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Jo Lynn Tyner Mu2e Background Layout CRV Importance Efficiency Simulation Gap Hits Dead Counters Local Drop Future Work References Effects of Single Counter Efficiencies on Mu2e Sensitivity and Mitigation Strategy for Individual Counter Efficiency Deficits Jo Lynn Tyner, Tim Bolton, Glenn Horton-Smith August 4, 2017

Jo Lynn Tyner E ects of Single Counter E ciencies on · Jo Lynn Tyner Mu2e Background Layout CRV Importance Efficiency Simulation Gap Hits Dead Counters Local Drop Future Work References

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Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Effects of Single Counter Efficiencies onMu2e Sensitivity and Mitigation Strategyfor Individual Counter Efficiency Deficits

Jo Lynn Tyner,Tim Bolton, Glenn Horton-Smith

August 4, 2017

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Background

I The mission of the Mu2e (Muon to ElectronConversion) experiment is to observe a muon toelectron conversion. This observation would beevidence of a charged lepton flavor violation process,thereby putting into question some parts of theStandard Model.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Mu2e Layout

[1]

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Mu2e Layout

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Mu2e Layout

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Mu2e Layout

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Cosmic Ray VetoImportance

I Cosmic Rays interfering with the detection devices inMu2e create background that can hide electronconversion events in noise.

I The Cosmic Ray Veto will measure cosmic ray strikesand veto the events from the final data.

[2]

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Efficiency

I To be considered a veto event, a signal must bedetected in at least three out of four counters.

I The counters must have a combined overall efficiencyof 99.99%.

I Individual counter efficiencies affect overall efficiency.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Simulation

I I have developed a simulation in which I generate anevent which consists of:

I four random integer generations representing possiblehits

I if this number is the individual counter efficiency, ahit count is iterated by one integer

I This hit count value is recorded (0-4)

I There are 1,000,000 events per simulation. After allof these have run, passing events and failing eventsare printed out.

I Passing evens have four or three hits, failing eventshave zero, one, or two hits.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Gap Hits

I To get an accurate overall efficiency, the gaps in thedetector need to be accounted for.

I Based on the design of the CRV-T, I calculated thereis about a 0.37% chance that a cosmic ray will hit agap.

I If the gap random number generation meets the0.37% chance criteria, the number of random numbergenerations representing possible hits drops to three.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Gap Hits

A printout from a gap corrected simulation.

I To meet the overall efficiency requirement, theindividual counter efficiency needs to be 99.65%.

I Note: The probability of hitting all four counters iscalculated by

(.9965)4 + 4 ∗ (1 − 0.9965) ∗ (.9965)3 = 0.9999

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Dead Counter

I Manufacturing and electronic malfunctions couldcause some counters to be dead.

I In all counters being simulated, there is a deadcounter condition.

I If the condition is met, there will not be a hitincrementation.

I A 99.8% individual counter efficiency with 0.2% deadcounters will result in the target overall efficiency.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Dropping the Local Pass/Fail Rate

I The individual efficiencies of the counters cannotchange once they have been manufactured.

I The target overall efficiency must be met eventhough some counters may experience failures.

I When a dead counter is present in the track,dropping the pass qualification to two or three hits,and the fail qualification to zero or one hits will solvethis problem.

I Using this local dropped pass/fail rate, the individualcounter efficiency can again be 99.65%.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

Future Work

I It is unknown if dropping the local pass/fail rate willincrease dead time a significant amount. This mustbe studied before the solution is put into play.

Jo Lynn Tyner

Mu2e

Background

Layout

CRV

Importance

Efficiency

Simulation

Gap Hits

Dead Counters

Local Drop

Future Work

References

References and Acknowledgements

[1] Corcoran, Marj. Intro to the Mu2e tracker. Mu2eSummer Student Lecture Series. July 20, 2015.[2] Technical Design Report. Mu2e Document 4299-v15.March, 23, 2015. Mu2e Document Database.

We would like to thank our Mu2e collaborators both atFermilab and Kansas State University. This project wasfunded by the National Science Foundation (NSF) andthe Air Force Office of Scientific Research (AFOSR)through NSF grant number PHYS-1461251.