SCIENTIFIC ABSTRACT TALALAYEVA, T.V. - TALALYAN, A.A

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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 'LO-6 ...... Card.3/3 2 90-1. S/020/6! /140/004/0' S/C2'~ -'-6/'B 0 V -2 S rl e: V .r,_ 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 t-zs g '6 T ., g j I : C. -J,1.111 ""CISIC 'A'. 'I 'o uo 2-1-P-3 JO -(21-0t-4 -A-V i .... joid -12 4 oc~ uw, Z..P..T Ctl .1yalcolgla -M-T"f -41 7. 411--luo ;,.,d -.dd C..J~s 131111 'J.4"T we 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