SCIENTIFIC ABSTRACT TALALAYEVA, T.V. - TALALYAN, A.A
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December 31, 1967
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SCIENTIFIC ABSTRACT
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Examination of the Structure of Lithium S/020/61/136/003/018/027
Alcoholates by the Yethod of Infrared B016/B052
Absorption Spectra. O-Li ... 0 Bond
vaovline or fluorinated oils) (Table 2). Since tert.-C4H9OLi is closely
associated, the authors conclude that lithium alcoholates aAd unbranched
aliDhatic radicals are even more closely 4seociated.,This explains their
insolubility or low solubility in solvents in which H~OLi is easily
tert'-C4
soluble. The authors approximately assigned the bonds of the four latter
alcoholates to the comDlex oscillations of the associated O-Li groups.
A more accurate assignment, however, will become possible by further
investigations. There are 2 tables and 21 references: 4 Soviet, 1 US, 3
British, and 2 German.
ASSOCIATION: P-4ziko-khimicheskiy institut im. L. Ya. KarDova (Physico-
chemical Institute imeni L. Ya. KarDov)
SUTAITTED: September 14, 1960
R R
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Card.3/3
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AUTHORS a a--, a.-; :~od~cnov.
T III' L E -letr.
PERTODIC,Ll flaur- SSSR Do` ady '40 no 7 - 85 0
1 i th ~u-r s ry s ab! 4 r. d i e,:`~ e -her and . thus 1~ I-e the
-a r cm a ' i c II th i u _- c o m,,- ou nd s ~h en v 1 11 h --,.; m a r. d z :, I v I I h i u w H, 2. c h f _- rm,
ternary :ompiexes of .-e =m"Posi-tion 2RLi-LiIX-2(C,-7,~) C 4r. ether soniu-ons
(Pef; 2 IL - V . Talalayeva , K_ Kocheshkov , DAN 104 , 260 (1 )c The
au t h c. r s 7-nvesti-Eated whether such ternary comi2lexes als: formed in the case
' meth--! -Ift-_ium, ,=rnary zom,-lexec cf r',Ie
I Cr-;-sta11_4ne
o
C Ii3Li, LiX 2 (C J2 0 (X Br, 1~ be isola--d from e~h;er solu-ions of
-1. HI - 1 4 u.- were obta:.--=d 'b- rea-tinz- ~e-,hZi chloride
__ n wh,-ch - - - .7 -
~cdide These c=lexes are s1-.ab-.-_ 1- ar=
od i d e d e e ra e -
i'ri7iarily !nt~ lt~ss
in case of 11-_~-1---
--ae _cS eXcess
Card
Ternaf-- com:Ae-e~i of met-yl
sclu-~-,*or. . z rys t- all in e pr~~ -- J- pi t a tes 5 n
u b r o,-,i 7. d e and ether are '13-med e CH',Ll--2L--,Br 3,(C.H., '0 or
CHT Li 5LiB-r,7(C H 0 This behavior Is simliar -,o that of binary ,!om-plexes
3 2
of al i. uha t i -- I i t h i um c o mp o u nd s w _i '-, h I -i th i u m., h al -, d e s IRL'-'-nLiX. n from 1~4
to 6) ~ which form. in the -reac-rion ~f alk-,,,-. hal -des and alInhatic RLi in
hydrocarbon media The monoetherat-- -fL methyl, 1--th,=. CH,Li-(C')H % 0,
- 5 )2
~,,uld b,? :s~lated 1"t-oz: the Pa'bcve-mentiont3d scl,-ltzons of m-ethyl
1 i t h a j!-,i ThIs -.a.-,.-~,Dund con'a---ns small of L4-Cl are
~,robably fine :~~-wder an !R cha--:te-~st~c
-rl,-~al , lnt~ ::ethyl thi-,;,-,. -s cbtair I
ed
re,- i ~ a - ed ' vcm e t 1, er s ~l u t i o n s by x:- e s s n - .bent arle an d h e ~rec 1--i tate
L j - -
dried in vac-io at :000C (Ref 7t A N Rcd.;-.--nov, D- N. Sh.'--~crin. T V.
Talal-ayeva, K A K o c h e s v . DAN 6 1 z SSS R OF-1-11-4
'0; rz%, AN SSSR, ser, z T. L Bro,.,m T
Ro i's i C G.-.: S C.- c r
is , howeve
0 r n n"= 7~:! C -oi- tions, a n d
c is :hloride t,.es Y r t~ s -1; 7:~ e rh I t'- 4-
ass-2-- at~d ~~.n es e-' -ir zo-rlex
I_r L e I
Card 2/5
2.z
Tiz!rnar-. of me th
C bate Of
b n - -en t art?
extre.,,ie inflar.'15c!.071 11 in Etir Orl-IS C-11 uyrol-sis of ~he reaultant powder
-at 2L~00.' accurdin~; to Ref- 0/ (K Zie.---ler. h Nagel Patheic-er, "s- anorg
u . a 1! 6 emn Chem , 262 34 5 (1955)) tiethyl lithiuim and methylene
..i'- , thium. .-iere used to ~,ol~rmerize ethylene with T i~
A K--cheshkov. V A Kargin, T V Talalayeva, T I Sogolova. 0. A.
Paleyev, Vysckomiolek. go-yed .- -1, 152, (1959); J- Folym Sci , 34, 121 (1959D
The IR spe-ti-im. of CH 3 Li in the ranee 2000-650 cm-' is not. afffected by
forma--on ~D~ t'-e ternarZ~ comj~lex of CH Li w4ti, ~-al~de and e*her
3 - 1-
R e 8 A '~cdionov T V T-'.Iala--,ayeva 1) Sh o --r., n , K , k
Ko c 11 e s c A:'. 0 ')-,6 0 The ca,;abllitv o~ for :Lr,~- ternaz~y
c o::!,c I e x;-~ s v; i h e a-nd litiiium bromide is no-, li~.Iited to -nli-2hatic and
arr,-,ati C -~Li but becomes a1sc evi-dent in, a s e o I ium ace tl; -L
des
,h,en i,:u-re acetj-lcn~~ is introdu~:ed int~D an s.1'.1tion of RLi
C;- CAI
" ;; = i-: -~ 11* ~: \ (2nta4ni,,.-- an equ~moleculaz- quantity of lithiumn
v;h:Lch =--,a-ns b,rc..-,-ide
b v i d acetylide -,-~eciu-,tates
.
Card
S.U.10NOVY A.P.; SHIGORIN, D.N.; TALALAYEVAL T.V.; KOCHESHXOV, K.A.
Infrared absorption spectra of some R - 0 - Li compounds.
Dokl. All, SSSR 141 no-3;665-667 If' 161. (MIFF. 14:11)
1. Fiziko khimicheskiy institut 3.m. L.Ya. Karpova. 2. Chlen-
korrespondent AN SSSR (for Kocheshkov).
(Lithium organic compounds-spectra)
V
'I, 1 1 ;1:." V;I.T
v n
7t
r n n::
r r,,,,y ~7,, rt, - n i yav r.,,j ;Y4-
n I tt v !7 i !~i n-, tit k r o u rl arvi
0:, 1 01 i th r-
-.Q In T-~ L, o- , m- ru-11 P-no th,,- i- j'~
otvr~~n~, a.
:)tyr~nc. 'he
te r , 2 - 52in,-,I:; i fior ( Sqd 11M 3 tl~~,ra LP Or r.
fn to initiator. Tile morloner nixtiiro, which was aidvn crop-
a!'L,2r :.catinFl- Lr, 60 - 90('C, cantaim-4 azoisobutyric --Zii din-;Lrilc
-i ~In: tinLor. Elpven copolymcirs of the albove nionomors were ob-
-,.' -d. .,',"h,ir iomprnitiano and prap~-rrdec, tire in Table 2. Til- h-it
v
!11 ~1', -7 th t h
p Y:.,, An t _w, tha f 1 "11-1 C I ur~ ro-
ncn'l L ro t!t!p- t, I'
tno "I"C
r :I :T ty ront: r -, in,;A und-i' i;~ni 1,r cn i i t itin Th
1,w :nincontr,.t a, :-.*,i;Mti tut,- 1, 7 ty r , n mu I v,
:n t~! t-m,~ extr,m.-ly low milo-:ul'ir we~lrht of Ov, pro-
"'h,, ru 2 tib ~ ?a The EnF! -,h- Inj;im - r f~r ii~
f-2 Q o
in J - Sr i 20 , 48 1 ~
V66; :-'. Prober, j.
ri,; t -i mlo I -~'mi 1 y:L rnyxh r, oyt~,I i rtoz: y AN '.;jl;.i till) t I util
r, cu la r C pound s o th~, ,.3 i
A ri 1 1 1 196 1
olyuxrin-i on tirle, yi,~14, co.-apo.34ton :*,:i intrin,-;ic vJ s-
1- Lei-,pnd : (,k) ieni:th, ho-arg; (B) copolymer
k C compor, i t )n of copcily-mer D) i -, tri r,.-.ic -v i3cclsi ties
o!, til., soluti"), , of C-,~Oolymcrs nt 20oC; copolmmers of
SIMONOV, A.P.; SHIGO.-IJN, D.N. ; L4LPtLAY~V
__ ~A -T-0 V. ; KOCIIESHKOV, K ~ A.
Association of +,--rt.C H-OU in the gaseous state. Izv.AN SSSR.-
l126' I
Otd.khim.nauk no .o: 162. !aRA 15:9)
1. Fiziko-khimicheskiy institut im. L.Ya.Karpova.
(Lithium butoxide-Spectra)
SDIONOVi A.P.; ShIGUhIR, D.N.; TALAIAYLVA, T.V.; KUCI=BKOV) K.A.
J.
Study of the lithium alcoholate structure by the method of infr*vd
absorption spectra; O-Li ... 0 bond. Izv. 1-11 SSSR.Ser.fiz. 26 no.W.-
1246-1249 0 162. (MIRA 15:10)
(Lithium alcoholate--Spectra)
1:5--
KDCIMHKOV K A PALEYEV, O.A., SOGOIDVA, T.I., SHEMMINA, N.I.,
RODIONOV, A.N.
Nouveaux compoaants des catalyaours de la polywrication do 119thylens
dans des conditions habitualles at inhabituellem.
Report submitted for the International Symposium of Macrowlecular Chemistry,
Paris, 1-6 July 63
RODIONOV A.N.; SHIGORIN, D.N.; MAIATEVA, T.V.; KOCRESHKOV, K.A.
Y --
Structure of complexes formed by aliphatic organolithium
compounds. DoIcl. AN SSSR 143 no.1:137-139 Mr 162.
OIURA 15:2)
1. Chlen-korrespondent AN SSSR (for Kocheshkov).
(Lithium organic compounds)
VASIL'YEVA, V.N.1 KOCHESHKOV, K.A.; TALA,ILA YIEVA ., T.-V-.-; PANOV, Ye.M.;
KAZENNIrM. G.V.; SOROKINA',--R.S.; I'IITRIY, O.P.
Dipole moments and structure of some fluorine-substituted
styrenes. Dokl. AN' SSSR 143 no-4:844-846 AP 162. (MIRA 15:3)
1. Fiziko-khimicheskiy institut im. L.Ya.Karpova. 2. Chlen-
kcrrespondent AN SSSR (for Kocheshkov).
(Styrene--Dipole moments) (Fluorine compounds)
GOLOVMMOV, I.B.; .'AI-'ONOV, A.P,,"' i,isLUNOV, A.K.~ TALALAYEVA, T.V.; TSAREVA,
KOCIU-~SKOV, K.A.
Nuclear magn-,tic re3onance SF-ctra and ebullioscopy of lithium
alcoholates. Doki. AN SSSR 149 no.4A35-837 Ap 163. (MIRA 16:3)
1. Fiziko-khlmic"Ileskiy institut im, L.Ya.Karpova. 2. Chlen-korre-
spondent AN SSSR (for Kocheshkov)
J~es-Speectra) (Ebullition)
(Lithium qIc,.oholq
RODIONOV, A.N.; TALALAEVA, T,V.; SHIGORIN, D.N.; TYUMOFEYUK, G.N.;
KOCHESHKOV, K.A.
Structure of complexes formed by aliphatic organolithium compounds.
Dokl. AN SSSR 151 no.5-.1131-1134 Ag t63. (MIRA 16:9)
1. Fiziko-khimicheskiy institut im. L.Ya.Karpova. 2. Chlen-
korrespondent AN SSSR (for Kocheshkov).
(Idthium organic compounds) (Chemical structure)
TALALAYEVA,, T.V.i RODIONOV, A,N.,- KOCHESHKOV,, K.A.
SynthesIs of de-uterio-substituted organolithium compounds. Dokl.
JAN SSSR 152 no.12-122-123 S 163. (MIRA 1629)
1. F�zlko,-khimicheskiy institut im. L.Ya.Karpova. 2. Chlen-
korrespondent AN SSSR (for Koche5hkov).
"Lithium organic compounds) (Deuterium compounds)
S -CjV, K-
1,. ; y -i:FSIIF
Zil
:Iates.
ithjur I
so! ble - L.
Gf (,%Ilp,.A 17: 5)
Y-r- and .6 18-64,4 Ap '64.
r-o-
'rALALIYEVA, ",V,; RODIONOV, AJJ.~ KOGHESHKOV, KA~
Mixed complexes of phenvil-",-~--,um, methyli-ithium, n-butyllithium,
and lithium halides. Dokl. Aff SSSR 154 no.1:174-177 Ja'64.
(MIR_A, 17~2)
1. Fiziko-khfmachaskiy instivdt. im, L.Ya. Karpova.
2. Chlen-korrespondent AN SSSR (fo~- Kocheshkov"
1.
TALALAYEVAP T.V., PETRIY, O.P., TIMOFEYUK, G.V.,; ZIMIN, A.V.;
KOCHESHKOV, K.A.
Synthesis oR7~,' -d-fluoro-O~,,Vj~-dialkyl ethylenes
by means of organolithium compounds. Dokl. AN SSSR
154 no.2;398-400 Ja'64. (MIRA 17:2)
1. Fiziko-khimicheskiy institut im. L.Ya. Karpova.
0
1- Chlen-korrespondent AN SSSR (for Kocheshkoy)..
77-65 EPA(s) -2/EWT (r)/EPF(C)/EPF(-a) -2/F.PR/FWP(J)/EWP(t)/EWP(b)/Rlip.(c)
Pc-4-/P-i----ZT/pr.-4/pt-lo/pu-.~4 IJP(6)/RPL
~ACCESSION NR: AP5006412 S/00r,2/65/006~'ii~ii664'2/0046i
iAUTHOR: Rodionov, A. N.; Timifeyuk, G.V.; Talalayeva. T. V.; 10
4i
')~ocheshkov, K. T-
~TITLE: Infrared spectra of certain'a6etylenides.of lithium, sodium, band potassium
iSOURCE: AN SSSR. Izvestiya. Seriya khimicheskaya, no. 1, 1965, 42-46
'TOPIC TAGS: spectrum analysis, acetylene'lacetylene compound, lithium, lithium
!compound, sodium, sodium compound,_p2lassium, potassium compound
ABSTRACT: The infrared spectra of certain a2phatic and aromatic acetylenides of
lithium, sodium, and potassium.were measured with a double-b6am Hilger~H-800 spec-
I
1trometer with prisms of.LiF, NaC1, and KBr (from 4000 to 460 cm-1)., Samples were
!taken in the form of a suspension in vase -line, and fluorinated'. oils and, were prepar&
in an atmosphere of dry argon. The infrared, spectra obtained'indicated character--:
fistic oscillation frequencies of the groups.found in this class of compounds
i(C-H,-=C-H(D),C=-C,=-C-C,=-C-H,=-6-Li). In comparison with the oscillation of acetylene
land its halide derivatives that of the EC-H and the CEC groups is.didplaced 50-100.-.
e
in the direction of the long waves, due to I ra- and intermolecular int X_
Icm int
;actions of these groups. A shift of the oscillation frequency of the bond of the I
Card .1/2
RODIONOV, MI.; TAIALA'fEVA, T.V.-, SHIGORIN, D.-N.; RODIONOVA, G.N,;
KOCW,SFKMT, -k.A.
Infrared spectra of isotope-substituted ethyllithium molecules.
Izv. AIN SSSR. Ser. khj.,n, no.4.604-610 165. (MA 18:5)
1. Fizilko-khimicheskiy institut im. L..Ya.Karpova.
L 5062-66 7-WT(m)/-~-'PFfc)/E',[P(j)__R-PL
ACCESSION NR: AP5025509 UR/0062/65/000/009/1607/1613
547.ItS+547.362+546.34
44
iAUTHOR: , Tajalayeva, V.; Timofeyuk, G. V. Rodionov, A. X.; Kocheshkov, K. A.
TITLE: Lithium acetylenides 'AJk,~~
SOURCE: AN SSSR. Izvestiya. Seriya khimicheskaya, no..9, 1965,,1607-1613
TOPIC TAGS: organolithium compound, acetylene, benzene, hexane, ether, lithium
ABSTRACT: The authors synthesized crystalline lithium acetylenides in benzene, hexane,
and ether in the range of 0 to -50C, using acetylene alkylacetylenes,jand solutions of
ethyllithium, n-butyllithium, n-amyllithium, phenyllithium, and R-tdlyllithium. The
products were analyzed for lithium, and their IR spectra were taken, In some cases, the
compounds obtained were decomposed with heavy water, and the deuterated products were
studied. It was thus shown that when acetylene reacts with solutions of organolithium
compounds, lithium acetylenide Is formed. When acetylene reacts with aliphatic organo-
lithium compounds In hexane at 0 - 25C, crystalline lithium acetylenide Is formed In 75 -
80% yield; when alkylacetylenes react with these compounds at -50C, lithium alkylacety-
Card 1/2
~cl rot 02-//
L 5o62-66
ACCESSION NR: AP5025509
lenides are formed in 75 - 90% yield. To refine the positions of the main bands in the Ift
spectra, isotope-substituted lithium acetylenides were synthesized by using lithium-6 and
euterium, and the IR spectra of the products were recorded. Lithium acetylenide is stable
on standing, apparently because stable complexes re formed between its molecules.
ASSOCIATION: Fiziko-khimicheakiy institut-im. L. Ya. va (P sicoc emi
Institute) Iff-I . .. - ____
SUBMITTtl): 25Jun63 ENCL: 00 SUB CODE: Oco rrC
NO REF SOV: 009 OTHER: 012
Card 2/2
L, G:'y N1. i y
Zhur. s-t,r-c4k',, kh-,,:r. Ja - F ?6,
J z 1 'r'-,c, -kh." 21 c- h ~~ ~s -i r a
~!..j T
A~LLIM. atl'
.5-37: D MLI qA
sij
21fect of barfurn oxIde on Som'a prqehf~if-af-kriltv.
Smol'kov and E.,V. Talahte-va (Af.V. Lo ioMoiciv State
Univ., Moscow). ~ Pit. Metal. i Afriollota 'A kad~ 11-mik
S.S.S.R., Viah KlIal 1,
for Industrial use (as mineral ninguets); 13noi
CaO, und other
metallic oxides are often added to the solid -solu. Such
oxides are themselves not magnetic ror Is i111c solid 801H
they fortit with V 0. netic. . Hoyt tl c~ addn3. allcet
the magnetic propertif, TT tb. rwighuhl f6-rite (in thii in-
stance, NialAgci -a)FLOj) isilhistratod bytijcftddn. ofO, 3.
10, 15, SM20 parts by %vt. in 100 (theparAinetur6be(ug the
same in all 6) to prepits. inado ceramically by Fe,03.
NlgO,-NiO, and BaO-nt.1300* for,.4 hr--.-- I.e inqg1letic.
properties mitusu d iht6il and max.
re Wore. magnet
raun&Wrictioh; androtation
and-4
-,)f the a to all casesJIm magnetic
yia~e (of' P'l."I of MD..
properties d...,..,-,ith creasing concr.
5 6 3 5 /4 7
AUTHORS: Belov, K. P. Talalayeva, Ye. V.
IT LE: The Galvanometric Properties of Manganese Ferrite (Gallvanomagnit-
nyye svoystva ferrita margantsa)
PERIODICAL: Zhurnal Eksperimentallnoy i Teoretiche9koy Fiziki, 1957t, Vol. 33,
tir 6 (12), pp, 1517 - 1519 (USSR)
ABS2RACT: The authors carried out measurements of the temperature dependence
of the galvanometric effect in a ferrite with 50 7~0 (Idol-%) MfnO and
50'/- Fe 0 Such a ferrite did not have too great a resistance and
,
on it ii ;a
s possible to measure the effect in the case of direct
0
current in the temperature Interval of room temperature up to 350
Elie ferrite -was produced by means of the usual 11ceramic" technolo-
.:-y from chemically pure oxides. As samples rods 0" 52 = length
and 25 mm 2 cross section were used. On the front surfaces of the
samples the contacts for current feed were fitted by burning in
a ~3ilver panste. The sample was located in a furnace with b4lilar
;;;ndin,; the furnace itself was in a. riagnetizin6 solenoid. The
~;_'lvanometric effect was measured by the me-zhod o-, the brii-]Ee not
~n e,.,uilibrium. At each given teciperattire ihe ei-ect-r1c resistance,
Card 1/3 the -alvanometric effect R/R , and the su~:cif'_ic -~a~neLization
Aj 7
1-he Ga-I'v:~nc,-.'ietric Properties of ManEarese Fdrrite
were me~;sured practically simultaneously. A diaEram s`ows the
curves of the temperature dependence of the longitudinal ----lvano-
metric effect; these curves were recorded for weak and 3tron-- mag-
netic fields. (AR/R), has negative values and decreases consider-
ably. At Curie point, however, a marked maximum of the galvanome-
tric effect is observed. Further details are 3-iven. It is of inter-
est that the longitudinal and the transversal -alvanometric effect
have the same sign. Howeverv apart from a nejative Galvanometric
effect, the authors also discovered a positive component of the
lQni~itudinal effect in man.-anese ferrite. A dia.-ram, which is attgall-
ad, illustrates this effect. The major part of the galvarometric
U
effect is caused by a paraprocess; its siul-n. is nelgative, and the
dependence A R/R is rigorously satisfied for it. At values
of majEnetization a "stru.-.c-le" between the negative Zaivanometric
effect and the positive component of the lon~-itud_inal effect takes
U -
place; this anomaly is not removed by coolin.- or rej;eated heatinz.
--,are are figures, and 6 references of are Slavic.
Card 2/3
The G~l -ic PrOperties of Manganese Ferrite
lvanomet,
m,
A'33CCI.-'-TIOlT: a..oscow State University
(1-loskovsleziy gosudarstvennyy universitet)
SUBMI210ED: JulY 30, 1957
AVAILABLE: Library of Con~ress
5 6 -3 -, /4 7
Card 3/3
TAULAYEV, Ye. V.
Arti?tgt~ tion of epizootic septicemia in the caterpillars
of Dendrolimus sibiricus. Report No.l. Ent. oboz. 36 no.4:845-859
157. (MLRA 10:9)
1. Biologo-geografichoskiy nauchno-iseledovatellskiy institut
Irkutskogo gosudargtvennogo universiteta im. A.A. Zhdanova.
(Forest Insects--Biological control)
(Siberia--Moths) (Bacteria, Pathogenic)
AUTHORS: bt-lov,V.P., and Talalayeva, Ye.V. 30V/155-58-2-46/4'7
TITLE: Temperature Depeffdehce of the Galvanomagnetic Effect and the
Electric Resistance of Manganese Ferrite in Poly- and Mono-
crystalline States (Temperaturnaya zavisimost' gallvanomagnitnogo
effekta i elektrosoprotivleniya v ferrite margantsa v poli- i
monokristallicheskom sostoyaniyakh)
PERIODICAL: Nauchnyye doklady vysphey shkoly. Fiziko-matematicheskiye nauki,
1958, Nr 2, pp 220-227 (USSR)
ABSTRACT: The comparison of experimentally measured electric resistances of
poly- and monocrystalline manganese ferrites shows that they have
the same order of magnitude (S polyer ' 200 ohm/cm, S monocr -800 ohm/cm)
Herefrom it is concluded that the electric resistance of the
manganese ferrite is determined by the ferrite itself (not by the
boundary layers between the grains). In the neighborhood of the
Curie-point the galvanomagnetic effect is influenced strongly by
the paraprocess; in the neighborhood of the Curie-point the curve
Ig p( I ) has a complicated crack with a flat point. The authors
T
measured a positive component of the galvanomagnetic longitudinal
Card 1/2 effect unusual for ferrites. The results are compared with those
Temperature Dependence of the Galvanomagnetic Effect and SOV/1-55-58-2-46/41'
'the Electric Resistance of Manganese Ferrite in
Poly- and Monocrystalline States
of Komar and Klyushin [Ref 2], Irkin and,Turov [Ref 101 and
others. The authors thank I.L.Popova (In5titute of Crystallo-
graphy) for giving a crystal.
There are 9 figures, and 11 references, 10 of which are Soviet,
and 1 American.
ASSOCIATION:Moskovskiy gosudarstvennyy universitet imeni M.V.Lomonosova
(Moscow State University imeni M.V.Lomonosov)
SUBMITTED. January 15, 1958
Card 2/2
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-A-V i .... joid
-12 4 oc~
uw,
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a
AUTI-'~ORS:: Be-',--v, K.P. Pcpcnva, A.A. and Ta'ai~~yeva, Ye.V.
'4L-:~
TITLE, The Eie~,trical a-ad Ga'LvanomaF_ra-tic Properties of Sir-;~-re
Crystals of rMlanganese Ferrite (Elektricheskiye i gal'-
vanomagn-itnyye s-,rcystva monokristallov iferrita margantsa)
PERIODICAL: Kristallo.-raf-iya, 1958, Val 3. Nr 6, PP ?33-9 (USSR)
ABSTRACT, The temperature dependence of the electrical resistance and
the longitudinal galvanomagnetic effect in single crystals
of manganese ferrit-e have been measured. The temperature
dependence cf the resistance is complicated. Near the
Curie point on the lines log r (1/T) breaks are
observed which have a step form, It is supposed that
these steps arise because at the Curie point crystals of
manganese ferrite transform to a degenerate electron
state. It is established that the deDendence of the
longitudinal gal,,anomagnetic effect on temperature, field
and magnetisation 4s analogous to the dependence observed
in metal ferrcmagneti~;s. The crystals of 11yinFe 20, used
were made by the Verne-il process and X-ray and chemical
analysis were used -rc establish. the orientation and
texture of the soecimens which were rods of about
Cardl/5 0,2 --m2Crosss--section and 1 cm length. The specific
6OV/;?O-3-0-l3/25
Th~e Electrical and Galvanomagnetic Properties of Single Crystals of
LanEanese Ferrite
resistan..-es r were of the S,~re order as that of the
polycrystalline material (I k.Q,..cm)- The conductivity is
assc.:-;iar,ed with the o3currence of ions in two valency
states in alternation in certain directions Th. e m.. u c h
smaller obser7.,ed ~iere than in the case of
magnetite JL-3 a consequence of the presence of
2. --!-3 anj fvjrj~-4
Mn+ h', " ons in the same set of equivalent
Positions and the absence of Fe+3 ions ., A graph ol-
the ccndu,-,ri-r_-%7 against, 11'emperaturve is gi%ren. Lc. g r
against T is .-oughly a straight line but is broken
into regions. Each can be described by r = A exp dE/kT
where dE 'has a d:.'Lferent- -ialue for each of six sections,
namely 0.',0 0.26, O~20t 0.32, O~50 and 0.32 eV The
region near .the Curie point (near 1037---
/T = 1.8)
was studied more i;losely. It is thought that on the
transition from the paramagnetic state to the Cerro-
0
magnetic the semi-conductor passes through a state of
electronic degeneracy ~as in a metal) and then become--
a semi-conductor aga-Ln. The slope of the line log r(l/T)
should be less in. the ferromagnetic state than In the
Card2/3 paramagnet--c.
30V~0-3-6-13/25
'."he Elestrical and Galvanomagnetic Properties of Single Crystals of
Manganese Ferrite
As in the case of most ferromagnetics, the longitudinal
galvanomagnetic effect in the region of technical magnet-
iaation has a positive sign. With increasing temperature
the sign changes toonegative at lower and lower tempera-
tures until at 2'/0 C the sign is always negative. The
effect is also plotted out as a function of the square of
the specific magnetisation.
There are 10 figures, 1 table and 6 references, 4 of
which are Soviet, 1 French and 1 English.
ASSOCIATION: Institut kristallografii AN SSSR (Institute of
Crystallography of the Ac.Sc.USSR) and
Moskovskiy gosudarstvennyy universitet im.
NI.V. Lomonosova (University im. M. V. Lomonosov)
SUBMITTED: July 12, 19510,
Card 3/3
TALA-LAYEVA, Ye. V. Cand Phys-Math 6ci -- (diss) "Study of tiie remperpt,,re
relationship of ma~-netic and aleotric properties of poly- and monocrlstlals of
I
ferrites of manGanese." '.10s, 1959. 10 pp (Mos State Univ im ". V. Lomonosov),
100 cocies. Bibliovraphy at end of text (12 titles). (KL, 41-59, 103)
Q
-5-
'~'q'30061P,
e j"'f
~JjT Hb~-, j ov -a~. iom ov 'a" aiayeva, Ye.
Tl- LE oi' t,ii--: jI,,roma.-,neLi,.; effect in ferrites
neal. "'urie point,
~-EHIUDICAL: i~lizika Lverdo;:;o v. i, 0 - 2. 19o1 , 4~6-446
TEXT: WIrien &,.easurin,-- tne galvanomagnetic effecc, tne magnetostriction,
and ot~ier ~i-~enomelna, it is necessary to take tnie effect p-roduced by
ma.-pietocaloVic effect occurving in '11-.e adiia~jatic application of the
I - - - - For the
magnetic :n tile ferromaEnet-- s~,acimen 4nto account.
purpose of excludin,' --e error arisinz- by tn-"Ls effect (which beco.Tnes
consider,able near cu;-ie point;, measurements are not carried out immediate-
ly after the applicai'Aon of the fie'--d i-eaSUI-0,ment), but only
some --ime 1~ thu
perature equil4brium between speci-en -and
the Lurroundir--, medium lias beer eSLa-,--1'ii--.ed ('~sot'-Ormal measuremen').
so'
are easi
ermial cond.-
Whereas in metal 1 ic f erronq~,,---ne- ics -.L -Y
realizable, t-~a-ls ureserits difficult~les in, -,:.e case of ferromL~~-netic
se.,miconductors because o. t-eir lo-w t-erma-I conductivity, and when
Clard 114
Icaourement ut' ti~, galvanomagrietic
D 1 2 /:E 20 4
measurin- IJ-,,~ j,:,Ivanoma, Tn
gnetic effect , consi:ierable errors may arise
L rhe preoeti t papa r fiie c ond 1 t i uno occ u.L L in,,~ i n t lie measurement of the
-alvanoriia:,-netic effe-,' are above al~ "re effect produced by
the adiabat!~_ temperature increase occurring wak-n anj'~Iying ti,,L- field.
.K. Zaveta assumed t'!-,at the imaximum j~ ti-,e jalvanomaglr.~_-tic effect of the
paraprocess near CurJ.e pcir- . the au-, .rors ti 4ocovered in ferr-ites, is
exclusive-Ly a :,onsequence the efflect prcd-_-_a_d by - ma-,~.-netocaloric effect.
it is now chat ~Iie drawn 'by ~,avet,~~L are incorrect. The
11 -
paper by Zaveta _V-TT _2 9t.c.
U is irsr, d~scuss"d in detail, For the
cnange in ota~,3 u o ap~~;yin- the ;he'd. 7avet;
-1 gave tne followin-
formula: ~2 R/R a-r- - bH; ~iere the first term makes tne contribution
of tLe lltru,~11 ,-alvanoma,:-,neLi-_, effect . and the tjecond na?es the contribution
Of the 11,wrui,611 ggalvanoma_.,nellic tATect. .;'!,is for!_)~Uia is, however, wrong,
2 71 '21
and it ought, to read R!.4
---cause all even effects
r_~, , 'L = a
near the Curie Doi;-,t dauerd in the same manner or. H 'viz. - H 2113).
Frow. this wronI-r formula Lnere resuit also the wrong conclusions drawn
by Zave-ra, 7or -L-e :~ui-~ose of bein'l able to e~3tiran_--,e ei-.e,
Card 2, .4
20120
,;/18 1 /6 1 /003/002/018/050
-e-1 sureme Bi 02/B204
W of the salvanoma.-netic
Produr,ed bY tLie magnetocaloric effect. it is necessary to compare a and b?.
The sum cf th-,-, coefficients 'ka-b' .'~ -may be determined from tne
m e a s u r e m e n z s o f f b c , i 7- a v e t a c a 1 s i s o v e d
to be wrong-ly determined by Zaveta. The meLhod he used is not.at all.
suited for determining bl, -Heve, the equations 6T T -
1~ a/)If ~ H
&T
and 61if/ft ~6T/k~-' are used for calculating "he "wrong" galvano-
m a n e t i c e f fec. t He re 1-rom, 'k i.~H is obtained
T 1p T
for the Curie po,.n, specif ic magnet ization). For Mn ferrite single
crystals thus ( A R/fj)(. -U:. 9, 1 C)- a results from experimental
determinations of t'ne -.ndividual quarilities '."data obtained by other
aut hors ) -and R /R " ~ -44 ~ 2 C -4 i s ob z ained f rom t he authors I ow-r,
data, Thus. the "wr-on-11 effect is smailer by a multiple than the
"true" effec'tt The I'magnetocaloric" temp-.~rature incre-ase AT a-,
Curie Lloint is foun6 to be 0.37,0C and causes a c-anze of 01- the
Card 3/4
,2 () i 1) 0
'61/03 '002/018/050
3/181/0 3/
!~'IeasuremenL of the gaivanomagnetic BE 1 U-2 // B 2 04
maximum resistance 3h-;r,6e ZLR~ It follows herefrom that the maximum oi
the true galvanomagnetic effect of tline paraprocass at Cur-le point
actually exists and is not only due to an "adiabatic" increase of
resistance, The existence of this maximum is proven also by tiie
exis!,ence ol' breaks in the log ~(,/V-curves in the Curie point of these
ferrites~ It may occur only in such 4ferrites as have a low activation
K-rivogllaz and S, A, Hybak are menticned, There are
ener '-y z,- ,
7 Soviet-bloc referen._-es.
-site
S ~Oc LAC 16 N oskovsk,-y gosudars,vennyy inivei L ~ imz .1, V~
Lomono~iova. Fizicheskiy 'Let (,ot--.7cw State University
imeni. ";. V., Lomonosov, Division of -_physics)
."ay 19*'CJ
Card 4/4
G 121
7,
-,4
A U TH o.`~ Talaiayeva. Ve. V.
T ITLE The temperature dependence of tno effect
-anese ferrites
n Man.
PERIODICAL Fizika tverdoo-o tela. v. 5. no, ). 10611. 441-d49
TEXT Various urobIer-ns concerning ferrites 'iave uo c r .ne presenu day
not been fully expla--ined. as e..-, ~Ce zonduction me-.~,hanism. ?.-he temperature
dependence of resistivity. und "ne .L) e.11" i Q r, 0 rhin run-e
-f ma~,net T-r-se uroblems are n.--,.- (-jn-y of rhecretJca, but
lc trans4tion, I
'Jca-c-li~ies
'so of practical interest because of the marir'o.!~ 'ec-,-nical app' I t
of ferrites.~ A report io 6r,.ven on of tilie even lo-ngitudinal
galvanomaEne-ic effect of I;cly- and monocrystalline manganese f,?rrites.
The invest il,;-at ions are a continuation of :;reiiminary studie-z. in 'this
field, The results obfa-~ned "or mono- ai--; polycrys'a-i'-ine .---ferrites V~
are compared in order tc clear ri,-,t~ part played by laverS. wl--~cn are
located betweer tirie- zrainS. in 1-0--.'.-r-*;jtaIIintf s-L~eoimen-s, Invest ii~7at ion. s
at jejpei~ature~,-. 'beio"V Car-~e o i t < PiLe longitudinal
L
Card
8
Tne te,;ilievatu.-t~ depen:lence of ~hle U
.;,,a,' vanom~al,-- po -nr2 0 e % `e 0
71
+ was nogative at rocm teir,~eraLure.
-a po s i t i ire c ompone r. t of ~ 'ne ongi t 'Ad --- nal e-al variomagne t ic
effect occtirred !in the crjoe ~P tljt~
and Fig. 1
shows ~-hel-lf- 'lej),Z:nJence of t',.e
om: fu-3 int ma 4;m e t -c effez,. nd -14 s :: o w s c.- n g i t u n a
6 a i r, o r, _7 n e r e c i' e r r T.-, -a r C ~ r yo Ll 1 9 _T-rorn ~ne course -calf-en
by ?hese t~_e C(_
-s 7iravin :"U~ i:, of
n e i, f i e c, io c ry s - .'le e c r a n j r c. p a r a p r C 0 S
I a y t i -i e r n c i ~: La i p a I -L! I f r, t,,.n rerr4cn of
0
M,
E!ijgnetio ~ransl'cr,at:.---n '-.- I - "I. - .
"ne PI act
produced by rhe pauaproces~, -ipon effect increases;
edl S!~Owed a we"! maximum cf t--,e ne,~-a7~-re --alvanomac-netic
e 1'ec t ":easure,---ents .n, -'urle poir,
are render(,-I --JJffi--~l.i--l '-v fl-.(- ircrease t I in
he cas e o I' ad 'v a, t i c f I d m, e a j em ~~n iie v i-,: t -,n s d i --l i n I sil. e d
-n e s t ima n -a e - f c -u ce e rn -i, -n o C -a r 1 c e, ff e c t az- on
Card 2/9
The tem'Lterature
~eljS of maximal---y resull s in an
:mono~!rystals~ and
Oz39LU r, alues cause a ~n -~-e -re~sured
(-c,yerystals'. Ti-.ese v L
,8R-value in t~.e maxian-um- of abou-, 84,"? '~' 0"1 111, T,:-,e C~se of polycrystals),
The maximum of zc're ~6R,',z'i-curl'es Tnus s .nc*.,,,a an P--ror of 'out wilt:hin
the region of Curie temperature th-41:3 maximu:,: -c.' galvanomaEnetic.
effect o-' ',,,e paraz~rczes--3 a,-.~,-,alll'y ext,,-~s -nax-,ma are -~',--.own for
n ex~-i
field of Q("O re 1~' mi, rt c r - 37 J, T
for a monocrys! al
obtained in nolll-~te g a s pL.- r,- Ez
an d L; tic I y,. ry s t a 1 ( 2 1 ri T. ito, range cff em n r -a t u r e tne
madnet-,zation in. rej-~onj of t 1! E., ~irc,;~ ort i.Dna I lo H
and r~ie -3ffec: i.F c s o v.,
and ~n, R e fact f e r curve loes not
1 7 0 cl r lc-ln io in manner
t hat e d a o r j e s e a r e c :--n c a I
r., r z' I o n e a r o c e s s
ma~rnet i zat S ,ear,, ;.r7. e r:, 7
Card
Tile
the rel`ati-~n
~Dc, 1:1 ry S a 1; 1 i ne
.n o n c ry -'o r r, t a! ua I e: U
0 y ;nd
respectivellY t f.-~r b t a i n,---,J in inttz-
1 n the region
above Curie remperat,.~re, re-gion of' the
paraprc)-,e~--s -i~i a quadra-tic f--zn,:t-,rn of il I r e b cj z i.. 1, c, r mo rlo -
I
arld fcl. ne m-ingane,3e
-, I t1lat
we,-, n, z a -ei --men j unde r-
-,qu'.e 1--, ~--Senrlal
6alvano-mu-netic
~J, rd~ authors
I [lank crofessor for h,,s
--e as we~ -a
A PoIjova for
arp 7 f j i,U 1, ~:? 0 t _:j
4
4 e b-,)- and
Card 4/9
The te-Derature dependence of the ...
fez
Soo fooo
0
'I 77f7~
7
4
0
Bi-02/B204
2 _~Cm z
livo
Nc. 2. TC5fnCpnTyplffl$T 3aBltClIMOCTh upoAo,%buoro
ramvaimmarnifTlioro -jfpfl)cxTa A.%u rjo.%mxpmcTa.,,.inne-
cicara o6pa,3ga 'N? 9.
10z f = 211.8' (1), 240.0* (2) 264X- (3), 278.3- (4), 283.6- (5), Ml,
(6). 293.6' (7); t
a
Card 61,
ON
cli
WN
C\J
lfs~(;t 654 'M R,09L '(f) .0794 OV999
UZ :2 C*sP ) 1'69 '(f) .9-6L '(7) .911 WZ91
-U.LllddQ41 Ull ri(vus3lidualfolq oJolfliffliew
-ant(mvim ojowivarodu 'zild
ol
00 oor M ON
OV -
0t-
001-
ON
co
ol."Yv
~ !Z11 -- ~
The temperature dependence of the ...
&~.io t.
t.4
to~
S/i8i/61/003/002/011,0/050
B5102/B204
0 r.
5 i~
~is
d"
-Ngst
'r- -, ~
Card 819
ju
J121
T
T
he temperature dependence of the ...
IT1 13
egend to Fig. 6: 6( -_
~Or P-OlYcrystal (288.:;OC)'_
curve !; for monoc-
260.80c - curve -ystal at
-115) tn
for the Polycrystal (curve 1),
U
obta-ired for 'he _POlYcrystals
at _300.40C (curve 2) in a
noble gas atmosphere, and for
/onocr.'stals at 260.80C
~C,UrVe 3), at 269.60C 'curve 10
and 204.20C (curve 5).
S/18!/61 003100210191050
B102/3204
O.,zC-z Cm
10 100 150 e13,
/,7U tl
11 17J ~l 7 117
fo
0
-20
Card 019
AR
4
ACCESSION NR: AP4033639 8/0188/64/000/002/0082/0084
AUTHOR: Talalayeva, Ye. V.; Chernikova, L. A.; Galkina, 0. S.
TITLE: zlectrical resistance of gadohnium films and massive specimens In the tempera-
ture, range 2-290K
SOURCE: Moscow. Universitet. Vestnik. Seriya III. Fizika, astronomiya, no. 2. 19".
82-84
TOPIC TAGS: magnetic phase transition, Curie point, molecular physics, gadolinium,
gadolinium electrical resistance, rare earth
ABSTRACT: The rare earth metals of the yttrium. subgroup have two characteristic
temperatures, 01 and 02, corresponding to two magnetic phase transitions. Below ~I
the temperatures these metals are in a ferromagnetic state, and above (to in an
antiferromagnetic state with a hellcold or similar structure. The temperature 02 is the
Curie point. Until recently, however, it had not been established whether gadolinium (a
member of the yttrium subgroup) has a 0 transition. In this paper, the authors investi-
gate the temperature dependence of the Z!;;~Ical resistance of massive gadolinium and its
films for the purpose of determbilng the influence of the 01 transition on these curves.
Card 1/7
ACCESSION NR: AP4033639
Electrical resistance was measured by the ordinary potentiometric method. Between 2
and 25K temperature was measured with a gas thermometer and above 25K with a copper-
constantan thermocouple. The masgive specimen of Gd (purity 99.8%) was 15.7 mm long-
and had a cross section of 0. 47 mm . Figure 1 of the Enclosure shows the dependence
RT/R 02 of the massive specimen of Gd on temperature (where RT is resistance at a
particular temperature, is resistance at the Curie temperature). At a temperature:
01 = 210K there is a small knee, with another near the Curie point of 290.5K. Figure 2
of the Enclosare shows the temperature dependence of the electrical resistance of three
fine films (thicknesses of 70, 100 and 180A) during the heating of newly condensed films
from 4.2 to 280K (curves 1, 2, 3) and during cooling to the initial temperature of 4.2K
after being held at a temperature of 300K for 40 hours. Figure 3 of the Enclosure shows
curves similar to those in Figure 2 for two thick films (380 and 500A). "In conclusion
the authors deeply thank Professor A. 1. Shallnikov for valuable advice and assistance in
the work and Professors K. P. Belov and Ye. 1. Kondorskiy for discussion of the results".
Orig. art. has: 3 figures.
ASSOCIA17ON: Kafedra molekulyarnoy fiziki. Moskoveldy universitet (Department of
Molecular Physics, Moscow University)
Card 2/7
_7
L 21 5-65 M(l) IJP(c)
ACCESSION Mi AP5=698 0/oift/65/007/004/01/0984 A . ....
AUTHOR: Belav, P.; Talalayeval Ye. V. Nudryavtoeva T. V.
TITLE: Thermomagnetic and galvan2Mgnetie effect in manganese ferrite '23
SOURCE: Mika tverdogo telap v. 7., no. 4o 1965.0 981-984
TOPIC TAGS: ferrite., manganese ferrite., thermomagnetic effects galvan~pmagnetic
effect, magnetic ordering
ABSTRACT: A simultaneous investigation was made of the even thermomagnetic and r4pC
galvanomagnetic effects in the same swap16 of single-crystal manganese ferrite.
Two samples were tested, one containing 6.5% excess of manganese, and the other.
containing an excess of iron with composition Mn 7Fe The thermomagnetic
0.. -2.1304-
effect,was measured by a null method using a photocompensation microvolt-ampere-
Weber meter F-18. The galvanotagnetic effect was measured by a bridge method, and
the magnetization by a ballistic method. The results showed that the thermolwg-
netic and galvanomagnetic effects have different behaviors. The thermomenetic ef-
feet has a maximum growth in the region of weak fields (in displacement and rota-
Card 1/2
TADIIAA-EVSKIY, G.V.
Maximum discharge rates in the ravines on eastern slopes of
the Yergeni. Hills. Melaor. i gidrol. no.2:40-42 F 162.
(MIRA 15:2)
(Yergeni Hills--Runoff)
TALALAYEVSKIY, G. V~
Quantitative estimate of the surface erosions of soils on the
eastern slopes of the Yergeni Hills. Meteor. i gidrol. no.l:
44-46 Ja *-63.- (MIRA 16-1)
1. Severo-Kavkazskoye upravleniye gidrometaosluzhby.
(Yergeni Hilis-Erosion)
TAL.~LOV, I. I. , inzh.
Detfirmining currents of damping windings in salient-pole
synchronous machines. Sbor.nituch.trud IM no.8:119-335 '58.
(Mnut 13 '- 10
(Electric motorB, Synchronouti)
TAIALOV, 1. 1., Candidate Tech Sci (dies) -- "Investigation of the distribution
of currents in the cores of the damping coils of synchronous machines". Moscow,
1959. 15 PP (Min Higher Educ USSR, All-Union Correspondence Polytech inst,
Chair of Electrical Machines and Apparatus), 200 copies (KL, No 24Y 1.959, 141)
TAAAT, M.Ye. LTalaat, M.E.];_~TALALOV, I.I., inzh. (translator];
SERGEYEV, P.S., red.; LARIONOT, Mo., tekhn.red.
[New approach to the calculation of synchronous machine
reactances] Hovyi podkhod k opredeleniiu induktivnykh
so-Drotivlenii sinkhronnoi mashiny. Moskva, Gos.onerg.izd-vo
19~9- 95 p. Translated from the English. (MIRA 13:7)
(Electric machinery, Synchronous)
TALALOV, I.I., inzh.
Damper winding currents in asynchronous operation of
salient-pole synchronous machines. Izv. vys. ucheb. zav.;
energ. 2 no.7:22-32 J1 '59. (MIRA 13:1)
1.1vanovskiy energeticheskiy institut imeni V.I. Lenina.
(Electric motors, Synchronous)
---- TkLAL~4) I. I. , kand. tekhn. naWc
C-ireu--. t trans -for-mations in the analysis of electric rach4nery.
Elektrichestvo no.4:34-38 Ap 161. (INDIA 14:8)
1. lvanovskiy energeticheskiy institut iiqeni Lenina.
(!~Ic;ctric machinery)
': A ! I I .' . V . ~,. . -. 1 `.~ I~i '~ '. '1~ ': - V7 .. If
. .. I il..
'I las 5-c---r am ir- -~ a w ma -.,~ri a! f ~:,aroj. 7 e s , --,a zv~,~ . --' -I' ~h . ne--' -
,:Z9 rio. I I : 19-22 N '6,3 . (ICRI. 17: i2 ;
1 . ~Samarkandskaya Feologorazverlochnaya ekspeditsiya.
TALALOV,J~A., aspirant
Herbicides for c-ntrolling weeds in onion and carrot fields.
Zashch.rast.ot vred.i bol. 5 no.2:23-25 F 160. (M-IRA 15:12)
1. Tashkentskiy sellskokho ystvennyy institut.
Nabekistan-Ohionsr (Uzbekistan--Carrots)
(Herbicides)
IA,12tLCIV,~~, L . I .
TALAJf-VA, A. I. -- "Certain indexes of tl-.-- Peactivity of the Organism in
Fneumonia of 'Younc, Children." Ivanovo, (Di-33ertation for the
0 -
De.-ree of Candidate in Medical Sciences).
So.: Fniz,maya Letop-Is', Nlo. 8, 19r6.
UssR/Zooparasitclo,gy Ticks and Insects - C--rriers of Disease G.
t i1mv,
.1i. Insects.
Abs Jour : Ref Zhux - Bicl.., No 11, 1958, 48231
Author : Tarvit-Gantar', I.A.) m-,lal,)va 11 P
Inst : Kirjiiz Scientific Research Institute of Epidem-foioCy,
NU-crcbiolo~7, and Fly~,!Jczic.
Title : The Mosquitoes o-1 Kirjiizi-" and Their Coimarative Rpide-
Liiolof,ical SiL7-ificance.
OriG Pub : SI). Tr. Kirg. n.-i. in-ta epidemol., raikrobiol. i ---iL;ilcny,
1956, vyp. 2, 90-96.
Abstract Ko abstract.
Card 1/1
SMIRTIOV. A.D.; TALAWYANA, ~.11.
"'
Growing crystals of substances insoluble in water by the difeusion
method. Xhim. v shkole 13 no.3:45-46 My-Je 158. (MM 11:5)
(Crystallization) (lead chloride)
TALA LYAN, A. A.
TALAUAN, A. A.: "The convergence of almost universally orthogonal
series.1t Acad Sci USSR. Mathematics Inst imeni
V. A. Steklov. Moscow, 1956. (DISSERTATION FOR
THE DEGREE OF CAND1DATE IN PHYSICOMATHEMATICAL
SCIEi%.,CE)
So.: Knizhnaya letop-is: No 15, 1956, Moscow
Calil N-L, :i~-F L 1 Dj 4, f
Transact-if.-ms Il-e Third All-unlon Mathematinal Congress, Mrscow, Jun-Jul '5E,
Trudy '5c', V. 1, Sect. Rpt.s., izdatel'stvc Pd-l SSSR, Muscow, 19156, 237 PP-
Talalyan, A. A. (Yerevan). On "he Convergence Almost
:,,~verpelriere of nj~thogonal Series. 105
SUBJECT USSR/MATHEUTICS/Functional analysis CARD 1/1 PG - 535
AUTHOR TILAWAN, A.A.
TITLE On the convergence of orthogonal series.
PERIODICAL Doklady Akad.Nauk 110j- 515-516 (1956)
reviewed 1/1957
Joining the investigations of Rademacher and Mentiov, the author announces some
new results without proofs
1. If Itfn (x)j is a complete normalized orthogonal system defined on [0'1]
then for every measurable function f(x) a series f a n Tn(x) can be
n. 1
determined converging to f(x) with respect to the measure, where lim an 0.
n :oco
2. If Jfn(X)j is a complete normalized orthogonal system defined on 190119
00
then there exists a series fan S*n(x) converging to zero with respect to
n=1
the measure, where not all a. are equal to zero and lim a n
n
INSTITUTION: Math.Inst. Acad.Sci. USSR.
TALAMAN, A.A.
Inetwel I "p'q"WVRW~'
Convergence in measure of series based on LP space loci. IzY. AN Arm.
SSR. Ser. fiz.-mat. nauk 10 no-1:31-68 157. (MLEA 10:6)
1. Institut matematiki i mekhaniki Akademii nauk Armyanskoy SSR.
(Series) (Sets, Theory of) (Functional analysis)
TALALYAN, A.A.; KHACHATARYIN, 1.0.
Inverse problem of best approximations. Iav. AN Arm. SSR. fiz.-Mat.
nauk 11 no.2:83-87 158. - (miu 11-6)
1.Institut matematiki i mekhaniki AN ArmSSR.
(Functido, Continuous)
TALALYAN, A.A.
Integral representation of measurable functions with kernels
originating un� tary, turansf ormations of the space ~.. (0, C;-) .
Dokl. AN Arm. SSR 26 no.5.-257-261 '58. (MIRA 11:7)
l.Institut matematik-1 i mekhaniki AN ArmSSR. Predstavleno M.M.
D--hrbash.vanom.
(Functions) (Transformations (Mathematics))
16(1.)
AUTHOR: Talalyan, A.A.
TITLE: On Universal Orthogonal
nykh ryadakh)
-.0
-Y/22-1112-1-2/9
Series (Ob universaltnykh orto----onall
PERIODICAL: Izvestiya Akademii nauk Armyanskoy 3SR, Seriya fil-iko-Inatemati-
cheskikh 1 nauk, 1959, Vol 12, !Tr 1, pp 27-42 (UGO"21)
ABSTRACT: '1he author uses notions and denotation2 of Me. Ven'shov
Z-Ref 1,2-7 and proves a generalization of a result of Men'shov.
Theorem: Let (1P (x) be a complete orthogonal normed tiystem
A n
of function' on [a,bl . For arbitrary measurable functions
F(x) and G(x) on Ea,bj with G(x), N , m> N j n ~ m the functions f (x) and f (x) ara
crtho-onal on a set E where mes E > b-a- 6
f- n,m m,n
Theorem: Let I fn(z) be complete in the sense of measure
Card 11/3
On the Representation of Measurable Functions by Series SGV/22-12-2~1/8
convergenc*. and jet the f(z) be linearly independent on an
arbitrary measurable set E , mes Z > a0->0 , where a b - a
I -
is a fixed numbe!-~ Then there exists a sequence (X) ~
With the properties n J
-Xi A
(x) a , f-(x) (x) b (x), n~1,2,,.
r
n n, -Kk n ~7- 1
(X) is asymptotically orthogonal
there
To every measurable function f(x) defined on 11a,b]
CC)
Jts a series
exi a (x) which converges on La b! to
2-- n ?n J
n-I
f(x) with respect to measure.
The proof of the theorem is based on former results of the
author Z-Ref 11,2_7.
Card 2/5
2
. On the Representation of 1~easurable Functions by SrjV122-, 12-2-1/8
Series
There are 2 Soviet referances.
ASSOCIATION: Institut matematiki i mekhaniki AN Ariayanskoy SSR
(Institute for Irathematics and IlechanicsAS Armyanskaya
SSR)
SUBLUTTED: February, l'j, 1958
Card 5/3
6," ~! )
Talalyan,A.A. S0'1/22-12-3-1/9
TITLE. Representation of an Arbitrary Measurable Function by Series in
Terms of Functions of the System of Schauder
i,nIODICAL: Izvegtiya Akademii nauk Armyanskoy SSR. Seriya fiziko-
matematicheskikh nauk, 19591 Vol 12, Nr 3, PP 3-14 (USSR)
ABSTRACT: Let 711-a, W 2-b, a2, be the sequence of all
rational numbers of the interval (a,b). Let T,(W,).l, (Fl(Y'O'
f (t) be linear on [a,b]. Let Y (W 92(t) be linear
1 2 1)=01 T2(W2)_1'
on [a,bj- Let (W be the interval containing V1.1 Let XP(t)_O
i ' "k n
Of iPW I and let k? (W W
outside 17, kI %?n(Y"n)_ n(t) be linear on ig n,
and (W W 0'
Theorem 1: For every measurable function f(x) defined almost
everywhere on [a,b] there exists a series to -f (x), lim 0
n=1 n In n-co n
converging
,, to f(x) almost everywhere on La,b3,
Theorem 2: f' iven an arbitrary complete orthogonally normed sy5-~em.
V~'
La -thogonally no- ed
Card I of functions (X)I defined on b], An oz
Repi,esentation of an Arbitrary Measurable Function SOV/22-12-3-1/9
by Series in Terms of Functions of the System of Schauder
,(x)l ith the following rropertiee can be fc--n':
system t~~ -
a) every ~ n(x) is a finite linear combinaticr- of the T,(-)i
b) to every measurable function f(x) defined an La,b] there ~.xists
Go
a series a converging to f(x) almost everywhere on
y . n kfx)
n=7
b].'
In both theorems f(x) may be equal to +oo, or -oo on an inter-al
of measure different from zero.
There are 3 references, 2 of which are Soviet, and 1 American.
ASSOCIATI07T:Institut matematiki i mekhaniki AN Armyanskoy SSR. Yerevanskiy
gosudarstvennyy universitet (Institute of llilathematics,AS
Armenian SSR. Yerevan State University)
SMEITTED: July 4, 1958
Card 212
TALATYAN, A.A.
Sequences, universal with regard to permutations, making up the bases
of space Lp, Ilokl. AN Arm.SSR 28 no.4:145-150 '59. (MUR& 12-11)
1. Institut matematiki i mekhaniki AN ArmSSR. Predstavlano akademikom
AN ArmSSR M.M. Dzhrbashyanom.
(Series, Infinite)
AUT [foTj A ~1'07/20 ',24 7
TI TLE S'U f S B 9 e s 0 vlne Soace
(7 T
z)
PEE'.IODI CAL: 'D a i y ic -a d S S R 17 o 1 2 1--pp 987-nag (USSR)
ABSTRACT.- f Y - Y - Pt gt~!Ierallized~
satisfy -!he -.-;onditioriss
9~!A a D.~; L ue. L y r a 1 s -a f f L I s rj -y I a r g- S!
Di r s j n a r ho' d6
1- ~M
r. I I M, m a x 0
ard Th-
T umala
a.
Summation of S eri z! Te rc, =- o f Ba s ~-e o f 2,-
Space L Pla b] p Accord! rig 1-~, ~.he M~ ;hcd-, of Cesaro
Is cenvergent- .1oT all suf fiit-ieatly large i; and if the sum
tends te a fini te Limit. valae for -4-~ oo . All the Cesaro
methods oC positive order are TI-methods.
Theore m i Let (x) it be a nox-med basis of L (a,b), P~;-Iq and
f(T) an alrflos~ everywhere firite measurable "'unction on La,b],
T' a d~)nuqerab',~. aequericc- oi TI-methods. Then In the system
ri
x) the ord--r i: fi;he Ze~m-,; c-an be altered so that for
-,he new ".r. Ther.? is a series C (X)
2- n TV
n= n
whi n 1. 95 lu m m aw i t [i Gne sum f-(-c) with every T' - method
11. 00
Meiz shcr-, ander the assumption of the ortho-
W, depe nden ~~e of the sys tam
Card
SIA_-Ma T 1 z n -, fSer ~:!3 i r T'mB a. a c- 3Df ;Ji~-
Spac,e L tnp of Cesaro
I.J." x. a r, dk ..i ride Tne assumpti cn c~ < ,m
n
A a r T E,. a; f -hat ona wm~ionsd above ana
C. n~-,rert gi -ten.
Th F. r,~ a eren-:~e3 of Trnich P-re Soviet., and ! Fren-~,h.
ASSOCIATIONj In3 t t makhaniki All Arm SSR (InstiFut~; of
M a - , 1 - )AS ATm. SSR)
PRESENTED, i e b,,,, A.U, Academician
SUBMITTED~ 0 b e
Card 1/5
85239
S/022/60/0 13/'002/0'10/01 1 XX
AUT'TOR: Talalyan, A.,,A CIII/C222
TITLE: On the Convergence and Summability Almost Everywhere of General
Orthogonal Series 0
PERIODICif-11- Izvestiya Akademii nauk Irmyanskoy SSR, Seriya fiziko-mate-
maticheskikh nauk, Vol. 13, No,. 2, PP, 31-61
TEXT: The author joins well-known investigations of Me-IMen'shov and obtains
the following principal results: Theorem I : There exists a complete orthogo-
nally normed. system ~ ~ ,Pn(x1 of functions defined on Ia,b] so that the develop-
ment of a certain f(x)4~_L 2 [_a,b-1 with respect to this system diverges almost
everywhere, that however, for every measurable F(x) there exists a series
00 a Tn (x) converging to F(x) almost everywhere on [&,bJ . Here F(x) may be-
Z_ n
n=1 V~
come + M or - cD on a set with a positive measure, Theorem II ; Given a
countable set of complete orthogonally normed systems f~(n)(X)~ n=
k
on [a,bl , Then there exists a linear regular method the matrl:'x Ila ik 11 of which
consists of z~eros and unities and which has the property that for every measur-
able function f(x) defined on [a,b_l and for each of the above systems there
Card 1/5
85239
On the Convergence and Summability Almost 5102 60/013/002/0101/011 XX
Everywhere of General Orthogonal Series C111YC222
9? (n)
exists a series 2 a (')(x) being summable to f(x) almost everywhere on
k ~- 1, k IP k
ja,bI according to the method T. - Theorem III~ Let S.'Pn(x)i be a normed base
of the space LpEa.bj, p.>1 and f(x) be an arbitrary measurable function on
Fa,b], Then in (x)~ the functions can be altered so that for the new system
L n I j;g~
there exists a series,~f. c (x) being summable with the value f(x)
I,f~n (x)i n=1 I f-~'-n
almost everywhere with respect to all Cesaro-methods of positive order.
Theorem I fdlows from theorem I ; Let the complete orthogonally normed system
-'Pn (x)~ on Fa,b] have the property that for a sequence a k3- I where
2
z ak + 00
k=1
the series
Card 2/5
85239
On the Convergence and Summability Almost
Everywhere of General Orthogonal Series
which the series
S/022/60/013/002/010/011 XX
CI11/C222
(2.1) f
n
n=I
of functions measurable almost everywhere, defined on Ea,b] is assumed to be
universal and where it is shown that if there exists a subsequence Ifk (x)
so that
(2-4) lim f k.(x) = 0
i-.)~oo I
holds almost everywhere on la,bj , then-the, terms of (2.1) can be altered for
every measurable f(x) so that the
almost everywhere on La,bI according
For the proof of this theorem the
furthermore the author's results
Card 4/5
00
new series z (X) is summ ble to f(x)
k=1 k
to all Cesaro-methods of positive order.
TI - summation methods of (Ref. 6) are used;
(Ref. 7).
85239
On the Convergence and Summability Almost S/022/60/013/002/010/Oil XX
Everywhere of General Orthogonal Series C111/C222
There are 7 Soviet references.
Abstracter's note : (Ref, 5) is a paper of A.A. Talalyan in Izvestiya
Akademii nauk Armyanskoy SSR. Seriya fiziko-mateipaticheskikh nauk, 1957v
Vol. 10, No. 3. (Ref. 6) is a paper of D.Ye. Men'shov in Bull.Soc. Math.
France, 1936, Vol.. 64, PP. 147-170. (Ref. 7) is a paper of A.A. Talalyan in
Doklady Akademii nauk SSSR, 1959, Vol. 26, No. 4 1
ASSOCIATION: Institut Matematiki i Mekhaniki AN Armyanskoy SSR (Institute
of Mathematics and Mechanics of the Academy of Sciences
Armyansicaya z:)btc)
SUBMITTED: January 12, 1960
Card 5/5
8'f 2 1L,
S/04 60/015/005/006/016XX
C 11 !YC-222
AUTHOR4 Tal&!Xan., 'A. 110
TITLE --T'K-e -R,-pr~, sent -a":ion of hlea-3urabl,~ Fu-n,:t:,c-ns by Sexiee
PFRIODICAI,~. U5pekh~4 matemat1-.:heR-k1.kh na-ak, -,960, 711,15, 110-5, pp~,77-141
7EXT: The mcs,~ e~Fpentiai part of the paper ronsiets 4n the in-estigation
o-f the que--ii.-,r.; Le.- ' (.x.) be. a haae -n the L Ta,b-', and f(x) be a
I r
n P ...
i r. e. a au r a b I e def--ned a2vi-.-st everyphez-a on ra,b7, does there exist a
(2)
1~orvarg,lng ',.-.ct f"x) aimt.,st everywhere (o~7 w~-+,h respect to the measure)? In
k, . -
the caE-f- :.'if The mpas,-,Ti~, -.onvergence the author gave afinal result in
12): Fo-r qv,~.-ry n-=ed "zase (x)'~ of the spare I. -I
(Ref". t -~ 1 slid
. n p ~~sb-q p~,, a-
every measurable funct~-Ion f(X) defined &.~;most -everywhere on ~ajb-,` there
exists a s-Zles ~2) w-4th soe~-f,-,:ients tending to zitro wh-L--h converges to
f(x) w~-th z=Epe-ct To the measure on 7ab- -,, In thE caE.e of the sorrrergence
only partial results are given. Extending the above
x) (beslds of the
question, the author Jnvest-gates which sequences f
C /:5
SAO)'4'2 60/015/005/006/016XX
C'I 1, Ig 222
1 C
The Representation of Measurable Punctions by Series
basee of the L p) have the property that. every measurable function f(x) is
repreaen'l-able in the form of the series ,-a nfn(x) whizh converges to f(x).
The present paper is a complete representatIon of the results obtained in
the mentioned. directiona a9 well as on the domain of similar problems, wh4n
es5ecially results of the author (Ref.12,20925), of P.L.U11yanoy (Ref.15,
24 ; of D.Ye.Men,she- (Ref-5,6,7,11,13,21) and NA.,Bari are given. There
axe 12 definitions, 21 theorems and 3 lemmas. Conteatai Introduction. � 1.
Definitions and auxlliary theorems. � 2. Proof of the principal lemmas,
� 3., Representatlor, of measurable functions by series with respect to
beaes of the space L � 4, Zero-series. � 5. Representation of measurable
functions by 5e-les according to the system of 11aar. � 6, Systems of
functions complate in the 5ense of the measure :~onvergencs. � 7- Repre-
sentation of measurable functicnsl by series �n terme of systems complete
in the sense of the measure convergence, � 8. Convergence to +oD of
Card 2/3
85214
The Representation of Measurable Function3
orthogonal series, � 9. Universal series'
Referenses,
The author mentions~ AAN.Kolmoicoro
mever, andj.Ya.Koz1ov, There are
Polish, 2 French an-d-2 American.
S/04 60/015/005/006/016,U
C1 1 1YC222
by Series
� 10. Unsolved problems.
, I.I.Privalov, Yu.B.Ger-
25 references: 15 Soviet, 6
SUBMITTED& September 16, 1959
Card 3/3
38332
/4,466
14.4000 C iii/ C 337)
AUTHOR: Tala,lyan, A. A.
TITLE: On Series Which are Universal With Respect to Permutations
PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya matematicheskaya,
1960, Vol. 24, No- 4, PP. 567-604
TEXT: Let f (x) be a se uence of almost ever,where finite measurab-
I n
le functions defined on r 0,11 . The series
co
(1) _:~ f n(X)
n=
is called universal (in the usual sense), if to every measurable
function f(x) defined on rO,11 there exists a sequence of in-
creasing natural numbers tnki , s,; that
(2) lim Sn (x) = f(x)
k --)- co k
almost everywhere on
n
(3) Sn(x)
Card 1/7
C 011] , where
fi(x) (n = 1,2,_,)
88332
S/038/60'102410041"008101OXX
C I 1 1/ C
On Series Which are Universal With Respect to Permutations
Definition 1. The series (1) of almost everywhere finite measurable
functions is called universal with respect to permutations in the
class of all measurable functions in the sense of convergence almost
everywhere (in the sense of convergence in measurable, in the sense
of summability almost everywhere by the linear method T), if the
terms of the series (1) can be transposed for every measurable f(x)
so that the new series
03
(4) W
k=1
converges to the function f(x) almost everywhere on [0 li(converges
in measure on Fo, 1 is summable with the method T aimost every-
where on LO, 1 1 ).
Definition 2: The series (1) of almost everywhere finite measurable
functions is called universal respect to subseries in the class
of all meaourable functions in the sense of convergence almost every-
where (in the senise of convergence in measure, in the sense of
Card 2/7
883 2
S/038/60 024/004/008-/010XX
C III/ C 333
On Series Which are Universal With Respect to Permutations
summability almost everywhere by the linear method T), if to every
measurable f(x) a subseries
00
(5) fnk(x) (n1-,:-- n2 nk
k=1
can be chosen from (1) which converges to f(x) almost everywhere on
Eo'11 (converges in measure, is summable almost everywhere by the
method T).
Theorem 1: Let ~fn(x)~ be a normed base in L p [0~11 , p > 1,, Then
there exists a series
CD
2 anf.(x) (a. real), where
n=1
(2) lim a 0
n --'> CD
with the property: Por every measurable f(x) defined on E0,1j the
Card 3/7
88332
S10381601024100410081010T,A
C !11/ C 333
On Series Which are Universal With Respect to Permutations
terms of (1) can be permuted so that the new series
Co
-7 a'IX IP0N(x)
k=1
converges in measure an O'l ] to f(x)~
I E
Theorem 2; Let "n ~ be a Haar orthogonal normed system: A series
CD tyn(x)i
(1) z anlfn(x)
n=1
exists so that for every almost everywhere finite measurable
function f(x) defined on [O,Ij the series
00
(2) an Irn (x) n n2 n,, <
k=1 k k
Card 4/7
88332
s/038/60/024/004/006/01OXX
C Ili/ C 353
On Series Which are Universal With Respect to Permutations
converges to f(x) almost everywhere on E0,1j
Theorem 3: If the series
OD
z U. n(x)
n=1
where un(x) are almost everywhere finite measurable functions de-
fined on Eo'i is universal in the sense of convergence in measure
with respect ~o permutations, then the terms of this series can be
permuted so th;--t the new series
00
U') (X)
k ~= K
is universal in the usual, sense.
Theorem 4: Let a Cesaro Lmethod of positive order be given. If
OD
:~;- fn(x),
n=1
Card 5/7
88332
3/01~8/60/024/004/008/01
C !!I/ C 353
On Series Which are Universal 'With Respect to Permutations O7X
where f n(x) are almost everywhere finite measurable functions
defined on E6,13 , is universal in the usual sense, and if
lim fn (x) 0 holds almost everywhere on EO,1 3, where
k --), 00k
n1< n 2 < < n k- 1, there exists a series I a n'f n(x), an-> 0, which is
Card 6/7
88332
S/038~060/024/004/008/01OXX
C 111 C 333
On Series Which are Universal With Respect to Permutations
universal with respect to permutations in the sense of summability
almost everywhere by a given Cesaro method.
The author mentions P. L. Ullyanov, N. K. Bari, Yegorov and D, Ye.
Men'shov.
There are 11 references: 7 Soviet, 2 Polish, 1 French and 1 American.
ASSOCIATION: Institut matematiki i mekhaniki AK nauk Armyanskoy
SSR Yerevanskiy gosudarstvennyy universitet,
(Institute of Mathematics and Mechanics of the
Academy of Sciences Armyanskaya SSR Yerevan State
University)
PRESENTED: by J. N. Vek-ua, Academician
SUBMITTED: June 8, 1959
Card 7/7
7
I ~oo
AUTHOR: Tal _a~yan,__A.A.
29836
S/044/61/000/007/005/055
C1II/C222
TITLEs On the limit functions of series in terms of bases of the
space Lp
PERIODICALs Referativnyy zhurnal,Matematika, no. 7, 1961, 5,
abstract 7 B 19. (Dokl. AN Arm SSR, 1960, 30, no- 3, 129-134)
TEXTt The author gives (without a detailed proof) assertions the most
essential of them generalize the results for trigonometric series proved
by D.Ye. Men'shov (R zh Matp 1959, 1378). E-g- there holds the theorem
(definitions cf. R zh Mat, 1959, 1378): Let F(x) and G(x) be measurable
functions defined on [0,1] so that G(x)!S F(x) almost everywhere. If then
a non-empty set of functions M - I Y(x,E)j satisfies the conditions
*(,) , 6) and r) , then for every normed base '(X) f of the spqce
L (0,I) with p> 0 there exists a series
p 00
Z anfn (x) (lim a n = 0) (1)
n-1 n-*oo
Card 1/1
On the limit functions of series
29836
S/04 61/000/007/005/055
... C111YC222
so that M is the set of all of its limit functions, while G(x) and F(X)
are its greatest lower bound and least upper bound with respect to the
measure on [0,11 . The author also gives an assertion having a new
character (even with respect to the form). Namely it holds the theorem a
Lat fpn(xq be a normed base of the L p(0,1) with p> 1. Then there
exists a series (1) so that for every set M ~0(x,E)3 and functions
P(x) and G(x) (G(x)!S F(x)) which satisfies the conditions v-), 8) and
a certain rearranged series (1)
00
Z ay k k(X)
k=1
has the property that M is the set of all of its limit functions, and GW
and F(x) are its greatest lower bound and least upper bound with respect
to the measure on [0,11 .
[Abstracter's notet Complete translation
Card 2/2
TALALYAN, A.A.; LMEYAIT, E.M.
Average polynomial approximation in a single circle.
Dokl.A11 Arm.SSR 31 n0-1:3-8-160. (MIRA 13:9)
1. Institut matematiki i mekhaniLri Akademii nauk Armyansk-oy
SSR. Predstavleno akad. All ArmSSR A.L. Shaginyanom.
(Polynomials) (Approximate computation)
S/022/61/014/003/002/008
D201/D304
AUTHOR: Talalyan, A.A.
TITLE: Convergence of a Fourier series in infinity
PERIODICAL: Akademiya nauk Armianskoy SSR. Izvestiya- Seriya
fiziko-matematicheskikh nauk, v. 14, no. 3, 1961,
35 - 41
TECT: The author derives a theorem stating the conditions in
which a trigonometrical series
00
0 1- a cos nx + b sin nx,
2 n n
n=1
which may be a Fourier series, is convergent in positive infinity.
Theorem: There exists a function f (x) for a given number p -, 1 of
the class Lp L- x, "I and a quantity A '--/- X, Yc/ such that: a)
the cross section of the quantity A with any interval in the limits
Card 1/11