the physics of high baryon densities
DESCRIPTION
and not so high. The Physics of high baryon densities. Probing the QCD phase diagram The critical end point Properties of mesons in matter Baryon density vs. temperature Probing cold dense matter Conclusions. B. Friman, GSI. Critical endpoint. C o l o u r superconductor. - PowerPoint PPT PresentationTRANSCRIPT
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The Physics of high baryondensities
• Probing the QCD phase diagram• The critical end point• Properties of mesons in matter
– Baryon density vs. temperature
• Probing cold dense matter• Conclusions
and not so high
B. Friman, GSI
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The QCD phase diagram
T
B
Hadronicmatter
Critical endpoint
Quark-Gluon Plasma
Nuclei
Chiral symmetrybroken
Chiral symmetryrestored
Baryondominated
Mesondominated
Colour superconductor
Neutron stars
Earl
y u
niv
ers
e
Neutron stars:-low T-high B
-strangeness-quark matter (CSC ?)
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T
B
RHIC
LHC
SPS
AGS
SIS
Critical endpoint
Quark-Gluon Plasma
Colour superconductor
Nuclei
High, low andintermediate energies
Need:
Different reactionsAB, pA, A..
Chiral symmetrybroken
Chiral symmetryrestored
The QCD phase diagram
Hadronicmatter
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The critical end point
Fodor & Katz:Tc 160 MeV, B
c 720 MeV
Fodor-Katz
Adiabatic extrapolation tofreeze-out curve: E ~ 10 AGeV
Critical point expected to moveto smaller B for realistic mq
Ejiri et al.
Ejiri et al. (Bielefeld-Swansea):B
c 420 MeVE 40 AGeV
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So far no convincing experimental evidence for the nuclear matter gas-liquid critical point
Signatures of the critical end point?
Critical point: fluctuations ofthe order parameter are soft
Ejiri et al.
Look for rise and fall of fluctuations! (E-by-E)(Stephanov, Rajagopal, Shuryak)
E-by-E fluctuations of:•transverse momentum (SRS)•pion multiplicity (SRS)•proton number (Hatta, Stephanov) . . . . .
Take care of finite time and finite size effects (Berdnikov, Rajagopal)
Exciting prospects, but still many unknowns!
Quark number susceptibility
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Effects of baryon density
Mass splittings becausecharge conjugation symmetry broken at nB 0
|K+> = |us>
|K-> = |su>
K+ K- K+
K-~100 MeV
0
500
0
1800
Mass
Overall attraction dueto scalar interaction:KN sigma term
Mass splitting dueto vector interaction:Weinberg-Tomozawa
Easier to produce K- in dense matter
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Kaon production near threshold
Ni+Ni (1.93 GeV)
Enhancement of K-
KaoS & FOPI @ GSI
Repulsive potential
Suppression of K+
Attractive potential
Calculation:Cassing & Bratkovskaya
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|D-> = |dc>
|D+> = |cd>
K+ K- K+
K-~100 MeV
0
D+ D-
500
0
1800
Mass
D-
D+
~50 MeV
Effects of baryon density (2)
Explore D-meson properties in dense matter at energies around charm threshold E 10-20 AGeV
D-Meson mass splittingat nB 0
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D-mesons:•heavy-light system•hydrogen atom of QCD
cu
Light-quark-cloudprobes chiral symmetry
Chiral partners of D-mesons?
D(1869)
D*(2010)
cu-system
~1/mQ
0-
1-
Heavy-quark-symmetry
(0+)(1+)
Belle(2003)
~Mq
D(2308)
D(2427)
Chiral mass shifts 420 MeV(constituent quark mass)
D(0+) D(0-) +
cs-system
Ds(1969)
(0+)
(1+)
BaBar (2003)CLEO(2003)
Chiral mass shifts 350 MeV
Ds*(2112)
Ds(2317)
0-
1-
Ds(2463)
cs
Ds(0+) D(0-) + K
Ds(0+) Ds(0
-) + /+ chiral symmetry:
chiral doubling of D-mesons (Nowak-Rho-Zahed and Bardeen-Hill, 92-93)
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Restoration of Chiral Symmetry
at non-zero baryon density and temperature
Role of chiral symmetry for hadron masses?
Explore dependence of hadron propertieson quark condensate
Chiral partners become degenerate
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D mesons in matter
If chiral doubling scenario for D mesons correct
then m(0+)-m(0-) 0 etc.
as qq 0 (chiral limit)
Harada, Rho, Sasaki (2003)
D-meson production in nuclear collisions offer a unique opportunity to explore chiral dynamics in dense matter
m(0
+)-
m(0
- )
0qq0qq
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Beyond mean-field approximation
Spectral functions change due to interactions
Nh
Nf ...)1(4)( NhN
N
hNh f
m
m
Low-density expansion:
Resonances in scattering amplitude:peaks in spectral function
M.LutzG.WolfB.F.
N N
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Baryon density vs. temperature
Baryon dominated matter: meson spectral functions determined by baryon resonances
Meson dominated matter: meson spectral functions determined by meson resonances
Resonances smeared by collision broadening
These effects must be unfolded before one can drawconclusions on chiral symmetry and masses
R.Rapp
Need high resolution, high statistics data at a wide range of energies (T vs. B)
Meson mixing at B 0
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Rise: threshold dynamics
Decrease: B 0
K = B/3 - S
= 2 B/3 + S
Strangeness and baryon density
Braun-Munzinger,Cleymans,Oeschler and Redlich
No peak for B = 0!
Wroblewski factor:
Peak ~ 30 AGeV
Sharp maximum in
K+/+
Not understood!
AGSNA49RHIC
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Probing cold dense matter in nuclei
Complementary information from
p A, p A, A, A …
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Photo induced ω production
Simulation by Meschendorp et al.
Measured at ELSA by TAPS collaboration
Data analysis in progress
+ A + X
0
Assume at = 0:m 660 MeV, 60 MeV
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Summary
•Critical endpoint: fluctuations
•Light-heavy mesons: mass splitting
•Chiral partners become degenerate•New D mesons
•Data at different energies/different B/Tuseful for unraveling meson/baryon resonances, meson mixing etc.
•pA, A, A etc. provide complementary information
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Most of them can be explored at the GSI Future Facility
Protons E 90 GeVHeavy ions (N=Z) E 45 AGeVPb E 35 AGeVStored antiprotons E 15 GeV
Some of these issues are being addressed at CERN SPS.
Comprehensive heavy-ion program with strangeness, charm, lepton pairs and photons