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Charm Physics Charm Physics @@
Klaus PetersRuhr-Universität Bochum and GSI Darmstadt
Beijing, Jan 14, 2004
2
K. Peters - Charm Physics @ Panda
Where is Darmstadt ?
GSI
3
K. Peters - Charm Physics @ Panda
Overview
The Panda Physics Program Charmonium spectroscopy Charmed hybrids and glueballs Interaction of charmed particles with nuclei (Double) Hypernuclei Many further options
Detector Concepts for Panda
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K. Peters - Charm Physics @ Panda
The GSI Future Facility
Existing GSI Facilities
Hadron Physics
Plasma Physics
Condensed Baryonic Matter
Atomic PhysicsRare Isotope
Beams
5
K. Peters - Charm Physics @ Panda
The GSI Future Facility
Panda
6
K. Peters - Charm Physics @ Panda
The Antiproton Facility
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K. Peters - Charm Physics @ Panda
The Antiproton Facility
Antiproton production similar to CERN,
HESR = High Energy Storage RingProduction rate 107/secPbeam = 1.5 - 15 GeV/c
Nstored = 5 x 1010 p
Gas-Jet/Pellet/Wire Target
High luminosity modeLuminosity = 2 x 1032 cm-2s-1
p/p ~ 10-4 (stochastic cooling)
High resolution modep/p ~ 10-5 (electron cooling)Luminosity = 1031 cm-2s-1
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K. Peters - Charm Physics @ Panda
QCD running coupling constant
2Q
transition from perturbative to non-perturbative regime
Q2 [GeV2]10 1 0.1 0.05p
ert
urb
ati
ve Q
CD
con
sti
tuen
t q
uark
con
fin
em
en
t
meson
s a
nd
bary
on
s
0 0.1 0.3 1Rn r [fm]
Transition from the quark-gluon to the hadronic degrees of freedom
perturbative strong
QCD
9
K. Peters - Charm Physics @ Panda
Hybrid mixing
Glueball mixing
Level Mixing
Light quark problemthe mixing
Mixingbroad stateshigh level density
I=1 I=0nn I=0ss I=½
a1 f1 f1’ K1B
b1 h1 h1’ K1A
JPC=JP+
JPC=JP-
Kaon mixingstrong interaction C undefined K1A-K1B
Isoscalar mixingstrong interaction IG, JPC identical η-η‘
Isospin mixingelm interaction ΔI=1 ρ-ω
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K. Peters - Charm Physics @ Panda
Level Mixing
Light quark problemthe mixing
Mixingbroad stateshigh level density
Better:narrow states
and/or lower level densitycharmed systems !
Ex
oti
c lig
ht
Ex
oti
c cc
1 - - 1 - +
0 2 0 0 0 4 0 0 0M e V / c2
10 - 2
1
1 0 2
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K. Peters - Charm Physics @ Panda
Charmonium Physics
DD
DD*
ψ(11D2)
ψ(13D2)
ψ(13D3)
ψ(13D1)
Mcc
[G
eV
/c2]
ηc(11S0)
ηc(21S0)
J/ψ(13S1)
χc0(13P0)
χc1(13P1)
χc2(13P2)
h1c(11P1)
2.9
3.0
3.1
3.2
3.3
3.4
3.5
3.6
3.7
3.8
3.9
4.0D*D*
ψ(33S1)
pp [G
eV
/c]
ψ(23S1)
χc0(23P0)
χc1(23P1)
χc2(23P2)
h1c(21P1)ηc(31S0)
3.4
4.1
4.8
5.5
6.3
7.1
8.0
JP=0- 1- 1+ (0,1,2)+ 2- (1,2,3)-
… Exclusive ChannelsHelicity violationG-Parity violationHigher Fock state contributions
Open questions …
ηc – inconsistencies
ηc’ - ψ(2S) splitting
h1c – unconfirmed
Peculiar ψ(4040)
Terra incognita for 2P and 1D-States
12
K. Peters - Charm Physics @ Panda
It is extremely important to identify as many missing states above the open charm threshold as possible and to confirm the ones for which we only have a weak evidence
This will require high-statisticssmall-step scans of the
entire energy region accessible at HESR @ GSI
Charmonium States above the DD threshold
13
K. Peters - Charm Physics @ Panda
3500 3520 MeV3510C
Ball
ev./
2 M
eV
100
ECM
Charmonium Physics
e+e- interactions:Only 1-- states are formedOther states only bysecondary decays moderate mass resolution
pp reactions:All states directly formedvery good mass resolution
CBallE835
1000
E 8
35
ev./
pb
c1
CBall, Edwards et al. PRL 48 (1982) 70
E835, Ambrogiani et al., PRD 62 (2000) 052002
e+e¡ ! Ã0
! ° Âc1;2! °° J =Ã
! °° e+e¡
p¹p ! Âc1;2! ° J =Ã
! °e+e¡
14
K. Peters - Charm Physics @ Panda
ECM
Resonance Scan
Measured Rate
Beam Profile
Resonance Cross Section
small and well controlled beam momentum spread
p/p is extremely important
15
K. Peters - Charm Physics @ Panda
Charmonium Physics with pp
Expect 1-2 fb-1 (like CLEO-C)pp (>5.5 GeV/c) J/ψ 107/dpp (>5.5 GeV/c) χc2 (J/ψγ 105/d
pp (>5.5 GeV/c) ηc´( 104/d|rec.?
Comparison of PANDA@HESR to E835charged tracks detector with magnetic field 15 GeV/c maximum mom. instead of 9 GeV/c10x higher Luminosity than achieved before 10x smaller δp/pstable conditions dedicated high energy storage ring
16
K. Peters - Charm Physics @ Panda
Charmed Hybrids
LQCD: gluonic excitations of the quark-antiquark-potential may lead to bound states-potential
for one-gluon exchange-potential
from excited gluon flux
mHcc ~ 4.2-4.5 GeV/c2
Light charmed hybridscould be narrow if open charm decays are inaccessible or suppressed
important <r2> and rBreakup
3
3.5
4
1 2
R/r0
V(R)/GeV
J/ψ
χc
ψ‘
Hcc
DD
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K. Peters - Charm Physics @ Panda
S1
S2
S=S1+S2
J=L+S
P=(-1)L+1
C=(-1)L+S
L
Simplest Hybrids
S-Wave+Gluon (qq)8g with ()8=coloured
1S0 3S1 combined with a 1+ or 1- gluon
Gluon 1– (TM) 1+(TE)
1S0, 0–+ 1++ 1––
3S1, 1–– 0+- 0–+
1+- 1–+
2+- 2–+Exotic JPC cannot! be formed by qq
18
K. Peters - Charm Physics @ Panda
Proton-Antiproton Annihilation
Production
all JPC available
Formation only selected JPC
p
p recoil
p
p
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K. Peters - Charm Physics @ Panda
Proton-Antiproton Annihilation
Gluon rich process creates gluonic excitation directlycc requires the quarks to annihilate (no rearrangement)yield comparable to charmonium productioneven at low momenta large exotic content has been proven
G
M
p
p
G
p
p
Production all JPC available
only selected JPC
p
p
H
Formation
nng
H
p
p ssg/ccg
M
p
p
H
nng
M
Hp
p
ssg/ccg
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K. Peters - Charm Physics @ Panda
0 2 4 6 8 12 1510
p Momentum [GeV/c]
Mass [GeV/c2]
Two bodythresholds
Molecules
GluonicExcitations
qq Mesons
1 2 3 4 5 6
Hybrids
Hybrids+Recoil
Glueball
Glueball+Recoil
ΛΛΣΣΞΞ
ΛcΛc
ΣcΣc
ΞcΞc
ΩcΩcΩΩ DDDsDs
qqqq ccqq
nng,ssg ccg
ggg,gg
light qqπ,ρ,ω,f2,K,K*
ccJ/ψ, ηc, χcJ
nng,ssg ccg
ggg
Accessible Charmed Hadrons at PANDA @ GSI
Other exotics with identical decay channels same region
conventionalcharmonium
exoticcharmonium
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K. Peters - Charm Physics @ Panda
Heavy Glueballs
Light gg/ggg-systems are
complicated to identify (mixing!)
Exotic heavy glueballsm(0+-) = 4140(50)(200) MeVm(2+-) = 4740(70)(230) MeV
Width unknown, but!nature invests more likely in mass than in momentumnewest proof: double cc yield in e+e-
Flavour-blindnesspredicts decays into charmed final states too
Same run period as hybridsIn addition: scan m>2 GeV/c2
Morningstar,Peardon, PRD60(1999)34509Morningstar,Peardon, PRD56(1997)4043
0+-
2+-
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K. Peters - Charm Physics @ Panda
Open charm discoveries
The DS± Spectrum |cs> +c.c. was not expected to reveal any
surprises, but chiral and heavy quark aspects meet
Potential model
Old measurements
New observations
0 1 0 1 2 3
Ds
Ds*DsJ*
(2317)
Ds1m [
GeV
/c2]
D0K
D*K
DsJ
(2458)
Ds2
JP
# 1267 53 Events in peak
Com
bin
ato
rial D
S*+
DS*+
(21
12
)
BABAR
DsJ*(2317)
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K. Peters - Charm Physics @ Panda
Ds[J][*]± Pairproduction in pp Annihilation
Associated Pair m/MeV/c2 JP Channel (+cc) Final State
Ds(1968.5) Ds (1968.5) 3937.0 0+,1-,2+,3-,4+ Ds+Ds
- 2K-2K++-
Ds (1968.5) Ds*(2112.4) 4080.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ Ds
+(Ds-) 2K-2K++-
Ds*(2112.4) Ds
*(2112.4) 4224.8 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds+)(Ds
-) 2K-2K++-
Ds (1968.5) DsJ*(2317.5) 4286.0 0-,1+,2-,3+,4- Ds
+(Ds-0) 2K-2K++-0
Ds (1968.5) DsJ(2458.5) 4427.0 0-,1-,1+,2-,2+,3-,3+,4-,4+ Ds+((Ds
-)0) 2K-2K++-0
Ds*(2112.4) DsJ
*(2317.5) 4429.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ (Ds+)(Ds
-0) 2K-2K++-0
Ds (1968.5) Ds1(2535.4) 4503.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ Ds+(D*-K0) 2K-K+KS+2-(0)
Ds (1968.5) DsJ*(2572.4) 4540.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ Ds
+(D0K-) 2K-2K++-(0)
Ds*(2112.4) DsJ(2458.5) 4570.9 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds
+)((Ds-)0) 2K-2K++-0
DsJ*(2317.5) DsJ
*(2317.5) 4635.0 0+,1-,2+,3-,4+ (Ds+0)(Ds
-0) 2K-2K++-20
Ds*(2112.4) Ds1(2535.4) 4647.9 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds
+)(D*-K0) 2K-K+KS+2-(0)
Ds*(2112.4) DsJ
*(2572.4) 4684.4 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds+)(D0K-) 2K-2K++-(0)
Ds (1968.5) D1*(2770) 4738.5 0-,1-,1+,2-,2+,3-,3+,4-,4+ Ds
+(Ds-+-) 2K-2K+2+2-
DsJ*(2317.5) DsJ(2458.5) 4776.0 0-,1-,1+,2-,2+,3-,3+,4-,4+ (Ds
+0)((Ds-)0) 2K-2K++-20
Ds (1968.5) D2(2870) 4838.5 0+,1-,1+,2-,2+,3-,3+,4-,4+ Ds+((Ds
-)+-) 2K-2K+2+2-
DsJ*(2317.5) Ds1(2535.4) 4852.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ (Ds
+0)(D*-K0) 2K-K+KS+2-(1-2)0
Ds*(2112.4) D1
*(2770) 4882.4 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds+)(Ds
-+-) 2K-2K+2+2-
DsJ*(2317.5) DsJ
*(2572.4) 4889.9 0-,1-,1+,2-,2+,3-,3+,4-,4+ (Ds+0)(D0K-) 2K-2K++-(1-2)0
DsJ(2458.5) DsJ(2458.5) 4917.0 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ ((Ds+)0)((Ds
-)0) 2K-2K++-20
Ds*(2112.4) D2(2870) 4982.4 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (Ds
+)((Ds-)+-) 2K-2K+2+2-
DsJ(2458.5) Ds1(2535.4) 4993.9 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ ((Ds+)0)(D*-K0) 2K-K+KS+2-(1-2)0
DsJ(2458.5) DsJ*(2572.4) 5030.9 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ ((Ds
+)0)(D0K-) 2K-2K++-(1-2)0
Ds1(2535.4) Ds1(2535.4) 5070.8 0-,0+,1-,1+,2-,2+,3-,3+,4-,4+ (D*+K0)(D*-K0) K-K+2KS2+2-(0-2)0
25
K. Peters - Charm Physics @ Panda
Charmonium mass shift in nuclear matter
Quantum
numbers
QCD
2nd Stark eff.
Potential
model
QCD
sum rules
Effects of
DD loop
ηc 0-+ –8 MeV [1] –5 MeV [4]
J/ψ 1-- –8 MeV [1] -10 MeV [3] –7 MeV [4] < 2 MeV [5]
c0,1,20,1,2++ -40 MeV [2] -60 MeV [2]
ψ(3686) 1-- -100 MeV [2] < 30 MeV [2]
ψ(3770) 1-- -140 MeV [2] < 30 MeV [2]
[1] Peskin, NPB 156(1979)365, Luke et al., PLB 288(1992)355
[2] Lee, nucl-th/0310080
[3] Brodsky et al, PRL 64(1990)1011
[4] Klingel, Kim, Lee, Morath, Weise, PRL 82(1999)3396
[5] Lee, Ko PRC 67(2003)038202
29
K. Peters - Charm Physics @ Panda
Further Experiments and Optional extensions
Hypernuclear physics 3rd dimension of nuclear chartFocus: Double Hypernuclei
Inverted DVCS - WACSMeasure dynamics of quarks and gluons in a hadronHandbag diagram – electromagnetic final states
Proton Formfactors at large Q2
s up to 25 GeV2/c4
D(S)-PhysicsSpectroscopy: Threshold productionBR and decay Dalitz plots with high statistics
CP-Violation in the D-Sector
30
K. Peters - Charm Physics @ Panda
Proposed Detector (Overview)
High RatesTotal σ ~ 55 mb
Vertexing(σp,KS,Λ,…)
Charged particle ID(e±,μ±,π±,p,…)
Magnetic tracking
Elm. Calorimetry(γ,π0,η)
Forward capabilities(leading particles)
Sophisticated Trigger(s)
31
K. Peters - Charm Physics @ Panda
32
K. Peters - Charm Physics @ Panda
Tracking: Straw Tube Tracker
Number of double layersSkew angle of dbl layers 1 and 15 Skew angle of dbl layers 2-14
150o
2o-3o
Straw tube wall thicknessWire thicknessGas
LengthDiameter of tubes in double layers 1-5, 6-10, and 11-15Number of straw tubes
26 mm20 mm90%He10%C4H10 150 cm4 mm6 mm8 mm8734
Transverse resolution sx,y
Longitudinal resolution sz
150 mm 1 mm
33
K. Peters - Charm Physics @ Panda
PID: DIRC (Cherenkov)
less space than aero gel costs of calorimeterno problems with field
BaBar@SLAC
34
K. Peters - Charm Physics @ Panda
Electromagnetic Calorimeter
Detector material PbWO4 (or BGO)
Photo sensors Avalanche Photo Diodes
Crystal size 35 x 35 x 150 mm3 (i.e 1.5 x 1.5 RM2 x 17 X0)
Energy resolution 1.54 % / E[GeV] + 0.3 % (PWO)
Time resolution 130 ps
Total number of crystals 7150
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K. Peters - Charm Physics @ Panda
Simulation on ppψ(3770)DD
using D±K±π±π±
backgroundsignal-to-background 1:O(107)background from DPM generator
plain reconstructionsignal-to-background 6:1
mass difference Δm=m2K4π-mK2π,a-mK2π,b
m=Δm+2mD,PDG
signal-to-background O(100):1
including Kalman fittingexpect another factor of 5
3.3 3.4 3.5 3.6 3.7 3.8 3.9 4 4.1 4.2 4.3
20406080
100120140160180
Mass from Δm (GeV/c2)3.3 3.4 3.5 3.6 3.7 3.8 3.9 4 4.1 4.2 4.3
1
10
102
counts
/hou
r/0.0
1 G
eV
Mass (GeV/c2)
36
K. Peters - Charm Physics @ Panda
Simulation on ppηcγγ
FermiLab E835|cosθ*|<0.25σ(ηcγγ) = 200 nb
signal-to-background 1:1
main background π0γ and π0π0
main cutsmissing mass squared <0.16 GeV2/c4
cosθγγ<-0.9999
signal-to-background(5.1±0.4):1
Mass (GeV/c2)
counts
/10k/0
.02 G
eV
2.8 2.9 30
20
40
60
80
100
120
140
160
180
37
K. Peters - Charm Physics @ Panda
Participating Institutes(with Representative in the Coordination Board)
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 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
45 Institutes from 12 Countries:
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
38
K. Peters - Charm Physics @ Panda
Press Release 16/2003, http://www.bmbf.de
05.02.2003
Bulmahn gives green light for large-scale research equipment "We are securing an international top position for German basic research"
...Basic research in the natural sciences has a long tradition in Germany. Its success is inextricably linked with the use of large-scale equipment at national and international research centres. "With the new concept, basic research in Germany will start from an excellent position when entering a new decade of successful work", Minister Bulmahn said.
Together with European partners, the Gesellschaft für Schwerionenforschung (GSI) in Darmstadt is to develop further its equipment in a phased approach and become a leading european physics centre. At least 25% of the costs amounting to €675 million are to be shouldered by foreign partners.
40
K. Peters - Charm Physics @ Panda
Summary & Outlook
The The PANDAPANDA experiment at the experiment at the
antiproton facility antiproton facility HESR @ GSIHESR @ GSI
addresses many addresses many important questionsimportant questions
in in open open and and hidden charm physicshidden charm physics
Status:Status:
Letter of Intent: Jan. 15, 2004Letter of Intent: Jan. 15, 2004
Technical Report: Dec. 15, 2004Technical Report: Dec. 15, 2004
Technical Design Report: 2005-2007Technical Design Report: 2005-2007
Commissioning: 2011Commissioning: 2011