SCIENTIFIC ABSTRACT SEIDOV, A.C. -
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CIA-RDP86-00513R001547710007-9
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Publication Date:
December 31, 1967
Content Type:
SCIENTIFIC ABSTRACT
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S19IDOV, A.G.
Breaking down the Maikep series in the area of Kazakhmamedtepe
(Kirovabad) by dyeing colloidal dispersion minerals. Dokl. AN
-Azerb.SSR 11 no.7:471-474 J1 '55. (MTRA 9:1)
I.Institut geologii imeni akademika I.M.Gubkina'All Azerbaydzhan-
.skoy SSR.
(Kirovabad-Geology, Stratigraphic) (Clay)
bTIDOV. A-G.'
Lithological and chemical characteriatics of clays and the cyclic
recurrence of the Maikop series In the Terter Valley (Mir-Bashlr).
.Dokl.AN Azerb.SbR 11 n0-11:78)-786 '55. WaA 9:5)
1. Institut geologii imeni akadeimika I.M..Gubkina AN Azerbayd8han-
skoy SSR. Predstavleno deystvitel'nym chlenom AN Azerbaydzhan-
skoy SSR Sh.A. Azizbekovym.
(Terter Valley--Clays) (Terter Valley--Geology, Stratigraphic)
SEIDOV, A.G.
I -- -:.,!.si~y-' of colloidal despersed clay minerals in the Maikop gas
and oil source bed of the Kirovabad oil-bearing in Azerbaijan.
Vop.min.osad.obr. )/4:613-638 '56. (MLRA 9:11)
1. Institut geologii Akademii nauk Azerbavdzhanskoy SSR, Baku.
(Kirovabad (Azerbaijan)--.Clay)
(Kirovabad (Azerbaijan)--.Petroleum geology)
SULTANOV, A.D.; SEIDOV, A.G.
"Minerals in sedimentary rocksw by I.A.Proobrazhanakii and S.G.
Sarkisian. Ravieved by A.D.Sultanov and A.G.Seidov. 4v.AH Azerb.
So no.io:167-169 o 1560 (MLRA 10:3)
(Rocks, SedimenLary)
'$EIDOV, A.G.
Petrology of Pliocene and post-Pliocene deposits In the Sar7dzhallar
regrion. Izv. AN Azerb. SER no-12:91-107 D 156. (W.U 10: 4)
(Sarydzhallar region--Geology, Stratigraphic)
SMIDOV,, A.G.
Minernlogy of I:, clays of the Maikop series In the KazAkhmnmedtape re-
gion Lin AzargRijani with summary in Russian]. Dokl. Al Azerb. SSR
12 no-7:485-489 '56. (MLRA 9:10)
(Knzakhmp-medteps region--Clay)
SEIDOV, A.G.
"Lithological and mineralogical characteristics of clays found in
producing strata of Azerbaijan." A.G. Koessovskala. Raviewed by
A.G. Saidov. Izv.Aff SSSR.Ser.geol. 21 no.2:108-113 F 156.
(MLRA 9:5)
1. Inatitut geologiiAN Azerb.SSR, Baku.
(Azerbaijan--Cla.v) (Kossovskala, A.G.)
. I~'r' ,
)2 2 2
C II (kl~k --'[(A -kl+, -
W D + WA-E -) 6 ( k2
L
4k 1 k2 2 4 PL 11 4
2 1)
- (E,, + A ~--- EEE 6 ( k' + IL+W)exp P. /kT 6(E E -E
-k1 _k nk nk k - k
2 2 1 2 2 1
where
Card 2/': n,, = (exp E ~L /kT-1) -1 ; nk-=(exp(Ek- ~ )/kT+ 1; 1( klIk2)_
SOV/126-7-2-25/39
Electron-Spin Relaxation in an Antiferromagnetic
is the exchanye integral for a conduction electron and a
d-eleci I is the reciprocal lattice vector, E is
the energy of a spin wave, and E is the energy oY a
conduction electron. The remaiang symbols have the
saine meaning as in Ref 4. Calculations of W,-, were
carried out in the same approximation as in the
corresponding ferromagnetic problem (Ref 2). It turned
out that 2 2 2 2
- iz::~ I J K0 1 k8i 1 0 zi
WC-0 2 - - _P 2 2 %T TE
27 hA kT 21T- hz A T
where 1 0 is the s-d exchange integral inside om atom,
J is the exchange integral between the d-shells of
neic-hbouring atoms 7 is the Fermi surface energy,
A is=D the transport i3tegral for a conduction electron
in a one electron theory, @ N is the Neel point, and
z is the number of nearest neihbours. 13 In a rough 14
estimate of W one may take A-,- 10- erp, I --.- 10 erg
C-e 0 01 0
Card 3/4 (Ref 2), 6 --, 100 K and '0_12
N L. er6. It follows
SOV/126-7-2-25/39
Electron-Spin Relaxation in an Antiferromagnetic
that lovi temDeratures-for which the calculations were
carried out VI C-e_'_~ 100/T . Details of these calculations
will be given ii, a subsequent paper.
(Note: This is a complete translation)
ASSOCIATIOM: Urallskiy gosudarstvennrj universitet imeni A.-MI.GorIkogo
(Ural State University imeni A. 1A. Gor'kLiy) and
Bakul,universitet (Baku University)
SUBLINTED; January 12, 1958
Card 4/4
9Z3
AUTHORS: Seidov, Yu,, and Berdyshev. A, SOV/126-b-1-20/25
TITLE: ationv
Spin-electron Relax -in Antiferromagnetics
PERIODICAL-, Fizika metallov i metallovedeniye, 1959, Vol 8, Nr 1,
PP 147-150 (USSR)
ABSTRACT7 If the system of spin waves of a ferromagnetic is in
some way brought out of the thermal equilibrium state,
it may re--establish this state via one of the following
three basic mechanisms,
1) interaction of the spin waves with each other;
2) interaction of spin waves with phonons;
3) interaction of spin with conduction electrons.
The first two mechanisms were considered by Tsukernik
(Ref 1), The present paper is concerned with the third
mechanism. The calculation is based on the s-d-exchange
model put forward by Vonsovskiy et al, in Refs 2 and 3.
The energy operator is taken in the form of Eq (1),
where J(_Z1, 'n ) is the d-d-exchange integral,
- _'> _10. 2
n n < 0. I(k' k is the interaction integral
J( I
1 2 1' 2 _41
Card 1/4 for the d-electron with states k 1 and k 2 of the
conduction electrons, a nc and a k. are the Fermi
66903
SOV/126-8-1-20/25
Spin --- electron Relaxation in Antiferromagnetics
operators, The transition from the Fermi amplitudes
ano to the spin operators and then to the b n operators
in the Ziman formjj~ism (Ref 5) may be carried out using
Eqs (2),.,,j~here w is the reciprocal lattice vector so
that el-IM is equal to +1 at the sites of one sub-
lattice and --l at the s.ites of the other, The d-part of
the operator given by Eq (1), H dd' is the same as that
in Eq (24) in Ref 5. The eigenvalues of Hdd are the
same as ZiMarLIs eigenvalues. The substitution for the
diagonalization of H dd is given by Eq r(3), where the
symbols are defined by Eq (4), and the C 'A are the Bose
operators., h denotes summation over nearest neigh-
bours, a h ei~it, H is the anisotropic magnetic field
and E is tae energy of a spin wave with a wave vector
~L and H 0. The sum of the operators representing
the energy of the conduction electrons and the energy of
the s-d-exchange interaction consists of two parts, the
Ca,d 2/4 first of which is given by Eq (5) and describes the LKI"'
translational ener-gy of the conduction electrons
SOV/126 - 8 -L-~.jo/ 2,5
Spin-electron Relaxation in Antiferromagnetics
"magnetized" by the spin wave field, Eq (5) may be
diagonalised in the same way as H d~' As a result,it
turns out that the levels of s-elec rons split into two
sub-.bands and the gap between them is proportional to
the magnetization of the sub-lattices, However, this
effect is not considered and an estimate is made only
of the effect of the s-.d-exchange interaction with free
conduction electrons. This interaction is described by
the second part of the s-d-exchange interaction operator
(Eq 6). Substituting Eq (6) into Eq (3) one obtains an
operator which de.scribes inelastic collisions of
conduction electrons with spin waves in which one spin
wave is either emitted or absorbed during each separate
collision. The change in the number of spin waves per
unit time can then be found in the usual way (Ref 7) and
is given by the last equation on p 148, where nk is the
Fermi distribution function a,.,c n is the Bose
distribution function. The a-,-Exagellrelaxation time
can then be shown to be given L Eq M~ It is shown L'K
that as a rough8 estimate this formula may be replaced
by AN,
Card 3/4 10 /T.
6690-4
SOV/126-8-1-20/?-5
Spin--electron Relaxation -in AntIferromagnetics
There are 8 figures and 8 references., 7 of which are
Soviet and 1 English.
ASSOCIATION; Urallski'y gosud.,ars-tvennyy universitet imeni
A,, M. Gor,kogo (UralfiState University imeni A.M.Gorlkiy)
SUBMITTED,, July 26., 1958
Card 4/4
85153
S/181/60/002/009/044/047/XX
B004/BO70
AUTHORS: Abakarov, Dzh. I. and Se dov, Yu. M.
TITLE: Theory of the Magnetic Suscept . ilityvof the Polaron
PERIODICAL: Fizika tverdogo tela, 1960, Vol. 2, No. 9, pp~ 2264-2267
TEXT: The pRrpose of the work was to calculate the statistical sum of the
Hamiltonian H expressing the interaction of the electron with the lattice
vibrations in a homogeneous magnetic field, and to construct a thermo-
dynamics of the polaron in the magnetic fields The statistical sum is
written as Z = Sp exp(_'A~), where 1/kT. From this, the following
equation is obtained: 1
(2)=Z(o) 3/2/j-Tr).
z (2p) (-(/shp) [~(chpv) ~1 v2).i/(2f1 ---A)ln
7-
0 1 - 1=71
(9). Here, A = (2/t)(chr - chtv)/(shr,(l - v r
2 hG~/2kT, andp=Aho~/2,
The limiting cases were studied. 1 1 A'~K 1 . Then E
=
E )112(l +,p2
(jf,) -ViY (hO/A /72)d (12'~ For r = 0, equation (12) goes
Card 112
3hlDOV., Yu.M.; GLISFYNOV, N.G.
Spin wave spectrum and megrietic susceptibility of the GuC12- 2H20
compound. Izv. AN Azerb. SSR. 'Ser. fiz.-mat. i tekh. nauk no-5:
75-77 163. (MIRA 17:3)
L56-,2
S/126/63/015/001/0c,3/029
E032/E114
A HUR:
TIT LE, ()n the theory of nuclear magnetic resonance (N~M) in
Cerro- and ntitiferromagnetics
PLUIODICAL: Fizilca meta Ilov i metallovedeniye, V. 15, no. 1, . 1963,
32-35
TEXT: The Green temperature functions are used to obtain
forrinilas for the N19Z frequencies in ferromagnetics and antiferror
magnetics (N.N. Bogolyiibov and 9.V. ryablikov, DAN SSSR, v.126,
1-959, 53. D.N. Zubarev, UFN, v-71, 196o, 72). In the former case
I-tie contrihiition (hip to conductiorl electrons to the MER frequency
is allowed for by including terms in the Hamiltonian which
represent the hy'perfine interaction of polarised electrons with
nuclei (M.A. Ruderman and C. Kittel, 11hys.Rev., v.96, 1954, 99)-
In thp case of antiferromagneticts the effect of nuclear spins on
tho antiferromagnetic resonance frequency is calculated. It is
noted that in distinction to ferromagnetics, the antiferromagnetic
resonance frequency for 11 2 = 0 does not vanish.
Card 1/2
ASKEROV, B.M-Y- SEIDOV Y M red.; BOGDATLISHVILI, D., red.izd-va;
A-_
Ij3RAG7L7UV,__R.__, feZm. red. __ -#
[Theory of transfer phenomena in semiconductors] Teoriia
iavlenii perenosa v poluprovodnikakh. Baku, Izd-vo AN
Azerb.SSR, 1963. 123 p. (MIRA 16:9)
(Semiconductors)
'CF I
.1.3 SSION h1i: AP4017569 S/0249/63/019/010/0015/Wl7
,i-W-MOR: Saidov, Yu. 1-1.
TITSE: Orbital diamagnetism of conduction electrons in ferroma netic metals
(?resented by Z. 1. Mialilov) academician, AN Azerbaydzhan,
SOURCE: AAN AzerbSS,11. Do)-dady*, v. 19, no. 10, 1963, 15-17
TOPIC TAGS: or'bital diamagnetism, conductiod electron, ferromagnetic metal,
ene.-Qr spectrun.
ABSTRACT: The influence of the internal field in ferromagnetic melk-lals on the
3z J. L,
m
tion.of conduction electrons is considered. It is found that for a vector
Dotential of the forn, r
A
2
The external field being directed alon&the 2 axis, the onerMr spectrum of the
conduction electrons in the effective ;d~ernal and internal) field is of the
N
L+ a+
I a+ a.,
t
2 j 2
-'a ire
Card 1/2
ACCESSION NR: AP4017569
-in tUs expression,
2)*
Lin
(H,+4,jAfo
Mc
E:k -E
N.
a are the Fermi operators and lnko are th.e state quantum numbers of the conduction!
electrons ih the effective magnetic field (In is the Landau level number and k0
is the z component of the wave vector). Orig. art. has: 10 equations.
ASSOCIATION: Instiiut-fiziki (Institute of PlVsics;~
SUBMNITTED: 290ct63 DATE ACQ# 18MAr64 ENCL: 00
SUB CODE: PH NO REF SOV: 003 OTFM: 000
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ASSOCIATION:
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_1L1 - .1 1
ACC NR: AP6000867 SOURCE CODE: UR/01'i'65/007/012/
-36,35/3638
AtJTHORS: Guseynov;-N. G.; Seidov,_ Yu. M.
ORG: Institute of Physics AN AzSSR, Baku (Institut fiziki AN AZSSR)
.TITLE; Contribution to the tbeory_of-thermal expansion in magnetical--,
ly ordered crystals 2-1 q 45- t~,
SOURCE: Fizika tverdogo te.1a, V. 7, no. 12, 19 3635-3638
TOPIC TAGS: thermal expansion, critical point, magnetic crystal,
.magnetic domain structure, antiferromagnetic material, spin wave
'ABSTRACT: Inasmuch as knowledge of the effect of magnetic ordering
on, the thermal properties yields information concerning the dependence .
.of the exchange integral on the interatomic distance and other data,
the authors derive a general formula for the magnetic contribution to..--
'thermal expansion in magnetically-ordered media. The calculations
pertain to crystals with structure of MnF 2' The standard Green's
functions technique is employed. The formulas obtained are applicable
Card 1/2
L 1,11117-66
'ACC NR: AP6ooo867
to magnets with tetragonal syngony in the entire temperature range
where magnetic ordering exists. In particular, expressions for the
spln-wave-induce~ thermal expansion in ferromagnetic and antiferro-''~;~
magneticcrystal Xare derived from the general. formula. The tberrrial
coefficients of antiferromagnetic crystals In both the
Parallel and perpendicular directions have terms both linear and
.Cubic in T at values above a certain critical temperature, and an
;exponential temperature dependence below this temperature. The
icritical temperature depends on the susceptibility and on the
anisotropy coefficient. It-is shown that the effect can be observed
,experimentally. Orig. art. has: 10 formulas.
SUB CODE: 20/ SUBM DATE: 2'6Mar65/ oRiG,REF: 004/ OTH REF: 003
Card 2/2,
ACC INRi
AP6036052 SOURCE CODE: IJR/0056/66/051/004/1084/1089
AUTHOR: Guscynov, N. G.; Seidov, Yu. M.
ORG: Institute of Physics, AN AzerSSR (Institut fiziki AN Azerbaydzhanskoy SSR)
TITLE: Maanetic impurity levels in antiferromagnetics
SOURCE: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 51, no. 4, 1966,
1084-1080
TOPIC TAGS: maonetic crystal, crystal impurity, -impurity level, Green function,
C,
antiferromagnetism, antiferromagnetic crystal
ABSTRACT: The problem of local magnetic excitations in antiferromagnetic
crystals with a sinale impurity center is consideted. A general solution of the
problem of oscillations of the spin system of an antiferromagnetic crystal contain-
ina an impurity magnetic atom is presented. It is sho wn that the Green function
01 such a. crystal satisfies the Dyson equation and can be expressed in terms o f the
Green function of a perfect crystal. Some of these local levels may be smaller than',
the spin wave gap in antiferromaornetics. Orig. art. has: 16 formulas. [Authors' 1
abstract] M]
r~,,q 1/1 SUB CODE: 20/SUBM DAT)!-,: 07Feb66/ORIG REF: 004/OTH REF: 002/
X F) JA 1),k
tegralL eqU;* ayin
a nonlinear in del g. arg~Meht.-,..
'conditions fojL. convergence of Tdnellii,it~koximation-s'~: e
Card'. 1/2
E~7(~)/EWT.(m) D P
ACCESSION MR: AR56i4jbg ---UR/0058/65/00O/004/V02VVO22
SOURCE: Ref.-zh. Fizika, Abs. 4VI71
-z. r
AUTHOR: S'eidov-,-
r
65
TITLE: Speed of nuclea6 reactionslin a dense medium
CITED SOURCE: Tr. Shemakhinsk. astrofiz. observ. v. 3, 1964, 25-39
s6
TOPIC TAGS: dwarf.star, nuclear reaction, heavy nucleus, proton interaction
TRANSLATION: The problem oe the'rate at which nuclear reactions take place in a
dense medium is examined with regard to heavy condensed nuclei under conditions
which may exist in stars of the white dwarf type. Calculations showed that the
rate at which energy is liberated as a result of the proton-proton reaction with
regard to the effect of condensed heavy nuclei (an, 10) is much lower than in cal-
culations with plasma models. There is a sharp minimum in the rate at which energy,--7
is liberated as a function of density in a dense medium. In this particular case,
this phenomenon may result in a reduction in the rate at which energy is liberated
from the surface to the center of a white dwarf. A. B.
SUB CODE., NP, AA 00
Card
SE1IDCVA) A. A.
SEIECIA, A. A. "The Treatment of Improperly Healed and Freshly
Broken Femurs by Intraosteal Fixation with a Iletal
Pin." Azerbaydzhan State Medical Inst. Baku, 1956.
(Dissertation for the Degree of Candidate in Eedical
Science)
So: Knizhnaya Letopis', No. 19, 1956.
M
TAMB RANSKIY, D.N., dotsent; SE DOVA. -A.A..- mladshiy nauchnyy sotrudnik
Surgical treatmont of fracturse of the femur by nailing. Vest.khir.
77 no-10:133 0 '156. (MLR& 9: 3.2)
1. Iz Azerbaydzlianskogo ini3tituta ortopedii i voestanovitellnoy
khirurgii, Baku,,
(FBWM-IPRACTURE)
S;-.idol:a K. - "The ef.~eCL ~)T' or-:,anic nietrogen soli improvers obtained ,from
acid -Detrcleum asnhalt on the Zield of agricultural croos", Izvestiya Akad. nauk
Azerbaydzh. SSRI, 191:9, No. 2, p. 6,8-79, -, Tr Armenian, resume in -Russian),
7
17 July (L#-Lopis 'Zhurnal 'nyPh St~,reyr, 1?, 191,0).
SEnWA, Kh.K.
Effect of nitrogen-organic fertilizer on corn and sunflower yields.
Dokl.AN Azerb.SSR 11 no.10:709-712 '55. (MLRA 9:2)
l.Predstavleno de*rstvitellnym chlenom AN Azerbaydzhanskoy SSR A.I.
Kareyevym.
(Corn (maize)) (Sunflowers) (Fertilizers and manures)