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APFB2011 August 25, Seoul. B=2 system in chiral soliton model. Byung-Yoon Park (Chungnam National University, Korea) V. Vento (Universidad de Valencia, Espa ña ) V. Mantovani, A. Drago (Università di Ferrara, Italia). Outline. Motivation Chiral soliton model B=2 system Discussion.
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APFB2011 August 25, Seoul B=2 systemin chiral soliton model Byung-Yoon Park (Chungnam National University, Korea) V. Vento (Universidad de Valencia, España) V. Mantovani, A. Drago (Università di Ferrara, Italia)
Outline • Motivation • Chiral soliton model • B=2 system • Discussion
Skyrmemodelfor Finite Density & Temperature B.-Y. Park & V. Vento, Multifaceted Skyrmion, 2010
Non-Topological Soliton Model Friedberg & Lee, 1977
Quark Energy Band Phys. Rev. C 36(1987)
z 0 0 z 0 0 x y y x 0 0 y z 0 0 x
No study on B=2 system ! & ?
Toroidal B=2 skyrmion 1988, Braaten & Carson, 1995, Leese, Manton & Schroers
Multi-Skyrmion system Rational Map Ansatz 1997 Houghton, Manton, Sutcliffe B=2 Torus B=3 Tetrahedron B=4 Cube B=5 with Dd2 sym B=6 with Dd4 sym B=7 Dodecahedron
Multi-Skyrmion system (continued) B=8 with Dd6 sym. B=9 Tetrahedron B=17 Bucky Ball B=5 Octahedron B=11 Icosahedron
Multi-skyrmion System (continued) Fullerine Structures 2001 Battye, Sutcliffe
Configuration A V Vq Vp VU Vs
Configuration B Vq V VU Vs Vp
Configuration C Vq V VU Vs Vp
Inter-soliton potential energy VB VA VC
Summary • We have obtained an approximated solutions to B=2 system in the model. • They can be used - in searching the better solutions for the studies of the nuclear force, - in constructing the dense system.
Future Work • Baryon-Baryon Interaction • Multi-Baryon Systems • Baryonic Matter