SCIENTIFIC ABSTRACT SHIROKOV, V.YA. - SHIROKOV, YU.M.

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SCIENTIFIC ABSTRACT
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14UZYCHU,KO, Nina Mbaylovna; YURKEVIGH, Tattyana. Yakovlevna; BAKIROV, A.A., prof., glav.red.; RYABUKHIN, G.Ye., prof., red.; USPENSKAYA, N.Yu.,prof.,red.; ZHDANOV,M.A., prof., red.; DOLITSKIYI V.A., dots., red.; SPIKHINA, A.Y., kanda geolo nauk, red.; YUDIN, G.T., kand. geol.-min. naukq red.; TABASARANSKIY, Z.A., dots., red.; BAKDOV, E.A., dots., red.; BYKOV, R.I., dots., red.; FaIKIN, K.V., kand. geol.-min. nauk, red.1 JOYAZEV, V.S., dots., red.; SHLiOKOV, V.Ya., st. nauchn. sotr., red.j YUVGAS, S.V.p ved. red.; NEVELISHTEYN, V.I., ved. red. (Geological conditions and fundamerrLal characteristics of oil and gas accumulations in the limits of the Bpi-Hercynian platform in the south of the U.S.S.R.) Geologicheskie usloviia i osmvnye zakonomernosti ra=eshcheniia skoplenil nefti i gaza v predelakh epigertsinskoi platformy iuga SSSR. Pod red. A.A.Bakirova. Mo- skva., Gostoptekhizdat. "1 1.1, (Central Asia] Sredniaia Wis. 1963. 442 p. Vol.3. [Volga Valley portion of Saratov and Volgograd Provinces) Saratovsko-Volgogradskoe Povo2zhle. 1963. 153 P. (MIRA 17:4) 1. Moscow. Institut neftekhimicheskoy i gazovoy promyshlennosti. BAKIROVI A.A.; SHIROKOV, V.Ta. Proapects for finding- ImTs oil and ga3 accumilation3 in the Tajik S.S.R. Sov. geol. 6-no.5.*51-62 My 163. (MIRA 16:6) 1. Moskovskiy inatitut naftakhimichookcry i gazovoy proa3h- lannosti, imeni I.M. OubIcina. (TaJiki3tan-Patroleum geology) (Tajiki3tan-Gas, Natural-Geology) T~-'IPOV, '1';.; SHIPOKOV, V.Ya. Water.3 and brInnn or oie meijoz-)i Tajik DepreBsion in connection wt,. Nefte,gaz.geol. i geofiz. no.12:1%- 1. Moskovskiy ordena Trudovogo KraL neftekhimicheskoy i gazovoy prorky:;h -38 1;,". 3 al,jp PIS unitary, finite 112, V2 . ..... I +M Ps unitary, finite 0; 1, 2, -M PIS unitary, finite 1/2, 3/2 . ..... -1 -M For P - Unitarity; mieasurements Nain invariants Aaclitional U Represer.- of representation accord- n2 2 > 0 invariants tation Ing to spin-variabJ13 -P ~1~ 2 2 CC F~ If T Pa- unitary. infinite n pia. unitary, infinite n P+n unitary, infinite > > I/V Bro Card 56-5-20/46 A Group-Theoretical InVC3tigation of the First Principles of Relativistic . Quantum Mechanics II. A Classification of Irreducible Representations of an Inhowgencous Lorentz Grorip which ar--. Slavic. ASSOCIATION- Moscow State Univi~rsity (Moskovskiy gosudarstvannyy universitet) SURMITTED: Deceaber I I , ! 956 AVAIIABLE, Libmry of Congress Card LA AUTHOR: Shirokov, 11u.M. 56-5-21/46 TITLE: A Group Theoretical Investigation of the First Princip2es Of Relativistic Quantum Mechanics III. Irreducible Representations of Classes P. and 00 and Not Fully Reducible Representations of an Inhomogeneous Lorentz Group (Teoretiko-grappovoye ra3smotreniye oanov relvativistskoy kvantovoy mekhaniki III. KeprivoU~e predstavlaniya klaasov PO 1 00 1 ne vpolne privodimyye predstav- leniya. neodnorodnoy gruppy Lorentsa) PERIODICAL: Zhurnal EkBpe-rim. i Teoret. Fiziki, 1957, Vol- 33, Nr 5, pp. 1208-1214 (USSR) ABSTRACT: The classification of the states of a relativistic quantum system is derived theoretically. The unitary and nonunitary characteristics for the classes Po and 0. are shown in the following table: Represen- Unitarity,mea3ure- Main in- Additional in-mriants tation ments according to variantis spin variables p2 01 rKl--4~ Card 1/2 P unitary, simple CC it 0 SH= �1 , S r =il =O' l v2. t 0 0 56-5-21/46 A Group Theoretical Investigation of the Fir-at Principles of Relativistic Quantum Mechanics III. Irreducible Representations of Classes PC and 00 and Not Fully Reducible Representations of an Inhamogeneous Lorentz Group P unitary, simple C( . 0 SH= ti , Sf0=tl'7-j PC unitary, infinite 0(-C > 0 SH= *1 :r 0 PIC unitary, infinite G( SH= t1 0 C nonunitary,infinite C < 0 S - ti P i0 H- e nonunitary,infinite cC= Cn mn n m>n mn correction to the kinetic energy of the n-th nucleon)& Furthert the correction term to the interaction -17aniltonian if' is mn investigated. This interaction correction formula is written down for 2 particles in the states Jos2 01 > 082 10---., 11p2/, O1N , 11P2 01> 1/2 1/2 3 112 with r 0 = 1.65-10-13cm(hw - 15 Mev), the potential is written down in the form V-V o(O-317 + 0.500 P + 0.183 PQ) f(r/a) and for the Gaussian potential course On Relativistic Corroctions to the SOV/56-36-2-19/63 Phenomenological Theory of,the Levels of Light Nuclei and for the square potential well (Ref 1) Vo . -33.6 Mev, A " 2.1.10-13cm . V(in kev) is calculated and compiled in a table. The correction was found to dependto a high degree on the shape of the potential and i3 of the order of magnitude 0.02 - 0.2 Mev for a pair of nucleons, 0.2-2 Mev for liCht nuclei, and 2-20 Mev for heavy nuclei. For nuclear levels it is of the same order as for nucleon pairs. There are I table and 3 references, 2 of which are Soviet. ASSOCIATION; Inztitut yadernoy fiziki MoskovskoGo gosudarstvennogo universiteta (institute for 'Nuclear Physics of Yoscow State University) SUBMITTED: June 16, 1958 Card 3/3 21(l) BOV/56-36-3-35/71 AUTHORS: Kaminskiy, A. K., �,hirokov, Yu. It. TITLE: On the Electromagnetic Radii. of the Lightest Nuclei in the Ground - and in the Lowes'EkaillMm States (Ob elektromagnitnyleh radiusakh legebayshikh yader v ouiiovnykh i nizahikh vozbuzll- dennykh sostoyaniyakh) PERIODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fiziki, 1959, Vol 36, T1r 3, PP 874 - 878 (USSR) ABSTRACT: In the present paper the authors calculate the radii of nuclei with mass numbers 5 - 8 for the ground- and the first excited states on the basis of experimental data on isotopic multiplets and scatterine of high energy electrons on nuclei, and they especially investigate the dependence of the radius on the excited state. In a figure, 4 diagrams show the de endence 3 of r on excitation energy: Figure a) for He5 - Li ' 0 b) for He 6 _ Li 6 _Be6 (in dependence on E of Li6 exe c) for Li a - Be a -B8 (in dependence on E of Be8) and exe d) for Li7 _ Be7. It was found that the nuclear radius of He5 Card 1/2 and Li5, as an exception, shows no monotonous increase with SOV/56-36-3-35/'71 On t:ie Electro,-_- -:,,-tic R!,. !ii a-*' the Lightest !Iuclei in the Gro-un':- and in the --owect ExcltatiocL.S~tes For the 2. excited level with E - 16.69 Yev the nuclear radios is smaller than for the firit aA also smaller than for the qround Btate. For Li7 - Be the nyclear radius in- creases rapidly with energy, for L17 - Be there is a weak clopondence, and the namo in the cace for the nuclear radius with A.=B. In general it may be said that, with the exception of the He5-Li5 doublet, the nuclear radii for all nuclei in- crease monotonously with energy. It was found that agreement between experimental data from the scattering of fast neutrons on nuclei and those calculated from the Coulomb (Kulon) energy difference can be improved by ssuming a different value for r for s- and,y-shells. For Lil, fo example, one gbtains o 13 Ir r. . 2-42.10- cm and rp . 1.32.10- am and for Li . 9 - - 2.65-10-13cm and rp - 1.07.10-13cm is obtained. There are 1 figure and 8 references, 3 of which are Soviet. ASSOCIATIO'T: Moskovskiy gosudarstvennyy universitet (Moscow State University) SUBMITTED: September 16, 195.9 Card 212 Shirokov, Yu. L'. SOV/56- 36- 3-, (", Y The Groun-Thco.~ctic.-.l Trcrtment of the Bases of Quantum ilcchanJes. V. (Teoretiko-gruppovoye rasr :;,:otreniy,~ osnov relyatjvi-;.skoy kvantovoy mel.,haniki. V.).Irroducible ul t.ie Inhomogencouo Lorentz Group Inclu-lir,- Sp;~tiacl tnd 'Leflections (Neprivodiryye prods tavloniya neodnorotino.-y* [~,rup.--y Lorentsa, vklyuchayushchey otrazheni,-a p:-ostrnr.:1tve i vo vromeni) ~!-DDICAL: Zhurntl e':3perirentallnoy i teoreticheskoy fiziki, 1959, Val )6, !~r 3, Pp 079-608 (USSR) Int A C-2: The praL~cnt 7. ended to carry out a systematic inve-,itication u-' timc reflection 1a%7 within the rr-: of the ordinary of the representation of th~.- inhomoi7,encoun :,,~xlup oithout using a certain form of enuatio-n -,ot-~cr. The Wigner-formulation of the ti.,.c reflection law -'q Cto~i2.t vith by a separate paper, and the is the care ',lc connected with the CPT theor.----". In the present 7a-.cr a--thor, by utilizing the re-ultr obtained by papers I - ;1, gives a complete classifi: .1.2-,,P-i 1/2 all irreducible rcp-rc::--!rt--tionc o1' the inhomocnnc--..,- ';r,)uP-*-'hro.-etica1 Treatnunt of tht, Danes of SO//56-3(--.1'5-,'6/7 1 .1, 'J,,rif;tjc ;uantum Mechanics. V. lr:-ed,~Cible lwpreccntations ol" the Lorentz Group Includir.,,~; Sprttial and Time Reflections Lorcii't.n. ,~,roup includin,-' jpace and time reflections. It in ~:hown 'that the concc.,jit of time parity cannot be intro,luc,2d for i,~,-~rticlos --.-rith a rest mass. For such parLiclas trio unequivalcni., cc~nc*ptz, -.-.,hich differ in respect zo .ime paarit~;, prof),,?r-A-:~s, jxist for a Civen spin. '.',ith th" -'lit. of t`1C conce -ot of % covering i_-roup it is --hown tnat fo-- j.~rxticlo-- half--Jlnt(--~-~er spins the number of possible rc':~rc--~ntr~ticnr; -.ith various reflection laws is larger than hitherto ns:~uned. Ther- r-re 4 tables and 9 references, 6 of -Alich Soviet. .'ookovskiy uaiver',:itet (Yoscow State Univer--it-,) T Sontonber 16, 1'. SHIROKOV, Yu. M., Doe Phys-Math Sci -- (diss) "Theoretico-group methods in relativistic quantum theory." Moscow, 1960. 12 pp; (Academy of Sciences USSR, Physics Inst im P. N. Lebedev); 150 copies; price not given; bibliography on pp 11-12 (30 entries); (KL, 25-60, 125) SHIROKOV, Yu.M. Spatial and time reflections In the relativistic theory. Zhur. eksp. I teor. fiz. )8 no.1:140-1.50 Jan '(0. (MIRA 14:9) 1. Institut yadernuy fiziki Moskovskogo gosudarstvennogo universi- teta. (Relativity (Physics)) (Particles (Nuclear physics)) 9u S/056/61/041/006/040/054 B109/B102 AUTHORSt Zelenskaya, N. S., Shirokov, TITLEs Relativistic corrections to the magnetic moments of H3 and He3 PERIODICALt Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 41, no. 6(12), 1961, 1934-1937 TEXT: Ageneral expression is derived for the relativistic corrections to t e nuclear magnetic moments arisinG as a result of non-Galilean relativistic corrections to the Hamiltonian of nucleon-nucleon interaction. According to F. A. Zhivopistsev, A. I. Perelomov, an4 Yu. M. Shirokov (ZhETF, 36, 476, 1959), the non-Galilean correction to nucleon-nucleon interaction has the form Card 1/4 t S/056/61/041/006/040/054 Relativistic corrections to the ... B109/B102 H' iiM,P, 4- i (P OHM") (P MR op. + d% + W.~ IPPI - (PL"--,,) (pp) + ip,p) 00- P = p ,, +,P,, - P (PM - P"), x = XM - X, denotes the interaction energy of the m-th and n-th nucleons. r of the non-Galilean relativistic correction to the nuclear .,.-?nt is- obtained from. (2) as Alt 2HM,, (e,,, + e,,) (n (r - R)J P 31 (et + e~)(Cr. - 13.) [n ((r (r - R) n Card 21,; dr . (I dr 31790 S/05 61/041/006/040/054 Relativistic corrections to the ... B109YB102 (3) has been calculated "or the 2 S1/2 'tate of mirror nuclei by using the wave function of the harmonic oscillator and the expression H - (W + u + BP + -~'P P V(r) (V(r) - Gauss or Yukawa potential). mn x Lr x r The results are shown in a table. Concluslonsi A) The relativistic non-Galilean correction exceeds considerably the correction of the spin-orbital interaction; B) the correction terms have the cirrect sign; the maximum value of 0.086 explains only 30A of the discrepancy between I theoretical and experimental values. The difference is attributed to the ef5ect of exchanee mecons, which has been discussed by S. D. Drell and J. D. Walecka ~Phys. Rev., 120, 1069, 1960). T),ere are I table and 13 referencest 4 Soviet and 9 non-Soviet. The four most recent references to Enrlish-language publications read az; followat L. D. Rearlstein, J. C. TurLf, K. Wildermuth. Nu--l. Phyz., 18, 23, ig6o; A. C. Butcher, J. M. 11c Namee. Proc. Phys. Soc., 1_4, 529, ~7959; R. A. Ferrel# W. M. Visscher, Phys. Rev., 102, 450, 1956; J. M. Berger. ?hys. Rev., 115t 223, 1959. Card 3/4 317 ~0 S/05 611041100610401054 Relativistic correction3 to the ... B109YB102 ASSOCIATIONs Moskovskiy gosudarstvennyy universitet (moscow state University) SUBAIITTEDt July 12, 1961 Legend to the 'fable: (1) shape and parameter of V(r) (V is given in 0 'YPv i in 10- 13 cm); (2) Gauss potential; (3) Yukawa potential. ;v, napamelpw Y(r) -0 B 0=. X-0,022111 A~L(Hl) 4 MHCS) AMR,) I AIL(Re) ar=1,73 111 0 -0,048 O,Ot4 -O,Ot4 a~1'94 1-1 0 -0,032 0,009 -0,009 a~1,55 0 -0,018 D,OD5 -.0.005 11memma.-i lOxans V, :- &9* a-1, 17 j.. 0 -O.DS6 0.026 -0,026 v,46.-w .-t &1 . 0 -0,056 0.017 --41,017 Curd 4/4 SIUR~!nV4 Yu. M. -- -- - - -t~-! ~~ - , , - . I "On the Conditions of the Mikrocovariance and Mikrocausality without any References to the Postulates of the Quantum Field Theory" report presented at the Intl. Conference on Ifigh Energy Physics, Geneva, h -11 July 1962 Inst. for Nuclear Research of the Moscow State University S/056/62/042/001/027;/048 B100102 AUTHORS: Cheshkcv~ A, A., Shirokov, Yu. M. TITLE: Invariant parametrization of the relativisti: scattering matrix PE'RIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, v. 42, no 1, 1962, 144-151 TEM Tne parametrization is first performed in the center-of-mass system A number of 7ersions, all of them relativistically noninvariant, are tested In so doin the authors base on M. Yacob, G. C- Wick (Ann of" - 7, 404 9 L. Wolfenstein, J. Ashk Ph,s 595, in (Phys. Rev., ft~, 947, -,9~52), 71, 1. Ritus (ZhETF, 1264, 1957); S. M. Bilenlkiy, L. I Lapidui, L D Puzikov R. M. Ryndinj~ZhETF, a, 959, 1958); and Ya. Fisher, S Ck.ulli (ZhETF, 36, 1740, 1960; .12, 1349, 1960). The scattering matrix 3 ~ms parametrized in the c.m.s. does not essentially differ from other parametrized matrices. However, the invariantly parametrized elements of the. S matrix are written in matrix form, in which no nonpkysicai parameter5 appear, and the particle chiralities are used to describe the initial an-a Card /2