Title: Topological Structure of Dense Hadronic Matter
1Topological StructureofDense Hadronic Matter
October, 2004 Seoul
V. Vento Universitat de València
Colaborators Heejung Lee (Universitat de
València), Byung-Yung Park (Chungnam Natl
Univ.), Dong-Pil Min (Seoul Natl Univ.)
and Mannque Rho(Saclay Hanyang)
2- Introduction
- Dense Skyrmion Matter
- Pions in Dense Skyrmion Matter
- Sliding Vaccua
- Vector Mesons
- Ongoing work
- Concluding remarks
31. Introduction
4(No Transcript)
5QCD
Effective Theory
Observation
6Quantum Chromo-Dynamics
Effective Theory at zero Temp./Density
Effective Theory at finite Temp./Density
7Skyrmes Old Idea
1960, T. H. R. Skyrme
8Skyrmes Old Idea
1960, T. H. R. Skyrme
92. Dense Skyrmion Matter
B.-Y. Park, D.-P. Min, M. Rho, V. Vento, Nucl.
Phys. A707 (2002) 381
10Two Skyrmions
1960, T. H. R. Skyrme
Product Ansatz
11Toroidal B2 Skyrmion
1988, Braaten Carson, 1995, Leese,
Manton Schroers
12Multi-Skyrmion System
http//www.damtp.cam.ac.uk/user/hep/research.html
solitons
13Simple Cubic Skyrmion Crystal
1985, I. Klebanov
U(xLC,y,z) ty U(x,y,z) ty
(E/B)min1.078 at LC5.56
14Half-Skyrmion Crystal
1987, A. S. Goldhaber N. S. Manton
U(xLC,y,z) tyU(x,y,z)ty
additional symmetry
(E/B)min1.076 at LC5.56
15FCC Skyrmion Crystal
1989, L. Castillejo et al. M. Kugler et al.
Y
16Half-Skyrmion CC
Y
Y
z
x
z
y
o
y
LF
X
X
z
z
x
(E/B)min1.038 at Lf4.72
17E/B vs. LF
18lttr(U)gt
193. Pions in Dense Skyrmion Matter
H.-J. Lee, B.-Y. Park, D.-P. Min, M. Rho, V.
Vento, Nucl. Phys. A723 (2003) 427 Nucl. Phys.
A741 (2004) 161
20Chiral Symmetry Restoration
21GellMann-Oakes-Renner Relation
22GellMann-Oakes-Renner Relation
23Brown-Rho scaling
24Deeply Bound Pionic States
Yamazaki et al., 1998
25Skyrme Model(mp0)
\
26p dynamics(r0)
\
p-skyrmion matter interactions
27(No Transcript)
28(No Transcript)
29p dynamics(r0)
\
Wavefunction renormalization constant Z-1
30Pion effective mass
31Pion velocity in medium
32Pseudogap?
p
fp
s
U still remains on the Chiral Circle But ltUgt0
Zarembo, hep-ph/0104305
33Zarembo, hep-ph/0104305
344. Sliding Vacuua
H.-J. Lee, B.-Y. Park, M. Rho, V. Vento, Nucl.
Phys. A723 (2003) 427
35Skyrme Lagrangian
Ellis Lanik, PLB(1985) Brown-Rho scaling,
PRL(1992)
mc 720 MeV, fc240 MeV
36Vacuum (r0) U1 cfc
37Naive Estimate
E/BM2(L)C2M4(L) Mm(L) C3V(C)
38E/B
39(No Transcript)
40In-medium quantities
41Without c
42In-medium pion velocity
435. Vector Mesons
B.-Y. Park, M. Rho, V. Vento, Nucl. Phys. A736
(2004) 129
44Hidden Local Gauge Symmetry
Vector Meson Dominance
45pions, chi, rho and omega
Bando, Kugo, Yamawaki, Phys. Rep. (1988)
46E/B without Omega
47E/B with Omega
48E/B
49ltsgt ltcgt without Omega
50ltsgt ltcgt with Omega
516. Ongoing work
52Skyrmion from Instanton
1989, M. F. Atiyah N. S.Manton
Introduce variables describing the single
skyrmion dynamics
53time component of SU(2) gauge potential for the
instanton field of charge N
time-ordering
constant matrix to make U approach 1 at infinity
constant rotation matrix
54E/B vs. LF
55(No Transcript)
56(No Transcript)
577. Concluding remarks
58The skyrmions role in dense matter
59(No Transcript)
60Skyrme model
- Universal theory of baryons and mesons
- Nuclei and meson fluctuations
- Nuclear matter and mesons in the medium
- .. Nuclear physicists dream!
- Caveats
- Still very primitive! Crystal structures which
- should be Fermi liquids? Quantum effects!
- Approach to QCD