Download - CC/NC SEPARATION STUDY
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CC/NC SEPARATION STUDY
Andy BlakeCambridge University
Friday February 23rd 2007
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Introduction
Andy Blake, Cambridge University CC/NC Separation, slide 2
• Have developed a PID for CC/NC separation
• PID is calculated using a likelihood technique, and extends the “standard” PID algorithm by incorporating some new PDFs and accounting for their change in shape as a function of energy.
• Code committed to “MadAbID” class in Mad package.
• Documentation also available in doc-db #2720.
• Will outline method and present some results in this talk.
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PID Variables
Andy Blake, Cambridge University CC/NC Separation, slide 3
Variables for CC/NC separation
• Event Topology Variables.
– percentage pulse height in track.
– pulse height per track plane.
– number of track like planes.
– percentage error in track fit.
• Event Kinematics Variables.
– reconstructed y.
• Event Energy and Charge.
– number of track planes.
– reconstructed charge.
• Relative CC/NC Normalization.
Test consistency with muon track.
Test consistency with CC interaction.
Incorporate CC/NCspectral information.
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PID Definition
Andy Blake, Cambridge University CC/NC Separation, slide 4
• PID calculated from the product of several 1D and 2D PDFs as follows:
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PID Variables: (I) Track Topology
Andy Blake, Cambridge University CC/NC Separation, slide 5
TRACK-LIKE PLANES vs TRACK PLANES
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PID Variables: (I) Track Topology
Andy Blake, Cambridge University CC/NC Separation, slide 6
TRACK PH / TRACK PLANES vs TRACK PLANES
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PID Variables: (I) Track Topology
Andy Blake, Cambridge University CC/NC Separation, slide 7
TRACK PH / EVENT PH vs TRACK PLANES
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PID Variables: (I) Track Topology
Andy Blake, Cambridge University CC/NC Separation, slide 8
TRACK FIT ERROR vs TRACK PLANES
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PID Variables: (II) Event Kinematics
Andy Blake, Cambridge University CC/NC Separation, slide 9
RECO Y vs RECO E
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PID Variables: (III) CC/NC Spectrum
Andy Blake, Cambridge University CC/NC Separation, slide 10
TRACK PLANES RECONSTRUCTED CHARGE
CC/NC NORMALIZATION
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PID Study
Andy Blake, Cambridge University CC/NC Separation, slide 11
• Cedar MC Ntuples.
– Far Detector (generate PDFs using 8.7e22 PoTs calculate PIDs using 2.9e22 PoTs).
– Near Detector (generate PDFs using 8.5e18 PoTs calculate PIDs using 2.5e18 PoTs).
• Event Selection.
– reconstructed track.
– successful track fit.
– contained track vertex.
• Construction of PDFs.
– PDFs constructed assuming no oscillations.
– 2D PDFs normalized to remove any spectral information. (i.e. divide out the shape of the energy spectrum).
– as a final step, try pre-selecting events with PCC=1. (i.e. create second set of PDFs for events with PCC<1).
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PID Results (Far Detector)
Andy Blake, Cambridge University CC/NC Separation, slide 12
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Purity vs Efficiency (Far Detector)
Andy Blake, Cambridge University CC/NC Separation, slide 13
Standard PID:
track PH/ event PH.
track PH/ track planes.
track planes.
Incorporate:
track-like planes.
track fit error. track charge.
reconstructed Y. (replace trk.ph/evt.ph).
pre-selection.
N.B: maximum values of purity*efficiency indicated by stars
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Purity vs Efficiency (Far Detector)
Andy Blake, Cambridge University CC/NC Separation, slide 14
Standard PID cutapproximately here!
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PID Results (Near Detector)
Andy Blake, Cambridge University CC/NC Separation, slide 15
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PID Results (Low Energies)
Andy Blake, Cambridge University CC/NC Separation, slide 16
E < 3 GeV
6 < E < 9 GeV
3 < E < 6 GeV
E > 9 GeV
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Summary
Andy Blake, Cambridge University CC/NC Separation, slide 17
• Incorporation of new variables into PID calculation improves purity and efficiency of CC/NC separation in both detectors over all energies.
• This will hopefully improve the sensitivity of the oscillation analysis!
• Possible improvements to this method:
– Separate fully and partially contained events.
– Separate neutrinos and anti-neutrinos.
– Incorporate other topology variables (e.g. pulse height profile of event).
– Incorporate another kinematic variable (e.g. x distribution).