1 / 29

University of Santiago de Compostela, Spain

|a 0 -a 2 | Measurement from Pionium Lifetime by DIRAC. Bernardo Adeva on behalf of DIRAC collaboration. University of Santiago de Compostela, Spain. IVth INTERNATIONAL CONFERENCE ON QUARKS AND NUCLEAR PHYSICS 5 - 10 June 2006, Madrid, Spain. DIRAC.

deo
Download Presentation

University of Santiago de Compostela, Spain

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. |a0-a2|Measurementfrom Pionium Lifetime by DIRAC Bernardo Adeva on behalf of DIRAC collaboration University of Santiago de Compostela, Spain IVth INTERNATIONAL CONFERENCE ON QUARKS AND NUCLEAR PHYSICS 5 - 10 June 2006, Madrid, Spain

  2. DIRAC DImeson Relativistic Atomic Complexes Lifetime Measurement of +- atoms to test low energy QCD predictions www.cern.ch/DIRAC Basel Univ., Bern Univ., Bucharest IAP, CERN, Dubna JINR, Frascati LNF-INFN, Ioannina Univ., Kyoto-Sangyo Univ., Kyushu Univ. Fukuoka, Moscow NPI, Paris VI Univ., Prague TU, Prague FZU-IP ASCR, Protvino IHEP, Santiago de Compostela Univ., Tokyo Metropolitan Univ., Trieste Univ./INFN, Tsukuba KEK. 90 Physicists from 18 Institutes

  3. π+ π0 π0 π Pionium lifetime Pionium is a hydrogen-like atom consisting of + and - mesons EB=-1.86 keV, rB=387 fm, pB≈0.5 MeV The lifetime of + atoms is dominated by charge exchange process into 00: at lowest order : a0 and a2 are the  S-wave scattering lengths for isospin I=0 and I=2. Pionium would never decay should the pion be a perfect Goldstone boson !

  4. Pionium lifetime in QCD At next-to-leading order in α and (md – mu )2 : J. Gasser et al , Phys. Rev. D62 (2001) 016008  = (5.8 ± 1.2)× 10-2 significant correction  non-singular relativistic amplitude at threshold Measurement of  (10%)  |a0-a2| (5%)

  5. Pionium lifetime in QCD The  scattering lengths have been calculated in the framework of Chiral Perturbation Theory (ChPT): G. Colangelo, J. Gasser and H. Leutwyler, Nucl. Phys. B603 (2001) 125. A self-consistent representation of the amplitudes also exists: J. R. Peláez, F. J. Ynduráin, Phys. Rev. D69 114001 (2004)

  6. K+→+-e+e (Ke4) decay a0=0.26±0.05 L. Rosselet et al., Phys. Rev. D 15 (1977) 574 a0=0.216±0.013 ±0.003(syst) a2=-0.0454±0.0031 ±0.0013(syst) New measurement at BNL (E865) S.Pislak et al., Phys.Rev. D 67 (2003) 072004 N→N near threshold a0=0.26±0.05 C.D. Froggatt, J.L. Petersen, Nucl. Phys. B 129 (1977) 89 a0=0.204±0.014 ±0.008(syst) M. Kermani et al., Phys. Rev. C 58 (1998) 3431 K+→+00 and KL→30 NA48 |a0-a2|=0.281±0.007 (stat.) ±0.014 (syst.) N.Cabibbo, Phys. Rev. Lett. 93, 121801 (2004) N.Cabibbo, G.Isidori, hep-ph/0502130 Experimental results

  7. Production of pionium The pionium is a Coulomb bound state: p+ and p-originating from short lived sources (r, K*, w,...) and resonance decays may form a pioniumatom. The differential cross section is: Lorentz Center of Mass to Laboratory factor. Wave function at origin (accounts for Coulomb interaction). Pion pair production from short lived sources.

  8. Annihilation: A2→00 Excitation: transitions between atomic levels Break-up(ionisation): characteristic “atomic” pairs nA • Qcms<3MeV/c • → in laboratory system E+≈E-, small opening angle θ<3mrad Method of pionium detection L.Nemenov, Sov.J.Nucl.Phys. 41 (1985) 629 Pionium is created in nS states then it interacts with target material: Coulomb and atomic pairs are detected simultaneously:

  9. Coulomb pairs.They are produced in one proton nucleus collision from fragmentation or short lived resonances resonances (, K*, ,...) and exhibit Coulomb interaction in the final state: Non-Coulomb pairs.They are produced in one proton nucleus collision. At least one pion originates from a long lived resonance. No Coulomb interaction in the final state Accidental pairs.They are produced in two independent proton nucleus collision. They do not exhibit Coulomb interaction in the final state Production of pionium Atoms are Coulomb bound state of two pions produced in one proton-nucleus collision Background processes:

  10. DIRAC Spectrometer Downstream detectors: DCs, VH, HH, C, PSh, Mu. Upstream detectors: MSGCs, SciFi, IH.

  11. DIRAC Spectrometer High high irradiation Tracking principles • Precison time-of-flight toreduce accidental and proton background • Strong e+e- rejection by Čerenkov counters • Unambiguous transverse momentum QT by upstream tracking (MSGC+SFD) • Longitudinal momentum QL measured by fast drift chambers and upstream tracks

  12. DIRAC Spectrometer Nucl. Inst. Meth. A515 (2003) 467. Downstream detectors: Drift chambers Cherenkov Time-of-Flight Pre-Shower and Muon Counters unseen Upstream detectors: MSGC/GEM SFD Ionisation Hodoscope

  13. Trigger performance

  14. Calibrations Mass distribution of p- pairs from  decay. =0.39 MeV/c2 Time difference spectrum at VH with e+e- T1 trigger. Positive arm mass spectrum, obtained by TOF difference, under - hypothesis in the negative arm.

  15. Time-of-Flight spectrum +- pairs Accidental pairs, different proton interactions in the target Coulomb pairs. From short lived sources. r < 3 fm, < R(A2p) Non Coulomb pairs. From long lived sources. r ~ 1000 fm.

  16. Analysis based on MC Atoms are generated in nS states using measured momentum distribution for short-lived sources. The atomic pairs are generated according to the evolution of the atom while propagating through the target Background processes: Coulomb pairs are generated according to AC(Q)Q2 using measured momentum distribution for short-lived sources. Non-Coulomb pairs are generated according to Q2 using measured momentum distribution for long-lived sources. Monte Carlo simulation is restricted to detector response only without relying on specific asumptions from proton-nucleus collision models

  17. 2D 2FIT TO (QT, QL) SPECTRUM 3 (accidentals fraction) measured from TOF 1 and  free parameters in 10 independent 600 MeV/c +- momentum bins Atom signal defined as difference between prompt data and Monte Carlo with  = 0

  18. PIONIUM BREAK-UP SIGNAL IN +- SPECTRUM · cos Transverse Longitudinal

  19. Pionium signal in Q =√ QL2+ QT2

  20. PIONIUM TRANSVERSE SIGNAL QL < 2 MeV/c QL > 2 MeV/c

  21. PIONIUM LONGITUDINAL SIGNAL

  22. DETERMINATION OF BREAK-UP PROBABILITY Coulomb-pair background NCC determined from fit 1 parameter: QM analytical factor: Acceptance factors idetermined by Monte Carlo simulation Different extrapolation domains: Standard choice is QLC = 2 MeV/c and QTC = 5 MeV/c

  23. Break-up probability as function of pionium momentum PBr

  24. PBr as function of QL upper cut

  25. Fraction of Coulomb pairs as function of momentum 1

  26. /(0.6 GeV/c) Coulomb pairs  1/40 Spectrum consistent with +- bound state formation Atom pairs Long-lived pairs (2) Coulomb pairs Softer spectrum (, ..) expected from Monte Carlo

  27. Breakup probability Summary of systematic uncertainties:  Source QL trigger acceptance Multiple scattering angle (± 1.5 %) MSGC background Atom signal shape Finite size correction (± 25 % ) Double-track resolution simulation ± 0.007 ± 0.003 ± 0.006 ± 0.002 ± 0.003 ± 0.003 Total ± 0.009

  28. Results from DIRAC • DIRAC collaboration has built up a double arm spectrometer which provides a pair relative momentum (Q) resolution of 0.5 MeV/c for Q<30MeV/c • More than 15000 of + - pairs from pionium break-up were observed • The analysis of Ni 2001 data provides a lifetime measurement which translates into an S-wave amplitude measurement at rest :

More Related