THE FORMATION OF SINGLE MESONS BY GAMMA QUANTA

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Document Number (FOIA) /ESDN (CREST): 
CIA-RDP80-00809A000600380447-4
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RIPPUB
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C
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2
Document Creation Date: 
December 22, 2016
Document Release Date: 
September 12, 2011
Sequence Number: 
447
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Publication Date: 
March 21, 1951
Content Type: 
REPORT
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PDF icon CIA-RDP80-00809A000600380447-4.pdf98.27 KB
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Sanitized Copy Approved for Release 2011/09/14: CIA-RDP80-00809A000600380447-4 1 COUNTRY SUBJECT HOW PUBLISHED WHERE PUBL'ISHED" DATE PUBLISHED LANGUAGE INFORMATION FROM FOREIGN DOCUMENTS OR RADIO BROADCASTS CD NO. CLASSIFICATION CONFIDENTIAL[BI N MENTIA1 Scientific -- Nuclear physics, mesons Monthly periodical Moscow Dec 1950 DATE OF INFORMATION 1950 DATE DIST..21 Mar 1951 50X1-HUM SUPPLEMENT TO REPORT NO. TNif DOCUNRMT CONTAINS INFORMATION AFFICTINO TNC NATIONAL DIPINSI OF THE UNITID STATES WITNIN THE MEANING OF ESPIONAGE ACT EO U. I. C.. EI AMP SS. AS AMINOSD. ITS TRANSMISSION OR THE RIVILATION 01 ITS CONTINTI IN ANY MANNIR TO AN UNAUTHORIIID PINSON IS PRO' MISITID IT LAW. REPRODUCTION OF THIS FORM If PROHIIITID. Zhurnal Eks erimental'no i Teoretichesko Fiziki, Vol 7IX, No 12, 1950, pp 1057-63. THE FORMATION OF SINGLE MESONS BY GAMMA KUAHTA A. M. Bardin and V. V. Mikhaylov Phys Inst imeni Lebedev, Aced Sci USSR L^ brief digest of the above report follows_7 The authors calculate the differential effective cross section of the formation of charged mesons by gamma quanta in the nucleons. The calcu- lations are carried out for scalar, pseudoscalar, and vector (with tensor bond) theories. The angular distributions of the mesons generated are graphed. The formation of mesons by photons was investigated by A. Sakharov (Zhur Eksper Teor Piz, Vol 17, p 686, 1947), by Benoist-Guental, Prentki, and Ratier (Comptes Rendus, 1950), and by Foldy (Phy Rev, 1949). In these works, however, they did not pay sufficient attention to the angular distribution of the mesons formed, which is of well-known interest in connection with the experimental works of Steinberger and Bishop (Phy Rev, 195,0), since the calcu- lations were conducted only according to the scalar and pseudoscalar theories. The authors of the present article calculate also according to the vector theory.- To clarify the nature of-the an gar distribution of mesons for practical regions of energies of gamma quanta (several 100Es Mev) one can with sufficient, accuracy consider the nucleons.as nonrelativistic particles. Therefore, it is' expedient, in the Hamiltonian described in the relativistic form for a system consisting of a nucleon in-electromagnetic and mesonic fields, as done.by Bhabha (Proc Roy Soc, 1938) and"Wentzel (Rev Mod Phy, 1947); to make a tran- sition to-Pauli's approximation for the nucleon (mesons, of course, are con- sidered as relativistic particles). As a result of this transition; one obtains' certain expressions for the interaction of nucleons with the meson field, namely, the (a) scalar variant, (b) pseudoscalar variant (in the,ca4 of gradient bond), asd (c) vector variant. STATE ARMY NAW AIR X . ? a Ni e ^r w.w_4 y~sWir+'~'l hu'N.+azd.4avl zwr.:+Mz~.-us.u...6.sEam.L:u _. r..a:,u .n.c.rrl l`uit>-ti:,ai Sanitized Copy Approved for Release 2011/09/14: CIA -RDP80-00809A000600380447-4 Sanitized Copy Approved for Release 2011/09/14: CIA-RDP80-00809A000600380447-4 1 r ETA! After a lengthy mathematical treatment the authors obtain the differential cross sections as a function of the angle for these three types. The authors thank M. A. Markov, who proposed to them this topic, for his aid in its execution. They also thank G. I. ICharlamova for her assistance in the numerical work. CONFIDENTIAL ?WibL+a.1z:M.fS.a. w?vuay9 ~w:u:?-'a'. ,w-w~:,oix:lu .~.i..;:SFk e.,Fc.nu:aS4+twtEU-+::3~:ald?~asYiFc;i': .~0:~4..ir..:6;u.:.d:.rur..b4+?>W:41~e~Jyr.~lik7C-aMSrta,iR~ii:Gt+Wstfr6:t :;_.~... _.S:__.;. Sanitized Copy Approved for Release 2011/09/14: CIA-RDP80-00809A000600380447-4