Note: This is a rather old study that I found on BEMC public AFS space and ported into Drupal. I don't know who conducted it or when. -- A. Kocoloski
On the subject of reconstruction made by cluster finder and matching, evaluation has been developed to determine how good is the reconstruction, efficiency, purity, energy and position resolution of reconstructed particles originally generated by simulation data.
Cluster finder is being evaluated at the moment using single particle events, which favors the evaluation of efficiency and purity. In this case, we can define efficiency and purity for single particle events as:
There are other quantities that could be used for evaluation. They are:
All these quantities can be studied as a function of the cluster finder parameters, mSizeMax, mEnergySeed and mEnergyThresholdAll. The results are summarized below.
Nothing was done to evaluate this parameter.
The purity as a function of mEnergySeed gets better and the efficiency goes down as this parameter increases. Some figures (the others parameters were kept as minimum as possible) are shown for for different values of mSizeMax for single photons in the middle of a tower with pt = 1,4,7 and 10 GeV/c.
The following plots were generated using energy seeds of 0.1 GeV (left), 0.5 GeV (middle), and 1.5 GeV (right). Full-size plots are available by clicking on each image:
Phi difference
Number of clusters
Energy ratio
Nothing was done to evaluate this parameter.
Nothing was done to evaluate this parameter.
The purity as a function of mEnergySeed gets better and the efficiency goes down as this parameter increases. Some figures (the others parameters were kept as minimum as possible) are shown for for different values of mSizeMax for single photons in the middle of a tower with pt = 1,4,7 and 10 GeV/c.
The following plots were generated using energy seeds of 0.05 GeV (left), 0.2 GeV (middle), and 0.8 GeV (right). Full-size plots are available by clicking on each image:
Eta difference RMS as a function of photon energy for different seed energies:
Phi Difference (BSMDP only)
Phi difference RMS as a function of photon energy for different seed energies:
BSMDE efficiency and purity as a function of seed energy
BSMDP efficiency and purity as a function of photon energy for different seed energies
The efficiency and purity as a function of mSizeMax get better as this parameter increases but for values greater than 4 there is no difference. Some figures (the others parameters were kept as minimum as possible) are shown for for different values of mSizeMax for single photons in the middle of a tower with pt = 5 GeV/c.