SCIENTIFIC ABSTRACT BAYTUGANTI, Y.G. - BAYUKOV, Y.D.

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MUM$ M.Kh,; SXCRNWCVl M.V.; MUSABLYANTSp R.N. LAYTY~I 1; Y~9.G! Safety problems in using oasing lines. Trudy V.NIITB no.11%3-12 159, (KERA 15:5) (Oil we2ls--Wpwnt and aupplies) RANVELY", Ghoice of efficient and safe devign of pipe alevutors for under- ground oil well repairs. Trudy VIIIITB no.13:21-29 l6c. (m.1RA 14:12) (Oil wella-Equipment and supplies) Y~~, Te.G., inzh.; XABANDV, V.I., insh.; TJMEDVA, A.$., inzh.; RAVIRA BIRTULISON, Th.A., inzh, - Attachmente to pumplag jacks. Bezop.truda v prom. 4 no.4:24-25 Ap- l6o. (Oil welIA-3quipment and suyplies) (KIM 13:9) KANMTAN, B.Ge, insk.;, BAYTUGANTI, Ts.G., inzh. Tabe elevators for underground repalring of vells. Bezop.truda v prom. 4 no.10:24-25 0 160. (KWA 13 -- U) 1. Vessoyusnyy nouchno-isoledovatellskiy inatitut po tekhnike bezopmenosti I neftpaoy promphlenuosti, Ba3cu. (oil wells-3kuipment and ewplies) BAITU izL* MANVELYAN. B.G.., Anzho; GIMTIj>tG. a Fastemng VA~Joe Of, an sia-dria suboaface pmping vnito Besop.tru& v yvan, 6 no,,7,.24 JI 162, Wpa 25:7) 1. VasisoyuxWy nauchno-Usladovatellskiy neftyanoy inatitut po tekbnike basopamoati* (oi:L won pmpiv) ASHiF,BREV, Tu)rmebay Ashimbayevichp nauchn. sotr.; #MTULESHEV) Turinmbek BVt i -y~eshev chp nauchn. sotr.; KOVAIXNKO sotr.; SHIM, F.S., kand. okon. naukjp otve redej LEVIN, H.L., red, [Labor productivity of Kazakhstan's machinery i*adustr7 m'd the factors of its growth) Proizvoditellnost' truda v mashinostroon!i Kazakhstam i faktory es rosta. Alm- Ata, Nauka, 1965. 209 p. (MIRA l8t6) 1. Institut ekonomiki AN Kazakhakoy SSR (for Ashimbayev, Baytuleshev, Kovalenko). USSR/Cultivated Abs Jour Author Inst Inst Orig Pub Plants - Foddore. M Ref Zhur Biol., No 12, 1958, 53687 )!tuliny 1.0. P AS Kazakh SM Peculiarities In the Davelopment of the Root System of Perennial Cereal Grasses in Grass Mixturee. Vestn. AV Khtd,*, 1957, No 9, 105-115 Abstract At the agrobiological station of Kazakh University: the perennial cereals, tall rye graas and dewgrass) develop better and produce a large yield of seeds oAid bay when 40 mixed vith alfalfa, but have a less developed and shal- lower root system than when sown in pure form. The depth of the root penetration in the case of the tall rye grass in grass mixture is 100-110 am, and 140-150 am vhen soun in pure form. In the case of dewgrass the depth cbs Card 1/2 Ifffeat of alf&1fa on the nitrogen nutrition of grasses when growing together, Text*AN Xazakh,SSR 17 no,1133-39 JA 161, (MIRA 14:1) (Alftlfa) (Grasses) BAMLINJ 1.0. Root system spread of some field c-"Dpiv in the Dshurim desert steMs. Izv. AN Kazakh. SSR. Ser. biol. nauk 3 no.1973--85 ja-F 165. (MIRA 1815) BAYTULINI 1*00 -- I Root sysIA6w. of #coo dominant plants of 3mbs Plateau de3ert asseclatiow. Bat. x1mr. 50 no.Stll.35-1143 Ag 1619 1 igM 32110) 1. Utyublaska7a opytnaya atamtsi7a kormov i pmatbiahobe KMHEKEZYAN, A.N.; BMURIN, M.N. Possibility of lightening and simplifying the standard design of vens on the Zhetybay oil field on Mangyahlak Peninsula. Burenie no.9:19-21 164. (YJ RA 18: 5) .1, Vaevoyuznyy nauchno-issledovatel'skly Institut burovoy takhniki. 0. S!". Baytiml.n.q, 0. Sh. "E~roblems of the Etiology and.~Omraratlve Evaluation of the Effective- ness zf Certain Thera,--3utic SuBstances In Bronchor-tv-umonla of Calves.I Min '4icher Edixcation. Alrm-ktR Zooveterinqry Inst. klma-Jta, 105~ (Dis I sertation for t~!e degree of Candidatp in Vet,:~rinary ScienceO - SO: Knizhnny8 1,4topist No. 27, 2 JU1Y 1955 BAYTUPJI-I, IN. A. FWurin, N. A. "Festure reri-ne of the canelg" Trudy Alina-At. vet.-zootekhn. in-ta, Vol. VI, 1949s p. ?66-77 So: U-3566s 15 March .53, (Letopis 'Zhurm.-I Inykh Statey, No. 13, 1949) BATTIJIR~N, M. A. "The Safeky Level in Feeding Vitamin A tio Cattle and How to Obtain 1-to" Cand Agr ScJj Alma-Ata Zooveterinary Instp Alma-Atas 1953. (RZhBiol, No 4, Oct 5h) Survey of Scientific and Technical Dissertations Defended at USSR Higher Educational Institutions (10) Sol Sum- No.481, 5 may 55 USSR/Disoases of rarm t~nimals. Disaasos of Unknown R-3 Btiology. Abs Jour a Rof 'Zhur-Biol,, No 20~ 19561 92745 Author j3Wurjina Inst -M%Wu~.o of Votorinary Scionco of tho Ka- zakh 13-aneh of tho- All-Union j'wadamy of Agricultural Sciences imoni Lenin. Titla I The Combined Tra4tmont -of Bro.hchopnoumonia in calVess ()-,IL,~ P*ibsTr. in-ta vot. Xazakhsk, fil,, VAMNILI 195?t 81~125431 ,~tstraaijtOn one.farwivtho Alma-Ata,-ro'gion up. to 65 porcentlof newborn ealv Ios used to be stri- ekon vith-,bronchopneumonia. Ylith the back- ground of* improved foo-ding, 60 sick calves Card 1/2 Otses, of'-P~ la 'D 396.365, -a 1,40 Pm Abs, jour Ref 'Ihur4i6l a; i9,081 96962 Author.. ]r t 13 : ~ ~ 74 h Institut, Itl 41P i Sa 4i e n cResearch Veterinary Inst it, : WLS fi Title The- Treatwent of Bronchopnewaonia in 014ves 7tth Intratracheal Injections of Penie-111in, wid Benolin. OrIg ?4b. :,T:~. Kazakbske no-is vett In-taq 1957, 91 ~ P-29-235 TAbstralot rorty-!t~w~:'ealves, yere - tre %ted. 4#er their... ~ ier6- d__ keeping -and - f6-6dInj coll~ljfibhs -T Zlhe.calves v) ore, intratj~ache ally inlboted,with 35U-4 '00 t~o~s&nd units of rovocalne salt of 'renicillir dilfted in 5 ml -,)X^ &a ecmolJ-n sus- pension once daily-for 5 -onsoovlive-days. In ordex to inhibit t*i)6~ cough ref.rul 5 ml 'of a pero out stispensloh of novwalrxi, viler 'e :Lhtro- diced 1-2 minutes before the.-pent-tin!A injec- tior, "T h treatment resultadlr~ -mring 75,~ Cardu, n_v)&WtK, Ya. !. and PETMVI V. M. "Bronchial pneumonia in lanbs.11 Veterinarlya, Vol- 37, No. 8. 196o, P. 51 Ove. KLEYNBOK, Ya.I.; PETROV, V.H., kand.voterinarnykh naak; HAYTURINA, O.Sh. kand.voterinanqU nauk; PCOLINOV, I.S., nauchriyy sotrudnijc,- ATSEN, Ye.A.., nauchnyy sotrudnik Bronchopneumonia rate in lambs, Voterinariia 37 10.8:51-55 Ag 160. (MM 15:4) 1, Iwtitut vaterinarii Kazakhokoy akademii sellskokhozyaystvewykh nauk. 2. Chlen-korrespondent AN KazWR (for Kleynbok). (Kazakhstan-Lambe-Diseases and posts) (Pneumonia) BAYTURSUgNff,-X,- Tryout of creative forcee. Sov.foto 22 no-4122-22 Ap 162, (MIRA 14:3)~ 1. Otveistvennyy eekratarl prav2eniya Soyuza zhurna2istov Kazakhoskoy M. (lasakhatm--Photography-Exhibitions) VOLAFOWCH, M.P.; BAYUKJO Ye.l.; SAUKHLI, T.M.; PAVLDGRADSKIY, V.A. , Longitudinal wave velocities in specimens of sedimentary r(cks, saturated with kerosene andwater, at high pressures. Izv. AN SSSR. Fiz. zem. no.3:71-?5 165. (MIRA 18:7) 1. Institut fiziki Zemll, AN SSSR i Institut geologii AN IzerbSSR. L 2844-M Wr(l)IEWA(h) GV-1 ACCESSION NRt AP5021277 UR/0020/6 AUTHDRSA Vol .arwUhs Me Pej Ba k 3 CT: TITLEs The velocity of ultrasonic longitudinal waves at high proaaura.in and gas reservoir rocks of Azerbaidzhan S=Et AN SSSR. Doklady, v. W0 no. 5p 1965, lin-lin TOPIC TAOSt ultrasonic wave.. seismic w& roA, high pressurel in 5 radioeleclp~. tric; device I Sllmftea on wm vao.0iti." iwe made on rocks in the. Gaspiah~--lowlar4' ud the Baku Archipelago., The rocks were t93ted at pressures up to hOOO k1K/ce la An M-5 radioclectric device was used for measuring wave velocities, and a IDA zirconate and tknWate unit with natural frequency or 500 kilocyclas was used in, both transmitter and reneivero The sedimentary rocks were cylindrical cores., 3 cm in diameter'and 000 00 Tests -3-15 cm longs taken from depths ranging from 1 35 m waris made on clay* siltstone, sandebone, and lim-eatond. All part"ent propertiis -of -the rocks --wwo- measuredo -- Ex periments ihowed a sharp -in=eaae in-, v looity. with a: pressures -iithiha- greatest-- I= t - - 200%) be:Lag' ob sorred, -i ve" w4we (uj 0 U Porous sand and 6W, Change in limestone proved to be least generally 15-45%*; SOV/49-59-6-13/21 AUTHOR;,~kyu~k,Ye~.I TITLE: A Method of Determination of the Elastic Parameters of Rock Samples. PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya geofizi-cheskaya, 1959t Nr 6v pp 895-897 (USSR) ABSTRACT: A method is described where the measurement of the velo- city of transverse waves is not required. It is based on the laboratory conditions of measuring the propagation of the lonritudinal waves calculated from the formula L VPM W- ;' (I - a)/p(l +- a)(l - 2,or)j 1/2. The samples of rock used in the investigations were syenite, sandstone.and an alloy of aluminium for checking . The measurement consisted of determining the ratio a/% PK (a - radius of a sample, %P, - wavelength of P. wave).. It was established that the velocity of V EM did not vary with Card 1/3 SOV/49-59-6-13/21 A Method of Determination of the Elastic Parameters of Rock Samples the frequency. The latter was measured with the gauges of 50, 125 and 250 kh. The range of the ratio aA PM was 0.1 to 2.0. The results are shown in Fig 1, where the ordinate represents the velocity of the longitudinal wave and the abscissa - the ratio aA The following elastic para- meters were determined (table on p 896): density p .4. Poisson cogfficient cy , Young's modulus E , shear modulus 0 . velocity of transverse waves VS 0 volume compress- ibility 0 , The ratio of VP, /V, was found to be 1.60 - 1.68 which agrees with the results found for real conditions. Card 2/3 . . BOV/49-59-6-13/21 A Method ot Determination of the Elastic Parameters of Rock Samples Thanks are given to M. P. Volarovich and 0.- 1. Silayew-for valuable advice. There is 1 figure, 1 table and there are 7 references, of which 5 are Soviet and 2 English. ASSOCIATION: Akademiya nauk SSSR, Institut fiziki zemli (Acadenw of Sciences, USSR, Institute of Physics of the Earth) SUBMITTED; April 26, 1958. Card 3/3 2- f UP H1,11P ju v !A--r al 10 IV 1 131 ass's Mill 5 v 0 TV ski -a I!Vt .V 31 1 1 'C Studying the e2Aetio properties of rock samples from a deep bore- hole at high pressures* Izv- AN SSM. Bar. geofiz. no.12:1736-1761 D-1600 (XMA 23929) I* Institat fitiki Zewli AN 88SR* (Rocks-Testing) Ollastic waves) 30 o AUTHORS: TITLE: PERIODICAL: 84664 S/020/60/135/001/017/030 B006/BO56 Volarovich, M. P. and Bayuk, Ye. I. The Influence Exerted by a Uniform Pressure of up to 4000 kg/cm 2 Upon tlielilastio Properties of Rock Samples Doilady Akademii.tauk SSSR9 1960, Vol. 135, No. 1, PP. 6548 TEXT: The authors investigated the elastic properties of rock samples under high universal pressur by measuring the propagation rates of longi- tudinal waves: V 172 - the propagation rate in a thin bar and V~ IV b - (E/ Q) ] / VP 05. ) 1 2 _ the propagation rate in an infinite medium (E - Young's modulus, 9 - density, 0 - Poiaaon coefficient); the experiments took place in a high-pressure chamber, in which the pressure could be varied from normal to 4000 kg/cM2. The ultrasotic velocity was measured by means of a pulse method, where a modified M KA-5 (IKL-5) type device was used. As transmitter and receiver ammonium dihydrophosphate Card 1/4 84664 The Influence Exerted by a Uniform Pressure B/020/60/135/001/017/030 of up to 4000 kg/cm2 Upon the Elastic Boo6/BO56 Properties of Rook Samples crystals were used; for the purpose of measuring Vp b, the authors operat- ed with 100, and for measuring Vp m with 600 kc/sec. The samples investi- gated had the shape of circular cylinders with 3 cm diameter and 16-20 cm l(Ingth. The various ore samples are numbered (of. Table 2). The results of measurements are shown in form of diagrams, the assignment of the curves to the samples takes place according to the same numbers. Fig. 1 shows the propagatio.1 rate of longitudinal and transversal waves as func- tionsof the pressure brought to bear upon the samplo. In general, the cu, within the range below 1000 kg/Om2 showud a steeper rise; in the further course, the pressure dependence of V is insignificant or V is entirely independent of pressure. Fig, 2 shows the Young's modulus and the modulus of shearing as a function of pressure. The course taken by this curves is similar to that in Fig. 1. The reaulto of the measurements of the Poisson coefficient at various pressures are given in Table 2: Card 2/4 84664 The Influence Exerted by a Uniform Pressure 3/020/60/135/001/017/030 of up to 4000 kg/OM2 Upon the Elastic B006AO56 Properties of Rock Samples Pratumirp Irv/nM2 Rock 1 500 1000 2000 4000 Gabbro 82 0.31 0.30 0.29 0.29 0.29 Gabbro-diorite 38 0.29 0.28 0.28 0.28 0.28 Granite 247 0.24 0.22 0.22 0.21 0.21 Granite 248 0.12 0.?1 0.19 Granite 249 0.12 0.16 0.19 0.19 0.19 Quartzite 22 0.19 0.19 0.19 0.18 Sandstone 213 0.18 0.18 0.17 0.15 0.15 Sandstone 105 0.19 0.19 0.19 0.16 0.16 Sandstone 94 0011 0412 0-15 o.16 0-17 ,arl 206 0.19 0.19 - 0.19 0.19 arl 207 0.21 0.19 0.19 0.19 - I There are 2 figures, 2 tables, and 6 Soviet references. V\/ ASSOCIATION: Institut fiziki Zemli im. 0. Yu. Shmidta Akademii nauk SSSR (Institute of the Physics of the Earth imeni 0. Yu. Shmidt of the Academy of Sciences USSR) Card 3/4 8466h The Influence Exerted by a Uniform Pressure S/020/60/135/001/017/030 of up to 4000 kg/CM2 Upon the Elastic Boo6/BO56 Properties of Rock Samples PRESENTED: May 18, 1960, by P'. A. Rebinderg Academician SUBMITTED: May I'l, 1960 Card 4/4 MAROVICH, ~~Yej.j LIMIN, A.I. 1-- MAotie propn-ties of rocks and the atmarptlon of elastic vayes by tbam at %Igh all-romd p"sawes.. Prim. ulltraakust. k leal. vashch. no.1335541 161. (HIRA :16s6) (Rocks-Elastle Properties) (Mastia va"s) VOLAROVICH, M.P.; BAYUK,, Ya.I.; ZHDANOV., A.A.; TOMASHEVSKAYA, I.S. Study of the elastic properties of rocks of the K21a Penin- sula under hydrostatic pressure up to 7000 kg./cm . Izv. AN SSO . Ser. geoflz. no.8tU78-1181, Ag t64 (MIRA 17t8) 1. Institut fiziki Xamli AH SSSR* AFANA59M.~ G.D.; BAYUKI., 19mcrys B.P.; VOUROVICHv M.P., ULz8v=9 BIV, Phy3ical 'propertieB and the absolute age of certain rocks In India and Ceylon. Uv. AN SSSR Ser. geol. 29 no.3t22-42 W16A (HIM 17 23) I* Inatitut geologii rudnykb mestorozhdaniyj petrograftij. minera- logii i gookhimii AN SSSR i Institut fisiki. ifwli AN SSST4 Hookwa. s1b=10#1j55joo511W11061 AOMMCK IM. AP4034338 "AUMOR: Afaaw 1yev# Go Do (Correspodding member); Volarovich, K. Pej Boyuk*, Too ~A;. Galdln.p N. Ye. TME: Investigation of velocities of elastic vaves In ultrabssic rocks or the lWnahesorsk Pluton under bigh (allal%d) pressure SOUM: AN MR. Doklady*0 ,f. 355# 00. 5j. *&p 1058-W1 VaVe TOPIC TAGS: elastic vaye velocity, scismia research,, tran vereal, veloc*tY* langitiYA"W wave velocity, rock &p, geology.. geophysics, high prewir6j, VUM=p Monabegorsk pluton., tectonics ABSTRACr: In preparation for the cadng geological-geogbysical (deep sclowe probing) of the Baltic rbield., the authors howe'lavestigated the velcelty of elastic V06VOll in ultrassic rocks of the Monebegorak pluton located In the central' p&A of the " Peninsula. M)e age of this rock (by the radioactive A4.Mthod) is about 3 x IV yeane The veloolt;f of both -fitudinal &A trensverse Vane .A vas datenzimA under pr*snum vp to 4..000 Me velocity of the 104AW VaVes averaged 7OWto em al"o. and that of the trawvms VMS C. d -1/0 VOLAROVICHIO GALDIN, N.Ye. Effect of high pressure on the elastic properties of rock samples collected along the outline of the area of deep seismic sounding in northern Karelia. Izv. AN SSSR. Fiz. zem. nc.1:109-115 165. (MIRA 18:5) 1. institut fiziki Zemli AN SSSR. "AUY 11, WD W.j i N. BAYI)K$ A wavtio 'n 1 and ga.A reservoirs ze..-baijanw. high prL,.zs-m-es. All 'SZ:R 163 no-5t-131- 133 I Ag (MIRA 1888) 'If.-Ititut V.,zlIk! 1"'wPit All' SSSR 1 Institut geo!3gii AN rbSSR. Sulnttte3 Noemly~r 10, ACC NRs AT6034505 S-Oul~CEFCODE-l.'"UR/0000/66/000/000/0064/0075 AUTHOR: Afans'yev, G. D.;_1M9j,_.YqtJ * Belikov, Bs P.; Borsuk, A. He; Volstrovichs t,s '11. P,; Zalesskiy, A. V.; Pavlogradskiy, V. A.; Sinyanov, I. Z. ORG; none TITLE: Preliminary data obtained by correlating physical properties of rocks from ;Northern Caucasus with geological and geophysical data 7 SOURCE: AN SSSR. Otdolenlys nauk o Zemle. Nauchnyy sovat po 'Aomplakenym issladovant- yam zemnoy kory i verkhney mantii. Clubinnoye stroyeniye Kavkaza (Abyssal structure of the Caucasus). Moscow, Izd-vo Nauka, 1966, 64-75 TOPIC TAGS: Reophysics, seismic prospecting, petrology, stratigraphy, /Caucasus ABSTRACT: The most important of the different age associations of igneous rocks in some of the structural zones of Northern Caucasus (the piedmont region, the foot- hills, the transverse depression zone, the granitoid zone and the axial zone of the Major Caucasus ridge) are described. The post-Selurian, posi;-Lower Carbonaceous, pre-Triassic, post-Lower Jurassic, pre-Middle Cretaccoxis and ~;enozoic formations are described. The magmatic geology of Northern Caucasus is compared with geophysical data. A new scheme is suggested for the deep structure of the territory. The ancient basement is shown to consist of Hercynian and older formations. In -Card 1/2 ACC NR: AT6034565- particular, a substage of lower Hiddle Paleozoic formations is differentiated. It differs greatlyin respect to its physicaLl properties from younger rocks of Upper PaleozDic and Mesozoic ages. In the region of the Major Caucasus this substratum has been completely reworked by upper Paleozoic granitic intrusions. Tht ancient rocks outcrop in a few areas; however, to the East the Caledonian basement is covered by Mesozoic and possibly Upper Paleozoic formations. It is believed that the deep seismic sounding conducted near Ellkholovo has located the buried extension of the Caledonia structure of the Western Caucasian foothills. Orig. art. has: 6 figures and I table. SUB CODE: 08/ SUBH DATS: 26Feb661' ORIG REF: 020/ OTH REF: 001 BAmov, i, Fadtory Managemant Efforts of the wipply divisiss Of A Plant to economize wAterials. Za ekoz.mat. No. 2, 1952. MS!Ihly List of Russi&A Accessions, Library of %;osgress, December 1952. Unclassified. EA;;-VaH A*.;L To - ---- ------- L 8603-66 E~tr(l)/EtIT(m)/EIIP(tll/E.~IP(b) IJP(c) JD ACOMION RRi AP,9Drft.1171 'UR/0339/65/000/ock/0076 1 AMCR1 henko M. A, TITM Determination of the tempero4ure dependence of the first'constant of the zagnetlp crystallogmphic wdsotrW an polycrystalline litbivm-alumimna ferrites SOMM V M. ritikap no. ho 20% 7641 TAGS# taTeraft" dependence, xNmetic ~"~s rgM ferriter lithium con- tain' alloy., aluminum containing &1lay). magnetic ofiturationj, magnetic suseept- Ibility ABI37RACT: Experimental results we presented of measurements of. the temperature dependence 0 the first constant cof wAgnetic crystaUogrspbic anisotropy (k3L in a series of polyorystallfte ferritea Lio.OY*2.5_&Al&04L, wbere a - Oj 0.21, 0.11P 095P amd 0.6. 2he measurements won wAde by the method of approach to saturation In the temperature Interval from 170 to "QKj, in a pulsating mgnetic Meld. 7he tests Nor madeAna cQwbIAW4Q-&3A-ac-(2500 -cps) -flelde --- 7he -results abow tbat-in-- fielde 1000-2000 oe the diffe"Aftel susceptibility can be described by the ex- f preselcm R a A/RF + B/91 + C/H' (As B.. 0 constantsp H magnetic field intensity) and tbat the teopmUre dependence of k.% Is in satlsfactai7 quantitative agreement Crd 3/2 ,I ~- Card 42 66 ~J%~) -J-D M JO M0 AM NRs APS004469 9: Ult/0048/66/030/0 06ii7/(KH;7 AIMEOR: .1styakov. N.S,.--: Rusov, 0.1. ORG: I MYSICS Institute of -the Siberian Mellon-of -the S�SR Academy of kelp-nces (Inatitut-fiziki Sibirskogo otdolonlya,Akadeali nt4jk SSSR) TITW: Forronalnetic resonance In multilayer film systems (Transactions of the Pecond All-UnIon SMalum on the Physics of Thin Forromwetto 11169 hold at Irkutsk 110 JUIT. to. 15 JU1Y 19") A SOUM: AN SSSR, Izventlya, Sorlya Micheakaya,v. 30, no. 1, 1966, 64-67 TOPIC TAM forromagnatIc film, mAgnotic thin film, Iron nickel allay, cobalt, so2y- bdonum, quartz, laminated nater1r.1,forronagnotic roxonance,superhigh frequency` ABSTRACT: The authors have Investigated the ferromagnetic resonanc 'e at 9 MR& of thin for r.-,**p*t1c Olus and vu t4loyer film systems consisting of alto'' to layers offj!=w '"o % S~e-,films were Vacuum evaporated at 10 0000 yaglLellS *11=4~knd guar -qmm ag in a I The - magnetic floldlat the rate of40 pa onto glass substrates heated to 200C# forromagaietic. resonancii a6morptiou: iiief neas'urod"In a rectangular citvity., resonator ex- cited in the T,Zit'A iode'an-A having a.Q factor of 1000. The 7-ma-diasister circular films,-fa-stmed to the end of a brass rod, were Introduced Into the resonator ,through a 7 so d1aneter bole In the 4md wall. The resonator was tuned with a teflon rod inserted through a hole In the side walle The magnetic field was. modulated at Card 1/3 L 274201-46 ACC MRs AP6004469 435 Rz'w1th 6--speclal windIng &?Ad Wang1ven a saw-tooth form by varying the current in the main windit*. - The resonance curva.s. w.erc_dIspIa?ed on. an oscilloscope or.recor with inr uIll1voltmeter. .Slngle-6Uyer films of composItion 16Fe-_79_X_i-_3Mo,1=dS_ 17F(TrONWoWt~Ickness from 400. to 2000 A were investigated. For the No-coutainin g f i-las Igo- rZonant vu4MetIc f Ield decrtased with Increasing thickness from 1214 Oe fwr a 400 1 film to 818 Oe for a 20001 film and the width of the resonance ranged between 33 and 47 Oe. This small width of the resonance absorption line In favorable for. practical applications. Data are veported on only tbree Co-containing ;Ilms. Of these,, Ithe thickest (2000 1) showed two absorption peaks separated by 60-80-00. No explanatiom for this in offered. A 6oo A film had a 34 Oe wide absorption line at 886 Os and a film of unspecified thickness 'between 1000 and 20M, A had a 38-Oo-wide absorption line at 861 Oe. Multilayer film systems having up to 10 layers were Investigated. In these systems the metal films were approximately 2000 .4 thick and the intervening quartz films w-..re from 2500 to 2000 .4 thick. As the nVaber of layers was increased the ab- sorption line became deeper and wider and began to evince complex structure. -A ten- layer system clearly showed four resonance peaks separated by 60-80 Oe. 7bis behavior fie ascribed partly to dipole-dlp~ple interaction between. neighboring layers,,as Bug- ly to. gested by D.Chen and A,H.Morrish (J. Appl. Phys., Suppl., 33 N 3 (1962)), and part the influence of the conditions of deposition. It was found that if thevacuum was broken between deposition of metal and deposition of quartz the structure of the Mb- vorption curve of the resulting multilayer system was considerably different from.that of a system which wai deposited vithout breakift the vaculim. Auxiliary %xporlmeuts with single-layer 20P*-SONi and 3(Wo-45HI-25Co films with and without quart;. L 1?410-66 ICC NRs OW4469 showed that the Presence of the quartz considerably reduced the strength of the resonant fiold and increased Ch* width of the reaonance~ Tb* J resonance lines of two-layor systems with quarts between the layers occurred at approximately th* same fleld,Atr*ng~b and were-of approximately the same width'-as those of the corresponding single films witb qnartz coverings.. SUB 00'D3-, 20/ ATb PRESS% 426o iA -A -L-24 8-66 VTM/EW(2 ~/VPO) 7 ACC MAt APbOL4256 SOURCE.C.'. CODEF UR101091667011700510930/DiF31 AUTHORt -Chistyakov# Nd Sq; -Ignatchanko# Ve As; B&Zgkov, 0* Agj kV3oV&6 So G 0 ORGI none TITLEt Certain UH? properties of multilayer SOURM Radiotekhnika-L.elaktronika, V. 116, no 5~j 19669 950-951 TOPIC TAGSs magnetic,'thlh film ABSTRACT: Tranimismi"' A'ad reflectioll factors of single-layer and oultilayer v2agnstLc*fLltd6 were measured in a waveguide system operating at I - 3 cm. Individual films were made by sputtering l7Fe8ONL3Ho alloy on a SlAss substrate heated to 200C in a vacuum of 10-5 mm Ug and in a magnetic field of ev 100 oe.: Multilayer films were made by insulating.eath filta layer by.a layer of SiO 1000 A thick. Experi- mental data (see Fig.,I) shows that the transmission factors for Multi- layer films (point 1-10 layers, 1000 1 each; point 2-40 layers, 500 each) substantially exceeds the same factor for- a single layer ~_104 filM (solid line) By breaking the film into layers, but keeping the same total-thickness$ skin depth is increasede This feet was substantiated by'switebing the films ia'a-cavity resonator and, L-card I 12 VDCI: 539.216.22:621&3184 noting the resonator frequency shift. The shift for multLlayer films- is greater than that for equivalent single-layer film and shift linearity is preserved-up,to total film thickness of.3 k 104 (30 layers 10,00 each) a- 'OrLgi arto hast 2- figures#, JBDJ. SUB CODEs 09/ 'SUBH 'DATIEs IIAP'r65/ ORIG REP 1005/ ATD PRESS: ar C d - . ~- ~& 1;&A . --- Investigation of enargy azd anL-ular -fistributims 02 jr"-mesonz produced by protons with energies of 470 and &SO VeV (11/50) C.~~,-,U'T-,Symposiiri oil High EnerGy Acceleratom and Pion Physics. Geneva 11-23 June 56 1n. Brancb #5 rwr.c 01- KY 7 1 - - slam --et!rA 'T L NzL'I gin,!~m ~n 51 OAYOKO~ ALM HOR BAJUKOV, J.D., 00ANESAN, J.C., NAPKIN, A.4. PA 203 8 TITLE The $,bsorption of y-Quanta with the j&verage Energy of 500 MeVin Lead , and Aluminium. (Russian) Copper PERIODICAL , . Zhurnal Eksperimentallnol I Tooret. Fiziki, 1957, Vol 32, Nr 1 PP 183-183 (U.S.S.R.) Received 3/1957 Reviewed 3/1957 ABSTRACT y-Vanta originate from the decay of neutral pions which were produced in the inner target of a phasotron by 660 MeV protons. These Y-quanta were recorded by a pair-like y-apectrometer with 12 channels, on which occasion the spectrometer was at a distance of 23 m from the target. Be- fore the collimator, which was fitted behind a protective wall of 4 m thickness, a device was arranged, by which the bundle of y-quanta was periodically interrupted by means of a lead absorber. The y-quanta record- ed by the spectrometer in the case of fully covered and not fully opened bundles were counted separately. For the determination of the coefficients of the absorption of the y-quan- ta in Cu and Al the semicircular lead disk in the rotating device was re- placed by absorbers of copper and aluminium. The frequent change of ab- sorber3 made it possible to carry out measurements without a monitor and to diminish the number of measuring errors. The bundle of y-quanta passing through the collimator was purified from electrons and positrons by means of a special magnet. The authors obtained the following values ( in cm*/g) for the coefficients of the absorption of y-quanta with the energy of - 500 150 Mev: 3 Card 113 y PA - 2038 The Absorption of y-Quanta with the kyerage Energy of 500 MeV in Lead, Copper, and Aluminium. Pb 0,1115 1 0,0025, Cu 0,0510 1 0,0025, Al 0,0295 � 0,0017. The absorption of the y-quanta at Ey - 500 MOV takes-place essentially by the production of electron-positron'pairs. As shown by computation results, absorption by photo effect and Compton effect amounts to -, 1,2 O/o in the case of Cu, and to -. 2 O/o of the total absorption cross section ir the case of Al.. The cross sections for the absorption of y-quanta found here agree w93.1 with the computed results obtained bf H. DAVIES, H.BM, L.MaIMON, Phys.Rev., 93, 788 (1954). It remains to be added that the data for 500 MeV y-quanta which agree with computation-e were obtained in the case of permanent pre,,tence of a lead absorber of 5,55 g/cma thickness in the bundle. If suche'a lead absorber, by wbich the bundle-is filtered, is lacking, cross sections which are larger by 10 0/0 SA obtained. When measuring 41-he absorption cross section of 2~O MeV y-quanta, no influence was found to be exercised by the additio- nal absorber by which the bundle is permanently covered. The cross section of the absorption of 280 MeV y_cpanta obtained here agrees with the re- sults obtained by J.W.DE-WME, A.ASKIN, L.A.BACH, Phys.Rev., 83, 505 (1951). The reason for the increase of the absorption cross section of 500 MeV y-quanta when an additional. lead filter was lacking could not be explained. Card 2/10 PA - 2038 The Absorption of y-Quanta with the Average Inergy of 500 Hev in L ead , Copper, and Aluminium. ASSOCIATION United Institute for Nuclear Research, Laboratory for Nuclear Problor-:. HWENTED BY SUBMITTED AVAILABLE Library of Congress Card 3/3 AUTROR --BAYUKOVI 7r# Dot SINLYEV A.N.r TYLPKIN A.A. PA - 2699 . TITLE Experim-entid-Compari son of the Energy Spectra of 3-Quanta resulting fron th* Decay of Neutral Pions (which were created by 660 MoV-Protons 911 Carbon- and Lead-Nuolei). (Eksperimoutall-noye sravn*niye suerastiabookikh op*ktrov kv&ntoy ot xispada x - mozonov, abrazovannykh na yadrakh ugleroda i ovintsa. protonami a onergiyey 660 MoV. Russian.) PZRIODICAL Zhurnal Eksperim, i Toorot. Piziki 1957, Vol 32, Nr 29 PP 385 - 386 (USSR). Received: 5/1957 Reviewed: 6AM ABSTRACT Yor a more exact comparis n of 2-quants created on light &Ad heavy nuclei the authors :arried out relative measurements of the fluxe of quanta within the various domains of the spectra t menti:n*d a vee The angle of observation in the direction of notion of the protons amounted to 0 . Measurements were carried out by means of a magnetic dcuble spetatrometer with 12 channels, The targets consisting of lead and graphite fitted Anto the vacuum chamber of the accelerator were-txoh d very minute. At low energies of j- qu t& E < TO Nov) a difference is - noticed on the 41--q to i tod3n oarbou and lead, This dif- forono* in connected ap W ontly with the modification of the angular distribution of the neutral pions. CARD 1/2 PA - 2699 Experimental Comparison of the Energy 'Spectra of a -quanta resulting from the Decay of Neutral Pious (which were created by 660 WeV-Protens on Carbon- aud Lead-Nuclei). This modification in due to the interaction of the bombarding protons with the nucleons of tb* nucleus on the occasion of strong abserptiol of mesons. The hard I.- quanta with the angla of observation 0 are essentially created on the occasion of the decay of these neutral pious which are created on that side of the nucleus which Is averted from the bombarding protons and in heavely screened off 'by the remaining nucleons of the nucleus, The soft quanta, however, are essentially created on the surface J thoLnUoleUe which in exposed to the protons* There- ferev a relative increase of soft 3-quanta in the spectrum is observed on the occasion of tLe creation ef neutral pions on heavy nuclei. Considerable differences are to be expected also in the energy distributions of the mesons created on light and heavy nucleie The energy,%stributions of the neutral pions created under aa angle of 0 n carbtn-~ and lead-nuolsi do not differ noticeably. Possibilities for a more oleo& study of these pion spectra are shown. (I table) ASSOCIATION: United Institute for Nuclear Research PRESIM29D BY: - SUMTM: 2. 11. 1956. AVAILARM: Library of Cougr*nne CAN 2/2 AUTHOR BAYUKOV, Yu.D., KOWDATIT, U.S., Tr.AFK'IN,, A.A. 56-4-5/52 TITUS TI% investigation of the rsnergetic and Angular Distribution of v*eaon3 Formeo,On Carbon Nuclei by Protons With An Y-nergy of 47o and 66o NeV. (Issledovanip anergetichaskikn i uglovykn rasprodelaniy ff*ezonov,obrazo- vannykh na yadrakft -iglaroda protonami 3 awrgLYW470 i 66o MeV -Russian) PsKIODIGAL Zhurnal Eksperim.i. T*oret,FWki,l957,,Vo1 32,,Nr 4,pp 667-67i(b-ts-s-R.) Received 7/1957 Reviewed 0/1957 ABsTRACT The results obtained by tne Investigation of energetic spectra on the oc- casion of tne decay of iyll-mesons produced on carbon nu.clei by protons with the energy of 66o WeV 13 discussed.The method of spectral analysis was u3sa.The neutral moacne have a very short life(5,,lo-15 see.). The experimental scheme is shown in form of an illwtratior.The carbon tar- get is inside the vacuum chamber of the accelorator and waj- irradiated with protons of the average enrgy of 66o MeV. The y-quanta formed in the 'target penetrated through an opening into a concrete wall or 4 a thickness and collimated through a diaphragm -4jito a lead block.The collimated bundle or y-quanta.,wnich was purified from charged particles by the magnetic field of a special clectromagnot,ponetrated into the converter of the 12-cnannal- led pair-spectromfiter.The apectrometer was set up at a distance of 23 m from the target in the direction of the tangent to the orbit of the protons. The author beer* gives a doWlea description of the pair spectrometer used, The differential cress section for the production of y-quanta on the carbon nuclei by protons with an energy of 66o MtV for 18L' in the laboratory sy- ca rd 113 stem amounts to d8 Z/a&)(l8o")-(l-5+ op2).io-87 =4/sterad. The ratio of The Investigation of the Energetic and Angular Distrioution 56-4-5/52 Of AISSOW Formed On Carbon Nuclei by Yrotons Witn An k;nergy of 47o and 66o Rev.. the flux of Y-quanta under the angles 0 and 1do" is equal to 5sl+Ux3* The energy spectra of the y-quanta is tnan analyzed. l.Dependence of the spectrum on the angular- and energotic distribution of tne"*osons.It follows that with the isotropic distribution of the wu-me- sons,indapandent of their energy distrioution,tne spectrum of the y-quan- ta is or symmetric shape with respect to the energy 1/2F_,,. 2.Uompari3on of tn* energy spectra of y-quanta on tne occasion or tne de- cay of if'-semons produced by protons with the energy of 470 Uev on tne nuc- lei of beryllium.Mustration 5 shows that tho energy spectrum of the y~ quanta of the decay of mesons pr~)duced by photons with the energy of 470 90(center of mass system) on the nu,)loi o.' caroon.At a proton energy of 470 NOV energies are produced,whicn. tire an a proximation to tne maximum possible energy attainable oy the meson in tne reaction.Witn an energy or 66o NO of tne proton3,me3onB with considerably lower energies are formed than is possible as a maximum, 3.Snergy spectra of e-zesons produced ay protons with the energy of 770 and 66o W.Mustration 7 shows the energy distribution of wll-aesors in the center of mass sy3te:.& for --arbon3 oy protons with the energy of 4?o MeV.0n the same illustration it shows the spectrum of ffO-me3ons.The energy- and angular distriuution ol 0- mesonawhich had been measured at a proton energy of lejo M9V shows that the nesons produced in this case which are neutral on the occasion of the collision of nucloons,absorb the greatest Card 2/3 pan of the free energy of the collisiton., as well as Aso the greatest an- A The Investigation of the Energetic and Angular Distribution 564-5/7~2 v4-Xesons of Formed On Carbon Nuclei by Protons With An Energy of 47o and 66o iiev. gular momentum.Tne same phenomenon is observed in the case of lower pro- ton energiesoAt proton energies of 470 Moll the spectra of ffu-,mssow pro- ducect on composed nuclei dixfor only slightly from spectra computed on the assumption that mesons are produced only with maximum energies, so that at a proton energy of 66o M*V a considerable dirference between tne spectra ootainea and those ccmputed at the same conditions is ObServeci. At a proton energy of 66o M*V ti4-maons with an energy that, is consideraD- ly lower than that which is possible as a maximum are mostly produced.Con- sequently it follows that in the case of tne production of mesons by tho proton energy of 66o MeV tne nucleons in tne final state acquire a high kinetic energy andstherefore0al3o high momenta.Witn an increase or proton energy fromWo to 66o X*V the anplar distribution of the ffl-mosons chan- ges considerably. ASUOCIATION United ln3tituts for Nuclear Research FRESM39D BI bUBKITTMD 28.1o.1956 AVAILMz Library of Congress Card 3/3 AUTHM Xu.DU TYAPKINp AsAss BAYUKQVj TITIZ _ The Energy Spectrum of y-quanta of the Decaying ,O-Meson Created by the Interaction of 660 MeV protons with Hydrogen Nuclei (Energsticheskiy spi:ktr y-imantov ot rasp&" YO-mezonov, obraz3vannykh protonami a energ4v 660 MOV n& ya&Wdi vodoroda. Russian), PatIODICAL Zhurne Eksperim, i Tooret, Fiziki, 1957, Vol 320 Nr 5; PP 953 - 956 (U.S.S.R.) ABSTR&CT The y-quants, were measured with the help of a scintillation telescopet on which occasion the production of vo-msons took place in such a man- ner that two targets one of polyten and one of carbon, were one after the other exposed to the inner of the phasobron. Besides, a number of double targets was alterningly irradiated in such a manner that., simul- tansously with the change of targetj also the y-counting device could be adjusted to this pair of targets* The angular distribution of One w0-mesons created by the collision of 660 May protons with H-nbclei has t1w form I + (Os3 + Oal) Coll 0 The wo-masons spectrum h;8 a marked maximuoi at $v 75 MOV, Furthermore it was established experimentally that the angular distri- Card 1/2 bution of the vfO-meaona created by p-p interaction is isotropic, 56-5-1/55 The Energy Spectrum of y-quanta of the Decaying wO-Xeson Created by the Intaraction of 660 NO protons with Hydropr Nuclei ASSOCIATIOW United Institute for Nuclear Research HWENTED Br SUBMITTED AVAILABL9 Library of Congress Card 2/2 SOV/120-58-6-4/32 "AUTHORS: u Kozodayev, M. S., Markov, A. A., Sinayev, A. N.9 in, A. AO TITLE: A Multichannel 3~air y-Spectromiter. 1. Calculation of the Main Characteristics of the y-Spectrometer (Mnogokanallnyy parnyy gamma-spektrometr. I. Raschet osnovnykh kharakteri- stik-gamma-spektrometra) FERIODICAL: Pribory i takhaika eksperimenta, 1958,, Nr 6, pp 23-29 (USSR) ABSTRACT: la a pair y-spectrometer the energy of the quanta is de- termined by measuring the total energy of the courponents of the electron-positron pair formed in a thin converter. The first 2-chaimel pair spectrometer was built by Dzhelepov (Ref4). Later spectrometers built on this principle were widely used in measuring the s .pactra of hard y-rays (ReLfs.2 to 8). The electron and the positron leaving the converter were deflected by a magaetie field in different directions and for certain values of their energy they enter ionisation counters connected in coincidence. For a given intensity of the magnetic field and a fixed position of the counters, such a spectrometer will record a fraction of the pairs produced by y-rVs in a given energy range. In a simple 2-channel Card 1/6 spectrometer In which one channel records the electrons and SOY/120-58-6-4/32 A Multichannel Pair y~spectrometer. I. Calculation of the Main Characteristics of the y-spectrometer the other the positrons, an increase ia the accuracy of measurement is associated with a marked decrease in the efficiency. Good energy resolution and high efficiency can only be s:Lmultaraeously achieved in a multioban-nel meter. In such a spaatrometer the efficiency may be inez~eased by a factor r_jn2 without loss of resolution-,, where z~, and n are the numbers of eleatron and positron counters. I-, sich a spectrometer se'veral energy intervals may be i at the same time. A number of suoh multichannel spect::~:-,. meters have been described (Refs.5, 6 and 8). The of a y-speetrometer as a measuring instrument is diAe3, ~,, ~.nf-d by its effioienoy an& spoetral sensitivity. In multichannel system it is necessary to take into aeoox characteristics for the various pairs of channels of the spectrum. In this connection, a discussion is given In the present paper of the dependence of the efficiency and spec- tral sensitivity of the separate pairs of channels on various Card 2/6 SOV/120-58-6-4/32 A Maltichannel Fair y-spectrometer, 1, Calculation of the Main Characteristics of the y-speetrometer parameters of the spectrometer: 1) Spectral sensitivit-V: the basic diagram of a y-speetro- meter considered in M paper is shown in Fig.l. in whieb the meanings of the symbols employed are indicated. In view of the finite width of the counters, the spectrometer records y-quanta in a certain energy interval from E y min to RY max . The corresponding spectral sensitivity curve is then shown in Fig.2a and is of triangular form with a dis- persion given by 1/6 L2/(r, * r 2 )? where 1-0 is the width of a 61 0 coUnter and ri and r2 are the distances from the con- verter to the oentres of the counters, respeetively. The effect of the width of the converter upon the spectral sensitivity is examined and it is shown that a converter of a finite width introduces a spread into the spectral line in the high energy region of y-quanta. As the angle 9 between the di--nection of motion of the y-quanta. and the Card 3/6 straight line connecting the centre of the converter with SOV/120-58-6-4/32 A Multichannel Pair y-spectrometer. I. Calculation of the Main Characteristics of the y-spectrometer the counter increases, the spread of the spectral line de- creases. At (p - 900 the width of the !:,-ectral serisitivity curve is independent of the converter width. The effect of the converter width gives a distribiCoion of tiNe form shown in Fig.2b, which has a dispersion given by: 4- 4 2 GOtg (P 2 2 180r1 'rP The effect of multiple scattering in the converter is estimated and expression._- are derived for this effect also. Finally,, an estimate ie given for the radiation loss experienced by the electron- positron pair on traversing the converter, 2) Efficiency; in this section the Bethe-Heitler expression for the probability of formation of a pair by a y-quantum, of Card 4/6 SOV/120-53-6-4/32 A Multichannel Fair y-spectrometer. I. Calculation of the Main Characteristics of the y-spectrometer energy E is used (Ref.13) with a modification described b Bethe Yet al in Ref.22. 3~ Multichannel system: in a multichannel spectr6seter the electrons and positrons formed by y-quanta of a given energy are recorded by a number of combinations,of pairs of counters. The electronic circuit of such a spectrometer Aduld rdeord coincidences between pulses from each eleetron counter with pulses from any positron counter. Thus, any combination of one electr6m:counter and one positron counter is, in fact, a 2-channel spectrometer. For a given geometry a spectrometer containing n channels records y-quanta in n-1 energy in- firvals of different mean energy. In practice, one seeks to find the form of the spectrum and the absolute intensJt7 in dne of the energy intervals. To find the form of the spec- trum it is sufficient to know the relative efficiency of recording for the different energy intervals, and this is given by Eq.(10). In order to obtain the absolute intensity in one of the energy intervals it is necessary to know the total absolute efficiency of recording of y-quanta in one of the energy intervals. "Ohis problem is not treated. Card 5/6 SOV/120-58-6-4/32 A Multichannel Fair y-spectrometor. I. Calculation of the Main Characteristics of the y-spectrometer V. V. Mellnikov is thanked for carrying out a number of calculations. There are 2 figures and 22 references, of which 4 are Soviet, 1 German 1 Soviet translated from English and the rest are Engiish. ASSOCIATION: OVyedinennyy institut yadernvkh issledovaniy (United Institute for Nuclear Studies) SUBMITTED: December 27, 1957. Card 6/6 SOV/120-58-6-5/32 AUT ov Yu. D . Kozodayev, M. S., Markov, A. A. Sinayev, A.N., Tyapkin, TITLE: A Multichannel Fair y-Spectrometer. II. Description of a 12-channel Spectrometer (Unogokanalln,7y parnyy gamma-spek- trometr. II. Opisaniyi dvenadtsatil-anallnogo spektrometra) PERIODICAL: Pribory i tekhnika eksperimenta, 1958, Nr 6, pp 30-40 (USSR) ABSTRACT: Application of a multichannel pair spectrometer in synchro- cyclotron work presents a number of specific requirements as far as counters of the ionising particles and the electronic system of the spectrometer are concerned. Since the beam intensity is high and consists of short pulses of 200 to 300 lis each at a repetition frequency of 40 to 80 pulses per see it follows that the apparatus must be very fast. ..It is desirable that the input blocks should have resolving times not greater than 1 lis. The large background intensity in synchro-eyelotron work means that it is always necessary to use a special selection system which records only electron- positron pairs. 'For this raason, in the spectrometer each component of a pair should be recorded by a number of counters in coincidence with sufficiently low resolving time. The Card 1/7 present paper describes a 12-channel y-spectrometer which has SOV/120-58-6-5/32 A Multichannel Pair r-Speetrometer. II. Description of a 12-channal Spectrometer been used over a number of years in studying the spectra of hard y-rays and neutral Ir-meson decays (Refs .2-6). The first variant of the spectrometer was built in lc)49. In 1951 and 1954 the spectrometer was modified to improve its --harac- teristics. The spectrometer described here satisfies com- pletely the above requirements and is based on the design calculations given in the previous paper (Ref.1) in th--'-s issue. 1) Magnetic ustem and Reometa of the instrument. The magnetic field is produced by an SP-56 electromagneT,. Fig.1 shows the disposition of the counters for two ty-lies ot demountable pole pieces. The gap between the poles ia _~_- o~,- and the maximum field in the gap is 18 000 oersted. Tite electromagnet current is stabilised to 0.1%. In studies of ~;ray s~e tra, in the energy region 20 to 200 MeV, 29 = JL800 iglb Zd in the energy region 100 to 450 MeV, 2(p - 900 Fig.la In thG former case semi-circular focussing of Card 2/7 SOV/120-58-6-5/32 A Maltichannel Pair y-Spectrometer. II. Description of a 12-channel Spectrometer electrons and positrons was used, and this led to increased efficiency (Ref.1) because it was posRible to use wider and thicker converters. For y-quqnta in the energy range 450- 600 MeV, 2v - 900 but the counters were at a larger distance from the converter. Copper converters were used (0.1. 0.3 and 0.5 mm, depending on the energy). 2) Resolving power and efficiency. Fig.2 shows curves of the total spectral sensitivity for the 7th energy interval for various values of E YO and thick- nesses Tk of the copper converters. These curves are based on the theoretical data given in the previous paper and are obtained by a statistical combination of the partial distri- butions due to a) width of the counters, b) width of the con- verter, c) multiple scattering and d) radiation. As can be seen, the form of the total spectral sensitivity curve is VexV nearly triangular which means that the total spectral sensitivit7.is governeA mainly by the width of the channels t. (see Fig.1 of previous paper, p 24, this issue). Card 3/7 SOV/120-58-6-5/32 A Multichannel Pair y-Spectrometer. II. Description of a 12-channel Spectrometer 3) Counters and selection system. The counters used were proportional counters having a Fylindrical stainless steel cathode, 10 mm in diameter and a molybdenum filament 0.1 mm in diameter. They were filled with (CH2(OCH3)2) at a pressure of 160 to 200 mm. The working voltage was 1600 to 2000 V. Th~ counters have an effective dead time not ex- ceeding 10 see. The efficieney of the counters for par- ticles with relativistic ionisation reaches 918% in a coin- eidence scheme with a resolving time of 5 x l&-7 see. The delay of the pulses due to dri;(t of electrons through the coun-ter San is less than 10-Y. The counters give. electri- cail pulses with amplitudes between 10-4 and 1 V. The large difference in the amplitudea requires the use of amplifiers having a wide dynamic range and an amplification of a few thousands. 6-fold coincidences were used and the number of random coincidences in each 6-fold channel was 0.02 pulses per see. The number of eleetron-positron pairs recorded per Card 4/7 SOV/120-58-6-5/32 A Multichannel Pair y-Speetrometer. II. Description d a 12-channel Spectrometer sec depended on the efficiency of the spectrometer with respect to the y-quanta in the measured energy interval and the form of the spectrum and was in the range 0.1 to 10 pairs per see. 4) Bleetronio scheme. A block diagram or the electronic part of the spectrometer is shown in Fig.3. Tts) left-hand portion of this diagren shows 6 co-ordinate counters of the electron series (a, - ad, 6 co-ordinate counters of the positron series (Bi - 3.) and 4 selection counters (All, AnI V and 'U"). Each of these counters in practice consists of a gr,)up of counters whose filaments are connected. A recorded electron or positron should pass through 3 counters (1 co-ordinate and 2 selection counters). A pair is recorded if a 6-fold'coincidence-takes place. Negative-going pulses from each counter are ampli- fied by a corresponding amplifier-converter (Fig.4). These amplifiers have a rise time of 2 x 10-4 see. Pulses from all the 16 amplifier-converters are applied to the main block which is at a distance of 1.5 m from the amplifier-converters Card 5/7 (Fig-5). Pulses from the selection counters are applied to a SOV/120-58-6-5/32 A Multichannel Pair y--Spectrometer. II. Description of a 12-channel Spectrometer 4-fold coincidence scheme while pulses from the co-ordinate counters are applied to mixers and in addition through.delay lines to a hodoseopic system consisting of 2-fold coincidence circuits and output uftivibrators. The pulse at,the output of a mixer appears in the presence of a pulse in at least one of the co-ordinate counters of a givenseries. Pulses from both the mixers and also from the 4-fold coincidence scheme are applied to a 3-fold coincidence scheme which produces the final output pulse. It follows that the latter pulse appears when a 6-fold coincidence takes pl4c6,1.4p.when a particle passes through at ledst one of the co-ordinate dountera in the electron series, through one of th) co-ordinate couaters, of the positron series, and all the counters of the se'Leetion system. The resolving time of the above coincidence schemes is 5 x 1o-7. 5) Method of measurement and treatment of results. Fig-7 shows the experimental 4trrangement. In Ws figure 1 is the proton trajectory, 2 is the target, 3 is the synchro- cyclotron chamberl 4 is a concrete wall, 5 is a collimator, Card 6/7 SOV/120--L58-6-5/32 Multichannel Fair y-Spectrometer. II. Description of a 12-channel Spectrometer 6 is a diaphragm 7 is a clearing magnet which removes electrons and positrons from the beam, 8 is an additional screen, 9 is the convertor and 10 is the spectrometer electro. magnet. Pig.8-shows a typical result obtained for the energy spectrum of y-quanta from neutral V-meson decays. The mesons were produced by 660 MeV protons at a carbon target. The spectra are measured at an angle of 180-00 to the direct- ion of motion of the protons. G.F.Zorin, B.A.Erasnovidov,L. A.Fadeyev and G.N.Stepanov are than ed for their assistance. There are 8 figures, 4 tables and 7 Soviet references. ASSOCIATION: Ob'yedinennyy institut yadernvkh IssledovaniY (United Ifttitute for Nuclear Studies) SUBMITTED: December 27, 1957. Card 7/7 85699 3/0~6 ;0/038/006/042/049/XX BOO 7B070 24~ 4 op 0/0, /M/ /M) AUTHORS: Bayukov, Yu. D., Leksin, G. A. TITLE: The Possibility of Using Nuclear Reactions to Obtain Data on in Interaction PERIODICIL: Zhurnal eksperimentaltnoy i teoreticheskoy fiziki, 1960, Vol. 38, No. 6, pp. 1907 - 1908 TEXT: Nuclear processes are considered in which transferred momenta are small also for large energies, and from whose theoretical interpretation it is possible to obtain data on it, xK, and KK interactions, as is shown here. This is shown for the process where a pion is produced by a pion. Use is made of the formula of Chow and Low which gives tho relationship between the cross 3ection for this process and the in interaction cross section for the case of small transferred momenta (Ref.1). It is shown that this formula can be applied without much error for the production of a meson by a meson on a nucleus, and that it is thus possible to obtain data on in interaction from the total cross section for a nuclear reac- tion of the type x + A 4 x + % 4 B. This is true especially for the Card 1/2 The Possibility of Using Nuclear Reactions B/056j6O/O3e/Joo6/O4?/O49/XX to Obtain Data on xx Interaction Boo6/BO7O 12 - - 12 reaction x + C 4 1 + X + N .Moreover, in momentum approximation? the formula of Chew and Low must be multiplied by 00 S2 . f I tf (r)eipr f(r)dr)2before integration. This function gives the 0 probability that the nucleus whose ground state is described by the wave function t(r) continues to remain in the ground state even when a momentum p is transferred to it. As is shown in a diagram, S2 falls rapidly with p. Only for p larger than 3 is this function greater than zero (for the case of the C12 nucleus considered here). K.A.ftr-MMItos an is thanked for advice ind help. There are 1 figure and 2 references: I Soviet and 1 Us. SUBMITTED: February 23, 1960 Card 2/2 27698 S/120/61/000/003/008/041 9032/13.14 AUTHORS: ._Rayukov, Yu.D., Leksin, G.A. and Suchkov, D.A. TITLE: Characteristics of Spark Counters Operated-..~ylith, Pulsed Supplies PERIODICAL: Pribory I'tekhnika eksperimenta, 1961, No., pp. 66 - 68 TEXT: The authors have investigated the characteristics of various spark counters operated with pulsed supplies. The principle of the experiments is illustrated in Fig. 1. The plane-parallel electrodes forming the spark gap were placed in a glass container which was evacuated and then filled with air, nitrogen, carbon dioxide, helium, neon and argon at 4arious pressures, p, respectively. The polished brass 2 electrodes were 55 x 55 mm in size. In addition, a further 4;ounter having dise electrodes, 30 mm in diameter and made from aluminium foil 7 P thick, was tested In open air. The distance between the electrodes was varied between 2 and 6 mm and the Card 1/7 27698 S/120/61/000/003/008/041 Characteristics of .... F,032/93i4 high-voltage pulse wasderived from a -r(-K-1 400/116 (TGI-1 400/16) thyratron controlled by A telescope consisting nf- two scintillation counters C1 and C 2 0 The thyratron pulse was delayed by 0-5 "ec relative to the passage of the particle through the counter. All the experiments were carried out with coomic-ray particles. In some cases, a constant clearing Voltage V 0 (0 to 2 kV) was applied to the counters-The limitivgxesixtor R 2 could be varied between fractions of an ohm and 1*4 k-Q . The remaining parameters are indicated In Fig. 1. The spark discharges of ~he counter were recorded continuously, by ear, or by counting electrical pulses induced inthe antenna of a scaling unit. Rig. 2 shows the results obtained for the efficiency R defined as the ratio of the recorded particles to the total number of particles passing through the counter (R2 = 0, Vo = 0, T,= 0.5 lisee) Card 2/7 27698 S/12o/61/000/003/oWo4i Characteristics of E032/9314 Fig- 3 shown typical efficiency curveb for various' clearing voltages and high-voltage pulse delays, -C The efficiency of a spark counter can be approximately calculated from the formula 1 - exp -n (d - v PI where n in the number of ion pairs produced in the discharge gap, v = Ke in-the charge drift velocity which depends on the clearing field c = V0/d and the mobility K By comparing this formula with the results shown in Fig. 3, one can estimate the mobilities of the charges i!I the spark gap. For air at STP it is found that K 3- a cm /sec , while for argon at p = 400 mm Hg K X 10 cm. /see. Fig. 4 shows the efficiency as a function of the delay -r- I -inUsoc, for R2 = 0, V0 = 0 and d = 6 mm - Acknowledgments to M.S. Kozodayev for discussions and interest in the work. Card 3/7 27698 S/120/61/000/003/008/041 Characteristics of .... E032/E314 There are 4 figures, 3 tables and I non-Soviet reference. SUBMITTED; juiy 4, ig6o Fig. 1: --t:: ~f-ikjW~AW .LPN. _t I U=== BAIUKOWS U.D.; LMINs G.A.; SUCHKOV$. D.A.; SHAIAMOV., Ya.Ya.,* SHEBANOV, V.A. -------- Backward elastic scattering of 2.8 bey/c %' -mesons on neutrons. Zhur.ekspA t#or.fiz. 1+1 n0-1352-55 Jl 161o (KML .14:7) 19 Latitut tooreticheakoy i ek8perimentalluoy fiziki AN SWRo (Mbsons-Scattering) (Neutrons) Bk=OV. ; LMMIN.9 G.A.; SHAUMOV, Ya.Ya. Elastic scattering of T- -Monona by 2o8 Bev./c noutrono. Zhur.ekap.i teordis. 41 no-4:1025-1030 0 161. (MIM .14:10) 1 1. Institut tooraticbeekoy i okoperimentallnoy fiziki AN SSSR. (Mooonso-Scattering) (Neutrons) s/95Y61/041/006/019/054 B102 B138 AUTHORSi Bayukov, Yu. D., Leksin, G. A., Shalamov, Ya. Ya. TITLIt Investigation of the react 'ion 7-+n--)ir+n+miP with a beam of mesons with a momentum of 2.8 Bev/0 PERIODICALs Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 41, no. 6(12), 1961, 1787-1792 NaT t The reaction *_+n -#1r+n+mirQ, m-1 t2 f was studied by means of a 50 cm long, 17-liter freon bubble chamber without magnetic field. The bombard- ing pions had a momentum of 2.8 + 0-3 Bev/o. The gamma quanta arising in I? decay were recorded with quit; high efficiency. From the stereophoto- graphs taken 221 single-pronged stars were selected, representing pion interactions with quasi-free neutrons. Only in two cases was KO formation recorded, so strange particle formation could be neglected in evaluating the results. The gamma and pion angular distributions were meuured and the multiplicity of the reaction was determined. Resultst In the rN o. m. 9. the angular gamma quantum distribution was anisotropic and Card 1/3 S/056J61/041/006/019/054 Investigation of the reaction ... B102/B138 asymmetric, the forward-to-baokward ratio was 1.76 + 0.30. In the laboratory system the angular r and e distributioni coincided within the limits of statistical error. The anisotropy in Ir angular distribution increased with the energy of the Tr" meson. The anisotropy in gamma distributions tended to decrease with increasing number of gamma quantas 1-7+0-4 for stars with one quantum, 1.7+0.5 with two and 1.5+0.7 for stars witS 3 - 5,r-quanta. In the lab-system-it was also greater for stars with Nioir-emission angles than for