oct. 5 th 2011 8 th international workshop on heavy quarkonium 2011 jim ritman mitglied der...

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Oct. 5 th 2011 8 th International Workshop on Heavy Quarkonium 2011 Jim Ritman Mitglied der Helmholtz- Gemeinschaft Status of PANDA

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Oct. 5th 2011 8th International Workshop on Heavy Quarkonium 2011 Jim Ritman

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Status of PANDA

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 2

Overview

Summary of PANDA physics potential

FacilityFAIRPANDA

Charmonium Benchmark Channelshc → ff → K+K- K+K-

Y(3770)→D+D-

X(3872)

Width Determination of the Ds0*(2317)

Conclusions

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 3

Summary of PANDA physics potential

• Confinement Why are there no free quarks?

• Hadron mass Where is the mass of the proton coming from?

• Are there other color neutral objects?

• What is the structure of the nucleon?

• What are the spin degrees of freedom?

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 4

Summary of PANDA physics potential

Meson spectroscopy: D mesons charmonium glueballs, hybrids, tetraquarks, molecules

Charmed and multi-strange baryon spectroscopy

Electromagnetic processes ( pp→e+e-, pp→gg, Drell-Yan)

Properties of single and double hypernuclei

Properties of hadrons in nuclear matter

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 5

FAIR Facility

FAIR → L. Schmidt’stalk on Oct. 4th

Founding of FAIR: Oct. 2010

Submission of building permits: Aug. 2011

Financing of HESRJun/Oct 2011

(RESR !) You are here

HESR

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 6

HESR

1011 Antiprotons from 1.5-15 GeV/c, fixed target L=1032

(Initially without RESR, stacking in HESR)

Stochastic and electron cooling ds=20-100 keV

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 7

PANDA

Forward SpectrometerDipole Magnet

Target Spectrometer

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 8

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 9

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 10

Micro-Vertex-Detector

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 11

Central Tracker

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 12

Central Tracker

Low mass, X/X0~1%

• 1.5 kg Straw tubes (4580×2.5g) • Close-packed layers• pressurized p=2bar

• 9 kg Mechanical frame

• srf ~ 150 mm, sz ~ 2.9 mm

• sp ~ 1% at B = 2 Tesla

• dE/dx (~8%) measurement for PID

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 13

Simulations of Charmonium Benchmark Channels

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 14

Performance Simulations for hc → ff → K+K- K+K-

Benchmark channel to study kaon tracking performanceMC-PID

Pbeam = 3.677 GeV/c

BR = 0.0027×0.5×0.5

D. Melnychuk, Warsaw

DIRC

DEDX

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 15

Invariant mass distributions

single events 20 MHz Rate

Performance Simulations for hc → ff → K+K- K+K-

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 16

Performance Simulations for Y(3770)→D+D-

Benchmark channel to study vertexing

Pbeam = 6.579 GeV/cBR = 0.30×0.095×0.095

M. Mertens, Juelich and D. Kang, Mainz

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 17

Performance Simulations for Y(3770)→D+D-

4C Kinematic fit appliedAcc.×Eff. = 5.0%

Only VTX-fitsY ~ 30 MeV

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 18

X(3872)

Detailed presentation this afternoon by M. Galuska, Giessen

(40 days)

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 19

Width Determination of the Ds0*(2317)

Nature of Ds0*(2317) unclear

Interpretation very sensitive to width~ keV - MeV

Current upper limit G < 3.8 MeV does not discriminate interpretations

PANDA will do a resonance scan to achieve a precision better than 100 keV

B.Aubert, PRD 74,032007

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 20

Excitation Function Scan of the Ds0*(2317)

Method

Sensitivity to width

Effect of the beam

resolution Dp/p ~ 10-4

M. Mertens, Juelich

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 21

Excitation Function Scan of the Ds0*(2317)

Simulated excitation function

c2-contour

Resolution of the width

Jim Ritman, Institut für Kernphysik (IKP) Juelich Slide 22

Summary/Conclusions

• FAIR is on-track

• HESR is funded, calls for tender ready to go

• PANDA going into construction phase

• Despite competion, PANDA has unmatched physics reach