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2 Probing Non-Perturbative QCD with
Antiprotons The PANDA Experiment at FAIR
- Introduction Why is QCD so much fun?
- The Physics Glue and Charm
- The Facility FAIR
- Accelerator and Antiproton Cooler Ring
- Detector PANDA
- Summary and Outlook
3Physics with Panda
Charmed hadrons in the nuclear medium
CP-violation (D/? - sector)
inverted deeply virtual Compton scattering
4QCD In Principle Simple ?
- Contains Self coupling of Gluons
- Coupling of Quarks to the Gluon fields
- Small coupling perturbative QCD
- Large coupling
- Lattice QCD
- Field theories with effective degrees of freedom
5Running Coupling Constant
perturbative
strong
QCD
Of particular interest Transition from the
quark-gluon to the hadronic degrees of freedom
6Physics with Panda
Charmed hadrons in the nuclear medium
CP-violation (D/? - sector)
inverted deeply virtual Compton scattering
7Bound States of QCD
8Flux Tubes and Hybrids
Simplified Lattice Approach
- Excitation of Flux Tube
- Additional angular momentum
- New (exotic) quantum numbers
Bali, 1991
Hybrid
9Charmonium Hybrids
Excited gluon flux
- Predicted by bag models, flux tube models,
constituent gluon models and LQCD. - Three of the lowest lying c?c hybrids have exotic
JPC (0-,1-,2-) - ? no mixing with nearby c?c states
- Mass 4.2 4.5 GeV/c2.
- Charmonium hybrids expected to be much narrower
than light hybrids (open charm decays
suppressed). - Cross sections for formation and production of
charmonium hybrids similar to normal c?c states - ( 100 150 pb).
CLEO
One-gluon exchange
10Charmonium Hybrids
- Annihilation is a gluon rich process
- creates gluonic excitation in a direct way
- 2 complementary techniques
- Production(Fixed-Momentum)
- Formation(Broad- and Fine-Scans)
- Momentum range for a survey
- p 15 GeV
11Bound States of QCD
12Heavy Glueballs
2- 0-
- For light gg/ggg-systems
- unique identification difficult (mixing!)
- Exotic heavy glueballs
- m(0-) 4140(50)(200) MeV
- m(2-) 4740(70)(230) MeV
- Flavor-blindness
- decay into charmed final
- states possible
Morningstar,Peardon, PRD60(1999)34509 Morningstar,
Peardon, PRD56(1997)4043
13Physics with Panda
Charmed hadrons in the nuclear medium
CP-violation (D/? - sector)
inverted deeply virtual Compton scattering
14Charmonium Positronium of QCD
Mass MeV
Binding energy meV
4100
y
(4040)
Ionization energy
P
( 3940)
3
2
0
3900
D
3
P
( 3880)
( 3800)
3
3
S
3
3
D
3
S
3
1
3
3
D
1
1
2
0
1
2
D
P
( 3800)
3
D
3
1
3
-1000
1
y
(3770)
D
2
0
2
P
3
3
D
3
2
P
3
D
1
2
3
2
2
S
3
2
S
2
1
1
1
2
P
1
3
Threshold
y
(3686)
600 meV
0
3700
1
2
P
3
0
h
(3590)
10-4 eV
c
-3000
c
(3556)
2
h
(3525)
c
c
(3510)
1
3500
c
(3415)
0
-5000
3300
1
S
3
810-4 eV
1
1
S
1
0
-7000
y
(3097)
3100
0.1 nm
-
e
e
C
1 fm
h
(2980)
C
c
2900
15Charmonium Physics
Open questions
?(33S1)
DD
?c2(23P2)
?(13D3)
pp GeV/c
Mcc GeV/c2
?c(31S0)
?c1(23P1)
Peculiar ?(4040)
?(13D2)
DD
h1c(21P1)
?c0(23P0)
?(11D2)
?(13D1)
DD
Terra incognita for 2P and 1D-States
?(23S1)
?c(21S0)
?c2(13P2)
h1c(11P1)
?c1(13P1)
?c - ?(2S) splitting
?c0(13P0)
h1c unconfirmed
J/?(13S1)
?c inconsistencies
?c(11S0)
16Advantage of Antiprotons
- ee- annihilation via
- virtual photon only
- states with JPC 1--
- Mass resolution is only limited by the beam
momentum resolution
17Recent discoveries hc (21S0) , X(3872)
- Discovery of the ?c(21S0) by
- Belle (BaBar, CLEO).
- Discovery of a new narrow
- state above DD threshold
- X(3872) at Belle ( CDF,
- D0, BaBar).
M(??c) 3637.7 ? 4.4 MeV/c2
_
M 3872.0 ? 0.6 ? 0.5 MeV/c2 ?? 2.3 MeV (90
C.L.)
18Physics with Panda
Charmed hadrons in the nuclear medium
CP-violation (D/? - sector)
inverted deeply virtual Compton scattering
19Hadrons in Nuclear Matter
- Currently at GSI
- many experiments devoted to the study of hadrons
in nuclei and hadronic matter - in-medium modifications of hadron properties
- KAOS, deeply bound pionic atoms, HADES
- hadrons with light quarks (u,d,s)
20How about Charm ?
- Mass splitting for D mesons expected !
- Probes
- Measure excitation functions for D production on
Nuclei with antiproton beam - Modification of the width of Charmonium states
near the D threshold
21D Mesons in Nuclear Matter
- Excitation functions Width of
Charmonium States
22Charmonium in Nuclear Matter Observables
Predicted rates at L 1032 cm-2s-1 few 10
few 100 events/day S.H. Lee,
nucl-th/0310080
23J/y Absorption in Nuclei
24Physics SummaryQCD Systems to be Studied with
PANDA
25The FAIR Facility (was GSI)
26HESR High Energy Storage Ring
27The PANDA Detector Top View
Length 2 m upstream, 10 m downstream
28Proposed Detector (Overview)
- High Rates
- Total s 55 mb
- Vertexing
- (sp,KS,?,)
- Charged particle ID
- (e,µ,p,p,)
- Magnetic tracking
- Elm. Calorimetry
- (?,p0,?)
- Forward capabilities
- (leading particles)
- Sophisticated Trigger(s)
29Participating Institutes(with Representative in
the Coordination Board)
45 Institutes from 12 Countries
- U Basel
- IHEP Beijing
- U Bochum
- U Bonn
- U INFN Brescia
- U INFN Catania
- U Cracow
- GSI Darmstadt
- TU Dresden
- JINR Dubna (LIT,LPP,VBLHE)
- U Edinburgh
- U Erlangen
- NWU Evanston
- U INFN Ferrara
- U Pavia
- IHEP Protvino
- PNPI Gatchina
- U of Silesia
- U Stockholm
- KTH Stockholm
- U INFN Torino
- Politechnico di Torino
- U Oriente, Torino
- U INFN Trieste
- U Tübingen
- U TSL Uppsala
- IMEP Vienna
- SINS Warsaw
- U Warsaw
- U Frankfurt
- LNF-INFN Frascati
- U INFN Genova
- U Glasgow
- U Gießen
- KVI Groningen
- IKP Jülich I II
- U Katowice
- IMP Lanzhou
- U Mainz
- U Politecnico INFN Milano
- U Minsk
- TU München
- U Münster
- BINP Novosibirsk
30Summary and Outlook
- The FAIR Project will include a dedicated
antiproton facility - World-class research covering the many facets of
non-perturbative QCD - Additional benefits
- Continuation of the ongoing GSI program
investigating hadrons in dense matter - Measurement of hadronic interaction cross section
CRUCIAL for the interpretation of QGP signals - (J/y suppression)
- The future beyond the future
- Direct CP violation in the Charm sector
- Gravitation experiments with ultra-cold anti
hydrogen - CERN AD program with 100 times increased
intensity and unprecedented beam quality!