Title: Recent results from FNAL E835 on the study of charmonium states in proton-antiproton annihilation
1Recent 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
2Charmonium 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
3Antiproton 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
4Detector
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)
5Experimental 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
6Event 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
7c0 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
8c0 mass and width
9gg 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
10gg 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
11c0?gg
Preliminary
Taking from the PDG
12hc?gg
Preliminary
- 18.9 pb-1 of data
- All the resonance parameters are measured in the
gg channel
13Interference 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
14c0 branching ratios
Preliminary
Using the PDG value
To be compared with the PDG
Using the result
To be compared with the PDG
15Electric 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
16ee- 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
17y branching ratios
Preliminary
J/yh
J/yp0p0
J/ypp-
ee-
18Conclusions
- 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-)