Status of PANDA at FAIR

1. Alexander Vasiliev on behalf of the PANDA Collaboration Status of PANDA at FAIR

2. 1. Introduction: FAIR, HESR & PANDA (FAIR – Facility for Antiproton and Ion Research) (HESR– High Energy Storage Ring) (PANDA– antiProtonANnihilation at DArmstadt) 2. Physics program of PANDA 3. PANDA detector 4. Schedule of PANDA 5. Conclusion Content of the report

3. SIS 100/300 • 50 MeV • SIS18 • p-Linac • 30 GeV Protons • HESR • Cu Target107 p/s @ 3 GeV • pbar production : • proton Linac 50 MeV • accelerate p in SIS18/SIS100 • produce pbar on target • collect pbar in CR, • cool in RESR (not in Start Version) • inject pbar into HESR • PANDA • Accelerating • Cooling • RESR/CR • CollectingAccumulatingPrecooling • 100m

4. EXP HESR - High Energy Storage Ring Injection of p at 3.7 GeV Storage ring for internal target operation

5. antiProtonANnihilation atDArmstadt Experiment performed at FAIR facility, near GSI, in Darmstadt, Germany A very high intensity p beam with momentum from 1.5 GeV/c up to15 GeV/c on a proton fixed target (or nuclear target), average interaction rate 20 MHz, s from 2.25 up to 5.46 GeV It will continue and extend the successful physics program performed in the past at facilities like LEAR at CERN and the antiproton accumulator ring at FNAL

6. Physics Program of PANDA • Physics program is aimed at finding new forms of matter in the interactions of antimatter with matter. Some specific parts of the program are as follows:- search for exotic particles such as glueballs and hybrids; - spectroscopy of charmonium states mostly above the threshold for pair D-anti-D-mesons, however below the threshold as well (study h_c width etc.); - study hyper-nuclei (including - double) and charm-nuclei, when the strange (one or two) or charmed particle "implanted" into the nuclei instead of the usual nucleon; • study electromagnetic form factors of proton; • etc.

7. Benefit of antiproton annihilation In electron-positron annihilations direct particle formation is possible only for the states with the quantum numbers J(PC) = 1 (--)

8. c c e+ e− 1 fm 0.1 nm Positronium Charmonium Dissociation energy 1000 7 900 23S1 6 23P2 21P1 ψ’’ 800 n = 2 23P1 23S1 5 700 23P0 ψ’ DD threshold 600 η’c 23S1 Relative energy (eV) 4 χ2 Relative energy (MeV) hc 23P2 500 23S1 3 23P1 χ1 400 21P1 bound states χ0 300 23P0 2 200 1 100 n = 1 ψ 13S1 0 0 ηc 13S1 13S0 –100 13S0 L = 0 L = 1 L = 0 L = 1 Singlet Singlet T riplet Singlet T riplet Singlet T riplet T riplet

9. The glueball spectrum from LQCD calculations

10. X and Y mesons Belle X(3872) Y(4260) Belle Y(4008)? X(3872) Y(4350) & Y(4660) BaBar Belle Belle BKωJ/ψ Y(3940) BaBar Belle X(4160) M(ωJ/ψ) M(ωJ/ψ) CDF Belle X(3940) e+e-DD*J/ψ

11. M = (4.433 ± 0.004 (stat) ± 0.001 (syst)) GeV Z+ (4430) - a new state of matter (tetraquark?) decaying into π+ψ’ − Γ = (0.044+0.017 (stat)+0.030 (syst)) GeV BELLE 7σ PRL 100, 142001 (2008) arXiv:0708.1790 [hep-ex]

12. PANDA: pp ➛ Z+(4430) + π− ↵ ψ(2S)π+ → J/ψ π+π−

13. Detector requirements antiproton momentum: from 1.5 to 15 GeV/c Lmax~2 · 1032cm-2s-1, high rate capability: 2 · 107s-1interactions nearly 4p solid angle for PWA p±, K±, p±, e±, m±, g identification displaced vertex detection – vertexinfofor D, KS,,  (c = 317 m for D±) photondetectionfrom 10 MeVto 10 GeV efficienteventselection & goodmomentumresolution

14. PANDA Detector • Target Spectrometer • Forward Spectrometer • Dipole Magnet

15. Superconducting Solenoid • Central field 2.0 T • Field homogeneity ≤2% • Norm. radial field integral ≤2 mm • Inner bore 1.9 m • Cold mass parameters • Length 2.7 m • Energy 20 MJ • Current 5000 A • Weight 4.5 t • Cable cross section 3.4 × 2 mm2 • Current density 59 A/mm • Yoke parameters • Length 4.9 m • Outer radius 2.30 m • Iron layers 13 • Total weight 300 t

16. Micro Vertex Detector • r / mm • Target rmax= 150 mm • 4 • 3 • 2 • 135 • 1 • Beam • 95 1 • 55 2 3 4 • 25 5 6 -230 • 6 disk layers • 4 barrel layers • Silicon detectors: • Hybrid pixel detectors (11 M channels) • Double-sided microstrip detectors (200k ch.) -170 20 40 70 100 160 230 z / mm

17. Central Straw Tube Tracker • 4580 Straw tubes • Al-mylar: d=27µm, =10mm, L=1500 mm • 21-27 planar layers in 6 hexagonal sectors • 8 layers skewed (3D reconstruction) • Time readout (isochrone radius) • Amplitude readout (dE/dx) • srf ~ 150 mm, sz ~ 3.0 mm • p ~ 1-2% at B=2Tesla

18. Central EMC Barrel Calorimeter 11360 PWO Crystals APD readout, 2x1cm2 Forward Endcap 4000 PWO crystals High occupancy in center APD or VPT Backward Endcapfor hermeticity, 560 PWO crystals

19. Energy resolution of 3x3 PWO prototype with photomultiplier-readout

20. Large Aperture Dipole • 2Tm for particles scattered in 0 – 10o (5o vertical) • Allows momentum resolution <1% • Large aperture (1x3m) and short length (2.5m) • Ramping capability due to lamination • Field integral 2 Tm • Bending variation ≤ ±15% • Vertical Acceptance ±5° • Horizontal Acceptance ±10° • Ramp speed 1.25%/s • Total dissipated power 360 kW • Total Inductance 0.87 H • Stored energy 2.03 MJ • Weight 220 t • Dimensions (H × W × L) 3.88 × 5.3 × 2.5 m3 • Gap opening (H × W) 0.80 − 1.01 × 3.10 m2

21. Forward Tracker • 6 Tracking stations: 2 before, 2 inside and 2 after dipole magnet • based on 1 cm pressure stabilized straw tubes • Each tracking station contains four double-layers: two with vertical straws two tilted by ±5° • Angular acceptance: ±5º vertically, ±10º horizontally • Momentum acceptance: down to ~2% of pbeam • Momentum resolution: ~0.5%

22. 380 layers of 0.3-mm lead and 1.5-mm scintillator, total length 680 mm Transverse size 55x55 mm2 Light collection: 36 fibers BCF-91A (1.0mm) PMT as a photodetector LED for each module as a light monitoring system Optical fiber for each cell for a precise PMT gain monitoring Forward Shashlik-type Calorimeter Detector size: ~3,6m x 2,2 m (54x28 cells)

23. Dependence of Energy Resolution on energy σE /E = a/E  b/√E  c [%], E in GeV Experiment data and MC fit: a = 3.5 ± 0.3 a = 3.3 ± 0.1 b = 2.8 ± 0.3 b = 3.1 ± 0.1 c = 1.3 ± 0.3 c = 1.2 ± 0.1 Good agreement with MC (with a residual momentum spread of 2.4% introduced to get linear term)

24. Other Sub-detectors of PANDA • Target spectrometer: • barrel and forward DIRC • barrel TOF (scintillator tiles) • muon system (in solenoid) • Forward spectrometer: • TOF (scintillator strips) • muon system (at the end of set-up)

25. Collaboration • At present a group of 460 physicists from55 institutions of 17 countries • Austria – Belarus- China - France - Germany – India - Italy – The Nederlands - Poland – Romania - Russia – Spain - Sweden – Switzerland - Thailand - U.K. – U.S.A.. Basel, Beijing, Bochum, BARC Bombay, IIT Bombay, Bonn, Brescia, IFIN Bucharest, IIT Chicago, AGH Krakow, IFJ PAN Krakow, JU Krakow, Krakow UT, Edinburgh, Erlangen, Ferrara, Frankfurt, Genoa, Giessen, Glasgow, GSI, FZ Jülich, JINR Dubna, Katowice, KVI Groningen, Lanzhou, LNF, LNL, Lund, Mainz, Minsk, ITEP Moscow, MPEI Moscow, TU München, Münster, Northwestern, BINP Novosibirsk, IPN Orsay, Pavia, IHEP Protvino, PNPI St.Petersburg, KTH Stockholm, Stockholm, SUT, INFN Torino, Torino, Torino Politecnico, Trieste, TSL Uppsala, Tübingen, Uppsala, Valencia, SINS Warsaw, TU Warsaw, SMI Wien

26. Schedule of • experiment • commissioning • installation at FAIR • pre-assembly • mass production • R&D • TDR • FAIR

27. Conclusions • PANDA experiment will have a great potential for discovery in addition to the LHC at a relatively high-energy antiprotons and, at the same time, due to the energy scan mode will determine the width of the resonances with an accuracy of a linear collider. • Studies will be performed at the antiproton beam storage ring with a stochastic and electron cooling (HESR) with energy up to 15 GeV. Expected to record in the world of pure intensity antiproton beam that provides up to 2х107 interactions on the target per second. • In addition to high-intensity, beam of antiprotons would be unprecedented in the degree of monochromatic, the expected level of p/p down to 10-5, which will allow the study of strong interactions with high precision. • PANDA detector is created using the most modern technology and provides a registration and identification of neutral and charged particles to nearly the full solid angle and energy range up to 15 GeV. • A commissioning of PANDA and the first data taking is planned for 2018.