Data Format GRAAL
VARIABLE | TIGER EVT RECON correspondence | DEFINITION | COMMENT | |
---|---|---|---|---|
Event | evtNo | event ID from 0 to total number of event | ||
nGemHit | number of good hits in one event | |||
GemHit_nHit | same as nGemHit | |||
GemHit_nHit_view | array of number of good hits for each view in one event | |||
GemHit_nHit_bad | number of bad hits in one event | |||
GemHit_channel | tchannel | channel ID from 0 to 63 readed by TIGER | ||
GemHit_chip | chip | chip ID | from 0 to 87 | |
GemHit_ROC | tgemroc | GEMROC ID readed by TIGER | ||
GemHit_FEB | tFEB_label | FEB label from 0 to 43 (L1 + L2) defined from mapping | from 0 to 43 | |
GemHit_plane | hit plane | (0=L1, 1=upper L2, 2=lower L2) | ||
GemHit_view | hit view | (2 = Phi, 3 = V) | ||
GemHit_strip | tstrip_v | tstrip_x | strip ID from mapping as a function of channel and FEB | |
GemHit_q | tcharge_SH | efine of the hit readed by TIGER + calibration from FEB | ||
GemHit_x | coordinate of the strip (in radiant if Phi, else in mm) | |||
GemHit_pos | hit position in X reference frame | |||
GemHit_z | hit position in Z reference frame | Z is minus the beam direction | ||
GemHit_time | t_min_ttrigg | hit time from the trigger time | ||
nGemCluster | number of cluster of hits in one event | |||
GemCluster1d_nCluster | same as nGemCluster | |||
GemCluster1d_plane | cluster plane | (0=L1, 1=upper L2, 2=lower L2) | ||
GemCluster1d_view | (2 = Phi, 3 = V) | |||
GemCluster1d_q | cluster charge in fC as sum of hits charge | |||
GemCluster1d_x | coordinate of the cluster (in radiant if V, else in mm) in CC no TPC yet | |||
GemCluster1d_z | cluster position in Z reference Z is minus the beam direction | |||
GemCluster1d_pos | cluster position in X reference |
GRAAL analysis procedure[edit | edit source]
GRAAL analysis is divided in three parts: reconstruction, tracking and analysis.
1) Reconstruciton: creates hits from the TIGER data and it clusterizes contiguous hits
2) Tracking: look for the best cluster for each detector and it measures the particle path and the residual distribution of the detector to this track
3) Studies the performance of the detector and of the cluster with a good residual distribution
Reconstruction:[edit | edit source]
-- Digitization --
Starting from the information of the output of TIGER Reconstruction Event (event.root) is associate to each collected signal the variables reported above.
The cut on the hits are the following:
Strip > 0 -> strpis are initialized to -1 and if there are problems this cut removes the hits if it is not properly filled
View > 0 -> views are initialized to -1
Channel != TP_Channel
Charge > 0.5 fC
-100 < Time < 150 ns
Remove noisy channel labelled here (chip,channel) --> (43,3), (46,26), (73,3), (87,45)
-- Clustering --
Contiguous strips are collected together where
Q_cluster = sum Q_hit
X_cc = charge centroid position
Tracking:[edit | edit source]
If cosmics run is analyzed then it divides L1 and L2 in three planes: top L2, bottom L2 and L1.
The two sides of L2 are used as tracking system. The cluster with higher charge is selected as the good one and a linear fit is performed with the two points.
If L2 top and L2 bottom are not firing at the same time then the track is not reconstructed.