SCIENTIFIC ABSTRACT YAEK, I.V. - YAGAFAROV, L.M.

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SCIENTIFIC ABSTRACT
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'23338 /61/CC1D/006/02'4/016`1 -'/A101 A OW //3 7/ I.V. AUMOR. (a ek) ~e TEM Sensitized phosphorescence of NaCl_Tl, Mn PERIODICAL- Referatinuy zhurnal, Fizika,, no. 6, 1961, 178, abstrao,, 6',D,::4 C'TT. 3-n-ta fiz. i astron. A74 EstSSIV, '1960, no. 12, 278 - 280) Tk-,s- auth-:~r studied the phenomenon of sensitized phospbores~!enoe in 21. Ife.C.1-71, M-n prs~~ared e- diffusion method from the gaseous phase. The- abs-orp- P h cs.re,trum of Fm was obtain(*d as well as the emission spectrun at ex- "'a-i= 4n regicn of transition 1SO--..--3P in i?ns of Tl+. ThR emission spec- of two main bands (trars4_tions 13p --)Paso in T1+ and G-:91 6S in ~tn2+) aorpearing I-,I +hA_ spentrum of afterglow. The phosphoresf.';ence spectrum in the re- gion of If 0-7~8 zran_:Iticn, measured a few minutes after discont'-nuation of ex- citat'l-on in the T1 absorption band, coincides with the fluorescence spectr= of rtr~2~, One. IM 2+ Ions is located 4n hs spectrin of phosph rescence excitation o? Mn the region of the absorption band S,---~71PIof Tl+ ions. in sy-etem.3 yielding Sensitized fluoresoence (NaC1 TI, Rn) the effect of "memorizing" of excitatf-on Card i/2 23338 S10581611OW1006102410631 3enz!tlize-d phosphore3cance of, NaCl-,Tl, Mn AOOl/AlOl plane do,~s not arise (RzhFi-Z, ig6o,, no.- 11, 31259); this, In the author opinion, Is acnne-,~ted with `-,he mechanism of sensitized p osphorescance of N&M-Tl, Mn whioh consistB in the, erarrj transfer from exoIted Tl.+, originated as a result of a re- ~~Oyrlblnetfon proaeBs, to M--q2+ lons being in Proximity. (Abatre-~~ter's no C.-mplete translatlon] Card 2/~2 24663 S/O 1611000100910031015 ul B101 B205 AUTHORS: Liyd'ya, G. G., Yaekj_I. V. TITLEt Formation of F centers in the KI-Tl.crystal by ultra- violet rays PERIODICAL: Referativnyy zhurnal. Khimiya, no. 9, 1961, 31, abstract 9E,213 (9B213) ("Tr. In-ta fiz. i astron. AN EstSSR'1j 1960, no. 12, 281 284) TEXT: The formation of F centers in monocrystalline layers of the KI (Tl) phosphor has been studied in detail., It was.found that the accumu- lation of light energy exhibits three different mechanisms, depending on the excitation energy: an electron-hole, an-exciton.., and a "delo- mechanism (RZhKhim, 1960, no. 9, 33849), all of which lead to the formation of F centers. The luminescence of-KI(TI) during excitation has also been studied. The steady luminescence consists of two compo- nents, i. e., a llrapid11.1~p (fluorescent lifetime shorter than I see and a "recombinative" one (fluorescent lifetime of the order of 1 min.. An Card 1/2 24-663 --3L, Formation oIf centers in the.... S/081/61/000/009/003/015 B101/B205 external temperature quenching is observable during excitation within the main absorption range: The recombinative part is quenched at 260 " 3700K. This occurs long before the internal quenching sets in. [Abstracter's note: Complete translation.] Card 2/2 68331 1 b -1 3 b/40 Yaelr, I.V. and Liy,,'Iya, G.G. AU OR- -Recombination Dxflinoscencr, in the TIME, Ucjt~~tioa o Bands of'Gortain Halides FERIODIU;1- Optlka i spelctroakopiya, 1960, Vol 6, Nr 1, pp 142-14-4, (US31R) ABSTRI'XT - L=inescence of actirator ions is excited in the fundkimental abscrutior-, bar4a, of alkali-halide pbosphors . Transfer of anergy fro-,, the !,As* to the; activa may occur 'via excitony, or as a result of ele proceases. Ir. tho latter alse, atth,~, lectron recombination lujiAnescence is possible (free electrons recombln5 nith holos loealized at or r-rar liualni~;scenco centres) or holo recombinatiou luirinesconer;i (holes rec=binn Y!Ith electrons localized at or near Iviaineseenco cantres). The rolativo importance of the!.:e prrlccs-,.e5 mas studied usinl; e-rcitation-sprictra of steady-state luminescence and recombination l=inescence (phcsphore3~,e_nce'). This ctudywav extended to fundamental absorption bands corracponding to e7-citor. formtIon. and "bard-band" transitions, Alicali lodidcr. (XIM., Csl.Ti, RbI-.Tl, Gdl,,-.Pb) .,p3.th fundwilental abaaaq~.ion t>anir, lying in the region I >165 m1i viare the obj oots of this Investl gati.o.%. Thr) axcitation spoctra of phoaphoresconco were the flinctio-m If '2) IM (V) Car hk 68331 ~~xcitation of Ru,;ombiratlon Lwainescence in,the Fundala-ental. 4bsorrptlon; Bandu of csrtaim-Halides. m h -i at a time t sinco I a ondl f . ro I'l IF, the intensity of ~%ftorFlm th 0 etcltatto'n. and B(V) la~ the intensity of the A-)~citiag'll &,.t Und or t I -conditions of total abrior;~tlon, (neglecting reflection loat;eG) thozo funotions;aro the pho8phoroi;cence yiql.d spectra. Th6.phophors -i:ara excited u6inG 11 C-ht of-186-225rvt 1'rait a.condensod 4park botween Zn. au, or, X> 210 mtL the phosphorz; ware alyw exdit- Al aloctrades. ~ In the regi v1th lig)it frota a h~,drr'Gon Imp Vassod throur)i a moaochromator of a -rophotomotor U-4. The qvatitity B(" was foun! Loin,, Rn anthracely.0 &Cr6or- FhO)3 pho r ea,c once vias recordod *1th a photoelectric o otom'-Nt,~r, h conjilatln6 of FEU-19, a d.c.-mnoliflor a%l an automatlc-racordin6 -y of potentiometer EPP-09.1 A special. ~,hoal chowed that th-, Intan3l+, loulinL.)SCence was proportional. to the intensity of tho excitina light. A fir the baae (curve 1), ,ura on p 1-13 shaws the absorption spectrum of the cocitation spectrum of Phosphor6s coneo (curve 2) and of steady s ats luminOsconce (curve 3) of KI vith 0.06 mol~7. of Tl (the uppar plrt of the figure) and of RbI.T1 (the lower Fart of the figural, . Th* excitatioa spectr9L of tholreina-Ining Iodides were similar. Three rogions can be distiniru'shod in.tho absorption spectr=,-, the activator abaorption (translitiona .13, o tPj in Tl+ ion;), th.o exciton absorption _~Pl an~ Ca rd z/3 (ex) and the abaorption correspondini to "band-band" transitions (e + p) I., ,nt -work 'Was carried out under the direction of Ch. B. Lushchik. There a Iro 1 figure and 11 references, 7 of which are Soviet, 2 English, 1 Gelman and 1 translation from Ca rd 3/3 English into Russian. SUBMITTED: June 10, 1959 4S' ~h 470 4& 'I. cl 00,6;2 0 4 ~% 0-~ 06 64 *~ Ot '? 0 -he --0, A60 OLE 4.6 0-20 *.bh t4, - pw Ql oe or* -t 0"'D 0 9 0, ~q cl, ~06 , ~14 :tc *0 4 4~4. 0 0 &0 01, 00 0.... ITV or -4? or Zo v 4,t 'Al~ k i2 2 ~ .I .0v 0 0,~- ~,-- *~~. I 0.~ cozr 0 ;? 0 06h Ik -1~ Q111 ~to 0 po 0-1 "a 00 r*4 t.006 ve -to G 0. 6 60 O's. VI 17 016 10 10 00 0 0 Q.,f 0c, 0 C'-r k0 60 00 64 k 04. ;P, ~h V, 0 %o 6, 0 :~v QQP 0&;S ,1.96 "?, "" Iloa ltr 00 49 06 6 0,) 0 9,Q, 0 0 , r e 4? 4~~ 0 "Ve C, 1 0 '1 64" 0 6j- -P 0 Lt 0" a O~ q6 q Ps 06 Ot 006 op ~17 % %,6 04 00 L, 4~q GIN, ;Z 14, 68332 AUTHORS s Kark, V. Ya., Lushchik, Ch.B. and Yaolt, I'V. T I TLS On Sensitized ?hosphoreseence of Halide Phosphor Grystals MRIODIULs Optika spektroskoplya, .1960, Vol 8, TIr 1, pp 144-146 (USS.R) -i*3TRkCT.- The paper deals vilth sensitized phosphorescence of activatoi allmli halide crystals. The mechanism of this phosphorescence differs radically from sensitized PhOGDhorescanco of organic molecules (Ref 11) and from sensitized luminescence of ZnS phosphors due to migratioli of holea. The authors in,7esticated the excitation spectra of phosvaorescance (the technique -was descrIbed earlier, Ref 13) of KBr%Tl,ln. It ras found that recombination luminescence of T1+ ions is excited or, absoxption in the thallium ab3orption bands and phou ph ores cence of indium on absorption in the indium absorption bands. The phosphor seem; to "remember" the natiare of excitation. Sensitized phosphorescence did not occur in lBr%TI,In. Follo-wing a cuggestion by ons of us Shvauts and Zirnits investigated sanGi-tized fluoroseenze of several poly.-activatod phosphors (Ref 14). In agreement with the do-ta reported R by &iorican workerj (Ref 15), a transfer of energy betwoin PV-1 ar4 Un++ was observ8dAn 1TaC'.jFb,1fn and KGlsPb,Lfn phosphors. 'livartu and; Zirn),ts found alia trarafer of enorgy from Tl'1' and Iri~ Jon-f to tin', 10-nu Card 1/3 in NaClM,Ka and NaGIsIn,Mn phorphors Malyshe-v found 51milar 68332 On Sanalti?ed Phosphorescence of Halide Phosphor Crystals SOV/51-8-1-3.9/4ri behaviour in GdBr2sPb,Mn and CdI2tFb,Mn system;& (Ref 16). The present authors attempted to find sensitized phosphorescence in system in-which sensitized fluorescence vas observed earlier, e.g. CdBr2sPbSMn -which exhibits strong recombination luminescence (Ref 3)u A figure on p 145 shows the excitation spectra of phosphorescence of Pbl~ (curve 1) and Mh++ ions (curve 2) of the latter phosphor. ~he spectra are identical and they correEpond to tho activator absorption by lead (transitions 1330 -+ 1P, and 1-130 -* 3Pl transitions in Pb44'ions). At 2.930K phosphorescence of Mn++ ions veg, observed many seconds after excitation.in the absorption bands of Pb++ ions 6P1 transition); this is, of course, sensitized pho3phoresconce of CdBr2:Pb,lfn. The figure also includes the luninoscence spectrum of CdBr2-Pb,Y-,l (curve 3) excited in the abisorz)tion bai-4 at 3.9 eV, the latter corresponding to the electron tr-ansition 13 ()-.1- 3PI In Pb++ ions* No bands appear in lwainescinoo, ono of which 'wac obsorved also in Cdlir2.-Pb and corrosponds to the transition IF] --.I, 'so in Fb4+ ions-The second band in curve 3 (at longer Cere 2/3 wavelengths) appears aiter introduction of manganese into CdBr2-.Pb Vr 68332 On Sensitized Phosphorescence of Halide Phosphor Grystali and corresponds to transitions 4G--C~ 'in Un++ ions. The figurT on P 145 includes also a qualitative phosphorescence spectrw, of CdBr2sPb,Un (clarve 1), obtained after excitation in the 3.9 eV bani. The similarity of the spectra at the moment of excitation and of subsequent pho;phorescence indicatez resonance energy transfer to Mn++ ions after excitation of Fb4+Jons and as a result of intermediate recombination processes. There are 1 fipure and 17 ref arences, 3.5 of, which are Soviet and 2 English. SUBMITTED; June 10, 1952 0,q%id 3/3 81217 S/0-rl/60/009/01/012/0,31 E203./3691 AUTHORS S Lushchik, Ch.B., UYVA, G.G-, Uok, I.V. and Tiy!ler, I.$. TIMIS The Mechanism of the Recombination Lumineacence of 4etivated Allmli- Halido,GrysfAlz FIRIODICALs Optikz Ispektroakopiya. 19610, Vol 9, Nr 1, pp 70-76 (USSR) ABSTRACT: This paper viam, presented in an expanded version at the Conference on Ph;~sics of Allmli-Halide Crystals (Tartm. June 1969). The authora roport and discuss the results of an Investigation of the reconbinatim luainescance (due to recombinationof eleativus and holas) and phatoohmnical transitions (optical blea hin ) in 101, Or and KI crystals activatoa with Gs;*, G64+. ln+ocS;f, T1+ and Pti+f-. The. cryatals were excited withl-raya and light In the regUms of =Uton and activator absorption bands and of the 'IbmzO-band" tmmitiono. The role of electron, hole, exciton and awaitization proceamea i9 dismmed. The discussion is illuatrat6d by excitation, lumineaccuce, the=01minescenco, optical flash stimulation. optical 9j24 thental bleaching spectra (Figvl-Q. There are 6 figures and 32 referenc,-A, Card 1/1 ZO of *h1ch are -Sovist and 2 Inglish. 'SUWTTNDs Septsuber 28, 1969 1116 S)6ly6l/000/014/010/019 114 -3) D207 D303 ~AUTHORS: Liyd'ya, G. G.j and~,~ek ~I. ..TITLEs External thermal and optioal quenohing of KIM photo- luminescence SOURCE: Akademiya nauk Estonskoy SSR. Institut fiziki i astrono- mii.- Trudy. No. 14, 1961. Issledovaniya po lyuminest- sentsii, 236-246 TEXT: --The authors studied'the effect of external quenching (heat- ing and infrared F-band illumination).on luminescence of the KI phosphor containing 0.05 mol. & Tl; external quenching means pro- cesses occurring outside luminescence centers.. A thin layer (4,u) was used and the Tl+ emission was selected by means of filters. The phosphor was excited with shor-Vultraviolet radiation in the fundamental absorption region. Excitation atAL = 219 i;u produced anion excitons and at A = 186 n~a it generated free electrons and holes. The rise curve showed th t luminescence consisted of two components: A "fast" component which rose to its steady-state va- -Card 1/2 3/61V81/000/014/010/019 External thermal and D207/D303 lue in less than 1 sec from,beginning of excitation and a "slow" ~component which reached the steady state in about 1 min. The fast component exhibited no optical quenching (it was unaffected by F- band illumination), but it was quenched thermally at 500 - 6000K. It was, thereforeq concluded that the fast component represen.ted "direct" excitation of activator ions. The slow component was quenched thermally at 250 - 3500K, indicating typical external quenching of recombination luminescence. P-band illumination Q, 680 ;u) quenched the slowcomponent when excitation produced inter- band traneitions, but the slow component was.enhanced when ultra- violet excitation generated excitons. A simile theory, accounting for the observed quenching and enhancement of the slow component, is given in the paper. Acknowledgment is made to Ch. B. 1jushchik who directed this work. There are 2 figures and 21 references: 19 Soviet-bloc and 2 non-Soviet-bloc. The references to the English- language publications,read as follows: H. Klasens, Nature, 158, 306 (1946); P. 111'eitz, Rev. Mod. Phys., 26, 7 (1954). SUBMITTED; August 9, 1960 Card 2/2 S/058/6Z/000/008/043/1,'24 AO61/A1O1 'AUTHORS: Lushchik, Ch. B., Liydlya, G. G., Soovik, T. A.;,~ ~ek I_. V. TITLE. The mechanism of the luminescence of alkali halide crystals under excitation by ultraviolet'and hard radiations PERIODICAL: ReferativnTf zhurnal, Fizika, no. 8,-1962, 42, abstract 8V294 ("Tr. In-ta fiz. i astron. AN EstSSR11, 1961, no. 15, 103 126; summary in English) TEKT: The physical processes taking place in ionic crystals under the action of UV and hard radiations are exanined.. Attention is chiefly-devoted to the interaction of different elementary excitations of the*basic substance with luminescence centers. An attempt is made to appraise the relative-role of ex- citon and electron-hole processes in.gamma and R luminescence. There are 7~ references. [Abstracter's note: Complete translation] Card 1/1 s/o58/6z/c-0o/oo8/o47/134 A0611A101 AUTHORS: Yaek, I. V., Eksina, T. I. TITLE; Non-isothermal relaxation processes in KBr-Tl single crystals exposed tol-radiation and*ultraviolet excitation PERIODICAL- Refiarativnyy zhurnal, Fizika, no. 8,.1962, 43, abstract 8V300 ("Tr. In-ta fiz. i astron. AN EstSSR", 1961, no. 15, 127, 137, sun-nary in English) TOM Non-isothermal relaxation'processes in deformed and non-defLormed' -.KBr-Tl crystals,excited by X-rays and also.by ultraviolet radiation In the.re- gion of activator and exciton absorption bands are.intercompared. The causes of divergences in the course of the relaxation processes for different forms of excitation are discussed. .[Abstracter's note': Complete translation] Card 1/1 , rl-a:~iilttzse"~awaw-iwa~----- -- - - --- - 89237 S/048/61/025/001/003/031 /113 7) B029/Bo67 AUTHORS: Luchik, Ch. B., Liyd'ya, and_Yaek,_-1----B-. TITLE: Mechanism of the processes of energy accumulation by crystal phosphors PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, v. 25, no. 1, 1961, 23-27 TEXT: The present paper deals with the following mechanisms of energy accumulation by crystal phosphors: production mechanism of F-centers'in crystals, and mechanisms of thermal and optical "de-excitation" of ion crystals. Three stages are distinguished in energy accumulation by crystals: 1) production of a long-lived excited state; 2) long-lasting conservation of the excited state; 3) processes.of"de-excitation" of the ~6tybtal. D. I. Blokhintsev (Ref. 1) showed that the electrons and holes occurring after excitation are localized at lattice defects which are far from one another. For this reason, their direct recombination is impossible, an~i the electrons or holes must be set free from the trapping ~centers for "de-excitationil of the crystal.. Intense ion diffusion prevents Card 116 89237 Mechanism of the processes of energy ..... B/048/61/025/001/003/031 B029/BO67 the crystal from remaining in the excited state for a long time. Even in the production of the simplest 'F-centers it is necessary to take account of both the active role of electron - hole processes and exciton, sensitizing, ion processes, etc. The number, nP of F-centers can be concluded either from the absorption XF_ n., from the intensity of luminescence photo- stimulated in Che F-region, or from the electron emission photo-stimulated from the F-centers. The accuracy of the two last-montioned methods exceeds the first by several orders of magnitude. Fig. 1 shovis the absorption spectra (1) and the spectra of the production of F-centers (2) for the phosphors KC1 - Ca, Tl;1KBr - Ga; KBr - In; and KBr - Tl. According to the data obtained, the P 1 states of monovalent impurity ions can be "de-localized" with a certain probability, which results in the formation of F- and V-centers in the basic material of the crystal. Fig. 2 shows the spectrum of the production of F-centers in KI - Tl as measured by the luminescence method. F-centers are formed not only in the ac region but also in the,ex (-220 m)u) and ep regions (-190 mp) with even stronger efficiency. The production mechanisms of P-centers in the ex- and Card 2/6 Mechanism of the processes of energy ..... S/048/61/025/001/003/031 ep~-regions differ from each other. The dislocation mechanism of the production of F-centers'needs additional investigations. The authors then discuss the mechanisms of thermal and optical de-dxcitation of ion crystals. The'third stage of the phenomenon studied here has been investigated in ~'revious papers. The thermal destruction of F-centers in alkali-halide crystals does not lead to their direct thermal ionization. For the NaCl, icl, and Or crystals, the thermal destructIon of F-centers in the range 100-3000K is connected with hole processes'l in the range 400-5000K, however, it is related to electron processes. The ultraviolet radiation at the same frequencies (in the ex and ep regions) is capable of producing and destroying F-centers. Finally, the authors demonstrate that alkali- halide salts are typical crystal phosphors. During an investigation of the luminescence of alkali-halide salts with excitation in the region of self- gbsorption of the crystal it has been found that many phenomena observed in these crystals are the same as in ZnS phosphors. This investigation was carried out at Tartu. Further details on this subject will be published later. This is the reproduction of a lecture read at the Ninth Conference on Luminescence (Crystal Phosphors), Kiyev, June 20-25, 1960. There are 2 figures and 3a references: 32 Soviet-bloc and 5 Card 3/6 89237 Mechanism of the processes of energy Tion-Soviet-bloc. ASSOCIATION: Institut fiziki i astronomii Akademii nauk ESSR (Institute of Physics and Astronomy, Academy of Sciences of the EBtonskaya SSR) Legend to Fig. 1:.spectra of absor tion W, of F-center production (2), '6f negative, excited absorption (35, and of the production of activator centers (4). - Legend to Fig. 2: 1) absorption spectrum, 2) spectrum of the excitation of steady luminescence, 3) of recombination phosphorescence, 4) of optical flash-up, 5) and 6) emission spectra in the case of steady luminescence an d optical flash-up, 7) s ectra of the stimulation of optical flash-up p 'Card 4/6 1/003/031, S/04YB61/025/00 Bo 67 B02 , - ener of - 9 - Mech6 ism of"tho Prpc . : esse9- ,v# gy *7~ . ......... VI ti Ca~d. 516 5/048/61/025/001/003/031 ~Mec hanism. .of'the pFooesses 'of---ener' 9T - - .BWq/bo67 2.. . 3 V v X ar 6/6 20838 S/048j6i/025/003/027/047 YI 3~00 0 15'3) 131,S) B104/B214 AUTHOR: Yaek, I. V~ TITLE: Investigation of the effectivencas of recombination lumines- cence of alkali halide crystal phosphors PERIODICAL: Izvestiya Akademii nauk SSSR. Seriya fizicheskaya, v. 25, no. 3, 1961, 379-380 TEXT: This paper was read at the Ninth Conference on Luminescence (crystal Phosphors) held in Kiyev from June 20 to 25, 1960. For a general investigation of nonisothermal relaxation processest a so-called "relaxation combine" was developed by the authors. With the help of this combine, the curve of thermal decoloration K(T), thermal de-excitation I(T), and thermo-optical det-excitation IX(T) of a crystal can be simultaneously reoordedl and the "instantaneous efficiency of thermo- luminescence" can also bd measured. The latter characteristic is do- termined from the formula: Q,(T) - I 4-n /-rd- Tt] T Card 1/3 ARM! 20838 Investigation of.the effectiveness... S/048/61/025/003/027/047 B104/B214 Here, I is the intensity of luminescence, and n the number of color centers. The:experimerital determination of this characteristic requires the simultaneous measurement of I(T) and k (T), since n mIT . These quantities were determined for single crystals of KC1-Tl, Ur-Tl, and NaCl-Tl irradiated with X-rays. The resul-,a are gzaphically represented in'Fig. 1. -The curves are schematic. Curve 1 represents the thermal decoloration of the F-bandp curve 2 that of-the band with Am . 360 m/-,, Curve 3 represents the thermal de-excitatic.1 (with separation filter for the luminescence of the Tl+ ions), and curve 4 shows Q(T) for the phosphor KCl-Tl. It is supposed that the step-like character of Q(T) corresponds to differentelectron and hole states+of the relaxation process. At the va rious staA;es, the value of Q(T) varies from 0 to co. The infinite values are due to the circumstance that in the range of investigation the ~P-centers are not destroyed and the observed thermoluminescence coincides with the decomposition process of other color centers. The vanishing of Q(T) is related to the low effectiveness of energy transfer from the recombination centers to the luminescence aenters~ and is usually obtained In the hole 3tatee of the relaxation procEBf3a Curves 31 and 41 in Fig. 1 Card 2/3 1a mpuo84 AUTHOR,3:: Yaek$ ile V.J% Okkj M 9 F T MiLS Rdbombina,tion luminescence spectra in KCI crystals activated with mercury- like ions _n6 SOURCE: AN Eatc SR. Institut Miki i astronom:Li Trudy*., no, 21,'1962 96 TOPIC~TAGS: spectra., luninescence spectra., act_~.vated crystal, emission c.enter., recombination. luminescence spectra,,,potassium c)Lloride crystal,, mercury like Aons ABSTRACT: By means'of.photoelectric methods; r,!combination luminescence spectra (spectra of.optical flash stimulated in the F-b-2nd,spectra of thermoluminescence and phosphorieseGnee) in 0:1-0a) KCI-Sn~ , zarA YCl-Pb phosphors previously, excited.-rith x-rays have been measured. The KOL.-In,, 01.6a and KCI-Sn clystals -.were prepared by the Stokbarger method and the rest by the Kircgoulus techniquee As spectrometer, a m onochromeAvor spectrometer SF-4 was wed with photoelectric multiplier Ya 4"033' aard potentiometer LTP-09., It is shown that the spectr.-a :compo3ition of electronic recombirational lumineacence corresponds in the main to (GA+ In+ -Ll+) and the activator ions in phosphors activated both by monovalent C rd ::l S104 62/026/004/008/014 B104%102 AUTHORS: Lushchik, Ch. B., Lushchik, ff. Ye. and TITLE1 Electron oscillation processes in luminescent centers of ionic crystals PERIODICAL: Akademiya nauk SSSR. Izvestiya. Seriya fizicheskaya, v. 26, no- 4, 1062, 488-496 TEXT: On,the basis of papers published from 1913 UP to the present time, a. review has been compiled on the rules governing the electron oscillation processes in ionic crystals. Special attention is devoted to effects involvin- excited states of impurity centers.- Results obtained for + 2+ + 2+ 3+ + alkali-hali.de crystals activated with Ga , e , In , Sn , Sb , TI Pb 2+ , and B.13+, and also for NaCl, KCI, KBr, and KI crystals activated with indium, gallium, antimony, germanium, and bismuth are discussed, This review articlefurther deals with the steplike dependence of the quantum yield of photo-effects in ionic crystals on~the frequenoy of the Card 1/2 Urd R-~P$7.A MoXtM94 s/048 16210261oO410081014 Electron oscillation processes ... B104/B102 exciting light. There are.5 figures and 1 table. ASSOCIATION: Illstitut fiziki i astronomii Akademii nauk ESSR ~(Institute of Physics and Astronomy of the Academy of Sciences Estonskaya,SSR) Card 2/2 -.'ACCESMON NR: 'AT,40MOI 8/2613 63/000/023/0165/0169 AUTHOR: Yuk, Is 17 Okk Us: Fe: TITIM Recombination luminesoOn"APectm Of KBr crystals activated with mercury-160 tons 6OURCE:, AN EMSE., Institut fisiki I astronomil. Trudy*. no. 23, 1963.. ;ssledovaniya po lyu3ninestsentaii Otesearch in luminescence), 165-169 A TOPIC TAGS: lumbascenoe, luminescence spalctruln, - alkali balide luminescence, mercury-like luminelacence'activator, recombimation luminescence, phosphor, cryst;a- line phosphort thermoluminescenoe. ABSTRACT: The authors point out that, for the study of the mechanism of recombination luminescence of cryi3talline phosphors, various optical. electrical and other methods are in use, the majority of which fall Into one of two classes: 1) Study of the action of radiation on excited or non-excited phosphors; 2) study of the relaxation characteristics of the phosphors. Various techniques for the study of thern Ineecence are discussed and their relati.'ve malts are analyzed. It Its noted that the study of thermoluminescence cannot completely roplace meamements of "Integral" curves of thermal glow, since the restoration of the cUtailed variation of the winn Intensity of thermoluminescenoe, Cwd 1/2 ACCESSION NR:; AT4020801 Important in a quantitative Investigation of the kinetics of the relaxation processes, to difficult and time coimuming on the basis of measured spectra. In this article, which to a continuation of the Investigation begun in a previous work (I. V. Yaek, M. F. M. Trudy* IPA AN ESSR, no. 21, 96, 1962), the authors investigated the recombination luminescence spectra of X-rayed KBr-phosphors. Thermal glow curves and thermo- lumine~cence spectra of Tl+-, In+-, Ga+-, Sn2+- and Pb2+_ activated KBr were mea- sured. . It was found thati the'thermoluminescence, spectra obtained coincide fairly well with the activator fluorescence spectra. There Is a discussion of the limits of applic- ability of the spectral investigation method of thermal glow. The thermoluminescence characteristics of Sn2+- activated phosphors and those of in- and Ga-activated phosphors were found to be sinillar. The hypothesis is advanced that this similarity is due to the ability of SnZ+V+ceni;ers to capture both electrons and holes (V+ to a cation vacancy). The reasons for the absence of thallium Ion emission during the low-tetnperature stages of the relaxation process are discussed. "The auth 'ora express their gratitude to Ch. B. Lushchik fox, his supervision of the work. Orig. art. hast 6 figures. NEW ON: Institut fiz*I I astronomit AN EstSSR (Institute 'of Physics and Astronomy SUBMITTED: 1IJazhG3 DATEACQ.- 07Apr64 -ENCU 00 SUB CODE: PH NO REF SOV: 026 OTHER: 002 Carld ACCISI ION NRS A10421*02 3/63/000/023/0170/0174 AUTHOR: Yeek,,I ;TITLE: Exc I tat I(xi of Impurl ty centers In alkell 60de crystals during electron- 'hole recomblnatlcma SOUR66 AN EstSSR* lnstitut.:flzlkl I astronomll..Trudy*, no. 23, 1963. rch In l1nescence), '170 Issiedovanlya po lyuminestsentsil (Resea .174 TOPIC TAGS: lumInesience, phos hor, crystalline phosphor, alkali halide, alkali P halide luminescence, photoexcitation, impurity ex'cltatlon, electron vacancyl electron hole recombination, luminescence center~actlvatlon Ants o6t tha ~th fol I" In- are the possible mecha Isms 11 ABSTRACT: Thi juthor po, t a ow g n of luminescence center.excitation,in al "ll halide crystals: 1) direct photoex- 'citation of the center; 2) excitation of the center by impact; 3) recombination excitation of-the center. Th4 fl~st two mechanisms have already been studied rather well; hoWever, the third mechanism - cehter"excitation as the result of the transmission to It of energy liberated during electron-hole recombinations - has. i thus far been.stpdied only,ln general terms...In*this article It-is established as of luminescence that, as a result of recombination processes either 301 stat -ce nt-to Tl**,areo a ra' are~ql! or anions adjace ex,cIted*.',.Th optIcal flash spect 7. . r1 ACCESSION NR: AT4020802 COM- (stimulated in. the F-band) and thermal glow of KI-TI, X-rayed at IOOK, are pared with Its fluorescence spectra excited In different absorption bands., Analo- gous data rylative to KBr-Pb phosphors lead to the conclusion that,Pb2+ centers assume the PI state as a result of the recombination processes. The author notet that, as a con:9quence of the laik of exporlmental data, It Is still Impossible to Indloate th predominant path of the excitation of.activator centers in alkali halide crystal's with ricombination luminescence. ."The author Is grateful to Okk for his help' In carrying out the &periment.11 Orig. arto.has: 2 figures@.. Z I K I -~'I ASTRONOM I I 'AN "(Institute of Phys~lcs,and.,-'- ASSOCIATION:.- INSTITUT.:Fl ESTSSR; Astronowt) - DATE ACQ: 07Apr -:F ;SUBMITTED: ENCL: 00 Ja~63 15 '002 oo~ SUB CODE*, PH REF SOV:. OTHER: % X.- A Card rz7 ACCESSION Nq: A P-50f 4516 6 7-4-, -1 Q -,AJKULXs. arl LiZ55FE. TZ;Festiva Seriva ftziChes1:.a'-a-' V.21~1' ro.l. -36LT~~- TOPTO TAGS: lumines;~ence, ionic crystal, recombination ILminescence, tiermolumines cence. radiation Pf 'r?c+ p ABSTRACr: The authors briefly review recent work in their laboratory .7oncerning the role of hole se f-trapping t-1 1 L pr. ~Mo r~ I I rid s L)ec I f i -iI I 7 W I 2-a ;)P~ nF i-tj f K -7 77, y 7 7,7 w J 32822-6q A-CCESSION NR: AP5004516 thermal release of s-ilf-trapped holes which, after m1grating to Ag", centers make it possible for reccabInation luminescence to occlir .3ven at 1(.,Yw ~em,)eranjres. An intense 'horm in ionic crvstal-". Fur, ier, invesr fgatllor rah-r. 4~6(-)CIATIQY- -ns+l f ! z 1 1 m a.i E.~, 5 5 R LI ILI f Ph s t cs arA As t ri)nn- tha PPry'! 00 SUB CCDF: SS . (?P -W 4 L 3281?-65 -1-M-e-) JD/J0 1 ACWS.SZON NR: AP500,1519 9/0048/65/029/001/0046/0049 SOURCE: Ali GSS?.. Iviestiya. Seriya fizieheskayn, v.29, no.1, 1965, 46-49 TOPIC TAGS: lunineszence, ionic crystal, alkali halid.~ cryatal, recombination lumi~ nescence, acti-vated crystal ABSTRAM The stimalation spectrum for optical flash in a KC1;T1 phosphor that had, been irradiated with x rays at 1000C was meaaured to quanttmt anorgles of about 4 eV. Four stimulation bands were found, of which two coincided with the F and K ab- sorption bands and the other two, at 1.85 and 3.3 eV, did not coincide with any kn-)w absorptimi ban.1s. A previously unknown stimulatet! absorption hand at 3.3 eV vai found, how.iver, In strongly 1rrqd1.it(,Ad KC':Ti but n:)t In KCI- In. Irradiation of the phosphor with 1.85 eV photuns led L~; decru~ase _t, the lrttens-,ty of tha 3 3 eV band and to increase of the absorption in the F bard. The temperature dependence Card 1/2 L 32317-65 -AMMSION UR: AMM1519 41 '7 nt4its t a &md t"no dm"rature'Ah e~-rejri'66~_ near 2 whero self-trapped boles are released. In this temperature region the absorption oi 3.3 EV photons decruased with i-ncreasing temperature. It is concluded that the ac- tivator centers Invc lved are electronic and It is hypothesized that they are the long gought at--!- 10 centers In the P, centers In KCI:AK. rtptlzal flash S t I M I I I A t PC, h r -1, 1 1 1 n ~ I J1 - . !, -v 1,1 ! , ~ h w .1 q t h r I 'j f th e I -I'/ e5 ga - I I Wa 3 F" f ~Unc g n ~i i gu re 9 . ASSOCIATIOM none SUBMITUD, OQ/--Jat~( 5 a-=L:. 00 L _~SUB CCDE.- ZZ SS OWP MR pop SOV. 006 OTHER: 002 L 2359-66 EWT(l)1EVrf (m)ID1.11(t)1EYIP(b) 1j'P(c) JD 780- MION NRs AT5021 VR/2613/64/000/028/0121/0127~ vq'or 1AUTHOM' Yaek, L V.; Meriloo, 16 A.; Savikhin, F. A. ..................... ..... ..................... Ir, I? TLBt Zino a 1fide p~~hdY~'w ith deep traps. u. ISOURCEt. AN Est:SSR. Inatitut fiziki i astronomii Trudy, no. 20, 1964- Isfilodovaniya po~lyuminestsentqii (Researchoo'n lumine scence)p ;21,-127 TOPIC TAGS:. zijac sulfide$ phosphor, emiesion.speebrum, thermolumineseence/ DVS.2 4 mono'6hromato I- SPMA.monochromatort FEU 10 photomultiplior .IABSTRACT: In order to investigate the deep trap thermoluminescence of zinc sulfide phosphors ,the authors synthesized ZnS-Bi specimens by mixing luminophosphor zinc- joulfide with 3PI'- BiG1 aotivator-and 4~lfo LiCl melt. The mixture was annealed for 2 3 lmir'i at, 11 50C in air.and.rapidly cooled.. The emission and.excitation spectra were Imec.'sured by using two monochromatorop and EL:hydrogen lamp was used for excitation The. thermoluminasc ,onIae curves showed two temperature peaks at T - 570K and T - 46;K0 The specimen:ali3o showed a single maximum red band at a wavelength of 610 nm. The hiE:h temperature thermoluminescence peaks are connected with thermal quenching lphemmena as shown in Fig# 1 -.on the Enclosure. The last intensity drop on these I cul'Ves occurs &mifhd 550K, It is shown that this rather unusual shift -to high .ACC_jqV&__AP70O4(17O_ SOURCE -CODE f-UR/004 8/66/03 6/009/1451/14 AlallOR: Kynembrop~Kh.Ps; OkkpM.F, ORG; Institute of Physics and Astronomy of the EstSSR Academy of Sciences (Inatitut fiziki i astronomii Akademii nauk EstSSR) TITLE: Optical and thermal electrons and photostimulated luminescence in KCl;T1 /Report, Fourteenth All-Union Conference on Luminescence (Crystal Phosphors) held at Riga, 16-23 Sept. 19657 SOURCE: AN SSSR. Izvestiya. Seriya fizichookaya, v. 30, no. 9, 1966, 1451-1463 TOPIC TAGS: luminescent crystal, potassium chloride, thallium, luminescence spectrum, recombination luminescence, temperature dependence, electron energy ABSTRACT: The authors have extended the investigations of two of them (~J.F.Okk and I.V.Yack, Izv. AN SSSR, Ser. Piz,, 299 46 (1965)) on photostimulated luminescence in ionic crystals to.include stimulation by radiation on the short wavolongth side of the F band. The luminescence excitation spectra of x-ray excited KCl!Tl crystals were recorded at 300 and 1060 X for stimulating photon energies from 1.6~to 4 eV. Four peaks were observed in the spectra: the F-band peak at 2.2 oV, thoIK-band peak at 2.75 eV, the T10-band peak at 3.3 eVt and a peak of unknown origin at 3.8 cV. The temperature dependenceuof the luminescence intensity for stimulation in the F, K, and Tl0bands were separately recorded for the temperature range from 80 to 300 0 K. The Crd 1/2 AP7004970 ACC NR. intensity of the F flush decreased monotonically with decreasing temperature; that of the K flash was almost temperature independent; and tho intensity of the Tlo flanh increased somewhat with decreasing temperature. The temperature independence of the X-flash intensity in in good accord with the findings of H. Kanzaki, T.Ninomiya, and K.Kido (J.Phys. Chem. Sol,, 22, 309 (1961)) on photostimulated conductivity. It is concluded from the present results and different findings of other authors that the K flash is recombination luminescence in 'which true optical (hot) electronp, rather than! thermal electrons, partIicipate. The reason for the increase of the Tlo-flash intensity with decreasing temperature is not known. The authors thank Ch.B.Lushchik for sug- gesting the topic auddiscussing the results* Orig, arte has: 2 formulas and 2 figures. SUB CODE: 20 SUBMIDATE: none ORIO.IREFt 002 OTH REF: 009 Card 2/2 U6SR/General Problerrm, of Pathology - Tumorr, T-5 Abs Jour Ref Zhur - Diol., No 4, 1958, 17452 Puthor : Kostyuk, V.I., Yayes, S.B. Inst : Title : Comparative Evaluation of TTeatment of Chronic Leukemias with Urethan, Edbichine~ Radioactive Phosphorus and X-Ray Irradiation. Orig Pub Probl. gematol. i perelivaniya krovi, 1957, 2, Nil 1, 33-35 Abstract babichine therapy given to 15 patients 14th chronic myelo- genous leukemia (CML) and to 8 with chronic lymphatic leukemia (CLL) has shown the efficacy of this method in cases of CML (remission iasting from 121 to 5 mos.) and its lack in cases of CLL. The value of this method was siSnificantly decreased at times by side effects and com- plications. The treatment with urethan of 10 patients with CML and two with CLL caused a clinical nrd hematolo- gicremission not exceeding 5 mos. The treatment with P32 Card 1/2 *NAM .pay MIM N4. M ' ~ r%RPU NMI 104 ro Allf~` ~ ~ i~w . _'USSR/General Problems of Pathology - Tumors. T-5 Abs Jour Ref Zhur - Biol., Tio 4, 1958, 1-7452 .(10 vith CNI and 5 with CLL) has demonstrated the inexpe- dience of this method, with the exception of those cases that had severe reactions to other methods. X-ray theran- py given to 11 patients with CML and 5 with CLL led, in the majority of cases, to 4.-13 mos. of remisuion. D.G.,,~ Y"S. S.B., Yourth conference of the Lvov Institute of Blood Transfusion. Probl. gemato i peral. krovi 3 no.1:60 Js-Y 158. (MIRA 11:3) (BLOOD-TRANSFUSION) A.W11 WHO N~KRASOV, ~.D.- SASSA, V.S.; YAFAYEV I V MAMIOFFEt R.M.; ZOLOTAF"A, O.G. Refrepatory concrete for vacuum-distillation furnaces. Ogneupory 28 no.1:26-30 163. tHIRA 16:1) 1, N&achno-issledovateliskiy institut betona izhelezobetona Akadamii stroitel'stva i arkhitektury SSSR'(for Nekrasov, Sassa). 2, Podollskiy zavod-tsvetnykh metallov (for Yafayev, Mamioffe, Zolotarevia). (Refractory concrete) (Electric furnaces) NAYKOV, A.S.; YAFAYIV, L.V. Improving and tailing's Of am other nonferrous metals* Tsvet.net. 27 no.4:45-49 Jl-Ag 154. (Aluminum) -1 F 1 \1 L ~ ~, A- ~ I I- ki, BAZIIZV.cXIY- TLktor Kamertovich; ISTRIN. Mikhail klakeandrovich; BARTASHIV, Ibor" Io)oaidovich; LYUHALINk. Soviya Livovna;,RXZNIK. Iosif Davydov-ich; OPAGIS, A.I., kandidat takhnicbeskikh nank. retsenzent: VISSARIONOV. B.G,inzhener, retsensent: jausainmKov, i.s., rstsenzmatw TRLIbMAN, retsenzeat; YAFAYAT retsenzeat; KOKAYEVA, 4.M....redaktor izdate.lstv*;')i Y., teknniche- skiy redaktor [Secondary nonferrous me.tals; a reference me,nuall Vtorichnys tavetn"" metal4; spra-,ochnik. Moskva. Gov.,nauahno-takhm. izd-vo lit-ry po 0 . I Imetallurgy of_cop Iper and lead] che 'rn'i I,*ts vetnoi metallurgii. Pt.3. Metallurgiia madi i svintma. _1957-344 p.- (KIBA 10:3 (Coppsr--~~Metallurgy) (Imad--Metallurgy). 1,606/001/002/04 Sp5 f e, IL Sol asovj G. tion furna Ilexx t' eva. o. distilla a TBOIRS I rLO-10 aT f or vac"M to COTIr"re toirl 26 0 from 1963, zill TITV&S no. remove i't pro- gneupory I d to . composition 0 ,,,aces-use iinF ite-periClaset -PERIODICI~Ll, iauction follol n9, of und Magn's motte as 001jeretc Of the I ined Ch the lini ,,,,y gro For of factory ree-Gra. strength T FIT I th ,ateri alloys a , diluted '111 -nd,coa ompressiorl inuM , fine- 0 eratureB -atel ,,,rates alum ter glass -silic, temP Via. f luo the ar,jed ormatio pose d' djum Of de' oC. destrur, ,a itIl So ti r -14500C is to at 1320 ea. W f,haracter ineset 11P ho compression filler. ref ractor~ shrink-ag' IUCO t Ihon heated. 50 Y'd6m int iiNoGitom-perature rec ter 3 of,the to 55000. af. 250 'softening PC es heated lap tructlo' n6th 2 r loadt. Chang 25~ des' ssion S.tre Thirty ~6t~ 6VP suffdTs mpre kg/ .- c-rote 2 by I-,00OG the 00 t '14500' or e COIA to tion a.tII of the Concrete d UP ied in % %t Ahe hete strong a 000 1 1 n )OOG 861'1 changes - . .I I to i2(. I . teglPere-ture f ive r, ar d' SMIZ631000100110021004 Refractory qonorete for... B1.17/B101 2 I is .200 - 256 kg/cm and the t h-fermal expansion' 0.6#- Operational tests with the new material at the Podollskiy zavod`ts,~etnykh metallov (Podol sk." Plant for Nonferrous Nletals~ !showed the followirjg.4~dvantages as compared with magnesite bricks and rammed liningi it to9k,40 days to "line and dry a vacuum diu~;illing,furnace. which is a 25% redqc~ion of the usual repair Work. After 20 months operation the concrete had,bocomwaosked with metal to a-depth o:t 20 - 40 mm.on~jq, whereas magnesite,lbricks and rammed lining -were complete.Ly soaked with m6tal after 12 - 13 months only. After 20 months the-compression strength was 100 - 120 kg/CM2.' Some places showed cracks of up to 6-5 mm,width and 50 60 mm, depth filled with metal, which is a disadvantage of the new material. Its high strength has the following causes; magnesite.and water glass surround the particles of porous chamotte with a chemically stable coat which.prevents impregnation of the.concrete by metal. The concrete is protected against penetration of the melt into deeper layers'b~ a* crust of new formations up to 8 mm thick% By the lining of vacuum distillation furnaces with the new concrete thus the Podolfsk.. Plant,for Nonfe~,rous Metals is'aaving of 13,000 rubles a. year. There are 4Jigures- Card 2/3 Ix .i--7 - - - ~ I - 11- -- ~ff' ~,TX offi~p~ f~M~~ I ?4' (7) AUTHORS: :Vinokurov, V. M., Zaripov,,'K. M., SOV/56-37-1-54/64 jgayevj~~i TITLE: The Fine Structure of the~?aramagnetio Resonance Spectrum of Tonkaya struktura spektra paramagnitnogo Natural Sapphire ( rezonansa yestesivennogo sapfira) PERIODICAL: Zhurnal eksperimentallnoy t teoreticheakoy fiziki, 1959, Vol 379 _Nrl, PP312-313 (USSR) APSTRACT: The authors investigated the paramagnetic resonance spectrum of some natural sapphire crystals at room temperature within the frequency range of 9600 - 9200 megacyoleat and tell of the re- sults obtained in the present "Letter to the Editor". The black- ish-blue color of the sap2hire was caused by F*3+- and T13+_ ions, which substituted the A13+ amorphously in corundum. Be- cause of the short spin-lattice relaxation timess the T13+_iona give no,effect~at room temperature, for which reason it is as- sumed that such an effect is due to the Fe3+-ions, which was confirmed by the present in 'vestigation. Korniyenko and Prokhorov Card 1/2 (Ref 2) already carried out an investigation of the fine struc- The Fine Structure of the Paramagnetic Resonance SOV/56-37-1-54/64 Spectrum of Natural Sapphire 3+ ture of the paramagnetic electron resonance spectrum of Fe ions in the Al 0 -lattice, and showed that the spectrum ob 2 3 served is possible as a reault of the here given Hamiltonian (1)o By basing upon these,and u3ing other results of reference the authors theoretically investigated the paramagnetic re- isonance spectrum of sapphire and numerically computed the con- stante of the Hamiltonian (I D a-F I and I a they found it to agree within the error limits with those of the Fe3+-ions (Ref.2) introduced artificially into Al 203' Also the splitting up of Fe3-resonanae lines found in reference 3 was likewise :found in the sapphire crys-,als. There are 2 figures and 2 Soviet references. ASSOCIATION: Kazanskiy gosudaretvenn3y universitet (Kazanf State University) SUBMITTED! March 28, 1959 Card 2/2 "s916 s/181/62/004/006/023/051 W00112 and Yablokov, Yu- 'AUTHORS: tafayev, N- R-P tic electron resonance of ;Ti in come silicate TITLEi :Paramagne S and phosphate glasse, 6, 1962, 1529 1534 PERIODICALt ~Fizika tverdogo telat v. 41 no and resonanoe,in silicate, phospbatet aramagnetic,eleotron TEXT: The p borate glassest to which were added K2 0, Na20, and U2 0 one after of another, Iwas investigated for 9330 and 450 tic/see at temperatures 00 and 770K. All samples contained 1 to 5 mole% Ti7O2- To obtain 3 3+ n the glasses, the latter were boiled with a smoking flame Ti, ions i To each charge were added carbonates gly reducing conditions. Under 3tron 5% by weight. of alkali metitis and carbon in quantities ofabout 0- ent Ti ions* -In contained no trival Conclusionss The borate glasses e Ti3+ ions 'are surrounded by und,:phosphate glasses, th - a distortions the silicate r storted in different degrees,' .., Th 8 of the nitrogen octahed a di The symmetries of lthe.sVrrounding Possess,a trigonal nature. card 1/2 S./181/62/004/006/023/051 Paramagnetic electron resonance ... B104/B112 3+ Ti- ions have*one and the samecharacter. However, the splitting of the orbital triplet in the phosphate glasses is larger than in the silicate glasses. In the iilicate glasses, the splitting is largest when the' ~Li- ions are roplaced b Na ions, and the Na ions by K ions. A y similar dependence of the.-splitting in phosphate glasses c-ould not be observed. If potassium,is replaced by lithium and sodium, the T13+ concentration in the glasses decreases. The results agree with the data of studies on absorption spectra in the visible region. There are I figure and 1 table. ASSOCIATIONt Leningradskiy gosudaretvennyy opticheskiy-institut im. S.-I. Vavilova (Leningrad State Optical Institute imeni 5. 1. Vavilov). Fiziko-tekhnicheskiy institut Kazanskiy filial All SSSR (Physicotechnical Institute of the Kazant Branch.AS USSR) SUBMITTEDt J'anuary 25, 1962 Card 2/2 5/056/62/043/005/054/058 B1 2 5/B,1 04 AUT11ORb: Gariflyanovt N. S., Yafayevp No R..~ 3+ TITLEt The paramagnetic electron resonance of Zr in glass bod.ies. PERIODICAL: Zhurnal eksperimentalinoy i teoreticheskoy fizik:6 V. 43, no. 501), 1962, 1978-1979 TEXT: Thefliethod of paramagnetic electron resonance (450 and 9320 mc/sec 3+ was used to investigate silicate glass bodies containing Zr (2 1ONa 20-70 Si02'lO;-,rO2) in mol-~) at 77 and 2950K. The narrow and symmetric line of the glass bodies investigated at 450 hic/sec and 77 0K has the spectroscopic splitting factor g - 1.69 + 0.01 and the width d H - 5 oe. The line width increases monotonically as the temperature rises fr& 77 to 2950K. at.which value a signal of the paramagnetic electron resonance* ceased to be observed. A broadand symmetric line'of the paramagnetic ,electron resonance Y, and SH - 126 + 6 oe ith geff ' 1.906 + 0.002 - -was observed at the'frequency 9320 Me/sec at 77 0K. it is assumed that in the glass specimens inve stigated the magnetic ion Zr 3+ has an octhahedral Card 1/3 S/056/62/043/005/054/058 The.,paramagnetic electron reitonance 1025/B104 3+(4d1, S=1/2) energy surrounding ftich is formed by(6 oxygen ions. The,Zr levels ate similar to the Ti 3+ ~3d16-1/2) levolu.: The fivefold degenerate orbital level of' these ions is split into a lower triplet and an upper doublet by the octahedral field of the Zr3t ions.' The width of the line having the ftvqtkency 9 - 450~ffic/sec of the paramagnetic electron resonance can be explained by the relaxation mechanism of Van Vleck. In addition to that mechanism the shape und width of the line having 9320 MC/sec are. due to the anisotropy of ~the g-factor and to vario.us strong distortions of the oxygen octahedron. The line'with 9320 hIc/sec arises -from the super- position of manf lines having various g-factors ~Lnd can be described by a spin-Hamiltonian of the form 'A H +; A i1 S + gzIPH'9z. The line of the (gxi X X gy I y y Z, 9-1 paramagnetic resonance of Zr., ,showed no hyperfine structure. ASSOCIATION. _Fiziko_tekhnic"skiy institut Kazanskogo filiala Akademii nauk USSR Uhysicotac~nical Institute of,the Kazan' Branch of the Academy of Sciences USSR) ..Card 2/3 The paramagnetic,.electron resonance ... 5/05.6/62/043/005/054/056 ~B125/B104 SUBMITTED: August 4, 1962 Card.3/3 L 18578-63 EWT(1)/EWP(q)/EWT(m)/BDS/EEC(b)-2 AFFTcASD/ESD-5/IJP(C) ACCESSION;NR: AP3001289 S/0181/63/005/006/1673/1677 AUTHORSi Yafayevt No Ro; Gariflyanovp No So; Y9blokov9 Yuo Vo iTITLE: E onance'of W. sup 5,+'ions- in glass _,Iectron paraffiagnetir. res SOURCEs Fizika tverdogo tela', v 5y no. 6p 19631'~1673-1677- TOPIC TAGS: elect:ron paramagnetic-resonance$ W,1, glass, silicate glassp phosphate glassp g-factor, hyperfine structure siii6a tetrahedron 'cons was studied 1'.tron par ama ABSTRAM he ele tavalent W _I gnetic resonance of pen in silicatevand pljosphate.glassesYat frequencies of 9320 and 440,megacycles ands at temperatures of-295 and 77K. At the low frequency and low temperature all bo the specimens displayed narrow symmetrical lines with a g-factor of a ut 1.6, shape of the lines being approximately gaussian. With gradual elevation of temperature the lines grew constantly broader and the position of maximu m absorntion did not change. At the high frequency and at 77Kt broad, almost symmetrical, lines were obtained in silicate glasses, but narrower and mo: asymmetrical lines~were found in phosphate glasses, The shapes of the lines and the values of the (1-factors did not change for silicate glasses on attaining room temperature. In the phosphate glasses, however$ the lines grew broader on f L 18 578-63 ACCESSION UR: AP3301289 the'rise in temperature, and the~asymmetry became less clearly defined. These results are explained on the'assumption that the W ions:are located within the silica tetrahedron,so- But more experimental work is needed,to determine the position preciselyo At the 440 megacycle frequency hyperfine structure was detected fiom thel.111183 isotope, In the glasses examined by the authors the signal of electron~magnetic resonance was observed only from pentavalent W9 which has,an electron spin of *. For other paramagnetic ions of W having a spin great than the lines of electron paramagnetic resona ce in glasses should be n blurred by,the fine structure&. Orig. art. hast 2 figures, I tablep and I equations ~Y ASSOCIATION: Gosudarstvenny*y opticheskiy:institut im. S. 1. Vaviloval Leningrad. (State )tical Institute) 63 r SUBMITTED: 04Feb6:3 DATE ACQ~ OIJul 005" SUB CODE: PH NO REF SOVt 004, OTHERt 2/2- Card. - YAPAYEV, R.Kh. Immunologic properties of Shigella, sonnel in experimental conditions; imminization of rabbits and passive Immunization of white mice. Zhur.mikrobioleepid9i immun. 'no#8:38-42 Ag 1,54, (ML'RA 7:9) 11 Is Voyanno-meditsinskoy akademii imeni Itrova. (VACO INS S AND VACCINATION, *dysentery vacc., immun. of rabbits & white mice) (DTSENMY AGILLART. Immunolog7, *vace.,-immm. of rabbits & white mice) YAFAYXVP R. Kh. immunological characteristics of Shigella sonnei in an erperiment on white mice. Zhur.mikrobiol.epld.i Immun. no-3:43-49 Mr '55. (MLRA 8:7) 1. 12 Icafedry apidemiologil s dizinfektaiyey (npch. prof. G.A. inameniskiy) Voyenno-meditsinakoy akademii imeni S.M.Kirova. (VACCINES AND VACCINATION, dysenterial vacc., i=un. properties of vace. prep. from Shigella 9onnei in white mice). (DYSIRITIW, BACILLARY, immunology. vacc. from Shigella sonnei. immun. properties in white mice) Y"AYET. R.rh 'IrnfItuma." edited bv N#I. Momkin, Reviewed bv R,Kh. lAfaev. Zhur.a~Lkrobiol.epid.i immun. 30 n0.71139-141 JI 159. (MIRA 12:11) (INYLUOU) (MOROMIN, N.I.) ---- - .- - -- -- ------- -- - --- 7f R.Kh., kand.moditainskikh nauk; SIROKOj A.L.9 prof* (deceasedlj._)~AMYE BELYAKOVY V.D. - YAPAYEN, R.Kh. "Essays on the theory.of,epidemiology" ty LI IElkin. Reviewed by V,D.Beil:lakov, R.Kh. lAfaev. Zhur.mi-krobiol.., opid. i i=mn. 32 '61 no.10 138.-11,0 0 (MIRA 14:10) ~MDFMI61DGY) (ELKIN, I.I.) YAFAYE-V ctic)n in -roi-jicnts. Zhur. Detec~,Jon of plaFU!~- 8XV1 ttaaVf)[r.!a lafe la". i imun. 40 no.Q-.93--.96 81063. (MIRA 17-5) mikrobiol.9 ep, iz Voyenn-mcditsinsllny ordepa Leidna a-kademli ~mew- S-l"a 'Kirov--. YAFAYEV, R.Kh. Differentiation between Pasteurelia pestis and P. pseudo- tuberculosis in rodenta. Zhur. mikrobiolo epida i immun. 40 no.5:23-26 My 163. (MIRA 17:6) 1. Iz Voyenno-meditsinskoy ordena Lenina akademii imeni Kirova. KUERYAVTSEV G.V., Kh. G - NOVITSKIY, V.Ye.;ZKAY~V,_~.I. Carbcxa agglomeration reaction (carbo-test) in the diagnosis of infectious nonspecific pol-yarthritis. Vop. revm. 3 no.33 63-67 R-SI'63 (MIRA 17-63) 1. Iz kliniki fakulitotskoy terapii (nachallnik prof. V.A. Beyyer) i kafedry epidemiologii. ( nachallnik - prof. I.I. Rogozih) Voyermo-meditsinskoy ordena Lenina akademi-.I imeni S.M.Kirova. L 34067-65 EEPAJ i pt-lo/Pad 1JP JD/Trd ACCESSIMi uR; AF5W5699 9/Gl29/65/0wj00z/oo27.joo2s 413 11,10 AUMOIXJ KaMMtt0vdjt YQ* G ; Heloruchev,, Le V,; YjfYLV~.', K!~leghova, V. D. TITLE; BrittlOnsill-a-lin permendur tyl3e alloys SOURCE.* Metallavedenlye L termichealcaya obrabotka metaLlov, not 2, 1.9651, 27-28 TOPIC TAGSo, Lrgj lloyp st-alt",~1GY9 alloy brittleness$ permendur alloy, alloy heat treabwnt alloy mechaa~eal groRerty ABSTRACT; Using perwendur-type alloys (Fe-Co alloys) a the authora attempted to establish the transition temperatures of the 6(-solid solution from a brittle to a nonbrittle sta~:e d.1ring cooling aLLd heating. The determination of these tempera- tures is impor:ant for establishing the optimal conditions for producLng bands of these alloy; by the coiling method. The experiments were carried out on band specimens 0.2 imn ttick rolled from billets of different melts, ne canpositi3nq of -~&Lch are given in d table, FVecimens of this baad 100 mm loag we-ce used to determine the temp-rature, upon heating to vhich britt:leness is eLimirwted after rapid cooling. To produce a brittle state these specimens were ieated in a vacuum furnace to 820-830C for 5 bra. and cooled at a rate of 50 deg/hr. The number of bends to fracture ras 5, compared to 121 after cold rolling but 5efoLe annealing. Card 1/2 L 3407-64 V The specimens were then heated in a salt bath to various temperatures held 5 min.# and rapidly otooled in cold salt water, then band tested. The results of e- a--: L 660C and-the:"tempdkiture,correspon the V ment-: 69 britti vests ~ d it heat hg - Va s - ding to devel-jpment of lbril:tleniess an cooLLng was 640C, The processes rmusiq; brittleness occurred rapidly but abrupt queadAng in water slowed them down* thus preserving a sufficient ductCIVof the alloy. Orig, art, has; 2 tables. ASSMMM Severoaizapadnyy zaachnyy polit:ekhnidheakiy institute Llorthwestern polytechnic correspondence institute); Laningradskiy.staleprokatnyy rimod P=ningra=eel riiLllag p at) SMMITTED: 00- ENCL: .00 SIM CODE: MH OMER; 003 1~~JRV qOV.- 000 YAFAYLVA, V..B.; VAILEYEV, A.3. Band in-t-erference iightfilters. Opt. i spek.tr. 17 no.1:102-112 il 164. (.',qFl 17:9) sk OW. ..!ACCESSiOM NR % AP'4042986 S/0051/64/017/001/0102/0112 I. !A :.,COAUTHORS: ,Yafa'yeva, V. B.; Valeyev, A.'.S. I ~:ITITLE:. Interference optical band filters '"SOURCE- Optika i spektroskopiya, v. 17, no. 1, 1964, 102-112 1; ..-ATOPIC TAGS: light interference, light filter, band spectrum, dielec-': P, tric coating,,optical transmission 'ABSTRACT: The,use of multilayered dielectric coatings for the con- of 6~tical filters that transmit a limited band of the ,~spectrum is considered'. The analysis is limited to narrow-band fil- ters wide up of alternating quarter-wave layers with large and small ;;refractive inAcest respectively, General equations are derived 'for the translr'41.ssion coefficient and bandwidth of such a filter by a method whick~ can be generalized to include~coatings made up of 'layers of morej than two,substances. Results of.electronic-computer ~Xard ACCESSION NRt KP4042986 RATS) V.G.; Un -G.M. Automatic press molding line at the Kiro7,plant. Lit. proizv. no.li:12-16 Ja 162. (MM 16:8) (FowWr'ies-Equipment and supplies) t, Zhur, In. 0 NEI b r;rrdena Lem'.nv. akadomil Imelil, YAFTMOV, P.I.,, kand. t&-hn. nauk .PTellmdziary calcalatim of the ac-~!,z-ar7 of the elem-a-rita !m a trianinplation serieso ~~bnr. nAuch. Md. KGRI i-io.IC814,6-150 161 m IRA I'l 8) S/194/61/000/012/071/097 D273/D30,1 AUTHORS:, Kanavalay, Ya. R. and Ya TITLE: Influence of ultrasonic oscillations on the toughness and plasticity of brass PERIODICAL: Referativnyy zhurnal, Avtomatika i radioelektronika, ~no. 12, x% 19611 16, abstract 12E91 (Vestsi IN BSSR, Ser. fiz.-tekhn. n. 1960, no. 4, 93-98) TEXT: The influence of ultrasound on the toughness and plasticity of 2-phase brass.tape A 53(L59) was studied. The experiments made use of a tube ultrasonic generator, together with a P114:2(G412) tube in the first cascade and 2 parallel switching valves PK74 (GK71) in the second. The output power of the generator was 300 volts. Launching of the ultrasound was done by a magnetostrictor -,h was joined a step concentrator. with a triple rod assembly to whit. The concentrator had a reinforcing flange at the nodal plane and was fixed to the vibrator by a especial nut of the same material, soldered to the assembly by brass solder. The plane of the joint Card 1/3 ~S/194/61/000/012/071/097 Influence of ultrasonic ... D273MG1 was polished. The fixing was carried out using a small tack. The vibrator was enclosed in a steel cylinder and fastened to it by a flange. Cooling the cylinder was effected by running water. The acoustic head was protected from the vibrations of the chopper by some sponge on -the upper part. At the lower end, the concentrator end was soldered to the studied sample (brass wire of diameter 1 mm). The amplitude of the oscillations was measured with a mi- croscope. After sounding and without unsoldering from the concen- trator, the.sample was discharged at room temperature, The zounding took place at 34 Kc/s at an amplitude of 0.0125 mm. Results of the experiment are given. The ultrasonic oscillations cause a simulta- neous decreat3e in toughness and plasticity of the brass; thus after 15 seconds of sounding the toughneca wan reduced by 9% and the re- lative elongation decreased by 50%i when sounding lastod more tfiari 15 seconds, the sample was destroyed. Ultrasound causes a lowering of all the characteristics of static toughness of brass and a de- crease in the work needed to cause destruction of the sample. Sounding in amorphous brass leaves the toughness and plasticity Card 2/3 m-wavA ps.~i t4 P44 WA,9MM kg- 'UMP S/194/61/000/012/071/097 Influence of ultrasonic D273/D301 practically unchanged..The suggestion is made that lowering the toughness of brass-as a consequence of sounding is connected with the transition of the metal in the stable state, and -the aimultan- eous decrease in plaiticity, and with the shattering of the crystal structure. The hypothesis is argued upon that the toughness of brass decreases as a consequence of the lowering of temperature with sounding time. 3 figures. 3 'Uables.-9 references, /'-Abstrac.- tor's note: Complete translation. 7 Card 3/3 SOV/81-59-5-15977 (S7 0 0 Translation from; Referativnyy zhurnal, Khimiya, 1959, Nr 5, P 327 (USSR) AUTHORS: Mikalinskiy, A.S.P Yakunchikov, V.N.,.Vallshchikov, V.I., .,Yafremkin., V.V,. TITLE: The'Refining of Amorphous Boron by Oxidation Burning In a "Fluidized Bed" PERIODICAL; Tr.~ Ural'skogo n.-i. khim. in-ta, 1957 (1958), Nr 5, pp 206-210 ABSTRAM The possibility is investigated of refining amorphous boron (AB) by.means.of oxidation burning in a fluidized bed (FB). Weighed portions (4 - 36 g)of AB, containing 85% of total B and 11% Mg, were placed in a chamotte crucible and air was blown in through the bottom of the crucible with a rate of 20 - 35 1/min, at a temperature of 20 to 4000C, and a burning time of 30 - 95 minutes. When.the reaction zone (RZ) of the furnace was heated up due to the hot air, a thermal gradient of 120 - 11100C was observed over Card 1/2 the porous bottomand in the. mass of the product, which brings S-ZF,-, --- - -- gcxmwwu~ - -- - -.--- -- - - - - - - -- - -. -_-- -D.; YUDMV, K.V.; )(U~ATOU, G.; YAGAFAROV, L.M. BAIAIWIN, A Cytolo&y of vagna4 smears during pregn.&*yj la-bor, anii puerper-iam. Akush. gin.'no. 1:42-44 Jan-Feb 1953, (GIML 24:2) 1. Stmdeuts. 2. Of the Department of Obstetrics and GYU0001097 (Head-- Prof. Be' Ta. Stavsk&Y&). Stavropol' medical Institute.