MARC

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035 |a (TOE)ost5440427 
035 |a (TOE)5440427 
040 |a TOE  |c TOE 
049 |a GDWR 
072 7 |a 73  |2 edbsc 
086 0 |a E 1.99: conf-770968-1 
086 0 |a E 1.99:lbl-6572 
086 0 |a E 1.99: conf-770968-1 
088 |a lbl-6572 
088 |a conf-770968-1 
245 0 0 |a Diffusion model predictions for kinetic energy, mass, angular distributions, and. gamma. -ray multiplicities in heavy ion induced reactions  |h [electronic resource] 
260 |a Berkeley, Calif. :  |b Lawrence Berkeley National Laboratory ;  |a Oak Ridge, Tenn. :  |b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,  |c 1977. 
300 |a Pages: 16 :  |b digital, PDF file. 
336 |a text  |b txt  |2 rdacontent. 
337 |a computer  |b c  |2 rdamedia. 
338 |a online resource  |b cr  |2 rdacarrier. 
500 |a Published through the Information Bridge: DOE Scientific and Technical Information. 
500 |a 08/01/1977. 
500 |a "lbl-6572" 
500 |a " conf-770968-1" 
500 |a International conference on nuclear structure, Tokyo, Japan, 5 Sep 1977. 
500 |a Moretto, L.G. 
520 3 |a In the present formalism the diffusion along the mass asymmetry coordinate has been generalized by refining the treatment of the radial and angular motion necessary for an adequate reproduction of the kinetic energy and angular distributions. The radial potential is used to evaluate the radial force. The interaction time and the average penetration for each l-wave are estimated. The diffusion calculation is then carried out for the duration of the interaction time. The angular rotation during diffusion is calculated for each fragment on the basis of the tangential energy. The resulting average deflection function shows the deep inelastic rainbow observed experimentally. The rainbow angle moves from positive to negative angles with increasing bombarding energy. Good agreement is obtained for the average final kinetic energy as a function of angle. The calculated Z distributions become broader as the excitation energy increases. The angular distributions for individual fragments show the characteristic disappearance of the side peaking and the development of forward peaking as the distance in Z from the projectile increases. The calculated Z angular and ..gamma..-ray multiplicity distributions are successfully compared with the experimental data. 
536 |b W-7405-ENG-48. 
650 7 |a Heavy Ion Reactions.  |2 local. 
650 7 |a Lepton-hadron Interactions.  |2 local. 
650 7 |a Scattering.  |2 local. 
650 7 |a Electromagnetic Radiation.  |2 local. 
650 7 |a Lepton-nucleon Interactions.  |2 local. 
650 7 |a Charged-particle Reactions.  |2 local. 
650 7 |a Angular Distribution.  |2 local. 
650 7 |a Gamma Radiation.  |2 local. 
650 7 |a Targets.  |2 local. 
650 7 |a Tantalum 181 Target.  |2 local. 
650 7 |a Multiplicity.  |2 local. 
650 7 |a Kinetic Energy.  |2 local. 
650 7 |a Ionizing Radiations.  |2 local. 
650 7 |a Nuclear Reactions.  |2 local. 
650 7 |a Particle Interactions.  |2 local. 
650 7 |a Interactions.  |2 local. 
650 7 |a Lepton-baryon Interactions.  |2 local. 
650 7 |a Deep Inelastic Scattering.  |2 local. 
650 7 |a Diffusion.  |2 local. 
650 7 |a Asymmetry.  |2 local. 
650 7 |a Radiations.  |2 local. 
650 7 |a Gold 197 Target.  |2 local. 
650 7 |a Energy.  |2 local. 
650 7 |a Krypton 86 Reactions.  |2 local. 
650 7 |a Distribution.  |2 local. 
650 7 |a Mass.  |2 local. 
650 7 |a Inelastic Scattering.  |2 local. 
650 7 |a Nuclear Physics And Radiation Physics.  |2 edbsc. 
710 2 |a Lawrence Berkeley Laboratory.  |4 res. 
710 2 |a Lawrence Berkeley National Laboratory.  |4 res. 
710 1 |a United States.  |b Department of Energy.  |b Office of Scientific and Technical Information.  |4 dst. 
856 4 0 |u http://www.osti.gov/servlets/purl/5440427-LE9kRm/  |z Online Access 
907 |a .b72098193  |b 03-07-23  |c 11-08-12 
998 |a web  |b 11-08-12  |c f  |d m   |e p  |f eng  |g cau  |h 0  |i 1 
956 |a Information bridge 
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952 f f |p Can circulate  |a University of Colorado Boulder  |b Online  |c Online  |d Online  |e E 1.99: conf-770968-1  |h Superintendent of Documents classification  |i web  |n 1