GLAST Large Area Telescope:

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Presentation transcript:

GLAST Large Area Telescope: Gamma-ray Large Area Space Telescope GLAST Large Area Telescope: Reconstruction Tracy Usher Stanford Linear Accelerator Center usher@slac.stanford.edu http://www-glast.slac.stanford.edu/software

Reconstruction Goals and Requirements Goal: To boldly go where no man has gone before… Requirement: Earn enough to make mortgage payment

GLAST Reconstruction Anatomy of a “Typical” Event Pair production is the dominant photon interaction in our energy range GLAST Reconstruction Theory Incident Gamma converts in the tracker In particular, conversion occurs in one of the converter foils – ie at a well defined location Resulting electron-positron pair range out of tracker (TKR)… No magnetic field, tracks are “straight lines” Resulting two tracks “point” back to incident Gamma And into the CsI Calorimeter (CAL) Measures total energy of electron-positron pair = Gamma energy Surrounding Anti-Coincidence Detector (ACD) vetoes any wayward charged particles What could be easier? Calorimeter (energy measurement) Particle tracking detectors Conversion foils (W) Charged particle anticoincidence shield  e+ e-

GLAST Reconstruction What Really Happens…

GLAST Reconstruction What Really Happens…

Tracking Overview “Standard” HEP Approach Raw Data 1) Hit Strips 2) “ToT” Clusters 1) Clustering: Associate adjacent hit strips to form clusters Top of LAT CandidateTracks Cluster Centroid (Center of hit strips) Measuring direction Silicon Wafer (end view) 2) Track Finding: Assume start point, direction and energy Follow track and attach clusters allowing for deviations due to multiple scattering, etc. NOT TO SCALE!! Hit strip (strip pitch: 228 μm) Cluster Width (Number of hit strips)

Tracking Overview “Standard” HEP Approach Track Finding (see previous page) “Vertex” vector resulting from combining the two fit tracks in this event Vertex Position = gamma conversion point Vertex Vector = gamma direction 3) Track Fit: Kalman Filter Fit to get final Track Parameters Clusters Tracks 4) “Vertexing”: Combine Tracks to determine conversion point and direction of the incident Gamma Note: a “vertex” can consist of only one track Errors at Clusters from Kalman Fit

Calorimetry Overview “Raw” Data Corrected Energy, “Position” per Xtal Corrections/Calibrations applied before this step! “Raw” Data Corrected Energy, “Position” per Xtal Incident Gamma e+e- pair (plus brems, etc.) MC Display of hit Crystals: Divides Xtal longitudinally into eight sections for display Shows Hit Xtal, does not show energy deposited – can’t really see shower development 1 GeV Gamma Clustering: Associate hit Xtals together to form clusters Gamma Energy: All hit Xtals are from incident Gamma – Energy is sum over all hit Xtals Backgrounds: Isolated sets of hit Xtals from own “cluster”

Calorimetry Overview Energy “leaking” out the bottom Flow of Gamma Energy 5 GeV Gamma Gamma Conversion Point Energy Correction Algorithms: 1) Shower Profile 2) Ineffeciencies due to Geometry 3) Leakage 4) etc. (see next slides)

Calorimetry Overview Gap between Towers 1 GeV Gamma Flow of Gamma Energy Gamma Conversion Point Energy Correction Algorithms: Ineffeciencies due to Geometry Given the direction of energy flow (from the reconstructed Gamma direction), can apply geometric corrections to account for energy “lost”, e.g. between towers

Putting It All Together Chicken… Track Finding/following needs starting values: Initial Position Initial Direction Initial Energy This from the Calorimeter… Or Egg? Energy Correction algorithms need gamma direction This from the tracking… Solution: Iterative Reconstruction First Pass Calorimeter Reconstruction Through Clustering Total Energy Cluster Centroid Cluster Axis Tracker Reconstruction Track Finding/Following Track Fit and Vertexing Good enough for 2nd pass Second Pass Energy Correction Algorithms Use “improved” energy

Background Rejection Example: Charged Particles in Tracker Project Track to plane of struck tile Calculate distance to nearest edge Sign Positive if track projection inside the tile Negative if track projection outside the tile Reject if inside the tile 1 GeV Muon Reconstructed Track Extra: Min I signature in Calorimeter Struck ACD Tile Projection of Track back to nearest ACD Tile “Active Distance” outside tile boundary no tile hit inside tile boundary [cm]

End of Reconstruction It will never be this good again