SCIENTIFIC ABSTRACT FALKOVICH,S.YE. - FALKOVAKIY, L. A.
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SCIENTIFIC ABSTRACT
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AUTTIOR: FA L I KOV I CH .109-5-10/22
TITLE: '--Gn-tlTe _Pre~iuiol_Fin Vi~, I. Coordinati~ in
Radiolocation jy:;tums in "'ho Case of Jlnuolieiont Inte--rations.
(C tocilrJosti V 0,10-
nykh Aste'I'll-l! Fri
IERIODICALt HadiotoldinP i !Zu.~tron 1:4-, 1)~7, Vt,,l NI. 1
U. s. S. it.
A 11STRACT: Tho author'L; wor% iij 1)~L:jod (;,ti L',W critori:i or lirvoision and
the genceral fOr;:111lfL(3 1"or the 3i -ral and the diaturlb-,trices
-d -(-- deor-ribed
at the output of a r- io r~!Ceutiun 1~14t,IL. ~huy I.L.1
'ior's jrauer i -1c! 1~ '57,
in the aut, .,:I i t U--onika, 19
Vol 2, Vr 4 , ')P 4150 - 46u- Cttleul~,.Lion for:.tulae Lrt~ cl,~rivnd
here for avora-Ea orror ui,uarua i;~ 'u:ifi :-~ieat3uru-uent of raiv-0.3,
and optimum paranoteri of ',Ile reCCDtiOn ICViCeS i1, the
cage of incolic!rent inte-~ratlon r,~ (Ititerminod froa the 1,cint
of view of procioioll. 11, io t,!iqL tho followitr, 13
neconvary for Oiv
accuracys 1) The (,f t:ie radio a:.i,.1ifiO_r h-s
to 'Oe brout.~hb iru linc ;.,ith fort or l.:,e sijpn-1 impu1scs.
2) Yhe- impul-se exiavaota.iLiAL; c' vidco line ha3 to have
the character of a derivition ot' the de-ItL function. 3) Record-
Card 1/2 ju.-,, jau,;t take place at the moment, cte the ouisa-e of the out-
109-5-1-0/22
On the Precioi~jn irj the Hi.cordin.,- a
in RadioeleCti-4C j!j 1,110 C..jjj )f
tions.
put volta-e Vxouj~', 7-cro. It i.; zlic,--11 Liat, i-, conzrast to
the linear det,-,otlcm of sLtmri,- Hie .:i-,~,'ification of
the optiatim form of the .-If thp radi.., ai-ipli-
fiu-r in the detectin,: of wcik. 'ut, co;:,lensated
by the corresj,u::ding of the u. ~!L~: Vl(leo
a~!i,,lifier and thut it, leads w, in Lhe lispersion
of errors.
(P ~;Javlc
Hot .,iven
PREjL"-!1ET) BYs
jiVAlLABL,: Lii)rtvj of Congress
(;ard --/?
FALIKOVICH, S.Ye.
.WWWNAWMM --
Precision In reckoning the distance coordinates in radiolocation
system@ based on incoherent signal storage. Radiotekh. elaktron.
2 no.5:601-608 Yq 157. (Radar) (KLVA 10:9)
AUTHOR: Fal'kovich, S.Ye. ~ 8011/109-4-1-25/30
TITLE: '- Poten ia Accuracy of the Determining of the Angular Co-
ordinates in Radar Systems (Potentsiallnaya tochnost'
otscheta uglovykh koordinat v radiolokatsionnykh 81stemakh)
PERIODICAL: Radiotekhnika i Elektronika, 1959, Vol 4, Nr 1,
pp 142 - 144 (USSR)
ABSTRACT: In the analysis it is assumed that the received signal is
reliably detected from the background noise. The problem
consists of evaluating the limiting accuracy in determining
the angular co-ordinate 0 when the single-pulse method is
employed (Ref 4). The mean square deviation:
(e %) 2m
of the readingo cl~( with respect to the true value of the
co-ordinate GO can be regarded as a measure of the
accuracy. It is shown that the accuracy can be expressed
by Eq (3) where P x(e) is the "a posteriori" distribution
of the probabilities of the presence of a target at all the
angular co-ordinates within a region 01 to if
Cardl/3
SOV/109-4-1-25/30
Potential Accuracy of the Determining of the Angular Co-ordinates
in Radar Systems
the antenna system consists of two reflectors containing
the radiating dipoles in their foci, and if these are
separated at distances D from each other, the maximilm
accuracy is expressed by:
0) 2 C2
2 (10)
2
4Q
where Q2 is the total energy of the signal and a 2
is the spectral intensity of the noise. Similarly, on
the basis of Eq (3), it is shown that if the antenna system
consiet5 of one refle,,tor and two radiating dipoles, the
maximum accuracy is exprppd by:
-~ff 2 Cr A
Card2/3 4Q2(2 In 2)2
SOV/109-4-1-25/30
Potential Accuracy of the Determining of the Angular Co-ordinates
in Radar Systems
where i!!~ is the width of the directionalpattern
of the antenna.
There are 4 Soviet references.
SUBMITTED: June 12, 195?
Card 3/3
AUTHOR: Fall1covich, S.Ye. sov/io9-4-4-8Z2k
~Frol)ability
ori"/Method to
TITLE: some Results of plying the "A Posteri
the Problems of Radar System Design (Nekotoryye
rezul'taty primeneniya metoda aposteriornoy veroyatnosti k
zadacham proyektirovaniya radiolokatsionnykh sistem)
PERIODICAL: Radiotekhnika i elektronika, 1959, vol 4, Nr 4,
pp 618 - 628 (USSR)
ABSTRACT: For the purpose of analysis it is assumed that the radiated
signal is expressed by Eq (3), the perturbing noise is given
by Eq (4), while the received signal is represented by Eq (5):
the black-face letters in these equations represent the
complex slowly changing amplitudes, while f 0 is the carr-
ier frequency of the signal. The reflected
signal is denoted by AT . The signal reflected from a
moving target has a continuously changing delay time, -it
and can be represented by:
i 0 if
Cardi/4 AT(t - -tt Re AT(t - Vt )e 4.10(t-td ejfl (6)
sov/iog-.4-4-08/24
Prqbability
Some Results o Applyine )f the "A Posteriori '/Method to The Problems
of Radar System Design
where the amplitude AT has a certain finite value during
tll-t~! period T and is zero outside this interval. The
phase y in the received signal is a random quantity
having a uniform distribution as Eepresented by Eq (3). The
energy of the reflected signal Q is constant and is
given by Eq (9). It is further assumed that the delay
time -r_t varies at a constant rate and is expressed by
Eq (10). The reflected signal can tt;crefore be written
in the form of Eq (12) Where I is defined by Eq (11).
Tile "a posteriorit' distribution for the whole set of the
received signals is given by Eq (13). The probability
can also be expreE sed by Eq (15) or approximately by
Eq (16); here q denotes the signal-to-noise ratio and
is defined by Eq (14). On the basis of the above equations
it is shown that an ideal radio receiver can be composed of
the following elements: 1) N linear channels; 2) N
Card2/4 detectors (terminating each channel), and 3) a device which
soV/log-4-4- '~'/24
Prgba~iA
Some Results of Applying the "A Posterl r3. eltfYod to the Problems
of Radar System Design
adds the outputs of all the detectors and performs the
weighting operation. Further analysis of the problem
shows that the optimum processing of radar signals includes
the process of coherent storage. The difficulties -
encountered in employing the storage technique are due to
the movement of the target and to the resulting frequency
shift in the reflected signal. When the signal duration
is T , it is recommended that the coherent storage should
be done within an interval of T/n where n is a digit
not greater than 10. The coherent storage can be done in
three ways: 1) selection of the signals which do not
require the elimination of the parasitic random parameter,
that is, the signals not requiring the velocity averaging;
2) application of multi-chAnnel systems which permit the
velocity averaging; 3) application of two-channel systems
which introduce a velocity correction. The signals which
permit the coherent storage without the velocity averaging
are of two types: very short signals whose duration does
Card3/4 not exceed 0.1 of the period of the maximum Doppler
SOV/109-4-4-8/24
Some Results o, Applying the "A Post cr?6Pk4""-4Wd to the Problems
71q
of Radar System Design
frequency possess this property. Also, the signals which
have a s-aw-tooth frequency modulation whose period is
equal to the storage time interval do not require the
velocity averaging. In general, the opt-imuin processing
of the signals reflected from a moving target can be done
in a device consisting of N channels; a velocity
correction k Al Is introduced in each channel; k
denotes the number?& channel and Al represents the
frequency shift between the channels. There are 5
references, 1 of which is English and 4 Soviet; 1 of
the Soviet references is translated from English.
SUBMITTED: February 20, 1957
Card 4/4
ile 76 0
AUTHOR:
86800
S/142/60/000/003/015/017
B192/E482
Fallkovich, s,ye.
TITLE: The Threshold Ratios for a Frequency-Diversity Radar
System
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Radiotekhnika,
ig6o, No-3, pp.404-407
TEXT: The fluctuation of the signal strength at radar receivers
can be reduced by employing frequency diversity systems (Ref.2)
-h1ch operate simultaneously at several frequencies. In such a
system the received signal s(t) is in the form of a sum of
independently fluctuating elementary signals sl(t), s2(t)--
sn(t) and can be represented in the form
Eq.
Card 1/ 7
4 n 1(2%10t + 4pi)
S(t) I 31(f) - S it, Re SIMe
ti 1-1
86800
S/142/60/000/003/015/017
E192/E482
The Threshold Ratios for a Frequency-Diversity Radar
The initial phases Vi and the amplitude parameters ci for the
various elementary signals si(t) are statistically independent
random quantities; yi has a uniform distribution p(~pi), while
ei has a Rayleigh distribution p(si). It is assumed that the
signal x(t) appearing at the input of the receiving device
contains a Gaussian noise of spectral density No and sometimes
the useful signal (defined by Eq.(l) ). It is shown that the
probability A for a radar system with the signal represented
by Eq.(l) Is given by (Ref-3)
A erp
Eq. 9;
(2)
Card 2/7
86800
s/142/60/000/003/015/017
E192/E482
The Threshold Ratios for a Frequency-Diversity Radar
2
where q, is the mathematical expectation of the ratio of the
energy of an elementary signal to the spectrum density of the
noise and zi is a random quantity which is a function of No,
X(t) and Si(t). Eq.(2) determines a system for optimal
processing of the received signal x(t) in a frequency-diversity
equipment. Such a system consists of n channels and a device
adding the outputs of the channels. Each of the n channels
comprises an optimal linear filter and a square detector. If the
received signal contains no useful signal, the distribution
functions for zi is
PN (Zi) = exp (- Zi (3)*
If the received signal contains a useful signal, the distribution
of zi is given by
Card 3/7
86800
s/142/60/000/003/015/017
E192/E482
The Threshold Ratios for a Frequency-Divcrsity Radar
Eq. PSjV(2j)-IjpjV~z,)- ep(- Z, (4)
(4) 1+ +q?
The random quantities zA are statistically independent. Now,
the threshold value of t e signal/noise ratio can be determined by
a simultaneous solution of
PV (z,- n) (6)
;:Eq. F-F(z.;n)--
(6)
and
(7) D - D(z.; n) PsN(r, n) dz. (7)
where F and D represent the probability of a false alarm and
Card 4/7
86800
S/142/60/000/003/015/017
E192/E482
The Threshold Ratios for a Frequency-Diversity Radar
the probability of detection respectively, PN is the
distribution function for n statistically independent random
quantities for the case represented by Eq.(3) and PSN is the
distribution function for the case represented by Eq:(4). The
final expressions for F. and D are
Eq. fp's (Z.):
Z'
(A) D +
where kon is defined by
Eq. I'(n: 4
By solving these equations it is found that the threshold value of
Card 5/7
86800
S/142/60/000/003/015/017
E192/E482
The Threshold Ratios for a Frequency-Diversity Radar
the signal-to-noise ratio is given by
Eq. q3 arc 4,, (F)
(C) I UOP - arc _?. W)
where arc 9n defines a function which is inverse to (Pn'
that is if x arc (Pn(y) the'n y = Yn(x). The values of the
threshold signal/noise ratio as a function of n for various F
and D are plotted in two figures. It is found that if the
probability of detection is increased, the threshold signal/noise
ratio is rapidly increased. By employing a frequency-diversity
system, the effect of the signal strength fluctuation can
considerably be reduced and so the energy necessary for detecting
a signal with a given degree of reliability is reduced. There
are 1 figure and 4 references: 2 Soviet and 2 non-Soviet.
Card 6/7
86800
S/142/60/000/003/015/017
E192/E482
The Threshold Ration for a Frequency-Diversity Radar
ASSOCIATION: Kafedra radioustroystv Ukrainskogo zaochnogo
polltekhntcheakogo instituta (Department of Radio
Equipment of the Ukrainian Correspondence Technical
Institute)
SUBMITTED: October 2, 1959
Card 7/7
8 L gh 13
S/109/60/005/009/029/030/AA
e1 E032/E514
AUTHOR: Fallkovich- S. Ya.
TITLE- Optimum Detection of Signals on a Background of Noise of
Unknown Intensity
PERIODICAL:Radiotekhnikn i elektronika, 1960, Vol.5, No.9,
pp-1539-1541
TEXT: The problem is formulated as follows. Suppose one is
concerned with the reception of signals s(tia) consisting of a
given function of time t and a set of random parameters a on a
noise background n(t), which can be approximated by gaussian
white noise. The spectral intensity of the noise N 0 is unknown.
This intensity is assumed to be random but constant in each
interval of observation (O;T). Using the measured oscillation
x(t) (O< t/ Y0(Z2) (8)
The function Y is the same both in Eqs.(7) and The
difference is tRat in the latter equation both Y and Y are
functions not only of the a priori,but also of the input Sata x(t).
For this reason the optimum system should consist of two channels,
namely, a Y shaping channel and a Y shaping channel. The paper
is concluded with the application o? the above theory to a number
of special cases. There are 3 Soviet references.
SUBMITTED: December 16, IL959
Card 5/5
ff.j
R1 I
86881
4/8;~- 0
S/108/60/015/012/CO3/009
B01O/BO59
AUTHOR: Pal$kovich, S. Ye., Member of the Society
TITLE: Correlation Functions and Spectra of Frequency-modulated
Radiolocation Signals
PERIODICAL: Radiotekhnika, 1960, Vol. 15, No. 12, pp. 13 - 18
TEXT: The author demonstrates the approximative calculation of correla-
tion function and energy spectrum from a given frequency-modulated radio-
location signal. The reverse problem, i.e., calculation of the frequency-
modulated signal from the given correlation function, is solved too. The
results may be generalized to signals of small amplitude-modulated band-
width and also to periodic signals. For a frequency-modulated signal of
the shape A(t) - Aocost2n[fot+e(t)]+9j (A. - amplitude of the signal;
f0 - carrier frequency; 9 - initial phase angle; e(t) - frequency swing),
A2 T(I
the correlation function (5) f(T) - --a coef2n[foT+8(t)-~(t-T)Jj dt Is
2 _ T
Y+T
Card 1/4
8t-'66' I
Correlation Functions and Spectra of S/108/60/015/012/003/009
Frequency-modulated Radiolocation Signals B010/B059
obtained if equal signal and modulation periods T are assumed.j(T~ is
different from zero for very small T-values only; thus, 6(t)-g -T OF(t)T
holds approximately, where F(t) ~L e(t); then, (7)
A 2 T12 dt
0 Cos 2n T + P(t) dt is obtained in the place of (5). The
.0,J Y- [ If 0 .111
T72 OD
energy spectrum-n(f) is given asfl(f) -_S t(-T) exp (-12nfT) dT. An example
00
with linear frequency swing function F(t) - 2Fmt/T , jtj-_4-T/2 (T - period
of modulation) is computed. If F(t) varies monotonically from one
extremum, (Fm ) to the other (-Fm), then the frequency-modulated signal can
be calculated from the given correlation function. Since t is a unique
function of Fs t T(F), one can substitute f - fo + F(t) for t in (7)
A2 f+F A2
0 _aid (f_f.)l
and, thus, y(-') I~L T(f-f )I cos(2nf-r)df and.Q(t). ___f
f -F df 0 2 df
0 m
Card 2/4
86681
Correlation Functions and Spectra of
Frequency-modulated Hadiolocation Signals
S/108/60/015/012/003/009
B010/B059
k2 T 2/T2)
(11). If, for instance, y(T) = exp(-xi U cos 2Rf0T is given, then
12-511111
t - V(F) - 2 T exp(-y 2/2)dy is obtained from (11).
Z ~Q(x)dx 7M -OD
The notations ares x - t/T and y - (f - f OVFM 1 so, F(t) (t/T),
u
where f-'(x) is the function inverse to f(x) m 1 exp(-y 212)dy. The
2 7rn J
co
approximation Ao(t)Ao (t - T)fVA0(t) is allowable if the signal has an
additional amplitude modulation, provided the amplitude-modulated band-
width is considerably smaller than the frequency swing. Thus,
r/2 2(t)cos f2i[fot + F(t)-r] dt and
A
2 _T72
1 2 E
.n(f) - - A P (f _f 0)]+L (p(f-f,)l for If_fojZ-Fm. Finally, the case where
0 df
Card 3/4
86881
Correlation Functions and Spectra of S/108/60/015/012/003/009
Frequency-modulated Radiolocation Signals B010/B059
the signal consists of M repeating periods is briefly discussed:
M-1
kit) - A(t - kT). In this case, the energy spectrum
aj f ) . 112 $Q__f1(n/T)jsin x UT(f-n/T)/7[MT(f-n/T )12 is obtained. There
nm _oD
are 2 Soviet references.
SUBMITTED: April 4, 1958
Card 4/4
PHASE I BOOK EXPLOITATION SOV/5513
Fallkovich- S-Ye-
Pri em radiolokstsionnykh signalov na fone flyuktuatelonnykh pomekh
fReception of Radar Signals Agqinst a Background of Fluctuation
Noises) Noscow, Izd-vo "Sovetskoye radio". 1961. 310 P, 10,000
copies printed.
Ed.: N.D.Ivanushko; Tech. Ed.: A.A.Sveshnikov.
PURPOSE: This book in Intended for radio engineers and technicians,,
and for students taking advanced courses in radio engineering
divisions of schools of higher education,
COVERAGE: The book deals with the statistical determInatlon of the
limit (potential) capabilities of radar systems with various types
of signals, and with theoretical problems related to the designing
of radar receivers, Basle factors determining threshold signal
Card-1/8"~-
A
Reception of Radar (Cont.)
SOV/5513
energy and the maximum accuracy of target coordinate readings In
reception against a background of stationary daussian noises are
studied. Emphasis is laid on the formulation and methods of
solving radar problems rather than on queitione of the practical
realization of the results of theoretical studies. The author
thanks V.I. Tikhonovo A.Ye."vishArin-ov,and L.S. Gutkin sho re-
viewed the book, There are 14 references; 53 Soviet (including
10 translations), 20 English, and 1 German.
TABLE OF CONTENTS:
Foreword
Ch. I. Definitions and
1. Some definitions
functions
2. Some definitions
3
Initial Relationships 7
and relationships for determined
7
and relationships for stationary
Card~:~
"VILIFTSM, Khatukell I.Ini:3eyevjf.!ti[Vil.an.,tlkyi, karid. tp~nn.
1. '.
rinuk-, FALIKOVICIIJ, Savell Yeremeyevich j~'P-jx(jvyk-h, %IA.
doktor tekhn. - na red. i nd-'V U;
VOLKOV, V.M., kand. tekhn. nauk, reZs',nze"n'~'
[.Leception of centimeter waves] Prylviannia santymet"OVYkh
klivyl I .Kyiv, Tekhxiika~ 1964, 291 1).
ZF,0-2/Z'.-IT(d)/F5S-2/FFP,-4/EZC(t)/*4-,ED-2 Pn-4/Pp-4/Pac-4/Pj-4
AH5004017 BOOK EXPLOITATION
UR/
Vilenskiy, Khatskel' Hoiseyev ich (Candidate of Technical Sciences);
Fal'kovich, Savelij:Y-8remiy-,evLch (Doctor of Technical Sciences).
Reception of centimeter wavea,(Pryytnannya santymetrovykh khvyl') Kiev,.
Vyd-va "Tekhnika", 1964. 0292 p. itlus., biblio. 700 copies
printed.
TOPIC TAGS: centimeter wave receiver, travelling wave tube, S11F
amplifier, negative feedback, tunnel diot;e amplifier, parametric
amplifier, maser, klystron, backward wave tube, receiver noise
reduction
PURPOSE AND COVERAGEt This book is intended for engineers, scien-
t i f i c. worke rs , and a tudents in adv an ce d rad i o eng ine e r in a cou rse a
in schools of higher education. The book deals with the theory.
computation, and design of receiving equipment for centimeter
radio waves. Methods of obtaining high aensL~Ivtty by reduciz.,,
random noise in the equipment and the design and construction cf
vhf receivers are em2hasLzed. Chapters 1. 111, and TV. with the
exception of section 21, were written by S. Ya. Fal'kovich;
Card 1/5
.-'3 i 6 1 -6. 5
AM5004017
Chapters 11, V, VI, VII, and sectfon 21 of Chapter IV were written
by Kh. M. Vilenslkiy.
TABLE OF CONTENTSi
Foreword -- 5
I: Sensitivity of Radio-Receiving Equipment
I . General information -7
2. Some supplementary definitions -- 10
3. Equivalent noise circuits 16
4. Antenna noise 22
5. Noise figure 28
II: Input Circuits of Centimeter Wave Receivers
6. General information -- 45
7. General methocla of computing input circuits 47
8. Intermediate (converted) frequency circuits 62
9. General characteristic of shf wave -- 69
10. Input circuitn employing coaxial and strip-type resonators
70
Card 2 /5
,L 38161-65
AM500.4017
11, Input circuits employing toroidal resonators 76
12. Input circuits with waveguide coupling stretchers 81
13. Input circuits employing wavegulde resonators with reactance
irises -- 86
14. Input circuits using wavaguLde resonators with resonance-type
irises -- 90
15. Input circuits using multichain waveguLde band-pass filters
93
16. Antenna switches for receiving centimeter waves -- 97
111. Frequency Converters
17. System of equations4nd equivalent cirdult of diode mixers--10f
18. Semiconductor diode mixers (crystal diodes) 110
19. Operating ralationships of miximr parameters 117
20. Optimum conditions for mixer operation -- 128
~IV. Super High-Frequency Amplifiers
71. Slif amplifiers based an travelling wave tubes -- 136
22 .5hf amplifiers using two-terminal networks with nagati,,,n
feedback -- 144
23. Tunnel diode amplifiers -- 152
24. rarametric amplifiers 161
ard
- 3/5
Af15 00 40 17
25. quantum (molecular) amplifiers 183
V. Uete rod yne a
26. deneral information 196
27. Heterodyne tieing a reflex klystron 197
28. Heterodyne*. using -a backuard-wave tube -- 2G1
29. Tunnel diode heterodyne 203
30. Heterodyne-mLxer coupling methods -- 206
vi. intermediate-Frequency Preamplifiers
31. General information -- 214
32. General theory of amplLfter stages -!,- 215
33. Theory and calculation of a cathode-grounded trinde amplifier
stage -- 223
34. Theory and calculation of a grid-grounded triode amplifier
stage -- 236
35. Cascade amplifier circuit 242
VII. Super High-Frequency Untte
36.deneral information -- 244
37. coaxiAl-type hf unit -- 247
38. Coaxial-strip and strip -type shf units 253
Card
4/5
L 5
AM5004017
39. Waveguide shf units 255
40. Coaxial-w aveguilde shf units 257
41. Shf unit using a balanced mixer -- 261
42. Shf unit using a travelling-wave tube 268
43. Sht unit uajug,,a parametric amplifier 274
44. Shf unit using a.Tnotecular amplifier 281
45. Method of coupling an if parametric am plifier and a frequercy
converter In ceatimeter-wave receivers -- 283
SUB CODE: BC SMITTEN "A8JuI64 MR REP SM 042
OTHER: 014
I-Card- 5 5,_
ACCESSION NR: AP4024734
5/0.109/64/009/003/0539/0545
AUTHOR: Fallkovich, 5. To.
TITLE: Noise-current correlation in tunnel-diode mixers
SOURCE: Radiotekhaika i slektronika, Y. 9, no. 3, 1964, 539-545
TOPIC TAGS: mixer, frequency mixer, diode, tunnel diode, tunnel diode mixer,
frequency converter
ABSTRACT: Hitherto, noise-current components in a tunnel diode have been
assurned to be either statistically independent or entirely correlated. The present
article trios to theoretically determine the real correlation that exists between
various frequency components of the noise current In mixer diodes. Fornuilas
are developed for the intensity and correlation of noise currents in an equivalent
circuit of a diode mixer. The application of general formulas is illustrated by a
nAcrowave-mixer equivalent circuit having a finite admittance for the receiving,
Card I /Z
ACCESSION NR: AP4OZ4?34
mirror, and internmiliate frequencies; formlas for noise-factor calculatiest are
developed. Orig. art. ham: I figuis, and 30 formul".
ASSOCIATION:
SUBMITTED: 30J&n63, DATE ACQ: IOApr64-
sun colm NO R1W SOY: 003
Cwd
ZNCL: 00
OTHER: 003
F:13-07-1'~"If,
ji.d llydilaullc stoj)-b~-3Lq)
.ti. rv,.112:40-41 D
SUDOPIATOV, A.; FALIKOVICH, Ya.; EMIMMN, A.
More attention to the freezing of fruits and berries. lhol.
tekh. 35 no.6:62-63 N-D '58. (MIRA 12:1)
Wev-Pruit. Prozen)
FALIKOYICH, Ta.
Manufacturing natursa alrups from frozen fruits and berries.
Ilholotakhe 35 no,6:63' N-D 158. (KIU 12:1)
(Xisv-Frult 4ulass, 7rosen)
KII-i-EYE"j, P.M.; LIFSHITS, G.I.; DIK, H.G.; BATRAKOV, V.I.; 'jLAVUTShIY, N.I.,
inzh.; FRID, N.Ya.; SUMPLA.'07, G.A.; iALYOVICIT, Ya.D., starshi..,
tekhriolop
Worthy welcome to the 22d Oongress of the 3PSU. Khol. teVh. 38
no.4-5-13 JI-Ag, 161. (1111.1A 15:1)
1. Direktor Moskovakogo khladokombinata No.3 (for Kireyev).
2. Glavn3nj inz~.. Moskovskogo khladokombinata No.3 (for Lifshits).
3. Glavnyv lnzh. Hoskovskoro kholodil'nika No.9 (for Uk). 4. Glavnyy
inzh. Moskovskogo kboloctil'nika No.10 (for Ratrak3v). 5. Glavnyy
inzh. Moskovskogo kholodillnika No.12 (for ~rld). 6. Direktor
Kiyevskogo kholodil'nika No.1 (for Sudoplatov).
(Refrigeration and refrigerating machinery)
;,-~re-7onki v kon'.,--tchrom proizv.?od~-,tvu. -rudy
pls!lch. prom,-rti, vy~-,- 6, 1949, n an :; v .
'SO: LCtoj-'ijI 'itatey, I:o. 1949
F-..T Yll . -
, !, I 1 ;.0.
~ 18111 FALlYWICII, Yu. Ye. 1 A. 1'.
Ochistka cti-lovogo spirta-riktifikata ot primancy.
I
Trudy Yrasnodarsk. in - ta ~Ishch. prom-sti, V~7-. 6, 1949, s.
SC: Letopis' ZhurnalInykh Statoy, 1'o. 29, 1-1-oskva, 1049
FALIKOVICH, Yu._ Ye. and MDZHOYAN, Ye. L.
"Factors In the Redistillation of Imourities in Ethyl Alcohol," Vin. SSSR,
12, No.2. 1952
FALIKOVICH, Yu.Ye.
Determining copper in wines and cognacs with the help of ion-
exchange reeins. Izv. vyo. uchob. zav.;piahch. tekh. no.3:144-
147 6c. (MIRA 14:8)
1. Krasnodarskiy
vinodeliya.
(Ion exchage
institut PSOMP Kafedra tekbnologU
resins) (Wine and wine m0ing-Analysis)
FALIKOVICH, Yu.Te.
Determination of tartaric acid in vine and wort b7 means of ion
exchange resins. Izvevy~eucheb.zav*;pi9hch*tekh. no.4:158-160 160.
(MMA 13: U)
1. ]Crasnodarskiy institut pishchervoy prowyehlonnosti. Xafedra tekh-
nologii. vinodoliya.
(Tartaric acid) (Wine and wine making--Analysis)
-iAL-1
Determining cations in pentose hydrolyzates by means of ion
exchange resins. lzv.vys.i2cheb.zav.; pishch.tekh. no.-3:3,3-36
162. O= 15:7)
1. Krasnodarskiy institut pishchevoy promyshlennosti, kafedra,
organicbeakoy Ichimil.
(Ion exchange resins) (Pentoses-Analysis)
FALIKOVICH, Yu,Ye.
Using ion exchange resins in the anlysis of pentose hydroly'ates.
Gidroliz.i lesokhim,prom. 15 no.8sl8-20 162. (MIRA 15:12)
1. Krasnodarskiy institut pishchevoy proaVahlemosti.
(Im exchange resins) (Pentoses) (Hydrolysis)
FILIXOVICH A Yu.Te.!_ Prinimali uchastiyes STANCHU, L,, student;
_----------5HUHEHJ31flAP G., studentka
Determining copper content of wine and brandy by memo of ign
exchange resins. Trudy KIPP no.22s375-378 161. (NIERA 16:4)
(Wine and winemaking-Analys~o)
(Ion exchange reslai)
FALIXOVICH Yu.Ye.
Determining tartaric acid in wine and must by means of ion
exchange resins. Trudy KIPP no.22s379-382 161. (KIRA 16:4)
(Wine and winemaking-Analysis)
(Tartaric acid) (Ion eKchange resins)
KULINEVICHS V.G.; FALIKOVICH, Yu.Ye.; PARFENTIYEVA, T.L.
Selective determining of xylite and YYlose content in their
mixture. Izv.vys.ueheb.sav.; pishch.tekh. no.ltl53-157 163.
WRA 16:3)
1. Krasnodarokiy institut pishchevoy promyshlennosti, kafedra
organicheskoy khimii.
(Hydrogenation) (Xylose)
KUL'ITEVICHi V.G.,* -TA!JkQ~~C.H,jt~,,,Ye.; PARFENTIYEVA, T.L.
Separate determining of sugars and polyatomic alcohols In
multicomponent systems. Izv. vys. ucheb. zav ; pishch. tekh.
no.6:11+7-149 163. iMIRA 17:3)
1. Krasnodarokiy politakhnichookiy inatitut, kafedra organi-
cheskoy khimii.
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04sm 1954, ffd~ 6, 6"C~-ne fluldiod citalyst is dective
W WaQving 11to heat d cmetion and ptimitting the u%e U
h4bly diApaw'd, holy friwtive uliflytts, but "Ukts;
i.-1 hie.1" C11, fAZL4OLq
bfllW fiteth. "reggth; it f,"
the highdivoupti. rate.
Mquid-phase CO l&yd:tjge=t" Is hichly wf~,Cflve low
CH. formatkX3 PtUftt-d%i -.ith LUW C-AtAySt r-I&~TtMMMg.
fkad catl,~efov-fxith a(LY Fe Catul)a. hut its Output is rf.11-
16*, Fized bed high-actMty Fe Catakyas can Give
Cwu ".ibavwfm of tho sInthesis gas in a drigle ttage
at thl,rAVISUre Ud 300 . M ',Pace VdOdUes of 2"
whimt C deptuftWu, However,
&~OWig 01 uLd catal diff"t aud the tc%np. must N,
cautrol!O closely toy"i I .
-I C de" tWu 25 rdere"es.
S/081/62/000/005/086/112
B162/B101
,VLJTHORS: Fallkovskaya, A. A., Vavul, A. Ya., Kheyfets, Ye. M.,
RaJ0T6_rF,_T.__F. _,L1a_tovq V. As, Pet y akin a, Ye. I.
TITLE: Efficiency of some molybdenum and organoaulfur compounds as
antiwear additives to lubricating materia13
PERIODICAL: Referativnyy zhurnal. Xhimiya, no- 5, 1962, 530,
abstract 5"J[224 (Sb. "Prisadki k maslam i topliva-i".
I!., Gostoptekhizdat, 1961, 71-79)
TEXT: It isEhown that the additive -15/30 (V-15/30), containinC a
complex compound of Mlo, greatly improves the antiwear properties of mineral
and synthetic lubricating materials; its action is particularly effective
when used jointly with organic compounds containing S, Cl, and other V2/3
elements. A disadvantage of the additive is its unsatisfactory thermal
stability in certain high-temperature lubricating materials. The Mo-organic
additive -15/1 (B-15/1) can be used for preliminary application of
antifriction nonoorroding films on friction surfaces; in this case,
Card 1/2
S/001/62/000/005/086/112
Efficiency of some molybdenum ... B162/B101
the efficiency of high-temperature lubrication using various lubricating
materials is greatly improved. The S-organic additive ~'-15/2/-t(V-15/2A) is
extremely effective as an antiseizing medium for high-temperature
lubricating materials. 1.5 - 3 A of it added to lubricating materials,
including those prepared on a base of Si-organic liquids, greatly improves
v capacity under conditions of high-temperature friction
their lubricating
of heavily loaded parts. Abstracter's note; Complete translation.-,'
Card 2/2
ACC NR-. AP1002569 C A, A) SOURCE CODE: UR/0413/66/000/023/0061/0062
INVENTOR: Fal'kovskaya, A. A.; Oberfel'd, M. Sh.; Kheyfets, Ya. M.; Rapoport, I. B.;
Puchkov, N. 6'.; Borovays,"'k."S.; Reznikov, V. D.
ORG: none
TITLE: Improving the antiseizure and anticorrosion properties and thermal oxidative
stability of lubricants. Class 23, No. 189109 (announced by All-Union Scientific
Research Institute for Petroleum Refining (Vsesoyuznyy nauchno-issledovatel'skiy
i institut po pererabotke nefti)]
SOURCE: Izobreteniya, promyshlennyye obraztay, tovarnyye znaki, no. 23, 1966, 61-62
TOPIC TAGS: lubricant, EP property, anticorrosion additive, thermal oxidative
Istability, xanthate additive, lubricant additive
ABSTRACT:
An Author Certificate has been issued for a method for improving the anti-
seizure (EP) and anticorrosive properties, and thermal oxidative stability
of lubricants. The method provides for the addition to the lubricants of
xanthates of the formula HDCSSR', where R and R' are higher and branched
alkyl radicals.
SUB CODE: l1/ SUBM DATE: 02Jul65/ ATD FREW: 5112
Card 1/1 UDC: 621.892.84
NAPORKO) A.G., kand.ekonom.nauk; BELENIKIY, M.N., kand.ekonom.nauk;
CILORI-IOV, P.N., dotsent; BELIKOV, S.P., kand.elconom.nauk;
K014ISSAROVA., U.N., prepodavatell; FALIKOVSKAYA, D.L., starshiy
'inzh.-akonomist
Necessary textbook on transportation economics (INconmics of
railroad transportation" by I.V. V"1. WAeftrovoll -N.&.: -
Vimichanko; G.S'-,- Raikher; E.D. Khanukov; a~d N.F. 'Chokhlov.
Reviewed by A.G. Naporko and others). Zhol.dor.transp. 43 no.S:
95-96 Ag 161. (MIEUt 14:8)
1. Zaveduyushchiy kafedroy "Ekonomika transportall Tashkentskogo
inatituta inzhenerwo zheleznodorozhnogo transporta (for Belentkiy).
2. Kafedra "Ekonomika transporta" Tashkentskogo instituta
inzhenerov zheleznodorozhnogo tram orta (for Chernov)'
(Railroads) (B~lov, I .V.5 (Borovol,'N.E.)
Vinnicbenko.. N.G.) (Raikher, G.S.)
amikov,, E.D.) (Khokhlov.. N.F.)
C
. - I -,~ - -i-- - -7 --
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~ ~ - -,-- ~ 11 - -
I J.: 11, / FATLIEC1,311'r,'AlA. TS. :'. FI-111211enjyD -,-jjjjjostijjLjj-
ramn-,.;~Lo vozrasta. Vrach~)Ib. R,,Jo, 111.4r), 1170. "', STD. 711-IL.2.
s C: L-AoPiss `10, 32, 19119,
a
'60
,
WON
,
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-
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00 Now do I up 6t Wqai~~- 11. G
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400
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4000
400
600
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Soo
ANDROSGV V.V.; FALIKOVSKAY-I,-K.V,.
.4 A
Improved method of fastening ties with screws. Pat' i put.khoz. 5
no,,4:12-13 Ap 161. (MIRL 14s7)
I* Zamestitell nachalinika Kishinevokoy Aiotantoii puti Moldavokoy
dorogi. (for Androsov)e 2e Starohiy inz"r stantaii Kishinev.,
Moldavokoy dorogi (for Fallkovskaya).
(Railroads-Ties)
GOIAS, I.; SOKOLOV. V.; W~�~-L
lw..
Liquidate water looses in domestic water pipe systeme. Zhil.-kom.
khos. 4 no.2:16-17 '54. (MIRA 7 - 3)
Oster pipes)
FALIKOVSKAYA, L. A.
Fallkovskays, L. A. - "The electrochemical protection of iron in water of various
compositions In the presence of Wdbitors," (Authors: Rosenberg, M. A., W'-
havskaya. L A.9 Pogorellakly, To. 1. and Yurkovskaya, F. B.) Nauch. zapiski.
(Dnepropetr. gos. un-t), Vol XXXr3:I, 1948. p. 19-31, - Bibliog: 15 items
SO: U-5240, 17, Dec. 53, (Intopis 'Zhurnal Inykh Statey, No. 25, 1949).
FAL KOV S KAffl, . .
. . ..
'7 -T-5r .
7
Coagulation of natural wstm. it. Kf. A'. Wiiz&~ L
NIR
ll
i
?
S
k
k
N
P
awa
ovs
a
rs a, stud
.
.Yur
aylk.
OUIA.ZOA
..
- 1. 43. 17-21(IOW); Rofto,41. Zkur. Kkins.
10.
1954. 140. M
cf. Sborxik Raba K41w. FdWela Dxepro-
.
pefrovsk. Uaiv' 37 9(195t).-Tht putpom of this Invivid.
11
l
i
h
4
1
nuts
ous com
t
e prom amt. of var
Won was to
or be remoyal o( suspcoded mattcr from satne naturul
vinitm, The tfIrttIvtntM Of coagulants was judged froin
their clearl"g effect and theaWlityi)(the waterto formscale,
l
C
l
I
I
ed w
M
"ArY 11OCIA-1111102 010(ttliftlif Of the walcr
oup
th PM
the optimal Concn. of lre'04.7140 for wnter from the rivtr
r
os. 000 mff.11. ituspended matter was
samara eoutc. apg
I
80ji'lliffso for watcr frow the riyer
76 juK.11. and of 12(.
l
Vokh,ya
uutg, nIxvut 450 mil./l. suspended mWer wax A)
~
mg.A. ItAfth acted tdinuitancously cut a "Itener avid a
Us olvilitud conen. for DoelmopetmA city
water C41111j. 2110 mg./I. purpowly ndtItil Laolln w-.tA IfX)-
L
USSR/Microbiology Sanitary Microbiology. F-3
Abs Jour : Ref Zhur - Biologiya, No 7, 1957, 26322
Author : Fal'kovskaya, L.N.
Inst : - I-*---
Title : Decontamination of Drinking Water by Ultrasonic
Vibrations.
Orig Pub : Gigiena i sanitariya, 1956, No i, 1i-14
Abst : A study was made of the bactericidal effect of ultraso-
nic vibrations, produced by a magnetostriction generator
at a frequency of 46 thousand vibrations per second.
Tests were conducted with stream water, artificially
por.uted with Bacterium coli, Bact. aerogenes and spores
of Bacillus subtilis. The bactericidal effect was increa-
sed sharply when intensity of exposure to sound wa i r -
ased from 0.7 to 1.2 and, particularly, to /1.8 c , and
attains 99 - 99.8% for Bact. coli and B. subtilis. Most
of the bacteria perish within 2 to 5 seconds of exposure
Card 1/3
USSR/Aicrobiology - Sanitary Microbiology. F-3
Abs J:)ur Ref Zhur - Biologiya, No 7, 1957, 26322
to sound of a layer of water up to 10 cm deep, and tur-
bidity up to 50 mg/liter dies not affect the operation.
The relation between bactericidal effect and intensity
of exposure to sound may be expressed for intensities
within the 0-3 - 1.2 watts/cm? range by means of the
formula N e-1-4x, where N is the number of bacteria
N0
after exposure, No is the number prior to exposure, x
is ultrasonic intensity in watts/cm:2, and e is the ba-
sis of natural logarithms, equal to 2.71. At an inten-
sity above 1.2 watts/cm:2, bacteria perish at a more ra-
pid rate, which my be derived from the relation
N 0.6 0.33x. At a rate of flow of the water from
No
Card 2/3
'USSR/Microbiology - Sanitary MIcrobiology. F-3
Abs Jour : Ref Zhur - Biologiya, 110 7, 1957, 26322
i to 10 cm per second) a similar effect is obtained
from exposure -to sound. The author believes that
the effectiveness of exposure to ultrasonic vibra-
tions of an intensity of 2 watts/cm? at a frequency
of 46 thousand oscillations per second is higher than
that of chlorine in decontamination.
Card 3/3
SHUBERT, B,2,'P:&MLIYAO A.M.; RUIZHIIISKIY, V.I.; SID=O, T.X.; AIMMA OVO
D.N.; SOKOUWo V.Y,g JAL'KOV8KAYAj__L,N.j BRUK-LEVINSON, T.Lq;
BELYAKOYA, A.N.; AVEUSHCHWO, R.A., red,
Isd-va; TOIKOF, S.Te, tokhn,red,
[Water purification for water supply to mmichins-tractor stations
and state farm] Ochistim vody dlia vodoonabzhentis poselkow
NTS i movkhosov. Xoskvag Izd-vo X-va komun.khos. RSM, 1957*
69 P. (MIRA 11:6)
1. Aimdentys komucallnogo khozymystys. Moscow.
(We ter-Purif tea t ion) (Water emply, Rural)
F VI L , K 0 ; -, Y~ - ~ '" , I- , V-` -
GORIN, G.S.! FALIKOVS
to
The water supply of Berlit. Vod.i san.tekh. no-9:31-36 S '57.
(MIRA 10: 11)
(Berlin--Water supply)
MIKOVSKATA, L., kand. takhn. nauk.
- . ~ 1 "-1- - 1. " I .. . .
Water supply In citles of the Gernma Democratic Republic. Zhil.-
kom. khos. 8 no.11:29-30 158. (MIRA 11:12)
(Gersanyg 11ast-Vater-supply engineering)
FAVIONSUY"NA-,
Ultrasonic dIsInfOOtIOn of water@ Vod* I *an, tekh. noel2t8-10
9 138. (mim n.-12)
(Ultrasonic Vg'v*�-PhYGiOlOglc&l effect) (Water--Disinfection)
GODES, I.G., kand. tekhn. nauk; FALKGVSKAYA'J.V,,, kand. tekhn.
nauk; BOIDTINA, A.V.p reT.-Tz_d_-va; K1040KH, E.M.0 tekhn. red.
[Using equipment developed by other branches of the national
economy for temporary water supply] Ispolizovanie tekhniki na-
rodnogo khoziaistva dlia vromennogo vodosnabzheniia. Moskva,
Izd-vo M-va koumun. khoz. RSFSR. 1961. 46 p. (MIRA 15:7)
1. Akademiya kowa-unallnogo khozyaystva.
(Water-supply engineering)
FALIKOVSKAYAP, L.N.
Water oupply In the U.S.A. Nauch. trudy AKKH no,22.,J 163.
L 44554-65
AM5012694 -BOOK- EXPLOITATION UIV,
iFallkovskap, mdmila
Organizing water supply for inhabited localitiest which have suf fered from mass
destruction weapons (Organizatsiya vodosnabzhenija nwelennykh punktov, postradav-
e10-1th ot oruzhiya n-assovogo porachaniya) Moscow, Stroyizdat, 1964. 55 P. illun-,'
biblio. 10,000 copies printed.
TOPIC TAGS: nuclear weapon, HW &gout., CW agent, water supply eyetemo water pol- i
lution, water purification, water sanitation
iPURPOSE AND GOVERAGEt Problems of the effect of mass destruction weapons on
water supply systems of pupulated areas are elucidated in this brochure, The
nature of the disruption of this system in brought out and recommendations are
given for the organization of water supply in stricken cities. The brochu-re is
intended for engineers and- vorke=-Iu-the vater-eupply field and also for a wide
circle of DOSAAF active memberG4-.-
TABLE OF OONTEYM:
introduction - - 3
-L 44554-65
AM5012694
Ch. I. Contemporary means of was destruction
Nuclear weapons 5
Chemical weapons 9
Bacteriological weapons 10
Ch. II. Preparation of a water supply system to operate in the case of use of mass
destruction means
Cities water supply lines 14
Settlements and village populated-areas water supply lines 26
Ch. III. Restoration and organization of the.water supply of a stricken city
Restoration of installations and water supply lines - - 32
Decontamination of water supply installations and purification of water 46
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ISLAIM 'EMBLI01 T~APFI CAL RI~POPT AID 48Q-I
BOO',- Cttll TJ12-~:0.1;55
Authors: LYUB!VUPvOV, V. N. , VASTLI'M, E. FA--IKIVSKIY. B. I.
'7u11 Title: A13PAWl"! TOOL5 AND '*-r-,IP A", U-77,
T
I MAIMF
Tr-,~nslitorrtnd Title: Abre7lvnyye Instrii-fnty i ikh lz,;-otovleniyol
POLI SHING' -)ATA
Origi'natlIng A,,vnimy: Ilona
Pulblishing Hou!;e: Stpte Sciont!"'ic nni Techninpl Publishing Fvms~~ of
Machilne-Building PM Shipbuilding Literetura
Br.- nch
Dpte: 'Lc)5-1 No- PP-: -176 No. of CoPies: 5,000
7,1itorivi Stpff
'741. 1 t or :Chlstypkov, A. P.,Engincer
Anrrpisnr; Aiv~,-ustinik, A. I., Prof., Dr. of Tech- Sci.
PtR?^S-": Anv-)rive,l b.-f th-i ScIrool Arlminintrption ill th, Miniitr,~r of
Bu!ldin- P.-, E- for technir-el )f 'n
-r.1 -P~!~Inc, "llil,; wirk crn be v1so uspd ra F reffl-mr!-i !')-)k
by enidne-rs, tec1-n1-i,-ns Pni s-pcinli-ln7 in V~s nr,)i,~ctlon of
Pbrasi-iq.
T7,T-- ')ATA
(bir Vp.,zillyev) rl-ncribes 1-7r*,n;1'-nT ml rolshin-
vnrl brslc of nrturr.-I 1-:11
112
Abrazivnyyo instrumenty i ikh izgotovleniye AID 469
artificial abrasive materials,, as well as abrasive tools, pastes,
emery cloths,, sandpapers,, etc.,, with their nomenclature. Part II
(by V. N. Iyubomudrov and B. I. Fallkovskly) discusses the tech-
nology of the manufacture of abrasive tools with the use of ceramic,
magnesia., silicate, vulcanite and bakelite bonds. Special attention
is given to ceramic bonding materials because they are widely used
and their processing, particularly their heat treatment, is more
ccmplicated. The book is provided with illfistrations, tablos and
diagrams.
No. of References: 49 (1931-1952)
Facilitiess Not given
2/2
DASHEVSKIY, Wye. Isaakovich; ZASLAVSKIY, Simon Shlemovich;
FALIKOVSKIY, B.L., inzh., retsenzent; PILIPE31KO, Yu.P.,
-I-n-zF.-,, -red.; GORNOSTAYPOLISKAYA, M.S., tekhn. red.
[Mechanization of the manufacture of metalworking and forg-
ing dies] Mekhanizatsiia izgotovleniia shtampov i press-form.
Moskva, Hashgiz, 1962 172 p. (MIRA .15:8)
(Dies (Metalworking))
FALIKOVSKIYO G., inzh.
Centralized transportation of ammonia water. Avt. transp. 43
no.12:13-14 D 165. (FIRA 18:12)
1. Ministerstvo avtotransporta i shosueynykh dorog Litovskoy SSR.
KOVANOV, V.V.,- PAVLENKO, S.M.: MEDELYANOVSKIYp A.N.;
BOGDANOVA, Ye.V.,- KIULE7pO.I.; KHILIKIN, A.M.; FALIAUV841Y,
GaA.
Method of phasic control of the blood circulation. Trudy po
nov. app. i metodno.1:86-92 163 (MIM 16:12)
M IKOVSKIT,,,,G.B.; WSNOVA, A.Te.
Comparative evaluation of valrous methods of placing a circular
vascular suture. Bkoper.khir. 4 no.5tl2-16 S-0 159. (MM 13:1)
1. Is irafedry topografichookoy anatocii I operativnoy khirurgit
(sav. - Prof. V.V. Kovanov) I Moskovskogo ordena Lenins zeditainekogo
Inatituta Imenl I.M. Sechenowa.
(BLOOD TBSMS. surg. )
FALIKOVSKIY, G.E.
Changes in hemodynamico following the exclusion of various
quantities of pulmonary tissue. Blul. eksp. biol. i med.
59 no.41l9-22 Ap 165. (MIRA 18:5)
1. Kafedra operativnoy khirurgii i topograficheskoy anatomii
(zav. - deystvetelinyy chlen AMN SSSR prof. V.V. Kovanov) T
Mookovskogo ordens, Lenina meditsinakogo instituta iwni Sr.-
chenova.
r.-. -1 1- :y I
. [I , ~. ~.
Tile placinF. organization and control of the -r,,,In,l oroce55 n . L;-~,,( i:,,illls of standard
t, .
construe tion "oskva Gjizle.~Iprom, 1--jV. 50 ~).
(Bibli,;tc&,ka te..stiL'Shchika) (5h-22219)
S3,2 5 3 - 1`3
M
1. FALIKOVSKIY, I. M.
2. USSR (600)
4. Peat
7. Effect of air parameters on the drying process of peat. Torf. prome,
29 no. 12, 1952.
9. Monthly List of Russian Accessions, Library of Congress, Marc 1953.
VnclassifrR.- -
IALIKOVS Noisayevich; LTKOV, A.Y., laureat Stalinskoy premil,
---'doktor reteensent; KHOKUTSKIT, N.D.. kandidat
tekhnicheskikh nauk, dotsent; SOKOWYA, T.Te., redaktor; IL'IrIM,
II.K.. takhnichookly redaktor.
[Drying and wetting bast fiber nateri&lsl Sushka, i uvlashnonie lubo-
voloknistykh materialov. Isd. 2-s, perer. i dop. Moskva. Gos. nauch-
no-tekhn. Isd-vo Kinisteretva, prow/shl. tovaroy shirokogo potreb-
lenita SSSI, 1954. 410 p. [Niorofilm] (KLRL 8:2)
(Bast) (Drying apparatus)
89220
S/05 61/040/001/026/037
44 2 ~Xo 7 2-/ 1.3 ?-5) B102YB212
AUTHORS: Abrikosov, A. A.9
TITLE: Raman scattering of light in superconductors
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 40,
no. 1 , 1961 , 262-270
TEXT: A study of the behavior of a superconductor allows many conclusions
as to its energy spectrum. The existence of a gap&in the energy spectrum
brings about an effect that at T-0 a radiation with a frequency smaller
than the threshold frequency 2A is not absorbed. Besides such experiments
with varied frequencies, M. S. Khaykin and V. P. Bykov have carried out
other experiments in order to determine the electron spectrum with the
help of Raman scattering of light in superconductors. At a sufficiently
high intensity,it should be possible to measure the distribution of astel-
lite frequencies spectroscopically. The main problem of such experiments
is that scattering is extremely small in connection with the fact that due
to the skin effect the light will only penetrate about 1o-5 cm into a body.
No satellite lines have been observed by Khaykin and Bykov; now the ques-
Card 1/6
89220
S/05 61/040/001/026/037
Raman scattering of B102YB212
tion comes up, how much the sensitivity has to be increased in order to
perform such an experiment successfully and how would such an effect look
like. To find out this was the aim of the present work.. The authors tried
to determine the frequency and angular distribution of a plane surface of
a superconductor, filling a serNkspace z>O at T.O. For simplicity the
incident and reflected waves wermik assumed to form only small angles with
the surface normal (sin2 g, sini~gNtIF-1;F-denotes the complex dielectric
constant). For most metals161-10. -Furthermore, the radiation frequency
was assumed to fall in the optical region. Since the absorption probabil-
ity of a quantum is B-(C.J,-rL, ) -~JS j0 12, it is possible to concentrate the
problem to determining the elements Sio of the scattering matrix, which
describe the transition from the ground state to the J-th state for elec-
trons of the outer field,A 2+At. (The incident wave produces a field in thD
metal which is characterized y the vector potential A 2) . The elements of
the S-matrix are determined by a method using quantum field theory, as
outlined by L. P. Gorikov (also A. A. Abrikonov and GorIkov, Ref- 4)-
Several eligible graph re examined, and it is found that only graphs of
the type are of interest. This expression is found for
Card 2/6 Y.
89220
B10561611040100110261037
Raman scattering of 3102/B212
the corresponding matrix element:-'it
5 = -ifd x, and the total bility
0
2
for all possible processes is given by
e4
A.' (A, (x) A' (x))
+
(X)'*p (x)> dxd;.
X. (X) (2)
For'
an..inf inite superconductor relation
.
d'P
(X)
(2ar
+
+ (XD 6.01 u2,8 (e e,) epje_,.) dip (3)
*0
W
., a . .. .
,
l
pw-x)
> .A UPUP8 e
W) *0 W e 5P)
UPVP8 (e + Pep) e'P(K-je)-dIP
(X) (X)>
T
(2x
so I/Elp + A2. EP V 0 P I -PO),
Card 3 UP, + to so), VIP (I to sp);
Q
89220
_2
S/056/61/040/001/026/037
Raman s'cattering of
BI02/B212
~hclds; I ap is an antieymme tric two-row unit matrix. The following expresslai
is then obtained: 2' e
PS JOI tGfR(q,)f(~)dq, (9- purface area)i
2m
and aftersome, intermediate calculations
one finds:
2 ~
opo iijo +A)E[qo-2A~ q 'A "'o- 2,6
f( 0
2 2141 K I where E and K are the
n v . q, L2 ~qo+M) q 0/2 ~q 0 +22
cOmPlete elliPtic'integrale, and
(q.) 8 A.r A; C0911 co +
I ~(n + cos. 6)' 4- 91110 COS 0 1), + X9
'in 4p
+
sin$ ip
cop 0, 1
Tn + Cos 0). + X.1 I(n cos 01 + W +
MIT
(q$.+ 4x20)2)2
Card 4
89220
S/056/61/040/001/026/037
Raman scattering of B102/B212
The reflection coefficient ddl'which' is'defiried as the fraction of energy
hitting the superconductor surface that is reflected in the angular inter-
val d4'11 and in the frequency interval dcjf is obtained as
2X4 Cos 0 Coss 0
do= r - -
n 7.r.,-11(!+.COOQ)(n"+X',+I)+,4n,~cosoix
X [(I cos' V) (n' + k3 _~ 1) + 4n cos O'l + sint 0 sin' O'co3 2(f (nl + xvX
X [(n cos 0 + 1)2 + X, Cos, 0] f(n Cos 0' + I)$ + X9 Coss O'l 1(n + Cos 0), + XI] X
Xf(n + cos o,), + w w,
L=2 co + 2A)
2 (ca W) A
/W - (0, - 2AN
K In 2xw da'd Q.
+2A
The'
value.for Nb is
dcl M-io- 12 P dUd,,~1/2b; P-1. It was thu's found that in order to be able
to observe such an effect, the sensitivity has to be at least 1o5 times
higher than in experiments of Khaykin and Bykov. Finally, the authors
thank Acgdemician L. D. Landau and M. S. Khaykin for'discussions, There
are 6 figures and 5 references: 4 Soviet-bloc.
Card 5/6
".. ,,.I
5/0~~/'2/043/00_' 52/063
:1310 4/3 102
U 0 5 11*.)rAosov, A. A., Fallkovskiy, L, A. -
T I 'T L 04, f!I(,,CtrOII Crjf.,r(.-,.y .3poclrui, for metals of the bimuth
t,.v p U
'I u:; i '~,,Ovu t' cis-;,`fzik v,
P 71-RIOD! C!~L: rnal 4,K s i, r!rI.T.,m tal
no. ,(q), 1962, 105()-1101
Ar~~-,nic, antimony anj b~ uth cave rhom',.oh-,iral lat"Ices 'ormed when
on
t o sublaltic&3 of a cubic lattice are m,;tuall,-, d-isplaced
~i-_6onal of the culb":. th.:. elf"C'ror, C~ectvumm IS
calculat.~I,i f~r a lattice dlfferin6 ~rr,,m ctJic. 2hen this
lattice -'is _4f.form.A so as to cause mutual di~,plzic-jment of the Iwo sublatt4c_,,_,,.
ahv ri 1~_-ement results in the metal undereoine; a transition of tht:
second Ajnd aht~reby the lattice constant is dc)-.-.bled. of carriers
diudnishes. The effect of such a deformation oa the -_-~Iectrozn ene rgy
spectrum is investigated, JeadinC to the formwila
E. -LI d I Q I vQ'I - T-23
Ca~d i ,/, -.63"o
7
c: /c, 5 6 2,'0 /0 0 /0 2 /0 6
Theory of tilectron ereriy npectrum. . . D 1 V4 J I U,~
L2 lit 0%
1 1
d
-
_.
11
It Q
Q
7
,
1
it
whure f !Ire the q n va 1 u e s t a tr i x
Dw
+ aw, + A 0
~~ Y 1)
i
2
A
0 bx-+O- bx. + ri .
/-Faxz+A
bx_+A_ bl'-tAL
b. -+A - bw~ + lq~
- A
+ ax
,
V7
caril 2P
4- 0
Y -j A- b.
)f.T
L)
_i ,6 62/043/003/052/0630
Theory ul' Iuctron energy spectrum... B 104%4
B102
f ~ vu, + ~w, T = cu,, eu� = e (u. � iu,), 6� ='du.,. (7),
L - bK. K is a quantity of the order of t1'.e inverse lattice parazeter,
is the dt-,formatior- vector, uik is the le.Ccrmatior, tensor. There are
5 figures and 1 table.
L 'S30CL.TTON: Institut fizichoskikh problem Akademii nauk SSSR (In-3titute
of Physical Problems of the Acadernj of Sciences USSRY
SUBI",ITT---D: April 23, 1962
Card 3 3
ANDREYEVO A.F,; FALIKOVSKIY, L.A.
All-Union~Conference on Low Temperature Research. Vest. AN
SSSR 33 no.1009-100 0 063. (KMA 16:11)
L 13637-63-
-SIO05616310"100611 93s/
-ACCESSION NR: AP3003123
AUTHOR: Fal kovskiy, L. As'
Theory of electron spedm1of biamuth-type metal a in a magnetic field
!SOURCE: Zhurnal ekaper,.1 teor,-flzW; ve noo 6j, 1961 1935-1940
blmmth-typa metal, g-factor., spin-orbit couplingj,
IOPIC TAGS: eleevon spectrum.
amagnetic level-
'ABSTRACT: The'enerayspectrum of,holes ahd electrons of bismutb,-type metals in a
:magnetic field is considered by starting with iesults previously obtained by the
-author and A. A. Abrikosov. (ZhVTF. vo 43, 1089 and 1083, 1962) in the absence of a
magnetic field, The analysis is devoted essentially to the determination of the
g-factor. The paremaguetic. addl 'on to the energy lo calculated in the quasi-.
'classical. apprmtimation, and is characterized by a g-factor that depends on the
quasi-momentum. It is shown that thia*deperidence is brought about by the noti.e-
able spin-orbit, coupling*, The symmetry of the g-factor is determined by the
SYMMetry of the Fermijurface. The calculation of the diamagnetic levels is
carried through to conclusion.only for holes and for the case when the mm,,gietic
field is paxvllel to the tx1gonal axis of -the crystal. Comparison with experiment
is limited by the experimental accuracy. "In conclusion, I want to e3qpresa my
bard 1/2