SCIENTIFIC ABSTRACT KUBAREV, A. - KUBAREV, V. I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000827010012-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 13, 2001
• Sequence Number: 12
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

-- - - - -- - -- - - -- -- - - - -- --
KUL"ARLV, Aley-w-vir
;11~~,,--~ ~n
Pressure conditions in pipe Vodni hosp 13 no.5:188-
191 163.
1. Hydroprojakt, PrahA.

--WNA'YEV-1---P G-FS--t- -kandtekbnnauk; -RUBAREV,- A'-I - s -inz
Methods for calculating dimension dieframe having the ck . and JKI
coefficients given by two limiting values. Vest.mash. no.91
313-37 9 '619 (KM 141g)
(Mechanical engineering)

ZIIUR'&'EVp V*O,l XUBAMN, AI,; USAN, M,V~
netemination of the zones of tolerance for 'the ajuatwnt of
mAohine tools# Priborostroonis no#2201-24 D 164.
(MIRA ISO)

KUBAREV, A.I.; USAN, M.V.j ZHUM;EVI V.G.
Organization of a preventive statistical control. Standarti-
zatalia 28 no.608-42 Je 164. (MIRA 17s9)
i~
t".
f
I
I

USAN, M.V.; Zliuftrav, V.G.; KURAREV, A.I.
-- ",- ,,
A
Effect of some technological factors on the operat!ng pr"Malon
of automatic lathes for longitudinal fz)rzm Ftar.. I instr.
35 no.1019-10 0 164. (K'RA 17,,12;'

KUBAREV, AJ
Determining the cost of an article In case of a change in its
productioi schedule. Standartizataiia 29 no.106-39 Ja 165.
(MIRA 18s4)
1. Vaesoyuznyy nauchncN-isoledovateltakiy institut po normalizatsii
v mashinostroyenii.

VMM=t V*Rkl UWWo A*I,
. , ".- . .... .....
14&tbanttftl 4oMco amd stsawdimuct6 auudartiateila
29 no.7tl&46 n 16~,-.- (mntA issn)

(A ) L 1876-66
ACC NR, AP50287" -1 - W - SOURCE COrE1 UP/0029/65/00OAKY7/0014/0016
q 1-L -) 5 1-) L) 5 5
AUTHORSs Verchenko, V, RO; KubaxvYv A. 1.
I J,
ORGI none
TITIZs' Mathematical statietice and standardization
SOURCEs Standartixatmiyal, no. 7# 1965t 34-16
TOPIC TAGSs scientific standard# statiatIc analysis, mchins industry. data
ampling, quality control t4' Vql -
AMTRACTS The Importance or statistIca !E!jn1* In standardization efforts is
qualitatively d1mousaad, 40 an appe*2 Is =de t* standardlxe statistical analysis
matliods and to wqxvA their vae In govornment atandards. Several areas which will
benefit from statistical analple n Usted, At pmantg mahim pwt
dimensions a" specified with tolmran=*"Mich aeame all compnwits to be at the
worst maxim or minimm &OSIVIS cm NhOw that It 10 M7
irp,dbable that &U oomponauts will have Um vorst arror, and thus tolerances can
be relaz*4 so as to pradwo mjar machining coat tmv1W. The fields of quality 14
control, rellAbilityp and meahl Life prediction wat =9 statistical am-Ijis-
U-clffialn meaningful reaultse It Is suggeated that standards and. wrking tables bs
established for sam3l tochaliquas In quality control, These should Include
single mawling (am mange at a out of 3 PU)t 6mble saspling (two Molest rk,
and p2, taken succeselvely out of 9 parts), and smaseelve samll (successive

L 11876-66
^161. NMI
AP50287"
testIng Of 10 2t 3 -- i P&ris) tsehftiqU68- C*ntinuoug statistical control of
industrial processes can be profitabLy applied until these techniques are replaced
bY aut0mt1* ccfttrol (uhich can maso benefit from statistical aw3jMig). The
problem of specifyim rellabIlIty, fat%w, and We parsintare In astchins, pdrts
aO,asaemblise mwt be considered from a statistical standpoint to bo mania".
is In the prooosa of developlagl, stanlardIsiogI, and publicixin nw1ow
-SU-HoUcal techniques for these Purposes.
SUB 00M 14,13 / BUSH DMI wA

\ /'~i I
J L
ACC NRi
SOMAGE COM UR/0o28A5/0W/0M/0O3)/0036
AP502874&C(m) -t
AMORSI hu~akov,, K. Po Kubarev IA. To
ORG i VIIIINHASh
TITLB: Aocolerated dotermination of rollability and 1 fe of machine parts j
SOURCE; Standartizatolymp no. 7j 19650 3)-)6
TOPIC TAGSi endurance tent machine industry, fat.'Lgue toot, reliability engineerin4
static load test, mechanic~i stress
ABSTRACT: Differeit methods for accelerated life and reliability testing are
discussed qun1JtRtivPjy, Simon 4ev. -'"Wt ;=atticil tz, Lm--
-vu. Q.%;0*Z0
mine the reliability and wear characteristics of a given machine,accelerated tests
must be performed which will give sufficient data in 3 to 6 weeks to predict the
long-term behavior of machine elements. This can be achieved by either inereafiing
the number of cycles per unit time, by intensifying the loads, or by both methodso
It has been shown repeatedly that wear processes and ratigue processes can be
extrapolated froni limited test data with an accuracy of + 1%. Although under
industrial conditions the scatter may be as much as + 150%, these extrapolation
techniques g1ve an excellent indication of average wear, life, and reliability,
When fati ~i ife4Jmltlng factor, the fatigue limit can be established by
everal increa~ &dad methods, much an a constant load increase to destruction,
:
tepuino "Load Increase to destruction, or cyclically increasing loads. Each or
LSS~d 1/2

L 12019-&
AP5029745
0
those methods has advantages for certain applications, Determining the fatigue
limit by the critical stress method In of particular interest, This method depends
on the energy hypothesis of fatigue, by vhich it has been established that the cy-
clio constant and the critical amber of cycles are constant for a given type of
metal, No specifio recomendations are made, &W the article represents a very
general, qualitative dimoussion,
SUB COIE 3 14/ SUBM DM I none

_307 &4
s/j4i/6,i/oo4/OO3/Ol5/O2O
IL ry,6 (// V, to) E I) 2/r.3 N
AUTHORS: Bespalov. V.I., Kubarev., A.M. and ScAcv-'.yev*A L.I.
TITLE: Experimental 1nv-e*tlgation of tht izifluen,;s of non-
homogeneities on the chard~Aer.iAttcq of moms delay
systems
PZRIODICAL: Izvestiya vysahikh uchebtiykh zavedeoiy~..
Pp. 534 .. 546
Radloflzika, v. 4, no. 3 1961 ,
TLXT i A theor *tiesl. investigat 10ti of t he I nf luenc e of ~non-
homog!uneities on the characteristits of d4l,)y _4VOLeMb has been
rep6rfed in Refs .1 (Rsdiotekhnika i tielitronika 1956. J~ 772)
and Refs 2 (Dokle Akennuk; 117, 209~ 195?1, The analyals was
carried out under the assumption UW tl)a indilrielusl cells of
the system could be described by mean~i of idealised quadripoles.
However, since such a description Is spliroxtmatt it to of
intersot to verify It experimentally. Consequontly. an experi-
mental investigation of the following t~lpes of delay lines was
undertakens Interdigital delay systems, metal-plate (cembfttypi
structures and chain& consisting of A number of resonators.
The interdigital system with two bave AxLrfacr-4 16 illustrated
Card 11~f ~

11764
5/11,1/il/004/003/015/020
Experimental investigation 9192/9382
in Fig. 1. The equivalent quadripol-e of a cell. separated by
sections AAI and BBI is also sho-n in the figure, The
matrix of this system is (Ref. 4 - A. Bloch, P.J. Fisher and
G.J. Hunt - Proc. IZE, 100, 64, 1931.),
z
cos(kb + --Cos(k~~ - (IcTzf -j t nIt/,)
V
A j sinjkt) (kt)
o'
JOC T cos(ke) Cos W&I
z
where w is the operating fr-equencyv
k w r;7 -,
t, in the length of the line qev~tlons`
Card 2/~~ ~~

4
s''.4--/Woo4/003/013/020
Experimental investigation
I/Z' = I/ZI IN
ZI v-r'P-/CI
z 1 4 C j
z j 76/' C0 are wave Impedanc*-s of the l1nes
formed by a stub and the lower base :iiirface a tktub and upper
base and by two neighbouring attibe respP:.tIv#IY,
C1, Cj and C 0 are the correbpi-,nding capac.itances per
unit I.engtbi
CTis the capacity between the end of a stub
and the bass;, of th6 opposite comb structures
The scattering equation for a chain corimi,.Riing of such
quadripoles in &I-ven by-,
Card 31~0;

S/14.1/61/004/003/015/020
Experimental investigation E192/L,382
A 4 A z
Cos ~0 22 Wr-TZ I g(k,!)l (1.2)
2
where yo is the phass of the wau*n. The %,.,att6r1ng character-
istica were taken experimentally by ij,.4ing two d6mountable inter-
digital structure,%. of -~Im;lar elanients. The system
was designed for operation at derimetre waves and had the
following dlmenqioDm~ period of th,~ D -. .10 mm:
diameter of a stub ; ~ 7-mmi length of a 6tub -~ , 90 mmj
the gap between the atubs h :: 2 mm-A-tA,.,qtdnce between the base
and the stub S could bevaried front 0 to 15 mm The measured
results are Illustrated In Fig. 3 (mmall together with
the calculated curves (solid lineoi). Single dim:ontuftuitles
in the system were produced by using Aipe,-iat calls in which the
position of a stub could be varied Th#- theoret.i--al v'alue of
the modulus of the r6flectLon cooffi,:tt-nT cloje to various types
of discontilluity can be found (row fornitl1ae gi.ven in Ref. 1.
Card 4 ~~/

~~;/14:41/004/003/015/020
Experimental investigation
Experimentally, the following types of di!- critinuLty were
investigatedi displacement or the i-3tub in the wrans-erse
direction (g changes by Ag), changeq ~.n the gap between the
stubsi displacement of the stub in tb-z plans.- of the structure
and changes of the length t of the -4tub, The value of the
reflection coefficient Irl . a funrtiot) of "..%/D 3.9 Illustrated
in Fig. 4, together with the calculated .lirvoq. Comparison of
the calculated and theoretical results~ %bowt, that if the
reflection coofficLent produced by the di,ocontinutties Is am 11,
this value can be found as a superpof3it.ic,n of the reflettion
coefficients due to Individual discontinaltie!v, The equival:nt
circuit of a metal -plat e(comb-type) struct,ire is i.n the form of
a chain of V -type quadr.lpoles, whose mair i~- or ar is In the forms
j Z t g (k-0)
-JAI = 1 (2.1)
JWC I - W CZ"' t g (k
Card 5

1~ 1 " " t~u
S/ 41/6i/oo4/003/015/020
Experimental investigation Piga/r382
where k r w R1, $
z is the wave impedance of the strip lAne formed
by the neighbouring platem jnd
in the height Of the PlateA
C is the capacitance between thi. t%nd of a plate and
the covet-,
The phase changes of the wave over a c01 ..are described by:
Cos to 0 a: I - w CZ tg(kfl/2
(2.2)
The experimental system investigated consitated of two metal
surfaces, one of which carried a number of' cquidistantly-spaced
metal slabs (paralleloptpeds) having d1mrnslons d -- '7.2 cm..
3 0 1*7 cm and ( t- 9.0 cm. The upper .9urfar-t of the ~aystem was
Parallel to the lower surface and itA distance from the metal.
slabs could be varied. The non-homogenejjtie!~ in the system were
produced by filling the gaps with m,!,tal platAzt Inserting pieces
of metal undor individual slabiq or rhtriFing the apar.,Lng between
the slabs. The results of the exp!~ m(-Tt,.ta art illustrated In
4t
Card 6/?~

3 %4
s/iiji/6.1/004/003/015/020
Experimental Inve,4tigation F 1 1.) 2 / 93 82
three figures, In part.1cul-%r*Fig. AO ,3how-A !he value of the
reflection coefficient as a function c)f the change of the
distance between two neighbouring The straight lines
of Fig. 10 were banod on calculation4 while the circles show
the experimenta.1 pointe. From these rxperiments, It is seen
that for small inhomogeneitlee, lh,,~ ai~r-vment between experiment
and approximate (aiculated results im )4a1 I ~ (a, t c,r On the
other hand.. for Iticrzaaing 6 el t 1i.h./h and Eb/b ,
considerable do-vi-ations from the thtcrpf. 9(faI.Sh# lines are
observed. The next Fy,.qtem to be Jnv~-! igated onyisted of a
number of rectangular rescnat.or6. coijpIt-d ov mearvi of narrow
slots; the eyetem ja Allustrated -in Fig. 12, The s-attering
equation of such a system Is In the forat
~.Uff Ifo BX/2
where B and X rtspreAent the aeries impedance and the
shunting admittane of' a quadripolt wltt~-.h ii5 equivalent to the
rectangular Y emenaLtor ,The formula w-i-q hv,.k-~d experimentally
by emplo~J.ng equipmerst consisting of #3 r~-&ngular channeJ having
Card 7/ IV

S/ i Is 1 161 /oo4/oO3/015/020
Experimental jrive4tigakion .... F192/R382
~ depth of 68 mm and width of 72 mm. rraps~-erse slots having
~ depth of 3 mm and width of I mm and Ppatod at 3 mm were cut
at the walls and the bottom of -the Metal. plates with
small. slots (jriAes) were Inserted into tj)ezie slots, The channel
was then covered with a plate which h3d -orre-.4ponding slots and
small apertures for measuring the fiell in the resonators.
The Inhomogeneitie.-i An. the sy%tem were pr,'iduc ed by changing the
parameters of a oell, i.e* Its dimenbivri (d and L) and its
position (a., ) .The results of the ex.PL-ctmenta illustracing the
change of the natural frequeny of the ystem are illustrated
in two figures. rn particular, Fig. 16 ahowi the frequency
deviation as a function of Za/a and '*'b/b . The straight
lines in the figure were obtained tht-or et ic ally., From the
above results, it is concluded that tho periodic delay structures
can be represented by the idealised quadripoles provided the!
non-homogeneities are not excessfv# rn most practical. Cases,
the results of experiment and theory ore in satisfactory
quantit t
agr 6ement
Card
7

30764
3/141/ft/oWoO3/015/020
Experimental investigation E192/E382
There are 16 figures and 7 references; 6 Soviet-bloc and
1 non-Sovi et -bloc. Tile English-language reference quoted is:
Ref. 11 - A. Bloch, F.J. Fisher and G.J. Hunt - Proc. IEE, 100,
64, 1953.
ASSOCIATION: Nauchno-issledovatel'skiy radiofizicheskiy institut
pri Gorllcovskom universitete (Scientific Research
Radiophy&cs Institute of Gorlkiy University)
SUBMITTED: December 15, 1960
Fig. 1:
Card 91?fli
C,

L .1,24 1-6) s/io3/63/018/004/004/006 #
A "FIT M S Bespalov, V.I. and Kubartv, A.M., Active Mem,;ers of the Society
TITLZ-: Calculation of losses for design of circuits forming
puisations of the current in Induction loads
FERIODICAL: Rediotekhnike, Y. 18, no. 4, 1963, 22-30
Tr=,: A system of linear algebraic equations to obtained loy a netbod
of pertUrbation. They permit making corrections, which axe stipulated by
the presence of. losses in inductions of the system, to the reactive el2ments
of the forming, dipole. The reactive parameters of the circuit, forming
a prescribed pulsation of the current In Induction loads without losses,
are assumed to be kncvn. Coefficients for the system of equations are ex-
pressed within parsm ters of an ideal circuit (without loss) and within par%-
meters of the original pulsation. This work is a continuation of that reported
in reference 2: V.I. Bespalov, A.M. Kubarev, Radlotekbnikca, v. 1.7. no. 7,
1162. 111e presentation considers the approximation of the pulsation with
Cara 112

L 12471-63 S/108/63/016/004/004/008
Calculation of losses for design ... 0
a final total of transient 'Tonics' the parameters of the forming dipole,
arA the formation of a gimal Ight angled pulsation consisting of two
harmonics (N%2). There are 3 figures and 4 roreign 1-ngage references.
SUBMITTED: January 27, 1962
.1
Card 2/2

ACCESSION NRs AP4019215 S/0056/64/046/002/0508/0510-1
AUTHORSs Kubarev, A. M.1 Piskarev* V. I.
TITLEt some results of an,experimental investigation ofthe affect
of a magnetic field on the radiation spectrum of a ruby laser
SOURCE: Zhurnal eksper. i teor. fiz., v. 46, no. 2, 1964, 508-510
TOPIC TAGS: laser, ruby laser, laser in magnetic field, laser line
splitting, laser frequency variation, laser cavity,, axial mode, ruby
laser spectrum, laser pulse modulation
ABSTRACT: A study was made of the time variation of the spectral
composition of radiation from a ruby laser to which a pulsed mag-
netic homogeneous field was applied. The delay between the start
of the field pulse and the laser flash could be varied.
of the ruby emission lines was- obtained at 1200K near the maximum
of the magnetic field. With decreasing field the mean value of the
Card 1/2

ACCESSION NR: AP4019215
frequency decreased in the stronger of the two lines and increased
in the weaker. The transitiorL_corresponding to the stronger line
- 4
is identified as -1/2E(2E)-ab but that of the weaker is not
J -3/9( A2)
identified. it is noted that the frequency variation is not smooth,
but is changed by discrete amounts from one cavity axial mode to
another. A regular decrease in the.generation frequency is observed'.
at room temperature. "The authorB Are deeply grateful to V. I.
Bes.palov and A. V. Gaponov for interest in the work and for a dis-
cussion of the results." Orig. ar ) bas: 5 figures.
ti
ASSOCIATION: Wauchno-issledovateV`,~kiy radiofizicheskiy institut
pri Gor1kovskom universitete (Scientific Research Radiophysics In-
stitute at Gorlkiy University)
OUBMITTEM 09AUVO3 DATz AtQ# MsrW SNCLI go
I
SUB COM PH NO RMr!8OV1 001 OTHER& 006
Card 2/2

2

ffim-

'i )f( :N B.f',% A.T. ; NACHVA Y, V. ~'.
Ultranonic taistlng of 30,nGrl?TJT Steel over a picklod sUrfnee.
Defektoskopila no. 5t84 965 'MJffA 191l)
I. Matoustovskly metallurgichoskly zavod i ChelyabJnakiy
politekhnicheskly InstAtut,

120-3-15/40
AUTHOR: Kubarev, A.V.
TITILE: A Sensitive Nuclear Magnetometer (Chuvstvitellnyy
yadernyy magnetometr)
PERIODICAL: I~ribory i Tekhnika Eksperimenta, 1957, lir 3, pp-57-60
(USSR)
ABSTRACT: A description is given of a puc'lear magnetometer which
can be used to measure the intdnsity of a c-3nstant magnetic
field and its non-uniformit~,/In the range 260-12 000 oersted
with an accuracy of 0.02-04 0 The method of resonant
5
3 em '6yed and measurement of fields
nuclear absorption if p1
having considerable non-,u niformity is achieved by a reduct-
ion in the size of the specimen and an increase in the sen-
sitivity of the recw~,Ing apparatus. A special form of the
specimen and a reger
gorating detector with capacitative coup-
ling, as well as ~ I ow band amplification of the resonant
, /11arr
siGnal and quart A brief descrip-
tion is rriven fcalibration is employed.
tj X the form of the specimen and -the condit-
i3ns and rang of ap.jication. A section throu-uh the speci-
men is shown'in Fig.3. There are 6 firures no tables and
7 reforenc.0s, 2 of which are Russian, 5 fln-lish.
A3.33OCIATION: Svc Olov Branch of theScientifle Research Institute for
Ca - ~1~2 Morology imeni-MI. Mendeleyev

e
KI I P A 74 11~ A,V,, C.-Ind 1'ech sci weanurv-ment, of nor-hmo,-Cno~is
A
e5 nrin C,
.T;agrt,~tic fields 1); the M(Ithori of nuclear riagrwtit. r, 0 - C
Len, 195", 12 vr) (Committee of ot:-ndards, "'e.-jsure9,,-L!A '.'cns~iring
Davico-,~; ander th(,- ,;o~incil of '!irdstert; USI;'tt. All-finion, z~ci I(es
Inst of '.'etrology irr D.I. Mendeleyev) 100 co,,des (F.L, 27-5t', 1l:,:)
- 113 -

sOV-120-5'3-3-15~ 3
AUTHOR: Zubarev, A. V.
TITLE: Moasurement of the Width of a Nuclear Absorption Line and
the Gradient of a Magnetic Field using Harrow B-n(I Impli-
fication (Iziaereniye schiriny linii yadernoi;o J-0 losheleniya
i 6radijenta magnitnogo polya pri u--kopolosnom usileni,i)
.PERIODICIAL: Pribory i Teldmika EI:speriT-wnta, 1958, Nr 3,
(USSR)
ABSTRACTi In the observation of nuclear n-agnetic resonance it is
often convenient to use narrow band amplification in order
to improve the signal to noise ratio and certain other
characteristics of the measuring appavatus. This was dis-
cussed in Ref.1 by the present author. The character of
the signals in the case of narrow band amplification differs
considerably from that obtained with wide band amplificat-
ion. The formation of the si-nal in the channel of a narrow
band amfliflor is discussed in terms of har,aDnix analysis of
the signal at the output of the resonance filter. Calculat-
ions for the case of linear r-~odulation, in -ca--ra- .-are
of frequency variation f1.2 7 f-j- (Ho � ho) where h 0
Card 1/6 is the modulation amplitude in the resonance region, lead

S'07-120-591-3-15/33
Measurement of the Width of a Nuclear Absorption Li-ne and the
Gradient of a Llagnotic Field using Narrow BanJ 1j.plificattion
to the following expanaiz)n coefficionto:
UO a p ( V2k2cr2 2%CT
a =- :V= ex C 03 - 1 (1)
1-1 7- 1V T2 T bl- = 0
when the signal
U UO 2 cr2) + exp (-(t + r)0/Cr2j)
= loxp(-(t - -C) /
is developed into a Fourier series. The cbove soluti~)n gives
a cos distribution of signal amplitudes in tho case of narrow
band amplification and shOV13 that phase ch--neos are t-rans-
formed into amplitude changes. The latter result learls to
a more accurate determinati)n of the resona-n--o even in the
caoe of conaiderable width of the resonance curve. PIZ.1
shivis an ex.T-,erimental graph of the anolitude distribution
Card 2/6

OOV-120-5,3-3-15/33
)f the Width of a Nuclear Ab3orption Line aad the Ga!'%_
_;nebic Field using Narrow Band Amplification
ic,-,,t Df a Mai
of a nuclear absorption si~;nal. In the ca~;o of wide sinuo-
oidal imodulation (ho ~> a) the resonance aboorptijn curve
may be rupresented by: 2
U(H) - U 0exp(-(HO-H) /a where
Ho = 21tf0/y and H is the field actinS on the nuclear
speciaton. In the case of sinusoidal modulati-in and the
resonance value of the measured field we have
H = H 0 + h0 sin w,,t and when h 192 = H0 + h0 we have
H - H 0 '+ ho + h0sin wt In the first case the signal
amplitude at the output of the narrow band f--'lter tuned U-o
Uho frequency w = 2w M is given by:
U 'U 2 a exp (2)
0 717
and in -the second case:
Card 3/6

SOV-120-58-3-15/3!,
Yjaa,-urc.~-,jcj1t of the Width of a Nuclear Absorption Line 'and the Grad-
ient of a 11-i-notic Field using Narrow Band AL.,iplification
1 -\/(U72a T,
UO = U
o=-IT h 0
-Ij OT-11710 .0.816 (1-1.352 +0) (3)
If the amplification coefficient of the filter is enual to
uii'fjy then:
exp (Or/h )2]
A = 1u1 VG/hO 0 (4)
1U-'1 1 - 1.352cy/ho
and provided a/h 0 is small, we have:
Card 4/6

; M-12 0-,51,-1- 3 -15/3 3
i4easure 'tient of the Width of it Nuclear Ab-,~orpti- 'in Id., -- Ctnd the Grad-
ient of a Lia~;netic Field using Narrow Band k-iplification
Cr 2 2 _ 0.04
0. 26 ho [A/1 2. c)6 A (5)
A2
In a non-liomogeneous fiold
a Ce CIO +. CH (6)
where c0 is the half width of the resonan(;e line in a
homogeneous field (natural width, effect of paramagnetic
ion!j, etc. being taken into account) and -ii H i3 the soread
due to the fact that the field is not h,-)-,,1oFeneous and is
given by:
= i I ,,, t (AH
U
II grad H1 al, ) M
where I is the axial length of the coil containing the
specimen. Thus by mea5urin6 the ratio of the amplitudes
riard 5/6 obtained with narrow band amplification at twice the

'~;OV-120-5-1-3-15/33
Measurement of the Width of a Nuclear Absor..-tion Line and the Grad-
ient of a lulaE;netic Field using Narrow Band Amplificau-ion
modulation frequency one obtains the width of the re3onance
curve and an estimate of the gradient of the .-,.Ia,~rietic field
provided ho;010-'151d . There are 4 figures, 1 table and
2 referencesi of which 1 is Soviet and 1 is German.
ASSOCIATION: Sverdlovskiy filial VINII metrologii (Sverdlov3k Braneb
of the VNII of Metrology)
SUBMITTED: July 7, 1957.
1. Nuclear magnetic resonance--Analysis 2. Narrow band
amplifiers--Applications 3. Narrow band amplifiers--
Signal to noise ratio 4. Mathematics--Applications
Card 6/6

_
i - i
Irrors In measurements of magnetic field Intensity by the
method of nuclear magnetic resonance. Ism-tekh. 20 no-l.37-39
A 159. (MIRA 11:12)
(Magnetic fiolds-Measurament) (Naclear magnetic resonance)

82892
S/120/60/000/02/023/052
AUTHORS: KubarM, WA and.Mezenev2,EW/A9382
TITLE: Oscillator for Studying the Electron Paramagnetic
Resonance ~1
PERIODICAL: Pribory i tekhnika eksperimenta, 1960, No 2,
pp 86 - 89 (USSR)
ABSTRACT: Two fundamental circuits employ$O in the investigation of
electron paramagnetic resonanEg::,at weak magnetic fields
are given in Figures 4. The first circuit is a
regenerative detector with a capacitance feedback, while
the second circuit in a regenerative oscillator with
grid current. The performance of the two circuits is
compared in Figures 1, 2 and 3. Curves marked with 11111
in these figures correspond to the oscillator with grid
current, while the curves marked with "211 are for the
regenerative capacitance-coupled detector. From these
Cardl/5

82892
S/120/60/000/02/023/052
Pjp24EJ82t
Oscillator for Studying the Electron a a a no ic Resonance
graphs It In seen that the oscillator with grid
current given a much greater sensitivity than the
regenerative detector. When the magnetic resonance
occurs, the inductance of the test coil in the
regenerative detector changes by:
A L c-- Or (XI - JX") a L (1)
where a is the filling coefficient,
X V- X1 represents the electron magnetic
susceptibility,
represents the dispersion, and
represents the damping.
The voltage change across the resonance circuit due
to the resonance absorption in expressed by:
dU kr
AU -'~k L C-.: 41'rY."aU OQ (2)
Card2/5 dL

S/120/60/000/02/023/052
FlA2/
Oscillator -for Studying the Electron Pa a agMic Resonance
so that the amplitude of the absorption signal at
the grid of the system is given by Eq (31, where T;
is the relaxation time, wo = yH 0 is the frequency of
the oscillator, y is the gyromagnetic ratio, ji is
the Bohr magneton,, h is the Planck constant, g is
the spectroscopic split factor and V K is the internal
volume of the test coil. The operation of the
oscillator with grid current can be analyzed in a
similar manner. It is shown that the change of the grid
current due to the resonance absorption is given by
Eq (4) and the amplitude of the signal at the grid of
the oscillator in expressed by;
2?rbaQ 2wLU2W It
U oko 0 (5)
1 +.Try2U 2Q2_2/w2 LV
0 K
Card 3/5

82892
S/12o/60/000/02/023/052
EJ224EflZet
Oscillator for Studying the Electron r m gn ic Resonance
where Q in the quality factor of the coil and
U0 is the voltage across the resonant circuit.
The increase of the sensitivity of the oscillator with
grid current with respect to the sensitivity of the
regenerative detector in expressed by Eq (6). This
formula is plotted in Figure 5 (the dashed line); the
solid line connecting the circl-es in Figure 5 was taken
experimentally. It is seen that the theory is in good
agreement with the experiment., An electronic magneto-
motor for accurate measurement of weak magnetic fields
was designed on the basis of the oscillator with grid
current. The resulting instrument is shown in Figure 6.
The device covers the frequency range from 1.35 to
40 Mc/s; the range is covered by means of three different
coils. The magnitude of the capacitance C is varied
from 11 300 pP, C I = 6 - 680 pF and
C2 = 3 240 pF# By means of this device it is possible
to measure the field intensities of the order of 1 Oe
Card4/5 with an error not exceeding 0.05%.

82092
:s/12o/60/000/02/023/052
111R2~9~82a
Oscillator for Studying the Electro a am gnetic.Resonance
There are 6 figures and 4 references, 2 of which are
English and-2 Soviet.
ASSOCIATION: Sverdlovskiy filial Vassoyuznogo nauchno-isslod-
dovatellskogo instituta metrologii
(Sverdlovsk Branch of the All-Union Scientific-Research
InstItute of Metrology)
SUBMITTEDt February 13, 1959
Card 5/5

86738
/l2o/6o/ooo/oo6/oI3/O45
E
032/E314
AUTHORSt and Mezenev, Yu.A.
TITLE: Apparent Change in the Gyromagnetic Ratio in a
Weak Magnetic Field
PERIODICAL. Pribory i tekhnika eksperimenta, ig6o, No. 6,
Pp. 52 - 53
TEXTt The electron and nuclear resonance absorption methods
are being widely used in various studies. in particular, in
precision measurements of magnetic fields. In the latter case,
use is made of the proportionalJty between the resonance
frequency of high-frequency oscillations wres ' which is
equal to the precession frequency w and the intensity of
the magnetic field H0 which is expressed by;
rem wo
(1)
where y is the gyromagnetic rntio. In the case of electron
resonance, Y guo A , where o 0 is the Bohr magneton, Qnd
Card 1/6

86738
S/l2o/6o/ooo/oo6/ol3/045
E032/E314
Apparent Change in the Gyromagnetic Ratio in a Weak Magnetic
Field
g is the spectroscopic splitting factor (g?--- 2) In the
case of nuclear resonances yn 0 $&Pn/I-% , where P in the
magnetic moment of the nucleus in nuclear magnetonsl Pn in
the nuclear magneton and I is the spin of the nucleus. In
a strong field*Eq. (1) is catisfied to a very high degree of
accuracy. However, in the case of weak field, the use of
Eq. (1) leads to a systematic error which increases with
decreasing magnetic field. This error is due to the fact that
Eq. (1) does not strictly hold for fields which are comparable
with the width of the resonance curve. In such cases, the
frequency of the high-frequency oscillations corresponding to
the maximum of the resonance signal is not equal to the
frequency determined by the resonance condition. 'This leads
to an "apparent" change in y or g for the specimenor
alternatively,to a change in the form of the resonance
condition. The average high-frequency energy absorbed by the
Card 2/6

86738
S/12o/6o/ooo/oo6/OJL3/045
E032/E314
Apparent Change in the Gyr9magnetic Ratio In a Weak Magnetic
Field
specimen from the exciting coil may be written down in the
form:
P(w) = wH2 "(W)
ix
(2)
For a circularly polarised high-frequency field in the case
of the electron spin resonance in the absence of saturationit
is known that the component. of the complex susceptibility
corresponding to absorption is given by:
X OWA (0 (3)
W2 + (Wo - W)2
where bkw = Yd is the half-width of the resonance curve in
units of frequency and c? is the half-width of the curve in
units of the field. Substituting Eq. (3) into Eq. (2), we
-Card 3/6

86738
S/120/60/000/006/013/045
Apparent Change in the Gyromagnetic Ratio in a Weak Magnetic
Field
obtain an expression for the absorption curve in terms of
frequency,and hence it can be shown that the value of the
frequency corresponding to the maximum of this curve in the
case of a weak field Is given by:
res 0 W /W0
In a strong field the first term of this expression can be
neglected. Using the relations for w, A w, y and g , it
can be shown that the apparent values of w and g in a
weak field are given by:
Y, = Y + -V2/H21 g, = 9 + gd2/H (5)
0 0
The dependence of the S' factor on the field H Was
determined experimentally by the present authors in the case
Card 4/6

86738
S/l2o/6o/ooo/oo6/OJL3/045
E032/V,314
Apparent Change in the Gyromagnotic Ratio in a Weak Magnetic
Field
of the electron spin resonance for a specimen of the free
radical of aa-diphenyl P-picrylhydrazine in fields down to
0.04 Oe, when the magnitude of the g'-factor increased up to
about 34. The experimental curve for g as a function of
H0 is shown in the figure on P. 53. The half-width of the
resonance curve for a specimen containing 95% of the above free
radical is 0,85 Oe and the magnitude of the g-factor in the
strong field is 2.0042. The observed functional dependence
is in agreement with Eq. (5) if the second term is corrected
by a constant factor of TT_ 2 , It Is clear that this effect
must be taken into account in nuclear magnetic resonance
studies in fields of the order of the Earth's field. In the
case of electron spin resonance, when the width of the resonance
curve is usually appreciable, the apparent increase in the
g-factor is already important at fields of I Oe or less.
Card 3/6

86738
s/L2o/6o/ooo/oo6/Ol3/O45
E032/E314
Apparent Change in the Gyromagnetic Ratio in a Weak Magnetic
Field
There are 1 figure and 1 English reference.
ASSOCIATION: Sverdlovskiy filial Vsesoyuznogo nauchno-
iseledovatellrkogo instituta metrologii
(Sverdlovsk Branch of the All-Union Scientific
Research Institute of Metrology)
SUBMITTED: November 16l 1959
Card 6/6

KUBAREV, A.V.
Calibrating electronic paramagnetic raBonance pickups for
magnetometry. Im.tekh. no.9t43-46 S 162. -(MIRA 15:11)
(Magnetic flslds.-~basurement) (Calibration)

KUBAREV, A.V.-
- . , ,
Quantum radiophyisice and metrology. Iza. tekh. no.10:5-7 0 163.
(MIRA 16M)

ACCESSION NR: AP4041344 6/0115/64/000/005/0025/b029
AUTHOR: Khinrikus, Kh. V* I Kubarev. A. V.
TITLE: Fundamental characteristics of quantum paramagnetic amplifiers
SOURCE: Izmeritel'naya tekhnika, no. 5, 1964, ZS-29
TOPIC TAGS: amplifier, ma-ser, quantum paramagnetic amplifierp
resonator paramagnetic amplifier, traveling wave paramagnetic amplifier
ABSTRACT: These characteristics of the quantum paramagnetic amplifier
both resonator type and traveling-wave type - are regarded as fundamental:
frequency band, gain, passband, input noise temperature, saturation power, gain
instability, and unilateralization (internal feedback). The recovery time and
amplifier loss are measurable special characteristics. A third group of
characteristics, single -valuedly determined by some of the above characterist'ics
includes: paramagnetic gain, resonator -amplifier efficiency, sensitivity. and
cord'.
262iha 6-M

ACCESSION NR: AP4041344
dynamic range. Formulas describing the fundamental characteristics based on
published (mostly American) sources are given, Origs art. has: 28 formula$$
ASSOCIATION: noni
SUBMITTED: 00 ATD PRSSSi 3074 ENCL: 00
SUB CODE: EG NO REF SOV: 003 OTHXR: 012
01

ilM

LESKOV, A.S.; KUBAREV, A.V.
Absolute measurement,'o the numbers of stable paramagnetic
_oenters, Izm. tekh.,nO.5t27-29 My 165. (MIRA 18%8)

ZUSSFR, A.P., Inz.h.; LAZL'BNIKOY. H.B.: KUR&M- . 0.N.
Using tipping forms in making nrocast reinforced concrete
fences [Suggested by A.P.Zueser, M.B.Lezebnikov, G.R.Kubarev]
Rate. i isobr. predl. v strol. no.6:10-32 '58. (WRk 1l.-10)
(Fences) (concrete construction-Formork)

PANAaNKO, VasMy Griporlyevich- K F rut.,~anzf~?nt; ZIVAISKIY,
D I xUtw&v Ll-
MsAa, retVOnZent; SVIRID67, M!Aijk,~r,V, L.Ii. ,
retsenzentj MKIFOROV, A.S.,, red.
(Study of materials used in carpenti-I and furniture iranufac-
turel Materialovedenie stoliarno-mebelinykh proizvodstv. Mo.-
skvap LeBriala promyshlonnost' , 1964. 204 p. (MIRA .18-3)

- I C - I I ,~ I , k
$ r . I ! .
6f i!C7,f?rT' b7 lntrr;,mnc,ua 1~; " -'~ !, - *--' 1 - 1 -
No. 4, 1952.
M3, . t h I List of Buy-i'm Accessions, Library of Gcn,,reqs, November 1952.

- .
. ... i - . . '.. I TI.
"'!:'~ m ~l 4, !~-' !1! " ~".' If. I-If winca i'le ! !, ". - I - F, I I - lr$at.,
v !itnl *K vor-rnl n,~l 1. 1 :10'-fratblo'-ii (~ a! I -t IF%; or , r-n--, In, -_ --nit Ole , )l
p .
' 9) 1, tw-oor, --VArwir It T ) , ocwl -).
.1 , 1)1T k~lll. ii

o c,7.
?"'o-,ccalne anl its Variatio,-,- .1-i `e )f
4ns',:01 ', rorolf~ i1 i lermatol'. (-,ulletin cvf Verprolog-
o 'chr
xt* 1954 k1li or,~,-2r),

I
1~' I ~
TN
Z"IN, A.S.;KLMARMY, X.Y.
'treatment of oozes& with Intravenous procalnee Test, vener., Kooky&
no. 4:15-16 July-An&. 1952. (UHL 23:3)
1. Professor for Unin; Docent for Xubarov, 2. Of the Skin~-Veuor-
sological Olinic (Road - Prof, A. S. Zonin). Kuybyshev Medical In-
stitute.
In treating ecZejTZ, intravenous injection of novoca-in together with tile
neces3ary local treatmont can accelerate the healing of acute inflawiatory
symptoms such as itching, and improves the sleep and the condition of the
patient in general. In chronic eczema, novocain which infiltrates the skin
is not usually resorbed. No marked effects of the novocain treatxkr.,t on
acute inflaliqatc;ry processes was observed.

XUBARM, X.To,dotsenti DITACHKOV, D.T.
Prevention of pyodermitis in workers employed by the Mchine-
building Industry. Test. von. I darn 30 no.10-25 U-7 156
(MM 9 M
1. Is kliniki koxhtqkh I venerichaskikh boleaney LWbyshavekogo
awditsInskogo, Institute, (say. kafedray-prof. A.3. Zenin) I mdiko-
sanitanoy ohaBti (nach. K.Te. Poltorstskaya) .
(SM DISO die. Pyoderma, prey. and control
piodernitin. prey. In Indust. workers)
(MUSTRIAL HTGMM
pyodsma
prey. of plodermitis in workers)

KOLESOIKOV, Vasiliy Pavlovich; KIJPA~M_,_Ntko1ay Vlaz:ovich; AVDETEV,
Md-'Ye- . -a.-
Boris Ivanovich; XUD WMJWP A.,, tel-chn.
red.
(Advanced technologiml processes in the machinery industry]
Progressivny~e tekbnologicheBkie protsousy v mnahinostroenii.
Kaliningrad) Kaliningradakoe knizhnoe izd-vo, 1962. 110 P.
(MIRA 15:11)
(Machinery industry-Technological innovations)

--K-UBAITIEVO P.I.
Additional artificial pollination of self-pollinatora, Bot.;
isel. Bel. otd. VW no.5:192-195 163. OMIPLA 17:5)

KUBAREV. P. I,
Additional artificial pollination of i4nter vheat. Agrobiologiia
n*40.10-111 Ja-F 163. (MIRA l6t5)
I* Polesakaya sell kokhmaystvannaya opytnaya stantaiya.
(Fertilization :f plants) (Wheat)

KUBARFV, P.I.
Differencen In the nucleic acid content botween tho rLilo
and female infloreacencov of corn. Flzlolrurt. 1-1
no.6:968-970 N-D 165- (11,1111A M12)
1. Leningradakiy se1'skokhozyaystvenxW institut. Stibraittod
Fohruary 1, 1965.

-KUBAIZV, S. T. and SJOKOLOV, N. D.
"On the Theory of Dependence of Molecular Spectra on Intermolecular Interaction."
report presented at the 4th International Meeting of Molecular Spectrosc6py, Bologna,
Italy, 7-12 Sept 1959.
Moscaw State University, Moscow, USSR.

24 (7)
AUTHOR: Xubarev, S. 1. SOY/20-126-5-i6/r~,i
-----------
TITLE: On the Influence Exerted by Intermolecular Interaction Vron the
Spectra of Molecules (0 vli anii mezhmolokulyarnykh vzaimo-
doystviy na spektry molekul~
PERIODICAL: Doklady Akademii nauk SSSR, 1959, Vol 126, Ur 5, PP 971 - 174
(USSR)
ABSTRACT: Intermolecular interaction produces a number of cpectroeoo'~ic
effects, the most important of which consists in the broadening
and shift of lines@ These are visible both In absorption and
Raman spectra* In the case of van der Weals' interaction they
are comparatively weakp in systems with H- or Li-bondeq how-
over# they are so strong that they may be considered character-
istio features of these compounds. The existence of a broad and
shifted band of the 0-H groupp for example, indicates the for-
mation of a hydrogen bridges The distribution of intensity with-
in the bands greatly depends on temperature* No unambiguous and
uniform explanation of the spectroscopic effects as a whole
(shift, broadening, temperature dependence in systems with hy-
drogen bonds) has been found as yet. One of the greatest diffi-
Card 1/2 oulties arises from the fact that not only in condensed but also

On the Influence Exerted by Intermolecular Interaction BOV/20-126-5-16/69
Upon the Spectra of Molecules
in gaseous media broad bands are visible. The author of this
article made an attempt to give a general explanation of any
state by Lax' method (Ref 3)- Mathematical considerations of
the absorption and Raman spectra are made in oemi-classical ad-
iabatic approximation. The results are briefly discussed. The
author finally thanks Professor N. D. Sokolov for his diacus-
sions. There are 6 references, 2 of which are Soviet.
ASSOCIATION: Moskovskiy gosudarstvennyy universitet im. V. V. Lomonoaova
(Moscow State University iwani It. V. Lomonosov)
FRESENTED; March 119 19599 by Ve N. Kondratlyeyj Aoadezician
SUBMITTED: March 6, 1959
Card 2/2

-11913
S/051/60/009/01/001/031
AVTWRi Kubarsv,- Sex. 3201/2691
TI TLI sOn Certain Froblaw in the Sptctros copy of Complex Molecules
PUIODIGAL iOptika I opoktrookopi7a, 1960. Vol 9, Sr 1. pp 3-6 (VSSR)
ABSTUM loporent And Stepanov (Rof 1) defined a complex molecule as a
multiatcuic moleaUe In *ich the degree of coupling between
nomal vibrations Is sufficient to produce continuous vibrationAl-
onorgy bands. The present author points out the approximate nature
of such a definition and then uses it to discuss the origiz of
continuous band# of complex molowlso. It is shom tbat the us*
of the oscillator approximation explains satisfactorily the
experinantally obderved temperature 4opendonce of the band peranotors
(e.g.,odft) of amplex molocules. The paper is entirely theoretical.
Acknomlod Ponta Are md* to N.D. Boicolov for his advice. Thor*
are 10 references, 8 of shieh are Boyi&t, 1 Inglish and 1 Japanese.
SUMaTTSDx July 18, 1950
Card 1/1

85236
3/048/60/024/60029MOAX
B013/B067
AIDTHOR: _Kubgreve S. I.
TITLE: Electron Spectr 'A of Compound Molecules
PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheekaya,
1960, Vol. 24, No. 6, Pp- T75 - 778
TEXT: In this paper, the author demonstrates that in the majority of
compound molecules tho princripal spectrometric effects can be studied
on the basis of Lax's relations (1). This method is based on the follow-
ing consideration: As has been shown already in Ref. 1, adiabatic
approximation can be used for the long-wave electron absorption of
compound molecules. If the application of adiabatic approximation is
justified, i.e., if a vibrational subsystem exists for several lower
electron states, the problems of absorption and emission of light can
be considered from one point of view. In this cace, the spectral
absorption and emission densities can be represented in a convenient
form by using the method of Lax (Ref.2):
Card 1/3 IW - Iexp (-2fi-Jt)I(t)dt,

85236
Electron Spectra of Compound Molecules 3/048/60/024/006/029/030/XX
B013/BO67
where the Fourier representations of the spectral absorption and
emission densities read as follows;
exp
Iabsorb(t) " SP(M exp[(itA)flbl M exp [(-itA)RI, (-OfiaA
(a -4 b) Bp Iexp (-~fi a)]
Iemiss (t) - Spim expk-iWfial eexpl("A)MA
(b --f a) SP (F)
P- distribution function of the vibrational states in excitation;
Ha and Ub vibrational Hamiltonians for the electron states a and b;
M - transition moment. The author demonstrates the applicability of
the method suggested by some examples, considering the formation of
continuous bands, their shape, and the mirror symmetry of absorption
Card 2/3

85236
Electron Spectra of Compound Molecules S/048 60//024/006/029/030/XX
B013YBo67
and emission spectra. Finally, he suggests the possibility of drawing
qualitativet and in some cases also semiqualitative, conclusions as to
some other problems by using the suggested method as, e.g,, the
temperature dependence of the bands, the temperature dependence
of the luminescence quantum Yield, the effect of solvents on molec-
ular spectra, etc. S. I. Vavilov i0 mentioned. The present paper was
read at the Eighth Conference on 'Luminescence (Molecular Luminescence
and Luminescence Analysis) which took place fn Minsk from October 19
to 24, 1959. There are 7 references; 6 Soviet.
ASSOCIATION: Institut khimicheskoy fiziki Akademii nauk SSSR
(Institute of Chemical Physics of the Academy of
Sciences USSR)
Card 3/3

5M
AUTHOR: Xubarev, S.I. S/020/60/130/05/051/06i
BO04/B014
TITLE: Light Absorptionland Luminescence of Complex Molecules
PERIODICAL: Doklady Akademii nauk sssR, 196o, Vol 130, Nr 5, pp 1067-1070
(USSR
ABSTRACT: The author describes a mathematical method used to solve the
following theoretical problems of long-wave electron spectro-
11 copy: the origin of the bands, their universal character
(S.I. Vavilov, Ref 1), their dependence on temperature and
Xexoit, and the problem of mirror symmetry. According to
M. Lax (Ref 5)9 the author derives equations (1) in adiabatic
approximation for the Pourier transformation of the spectral
density of absorption and emission. The general form of these
equations permits various approximations. A blurring of spectral
lines of the order of some 100 cm-1 is thus calculated by a
semiclassical study of the degrees of freedom which correspond
to conditions (2) and (3). In the case of complex molecules
this blurring is sufficient.for the development of a band.
Card 1/3 Another explanation of the bands proceeds from the actlcn of

Light Absorption and Luminescence of
Complex Molecules
ASSOCIATION:
Card 2/3
81020V
.~0/130/05/031/061
B004/ 14
the peripheral groups of complex molecules. The uniYersal
nature of the bands to explained by the central limit theorem
(Ref 12) according to which the distribution of the normalized
uantity q a (V - ';)d with n--+oo tends to the normal function
2vt% position of the maximum, d2 . second moments, n - Di.ni,
z
where ni denotes the number of oscillators with the frequenoy I
the average according to Planck. The temperature dependence
ifis determined by calculating several first moments or the 6
traces of equations (1). For mirror symmetry some solutions are
obtained from equations (1), one of which may be regarded as
the development of V.L. Levehinfe condition. An equation (14)
is written down for the symmetry line Ast which indicates that
the frequency of electron transition is shifted toward the
absorption maximum in aooordanoe with experimental results
(Ref 16). The author thanks Professor N.D. Sokolov for his
valuable advice. There are 16 references, 14 of which are Soviet.
Moskovskiy gosudarstvennyy universitet im. N.V. Lomonosova
(Moscow state 'University imeni N.V. Lomonosov)

Light Absorption and Luminescence of 31020V60113010510311061
Complex,Molecules B004/ Jm,0 14
PRESENTED: October 10, 1959, by V.N. Kondrattyev,,Academiciazi &,~
SUBMITTED: October 7, 1959
Card 3/3

E--- -- - -
KUBAM, S. I.
Cand Phys-Math Soi, Dies -- "Certain problems on the spectroscopy
of complex molecules". Minsk, 1961. 13 pp, 21 om (Acad of Soi
BSSR. Joint Council of the Inst of Physics, Inst of Math and Computer
Engr and the Dept of Solid State and Semiconductor Physics, Acad of
Sci BSSR) 180 copiea,,:No charge (KL, No 9, 19610 p 175, Wo 24252).
51-548iit

~-.,XUBARET v S. I.
Influence of vibraticna on the limiting lt=inencence polarization
of conplex molecules. Opt. i spektr. 10 no.4:535-537 Av 161.
(mru 14:3)
(rA=i escance)

-L 18090-63 EWT(1)/FCC(w)/BDS AFFTcAsD/ijr(c)
i,,,-ACCESSION NHs AT3002187 6/29h1/63/0Ol/bOQ/0OO3/0OO8
`114UTHORs Kubarev, S. I.
71TLEs One-dimensional model for absorption and emission calculations of coylez
Valecules
SOURCEt Optika i spektroakoplya; abornik statey. Y. ls Lyuminestsentoiyao
Moscow, Izd-vo AN SSSRI 19632 3-8
TOPIC TAGSt absorption bandp emission band, complex moleculep quantum machanicap
Stokoa-lines, half-width
i,
AWRACTs The author has discussed the application of the one-dimensional model
to determine the spectroscopic characteristics of complex molecules, It is
shown that although it is not a very rigorous method, the one-dimensional model
is useful in presonting approximate methods to solve problems relating to
absorption and emission bands in complexly structured molecules. A formal
application of such a model is the semiclassical approximation vhich is a mom nt
expansion technique with Hamiltonians given in Boas operators, The author notes
that in all one-dimensional calculations the choice of the particular expansion
Card 1/2

L U090-63
ACCESSION NH: AT3002187
parameter implicitly assumes a temperature of the order-of 3000K. Furtherimore,
the one-dimensional quantum mechanical model gives rise to a large discrepancy
between the half-width (of the frequency spectrum curve) and the Stokes-3hift,
Orig. art. ha33 14 formulas and I table.
ASSUCIATIONs none
sr
.jBmiT,rED, 16mar62 DATE ACQs 19.4ay63 ENCLs 001
SUB COM PH Nd REF sov, 007
OTHERs 0061

L Ijp(c)
,ACCESSION NR: AP5019731 UR/03 79/65/00 1/0 G2/0229/02,11
AUTHOR- Kub-trcv, S.L;
TITLE: Calculation of Idnetle coefficients for certain organic scnlconductora-~/,4
SOURCE: Teorcticheskaya, ( ekspertmental'naya khimiya, v. 1, ro. 2, 100, 2 -241
TOPIC TAGS: organic semiconductor, electron mobility, anthracerle, r1aphthalene, electric
conductivity, band theory;
A13STRACT: An approximate solution to derived for the kincti* equation for semiconductors
with a narrow conduction band (such as naphthalenc$nd anthra~ienv.).j On the basis of this
solution, certain kinetic coefficients were cal a. Tfi6 contri t1dn of transfer proc-
esses into the relaxation time was taken into account. A numericol estimate of this contri-
bution for the electrical conductivity shows that when transfer prmuses are considered,
the conductivity decreases approximately by a factor of two. The temperature dependence of
:'the mobility obtained agrees qualitatively with the experifnentai data, which lead to a rela-
i tion of the typo Using the approximation under consideration, a very