SCIENTIFIC ABSTRACT VLASENKO. N.A. - VLASENKO. N.A.

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SCIENTIFIC ABSTRACT
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AUUH00%, =1 LE - On the mechanism of excitcation of zlectro', lineacence in ZnS-,vn '-"5, "'7_4-3 MMIE: 0-otika i spek-trosko-pi-va, v. TOPIC SIM elpctrol-,ninesc.!nce excitation, zinc Sulfide or. poss'-IlLy, brea~_~jwn vo'ts.,:;e optical materialp thin exci ati ABSTRACT: The influence of the thi.-Imess of a sample on the probability of excita- tion, Of clectrolumIncsCence ir, 72S-1.,n Iii-r.-3 ~-az fnvestigated vith an aim at deter- =nlr.,:~ ur~~i`,~_ous4 the r_-xc'_ta-_icr,, =ecnanisiz. D, is shown tha-~ sucln ar. e:cperimer,~_ m;_,kes it -o unicuely w-etxner t-c- M Q, C L I S r e S -)0 i_. Z If - r- '_'o obtala sa=,,t:s of different thi-ki~,E~3_z vf-_- --,.-e t~-.-C-ste~; Me--`CC, f- one of t~.e aut'n'Drs (Vlasenko, 'with YU- A- Fopkavr O-pt. I &Pa.' r. V. 0. o.L., 7~- c films ranged in thickness fro= 0.04 to 2.0 ji, and the Fn concentration was 0-5 Lvt.%. The electrolumiaescence was excited with a 20W cps field to permit applica- C., L 43871-65 ACCESSION NR: Ap5oo6435 tion of a higher voltage then in the caZe et" a Qc f1cl-A. The avera-g_e brighlness Plele was determilred by the a..'! I E771 t' X C1 -:7. ca:,ca~-e:3 u,: n ~e el -L d S and a c ec ro e c f e I d r a-n I ~'~Dr erc st i r- t h e woz- 4 , a:-i d Y u -'pfai t i m; in discisslo s." axt. has. 4 fjCzu;-e5, 9 A S S OC DMON None Card 2/3 3 7 -LED Card 3/3 VLASENKO, N. A., Cand Phys-Math Sci -- (diss) "Photo- and electrolualin- escence of the sublimate-phosphor ZnS-VIn." Khar'kov, 1960. 16 pp; (Min- istry of Higher and Secondary Specialist Education Ukrainian SSR, Khar'- kov Order of Labor Red Banner State Univ im A. M. Gorlkiy); 150 copies; free; bibliography at end of text (10 entries); (KL, 25-60, 126) VIASINKO, N.A.; POPKOV, Yu..A. In-estigating the electroluminescence of a ZnS-Ma sublimate phosphor. Opt.1 spektr. 8 no.1:81-88 Ja 160. (MIRA 13:7) (luminescence) (Zinc (sulfide) 51-5-16/26 AUTHORS: Sinelinikov, K.D., Shklyarevskiy, I.N. and Vlasenko, N.A. TITLE: Double Refraction of Fluoride Films. (Dvoynoye Lucheprel- omleniye plenok fto:ridov) PERIODICAL: Optika i Spektrosko3)iyAtl957j Vol.2, Nr 5, pp.651-657 (USSR) ABSTRACT: Studies of films obtained by vacuum deposition show that they consist of microcrystallites separated by pores. Both the form and the orientation of these microcrystallites de- pend on the nature of the substance, thickness of the film and the conditions at deposition (speed of evaporation, pressure in the vacuum system, temperature and nature of the basel direction of the evaporated beran). It is known that a substance consisting of correctly oriented isotropic par- ticles of a refractive index 1Aj. and with the pores filled by a medium with a refractive inde-t ,&2 is anisotropic if at least one of the particle dimensions and the distances be- tween them is small compared with the wavelength of light. Double refraction produced i.n such circumstances is called the double refraction of form. The optical properties of such a body are determined by the refractive indices of its component parts and by the'relative volumes of these parts. Uard 1/3 Double refraction of fluoride films. 51-5-16/26 The absolute size of the particles, so long as it is smaller than light wavelength; is not important. For many substances the dimensions of microcrystallites and the distances be- tween them are considerably smaller than visible light wave- length, and therefore in that region one would expect anisotropy of the film. Double refraction was, in factf found by the authors in films of CaF2f BaF2, LiF, ,)'bS? V205 and other substances obtained by deposition on a :class base in vacuum.On introducing such a film between two crossed nicols one can observe fairly strong transmission in the field of vision. This transmission is at maxiTmi when the glass with film on it is so oriented that the dir- ection given by the cro3s section of the plane of the base with the plane of incidence of the evaporated molecular beam is at an angle of 450 to the direction of polarisation of the nicols. Wetting of the film by liquids of various refractive indices decreases the intensity of the transmitted light. The transmission becomes zero on wetting with a liquid whose refractive index is equal to the refractive index A of the bulk substance. Double refraction of t'Ide films may be also studied by an interferometric the fluor method. On a glass plate a semi-transparent silver layer is Card 2/3 deposited. On silver a calcium fluoride layer in a form of a Double refraction of fluoride films. 51-5-16/26 symmetrical hill is deposited which is then covered by another semitransparent silver layer. In monoch-romatic light a system of double rings is observed (Fig.2). The equal chromatic order lines are split in a similar way. (Fig-3). The results show that the fluoride layers possess biaxial double refraction and that the plane of the optical axes'coincides with the plane of incidence of the molecular beam. The orientation of the refractive index ellipsoid relative to the layer of the film depends on the angle of incidence of the molecular beams on to the base in the pro- cess of the deposition of the film. The magnitude of the double refraction also depends on this angle of incidence. The results are shown in Figs.6 - 10. There are 10 figures, and 11 references, of which 8 are Slavic. ASSOCIATION: Kharkov State University (Kharlkovskiy Gosudarstvennyy Universitet) SUBMITTED: October 15, 1956. AVAILABLE: Library of Congeebs Card 3/3 ACCESSION MR: AP4020933 AU211OR: Vlasenko, X#A* Lisitsag V. P. ead sulkids layers TITLE: Optical Constants of Photosensitive I SgURCEt Optika i spektroskoplya, v.16, n0.20 19640 ~97-303 TOPIC TAGS% optical constantp reflection, transmitlance, transaissiong absorptioa.,J absorption coofficient, Index of rofractiont lead sulfidet lead sulfide coating# i exciton absorption ABSTIUCT; In view of the potential value of PbS film and coatings, prepared by chemical procedures, for detection of Infrared radiation, there wore measured the :optical constants of such layers in the approximate range from 0.4 to 5.5 A. A fur-,.:, ther purpose of the work was to elucidate the nature of the long wavelength plateau, adjacent to the fundamental absorption edge. The thickness d of the layers were dV~ -.termined to within 1% by an interforometric method. The transmittance T was ed by mcaz)s of SP-4 spectrophotometer in the 0.4 to 1.2 1A Interval and by means ofit'' , IXS infrared apectrometer in the 1 to 5.5 1A range. The reflection coefficients R from the Inyor side and.R' from the gubstrato side were determined by oomWlson of*-.~ a/.:3 !ACCESSION MRS AP4"" ~:the reflection from the specimen with the reflection from a standard mirror with a 1known R; a UU-2 monochromator with an AgS photocell wasused for the visible region- measurements; an IKS-6 spectrophotorieter for the measurements in the infrared. The 11values of the absorption coefficient k and the index of refraction n were calculat-: Died on the basis of the measured values of T, R, R' and d by means of formulas ad- ~Jduced in the paper. The inferred values.are presented in the form of curves and a 11table for n, and compared with the corresponding constants for PbS single crystals,-,i 't iltaken from the literature. In the I to 4 p region the Index of refraction changes II'little, but remains consistently below the value for single crystals. In the wave-I 1:length region below 3 g the absorption spectrum of the films agrees with.'the abscrp~ I 1:tion spectrum of single crystals, but In the longer wavelength region exhibits ad- ditional absorption that depends to some extent on the size of the crystallites. This additional absorption is tentatively attributed to the presence in layer crya-: tals of a high concentration of structure defects, for this absorption tends to do-.- crease with increasing crystallite size. The nature of the absorption platoau in 'discussed and the absorption In this region is associated with an exciton mechan- ism. "'llie authors are sincerely grateful to V.Ye.Lashkarev for his interest In the work and discussion of the results, and to PoP.Pbgoretakiy and ZXoxhallmonova for! 2/3 .'Card, - - ----------- r"n ACCESSION NRs AP402W33 assistance in carrying out the measurements." Orig.art.han: 7 formulas 4 figures and 1 table. ASSOCIATION: none ~MUITTED:, 2SApr63 DATE ACQ: 02Apr64 EUM: 00 SUB CODE- PH NR REY 80V;. 005 OnMRZ008 --------------------- VLASENKO, N.A.; LISITSA, M.P. Optical constants of photosensitive films of lead sulfide. Opt. i spektr. 16 no.2t297-303 F 164. ()URA 17-4) Vj,,tSFjjj:0, if.A.; h,'JIMFENK0, V.F. FlectrolumInescence Of C6S 3ingle c-_;,3talB- On-_ i spektr. 16 no. 4:642-650 Ap 164. (iGRA 31-7:5) VLASENKO,, N.A.; MLU)SLAVSKIY, V.K.; SHKLYAREVSKII, I.M. On the appearance of Brewster band -and superposition bands. Opt.i spektr. 13 no.2:250-255 Ag 162. WIRA 15:11) (Spectrum analysis) VIASENKO, N.A. Effect of temperature on the electrolunLineseence of the ZnS-Yn phosphor sublimate, Opt. i spektr. 8 no-3:414-1+17 Mr(160. MIRA 14:5) (Zinc sulfide) (Luminescence) .~2 t4 d15_0 0 AUTHORs Vlasenko, N.A, TITLE: The Effect of Temperature Sublimated Phosphor ZnS-Mn PERIODICAL: Optika_i spektrosiopiyal PP 1+14 417 (USSR) 6 84 810511 008/03/028/038 E201/2191 on Electroluminescence of a 196o, Vol 81 Nr 3, ABSTRACT: The re orted temperature dependences of electrolumines- cence Mfs 1-7) are contradictory and, thereforeq the author undertook an investigation of the effect of temperature on the properties of electroluminescent phosphors with the purest possible chemical composition. I For this purpose the author prepared ZnS-Mn in sublimated form and studied its properties in the region 100 - 500 0K. Below room tem erature measurements were carried out in a special optiM cryostat. By using a heater in this cryostat the temperature in it could be raised to 70 OC. For measurements above room temperature the samples were Placed on a solid copper block in a special oven. Card Temperature was measured with a copper-constantan thermo- l/ 5 couple. A photomultiplier FEU-17 was used as a receiver. It was~connected to an amplifier and a galvanometer. 69842 S/051/60/008/03/028/038 9201/El9l The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn Electroluminescence was excited with sinusoidal voltages and hotoluminescence was excited with the mercury line at 395 my. The luminescence intensity above room temperature was measured under steady-state conditions and below room temperature it was measured while the sample was slowly heated (1.5 deg/min). The author recorded also the electroluminescence spectra at various temperatures. From these measurements he constructed the temperature dependence of the relative number of quanta emitted per unit time under given conditions of excitation. Such temperature dependences were constructed for photo- luminescence (curve 4 in Fig 1) and for electroluminescence excited with 200 kV/cm at 200 c/s (curve 2 in Fig 1) and 2000 cls (curve 3 in Fig 1). These curves show that up to about 200 OK the number of quanta emitted per unit time (NINO) in photo- and electroluminescence remains constant Card and at higher temperatures (up to about 250 OK) the value 2/5 of NINO falls slightly. Above 250 OX the photo- and electroluminescence curves diverge completely; the value 69842 s/o5i/WoOS/03/028/038 E201/E191 The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn of NINO for electroluminescence rises sharply with temperature, while NINO for photoluminescence falls rapidly. The rise of electroluminescence is accompanied by a rise of current through the sample. It was also found that an increase of temperature alters the intensities of photoluminescence and electroluminescence and bands are broadened (this broadening is proportional to VY at T>250 OK). The integral luminance of electro- luminescence (curve 5 in Fig 1) behaves gimilarly to the value of NINO for electroluminescence, i.e. it also rises strongly with temperature above 300 OK. The curve showing thermal de-excitation (1 in Fig 1) has one maximum in the region 130 OX which is due to excess atoms of zinc. NO thermal de-excitation (thermoluminescence) was observed if the sample was not subjected to ultraviolet excitation before heating. No resemblance was found between the thermoluminescence curve and the temperature dependence of Card electroluminescence (cf. curves 1, 2 and 3 in Fig 1). It 3/5 follows that the traps responsible for the 'Uhermo- luminescence peak at 130 OK do not play any role in the 69842 8/051/60/008/03/028/038 E201/R191 The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn process of electroluminescence between 100 and 500 OK. From the logarithmic dependence of the electrical conductivity on the reciprocal of the absolute temperature (curve 1 in Fig 2) the author deduced that there are two types of donor levels in the phosphor, whose depths are 0.11 and 0.38 eV. The observed temperature dependence of electroluminescence can bb explained on the basis of the collision mechanism of excitation and thermal ionization of donors which occurs more easily in the presence of a field. Lt low temperatures the conduction electron density is governed mainly by the shallow donor levels. In strong external fields (-./100 kV/cm) these levels are completely ionized even at low temperatures, i.e. the number of electrons which can be accelerated by the external field and can thus excite the activator centres by collisions is independent of temperature and consequently electro- Card luminescence is also independent of temperature. When 1+15 temperature rises so that ionization of deep donor levels becomes possible, the intensity of electroluminescence increases with temperature because of the increase in the 69842 S/051/60/008/03/028/038 E201/E191 The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn number of collisions which excite the activator centres (curve 2 in Fig 2). The author investigated also the frequency dependence of the electrolumineseent intensity at various temperatures (curves 1-If in Fig 3 show this dependence at 105, 293, 360 and 410 OK respectively). on increase of the frequency a noticeable rise of the electro- luminescent intensity occurs at higher temperatures (curves 2 and 3 in Fig 1) because the number of donor centres ionized in one half-period of the applied voltage decreases on increase of the field frequency. For the same reason the frequency dependence of the electroluminescent intensity is altered on increase of temperature (Fig 3); this occurs when the probability of ionization of deep donor levels, made easier by the applied field, rises with temperature. Card Acknowledgements are made to K.D. Sinellnikov, I.N. 515 Shklyarevskiy and V.K. Miloslavski for-thei advice. Tnere are -3-figures and 9 references, of which 3 are Soviet, 4 English, 1 French and 1 German. SUBMITTED: August 17, 1959 /51 -7 -4-12,/32 -'XTFOR: Vlasenko, TITLE Investig-ation. of the Fundamental ..bsorption "ipectrum of Zinc ~;ulphide P -, ?d OD ILL .Optika i spektrcak,)piya, 1959, Vol 7, !lr 4, ap 511-517 (UVOSR) ABST1,CT: The author investipted the fundamental absorption spectrum (in the soectrdl ragion 220-600 m1i) of zinc sulphide fi1xis proclucod by vacuum deposition at 5 x 10-5 mm Hg. Glass and quartz plates were used as the substrates'. Zinc sulphide was heated in vacuo before evioonttion In order to removo --ossible chloride and sulphate impurities. The rate of deposition of th.a film Yr-;Ls varied frow 200 to 2000 A/min. To avoid the effects if interference in the r~jglon of vioak ~,.bsorntion (A > 335 nji, the author used a ;tat'hod described earlier (Ref 13). In the region of strong absorption (,~ < 335 MILI the absorption coefficient was determined in the usual ruy by co-Lpiring transwission of two samples of different known thicknesses. Thase thicknesses xera such that trdnsinission did not -4xceed 10-20Y9, under these conditions the error due to disregard of interference vas saall (3-5;,~). xransmission was m6asurad by means of an SF-4 spectrophot=ater. The thickness of the filias was Card 1/4 determined interferometrically tc within 1-2~L The errors in C',* 07/51 -7 -4-12/32 Investigation of the Fundamental -'_bsorption Lpqctrj,~i of Zinc Ziulphide d atorinining the absorotion coefficient varied from 2 to 5~.. ~`trong absorption (_104CM-1) was o'buerved at wavalangthg below 365 m1i. A weak maxim= (_:Lo5cm-l) was observed at 325 m1i and with further dscreas6 of wavelangth absorption rose to 7 x 10 5 GM-1 (at 220 raji). An absorption "tal,l'! extended into the visible region (-500 m1i) -.vhgr,3 the absorption coefficient amounted to 100 cm-1. .111 this is shown in FIG 1. Heating (arinealing) of zinc sulphide films in vacuo or In bulphur vapour at tempo raturas a t)ove 40000 af fected strongly the loug-wavelongth (;k > 330 mji) part of absorption. .,bs orptioa of annealed f ilms at )k > 330 n4l was much siaaller than that of non-annealed films, approaching the values observed in absorption by massive ZnS crystals. Lnn(;aling produced also a small rise in absorption at 270-330 m1i (Fig 2). The author recorded also the absorption spectrc, of non-annealed (Fig 3) and annealed (Fig 4) ZnS films at -1550 (curves 1), +170 '(curves 2) and +240oC (curves 3). At A< 280 mIL the spectrtL viere found to be die-placed toviardi; longer wavelengths on increase of temoaruturs and the t%.i:)srature coefficient of displace.aent vas -2.2 x 10-4 OV/deg C. 71hen tau-e.7ature was lon,3red the absorption e fjaximum(325 mp)moved towards shorter vavelengths, became sharper and higher (Fig 4, curve 1). The tataoerature coefficient of dispiaceaent of t.-.9 long vavelen.-th absorption edge (at 340 mp) in annealed samples card 2/4 607/51-7-i-N/32 JnvestiGuticn of Via F~mdamant-l "'bsorptiou wpectrum of Zinc Zulphide war. -4.4 x 10-40V/dog C. YIg 5 shows the wavelength dopeOenca of the difference t;etwean the absorption coefficients of non-annealad and aruioaled films. This depondence has a uaxi;muia which rises ia value, becomea sharper and is displaced to-wards shorter wavel,3ngths on lowerin& of temperature. Absorption by zinc sulphide at~< 270 m1i is indopendent of the inethod of preparation of the sample and is due to transitions from the 'valence band to the conduction band . The exoeriin,3ntal data show th.tt the absorption coefficient in the region 230-i7O m~L Is proportional td (%~' - SG)l*S'where S is the energy of the absorbed photon and BEG Is the forbidden energy gap. Lt > 270 m1i this dependence of the absorption coefficient on (H EG) is no longer valid because of tne presence of the absorption band at 325 m11 which is not resolved at room temnerature. This band represents formation of the first excited state of the lattice by transition of electrons fron negative Ions to the nearest positive ions. The long-wavelength absoration observed in an-preparad films and absent in annealed films as weil as in large crystals, is due to lattice defects such as Card 6/4 SOV/51-7-4-12/32 Investigation of the Fundamental Absorption Spectrum of Zinc Sulphide dislocations or grain boundaries. It is possible that this absorption is related to localization of the excited state of the latzice at the lattice defects. Acknowledignents are made to K.D. Sinellnikov, I.N.'Shiclyarevskiy and V.K. 'u1ilos1avs1ciy for their advice. There are 6 figures, 1 table and 23 references, 5 of wrtich are Soviet, 13 English, I Dutch, 2 German and 2 translations from English into Russian. SUBLIP.MED: January 19, 1959 dard 4/4 -.. VLASE1rKO, N.A.; MILOSLAVSKIY, V.K.; SHKLYAR&VSKIY, I.N. Interference of luminescent radiation from sublimate phosphors. Opt. i Bpektr. 11 no.3:403-409 S 161. (MIRA 14:9) (Phosphors) (Luminescence) 68206 0 0 sov/58-59-5-11644 Translation from, Referativnyy Zhurnal Fizika, 1959, Nr 5, pp 246 - 247 (USSR) AUTHOR: Vlasenko. N.A. TITLE: New Method for Measuring the Absoprtion Coefficient of Substances in -111 in Yj 1 _ms TI/ PMIODICAL: Uch. zap. Kharlkovsk. un-t, 1958, Vol 98, Tr. Fiz. otd. fiz.-matem. fak., Vol ~,'_jTp 32-1 - 32-3 ABSTRACT- A method lacking the distortions due to erence phenomena is proposed for measuring the light absorption coefficient of a substance in thin films, For this purpose a light beam, which has been linearly polarized in the incidence plane, is aimed at the thin film of a substance under the Brewster angle. In this case the reflection co- efficient is equal to zero, and multiple reflections leading to the arousal of interference distortions do not take place. The absorption coefficient in this case is calculated from the formula: 1n I2/Il (t727cos r Card 1/2 where 11 and 12 are the intensities of the light passing through a 682o6 SOV/58-59-5-11644 New Method for Measuring the Absorption Coefficient of Substances in Thin Films plate having the thicknesses t1 and t and r is the Brewster angle. Using an SF-4 spectrophotometer, the author verifiXthe method experimentally on ZnS films 3,500 and 1,:100 A thick in the case of wavelengths ranging from 3,300 to 5,000 X. This method may find an application inihe investigation of the absorption of light by sublimated phosphors. K.S. Vulffson Card 2/62 68A4 2-4, 3 P 6 C-71151- -8 -1-14/40 OJTHORS Vlasonko, IT.A. and Po 1cov, YU.A. ,y TITLEs Investigation of El octrolumines cone a of the Sublimated US-Mn Phosphor ~,j PBRIODICAL: Optika I spektroskonlya, 1960, Vol 8, Nr 1, pp 81-88 (USSR) ABSTRA.CT: The authors used Vlasen1co's method (Ref 4) to prepare ZnS-Yn phosphors. Pure zinc sulphide and metallic manganese were evaporated In 10-,%n Hr' vacuum fran tantalum, boats onto a glass plate coated with tin dlox~b (the latter served as the transparent olectroJe). The ohosohor layers obtained in this vay here heat-treated at 500-5560C in order to diffuse the activator into ZnS and to produce good crystal structure in the films. On top of the phosphor layer aluminium -was deposited to servo as the second electrode. In some sam.olos a dielectric layer (for example polystyrene) ms deposited betwcten the phosphor and the aluminium electrode. ZnS-21n phosphors prepared in this way had orange luminescence when excited with electron beamc, X-rays, ultraviolet light or by means of alternating electric fiolds, The Pr9sent paper dbals with electroluminescence of sublim-ted ZnS-Mn films excited from an audio-frequency oscillator ZG-10. T'is authors Investigated Gard 1/4 the electrolmiinesconce spectrum, luminance -vaves, dependence of "he Integral luminance on the intensity and freqiency of the apnlio~ 6831h 507/51-6-1-14/4C investigation Of Slactroluminozicanca of the Subltiahted ZrZ-L:n Pho&phor field and certain electrical properties. The alactroltuilno5cance spectrum was a simple band of 0.20 eV half-width and a rtaximum at 2.13 OV (58Z mA), it was oractically Indeptindent of the intensity and frequency of the applied field, Luminance waves wore found to become itiore t_1,Yrnm0,ric -4th increase of tho applied field frqrVaency (Fig 1). The luminance -save paah rose by 2-.7 orders of maViitude with increase of the applied field intensity from 3.4 x 105 to 5.0 x 105 Vcm (Fig 3). The ratio of negatiTe to positive luminance peaks (peaks during negative and positive half-periods of the R~cplied field) was also strongly affoctod by the fiell, at 9 = 2 x 105,7 cm this ratio was 4.5 and it f all to below I at 3 = 5,6 x 105 Veja (Fig 2). The integral electroluminescence luminance depended on the Mn concentrition, at the ooti=vn concentration (0.003 g/g) it -was 0.02 stilb for samples 3 IL thick In a 4 x 105 V/cm ar,3 3000 c/s field. The Integral luminance rose by 6-8 orders of magnitude -when the field intensity increaced by a factor of 5-6 (Fir, 4)'~ this rise is Lauch greater than in -,ovider phos phors . At a ~,ivon field intensity the lLuainanca rcs a also with thickness of the ~ampples . The li=lnance was proportional to the apolled field frequency at lom frequencles 'out Card "./4 above 5000 cls it r-_nched saturation, the lwnlra~~cence was indepenllrt 66314 .-Ov I., Investir,ation of Electroltuirrioscence of the Sublipitige ZEO-Ifn ilhoi~hor of the frequency, orovided the resistance of the trAnsparent electrode was small coinp,,red with the Unpadanco of the slv!iple. At high applied field intensitlei the authors observed rion-linemjr effects in the current-voltage characteristics of the phoi;phor (Fig 5); deviations from Ohm's law -wore foijndl in fields -reater than 3 x 104 V/cm (Fig 6). When the upper electrole was In 51Q.,iediate contact with the phosphor (i.e. no intortiediate dielectric layer) slight rectification was observed at that electroie. At low temperatures (115-2501K) the functions log 0-= f(I/T), m1hore 6 is the electrical conductivity and T is the abaolute temperature, are straight lines Ahoso slopes depend somenhat on the intensity of the applied field (Fig 7). Above iSOOK (1/T = 0.004) a s)isrper rise of %he electricai corductivity with temperature was observed. The results obtained show -that electrolttminescence of subliiiiated US-16n DhosphrrG is intrinsic luminescence and it Is produced throughout the samnia. The authors found alzo shallow (--0.1 eV) donor levels in ZnS-4fn layers. The ionization energy of these donors depends on the applied field in agraerent with Frenkel's theory of Card 3/4 thermal ionization aid9d by electric fields. AcknwsledUiionta are q1 1 68314 Invostigation of Blectrol~=inwconce of the Sublirmted ZnS-Mll ph SOV-51-8-1-14/40 os; phor made to K.D. 3inellnikov who suggestorl the subject ard to 1.1!. Shklyarevsk.iy and V.1, Miloalavskiy for their advice. Th-3r3 aro 9 figures and 11 references, 3 of -wniQh are Soviet, b. English, I translation from Englizh into Russian and I Dat--h .~ V SMUTTED- June 15, 195~1 Gard 4/4 AUTHORS: Vlasenko, N.A., TITLE: On the role of of luminescence 42192 S/051/62/013/004/oo6/023 E039/E491 Pavlova, Ye.N. additional impurities in the formation centres in the phosphor ZnS-Cu PERIODlCAL: Optika i spektroskoplya, v-13,.no.4, 1962, 550-553 TEXT: Samples of ZnS with various levels of impurities were prepared by evaporation in vacuo as described in an earlier paper. In order to facilitate diffusion and recrystallization, the condensed samples were heated to 550*C while still under vacuum. It is shown that the absence of luminescence in the case of ZnS-Cu without an additional co-activator is associated with the deposition of the copper in the form of colloidal particles. The effect of two types of additionaljmjSurity is studied: 1) impurities which compensate the surplus charge arising from the substitution of Zn2* by ions of Cu+ (e.g. Cl); 2) impurities which have the same valency as the ions in the 'basic lattice (e.g. Mn). The addition of small quantities of 1-in to ZnS-Cu stimulates the green Cu luminescence together with the orange Mn luminescence. The most intense green band is obtained for a Mn concentration of 10-5 g/g eq. and the Card 1/2 5/051/62/013/004/000'/023 On the role of additional E039/E491 intensity of both bands falls sharply when the Cu concentration io-3 g/g eq. A comparison of the green band phosphor ZnS-Cu,,Nin and ZnS-Cu,CI with the blue band phosphor ZnS-ikg,N,',n and ZnS-AS,Cl shows that the additional impurity does not form a constituent part of the lui-.iinescence centres but only assists in the introduction of the activator creating the centres. There are 3 figures. SUBIMITTED; August 15, 1961 Card 2/2 VLASEHKO N.A -- Influence of the temperature on the photoluminescence of ZnS--)ta phosphor sublimate. Opt. i spektr. 8 no.6;W-854 Je 160* (MIRA 13:8) (Zinc sulfide) (Imineseenco) SHKLYAR37SKIY, I.N.; jVIASI2IED_t ~I.A.-_MIWSUVSKIY. V.K.; NOSULXM, N.A. Value and sign of the phase difference Azgp-SS. Opt. i spektr. 9 no.5:640-643 N 160. (MIRA 13: 11) (Reflection (optics)) (Metals--Optical properties) Ll. 12s-0 0 A1JTHORt Vlasenko, N.k i TITLE: Th~eEfffeet 'oemperature Sublimated Phosphor ZnS-Mn N PERIODICAL: Optika i spektrosiopiya, PP 1~14-417 (USSR) 69842 8/051/60/008/03/028/038 B201/9191 I on Electroluminescence of a 1960, Vol 8, Nr 3, ABSTRACT: The reported temperature dependences of electrolumines- cence (Refs 1-7) are contradictory and, therefore, the author undertook an investigation of the effect of temperature on the properties of electroluminescerit phosphors with the purest possible chemical composition. For this purpose the author prepared ZnS-Mn in sublimated form and studied its properties in the region 100 - 500 0K. Below room tem erature measurements were carried out in a special opticai cryostat. By using a heater in this -emperature in it could be raised to 70 OC. cryostat the Ak, For measurements above room temperature the samples were placed on a solid copper block in a special oven. Card Temperature was measured with a copper-constantan thermo- 115 couple. A photomultiplier FEU-17 was used as a receiver. It was connected to an amplifier and a galvanometer. 69842 3/051/60/008/03/028/038 9201/El9l The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn Electroluminescence was excited with sinusoidal voltages and hotoluminescence was excited with the mercury line at 395 mp. The luminescence intensity above room temperature was measured under steady-state conditions and below room temperature it was measured while the sample was slowly heated (1.5 deg/min). The author recorded also the electroluminescence spectra at various temperatures. From these measurements he constructed the temperature dependence of the relative number of quanta emitted per unit time under given conditions of excitation. Such temperature dependences were constructed for photo- luminescence (curve 4 in Fig 1) and for electroluminescence excited with 200 kV/cm at 200 c/s (curve 2 in Fig 1) and 2000 c/s (curve 3 in Fig 1). These curves show that up to about 200 OK the number of quanta emitted per unit time (NINO) in photo- and electroluminescence remains constant Card and at higher temperatures (up to about 250 OK) the value 2/5 of NINO falls slightly. Above 250 OK the photo- and electroluminescence curves diverge completelyi the value 69842 B/051/60/008/03/028/038 E201/B191 The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn of NINO for electrolumineseence rises sharply with temperature, while NINO for photoluminescence falls rapidly. The rise of electroluminescence is accompanied by a rise of current through the sample. It was also found that an increase of temperature alters the intensities of photoluminescence and electroluminescence and bands are broadened (this broadening is proportional to VY at T > 250 OK) . The integral luminance of electro- luminescence (curve 5 in Fig 1) behaves similarly to the value of NINO for electroluminescence, i.e. it also rises strongly with temperature above 300 OK. The curve showing thermal de-excitation (1 in Fig 1) has one maximum in the region 130 OK which is due to excess atoms of zinc. No thermal de-GYCitation (thermoluminescence) was observed If the sample was not subjected to ultraviolet excitation before heating. No resemblance was found between the thermoluminescence curve and the temperature dependence of Card electroluminescence (cf. curves 1, 2 and 3 in Fig 1). It 3/5 follows that the traps responsible for the thermo- luminescence peak at 130 OK do not play any role in the 69842 8/051/60/008/03/028/038 E20l/Rl9l The Effect of Temperature on Electroluminescence of a Sublimated Phosphor ZnS-Mn rocess of electroluminescence between 100 and 500 OK. ; rom the logarithmic dependence of the electrical conductivity on the reciprocal of the absolute temperature (curve 1 in Fig 2) the author deduced that there are two types of donor levels in the phosphor, whose depths are 0.11 and 0.38 eV. The observed temperature dependence of electroluminescence can be explained on the basis of the collision mechanism of excitation and thermal ionization of donors which occurs more easily in the presence of a field. At low temperatures the conduction electron density is governed mainly by the shallow donor levels. In strong external fields (--alOO kV/cm) these levels are completely ionized even at low temperatures, I.e. the number of electrons which can be accelerated by the external field and can thus excite the activator centres by collisions is independent of temperature and consequently electro- Card luminescence is also independent of temperature. When V5 temperature rises so that ionization of deep donor levels becomes possible~ the intensity of electroluminescence increases with temperature because of the increase in the The Effect of Temperature on Phosphor ZnS-Mn 69842 s/o5l/60/008/03/028/038 E201/El9l Electroluminescence of a Sublimated number of collisions which excite the activator centres (curve 2 in Fig 2). The author investigated also the frequency dependence of the electroluminescent intensity at various temperatures (curves 1-L~ in Fig 3 show this dependence at 105' 293, 360 and 41o OK respectively). On increase of the frequency a noticeable rise of the electro- luminescent intensity occurs at higher temperatures (curves 2 and 3 in Fig 1) because the number of donor centres ionized in one half-period of the applied voltage decreases on increase of the field frequency. For the same reason the frequency dependence of the electroluminescent intensity is altered on increase of temperature (Fig 3); this occurs when the probability of ionization of deep donor levels, made easier by the applied field, rises with temperature. Card Acknowledgements are made to K.D. Sinellnikov, I.N. 515 Shklyarevskiy and V.K. Miloslavski fo-r-their advice. There are j7igures and 9 references2 of which 3 are Soviet, 4 English, 1 French and 1 German. SUBMITTED: August 17, 1959 39869 S/051/62/013/002/003/014 E032/F,514 - AUTHORS. Vlasenko,_N.A'., Miloslavskiy,V.K.-and Shklyarevskiy,I.N. TITLE: On the origin of Brewster and super-position, frin-cres PERIODICAL: Optika i spektroskopiya, V-13, no-2, 1962, 250-255 TEXT: The conditions necessary for the appearance of Brewster fringes in white light and super-position fringes in monochromatic- light are discussed in the general case with allowance for multiple reflections within each plate. The two types of fringes are carefully defined and the differences between them are brought out. In each case an explicit relation is given for the ntensity distribution. In the case of Brewster fringes, the orresponding intensity-distribution formula is used to establish a condition for the continuity of the achromatic fringe. In fact the achromatic fringe is continUous (visual observation) provided t 61,) > 2.5, where t is the plate thickness bLnd AVIJ is the wave number difference corresponding to the spectral range employed. The final section is concerned with the analysis of Brewster fringes which are produced when a two-beam interferometer, e.&. the Jamin interferometer, is crossed with a silvered plane- Card 1/2 On the origin of Brewster and ... S/051/62/013/002/008/014 E032/E514 parallel plate. Analysis of the corresponding intensity distribution shows the presence of several achromatic fringes and it is suggested that these fringes may be useful in speeding up the adjustment of two-beam interferometers. They may also be useful in rapid-order counting an&the measurement of the thickness of plane-parallel layers. There are 5 figures. SUBMITTEDt July 17, 19.61 ,Card 2/2 SM55 S/O 51/60/00?3/0 6/016/(M 4 Z #JP0 2201/1691 AUTEIORs Vlasenico. N40 TITIZ s The Iff act of Temperature on Photolumines cone* of the SublLuated Phos phor US -Nn PHRIODIG&Ls Optilca I spektroskopiya, 1960, Vol 8, Nr 6, pp 847-854 (USSR) ABSTUM The effect of temperature on the absorption (Fig 1) and luminescence spectra (Figs 2, 3) of the sublimated phosphor ZnS-Mn was investigated between 100 and 5500K and the temperature dependence of the relative quantum yield of luminescence us& obtained for samples with amounts of MA from 0.05 to 5% (Figs 4, 5). The results obtained more used to deduce the mathaniam of excitation of luminescence contras, the nature of luminescent and radiationleas transitions and kinetics of concentration quenching. Acknowledgments are made to K.D. Sinalinikov, I.M. Shklyarovskiy &ad V.K. Miloslavskriy for their advice. There are 5 figures and 18 references, 4 of vhich are Soviet, 8 English, 2 Dutch, 1 German, 2 mix4d (Dutch, German Card 1/1 aW Inglish) and 1 translation f rem English into Russian. SUM TT2D s October 19, 1959 SIliEr '11TKOV, K.D, Af. V.LASMOj N.~.. C-)mmlox Interfetance lipht tillt4rx wlt)~, izprovad :hara!torIsti~i, A:, ()-t. i aDektr. WIJU. 16:6) (Light filterB) (Interference (Ltght)) f 4- ! -q .~ ~ I 9~, ~,, ~ - - SIMMINIEDY, K.,D.; SMMYAREVSKOY, I.N.; YLASRAM, No v *,~?P"O-.~ Optical characteristics of complez interference light filters. Zhur.tekh. fiz. 26 mo.1:96-101 J& 156. (KLRA 9:6) (Light filters) VLASENKO, N.A.; FAVLOVA, Ye.N. Role of additives in the formation of luminescence centers In Znp6W phosphor. Opt. I spektr. 13 no.4:55pr-553 0 162. (MIRA 16:3) (Phosphors) ACC NRt AP7004961 SOURCE CODE: UR/0048/66/030/009/1427/1429 AMOR: Vloseako.N.A.;.Vitrikhovskiy,N.I.; Denisova,Z.L.; Pavlenko,V,F. ORG: none TITLE: On the nature of the luminescence centers in cadmium sulfide /ifoport,Fourteenth All-Union Conference on Luminescence (Crystal Phosphors) hold at Riga, 16-23 Septo 19657 SOURCE: AN SSSR. Izvestiya* Boriya fizicheskaya, v. 30, no. 9, 1966, 1427-1429 TOPIC TAGS: luminescence, cadmium sulfidev luminescence center, annealing, lattice defect ABSTRACT: The authors investigated the Influence of hent treatment In vacuum and in 1 sulfur vapor, cadmium vapor, oxygen, and hydrogen sulfido nnd the presence of Group I and Group III doopants on the red, orange, and green luminescence of cadmium, sulfide crystals and films in order to determine the nature of tho corronponding lurAnescence centers. The crystals were grown from the gaseous phase by sublimation and synthesis,: and the polycrystallino films were doponited in vacuum. Tho green luminoficenco ceriWea were found to be thermally labile and It was not possible to produce them by any heat treatment. These centers were more stable in a sulfur atmosphere than in the other atmospheres; it is concluded that they are associated with local sulfur excesses in the lattice arising during crystal growth. Group III doponts Increased the intensity 1/2 ACC NRz AP7004961 of the green luminescence and Group I dopants reduced it. The activation energy for thermal quenching of the green lumineacence was found to he ).14 !~ 0.01 eV, Jn ment with the difference between the width of the forbidden 4and and the onergy of the emitted photons. The orange luminescence was enhanced bf anneal in an oxygen atmosphere and depressed by anneal in other atmospheres. Fr)m this and the findings of D.A.Kulp (Phys. Rev., 125, 1865 (1962)) concerning the aVects of electron bom- bardment it is tentatively concluded that oxygen favors the .'lormation of interstitial cationic defects in the form of singly charged interstitial oadmium ions, which are responsible for the orange luminescenco. The red luminescenfjo was found to be en- hanced by heating In vacuum or in a cadmium atmosphere and 1r, the presence of Group I dopants; from these results and from other data in the literature it is concluded that the red luminescence is due to recombination of an electron with a hole trapped at-a sulfur vacancy, Orig6 arte has: I figure* SUB OUDE: 20 SUBM DATEr none ORIG, RjW: 000 OrH RUI 008 Card 2/2 ACC NRs AP7004974 SOURCE CODE: UR/0048/66/030/009/1463/1466 AMORI. oqS*A& DRG: none TITLE: Polarization effects in electrolumincacent ZnS;Kn filmi /Report, Fourteenth All-Union Conference on Luminescence (Crystnl Phoaphors) hold iit Riga, 16-23 Sept. 19657 SOURCE: AN SSSR. Izvostiya. Sorlyn fizichookaya, v.30, no.9, :.966, 1483-146G TOPIC TAGS: electroluminescence, zinc sulfide, manganese, electric polarization /- (,M1A10 PIIC?IV- ABSTRACT: The authors have investigated polarization effects I.n 0.25 micron thick lilms o9 a ZnS:Mn clactroluminophor between Sn02 and Al olactroden. The matallic electrode was separated from the luminophor by a 100-150 A thick layer of SiO. it was found that when a steady voltage is applied to such a cell it becomes polarized and the luminescence intensity rapidly drops by a factor of about 100. The polarized condition persisted for several hours when the cell was short c4rcuited, but the cell could be restored to the unpolarized condition by irradiation with photons having energies between 1.6 and 3 eVe When to a polarized cell there was applied a voltage of the same sign as the polarizing voltage there resulted only weak luminescence, but when a voltage of the opposite sign was applied, the initial luminescence flash was brighter then that trom an unpolarized cell. The luminescence intensity (both of the initial flash and in the steady state) was higher when the aluxinum electrode was the Card 1/2 ACC NRt AP7004974 anode when it was the cathode, and the duration of the polarizLng and depolarizing processes also depended somewhat on the polarity. The presenc-i of moisture reduced the polarization and accelerated the depolarizing process. It is hypothesized that the polarization is due to accumulation of free carriers at tha luminophor-electrode boundary as a result of entrapment of electrons in deep traps. The ratio of the polarization field to the polarizing field was evaluated as the ratio V2 - Vl)/V21 where Vl is the initial polarizing voltage and V2 is the voltage of the same sign thati must be applied to the polarized cell to produce an initial flash of the same intensity as the flash produced by application of V, to the unpolarized,call. This ratio was found to be-~about 0.35 and to vary little with the magnitude tind sign of the polar- izing voltage. The polarization effects provide a simple explanation for a number of experimental facts,.including: 1) the low brightness achieved by application of successive pulses of the same sign; 2) the strong influence ol a test pulse of oppo- site sign on the brightness produced by the following ten to twenty exciting pulses; 3) the differences in the slopes of the voltage-brightness characteristics for different types of excitation; and 4) the transition phenomena that occur when suc- cessive pulses of alternating sign are applied to the unexcited phosphor. Orig. art. has: .1 formulae 2 figures and I table4 SUB CODE: 20 SUBM DATZ: none ORIG, REP: 002, OTH REF; 001 Card 2/2 ACC NRI AP7004975 SOURCE CODE: UR/0048/66/030/009/1467/1469 AUTHOR: Vlasenko,X.A.; 7-frnI0,S,A, ORG: none TITLE: Investigation of the characteristics of low-voltage electroluminescent ZnS:Ya films under pulse excitation /Report, Fourteenth All-Union Conference on Luminescence (Crystal Phosphors) held at Riga,, 16-23 Sept. 19657 SOURCE: AN SSSR. Izvestiya. Sariya fizicheskaya, v. 30, no.9, 1966, 1467-1469 TOPIC T4',GS:, clectroluminescence, zinc sulfide, manganese, time constant, pulse rate, I 0 ic brightaesG AMTRACT: The authors have investigated the pulsed characteristics of thin electro- luminescent ZnSMa films produced by the two-stage technique of N.A.Vlasenko and Yu.A.Popkov (Optika i spektroskopiya, 8. 81 (1960)) in order to assess the technical possibilities of those low-voltage electroluminophors. It woo tound that on appli- cation of a 0.1 to 1.0 millisec square pulse the brightness would rise exponentially with a time constant of about 0.3 millisec for the duration of the pulse and would then decay exponentially with a time constant of 1.2 millisec. Experiments with an equivalent circuit showed that these time constants are much longer than the RC con- stants of the cell. It is hypothesized that the long time constants are associated with the long lifetime of the excited state of the tin2+ ions, with carrier entrapment processes, and with polarization effects. It was not possible to achieve a brightness exceeding 5 to 10 nit with excitation by pulses of the same sign, but brightnesses several orders of magnitude higher could be obtained by excitation with pulses of Card 1/2 AUF- NK: AP7UU4975 alternating sign. The brightness increased linearly with the pulse repetition rate for rates betwoen 20 and 1000 Hz and was proportional to the 8-th to 10-th power of the pulse height for brightnosses below 20 nit. The dependence of the brightness on ihe pulse duration for fixed height and repetition rate was more complex. It was found that brightnesses of 10 to 20 nit could be achieved with 10 to 50 microsec pulses of heights below 30 V and repetition rates from7100 to 300 Hz. It is concluded that the investigated electroluminophors are suitable for use in sigtL indicators, matrix indicator scroens, and other devices that do not require a duty factor higher than 0,001. Orig. art. hau: 3 figurea. SUB CODE: 20 SUBM DATE: none ORIG. REF: 002 OTH REF: 001 Card 2/2 ANTONOV, A.Ye.-, VLASENKO, N.B. Distribution of phosphates and silica in the southern Baltic in 1957-1959. Trudy BaltNIRO no.7:70-77 161. (MIRA 15:2) (Baltic Sea--Phosphates) (Baltic Sea--Silica) ------ "JA i"Yll' 0 none T:T i'*_7-' lnve:;tij-'ation of c"naracteriztics. of low-voltage clectro-luminescent Zr.S-'4n__ f` 'Uadcr pulzcd L:xCi'La;;i0i-' SOU7CE: ZhurnLLI prikladnoy spektros?opii, V. 5, no. 1, 1966, .67-72 120:1170 TAGS: zinc sulfide optic =,ateriul, c1cctroluminescence, light excitution, optic A;-.).'3'I:';L,CT :1ra:-,.much, a-z in most practical a-pplic.~tio.-.G f -Ims are u~3ea unaer pul:;ud exc-itation conditionL;, the authors; the brightnesz waves, ti:"'C constant of 1"Lz;-.ireocercc buildup and attunuation, and the dependence of the avera-c bribr-htnezs of low-voltage ZnS-14a A1111;-,is on the duration of the voltage pulse, t1ne frequency, amplitude, and polarity in the case of rectangular pulses. The ZnS.Mn fil:m was produced by a method described earlier (Opt. i zpcktr. v. 8, 81, 1960) an -i electrode, nlaccd betweer. a transparent electrode (Sn02 or In2O3 ) and an aluninuL he ~a-z-ter be4n- separated from the ZnS.,""n by an insulatin- SiO layer. '~.'he tests were mad to IG-3 cn2 on unit cells ranging in area from 0.5 A flash of brightness was ob- served when a unipolar pulse was first applied to the sample, or when the polarity of Cord 1/2 UDC: 535-376 i. o906-67 ACC MR: AP6027901 the pulses was reversed. T.-Ie averaf~e bri,-ntness of the electroizz--inescence was found to increaze appreciably on going from unipoiar exciting pulse,-, to alternat ting pulses. I The use oil alternating pulses made it possible to obtain an average brightness not 0 X .lo-wer than 15 -- 20 nit at a pulse amplitude 21 30 V, pulse duration z 20 psec, and a ition frequency > 200 cps. An equivalent circuit of the elect ro-IlLmine scent eel ,repet Ili ;is used to explain the kinetics of the clectro-lumineseence and the values of" the coulvalent-circuit parameters are evaluated. The electro-luminescence buildup ti,-,.c 1was approximately 4 X 10-4 Sec, and the decay 'time was 1.2 x 10-3 sec. The values were much larger than the tire constant of the equivalent circuit, from which it is deduced that t1ric growth time of 'the elect ro-luminescence in the films is connected with the dur"-tion of the excited state of -the Mn2+ ion, and not with the capture of the carriers. It iz; concluded zhat -the phtosphlor ZnS.r~n can be successfully used in many electro- ;l-,zr.incsccnt devices which do not require very large oT 'A-duty cycles (in different ;caaracter-diizplay natrix screens etc.). The authora than% V. 1. Kislyuk and 1. Yu. .~_- r "nelp with the experiment and Doctor of Phyro-rcal X hematical Sciences 14. Shabli, ~o P. Lisitsa for interest in the work and a discussion of the results. Orig. art. has: _-an uu~iez d 4 formulas SUB CODE; 20/ SUBMI DATE: 18Feb65/ OBIG Mr. 002/ OTH REP: 001 Car-d 2/2 PALKINJ A.P.j XOROTKIKH, G.G.;_V1ASENKO,_N.B. . Interaction in the systems: GdC12 - ZnC12 - Al and CdCl - Tlbl - A.I. Zhur. neorg. khim. 5 ub.3:637-641 Mr 160. (AIFU 14:6) (Cadmium chloride) (Zinc chloride) (Aluminum) (Thallium chloride) VLABINKO, Hikolay Dmitriyevich; FISHMAN, Yakov Hatanovich; BMMLYANSXIY, V.A., - redaktor [Mechanization of threshing operations] Mekhanizatoiia rabot na tokakh. Moskva, Goo, lzd-vo selkhoz. lit-ry, 1956. 91 p. (mLRA 9:11) (Threshing) VTASINO, N.D.. inzh.; RALITSSV, Yu.I., inth. Pneumatic belt-type grain cleaning macbins. Trakt.1 sell- khosmanh. no.10:31-32 0 '59. (MIRk 13:2) 1. Vaerouslyokiy nauchno-loolodovatel'okiy inRtitut inalchani- sateii i elektrifikateii sellskogo khozyaystys. (Grain--Cleaning) VLASENKO, N. D. 4650. VLASMEO, N. D. i FISHCFYM, Ya. N. 14ekhanizatslya poslevborochnoy obrabotki zerna v borisovskom zernosovkchoze Omskoy Oblasti. Mf., Izd.--,ro 11-va ssoulkhozov SSSR, 1954, 44s. s. 111. (54-58o68) p 633-1:631.36(57-14) SO: Letopis' Zhrunall nykt Statey, Vol. 7, 1949 VLAM~99,14-1,(-KiZev) Raising the qualifications of public health s7stem organizers without discontinuance of work. Vrach. delo no.6:133-134 Je 162. (PUBLIC IMTH AEMINISTRATION) STRUYEV, I.A.;,VLASENKO, N.I. (Kiyev) Toward better training for public health organizers. Vrach. delo 4:M-125 Ap 162. (PUBLIC 1EALT11 ADMINISTRATION) (MI--~A 151:5) VLASKSKO, N.K.; PANCHENKO, A.A. In reference to A.K.4sklila article "Causes of priming of boiler water in the Shpanov Sugar Factory." Sakh.prom-31 no.9:51-52 S '57. (MIRA 10:12) 1. Ukrgiprosakhar. (Feed water) VIASE Role of herds in zooprophylaxis of malaria in cattle drives in the Baraba Lowland. Ked.paraz. i peraz. bol. 26 no.3:336-339 Ky-Je '57. (Knu 10:11) 1. 1z kafedry obahchey biologii Novosibirskogo meditsinakogo instituts. (MALARIA. prevention and control, in cattle breading (Rus)) (CATTIM, prev. of malaria in cattle breeding (Rus)) VIASMO. N.14. the development of eado- and exop~llic stan"rds of behavior of gono-active Anopheles maculipennio messeae females in the Baraba lowland. Ned.paraz. i parez.bol. 26 no.4.,436-439 Jl-Ag '57. (MIRA 10:11) 1. Iz kafedry obahchey biologii Novosibirskogo meditain8kogo institute (dir. institute - prof. G.D.Salesekiy, zav. kafedroy X.M.Vlaaenko). (MMqUITONS, Anopheles maculipeanis, role of behavior of females in eradication (Rua)) VL /9 S jAlH, e tv USSR Zooparasitology. M1teB and Insects. G-4 Carriers of Disease Agents. Abs jour: Ref Zhur-Biol., No 20, 1958, 911M. Author Vlasenko N M. even Inst Title The Part Played by Cattle Herds In Malarial Hygi- -he Pasturage System of Livestock Rais- enics Where t ing is Used in the Barabinsk Lowlands. Orig Pub: Med. parazitol. I parazitarn. bolezni, 11057, 26, No 3, 336-339. Abstract: In the Barabin3k lowlands two methods of raising driven livestock are used. In the first method, the dairy herds graze about the steppes far from the field camps. These field camps are separated and at a considerable distance from one another; the crevis are usually located near a source of Card 1/3 USSR / Zooparasituology. Mites and Insects. G-4 Carriers of Disease Agents. Abs Jour; Ref Zhur-Biol., No 20, 1958, 91106. Abstract: water supply, which becomes subsequently the breed- ing place for Anepheles larvae. Hungry gonoactive females assemble in the habitations of the workers where they attack human beings during the early evening and in the daytime, a long time befo-re the herd is driven back home and the period of maximum mosquito activity is reached. After the herd is driven back for milking, the mosquitoes mainly at- tack the animals. Under these conditions the con- tact between human beings and mosquitoes becomes more frequent. The precipitation reaction shows that mosquitoes with human blood in their stomachs total about 21.5 to 31.3% and only in rare instances 7.5 to 9.8%. According to the second method the dairy herds, heifers and milk-fed calves graze on Card 2/3 45 USSR / Zooparasitology. Mites and Insects. G-4 Carriers of Disease Agents. Abs Jour: Ref Zhur-Biol., No 20, 1958, 911o6. Abstract: adjacent pastures; the heifers are kept at night in covered sheds near the field camps. Th-e dairy herd grazes day and night on the pasture at a dis- tance of 3 to 5 kilometers from the field camp. The working crew quarters are located flush on the grounds of the general field camp. A greatly atten- uated contact between humans and the Anopheles is then brought about by the mosquitoes being diverted by the cattle herds kept at night in the stalls. Under these conditions mosquitoes having human blood in their stomachs total about .3 to .6%. The ef- fect of the correct organization of pastureage on the incidence of malaria is analyzed. -- N. Ya. Markovich. Card 3/3 V L SF Al""-)j ~V ~ I-r" -USSR / Zooparasitology. Mites and Insects. G-4 Carriers of Disease Agents. Abs Jour: Ref Zhur-Biol., No 20, 1958, 91093 Author :-~L~-,e Inst : Not given. Title : The Degree of Development of Endophilic and Exophilic Behavior in Gonoactive Females of Anopheles Maculi- pennis Messeae in the Barabinsk Lowlands. . Orig Pub: Med. parazitol i parazitarn. bolezni, 1957, 26, No 4J, 434-439 ores. Eng.) Abstract: The degree of exophilia in Anopheles maculipennis masseae mosquitoes as well as the possibility of their contact with human beings were studied in localities where the livestock is driven out ~Ylto pastures, in those sections of the Barabinsk 11-W- lands which are well supplied with water and are Card 1/.4 Z' ! :SSR / Zooparasitology. Mites and Insects. G-4 Carriers of Disease Agents. Abs Jour; Ref Zhur-Biol., No 20, 1958, 91093 Abstract: thinly populated. The mosquito hunt was carried out on roads used by herds of cattle, on pasture lands and near the sites where the herds are sta- tioned in the evening and at night, usually situ- ated far from villages and at a distance of 1/2 to 2-1/2 kilometers from f--,eld stands. The main mass of mosquitoes collects during the daytime in places occupied by cattle and in the dwellings of workers. Only very few females were found In natural shelters nedr the herds. No Anopheles larvae were discovered In reservoirs near the cattle pastures. An analy- sis of the stomach contents of mosquitoes caught in barns, cattle sheds, huts and houses disclosed that the main mass of mosquitoes feeds on farm ani- mals (68.36 to 99.5%), but that they use buildings Card 2/'4 42 USSR / Zooparasitology. Mites and Insects. G-4 Carriers of Disease Agents. Abs Jour: Ref Zhur-Biol., No 20, 1958, 91093 Abstract: as their shelters. A small exophilic population of Anopheles m. messeae was found in 1950 close to those places where cattle were stationed in holes near tree roots and in brushwood. The main mass of mosquitoes consisted of females with fresh blood. The average age of the exophilic population was younger than in females of the endophilic popu- lation. In the first instance older females amoun- ted to 5%, while in the second instance they amoun- ted to 21%, which is a proof that the natural shelters are less favorable and that the mortality of mosquitoes living in them Is considerably higher. The temperature in natural shelters is lower than In buildings, especially at night when the temper- CD ature difference reaches 5 to 70C. The author also Card 3/4 ,USSR / Zooparasitology. Mites and Insects. Carriers of Disease Agents. I.sbs Jour: Ref Zhur-Blol., No 20, 1958, 91093 P,-4 Abstract: noted an absence of exophilic population In other sections of the Barabinok lowlands. -- N. Ya. Markovich Card 4/4 43 Tlasenl:6, ZT. IlThs-, ecolo-ical, re~iuircments for th,~ -n(-! 7--rophylr!xis cl of mnlaria i,n tho Barnba of lly,-Iene, ll-'Iicrobiolo~-_-7, and .~Crnd lef-ld Sci Uf-"F)P. ree octo- 10- i cAd X,oricow, 1.956 (DisserVition 'or th-.~ de,- in Ilio Scionnes lrni7.hnaya leto7)is I No. 25, 1956. Moscow VLASMIKO, N.S. arkhitektor .-Y Choosing a model and locating dwellinj~s for construction workers at a district thermal electric station. Trudy Ural.politekh.inst. no.109:48-52 161. (MIRA 14:7) (Electric power plants) (Dwellings) YLASINKO.N.Y. I -- . - - , , -, - -.- - -,; '' . Longitudinal and torsional vibrations in drill-pipe columns. Nauch. sap. LMA Vviv.fil. AR URSR no.1:61-76 '53. (MLRA 8:11) (Oil well drilling) ol"142, G-jt~snt. T, P. Wln V. I., 04e;!i6evsky, Y. T., ang A i, j,:?tf) fcr fu cc VLASENKO, Nikolay-Vasillyevich, kand.tekhn.nauk, dotsent Study of the performance of a slide contactor in transformer oil. Izv.vya.ucheb.zav.; elektromekh. 5 no.10:2195-U97 162. (MIRA 15:11) 1. Kafedra, elektricheskikh mashin LIvovskogo politekhnicheskogo instituta. (Electric motors.. Direct current) 112-3-5743 Translation from: Referativnyy Zhurnal, Elelrtrotekhnika, 1957,' Nr 3, P.99 (USSR) AUTHOR: Vlasenko, N.V. TITLE: Theoretical Principles in the Experimental Determination of Heat Transfer -Coefficients in an Electric Machine (Teoreticheskiye osnovy k eksperiments,11nomy opredeleniyu koeffitsiyentov teploperedachi v usloviyakh elektricheskoy mashiny) ' PE~ODICAL: Nauch. zap. Llvovsk. politekhn. in-ta, 1955, N_r 34, pp. 161-175. ABSTRACT; The problem of experimental determination of average heat transfer coefficients in existing machines is stated, and a technique for computIng overheating is proposed. The heat cycle Is Bet up, and.thevalues of specific thermal resistance are determlYied depending upon the machine geometry, heat emission coefficient and type of ventilation (axial or radial). The resulting specific thermal resistance is determined; the application of the results obtained are considered for thermal design of machines with a nonsymmetrical distribution of the-heat flows along the axis of machines and for long machines Card 1/2 112-3-5743 Theoretical Principles in the Experimental Determination (Cont.) with sectionalized ventilation. The application of the pro- posed technique to e.,cperimental determination of the heat emission coefficient in a machine is discussed. A.I.M. ASSOCIATION: Llvov Polytechnical Institute (Llvovsk. politekhn. in-t) Card 2/2 BARDACHEVSKIY, V,T,; VELICHM, Yu,T,; VLASEIMO, N.V.; GUBENKO, T.P.; DRYAXMDV, A.I.; KARANIZYICVI'r.139*',---'KiintSHIN, L.V.; MAKSIMOTICH, N.G.; SOKDLIZIITSKIT, G.Z, M,G, Liukov, Izv. vyse uchabs zave; energ. no.5:127 MY 158. (Liukov, Mikhail Grigorlevich, 1915-1958) (MIRA,41,1:8) L 38 476-56, -EVT ( I ACC NRz AR6017225 SOURCE CODE: UR/0058/65/000/012/BO11/BOll AUTHOR: Vlasenk2,,,P?. V., ,Panteleyeva, N. L.; Senik, V. I. TITLE: The potential on the axis of a conducting disk with a concentric hole, excluding the edge effect SOURCE: Ref. zh. Fizika, Abs. 12B125 REF SOURCE: Tr. po teorii polya, vyp. 1, 1964, 55-58 TOPIC TAGS: disk, edge effect, charge distribution, electric potential, charge density ABSTRACT: The problem under consideration is the potential of the axis f a conductLrig disk with a concentric hole excluding the function of the electric-char~! distributirZ'I' on its surface when the surface density of the electrical charge is assumed to be constant. (Based on authors' abstract] AM] SUB CODE: 20/ SUBM DATE: none Card L AR~017226 SOURCE COnE- UR/0058/65/000/012/BO11/BOll ATj7HOR: Vlasenko, N. V.; Senik, V. 1. TITLE: The potential on the axis of a conducting disk with a concentric hole, taking the edge effect into account SOURCE: REf. zh. Fizika, Abs. 12B126' REF SOURCE: Tr. po teorii polya, vyp. 1, 1964, 59-63 TOPIC TAG3. conducting disk *edge effect, electric potential ABSTRACT: The problem under consideration is the otentia.1 on the axis of a conductng! disk with a concentric hole in consideration of the edge effect. [Based an authors abstract] SUB CODE: 20/ SUBM DATE: none i Card -i /i VIASMO, 0.1e, dots. ; W.LZ - rtbain errore that students make in their mathematia at-idles and methods for their correction. Nauk. zap. ChIDPI 11049-357 157. (Mathematics-Study and teaching) (MIU 11:5) VLAS---Jflio~ 0.1.; LEV:-'HENK-0, G.V.; M~REK, B.A.; TEODOIZOVI(~H, O.K. bafec t3 of ce ra -,,lIi --, 41al I ungs t,,~n-nj Cke Ir c ~a,7 ? . t. I ',' 5 r,,o.6,:1)4--lrj4 j'6 165, ~M-LRA 18:8) 1. institut nrobl!amrra'kc-rialovL-,rfe-iiya AN 1fIcr&")Ft. -66 W(k /DIT W /711.1p W bomp ( 0IJP(C) IJD/~~JJG ZC NRj AP5013252 .63OURrE CON,: UR/0226/65/000/005/0058/oo62 AUTHOR: Teodorovich, 0. K.; Levchenko, G. V.; Xlaseriko, 0. L. 1.115' ORG: Institute of Problems of the Science of Materials, AN UkrSSR (Institut problem materiZovedeniya AN UkxSSR) TITLE: Effect of silicon in the molding and properties of tungste -nickel-coppe contacts IVI -~ -7 SOURCE: Poroshkovaya, metallurgiya, no. 5, 1965, 58-62 TOPIC TAGS: silicon containing alloy, tungsten containing alloy, copper containing alloy, nickel containing alloy, electric conductivity, tensile strength, specific resistance, powder metal molding ABSTRACT: It was found that small additions of silicon in copper (up to 1%) improve the process of impregnating tungsten-nickel-copper contacts, and eliminate waste due to pores and cavities caused by the reducing effect of silicon and increase in the fluidity of copper. The electric conductivity, hardness, contact resistance, and tensile strength of tungsten-nickel-copper compositions change slightly on introducing small additions of silicon into copper. This is best done by im- pregnating tungsten-nickel-copper blanks in previously silicated graphite molds. Orig. art. has: 6 figures. [Based on author's abstract.) Powder Metallur SUB CODE: 3-1/ SUBM DATE: 20Mar6h/ ORIG REF: 003/ Card 1/1 V,-g GRUSHKO. Y~.Me; DIKU71, P.P.; SHABAD, L.H.; RUXAVISHNIKOVA, T.I.; ZAK, L.M.; VIASH11KO, O.M. Comparative study of air contanination b a cancerogenic substance (3.4-benzopyrene) in Irkutsk andAngarok [with summary in Znglish]. Gig. i san. 23 no.4:7-10 Ap 1,58. (MIRA 11:6) 1. rz kafedry obahchey giglyarq Irkutskogo meditainakogo institute, l,qboratorii eksperimentallnoy onkologii Instituts onkologgii AMN SSSH, Irkutskoy oblastnoy sanitarno-epidemiologicheekoy stant8ii t Irkutskogo energeticheskogo upravleniya. (AIR POLLUTION, determ. by 3,4 benzopyrone in sampling of snow flakes (Rue)) (BENZOPYRIOM. determ. 3.4 benzopyrene in sampling of snow flakes in air pollution determ. (Rue)) VLASBKO,, Petr Ignatlyevich; TEPLYAKOV~ G.V.., red.; IT40,S)IIEVSKAYA, -.. - - - A.A... tekhn. red. [Lofty initiative] Krylatyi pochin. Donetsk, Donetskoe knizhnoe izd-vo, 1963. 49 p. (MIRA 16-12) 1. Sekretart Chistyakovskogo gorodskogo komiteta Kommunisti- cheskoy partii Ukrainy (for Vlasenko). (Donets Basin--Coal mines and mining-Technological innova- tions) 1; 15647-63 S/0286/63i'000/002/0026/0027 ACCESSION HR: AP3000840 AUTHOR:, Li~_~Lnshuk, H. D. Wasenko. P4 I.; ~'pi:arenko, 0. K.; TkzAchen~*,, V. A.; Prosvftiii, A7. H. TIIU: Installation for klectron-be Weldin of tubes idth tube panel$. ~a we Class H 05b; 21h, 30 sub 10, Noo 152714~1" SOURCE: Byul. isobreteniy itovarnykh tnakov, no. 2, 1963.~ 26-27 TOPIC TAGS: elekctron-beam wlding, automatic program coixtrol, welding ABSTMM.- Installation for alectron-bean welding of pLpe with pipe panels, containLng an electron-beam welding gun with magnetic deflection system, a .rotating table for fastening and rotating the work piece during the welding process, and an automatic control system for sequential operation of individual tiechanisms; its distinguishing feature is that in order to automate the welding process, tho table is provided with two land screws with a drive system for moving the article in two mutually-perpendicular directions when It comes time L 2.5647-63 ACCESSION NEt: AP3000840 -t* weld the next tube, and the con trol system contains a pro gram unit with rela elements for automatic control in accordance with a program recorded an a punched tape or some other program carrier. OrLg. art. bas: I figure (s*G Enclosure 1). Abstractor's note: complete translationj ASSOCIATION: none SUBKTMD-. 11 Sept 61 DATE ACQ: 28 MAV.6S RNCL: 01 SUB CODE: MD, ML NO REP SOT: 000 000 Card tar_ I :K - -11,~!~~~---~---L-ll~Vlt~)nu~-~lali-lz"_"i-_~e2 MEEMIM C-7 r7 DATMMKO, M., doteent. iepolnyayushchiy obyazannost' taveduyushchego; OUXENKO, P.K., kandidat meditsinskikh nauk; vusmo. Pa.. airektor. Pathogenic therapy of trigeminal neuralgia. Stomatologiia no-3:30-36 '53. (MLRL 6:7) 1. Kafedra khirurgichaskoy stomatologii Miarlkovokogo maditainskogo stomato- logicheskogo instituta (for Datsenko and Guzenko). 2. Kharlkovskly medi- tainakiy stomatologicheskiy inatitut (for Vlanenko). (Trigeminal nerve) (Neuralp gia) VLASEUKO, P. V. "The variability of diphtheroids in association with ataphylocci.11 Min Higher Education Ukrainian SSR. KharIkov Order of Laboi Red Banner State U imeni A. M. GorIkiy. Khar8kovs 1956. (Dissertation for the Degree of Candidate in Biological Soiences). SO: Knizhnaya letopis'. No. 16, 1956 VIA ~iEIIKO. ?. V. 5*1 1 ?sthogenic role ,)A' diphtheroids. Vrach.4alo no.9:951-953 157. (HLRA 10., 9) 1. -Kaferlre biol-o 'git t kafedra mikrobtolVgit Khvr'kovsk-3R:o maditqinskogo inotituta ( X, C. Ti I j~ j R i CGN N I C ) A -4 .1d"bes Pathogenic for Man F USSR / microbiology. tv' and Animals. Aacteria, Root Bacterlas Abs Jour! Ref Zhur-'Biol L) 1958.. No 17.. 76809. Author : Vlasenko P V Inst : No~v Title - New Pathogenic Varieties of Diphtheriods. Orig Pub: Vrachebn. delo.. 19571 No 10, 1043-1046. Abstract: The changeability of 2-2 avirulent strains of diphtheroids (D) in association with 6 virulent strains of Staphylococcus albus and St, aureus were Investigated In vitro, Of the 22 strains, 13 be- longed to Corynebacte Ium hoffmani, and 9 were not identified with any of the species of D des- cribed. Associative cultivation of D and staphylo- coccl (S) were conducted BPM with serum with pH 7.6 for 1-1/2-2 months at 37C without subculturing. Card 1/3 NIt lel"'~ ;'?, --j--cr USSR / Microbiology, Microbes Pathogenic for Man F-4 and Animals. Bacteria. Root Bacteria. Abs Jour: Ref Zhur-gfol.,, 1958, No 17., 76609. Abstract! As a result of combined growth with different strains of S, the strains C. hoffmani almost did not change, but all remaining strains of D sharply changed morphologically, tinctorially and cultur- ally in the direction of Identity with the diph- theria rods. Pigmentation of columns of D changed according to the pigmentation of the columns of S of the associate (induction). The antIgenic struc- ture of D, by changing, attained antigenic proper- ties corrinon with S. The changes of D appeared In a determined order., but the degree of stability depended on the length of the association. After the combined growth with S for 30-45 days, the pro- perties attained by D were Inherited in many gen- erations kept in a pure culture for 8-10 months. Card Z/3 5Z I USSR / Ficroblology, Microbes Pathogenic for Man F-4 and Animals. Bacteria, Root Bacteria. Abs Jour- Ref Zhur-Blolik 19580 No 17, 76809. Abstracts With intracutaneous introduction in rabbits, 11 of the 12 changed D's caused local suppurative inflammation,, -- M. Ya, Boyarskaya. Card 3/3 Y", inzh., reteenzent; PILIPE14KO, SOLOKKA, Yakov Pedorovich; V YU.P.) inzh.) red.; GORNOSTAYPOLISKAYA, M.S., tekhn. red. (Mantffacture of bimetallic parts] Froizvodstvo dvukb--Ioinykh detalei. Moskva., Mashgiz, 1962. 116 p. (MIRA 15:4) (Metalwork) (Laminated metals) ,.I -'~' '-I t tt ptsesofsUas of wwd IvbmAWq P, Nautk..rkk. Kowleowbii P, Afti'd 41 . A A P-19,411Y Zoo 00 '00 '00 00 of, .,90 Alm *lfdtl.4,FGKAL UT(RAT1,91 CLA$11FICATION I L WOO K d it 9 It It 4still a.- 's, (too AA I S It W-6 bi 1) ii 00 KA OL e 0 0 0 0 0 0 0 0 0 0 0 0 f 0 0 a 0 S/739/60/001/000/015/015 EO2O/E185 ~'AUTHORS: V_1ase_nko_.___S_P_._ Candidate of Medical Sciences; KheXfets, Yu.B., Junior Scientistj and Chil-Akopyan, L.A., -TITLEt The effect of ionizing radiation'upon.oxygen consumption and certain aspects of carbohydrAte metabolism .SOURCE: Akademiya nauk Armyanskoy SSR. Sektor radiobiologii. Voprosy radiobiologii. v.i, ig6o, igi-196 TEXT: An investigation was made of 'the e,ffects of insulin and X-4rradiation given singly or in combination',--upon the oxygen .consumption, blood-sugar level and glyqogen content 'of the .1eucocytes in rats. Exposure to 600 r was followed by a fall in all these quantities, which attained minimum values after 1.,5-3 h. A return to normal levels occurred after 24,hours. In animals* .given a single dose of insulin w 'ithout irradiation the blood sugar and oxygen consumption fell similarly, but a.rise in glycogen :,con,tent of the leucocytes occurred after hours and persisted .1 :for 24 hours. The combined action of insulin and irradiation did iCard 1/2