Recent results from FNAL E835 on the study of charmonium states in proton-antiproton annihilation - PowerPoint PPT Presentation

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Recent results from FNAL E835 on the study of charmonium states in proton-antiproton annihilation

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389 52. 290 50. 130 33. G(J/yg)exp (keV) (4.9 0.7) 10-9. 430 ... J/yp p- e e- Preliminary. Matteo Negrini. Photon 2003. Frascati, 07-11 April 2003. Conclusions ... – PowerPoint PPT presentation

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Title: Recent results from FNAL E835 on the study of charmonium states in proton-antiproton annihilation


1
Recent results from FNAL E835 on the study of
charmonium states in proton-antiproton
annihilation
  • Matteo Negrini
  • Università degli Studi di Ferrara - INFN
  • Photon 2003 Frascati, 07-11 April 2003

2
Charmonium spectroscopy in annihilation
  • ee- annihilation ? only JPC1- states directly
    formed (J/y and y)
  • gg fusion ? all C (J?1) states directly
    accessible
  • B factory
  • annihilation ? all the states directly
    formed through 2 or 3 gluons intermediate states
  • Large hadronic background
  • Detection of electromagnetic final states

3
Antiproton beam and target
  • TARGET
  • Hydrogen gas-jet target
  • Hydrogen clusters density
  • 1 41014 atoms/cm3
  • The H2 target density can be tuned to obtain
    constant luminosity
  • L INST 21031 cm-2s-1
  • Target dimension ? 7 mm
  • BEAM
  • Antiprotons are accumulated until the desired
    current is reach. Then they are stochastically
    cooled and decelerated to the desired energy
    (continuous beam)
  • The total CM energy can be determined directly
    from the antiproton beam parameter
  • sE?400keV - sE /E?10-4
  • Beam dimension ? 5 mm

4
Detector
Threshold Cerenkov counters (Separation of high
energy e from the hadronic background)
Electromagnetic calorimeter (12ltqlt68)
Luminosity monitor (Solid state detector. Counter
of elastic interactions at 90)
Charged tracking system (15ltqlt60)
5
Experimental technique
  • The beam energy is moved to scan the resonance
    (precision sE?250 keV)
  • The number of events N at energy E is obtained
    as
  • L instantaneous luminosity
  • G(E) beam energy distribution (gaussian)
  • e detection efficiency
  • The resonance cross section is obtained by
    deconvolution of the measured rate with the beam
    profile

6
Event selection where final state includes ee-
  • Selection of electron / positron candidates
  • high energy deposition in calorimeter
  • signal in the hodoscopes
  • signal in Cerenkov
  • Electron Weight (EW)
  • Maximum likelihood method for the single
    electron selection based on calorimeter cluster
    shape and pulse height in Cerenkov and
    hodoscopes.

EW1EW2gt1.5
Background
  • Kinematic fit

7
c0 mass and width
Luminosity 33 pb-1 (20 pb-1 on resonance) on
17 energy points Selected channel radiative
decay to J/y N. Selected events 400
Electron Weight
Kinematic Fit
8
c0 mass and width
9
gg final state selection
  • Exactly 2 on-time clusters in the central
    calorimeter with high energy deposit and
    invariant mass within 20 of ECM
  • No undetermined-time extra clusters with
    invariant mass within 35 MeV of the p0 mass
  • 4C kinematic fit to gg
  • cos(q) cut to improve signal to background
    ratio

10
gg background (feeddown)
  • Background mainly from
  • where one or more photons are missing because of
    acceptance or calorimeter energy thresholds
  • Measurement of the cross section for the
    background processes and Monte Carlo
    determination of the background contribution
  • Comparison with measured gg cross section for
    off-resonance points

11
c0?gg
Preliminary
Taking from the PDG
12
hc?gg
Preliminary
  • 18.9 pb-1 of data
  • All the resonance parameters are measured in the
    gg channel

13
Interference between ?c0 ?p0p0 and the
continuum
Preliminary
Measurement of the cross section for the
process in the c0 energy region
Interfering (helicity 0)
Non-Interfering (helicity 1)
Resonant
500000 p0p0 candidates
14
c0 branching ratios
Preliminary
Using the PDG value
To be compared with the PDG
Using the result
To be compared with the PDG
15
Electric dipole trasition (P?Sg)
  • The value obtained for G(c0?J/yg), using the new
    total width and the BR measurements, is
    consistent with the theory of electric dipole
    transition

G(J/yg)exp (keV) k (MeV) G/k3 (MeV-2)
c0 13033 304 (4.61.2)?10-9
c1 29050 390 (4.90.8)?10-9
c2 38952 430 (4.90.7)?10-9
16
ee- final states selection at the y
  • y and J/y detected through their ee- decay
  • All the exclusive channels are selected with
    kinematic fits
  • 14.3 pb-1 of data in the y energy region
    collected in year 2000
  • 12.4 pb-1 on resonance ? 32862 events
  • 1.9 pb-1 off resonance ? 66 events

Preliminary
17
y branching ratios
Preliminary
J/yh
J/yp0p0
J/ypp-
ee-
18
Conclusions
  • Charmonium states are studied in proton
    antiproton annihilation detecting electromagnetic
    final states
  • Extensive study of the cc0 ...
  • Mass and total width
  • gg width
  • Interference in p0p0 decay
  • ... and of the hc
  • Mass and total width
  • gg width
  • New measurement of BR(y?J/y X) and BR(y?ee-)
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