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Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th , 2011 nted stereo hits, formed by the intersection of 2 clusters within 35) n Recognition Concept: Start with a 2D Circle Fitter, using these ere how well this works. ew this 2D fitter as part of the Pattern Recognition Algorithm, whos g off good straw hits to the Kalman Fitter. 1

Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

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Page 1: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Status of Pattern Recognition for the T-Tracker

Hans Wenzel, Hogan NguyenMarch 12th, 2011

Introduction

Hans implemented stereo hits, formed by the intersection of 2 clusters withina plane (0-35)

Basic Pattern Recognition Concept: Start with a 2D Circle Fitter, using these stereo hits.

We analyze here how well this works.

Note: We view this 2D fitter as part of the Pattern Recognition Algorithm, whose goalis to handing off good straw hits to the Kalman Fitter.

1

Page 2: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Outline

- Quick Review Of Basic Concepts and Previous Work(http://mu2e-docdb.fnal.gov:8080/cgi-bin/ShowDocument?docid=1337)

- Z information from the 2D Fitter

- Evaluation of simple pattern recognition with Accidental Overlays

- New Tools to Help Pattern Recognition (Hans)

Page 3: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

6 Configurations for Stereo Hits

Panels Used Plane-----------------------------------------------

0 & 1 or 3 & 4 even plane 1 & 2 or 4 & 5 even plane 2 & 3 or 5 & 0 even plane

0 & 1 or 3 & 4 odd plane 1 & 2 or 4 & 5 odd plane 2 & 3 or 5 & 0 odd plane

3

Page 4: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

4

systematicshift in position

strawcluster

strawcluster

electron

Example:

polar angle = 72 degreesPhi angle = 90 degrees

No Shift in Y coordinate.

Systematic shift in X coordinate =

(19/2 mm)/tan(90-polar)*tan(30) = 17 mm

trueposition

Systematic Shift of Stereo Hit Position

StereoHit Position

Page 5: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Fit Minimizes Perpendicular Distance To Circle.

3 free parameters for a 2D circle:

X0, Y0 is the fitted center, and R is the fitted Radius Notes

NO SEARCH ALGORITHM – ALL Stereo Hits are used in the FIT

Errors Calibrated From MC(see Next Slide)

Adhoc Correction done toaccount for polar angle dependence of the StereoHit.

Can do it rigorously later

5

Page 6: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Radius of Stereo Hit - Radius of True Hit

Confi

gura

tion

num

ber

Errors Used in the 2D Fit. Calibrate using Monte Carlo

6

Radius Error of 2 mm Phi Error of 5 degrees(Phi not used in the fit)

Phi – True Phi

Page 7: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

allow 1 iteration to refit excluding theworse chi2 contributor

Fit Consistency

Low ProbabilityFits due toMultiple Scattering,Interactions, andPathological ClusterShapes

7

Rejecting Low Probability EventsKeeps = 83% (NO OTHER HITS)

Page 8: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Delta phi = angle of stereo hit with respect to first stereo hit

Period in Z = Position drift in Zfor ONE complete orbit rotation.Calculated ASSUMING p=105 MeVHypothesis

Z Period number (dimensionless) =Number of Z periods

first hit

second hit

third hit

DefinitionZ information from the 2D fitter

Page 9: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Ideal Case

DeltaPhi

Z Period Number (calculated assuming Conversion Electron Hypothesis)

All Hits from Conversion Events Lie on theCurve, Independent of Polar Angle of Conversion Electron

Page 10: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Z period Number (dimensionless)

Delta Phi (degrees)

Monte Carlo Truth Positions Used& Selected P > 103 MeV

Radiated ConversionElectrons cause off-diagonal points

Rotation Angle (Phi) versus Z

2000generatedconversionevents

Page 11: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Z period Number (dimensionless)

Delta Phi (degrees)

Rotation Angle (Phi) versus Z Reconstructed Stereo Hits Used

Errorsin definingthe First Hit(1% effect)

2000 generatedconversion events

Page 12: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

Overlay of Accidental Hits onto Conversion Events

Process Rate Per Microbunch Number of Clusters

Pure Conversion -- 23

Ejected Protons 5628 16 (After ADC cut)

Decay In Orbit* 36K 4

Pion Capture 75 7 Cosmics small ~ 0

Electronics Noise Study Not Done TBD

* Generated only DIO with E>60 MeV to save computing time

Thanks to: Gianni, Bob, Craig for Rates

Page 13: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

100 Pure Conversion Electron Events ( cos(polar) = 0.3)

deltaPhi

Z Period NumberStereo Hits in Circle-Centered Coordinates

Fit Cut Eff = 83%

Page 14: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

100 Conversion Electron Events Overlayed with Pion Capture

deltaPhi

Z Period NumberStereo Hits in Circle-Centered Coordinates

Pion CaptureAdds ~ 7 ClustersPer Event

Fit Cut Eff = 66 %

Page 15: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

100 Conversion Electron Events Overlayed with DIO Events

deltaPhi

Z Period NumberStereo Hits in Circle-Centered Coordinates

DIO Adds about 4 ClustersPer Event

Fit Cut Eff =70 %

Page 16: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

ADC is Critical for Removing Proton Ejection Events

Conversion Events Proton Ejection Events

ADC < 6 KeV

Page 17: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

100 Conversion Electron Events Overlayed with Proton Ejection Events

Proton Ejection Eventsadd 16 more clustersper event (after ADC cut)

Fit Cut Eff = 10 %

Stereo Hits in Circle-Centered Coordinates Z Period Number

Page 18: Status of Pattern Recognition for the T-Tracker Hans Wenzel, Hogan Nguyen March 12 th, 2011 Introduction Hans implemented stereo hits, formed by the intersection

What Next

- The ADC cut is critical. It is doing the lion’s share of removing bad hits.

- Simple 2D fitter with NO search algorithm fails with accidentals

- Need to Beef up the 2D fitter with a search algorithm

- Hans will discuss other tools.