half- skyrmion matter & quarkionic matter
DESCRIPTION
HIM-WCU workshop Hanyang U. Oct. 31 , 2009. Half- Skyrmion Matter & Quarkionic Matter. Byung -Yoon Park ( Chungnam Nat’l Univ.). Collaborators. M. Rho( Saclay , Hanyang Univ.) V. Vento(Valencia Univ.) D.-P. Min(Seoul National Univ.) H.-J. Lee( Chungbuk National Univ.). Contents. - PowerPoint PPT PresentationTRANSCRIPT
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Half-Skyrmion Matter&
Quarkionic Matter
HIM-WCU workshopHanyang U.
Oct. 31, 2009
Byung-Yoon Park(Chungnam Nat’l Univ.)
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Collaborators• M. Rho(Saclay, Hanyang Univ.)• V. Vento(Valencia Univ.)• D.-P. Min(Seoul National Univ.)• H.-J. Lee(Chungbuk National Univ.)
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Contents1.Skyrme Model ?2. Dense Skyrmion Matter3. Dense & Hot Skyrmion Matter4. Summary
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1. Skyrme Model?
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Skyrmion Model
U(x) : mapping from R3-{ }=S3 to SU(2)=S38
topological soliton
1960, T. H. R. Skyrme
R ~ 1 f m M ~ 1.5 GeV
BARYON ?
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proton neutron
1919 Rutherford1932 Chadwick
pionproton neutron
1935 Yukawa
Hadronic World(Skyrmionist’s Viewpoint)
pion
1960 Skyrme
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SU(2) Collective Coord. Quantiza-
tion N, DSU(3) collective
CoordinateQuatization N, S, X,
D, S*, X*,W
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N, S, X, D, S*, X*,W
Hedgehog Soliton
SU(2) collectiveCoordinateQuatization
bound kaon
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N, S, Xc, D, S*, X*,Wc
Hedgehog Soliton
SU(2) collectiveCoordinateQuatization
bound D,D*
c c
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Multi-Skyrmion system
B=2 Torus B=3 Tetrahedron B=4 Cube
B=5 with Dd2 symB=6 with Dd4 symB=7 Dodecahedron
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Toroidal B=2 skyrmion1988, Braaten & Carson,
1995, Leese, Manton & Schroers
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2. Dense Skyrmion Matter
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2. Dense Skyrmion matter
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Two skyrmions in the most attractive configuration.
2. Dense Skyrmion matter
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1985, I. Klebanov
(E/B)min=1.078 at LC=5.56
Simple Cubic Skyrmion Crys-tal
U(x+LC,y,z) =ty U(x,y,z) ty
y
Y
z
x z
xx
x
Xy
LC
o
2. Dense Skyrmion matter
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Half-Skyrmion Crystal
U(x+LC,y,z) =tyU(x,y,z)ty
1987, A. S. Goldhaber & N. S. Manton
+ additional Symmetry
w.r.t.s -s
(E/B)min=1.076 at LC=5.56
y
z x
X
LC
s=-1s=+1(Lb/2 above)
0
2. Dense Skyrmion matter
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U = exp(i F(r)t r ) ^.
Half-skyrmion?
F (r )
r
pU =-1
2. Dense Skyrmion matter
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U =-1 U =-1U =+1
2. Dense Skyrmion matter
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U =-1 U =-1U =+1
2. Dense Skyrmion matter
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B=4 skyrmion
2. Dense Skyrmion matter
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1989, L. Castellejo et al. & M. Kulger et al.
y
Y
x
x
Xy
z=LF/2 plane
Y
o
z
z z
X
z
LF
z=0 plane
FCC Skyrmion Crystal
2. Dense Skyrmion matter
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Y
X
(E/B)min=1.038 at Lf=4.72
o
z
Y
z z
X
z
LF y
x
x
y
Half-Skyrmion CC
2. Dense Skyrmion matter
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E/B vs. LF
2. Dense Skyrmion matter
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<U>=<s>
Chiral symmetryrestoration
in dense matter?
2. Dense Skyrmion matter
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static soliton config.fluctuating
pions
Pion in the dense baryonic matter?
classicaldense matter
config.
2. Dense Skyrmion matter
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Skyrme Model(mp=0)\
Pion fluctuation in rB=0 spaceVacuum : U=1
2. Dense Skyrmion matter
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p dynamics(r=0)\
+ p-skyrmion matterinteractions
Skyrmion matter
Pion fluctuations on top of the
skyrmion matter
2. Dense Skyrmion matter
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p dynamics(r=0)\
2. Dense Skyrmion matter
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p dynamics(r=0)\
2. Dense Skyrmion matter
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p dynamics(r=0)\
In-Medium pion decay constant ?
In-Medium pion mass ?
2. Dense Skyrmion matter
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pion effective mass
H.-J. Lee, B.-Y. Park, D.-P. Min, M. Rho, V. Vento, Nucl. Phys. A (2003)
!
2. Dense Skyrmion matter
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fps
pPseudogap?
Zarembo, hep-ph/0104305
U still remains on the Chiral Circle
But <U>=0 Chiral Symmetry Restoration
2. Dense Skyrmion matter
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Skyrme Lagrangian
Trace Anomalyof QCD
2. Dense Skyrmion matter
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Skyrme LagrangianEllis & Lanik, PLB(1985)
Brown-Rho scaling, PRL(1992)
mc ~ 720 MeV, fc~240 MeV2. Dense Skyrmion matter
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fc c
V(c)
Vacuum (r=0)U=1 c=fc
fps
p
<c>
U cU
<U>
2. Dense Skyrmion matter
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Naive Estimation
E/B=M2(L)c2+M4(L) +Mm(L) c3+V(c)L3
2. Dense Skyrmion matter
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Naive Estimation
2. Dense Skyrmion matter
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E/B
<c>=0 phase
Chiral phase transition
<c>=0 phase/
2. Dense Skyrmion matter
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<c> & <U>
<s><c>
PseudogapPhase?
cS Phase
cSB Phase
mp=0
2. Dense Skyrmion matter
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p
Pseudogap still re-mains?
fp
s fp
s
s
*
*
cSB Phase
Pseudo-gap
PhasecS
Phase
p
p
2. Dense Skyrmion matter
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3. Hot & Dense Skyrmion Matter
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?
2. Hot & Dense Skyrmion matter
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Skyrmion Soup
Condiments : dilaton vector mesons Heat
Main ingredients : pions
B.-Y. Park, H.-J. Lee, V. Vento, Phys. Rev. D80 (2009)
2. Hot & Dense Skyrme matter
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Skyrmion from Instan-ton1989, M. F. Atiyah & N. S. Manton
time component of SU(2) gauge potential for the instanton field of charge N
time-ordering
constant matrix to make U approaches 1 at infinity
constant rotation matrix2. Hot & Dense Skyrmion matter
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E/B vs. LF
2. Hot & Dense Skyrmion matter
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B.-Y. Park, D.-P. Min, V. Vento & M. Rho, Nucl. Phys. A707(2002) 381
2. Hot & Dense Skyrmion matter
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B.-Y. Park, D.-P. Min, V. Vento & M. Rho, Nucl. Phys. A707(2002) 381
2. Hot & Dense Skyrmion matter
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2. Hot & Dense Skyrmion matter
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Pion Gas!
P = T4p2
30 E/B = 3PV
E/B=(M2(r)+3PV)c2+M4(r) +V(c)/r 1/3
2. Hot & Dense Skyrmion matter
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Conclusion
2. Hot & Dense Skyrmion matter
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SummarySkyrme Model can be applied to
study (1) dense hadronic matter (2) hadron properties in dense matter
4. Summary
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Thank You!