Pion Analysis Absorption + Charge Exchange Jake Calcutt July 11, - - PowerPoint PPT Presentation
Pion Analysis Absorption + Charge Exchange Jake Calcutt July 11, - - PowerPoint PPT Presentation
Pion Analysis Absorption + Charge Exchange Jake Calcutt July 11, 2019 Jake Calcutt 2 Introduction In addition to the total (elastic + inelastic) cross section, exclusive (subsets of inelastic) pion-Ar cross sections provide useful information
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Introduction
In addition to the total (elastic + inelastic) cross section, exclusive (subsets of inelastic) pion-Ar cross sections provide useful information Have the added benefit of unique signals Exclusive channels:
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My Goal
For now: build an event selection for Absorption and Charge Exchange events Eventually: Make a cross section measurement across range of momenta This talk: shows some studies of MCC11 in my progress towards the event selection
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Event Topologies
π+ X π+ X π0
Absorption Charge Exchange
X = Nucleons
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Signal Definiton
Birds eye view: Pion interaction with no charged pions in final state
- Look for interactions without MIP in final state
- Attempted cutting on average dE/dX along the track
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dE/dX of Daughter Tracks
Looked at all reconstructed daughters coming out of the primary pion tracks Averaged dE/dX from Collection plane by number of hits Backtracked reco daughters to true PDG (provided by the MCParticle contributing the most deposited energy)
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dE/dX of Daughter Tracks
Abs+Cex All BG Pion Interactions Abs Cex
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Observations
Within this signal there should be no charged pion daughters Scanning these events showed that these backtracked to the incident pions More on this later
Abs+Cex
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Observations
Particularly in Absorption, there is a peak in dE/dX < 2 MeV for protons Need to investigate
Abs
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Observations
The gammas from the pi0 decays are quite often reconstructed as tracks, and contaminate the MIP-like region Will come back to this in a few slides
Cex
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Observations
Muons are sometimes associated as daughters to the signal Later: I have some insight on this
Cex
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Pions Associated as Daughters
Cursory glance at events show tracks splitting at elastic scatters This is working as intended (I did not realize this at first)
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Need to change the way I treat/think about these tracks Normally, I think about pions similar to Geant: the pion is one track up to the inelastic interaction/decay → elastic scatters along the track are included in this Now: Should I treat this as BG? What about low-angle elastic scatters that aren’t reconstructed?
Pions Associated as Daughters
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π0 Decay Gammas
The shower CNN ID can be used to pick out gammas from π0 decays and disregard during MIP-rejection Sum up scores from all hits in a track, divide by N hits
Cex BG
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χ2-based PID
Tingjun pointed me to a PID technique developed for MicroBooNE: Fitting reconstructed dEdX vs Range to proton template More sophisticated than average dEdX along the track
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χ2-based PID
Abs+Cex BG Still need to deal with Pi0 decay and charged pion reco “issues” Implemented in ProtoDUNETrackUtils
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Muon Daughter Tracks
Started investigating where muons are coming from (should be none from Decay since I’m only looking at EndProcess == “pi+Inelastic”) Looking at true origin and backtracking the parent particles Decay: product of primary decay Decay+: primary daughter decay Decay++: primary granddaughter decay
Abs+Cex events 2 Total
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Muon Daughter Tracks
Started investigating where muons are coming from (should be none from Decay since I’m only looking at EndProcess == “pi+Inelastic”) Looking at true origin and backtracking the parent particles Decay: product of primary decay Decay+: primary daughter decay Decay++: primary granddaughter decay
BG events
More downstream decays from π+ → π∓
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Daughter Track Starting Points
Investigating why cosmics are assigned as daughters. Tried looking at distance to end of primary track Note: distance comes from closer of start or end of daughter track to end of primary track
Abs+Cex BG
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Daughter Track Starting Points
Hand scanning a few events from
- MC. I noticed this interesting case
(High stats sample w/ sce, run 2, subrun 3, event 484) Beam π+ (28) has an elastic scatter, Pandora recognizes this and creates a new track (23). It ends in an inelastic interaction and creates a proton (70) that is associated as 28’s daughter. Additionally, a cosmic (30) is associated as a daughter
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To-Do
- Reconsider how I’m treating elastic scatters before the inelastic
interaction
- Disregard Pi0-gammas in MIP-rejection in daughter tracks
- Look into shower daughter information
- Look at MCC12 (these studies was done using MCC11)
Thanks for listening
Jake Calcutt