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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. - PowerPoint PPT Presentation
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B=2 system in chiral soliton model
Byung-Yoon Park(Chungnam National University, Korea)
V. Vento(Universidad de Valencia, España )
V. Mantovani, A. Drago(Università di Ferrara, Italia)
APFB2011August 25, Seoul
Outline
• Motivation• Chiral soliton model• B=2 system• Discussion
B=4
Skyrme model for 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)
No relative orientation!
y
z
x
y
z
0
x
0 0
0
0 0
00z
xy
No study on B=2 system
! & ?
Toroidal B=2 skyrmion1988, Braaten & Carson, 1995, Leese, Manton & Schroers
Multi-Skyrmion system
B=2 Torus B=3 Tetrahedron B=4 Cube
B=5 with Dd2 sym B=6 with Dd4 sym B=7 Dodecahedron
Rational Map Ansatz 1997 Houghton, Manton, Sutcliffe
Multi-Skyrmion system
B=8 with Dd6 sym. B=9 Tetrahedron B=17 Bucky Ball
B=5 Octahedron B=11 Icosahedron
(continued)
Multi-skyrmion System
(continued)
Fullerine Structures
2001 Battye, Sutcliffe
B=2 system in chiral soliton model
Model Lagrangian
Hedgehog Solution
B=1 hedgehog solution
Product Ansatz for B=2 system
Configuration A
VqV
V
VU
V
Configuration B
Vq
V
V
VU
V
Configuration C
VqV
V
VU
V
Inter-soliton potential energy
VA
VC
VB
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