Difference between revisions of "Photon Reconstruction in b1pi events 02/10/2012"

Revision as of 17:42, 13 February 2012

BCAL

Thrown photons

Look at the distribution of decay photons from the pi0.

For comparison with reconstructed data, useful to look at z rather than theta. This is the z that the photon would reach the inner radius of the BCAL, given its momentum and vertex.

Reconstructed photons

Spectrum of reconstructed "photons"-exclude clusters that can be matched to a charged track.

Where does each of these peaks come from?

• Broad peak around 125 cm due to protons?
• Peaks at upstream and downstream ends of detector from noise that cause garbage timing info?
• Other three sharp peaks? Look like FDC structure, but spacing is not right?

Cuts

• A timing cut fabs(t_shower-t_flight) < 1 ns can be applied to remove many of the extra "photons". (Red curve below)
• I don't think low energy showers are well understood at the moment, so remove clusters with E<60 MeV. (Green)
• Also, cut out a problem area at forward angles and lower energies (E<150 MeV && z>300 cm) (Blue)

More work needed to optimize cuts.

With all cuts:

Number of "photons" decreases from 60,000 to 17,000.

Two gamma invariant Mass

Look at pairs of 2 BCAL photons and 1 BCAL+1 FCAL photon, with the cuts described above. Using truth vertex information.

Compare KLOE algorithm to GlueX algorithm.

Black is KLOE, red is GlueX. Fits are to gaussian + straight line.

GlueX has less background, the fit also indicates that it has a taller peak, but I don't know how much this fit can really be trusted.