<<

HadronHadron spectroscopyspectroscopy inin diffractivediffractive andand centralcentral productionproduction processesprocesses atat COMPASSCOMPASS

Prometeusz Jasinski for the COMPASS collaboration

- Diffraction 2010 - Beyond the qq model

Constituent model QCD prediction: states beyond

Color neutral qq systems Hybrids: qqg Quantum numbers (IG) JPC : (qq)(qq) P=(-1)L+1 C=(-1)L+S G=(-1)I+L+1 → “Spin exotics” JPC multiplets: 0, 0, 1, 1, 1, 2, …      Forbidden: 0 , 0 , 1 , 2 , 3 , ... : gg, ggg

Production mechanisms

Diffractive Scattering Central Production The COMPASS 2008/2009

The COMPASS Spectrometer 2008/2009

Beam properties Beam properties Beam energy 190 GeV/c² Beam energy 190 GeV/c² Beam composition:   Beam composition:  :  : p = 0.97 : 0.024 : 0.008  :  : p = 0.97 : 0.024 : 0.008 or   or  :  : p = 0.24 : 0.014 : 0.75  :  : p = 0.24 : 0.014 : 0.75 Up to 5 x 10⁶ particles/s Up to 5 x 10⁶ particles/s

beam

The COMPASS Spectrometer 2008/2009

CEDARCEDAR detectors detectors for for beambeam particle particle identification identification

The COMPASS Spectrometer 2008/2009

CEDARCEDAR detectors detectors for for beambeam particle particle identification identification

Cerenkov Differential counter with Achromatic Ring Focus

The COMPASS Spectrometer 2008/2009

RecoilRecoil proton proton detecto detectorr aroundaround 4040 cm cm long long lH2 lH2 target target oror ArrayArray of of solid solid state state discs discs

The COMPASS Spectrometer 2008/2009

The COMPASS Spectrometer 2008/2009 Further important upgrades ECALECAL Laser Laser monitoringmonitoring system, system, radhard glass, Sandwich veto radhard glass, Sandwich veto shashlikshashlik modules modules matchingmatching the the spectrometer spectrometer acceptanceacceptance

RICHRICH upgrade in 2006 SeveralSeveral tracking tracking upgrade in 2006 detectorsdetectors upgraded: upgraded: coldcold Silicon Silicon stations, stations, PixelPixel GEMs, GEMs, Micromegas,Micromegas, ...... And much more not mentioned here. Some results of  p →   p recoil

- - - -   ● Visible well established  Isobar a (1260), a (1320) andIsobar  (1670) X 1 2 X 2 +/0 0  ● COMPASS observed in 2004 data  the exotic (JPC=1) (1600) (see next talk) -/0 0  ● The run will exceed world's statistics p p target by a factortarget of 100 p p recoil recoil

First PWA results of  p →   p     recoil

Reduction factor of ~1/2 as expected by isospin symmetry

Isobar model, 42 waves including background, mass independent fit, comparison of neutral and charged modes with normalization to a 2 Selected results of  p →  p    recoil

 -  -  -  - Analysis of diffractivelyIsobar produced X X  systems  0 PWA currently being performed  More results expected soon  0 p p target target p p recoil recoil

Selected results of  p →   p     recoil

 -  - ● Isobar Tagging incoming beam Kaons X ● Many states in the  system need  confirmation ● Outnumbering previous results  p by a factor of ~3 target p recoil

Selected results of  p →     p   fast     recoil

- -   + ● Analysis of 4 pion central production  demonstrates the spectrometer's  - excellent acceptance and resolution X ● Looking at the region around f (1500) + 0  to study the previously quoted p target - existence of more than one resonance  p recoil

Selected results of  p →  K Kp   recoil

●final state analysis  -  -  -  - ● PID of charged Kaons by RICH Isobar ● K identified byX decay vertex  +/0 s  0 ● separation of centrally and diffractively X produced systems by rapidity gap  -/0  0 p ● Analysisp of disputed branching ratios of target resonancestarget such as f (1370) p p 0 recoil recoil

Some results on  p →   p     recoil Selected results for p p → p     p      recoil p p p p ● Tagging the proton in the h+ beam → Isobar Isobar X ● Hadro-producedX / ● Accessing regions of high masses and+ angular momenta  ● Rich baryon spectrum to be  - p p target distinguishedtarget p p recoil recoil

Summary and outlook

● After the spectrometer upgrade COMPASS took data with different hadron beams in 2008 and 2009

● both, charged and neutral, final state particles accessible →

● COMPASS has access many interesting channels in Meson and Baryon spectroscopy

● COMPASS statistics exceeds the one by previous experiments by a factor of up to 100

● Analyses using PWA techniques are ongoing

● We are expecting much more interesting results very soon

● interesting results expected very soon, also with nuclear targets

● Collaborators are very welcome!

Thank you

Backup slides

Details of PWA for 3 pi final state

Gottfried-Jackson Frame

Additional plots for Ks Ks

The diffractive process is still clearly visible in the invariant mass of Kpi as resonances.

Additional distributions for pKK