PAX experiment PAX: Polarized Antiproton Experiments 1 dr. Paolo Lenisa Universit di Ferrara and INFN - ITALY ECT Workshop: Hadronic structure of the nucleon Trento, May 9-13 PAX experiment PAX: Polarized Antiproton Experiments 2 Yerevan Physics Institute, Yerevan, Armenia Department of Subatomic and Radiation Physics, University of Gent, Belgium University of Science & Technology of China, Beijing, P.R. China Department of Physics, Beijing, P.R. China Palaiseau, Ecole Polytechnique Centre de Physique Theorique, France High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia Nuclear Physics Department, Tbilisi State University, Georgia Forschungszentrum Jlich, Institut fr Kernphysik Jlich, Germany Institut fr Theoretische Physik II, Ruhr Universitt Bochum, Germany Helmholtz-Institut fr Strahlen- und Kernphysik, Bonn, Germany Physikalisches Institut, Universitt Erlangen-Nrnberg, Germany Langenbernsodorf, UGS, Gelinde Schulteis and Partner GbR, Germany Department of Mathematics, University of Dublin,Dublin, Ireland Universit del Piemonte Orientale and INFN, Alessandria, Italy Dipartimento di Fisica dellUniversit and INFN, Cagliari, Italy Universit dellInsubria and INFN, Como, Italy Instituto Nationale di Fisica Nuclelare, Ferrara, Italy PAX Collaboration Spokespersons: Paolo Lenisa Paolo Frank Rathmann Frank Rathmann PAX experiment PAX: Polarized Antiproton Experiments 3 Dipartimento di Fisica Teorica, Universita di Torino and INFN, Torino, Italy Instituto Nationale di Fisica Nucleare, Frascati, Italy Andrej Sultan Institute for Nuclear Studies, Dep. of Nuclear Reactions, Warsaw, Poland Petersburg Nuclear Physics Institute, Gatchina, Russia Institute for Theoretical and Experimental Physics, Moscow, Russia Lebedev Physical Institute, Moscow, Russia Physics Department, Moscow Engineering Physics Institute, Moscow, Russia Laboratory of Theoretical Physics, Joint Institute for Nueclear Research, Dubna, Russia Laboratory of Particle Physics, Joint Institute for Nuclear Research, Dubna, Russia Laboratory of Nuclear Problems, Joint Institute for Nuclear Research, Dubna, Russia Budker Institute of Nuclear Physics, Novosibirsk, Russia High Energy Physics Institute, Protvino, Russia Institute of Experimental Physics, Slovak Academy of Science, Kosice Slovakia Department of Radiation Sciences, Nuclear Physics Division, Uppsala University, Uppsala, Sweden Collider Accelerator Department, Brookhaven National Laboratory, Broohhaven USA RIKEN BNL Research Center Brookhaven National Laboratory, Brookhaven, USA University of Wisconsin, Madison, USA Department of Physics, University of Virginia, USA 178 physicists 35 institutions (15 EU, 20 NON-EU) PAX Collaboration PAX experiment PAX: Polarized Antiproton Experiments 4 The PAX proposal Jan. 04 LOI submitted QCD PAC meeting at GSI Workshop on polarized antiprotons at GSI F. Rathmann et al., A Method to polarize stored antiprotons to a high degree (Phys. Rev. Lett. 94, (2005)) Technical Report submitted QCD-PAC meeting at GSI Polarization enters in the core of FAIR PAX experiment 5 Outline WHY? Physics Case HOW? Polarized Antiprotons WHAT?Staging Detector and signal estimate WHERE AND WHEN? The FAIR project at GSI PAX: Polarized Antiproton Experiments PAX experiment 6 Physic Topics Transversity Electromagnetic Form Factors Hard Scattering Effects SSA in DY, origin of Sivers function Soft Scattering Low-t Physics Total Cross Section pbar-p interaction Physics Polarization Staging Signals FAIR PAX experiment 7 Physics Case: Central Physics Issue Transversity distribution of the nucleon: last leading-twist missing piece of the QCD description of the partonic structure of the nucleon directly accessible uniquely via the double transverse spin asymmetry A TT in the Drell-Yan production of lepton pairs theoretical expectations for A TT in DY > 0.2 transversely polarized antiprotons transversely polarized proton target definitive observation of h 1 q (x,Q 2 ) of the proton for the valence quarks Physics Polarization Staging Signals FAIR PAX experiment 8Transversity -Probes relativistic nature of quarks -No gluon analog for spin-1/2 nucleon -Different evolution than -Sensitive to valence quark polarization Properties : Chiral-odd: requires another chiral-odd partner Impossible in DIS Direct Measurement ppl+l-Xppl+l-X ep eh X Indirect Measurement: Convolution of with unknown fragment. fct. Physics Polarization Staging Signals FAIR PAX experiment 9 Transversity in Drell-Yan processes p p QLQL Q l+l+ l-l- Q 2 =M 2 QTQT Polarized Antiproton Beam Polarized Proton Target (both transversely polarized) M invariant Mass of lepton pair Physics Polarization Staging Signals FAIR PAX experiment 10 PAX: s~ GeV 2, M 2 ~ GeV 2, =x 1 x 2 =M 2 /s~ Exploration of valence quarks (h 1 q (x,Q 2 ) large) A TT for PAX kinematic conditions A TT /a TT > 0.2 Models predict |h 1 u |>>|h 1 d | Physics Polarization Staging Signals FAIR RHIC: s = 200 GeV, M 2 100 GeV2 =x 1 x 2 =M 2 /s 2x10 -3 Exploration of the sea quark content (polarizations small!) A TT very small (~ 1 %) Barone, Calarco, Drago Martin, Schaefer, Stratmann, Vogelsang A. Efremov et al. Eur. Phys. J. C 35 (2004) 207 PAX experiment 11 Energy for Drell-Yan processes safe region: MM J/ M 2 J/ /s QCD corrections at smaller M? H. Schimizu, G. Sterman, W. Vogelsang and H. Yokoya, hep-ph/ V. Barone et al., in preparation Physics Polarization Staging Signals FAIR PAX experiment 12 NLO corrections: cross section Physics Polarization Staging Signals FAIR PAX experiment 13 NLO corrections: A TT Physics Polarization Staging Signals FAIR PAX experiment 14 ql+l+ l-l- ql+l+ l-l- All vector couplings, same spinor structure Measure A TT also in J/ resonance region M. Anselmino, V. Barone, A. Drago, N. Nikolaev Physics Polarization Staging Signals FAIR Resonance region PAX experiment 15 Proton Electromagnetic Formfactors Measurement of relative phases of magnetic and electric FF in the time-like region Possible only via SSA in the annihilation pp e + e - Double-spin asymmetry independent G E -G m separation test of Rosenbluth separation in the time-like region S. Brodsky et al., Phys. Rev. D69 (2004) Physics Polarization Staging Signals FAIR PAX experiment 16 p (GeV/c) Study onset of Perturbative QCD Pure Meson Land Meson exchange excitation NN potential models Transition Region Uncharted Territory Huge Spin-Effects in pp elastic scattering large t : non-and perturbative QCD High Energy small t: Reggeon Exchange large t: perturbative QCD Physics Polarization Staging Signals FAIR PAX experiment 17 pp Elastic Scattering from ZGS Spin-dependence at large-P 90 cm ): Spin-dependence at large-P (90 cm ): Hard scattering takes place only with spins . D.G. Crabb et al., PRL 41, 1257 (1978) T=10.85 GeV Similar studies in pp elastic scattering Physics Polarization Staging Signals FAIR PAX experiment 18 Outline WHY? Physics Case HOW? Polarized Antiprotons WHAT?Staging Detector and signal estimate WHERE AND WHEN? The FAIR project at GSI (D) PAX: Polarized Antiproton Experiments PAX experiment 19 Polarized internal target point-like5-10 mmfree jetlow density10 12 cm -2 extended mmstorage cellhigh density10 14 cm -2 Physics Polarization Staging Signals FAIR PAX experiment 20 Atomic Beam Source NIM A 505, (2003) 633 The HERMES target Physics Polarization Staging Signals FAIR PAX experiment 21 The HERMES target Atomic Beam Source NIM A 505, (2003) 633 P z+ = |1> + |4> P z- = |2> + |3> m j = +1/2 m j = -1/2 m i =-1/2 m i =+1/2 1 |1> |2> |3> |4> ee-ee-p |1> Physics Polarization Staging Signals FAIR PAX experiment 22 The HERMES target Atomic Beam Source NIM A 505, (2003) 633 Storage cell NIM A 496, (2003) 277 Physics Polarization Staging Signals FAIR PAX experiment 23 The HERMES target Atomic Beam Source NIM A 505, (2003) 633 Storage cell NIM A 496, (2003) 277 Diagnostics: Target Gas Analyzer NIM A 508, (2003) 265 Breit-Rabi Polarimeter NIM A 482, (2002) 606 Physics Polarization Staging Signals FAIR PAX experiment 24 Performance of Polarized Internal Targets P T = HERMES H Transverse Field (B=297 mT) HERMES DzDz D zz P T = Longitudinal Field (B=335 mT) HERMES: Stored Positrons PINTEX: Stored Protons H Fast reorientation in a weak field (x,y,z) Targets work very reliably (months of stable operation) Physics Polarization Staging Signals FAIR PAX experiment 25 Principle of spin filter method P beam polarization Q target polarization k || beam direction tot = 0 + PQ + || (Pk)(Qk) transverse case:longitudinal case: For initially equally populated spin states: (m=+) and (m=-) Unpolarized anti-p beam Polarized H target Physics Polarization Staging Signals FAIR PAX experiment 26 Principle of spin filter method P beam polarization Q target polarization k || beam direction tot = 0 + PQ + || (Pk)(Qk) transverse case:longitudinal case: For initially equally populated spin states: (m=+) and (m=-) Unpolarized anti-p beam Polarized H target Polarized anti-p beam Physics Polarization Staging Signals FAIR PAX experiment 27 Principle of spin filter method P beam polarization Q target polarization k || beam direction tot = 0 + PQ + || (Pk)(Qk) transverse case:longitudinal case: For initially equally populated spin states: (m=+) and (m=-) Expectation TargetBeam For low energy pp scattering: 1 30% after hrs (10 11 pbar) Physics Polarization Staging Signals FAIR PAX experiment 38 Spin-filtering with hadronic interaction Model A: T. Hippchen et al. Phys. Rev. C 44, 1323 (1991) P Kinetic energy (MeV) Model D: V. Mull, K. Holinde, Phys. Rev. C 51, 2360 (1995) P Kinetic energy (MeV) Physics Polarization Staging Signals FAIR PAX experiment 39 Outline WHY? Physics Case HOW? Polarized Antiprotons WHAT?Staging Detector and signal estimate WHERE AND WHEN? The FAIR project at GSI (D) PAX: Polarized Antiproton Experiments PAX experiment 40 Staging: Phase I Physics:EMFF pbar-p elastic Experiment: pol./unpol. Pbar (3.5 GeV/c) on int. pol. target Independent from HESR running Physics Polarization Staging Signals FAIR PAX experiment 41 Staging: Phase II EXPERIMENT: 1. Asymmetric collider: polarized antiprotons in HESR (p=15 GeV/c) polarized protons in CSR (p=3.5 GeV/c) 2. Internal polarized target with 22 GeV/c polarized antiproton beam. Physics: Transversity Second IP with minor interference with PANDA Physics Polarization Staging Signals FAIR PAX experiment 42 Outline WHY? Physics Case HOW? Polarized Antiprotons WHAT?Staging Detector and signal estimate WHERE AND WHEN? The FAIR project at GSI (D) PAX: Polarized Antiproton Experiments PAX experiment 43 Kinematics and cross section M 2 = s x 1 x 2 x F =2Q L /s = x 1 -x 2 Estimated luminosities: Fixed target: 2.7x10 31 cm -2 s -1 Collider:1-2 x cm -2 s -1 M (GeV/c 2 ) 22 GeV collider 2 k events/day Physics Polarization Staging Signals FAIR PAX experiment 44 A TT asymmetry: angular distribution Needs a large acceptance detector (LAD) Asymmetry is largest for angles =90 Asymmetry varies like cos(2 ). Physics Polarization Staging Signals FAIR PAX experiment 45 Designed for Collider but compatible with fixed target Cerenkov (200 m) (20 m) GEANT simulation PAX detector concept Physics Polarization Staging Signals FAIR PAX experiment 46 Estimated signal for h 1 (phase II) 1 year of data taking Collider: L=2x10 30 cm -2 s -1 Fixed target: L=2.7x10 31 cm -2 s -1 Physics Polarization Staging Signals FAIR PAX experiment PAX: Polarized Antiproton Experiments 47 Beam (MeV/c) (GeV 2 ) e+e- (nbarn)* L (cm -2 s -1 ) Days DS Days SS x x x N pbar = 1x10 11 f=L CSR / c d t =1x10 14 cm -2 Q=0.8 (p pol) P=0.3 (pbar pol) =0.5 Estimated signal for EMFF (Phase I) PS170 and E835 PAX could run down to 200 MeV/c with double polarization Running days to get O = 0.05 Polarization Staging Signals Timeline PAX experiment PAX: Polarized Antiproton Experiments 48 BNL E838 Estimated Signal for pbar p elastic (Phase I) Cross section estimation for p=3.6 GeV/c, =120 Event rate ( t=0.1 GeV 2 ): 2 hours to get N 10 Polarization Staging Signals Timeline PAX experiment PAX: Polarized Antiproton Experiments 49 PAX Integrated Luminosities for Physics Cases pb -1 fb -1 Integrated Luminosity EMFF, DSA, s=3.76 GeV 2 ppbar elastic, DSA, t=4 GeV 2 Phase-I: L=1.510 31 cm -2 s -1 Antiproton Beam Polarization P pbar =0.3, Proton Polarization P p =0.8 Phase-II: L=210 30 cm -2 s -1 EMFF, DSA, s=9 GeV 2 Absolute Error DSA =0.05 h 1, DSA, M>2 GeV, =10% h 1, DSA, M>4 GeV, =20% (1 y) (4 y) (1 y) PAX experiment 50 Outline WHY? Physics Case HOW? Polarized Antiprotons WHAT?Staging Detector and signal estimate WHERE AND WHEN? The FAIR project at GSI (D) PAX: Polarized Antiproton Experiments PAX experiment 51 Faciltiy for Antiproton and Ion Research (GSI, Darmstadt, Germany) (GSI, Darmstadt, Germany) -Proton linac (injector) -2 synchrotons (30 GeV p) -A number of storage rings Parallel beams operation Physics Polarization Staging Signals FAIR PAX experiment 52 FLAIR: (Facility for very Low energy Anti- protons and fully stripped Ions) SIS100/300 HESR: High Energy Storage Ring: PANDA and PAX NESR CR-Complex The FAIR project at GSI The FAIR project at GSI 50 MeV Proton Linac Physics Polarization Staging Signals FAIR PAX experiment 53 Phase 0: Polarization tests, polarizer design and construction. Phase I: GSI Physics: EMFF with fixed target Phase II: HESR+CSR asymmetric collider Physics: h 1 Timeline Timeline Physics Polarization Staging Signals FAIR PAX experiment 54 Conclusions Challenging opportunities accessible with polarized pbar. Unique access to a wealth of new fundamental physics observables Central physics issue: h 1 q (x,Q 2 ) of the proton in DY processes Other issues: Electromagnetic Formfactors Polarization effects in Hard and Soft Scattering processes differential cross sections, analyzing powers, spin correlation parameters Staging approach Projections for double polarization experiment (tests) : P beam > 0.30 L> 1.6 10 30 cm -2 s -1 (Collider), L 2.7 10 31 cm -2 s -1 (fixed target) Detector concept: Large acceptance detector with a toroidal magnet PAX experiment 55 Georg Christoph Lichtenberg ( ) Man mu etwas Neues machen, um etwas Neues zu sehen. You have to make something new, if you want to see something new