
ASSOCIATION: Institut fiziki AN USSR Kiyev (Institute of Physics of
the
AS UkrSSR, Kiyev)
SUBMITTED: April 18, 1960
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-- - - - - -------- -- -----
S/181/60/002/012/006/016
B0061f3063
Legend to Fig. 1: 1) Holders; 2) Germanium)vaporizer; 3) Hot cathode;
14~ Heaterl fl Windowei 6) BaO vaporizer; 7 Photoelectron collector;
8 Getter; 0 Ionization pressuie gauge;.10) Car--iage. The germanium
coming from the vaporizer is precipitated on the hot i~art of the base
as a crystalline filmi.and.on the cold part as an amorphous one.

86807
~11994& (320/1 ( "S/185/6o/oo5/Ooi/bo6/oi8
A151/AO29
16' A6-42
AUTHORS: Boftyak, P.G.':; Marchuk, P.M.; Mityans'kiy, G.F.
TITLE: Photo-Electronic Emission of the Intermetallic"Compounds M92Sn
and
InAs
PERIODICAL: Ukrayinalkyy Fizyc,hnYY Zhurnal, 1960, Vol. 5, No. 1, PP.
65 74
TEXT., III Only the spectral characteristics,of the photo-effect of
the A'IBIV
and A B type compounds are studied which are characterized by small,
one-or-
der widths of the restricted, energy zone. The films M92 Sn were
obtained by means
of the dondensation of a tungsten strip cleaned in a vacuum. For
studying the
film of a changeable composition o -Mg - Sn, the distribution of the
thermo-elea-
tronio effect of the yield T tem ABSTRACTOR'S NOTE: Subscript temp
(temperatute)
stands for the original T (tempepatura)j along the strip 5 was
determined. The
results are given in Figure 3, where the curve 1 shows the
distribution offftemp
along the surface of the tungsten strip. Further, the film was applied
on the
strip, which again was cleaned in a vaeux;m. After that, the curve 2
was obtained.
A repetition of this cycle yielded a curve which coincided with the
curve 2. Af-
ter a third investigation of the film, a distribution was obtained for
it which

86807
S/1B5/6o/oo5/0o1/oo6/oi8
A151/AO29
Photo-Electronic Emission of.the Intermetallic Compounds Mg2 Sn
.and InAs
is illustrated by the curve 3. For various sections of the film
characterized
by the curve 3, thelauthorv have determined ?,1e spectral
pboto-electrio sensitivi -
ty Il toward ~2 of the C33 Sb-photocathode: The results are
shovnl. Ir
Figure 4. Each curve Is marked by a figure T*ing the coordinate
of the invest.-1&3~
ed section according to 'the data of Figure 3. The
photo-electronic properties of
Mg arb characterized by the curve 28, those c;f M92Sn by the
curves 10, 13 and 16.
It was established that the optimum value of the yield effect
in respect to the
photo-electronic emission is achieved for a-metal surface at
values t within th?
limits 4-20 and for the surface of Mg,,Sn at tt7o. it can also
be seen that in
the case of a photoelectronic yield erfect of only about 2 ev,
the values of the
quantum yield in M'923n remairi small, reaching only the tenth
part of a percent
even at the highest values of h9 = 5 ev. For studying the
photo-electronic emis-
sion of InAs, an Investigation was carried out of the surface
of the break of a
massive crystalline sample obtained in a high vacuum. The
results of photo-elea-
trio measurements conducted on a clean, newly-obtained surface
are shown by dots
on the curve 1 in Figure 7. In the *case of a
conseoutive'deposition of BaO mole-
cules on the surface of InAs, the yield effect is decreasing,
according to which-
the'characteristics 2,3 are obtained. The curve 4 corresponds
to a state.of the .

86807
S/185/6o/05/01/006/018
A151/AO29
Z~r-zo-Electronic Emission of.the Intermetallic Compo~xnds MSRSn and
InAs
with a concentration of barium o~cide molecules which is already higher
Zn the optimum concentration. For comparison Figure 7 depicts also the
curve
cbtlained for a Cs Sb-photocathode, which ata- 400 m,"had a qunntum
yield of
A comparDon of the ipectral Jos o~ the 3 intermetallic
,*aracterist
compounds Sn, InAs and Cs,Sb shows that the firattwo compounds differ
from
MIIr2 Z)
ev
the latter one by efficiency values and appe~arance. Even at a
distance of 3
from the border, they do not scow any~,tendency to saturation and have
lesser ef-
ficiencies than Cs3 Sb by one order or more. By making a-comparison of
the.values;;
f 'for. Mg2Sn, InAs, and Gs Sv (Ref - 7) including here the data for
Ge'. (Ref.0
the tendency toward a decrease o~ A 'If is'noted which,occurs when the
energy of
the electronic affinity is also decreasing. There is, however, no
direct propor-;
t--~onall relationship between the electronic affinity andnT, which
shows that there
are still other factors affecting the, value !'P There are 8 figures,
2 tables --nd-
8 references: 6 Sovieti, 1 English and,l Germ'an.
ASSOCL*iTION:'Instytut Fizyky AN URSR (Institute of Physics, AS
UkrSSR).
SUBMITTED: July..6, 1959
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96807

S/185/60/005/001/006/018

A151/AO29

Photo-Electronic.Dnission of
the Intermet~alic Compounds,blg2Sn and InAs

FiM!re 3:

TiM!re~ 4:

Plic. 3.

24919 3/18 1/6 !/003/006/016/031
B102/B201
AUTHORS: Borzyak, P. G-, Miroshnichenko, L. S~, and Fedorovich, R. D.
TITLE: Optical properties and photoolectron emission of Mg,~Sb2
I
PERIODICAL: Fizika tverdogo tela, v. 3, no. 6, 1961, 1778 - 1785
TEXT- Mg3 Sb 2' the intermetallic compound of type 11_~L -Vbstudied
the most
thoroughly heretofore, has been examined by the authors for its
photoelec-
tric and optical properties. The Mg3Sb 2 films used for the
investigation
were prepared in different ways from pure magnesium and pure
antimony% the
initial substances had been supplied from the Institut obshchey i
neorganicheskoy khimii AN USSR (Institute of General and Inorganic
Chemistry
AS UkrSSR) by V. P. Zosimovich. The photoelectric characteri s tics
of thefiIns
prepared in three different ways were the same. A method described
pre-
viously (FTT, II, p. 45 and P. 3020, 1960) was used to determine the
optical constants: the measurement of the reflection and transmission
coefficents of light under exposure from front and rear. The
monochromator
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24919
Optical properties and photoelectron...
SIIB1161100-100610161031
B102/B201
of an C~-4(SF-4) spectrophotometer was employed for
measuremenzs in the
254 - 578 m~L spectral range, while a YtI-2(UM-2)
monochromator was used for
the 450 - 1100 m/k range. An OCK-12 (ISK-12) spectrometer
was used wi~_.I
;WOOO m/k. Since absorption is dependent uponX ', variously
thick films
were used for different spectral ranges. Since, however. a
considerable
light scattering was already observable for d~ I , the
longwave limit for
the experiments was set at hV - 1.55 ev. For wavelengths
outside the region
of self-absorption, only the refractive index was
determined, namely, by an
interference method. Films up to 3,U-could be used for this
purpose. Beyond
the self-absorption region the refractive index was 1i -
4.7, and the dielec-
tric constant at high frequencies was k = M1. As may be seen
from dia-
grams (1-R) .,f(hv), light with hV> 3.3 ev is practically
absorbed fully
in jayers of 50 m~&. The light source in the measurements of
photoelectron
emission (with SF-4 and Kn-28(ISP-28)) was provided by a
mercury-quartz
lamp of the type nPK-4(PRK-4); the light energy at the input
of the mono-
chromator was determined by means of standard photocells.
The photocurrents
were measured by a d-c amplifier. The measured energy
characteristics (as
compared with those of Va 3Sb) are as follows:
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S11 8 1/6 !/'jjc)3//.DO6/;Ol 6/031
Optical properties and photoelectrgW~ B102/B201
Characteristic Na Sb Mg Sb
[e vj 3 3 2
~P-hoto 3.2 3.8
AE 1.1 0.8
Effin 2.1 3.0
a
1.1 1.8
El 1.0 1.2
affin
TP,hoto 2.1 2.0
The data for Na 3Sb are taken from V. P. Bibik, who works at the same
laboratory as the authors. Eaffin is the energy of the electron
affinity
of the initial surfaces, E , that of surfaces with a work funGtion re-
af f in
duced bydy,& is the forbidden-band width. A. F. Mallnev and M. P.
Yesellson are mentioned. There are 6 figures, I table, and 1)
referencest
10 Soviet-bloc and 3 non-Soviet-bloc. The references to
English-language
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24919 S/181/61/003/006/016/031
Optical properties and photoelectron... B102/B201
publications read as follows: T. S. Moss. Proc. Phys. Soc. ~11 982,
1950;
P. Gdrlich. Recent Advances in Photoeirtission. "Advances in
Electronics and
Electron Physics", Acad. Press, No. 4, 1959. W~ E. Spicer. Phys.
Rev. 112,
114, 1958-
ASSOCIATIObl: Institut fiziki AN USSR Kiyev (Institute of Physics AS
UkrSSR Kiyev)
SUBMITTED: October 28, 1960(initially) and January 9, 1961(after
revision)
Card 4/4

BORZXAKq P.G.; KATRICH, G.A.; SARBEYO O.G.
Electron emission from CdS during current flow. Fiz.tvar.tela
3 no.7:2186-2188, J3. 161. (Iff-RA 14:8)
1. lustitut fisiki AN USSR KI Ve
.0 T (Cadmium sulfide)
(Electrons-Wasion

)o
33371
S/181/62/004/001/049/052
B112/B138
AUTHORS: Bibik, V. F., and Borzyak, P. G.
TITLE- A new type of alternating photoconductivity in cadmium
selenide crystals
PERIODICAL: Fizika tverdogo tela, V. 4, no. 1, 1962, 296 - 297
TEXT: Alternating photoconductivity was observed on CdS crystals with
6
resistivity of 10 ohm-cm, which were provided with indium contacts and
placed in a high vacuum.- This photoconductivity was essentially
different
from that observed by Harnik and Weisz. The spectral characteristic,
illustrated by curve W/W = f(;L) clearly shows the change in sign of
photoconductivity, which occurs at 520 - 530 MIA. Harnik and Weisz
observed
such a change at ;L> 650 mp AI/W denotes the illumination-induced
increase
of current related to equal values of luminous energy. The course of
the
volt-ampere characteristics also reveals this alternation in
photoconducti-d-,
ty, which is always positive at weak fields, becoming negative at
fields of
the order of 102v/cm. Harnik and Weisz found negative
phot-oconducti-,rity at
weak and medium fields, with the change to positive at E> 104 v/cm.
The
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A new type of alternating ...
33371
S/181/62/004/001/049/052
B112/B138
authors succeeded in producing a crystal in which the change in
sign could
also be observed in dependence on the illuminated part of the
crystal.- One
part displayed this alternating photoconductivity, and the otheronly
positive iphotoconductivity, independent of A or voltage applied.
The lux-
ampere characteristic of the latter is norm alv that of the
negative photo-
conductivity shows a rapid incrpase-up'to -15-lo-7a, then it
remains constant
Its mechanism may be explained on the assumption of photoexcitation
of
minority carriers from local levels, which recombine with majority
carriers.
Applied to the change in photooonductivity, however, this model is
compli-
cated by the voltamperage charaDteristics, which indicate that
field not
only determines its level, but also the sign. There are 2 figures
and 5
non-Soviet references. The two referonces to English-language
publications
read as follows: E. Harnik, S. Z. Weisz. Proc, intern, confer. on
semicond.
phys., Prague, p. 1053, 1960; R. Frerichs. Phys. Rev. j2, 594, 1947.
ASSOCIATION% Institut fiziki AN USSR Kiyev (Institute o'~ Physics
AS UkrSSR
Kiyev)
SUBMITTED: August 14, 1961
Card 2/2

AUTHORSt
TITLEt
431o6
S/lai/62/004/011/001/049
B102/B104
Bibik, V. F., Borzyak, P. G., and Sarbe~, 0. G.
Emission of non-equilibrium electrons from cadmium sulfide
PERIODICAL: Fizika tverdogo tela, v. 4, no. 11, 1962, 3003 - 3009
TEXTs The characteristics of non-equilibrium electron emission ftmCdS
crystiib i.;
were investigated and the effect 9f illumination was measured. In a
previous work (FTT, 3, 2186, 1961) it had been shown that the electron
emission from CdS is affected by an electric field far stronger than
that:
due to the potential difference applied. An bhmic probe was used to
measure this field along the crystals before and after,the treatment
known
as "forming". In the previous work the treatment was given in vacuo'
whereas now- it was carried out in air. This was found to have a
substantia
effect on the potential distribution within the crystal (Fig. 1). The
strong field was observed also in the electrooptical effect. The
forming
leads to the formation of two zones within the crystal which are
separated
by a thin layer (0.02-0.06 mm) exhibiting a high potential drop. This
separating layer, can be made visible in transmitted light
(jL520q_VA)1. At
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S/161/62/004/011/001/049
Emission of non-equilibriuip, n. B102/BIO4
the point where the potential drops sharply, the electron emission
current
has a peak. Further, the forming either increases or decreases
resistivi-
ty; some crystals showed aikind of rectifying effect. In most
cases, the
emission increased considerably on being illuminated, whereas in
some
cases emission occurred already at potentials much lower than
those re_ V
quired for observing dark emission. Illumination with hw< 5 ev
produces
no electron emission if no potential is applied to the crystal or
if no
current is flowing through it. The conductivity of some crystals
was
found to be completely Independent of illumination. In order to
clarify
these effects, the spectral characteristics of photoconductivity
and light
emission were measured. The results differed between various
crystals.
For the crystal whose potential distribution is shown in Fig. 3,
the
energy of the electrons emitted was calculated from the emission
current
density to be -_ 1.4 ev. Thelfield strength within this crystal
appears
to have the order of 2-3-10v/cm, which is high enough for the
electrons
to collect sufficient energy:for emerging into the vacuum. On
illumina-
tion, photoconducting crystals increase the conduction electron
concentra-
tion and moreover intensify..the field in the emitting regione,
thus
causing or intensifying the,dark emission. Electron
photoexcitation in
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5/181/62/004/011/001/049
Emission of non-equilibrium ... B102/B104
the strong-field regions is negligible. There are 6 figures. The most
important English-language references area J. Z. Moll et al. Phys. Rev.
Lett. 7, 87, 1961; R. E* Simon, W. E. Spicer, Phys. Rev., 119, 621,
196al
J. Appl. Phys. 31, 1505, 1960.
Institut fiziki AN USSR Kiyev (Institute of Physibs AS
UkrSSR, Kiyev)
SUBMITTEDo April-9, 1962
Fig. 1. Potential distribution along
the crystal before (I) and; after (2)
'If orming"
IM
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J
~q, 2, S/058/62/000/008/088/134
Lo A062/A101
AUTHOR: Borzyak, P. G.
,TITLE: Phenomenon accompanying the photo-cmf effect in Cs3Sb
PERIODICAL: Referativny-y zhurnalp Fizika, no. 8, 190, 31, abstVact
8E226
(In collection: "Fotoelektr. I optich. y'avleniya v
PoluProvodnikakh".
Kiyev, AN USSR, 1959, 330 - 332)
TEXT: It is noted that the photo-emf, arising when the regions
adjacent to
the electrodes of a Cs Sb film are illuminated with a monochromatic
luminous probe
(the electrodes were ogtained by incorporating Pt into glass, by
heating) rapidly
decreases after the light is switched off, as though a countar-emf
gradually growr~.
The decay time of the direct and reverse current decreases wi 'th
the increase of
~the film temperature. The dependence of the photoconductivity of
the illumiilated
region nearby the electrode on the voltage applied to the film is
determined. The
C53Sb film is not peculiar since the value of the activation energy
6E - 0.76 eV
is in good agreement with the literature data (N. D. Morgulis, B. I.
Dyatlovitakays;
"Dokl. AN USSR", 1939. no. 4. 33, "Zh. teor. fiz.11,194o, io, 657;
S. Yu. LukYanov
Card 1/2

S/058/62/000/008/088/134
Phenomenon accompanying the photo-emf effect in Sb A062/AI01
Cs3
and I. S. Mazover, "Zh. eksper. i teor. fiz.", 1939, 9, 1459). It is
difficult
to interpret the observed phenomenon only by electron processes without
havinj
recourse to a hypotheoia on photochemical proceases.~
0. Shustova,
[Abstracter's note: Complete translation]

DDRZYAK, P.G.; SARBEY, O.G.; TOMCHUK, P.M.
Symposium on Hot Electrons,, beld in Kiev. Vest. AN SSSR
33.no.10t
100-102 0 163. (MA 16tllj'
0
I

48-65,
ACCESSION -NR.- AP4043.33,7,,
S/Olbi/64/60.6/00S/12-249/2255,.

30FLY'AlKy P.G.; ~ATRICH, G.A.-, SLRB-'Y', O.G.
FfJrect of light on surfaab conduction of germanium in the
case of a
clean surface. Fjz. tver. tela 7 nc.9,.2803-2808 S 165.
(MTIM 18!10)
1. institut fJziki AN UkrSSR, K~Yev.

BERIOVSKIY, V.M., Inzh.; AOI~ZTAK, Yq.G., inth.;
SlITYPA, Ye.P., inzh.;
MINEVIGH, A,B., izzhq
Automated electric driTing;of mine hoisting machines
with a
revolving stator. Gor.-.zhur. no, 12:49-52 D 165,
(MIRA ISOZ)
1. Darlkovakiy elaktromekhanicbeskiy zavod.

BDRZYCII, F~-,r-u-La; FAI-ICKI , Zdz~,Slz~
from the psyeblatrIc ly:lnt of 7~ew. Neurol, rpiaro-
chir., ps- ', 11
ycmiat. fol. U iia.42599-592 "--A9 164
I. Z Yilinikl 'Thorob Psychll~!zny~2h kka,ie:, ii
Miedycznej w Wny,~?Ik.-u
(Kierown-~"-,c.h prof. dr. med. T. B-,L"A. I k I ~) .

VarmO.. GALUSE0, Pav,:21
. . ......................
ClIni.c.al olwervattcfis cm the action of tindal in
payt4ila trio
treatment. lqeurol.5 nellrocbi.r., psyclviet.
."(-d'. 1-4 no-Lz~
N9-f:V. JI-Ap t~l~
1. Z' KI.;_niki Chorob ~'t-yclilcznych A~itdtmii
Vedynzre-'
Gdanqk-u Nierounniln prof. dr. med. I L, T. Dili
kiev'j oz).

Dorzyk Z. Wet-Sptunlij of *3nft 6y a Uniform WAtnX blethal

,Pvzq-renltj ramll.na rnokro ayatemern grzobnpq - jednolltyrW'.

labs-
(Praeo last Wl6klen. Xc~ 14), Warszawa. ~954, WPIAS,!.' pr~, 8 figs4,
91

Ing process in th Irom
The wet spinn -e Prodoction of carded yam

ramlefibres Is discussed-The
technological procen consists in a uniform

processing of tho.total
amount of'raw-ma(MM withowt dMerenuatAon..

carding-lechnology.
Ch6talcally deittimmed, etnuls1fied,
Lis to Co)llbjnlg- of

rhftfibhlc:dty softmed, and twlc6.carded, the
fibres aro furt her procmel

methods us6d.ln Jho production of cnrded
yurn. The yam thus vbw

talned slinwaW, ter Quality Indexes than cardLd
linenyarn butivinferlor,

as regards unOrmity,to wonted (combed) lizien
yorn,

BDRZYK) Z. ; 1" .
Remarks on the English flp-% spinning rdll. p. 219.
(FIRM-11SL ULOKIUMNICZY. Vol. 11., No. 5, T-!ay 1957. Warszawa,
Foland)
SO: 'Nonthly List of East &iropean Accessions (EEAL) LUC. Vol. 6,
No. 10, October 1057. Ulicl.

, m
f

BO~ ~F ~F,; DOLGANOV, V.A.
Conditions for the operation and life of car,-, In Ymznetsk
Basin
mines* Vopebezopev ugoll.shakh. 4:270-282 164.
(MIRA 18:1)

I - - -------- -- --- ---- -- ---
BORZYKH, P. L.
."Cfiaracteristic Coilrae of Pneumonia Under Sulfanilamide
and Penicillin
Therapy." Cand Med Sci, Khar1kov State Medical Inst,
Kharkov, 1953. (KL, No
1, Jan 55)
Survey of Scientific and Technical Dissertations Defended
at USSR Higher
1~ Educational Institutions (12)
SO: Sm. No. 556, 24 Jun 55

KATSIYNVSKIY, V.A.. dote.; SORZYXH, P.L.. kand.med.nauk
00 woo"
Treatment of dysentery wlth"I*u"r"fo~Wlllin. Sov.med. 21
no.11:71-74
b '57. (MIRA 11:3)
1. Is kafedry Wektsionnykh bole%ney kzav.-dotsent V.A.
Katsiyevokly) Stanislovskogo meditsinskogo instituta
(dir.-doteent
G.A.3abenko).

BORZY101, P.L., kand.med.nauk
Use of oxygen in infectious hapatitia. Vrach. delo no
5s94-95
My 161. ?MIRA 14;9)
1. Kafedra infektsionnykh bolezney (zav. - dotsent
V.A.Matsiyevskiy)
Stanislavskogo meditainskogo instituta.
(HEPATITIS, INFECTIOUS) (CXYGEN-THERCEUTIC USE)

BORZTXHI P.L.
Rectoremanoscople and kymographic examinations in dysentery,
Vrach.delo no','3t'145-146 Mr 163. (MM 16s4)
1. Kafedra infektsionnykh bolezney (zav. - dotsent.V.A.
Matsiyevskiy) Ivano4rankovskogo meditainBkogo instituta.
(DYSENTERY)

,MATSIYEVSKrly V.A.; . RZIKH..- P.L. (Stanislav)
--:7. -,~. , --
Efficacy of the com~imed treatment of protric-ted and
chronic
dysentery with antibiotics and immogen; abstract. V.A.
Matskievskii, P.L. Borzykh. Kaz.med. 2-hur. no.19.117-118
Ja-.F"61 (MIRA 16-L1)
A
4-

D=71M, Me (stantelys. Ohollmr)l NATALINOT, IX
(stautsiya. Cholker),
Introbolvg advwmd toohnology In a" repair in the Cholkar
shop,
941, 'dore transpe 39 no*M73-74 D 157. (UM llrl)
1. Shobalfulk tokbulabookoto byuro Obellcarskno
otdolonlys dorMl
(for Urmyth), 2. Samostitell umballullm Oh*Umrpkogo
vagomago
=ww%lm (for lbulluff).
(CholkiLr--Ullroads--Ous-YALintowmas and repair)

BORZYKH. V., Geroy Sotsialistichookogo Truda
Unselfish work. Kant. ugl. 7 no.8:6 Ag 158. (MINA 11:9)
I.NachalOnik uchastlm shakht7 No.3-7 tresta
Krannoluchugoll.
(Coal mines and mining)

ACCIMIN
U: AM311D
AUMR: 508,07ftba 46
MUS Proposals as 06 detiermimotlosi~ of the -1wer bousidery of
upper-lovet sloude
SOURCE: Tashkent* SrodnessiatekLy usueboo-loolodovatel'okLy
Sidrometeovelegi-
stitut. Tnwly*, go. 10(25)o 1%3* Voprosy* aviatoLosooX motsocologii
cheskiy In
(Problems in aviation matsoroleV)j, 104-193
TOPIC TAGS: meteorology, clowd, cloud boundery, radiosonde,
atmospheric bmidity,
smear". vapor trail
ABSTUM The author propose two methods for the determination of the
lower
boundary cof upper-level clouds. One method is based on the use of
radiosonde date
and the second an the-general patterns of distribution of humidity
in the free
atmosphere. The methods were developed on -tho basis of data from a
large number
of cases. but the effectiveness of the methods has not been checked
under various
synoptic conditions. . It is ohms that by plotting on an smagram the
points
corresponding to the ibeight, of the lower boundary and points for
temperature or
specific bumidity the points will be grouped along volt-defised
isogromse By
obtaining the averaged values of specific humidity at the lower
boundary of cirrus
we= and cold oessone &M date for surface conditions with eow,46.1 mb

f
ACCUSION M: AT4031125
iIt Is possible to determine the height of the lower cloud boundary
by one of a
curve of vertical temperature disteLbution. Stratification can be
taken Into
account using radiosonde data. The proposed method alto can be used
for detersive-
tion of the Might of the loves boundary of the layer wLtb Panditious
fawrable
for fornation of vapor traits. The error to this method does not
exceed 8-10L.
The described method is unsuitable when the radiosonde station is
ever 150-200 ke
distant or when the radiosonde data is over 9 bours old. In amb cases
it is
possible to use three fonw1as derived by the author which give the
same results
with an error of 15-209. Thus, on the basis qf the results the first
method to
Imore successful. The editor bas comessited on Ithe 4eticle. noting
it to mat wLtboft
value but.-Is based on certain dubious a" debatable promises. 11o
distinction to
made,between different types of cirrus clouds, synaptic processes ace
set taken
into-,scon6st and vertical eavemente are ignored. Tba- emphasis on we
of surfice
it -data ,"- keiix~ the claimed accuracy very surprising. The value
of specific bmaidity.
(to the third decimal place) cited by the author to desmed
unjustified. The
assumption that the conditions for formation oi vapr trails end
circus clowds
are identical is unwarranted. Oirige arte *mat 21 forsuleatt 2
figures 04 2 tables*
213

BORZYMOWSKI, &drzej
Limit property of a tangential derivative of the potential
of
a double Uyer. relative to a ocnductib:Uity equation.
Matematyka
Varazava Pol no,2g"-l , 64 !
1e Department of Mathematics *A*,, Teabnical University,
Warsaw.

L 32o80-66 T/EWP(l) bP(cY WW--------
ACC NR, AT5026390 SOURCE CODE: PO/2543/65/ooo/oo4/oi43/O156
'9
AUTHOR: Adamczyk, Henryk; Borz*owskJLO Andpzej
ORG: Department of Mathematics "A"
TITLE: The tangential discontinuous boundary problem for the
generalized
of heat conduction (the method of successive approxisations)
SOURCE: Warsaw. Fol4technika. Zeszyty naukove, no. 1o6, 1965.
matenatyka, no.
143-156
TOPIC TAGS: tangefitial boundary problem, heat conduction equation,
successive
approximation method
ABSTRACT: By applying the method of successive 122r"tiMm. the suthor*
Inves-,
tigate the problem of determining a function u(A, t) which satisfies
the Initial
condition
21m 0
and the boundary condition in whicb-synbols uj(Pt), ...9 Ur (Pst)
denote the
tangential derivatives of u and d tA the transversal 491"ve of the
function
Card 1/2

L 32080-66
ACC MR, AT5026390
U(A.t) (2).
JA-*1
SP.O(PPOR(POO +
and is a solution of the equation
(3)
at each point of the region AX (0, T), where A Is the difference
of,the'space RD
(n Z 3) and the sun of (n-l)-diwnsional disjoint L&VAwv surfaces D
bi - 1. - - -P)
as vell as the regions bounded by those of the closed surfaced Aj.
he functions
vhich appear in the condition (2) are given on the surfaces Do&
excep points..
of tb:e finite system of (n-0-diserAlonal d1s;oJLnt closed surfaces
8 tk*ll
0 1 vbich are
placed on the surfaces Dj. Orig. art. ban: 4T formulas. [Based on
suthor's
abstract)
SUB CDEE: 12.2o/amm DATz: 18)ky64/ oRiG REr:-.OOT.
Card 2/2

BORZYMOWSKI, A. (Wart2&,je)
-- ,
Propertice of tAngent,',Ial derivatives of a solution
of
a parabolic equation in a noneylindrIcal. domain and
*,chair
application. Prace matem Xrakow 8 no.2:193-215 164,

BORZYNSKA, _)5-Qzena; JONCZYK, Barbara; SYRUWATKA, Tadeusz; WYSOCKI,
Eugeniusz
Prelimina y evalualtion, of antibacterial properties of arydil soaps.
Prxegl. epidem. 15 no-3:325-329 161.
1. Z Laboratorium Technologic=ego Dozynfekcji,, Dezynsekaji,
DeratyrmcjL~-Ministerstwa Zdrowia i Opieki Spolecznej Kierowrdk:
dr Konrad Zembr=ski.
(AINTISEPTICS) (SOAPS)

F?TM3.5U, Aiirel, prof,.- W9, Nicolae; KISS,
Arpad, asist.; MADAMS, loan,
I
aidat; YATASAN, Nlnftp~ asist.
Rq,arding the size of the atmospheric refraction
coefficient
K and the prp,4qion of the trigonometric leveling
at great
distances. i,e. geodezie 8 no.4-28-41 164.

OVAT'IA
CZECHOSL A
P.- Pediatric Hospital for Psychiatry (Detska Psychiatricka
ffe-01-TKI, Dubi v Krusnych Horach,
"Play Therapy Contribution to Child Psychotherapy*"
Prague, Ceskoslovenska Psychiatrieq Vol 62, No 4, Aug 66, pp
247 - 257-
Ab _7: Play Is a charac-
Astract Juthorts English summary modified
taristic and dominant spontaneous activity of childhood; psycho-
pathological.dynamism is Rlso found in childhood. Toys divided
into functional groups are used by the author to establish
communi-
cational, projective and expressive means to establish a
permissive
therapeutic relationship; the purpose is to eliminate pathological
interpersonal stereotypes and reactions. anpirical rating scales
of the treatment are presented. The dynamic orientation of this
approach is stressed. 8 Westerns 4 Czech references. (Manuscript
received 14 Aug 65).
72 -

-- ----
BOSACEK, V.; POLAK, R.; KUCERA, E.; DANES, V.
--------
Swface and structuial properties of aluminum oxide
after its
treatment by halogens. and ablulnuatetrafluobgrate. Con
Cz Chen
27 no.Ils2575-2585 N 162.
1. Institut fur physikalische Chemis,
Tachechoslowakie6be kka-
dazie der Wissenschaften, Prag.

BOSACEK, Vladimir; POLAK, Rudolf
Simple calorimeter for determining the wetting heat of
powder adsorbents. Chem listY 57 no. 5; 514-518 My 163.
1. Ustav fysikalni chemie, Ceskoslovenska akademie ved.,
Praha.

BOS&,'EK, V; POLAK, R;.KU6I-;RAI E; DANA,, V.
Czechoslovakia
Institute for Physical Chemistry,_Czechoslovak
Academy of Sciences Prague (for all)
Prague, Collection of Czechoslovak Chemical Commulli-
cati2ns, No 11, 1962, pp 2575-25U4-
"Superficial and..Struct-ural Properties of Aluminiumoxyde
Treated with Halogens and Aluminiumtetrafluoborate.11

BOSACEKV V.
Gan ohrovatographio separation and adsorption of
noble gases,
oxygen and nitrogen on modified seclites of type
X. Coll Cz-
chem 29 no.8sl7cY.7-180Z Ag 664.
1. Institute of Physical Ghemistry., Czechoslovak
Academy of
Saienc-sess pragu~.

BOSACKI, K.
"Hannering Machines with Double Action." Tr. from the Polish.
D. 109 (Strojirenstvip
Vol. 3, no. 2, Feb. 1953,-Praha)
SO: Monthly List of East Euronean Accessions, Vol. 3, no. 2,
Library of Congress,
Feb. 10,54, Uncl.

C. rE i
T4' ST t!
u -03
mi c T,
rv
In
1.3, 11:3. -3, 61,
svt,hor foun,.4 a ne-w ccc;urz-arjoe of*
R r t) 1.1'a r D a n u~hn Rt S v a t o .4 u r sra,

USSR / Cultivated Plants. Fruit Trees. Small M-7
Fruit Trees.
Abs Jour: Ref Zhur-Biol., 1958, No 16, 73163.
Author :_Bosak. D. YP_
Inst : Not given,
Title :Influence of Leaf Apparatus on Ability of Gooseberry
Shoots to Take Root.
Orig Pub: Sad i ogorod, 1957, No 8, 46-47.
Abstract: During hilling of the lateral gooseberry shoots
and of the bottom branches of the shoots, filling
up the leaves and shoots with earth leads to a de-
crease in quantity and quality of planting material.
The more the leaves remained above the soil at the
ends o2 the hilldd shoots, the better they grew and
took root. -- V. V. Yastrebova.
Card 1/1

9
I
mmmw~ I

1: 30997-66 9-1T(M)/5-TP (V)/T/DrP(t)/aJT (k) IJP(c) JD/HK
IV) -'r6bitt CION's "0R/0%11/66/0001003/0119/0119
ACCF"
~.-INVENTOR: Gurelfth. S- NO 50mak. L. K.
ORG: none
TITLE: Flux for welding 11 ht metals and alloys. Class 49- No
[announced by
a 4"a
"I Yd-i MnR c-L -a.
-the Institute of Electric Ve Ye. 0. Paton,AN UkrSSi (Institut
elektronvarki
AN UkrSSR)J
SOURCE: Izobreteniyaq promyshlennyye obrazt9y, tovarnyye znaki,'no.
3, 1966, jig
TOPIC TAGS: titanium, titanium weldingi submerged are welding,
welding flux
ABSTRACT: This Author Certificate Introduces a flux cont. aining
C.aF2*and N&V for'
welding light metals and alloys. For welding titanium and titanium
alloys, 3% of
SrF2-SrClz is added to a flux containing 92% W? and 1% NaF21b JAZI
SUB CODE: 131 SUBM DATEs 27Nov64/ ATD PRESS. /Z/
Card 1/1 ~C-

GUREVICH, S.M., doktor teklm. naujq_T~TSP L.K., inzh.
Effect of calcium flouride on the technological
properties of
AN-T fluxes. Avtom. svar. 17 no-11:47-50 N 164
(MIRA, 18:1)
1. Institut elektroevarki imeni Ye.O. Patona AN
UkrSSR.

KUTAJ.; EISELT, b., MUDr.; BOJANOVSKY, I.; WAK.,,K.
N Sport efkiciency and strength in the aged. Cas. lek. cesk.
104
no.13:351-356 2 AP 165
1. Vyzkumny ustav telovychovny v Praze (reditel: MUDr.
E.Eiselt).

BOSACEM, J.
The effect of medium composition on the metabolism of isolated
rabbit
kidney cells. Physiol. Bohemoslov. 11 n0.1:39-45 162.
1. Iaboratory for Cellular Metabolism,, Institute of Biology,
Czecho-
slovak AcadwW of Sciences, Prague.
(KIDNErS mstab) (TRYPSINS pharmaeol)

BOSACKOVA. J.
Electrolyte distribution and-volume changes of
isolated kidney
cortex cells at OOC. Physiol. Bohemoslov. 11
no.4!294-299 162.
1. Laboratory for Cellular Metabolism,
Microbiological Institute,
Czechoslovak Academy of Sciences Prague.
(POTASSIUM) (CALCIUMJ (KIMiEYS) (TEMPERATURE)
(DIURETICS MERCURAL)

BOS" (BratimU~R, ulica Obrancov mieru 41).
. Juraj
On certain class of oriented gmphs. VAt fyz cas
SkV 12
no.2:81414 162.
1, Kabinst matematiky Slowenskaj'a1cademis vi*dy
Bratislava.

BOSAK. JuraJ
c-------
B-semigroups. Mat fyo cas SAV 31 no.102-44 161.
1. Kabinet matematUW, Sloveneka akademia vied,
Bratislava,
ulica Obrancov nieru 41. - -

BOSAI, Juraj
Ganoral powers in somigroups. Hat fyz cas SAV 13 no.2-.
137-146 163.
1. Ceskoolovenska akad mia ved,, Kabinet matematiky
Slovenskej akademia vied,, Bratiolava.. ul, Cbrancov mieru 41.

Bc%q-AK, Juraj
On subseudgroups of samigroups. Mat fyz cas SAV 14
no.'s
289-1196 164.
1. Cabinet of Mathematics of the Slovak Acadenq of
S04 ences,
Bratialava, u1. Obrancov mieru 41.

GOLU, Jan; BOSAK, Toodor; OGONSKA, Aniela; SZALAJKO, Mari&
Hairdresser and barber shopa; as a possible link in the
epidemiological chain of infectious diseases. Roczn panstw
aakl hig 14 no-5s407-414 1,63.
1. Epidemiological Section of the Voivodeship Station for
Sanitation
and Epidemiology, Szczecin.

BOSAKp V.D., inzh.
The problem of saying boron . Stroi. i dor. mash. 7
no,8:39
Ag 162. (KM 15:9)
(Bronze) -

BOSAK, Yura7 [Bosak, Lura,
- ------ AU
On radicals of semigroups. Nat fyz cas 12 no.3:230-234 162.'
1. Kabinot matematiky.Slovenska akademia, vied,, u1. Obrancow
mieru A+Is
Bratislava*

L 00673-67 /EWP(QjW(_
"6015251'. 251 6100 05/0070/0071
SOURCE CODEz URIUL
AUTHOR: Bosak, L. GurevLch' S. M.
17
~ORG: Institute of Electric Welding In. Ye. 0. Paton, AN UkrSSR
(InStitut
clektroavarki-All UkrSSR),
TrM: Nonhygroseopic flux for weldi titanium And its alloys
SOURCE: Avtomatichaskaya. evarka, no..5, 19669 7 -71
TOPIC TAGS: titanium anqr, weld ing,flux,' welding, titanium, are
welding, strontium,
compound, chlorine compound/AN-Tll w9lding -flux, M'titanium
A~STRACT-. The fluxes used in the automatic and semiautomatic are
welding of Ti and-
its alloys are more or. less hygroscopic, since they contain chlorides
of alkali and
alkali-earth metals. .. This harbors the danger of the contamination
of the Ti and
Ti-alloy weld metal with oxygen a-ad hydrogen. Hence, the author has
experimentally.
developed a nonhygroscopic welding flux on investigating 10 different
compounds.
Findings: the minimum (virtually nil) hygroscopicity is displayed by
BAF -B'C'2 and
2
SrF2*SrCl compounds. Since the salts of Ba absorb X-rays and thus
complicate
420graphe inspection inclusions in weld metal, the nonhygroscopic flux
was
~
Lra of slag
developed on the-515.11 or the compound SrF2'SrC'2. The compound was
malted on usiog
UDC: 621.791.04:669.295
rnrd 1/2

L 00673-67
ACC NRs AP6015251
44.5 wt.% SrF2 and 55.5 wt.% SrCl2 and the flux base, an using
wt.% NaF. After this-both the compound and the flux 99 wt'% CaF2
and:
anulated to the
base-were gr
required size by cruShiAg,and sieve-screening and automatically
mixed in mutual pro-
portions of 7 and 93% by weight, respectively, thus assuring a 4
wt.% content of
composition 'of SrF2*SrC'2. The flux ob-
SrC12 in Accordance with the stoichiometric
tained by-this method pr6duce's.-Satisfact*ory-volde-lh the prenuce
Of welding currents
of up to 600-700 a. The weld surface is lustrous, silvery, which
demonstrates that
the slag provides adequate protection for not only the weld pool
but alsothe
solidifying weld. This is of great significance to multi-layer
welding, since it
dispenses with the need to clean the surface by mechanical means
every time before
the next.layer is deposited. This newly developed welding flux has
been named
A-H-Tll. The insignificant hygroscopicity it displays is chiefly
due to the absorp-
tion of moisture at grain boundaries. When exposed to air, this
flux virtually does
not absorb any moisture. Tests of mechanical properties of the 10-M
thick joints of
N VTl technical titanium welded with the aid of this flux produced
satisfactory re-.
Fiults. Orig. art. ham 2,figures and 1 table.
SUB CODE: 11,13,07/ _~.S= DATE: .24Sep65/ MIG REP: 002
2/2
Card

SAMSONOVP G.V.; BOSAK L.L.
Substitution of cations in benzylpenici2lin on ionites.
Med.prom.
16 no.7:32-34 Jl 162. (KERA:9)
1. Institut vyaokomolekulyarnyth soyedineniy AN SSSR.
(PENICILLIN) (ION EXCHANGE RESINS)

MOSAX, M.
Vitebsk silk factory. Imb.1 sial. 32 no.12:11 D 156.
(KM 9:12)
(Vitebsk.-Silk mnuraeture)

BOaa, Toodor; DWOUK,, Zbigniew; GOLBAp Jan; OGONSKAf
Aniela
Codtrol of mosquitoes in populated settlements and
adjacent open
ar"s of the island Karsiborz. Przegl. epidem. 15
no-1:59-66 161.
1. Z Wojewodz)dej StaoJi Sanitamo-Epidemiologicznej v
Szczecinie.
Dyrektors lek. nod. Z.Dworak.
(MOSQUITO CONTROL)

EISELT, Z.; BOJANOVSU, I.; BOSAK9 Vle-
Blood picture In aged males, Cas,lek,cemk 100
no.22:686-689 21.4 161.
le Vyzkmy ustav tolovyehovny, Praha, reditel MUDr. Z.
liaelt.
(BLOOD Cl=) (SIX) (AGING)

~--_r__~L4_04 6 EWT AT
1 (As N),
ACC NRI AP601,9316 SOURCE CCDE: UR/0057/66/036/005/0958/0960!
AUMPR: -BoseZkin, V."~.8o;-Favlovskly, A. 1. Vn
ORG: nofie
TITLE: On the possibility of compensating the space charge
of,pulsed electron beam
SOURCE: Zhurnal tekhnIcheskoy fixiki, v. 36, no. 5, 1966, 958-960
.-TOPIC TAGS: electron beam, apa~~ eikarie, positive lon, gai
lonisiation, gas pressure
ABSTRACT: The effect of residual gas pressure on the passage of a
pulsed electron
beam through a metallic tube has beiin Investigated with the
apparatus diagrammed In
.,-the figure. The.electron gun.was activated with a 300 W pulse
with a short rise tim
',aiid an approximately exponential decay with a half time of 12
Wee. The beam was col.
limated with the system of several 5 = diameter apertures. At the
output of the col
S limator the current density woo 5 AAM2 and t1w
angular spread of the boom was 50. The inter
nal diameter of the 50 ca long metal tube 3 was
a 5 ma. The current to the collector 5 was re-
~T
1. . .. _ ~ __ - - - - _,_~Ikv corded with an oscilloscope and was
Investigat-
Diagram of the apparatus. 1 - col- ed as a function of the
residual gas pressure
limator; 2 grid; 3 - metallic tube; (varied from, 2 x 10-5 to 2 X
10~4 M Hg) and
4 - foil; 5 colledtor. the potential an the grid 2. When the foil 4

L-134-04-66
f-b
ACC NR: AP6015319
was absent and the grid was at ground potential the current to the
collector was small
and indepondent of thexesidual gas pressure. When a positive,
,A-0tential was applied
to the grid the collector current increased with Increasing reiUual
gas pressure.
When the grid was 200 V positive the collector current was 10 WON
greater at a re-
sidual gas pressure of 2 x 10-2 mm. 11C than at high vacuum or
witk,ihe grid grounded.
Similar behavior was observed when the 10 micron aluminum foil 4 was
in place. 7be
observed effects are ascribed to compensation of the-space charge of
the beam by
positive ions of the residual gas. It is suggested that the effect
of the pasitively-:.
charged grid 2 is to prevent escape of positive Ions from the
Interior of the metalll
tube 3. Orig. art. has: 2 figures.
SUB CCDE: 20/ SUBM DATS: 29Jul65/ ORIG IM: 001/ OM IMF., 004
Card 2/2

BOSANAC, B.
'Yugoslavia (430)
History w4 Description - SerIals
Th* significance of Opor O~ In RMUML40 po 110
RMEW OF 13T ATIONAL AFFAM. (Federation
of Yugoolav Jowmalfta) Beograd. (Fortnightly
Journal an International problus.. ftblIsIM also
In Serbo-Croatian an MIJUAMMM Politika, &M In
last Warovegg Accessim List, LlLkw7 of
Congress,, Tole 1. no. 13, X"dO*r 2932.
UNCLASSIPM *Card 1 of 24

BDSANACO N.
Tupelavia (430)
History and Description - Serials
Ikys wd some in the subversive activity
against Yugoslavia. po l3e RaseifloatIon
of the Bulgarian I RVIN
k;
OF IFfMATIONAL ~ M ederation of
Yugoslav Jburnalists) Beograd, (Fortniabtly
Rag �Wyean Accessions Ust. Ubrary of
Congresso Vol* It- noe.139 November 1952o
MMASSMED *Card I of 28

BOBANACP Be
Yapalsvia (430)
Journal on international problems.
Published
also in SerboAroatian as j2jVpjt2ft =Iuht
and In French as UM J2 La Pol -yondials)
9
Vol. 3, no. 12, Jima 16, 1952.
East Varoyean kocesdons Litt. Library of
Congress, Vol. 1, no. 13, November 1952,
INCLASSM *Card 2 of 28

BOSkUC, B.
Yugoslavia (430)
French as Revue do Ua Poli yndial0j,
VdI* 3p Do* 16, 14is-t-1-69-V9_52.
Vast Dwopean Accessions List, Librairy
of Congress, Vol, 1, no, 13, November 1952,
MCUSSIMM ICaM 2 or 20

PHASE I BOOK EXPIDITATION YUG/5527
Bosanac, Tomo
Nuklearna propulzija (Nuclear Propulsion) [Belgrade, Export
press, n. d.1 No. of copies printed not given.
Sponsoring Agency: Savezna Komisija za Nuklearnu Energiju.
4e 04,
Reviewers: V jislav Babic, Eng~neer, Ljubomir Barbaric,
Engineer,
nd Salom Cca, Engineer. Ed.: Aleksandar Spasi4c*. Tech. Ed.:
ivorad Atanackovec.
l
PURPOSE : This booklet is intended for general readers
interested
Ir -the utilization of nuclear energy as a means of
propulsion.
COVERAGE: The author outlines the present state and prospects
of utilizing nuclear energy for propulsion of ships, aircraft,
rockets., and land vehicles. Concise information on funda-
mentals of nuclear physics and generation of nuclear energy
is given. Various types of nuclear reactors are described and
schematic representations of nuclear propulsion systems are
Card---j-/4--

Nuclear Propulsion
YUG/5527
given. Progress made In tYr USA, the Soviet Union, and some
European countries In the field of nuclear energy utilization
is reviewed. No personalities are mentioned. There are no
references.
TABLE OF CONTENTS:
Foreword
Introduction
Nuclear Reactor
3
5
7
Ch. I. Ship Propulsion 11
Application problems 12
Conditions on ships 20
Propulsion systems 22
Types of reactors 24
Utilization of fuel 28
Schematic representation, of propulsion systems 28
C ard-2/4

BOSANAC, T.
InternatiorAl Conference on the Peaceful Use of Atomic Energy.
p-.335
ELEK?ROPRIMDA. (Zajednica jugoolovendka slektroprivrede)
Beograd. Vol.
8, no. 6. Nov./Dec. 1955,
SOURCEt last European Accessions List. (EM). Library of
Congress, Vol.$
no. 12, December 1956

BMUCIC, K.; COCKCVIC, B.; VARICAR, M,
Meauring the specific beat of solids in the dependency of
temperatures. Obs mat fit 7 n0.2182-87, 160. (Ew 9:12)
L Fisicki inatitut Priradoelownio-matematickog fakulteta
u
Zagrebu.
(specific beat)
(Calorimeters and calariustry)
(Solids)