Mesonic and dibaryonic excitations in the. pi. NN system [electronic resource]
A ..pi..NN theory, incorporating mesonic and dibaryonic excitation mechanisms, is introduced to give a unified description of NN and ..pi..d reactions. The mesonic mechanism is built into the theory along the line of the Paris potential. The dibaryonic excitation at short distance is introduced acco...
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Format: | Government Document Electronic eBook |
Language: | English |
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Argonne, Ill. : Oak Ridge, Tenn. :
Argonne National Lab ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,
1984.
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Subjects: |
MARC
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245 | 0 | 0 | |a Mesonic and dibaryonic excitations in the. pi. NN system |h [electronic resource] |
260 | |a Argonne, Ill. : |b Argonne National Lab ; |a Oak Ridge, Tenn. : |b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, |c 1984. | ||
300 | |a Pages: 17 : |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 01/01/1984. | ||
500 | |a "conf-840784-2" | ||
500 | |a "DE84016318" | ||
500 | |a Nucleon and nuclear structure and exclusive electromagnetic reaction studies workshop, Cambridge, MA, USA, 23 Jul 1984. | ||
500 | |a Lee, T.S.H. | ||
520 | 3 | |a A ..pi..NN theory, incorporating mesonic and dibaryonic excitation mechanisms, is introduced to give a unified description of NN and ..pi..d reactions. The mesonic mechanism is built into the theory along the line of the Paris potential. The dibaryonic excitation at short distance is introduced according to current understanding of six quark dynamics. The effect of the 2⁺, T = 1 six-quark state on NN and ..pi..d scattering is presented. The implication of the theory in the study of electromagnetic interaction with deuteron is discussed. 11 references. | |
536 | |b W-31-109-ENG-38. | ||
650 | 7 | |a Phase Shift. |2 local. | |
650 | 7 | |a Elementary Particles. |2 local. | |
650 | 7 | |a Extended Particle Model. |2 local. | |
650 | 7 | |a Mathematical Models. |2 local. | |
650 | 7 | |a Peripheral Models. |2 local. | |
650 | 7 | |a Potentials. |2 local. | |
650 | 7 | |a Dibaryon Resonances. |2 local. | |
650 | 7 | |a Nucleon-nucleon Potential. |2 local. | |
650 | 7 | |a Nuclear Forces. |2 local. | |
650 | 7 | |a Mesons. |2 local. | |
650 | 7 | |a Baryons. |2 local. | |
650 | 7 | |a Postulated Particles. |2 local. | |
650 | 7 | |a Fermions. |2 local. | |
650 | 7 | |a Meson-baryon Interactions. |2 local. | |
650 | 7 | |a Pions. |2 local. | |
650 | 7 | |a Nucleon-nucleon Interactions. |2 local. | |
650 | 7 | |a Baryon-baryon Interactions. |2 local. | |
650 | 7 | |a Baryon Resonances. |2 local. | |
650 | 7 | |a Bosons. |2 local. | |
650 | 7 | |a Bag Model. |2 local. | |
650 | 7 | |a Boson-exchange Models. |2 local. | |
650 | 7 | |a Particle Interactions. |2 local. | |
650 | 7 | |a Obe Model. |2 local. | |
650 | 7 | |a Isobar Model. |2 local. | |
650 | 7 | |a Interactions. |2 local. | |
650 | 7 | |a Resonance Particles. |2 local. | |
650 | 7 | |a Pion-deuteron Interactions. |2 local. | |
650 | 7 | |a N Resonances. |2 local. | |
650 | 7 | |a Ope Model. |2 local. | |
650 | 7 | |a Delta-1236 Resonances. |2 local. | |
650 | 7 | |a Hadrons. |2 local. | |
650 | 7 | |a Quarks. |2 local. | |
650 | 7 | |a Pseudoscalar Mesons. |2 local. | |
650 | 7 | |a Composite Models. |2 local. | |
650 | 7 | |a Quark Model. |2 local. | |
650 | 7 | |a Hadron-hadron Interactions. |2 local. | |
650 | 7 | |a Particle Models. |2 local. | |
650 | 7 | |a Nuclear Physics And Radiation Physics. |2 edbsc. | |
710 | 2 | |a Argonne National Laboratory. |4 res. | |
710 | 1 | |a United States. |b Department of Energy. |b Office of Scientific and Technical Information. |4 dst. | |
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