SCIENTIFIC ABSTRACT ADAMOV, M. N. - MOSKVA, V.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000100320007-8
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 5, 2000
• Sequence Number: 7
• Publication Date: December 31, 1967
• Content Type: SCIENCEAB

Dispersion formula in a metal model of a molecule with
conjugated bonds. (Cont.) 51-3-22/24
calculated value is 10 times too large because the frequency
of the D-line of sodium is close to the natural frequency
of an allowed C1OH12 electronic transition. The benzene
molecule is represented by a circle of radius R = 3a/Ir,
where again a = the length of the C-C bond. The results
for the polarizability at the D-line of sodium agree well
with the experimental values.
There are 2 tables and 4 references, 3 of which are Slavic.
SUBMITTED: October 12, 1956.
ASSOCIATION: Physics Department, Leningrad State University.
(Fizicheskiy Fakulltet Leningradskogo Gosudarstvennogo
Universiteta).
AVAILABLE:
Card 2/2

24(5) ZGV154- 58-4- 18/ 1 e
AUTHORS: Adamov, M. N,-, Orlov, B, I.
TITLE: Computation of the Polarizability ofrFt--Electrons on
the Basis of
a Metallic Model 'Nith 6-Shaped Potential Sources (Raschet
polyarizuyemosti5-t-elektronov na osnove metallicheskoy modeli
8
~-obraznymi istochnikami potentsiala)
PERIODICAL; Vestnik Leningradskogo universiteta. Seriya fiziki
i khimii,
1958, Nr 4, pp 182-167 (USSR)
ABSTRACT:
The most simple metallic model holds only in the ~~ase of a
con-
stant potential in the system of the conjugate bonds. In the
real molecule for the model a step-like potential is assumed
and
in a boundary case as a model with S-shaped potential sources
in
the points where an atom is located. The computation of the
polarizability (according to references 1-3), which holds for
any type of model, permits also for the model under investiga-
tion with &-shaped potential sources the solution of the
Schr6dinger equation corresponding to it, This is carried out
on
the basis that the -.~.-source contributes ui - -g6(8-8 i) to
the
Card 1/2 potential energy of the electron, with E(s-s denoting
Dirac
uscom-Dc-60.,884

SOV/54-56-4-16/16
Computation of the Polarizability of 5-F-Electrons on the
Basis of a Metallic
Model With S-Shaped Potential Sources
&--function, e - the coordinate along the outline of the mode],
ai - the value of s at the location point of the source, g -
a parRmeter expressing the intensity of the so rle. The expres-
sion for the polarizability a ie formed from 7 0~, the wave
function unperturbed by the external electric field and
(1) - AL with the wave function perturbed by the field.
(40 F F=0
-2 f~ (o N d5. The expression for theV-electron-polariz-
ability is obtained by the further mentioned connections and as
a function of the source intensity g, the energy-parameters
"'k ancO_nand the dimensions of the model. A computation,
carried
out according to the given formulae for benzene which can be
regarded as a hexagonal model with six potential sources (each
potential source has the value 9 0.733) represents the value of
theii--electron-polarizability a 59~2 which is in the same
hexagonal model without potential sources only a = 47.0. There
are 5 references, 4 of which are Soviet,
Card 2/2

ADAMOV, M.N.; ORWV, B. I.
Calculation of the polarizability of Z-alectrons on
the basio of
a metallic model with S-shaped field source [with
summary in
Inglish]. Vest. IDU 13 no.22:182-187 '58. (MIRA 12:4)
(Blectrons) (wave mechanics)

AUTHORS: 'd 11. , Veselov, 1.11. G. , Sov/i!6-22-9-1 '1o
-421La-v.L 1-1-1 - - t
Rebane, T.-r7`
TITLE: The Electric and Magnetic Properties of Moleciiles
With
Complicated Structu-re Calculated on the Basis of 'L~-.e
Free-Blectron Model (Raschety elektricheskikh i ma~.,
nitnykh
svoystv slozhnykh molekul na osnove modeli svobodnykh
elektronov)
PERIODICAL- Izvestiya Akademii nauk SSSR. Seriya
fizichesk~,.va, 19,1)8,
Vol 22, Nr 9, pp loll,) - lo18
ABSTRACT: The authors succeeded in computing the
polarizability
and the diamagmetic susceptibility of n-electrons
on the basis of the simple model of the free electrons.
The polarizability a of atoms and molecules usually
is computed by perturbational methods. For the com-
putation of the n-electron longitudinal polarizability
Card 1/14 of the polyenes C 2nH2n+2 the formulae

TlYe Electric and 14agnetic Properties of Molecules With
SOV148-22-9-1140
Complicated Structure Calculated on the Basis of the
Free-Electron Ylodel
4En
an (w) =T-4 Pn
(_,)n_cos p11L
Plin p L
n
(-1)n
, -c os qnL
+ sin q L 72 (2)
n
and 0
an(O) = 12n4n2 (15 - n n
were employed. The results, toLgether with the results
obtained by Bolton (Ref 1), are listed in table 1. The
polarizability of the electrons was also determined
for the case of a rin6-shaped and a hexa,,- ..
,on-l nolectile.
A simple wthematical scheme was worked out, which
allovis to determine the wave function and the on,-r[,y
spectrum of the Ti-electrons in the majr-_~tic .'--'--id very
exactly. If the one-dimensional potenti;li of the
conjuJate bonds is everywhere equal to zero, the problem
Card 2/4 is represented by the determinzat'ion of the
ei-envectors
L,
(3)

The Electric and liagnetic Properties of Molecules Iffith
SOV/48-22-9-1'41o
/I
Complicated Structure Calculated on the Basis of the
Free-Electron 11"odel
of the Hermitian matrix. The energy spectrum of the n-
electrons in the magnetic field and their dia-a,~-netic
susceptibility are determined according to the secular
equation ~et W = 0. This computation method of the
diamagnetic susceptibility can be extended also to
the case of a variable one-dimensional potential. The
method allows to consider the influence of the intramo-
lecular periodic field as well as the deviations from the
periodicity. Starting from the matrix-formulation of the
problem the connection between the methods of the free
electrons and of the molecular orbits was investi_rated.
The agreement of the energy spectra shovis by means of
the results obtained by the semi-empirical method due to
Pariser, Parr and Pople (Ref 4)that the depth of the
potential well in the place wbere the atom j is situated
is given by the equation
V ' ~(2 - q )I + qjF - N ~. This equation validates
j 2 j j j~ i
Card 3/4 the semi-empirical formula sul-I-ested by
Veselov and

The Electric and Magnetic Properties of I-Iolecules
'~Vithl SOV/48-22-9-1/40
Complicated Structure Cal-culated on the Basis of the
Free-Electron L'odel
Rekasheva (Ref 5). This formula describes the relation
between the shape of the bottom of the potential well in
con.jugate molecules which contain hetc-ro-atoms, and the
potentials of the electron affinit'.,), and the ionization
of single atoms. There are 2 tables and 5 references,
2 of which are Soviet.
ASSOCIATIONI: Leningradskiy gos..universitet im. A. A.
Zhdanova (Lenin
grad State University imeni A. A. Zhdanov)
Card 4/4

AUT11O.1,. Adamov, M1. N. SOV/76-32-9-21/46
TITLE: Calculation of the n-Eie(,tron Polarizability
Te-nsor for
Butadiene and Benzene 114olecules (Raschet tenzora polyari-
zuyemosti n-elektronov v molokulakh butadiyena i benzola)
PERIODICAL: Zhurnal fizicheskoy khimii, 101)8, Vol 32,
.'%'r 9,
pp 2087 - 2093 (USSR)
ABSTRACT: The components of the tensor for trans-butadiene
amount to
('X XJR = 54,0 (a YY )TC = 2,6 WXY)n = 9,0 in atomic
units. Basis of the calculation was the metallic model.
The wcepted coordinate system corresponds to the
symmetry axes ( x and y correspond to S., the x-axis goes
through the center of the C-C-bond; z c6rresponds to 0 2).
The result for benzene was A Tr = 47,0 for the hexagonal
model; a- ~ 50, 7 for the circular model. The approximate
it
formula is verified for the -t IE of benzene, as well as
at (.X XX) T1 and (1X xy) Rof butadlene, though only the
transition
with minimal excitation is under consideration. The
Card 1/2 approximate value of (a YY )n of butadiene
corresponds to

Calculation of the r~-Electron Polarizability Te,3or for
SOV/76-32-9-21 4
o
Butadiene and Benzene Molecules
the true value if the two following transitions are
taken into account. Collaborators were the students of
physics I. S. Milevskaya and B. I. Orlov. There are 2
figures, 1 tLLble, and 7 references, 5 of which are Soviet.
ASSOCIATION:Leningradskiy gosudarstvennyy universitet im.
A. A. Zlhdanova
(Leningrad State University imeni A. A. Zhdanov)
SUBMITTED: April 5, 1957
Card 212

14 CY /;L
S/020/60/133/02/17/068
B019/bO60
AUTHM-, Adamov, M. H.
----------------
TITLE. Integral Representation of the Dispersion Formula for
a Hydrogen Atom in the Ground State
PERIODICAL. Doklady Akademii nauk SSSR, 1960, Vol. 133, No.
2,
pp. 315-317
TEXT, The quantum-theoretical expression (1) for the optical
polarizability of a hydrogen atom or of a hydrogen-like ion
in the ground
state is written down in the introduction. The ordinary
dispersion
formula (3) is obtained by expanding the function ~(74;i~,)
according to
the eigenfunotions of the operator Ho. Calculations
according to this
formula are very difficult because of their slow
convergence, and it is
shown here that it is possible to oonstruct an integral
representation
of the dispersion formula, Formula (4) is set for ~ (4;u)),
and is
substituted into (2). Finally, equation (14) is obtained
for the
dispersion formula with the aid of a Laplace transform. The
calculation
Card 1/2

Integral Representation of the Dispersion
S/020/60/133/02/17/068
Formula for a Hydrogen Atom in the Ground BO19/BO6O
State
of the polarizability for low frequencies of the electric
field is
discussed next. This closed representation of the dispersion
formula
can also be obtained for excited states of the hydrogen
atom, but
complications arise due to degeneration.
ASSOCIATION: Leningradskiy gosudarstvennyy universitet im,
A. A.
Zhdanova (Leningrad state University imeni A. A. Zhdanov)
PRESENTED: March 25, 1960, by V. A. Pok, Academician
SUBMITTED: March 2, 1960
/C
Card 2/2

ADAMOVI M.N.; KAGANt V.K.; ORLOVt B.I.
Dispersion formula for an electron in a potential
well of finite
depth and the optied polarizability of molecules.
Opt. i spektr.
10 no.2s276-279 F 161. (MIRA 14:2)
(Electrons) (Molecule&-Optical properties)

89218
9/05 61/040/001/024/037
B1 02YB212
AUTHORS: A _V.L_jt,_j Zubkov , V, A.
.Ldi!movL
TITLE: A commentiD the variational calculation of
polarizability
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy
fiziki, v- 40,
no . 1 1 1961 0 246-248
TEXT: In the derivation of Kirkwood's formula and similar
variational
formulas for polarizability the requirements which result
from the ortho-
gonality of the perturbed wave functions, were not
considered. These for-
mulas therefore give a higher value of the polarizability of
excited eleo-
tron states. The authors' aim is to show that if these
requirements are
taken into account when setting up the trial function for
variational cal-
culation of the electron polarizability in the excited statel
results are
obtained which agree well with exact values# (i.e., they
approach them from
below). M variational problem of determining the
polarizability
ai - -2E 1 2 for the i-th'slectron state is formulated as
follows:
E (2) 0 j 191 (1 (1)(H0 - E (0)) T (')dr + 2fTi MZT i(O)dvi
the
i I Imin 0 ~i i i
Card 1A

89218
8/056/61/040/001/024/037
A oommenttD the variational.... B102/B212
normalization of the perturbed funotion T I results in fl?
iM7i(0) d.T . 00
and the orthogonality of the functions Ti with respect to Tk
(describing a
state lower in energy than the i-th state) yields
fTi(1)'Fi(O)d, - -frk(l )Ti(O)d, -zik/(Ei(o)- Ek(O)). The
polarizing field
is assumed to be along the z-axis. The Buler equation
E (0)),r (1) . (X - z)? (0) + L T (0) ' with X - E (1) . Z and
i i i i k k k i i ii
Xk 0 chebke with the perturbation theoreti6al equation for Ti
(1);
Substitutingsi K - (fi)ii]Ti Of (fi)ik - f7i(O)fiTk( O)di, yields
(0) - M- (0)) - (f
Ti - N - (fi)i 1~ 4 Oik'Fk(O) ' where cik ~ Zik/(Ei Fk i)ik*
When-introduced into the initial equation this gives:
(2).
E j Eli, n . 2[(z - zii) + I (grad fi)2 + 21c [(E~(O)- E (0))f +
4 11 k ik i i
Card 2/4

A comment'to the variaticral ...
.89aa
S/(056/61/040/001/024/037
3102/B212
+ ik' +~k aik(Ek(" Ei(o)),P For f w-a z'one obtains instead of the
i -i
2
Kirkwood formula (6) ai 41z j , a new variational formula (9):
ii _ (zoo), 2
a z2 - (Z ~2 '(zi )1] 2/ [1 + 2 ~(%(O) - N(o))(z 2] - 2 2
ii IV k ik) k(zik)
(E (0) E (0). Be
i k veral values of the polarizabilities a n1n2m of hydrogen
states computed.~ by using formulas (8) and (9) (the first two
lines) are
compared with exact values in Table.1 (last line). Parabolic
quantum num-
bers n 1 and n2 and the magnetic 'quantum number m characterize the
state;
Table 2 shows analogous values for several states of an electron
moving in
an infinitely deep potential well having a length of 1 - 10 atomic
units
(an is the pQlarizability of a state characterized by the quantum
number n).
The new formula, unlike the Kirkwood formula, always gives values
that do
not exceed the exact ones. The formula can be used to calculate the
polar-
izability of many electron systems. Finally, it is pointed out that
taking
the orthogonality of the perturbed wave functions into account
should also
be important in other variational calculations of quantities in
second
Card 3/4

89216
S/056/61/040/001/024/037
A comment to the variatichdoes B102/B212
perturbation-theoretical approximation. There are 2 tables and 5
refer-
ences: 2 Soviet-bloo and 2 non-Soviet-bloo.
ASSOCIATION:
SUBMITTED:
Card 4/4
Leningradskiy goeudarstvennyy universitet (Leningrad State
University)
Hua
July 14, 1960
C11" cost
14,5
11377
Table 1 and 2

no OOPMYJI
e (8)
4
f96
14,

1

916

90
2450
1296

no ,Op,,,.,
e (9)
4
148
14'

14
1296

ToquGe snqene

fG8
15(

Tmqlfas 2

no
Popuyne (8)
42,7
.199,7
241.5
257
0

no (

Popuy-ne (9)

42,7
L

-t4,O

8,5
,
-5
5 3
3

Toliff0e 311Viewte
_

43.9
3

-13,1

-7,8

,
:
:4
-4,8
8

INN

ADAMOVP M.N.; TUPITSYN, I.F.
Theoretical study of reactivity in substitution
reactions of
molecules with conjugate bonds using the free
electron method.
Part 1. Alternant and nonalternant, hydrocarbons.
Vast. LGU
17 no.16:47-57 162. (MIRk 15:9)
(Chemical reactions) (Hydrocarbons)

ADIMOV. M.N. - TUPITSYN, I. F.
--- - 6
Theoretical study of reactivity in substitution
reactions of
molecules with conjugate bonds using the free electron
method.
Part 2o Six-membered nitrogen heterocycles. Vest. LGU 17
no.16:58-
65 162. (MIRA 1~:9)
(Chemical reactions) (Heterocyclic compounds)

ADAMOV, M.V ; TUPITSIN, I.F.
Theoretical study of reactivity in substitution
reactions of
molecules with conjugate bonds using the free electron
method.
Part 3 'Five-membered nitrogen heterocycles. Vest.LGU 17
no.224+18 162. (MM 15:12)
Ii (Witrogen compounds)

L 11117 -630
ACCESSION NR
54TWIMS AF.-FTC,,A5D
AP3002781
S/0051/63/0114/006/0737/0744
AUTHOR: Adam v. M. N,,#. Kagan, Ve Ko; Orlov,_B. I.
TITLE: New method for calculating the 0 tical polari.:,ability of
the hydrogen atom
SOURCE: Optika i spektroskopiya, v. 14.. No. 6, 1963, 737-7"
TOPIC TAGS: optical polarizability, atomic hydrogen
ABSTIMT: Starting with the quantm-dispersion theory expression for
the Polaris-
ability as a function of the radiallion frequency, the authors
deduce an integral
represantation of this fomula applicable to the hydrogen atom and
one-electron
ions. 'ne integral expression was used to r;alculate the
polarizabil-ities of the
hydrogen atom in the ground state and in low-lying excited states
%,ith n = 2. For
the ground state, with increase of the frequency of the radiation
from 0 to 3/8
atomic units the polarizability increase3 monotonically, At this
first natural
frequency (3/8 atomic units) the function has a discontinuity and
changes sign;
further the polarizability agaiii increases and goes to 7ero when
the frequency
equals CLbout 0.404 atomic units. Thus, radiation of this
frequently should pass
through atomic hydrogen without refraction, The behavior of the
polarizabil-ity
.Is a function of the radiation frequency for hydrogen in
low-lying excited states
Card 1/),

L 11117,.63
ACCESSION NR: AP3002781
is similar, ~ut~the.,naturAl~,frequencies.correspondiij to
discontinuities-are
differeA, Orig. art* has: about 66 formulas and U.). tableso

ADAMOV , 14. N.; KAGAN, V. K.; M'RhITE, T. K.
Calculating the Stark effect in the hydrogen atom.
Vest. ILU
19 no.10:31-39 164. (MIRA 11-7:7)

ADAMOV, M-N.; L,VAMT()V, R.A.
-~. ... .... -.-
Calculation of single-ele'-tron three-certer Aniel7n~is.
Zhur. strakt.
khirn. 5 no-50.759-764 S-0 164 (KIRA 18:1)
1. Fizicheskiy institut Leringradskc~o psudar6-,venrlogo
imirez.-
siteta.

ADAMOV, M.N.; KAGAN, V.K.; ORLOV, B.I.
Calculating the optical polarizab.Ility of the
hydrogen atom
by means of a power series. Opt. i spektr. 19
no.2:300-
302 Ag 165. (MIRA 18:8)

ADAMOV, M.N.; REBANE, T.K.; EVARESTOV, R.A.
Variational estimation of values com,.uted In the
second approxima-
tion of the perturbation theory. Teo--et. i eksper.
khim. 1 no.5t
588-594 S-0 165 (MIRA 19:1)
1. Fizicheskiy institut Leningradsko,-o
gosudarstvennogo univer-
siteta. Su'cmitted June 23, 1965.

L 0475P~- MWIF (1) 0 /EI'l
ACC NR1 AP6025963
SOURCE CODE: UR/0051/66/021/001/0106/0107
I
AUTHOR: Adiwiov, M. N.; Wlyedkov, V. D.
S
ORG: none
TITLE: Quadrupolar and polarization potentials of the hydrogen
molecule
SOURCE: Optilca 1 spelctroskoplyn, v. 21, no. 1,1966, 106-107
TOPIC TAGS: perturbation theory, electron polarization, hydrogen
atom reaction,
ABSTRACT: The role of the quadrupolar and polarization
potentials in the quantul-41-
chanical calculation of collisions using second order
perturbation theory was investi-
gated. Consider the system e-H2. The total energy E(r) = El(r) +
E2(r), where El is
the energy calculated fr*m first order perturbation theory and
E2 that calculated from'
second order perturbation theory. El is dominant both as r
approaches zero and as r
approaches infinity. However, the polarization potential E2
becomes dominant begin-
ning at distances r z ro = 2.5 atomic units and continues to
exceed 91 up to a distance
r0at which point 82 starts to become negligible again. In
calculating El using a
Weinbaum wave ftmetion and elliptical coordinates one finds that:
E, ds + dt I 'S P2 (003 8) 4 d1yS p,(coso) Qp,(,,00)~
+ -5 Y
2r3 -TP+IS -2,3
Coo 1/2 UDC: 539.192-: .546.1l..01-.

L 04758-67
k
C NR: AP60259(63
where d = 1.42, 0 a 1.694, S = 0.672, y = 1.228, a 1.409 and P2 is
the-Legendre func-
tion. The first term in the brackets is the nuclear quadrupole term
and the second is
the electron quadrupole tern, while Q is the total moment. The
experimentally deter-
mined value of Q electron ~ 1.1910.07 while in this calculation Q
electron m 1.42 and
Q = -0.596. 92 was calculated to be:
Ej - I a M r-I + 0 (r-1),
2
where aV--0 a 4.9, aV., ~ 6.5, 1/30 V=1 + 2a V=0 5.4. Taking into
account the
slight dependence of a an v one finally obtains the equation for the
total energy:
Q
E (r) - P2 (COS 8) + 0 (r-S).
2r3
Therefore, in the direction perpendicular to the molecular axi3 (v =
0) 91 becomes
larger than 92 when r ~: 18. Thus in the scattering region the
polarization potential.,
does not play a smaller role than the quadrupolar term and must be
taken into consi-
Ideration. Orig. art. has: 5 formulas. [141
B CODE: 2%; 07 SUB'M DATE: 24W;165 ORIG REF: 001 OTH REF: 003
kh
2/2

ACC NR, AP6036952 ( Al
SOURCE C-ODEt---UR/-0181/66/008/011/3173/3176
AUTHORs Adamovp M. No*, Ledovskayaj Yet M,; Rebanep To Ko
ORGt Lenin ad State University im. At A. Zhdanov (Leningradskiy
gosudarstvamyy
universitetv
TITLE: Variational calculation of the polarizability of the
F-center in alkali
halide crystals (point lattice approximation)
-SOURCEt Fizika tvardogo telap ve 8v no* lit 1966P 3173-31?6
TOKC TAGS1 F center, alkali halide, variational mothodp ground
state
ABSTRACTI In order to calculate atomic shifts and frequencies of
local oscillations
in.crystals with defects, it is necessary to estimate the static
polarizability a
of.tho dofacts and ions of the crystal base; this was done both
from above and from
,below. A variational method of the perturbation theory was used
to findo in the point
17,lattice approximationg the narrow interval in which is located
the value of the polar-
."Ai,~bility of the F-center corrrosponding to the model
potential V(r). The following
.I.Jwave function was used to deacribe the ground state-bf the
F-centert
73 4
.7w e
Optimum values of parameter y for NaCl crystals were determined
from the requirement
112

ACC NR, AF6036952
of minimum energy of the electron described by this function
and located in the field
of a nonpolarizable point lattice.with an anion vacancy. The
excitation energy
C Els was found to be
Ty
The estimate from above gave ct > 1 523 and the estimate
frombelow, cL < 15-556
The two sets of estimates for various alkali halide crystals
are tabulated. It is
concluded that the variational calculation gave a precise value
of the polarizability
of the ground state of the electron moving in a field with
potential V(r). Since,
howevery the model potential V(r) describes the F-cantor only
approximately, the re-
sults of the calculation may differ from the actual value of
the polarizability of the
F-center, being probably somewhat high. The numerical
calculations were performed
with a BF,314-2 computerl and the program for calculating the
optimim value of paramoter
Y was written by B. Ya. Frazinskiy. Authors are grateful to I.
V. Abarenkoy for dis-
cussing the work. Orig. art. hass I table and Ii formulas.
SUB COM 20/ SUBM DAM OBFeb66/ ORIG REFt 0051 OTH RM 003
212

iwAmciv, N. 13.
"On the Clinical. Observations of Primary Cancer
of the Liver"
Terapev-ticbeskiy Pakhiv 25:50-52, 1953, USSR
abs
B-80127,, 2 Nov 54

ADAMOV, N.T,
~Rffect of intraostesus blood transfusions and injection
of
therapeutic serum on blood proteins and their fractions in
tuberculosis. Dokl. AN Uz. SSR no.2:63-65 '58. (MIRA 11:5)
1.Okruzhn.oy vo3rennyy gospitall. P~redstavleno akad. AN
UzSSR A.Yu.
YunusovyM.
(Tuberculosis research) (Blood)

ADAHOV, N.T.; MMUMOVSKIY, I.Ye.
Mxpelling ascarids and whipworms by the use of
oxygen in
patientB with tuberculosis. Uzb.blol.zhur.
no-5:69-73 '58.
(MM 12:1)
l.--Okru2hnoy voyennyy gespital' Turkmenekogo
voyennogo okruga.
(atYGBN--TRMMF-",IC USE) (URMATODA) (ASCARIDS AND
ASCARIASIS)

ADAMOV, IT.T.; 111KISHIN, K.Ye., kand. mad. muk..;
SIMY-011, F.K.
I--
Diagnostic value of spot roentgenography in pulmonary
tuberculosis.
Vent. rent. i rad. 33 no.6:19-22 11-0 '58. (MIRA 12:1)
(TUBERGUIOSIS. PUD4011LU, ding.
aimed x-ray (Rua))

ADAMOV, N.T.
Intre-oassous blood transfusions in pulmonary
tuberculosis and
their effectiveness [with slimngry in French].
Probl.tub. 36
no.1:64-67 158. (MIRA 11:4)
1. Iz Tashkentakogo okruzhnogo voyennogo gospitalya.
(NMERCULOSIS. PUIXONARY, ther.
blood transfusion, intraosseous admin. (Rua))
(BUND TRAPSYUSION, in vraious dis.
pulm. tuber., intraosseous admin. (Rua))

ArAMOV, 14. T.: Master Med Sci (diss) -- "Intraosteal
transfusions of blood and
therapeutic serum in pulmonary tuberculosis and their
effect on hematopoiesis
and certain biochemical indexes". Samarkand, 1959. 20 pp
(.Samrkand State Med
Inst im Acad I. P. Pavlov), (KL, No 14, 1959, 122)

ADAMOV, N. V.
S-ar quelques proprietes des intep-rales dlune equatinn du
sec-nd ordre a coeffici
periodiques. C.R. Acad. 7ci., 107 (19,113), 1280-1282.
SO: l4athematics in the USSR, 1917-1947
edited by Kurosh, I...G.,
'larkushevich, A.I.,
Rashevskiy, P.K.
Moscow-leninf-rad, IP49

t
7
oscillat on d s i-,~'--c'Crahs do Vcquati:~:-. ,u OrcIre,
Cllocffv,'-,~ntf~ pcrlodi,mc-~3 C~t f7ur quOl Olo at r- i-
e'. o t or- F~vo~rsva u -u lxiv%~.'-Ll
'Lwavnoni::~'l pervo~70 P=, 2c')
S j. t',C U
edit-d by Kw-osh, A.G.,
;"as'-evskiy, P.11'.

ADA"10AT, 14. V.
0b oemoln metode posladovatellnykh priblizheniy. DAN,
P-7 (193F', 21C~-224.
SO: Mlathematics in the USSR, 10,17-1947
edited by Kurosh, A.G.,
'larkushevich, A.I.,
Rashevskiy, P.K.
Moscow-Leningrad, 194F

ADA-M'OV, - N. V.
0 nakhozhdenii periodicheskikh resheniy obyknovennogo
differentsiallnogc, uravreniya
pervogo poryadka metodom posledovatellnykh p1riblizheniy.
DAN, 19 (193F), 15-20.
SO: Mathematics in the USM, 1917-1947
edited by Kurosh, A.G.,
Markushevich , A. 1. ,
Rashevskiy, F.K.
Moscow-Leningrad, 1948

-ivz

--, - - . I - - - - , - ---- -- -- - - - - .-
I ~'. - - ~; I - - - - - - , I - ~ -- -- -- -- - - -- '. . - - - , - - -
11~
~.~
[Standard technological charts for installing interior gas
-MrAl 4 nA a 1 Ti-nnvvn 6-"#!- --

KARASEV, A.P., inzh.; LISITSYN, S.N., inzh.; MAZO,
A.V., inzh.;
ADAMOV, O.Y., inzh., red.; GELIN, M.M., inth., red.;
red.izd-va; LAGUTINA, I.M., tekhn.red.
(Standard technological designs for the plumbing of
interior cold and hot water-supply and sewerage
systems)
Tipovye takhnolo.vichaskie karty na proizvodstvo
rabot
po montazhu siB tam vnutrennego kholodnogo i
goriachago
vodosnabzheniia i kanAU20tgii. Moskva, GoB.izd-vo
lit-ry
po stroit., arkhit. i stroit.materialam, 1958. 4) p.
(MIRA 12:9)
1. Russia (1923- U.S.S.R.) Gosudnrstvennyy komitet
po delam
stroltellstva. 2. Montazhnyy otdel Gosudarstvennopo
pro-
yektno.go inBtituta Santekhproyekt (for Karasev,
Lisitsyn, Mazo).
(Plumbing--Standards)

inzh., red,; GELIN, N.M., inzh., red,; KNITS, A.P.,
red.izd-va; LAGUTINA, I.M., tekhn.red.
I
[Standard instructions for erecting steam hosting
plants]
Tipovye tekhnologicheakie k6rty na proizvodstvo rabot
po montazhu
otopitelluykh kotellnvkh. Moskva, Gos.izd-vo lit-ry
po stroit.,
arkhit. i stroit. materialam, 1958. 50 P. (MIRA 12:3)
1. Moscow. Gosudarstvenun proyaktnyy in8titut
Santekbproyekt.
(Boilers)

--ADAMOV, O.V., inzh.,red.; GELIII,M.M.,inzh.,rF3d.;
IWITS, A.P., red. Izd-va,;
--------LWtUTINA, I.M., tekhn. red.
[Standard technological diagrams for installir~g central
heating
systems] Tioovye tekbnologinheakle k-arty na
proizvodetvo rabot
po montazhu sistem tsentralinogo otooleniia. Moskva.
Gos.izd-vo
lit-ry po stroit, arkbit. i stroit. materialam, 195B. 71
P.
(MIRA 11:12)
1. Russia (1923- U.S.S.R.) Gosudarstvennyy komitet po
dalam
stroitel'stva.
(Heating)

GENIN, H.Ta..inzh.; XHOTKKVICH, S.G., inzh..;- ADAMOV,-
O.V.,_1nzh., retsenzent;
VINOGRADOV, I.Ta., inzh., retsenzent; BELOUSOV, V.V.,
inzh., nauch-
nyy red.; NI1W4YAGI, D.K., red.izd-va; MOVEDEV, L.Ya.,
tekhn.red.;
STEPANOVA, B.S., tekhn.red.
[Machine tools and mechanisms used in sanitary
engineering] Stanki
i makhanizmy dlia proizvodBtVa sanitarno-tekhnicheskikh
rabot.
Moskva. Goo.izd-vo lit-ry po stroit., arkhit. i
stroit.materialam,
1959. 179 P. (MIRA 13:6)
(Sanitary engineering--Equipment and supplies)

ADAMOV, O.V. ; FIlflMLISHTHYN, S.M.
".1". . .. ~--Yofk practices in pipe bending. Yod.i
san.tek-h. no-9:31-32
S 159. (MRA, 12:12)
(Pipe bending)

ADAMOV, O.V.; IVAITOV, K.N.
------ -.-
Length of short t1ureads on pipes of sanitary
engineering systems.
Vod. i sau. tekh. no.11:15-17 V '59. (MIRA 130)
(Pipe fitting)

MIRONOV, Konstantin Androyevich; SHIPETIN, Lev
Ionifovich; LIVOV, M.A..
kand.tokhn.nauk, retsenzent;--ADAWV-, P.G., inzh.,red.;
POLYAKOV,
G.F., rod.izd-va; TIKIMNOV. A.U., takhh.red.
Peasuring Instruments fnr une In connection with thermal
procasses; refaronce manual] Toplotekhnicheskia
izmeritellve
pribory; apravochnya materialy. Izd.2., parer. I dop.
Moskva,
Gos.nauchnn-tekhn.izd-vo mashinostroit.lit-ry, 1958. 896
p.
(Physical instruments) (14IRk 11:12)

S/112/59/00O./012/05-3/097
A052/AO01
Translation from~ Referativnyy zhurnal, Elektrotekhnika, 1959,
No, 12, p, 192,
# 24962
AUTHOR;, -Adamov, P.G.
TITLE. Problems of DeZ21opintthe Production of instruments and
Automatic
Devices and of Designing New Types of Them
PERIODICAL~ Opyt raboty prom-sti Sovnarkhoza (Moskov. ekon,
adm, r-n), 1958,
No. 4, pp, 36-43
,EXT,, The prospective plan of development of the Moscow
in.strument--indus-
try for 1959-1965 is discussed, There are 11 illustrations.
Translator;s note,: 1-nis is the full translation of the
original Russian abstract.
Card 1/1

Val; I im " - - - .. - - - ~ . -I-1 r-
A 5 - - - AIL',
.A k
Kbac" ;A& imp Whirl I v I=* T iffiATWO t9o g0& [CoIj to the
In Iran in January 19191 Prirv&, Mouour, 39(2):20-29. Feb. 1930.
2 figs, MC-Durins it* winter 19411,1949, great tcmp~rat ire
amoinalies o,,t-urIvd over
90 Furopa "I C"trAl Asia. Continuous souvratorrus mQ omm
(mvilitil um rrrd o%vf all of
L4jrki-tsn. 'Ile trnipersturv fell to