Difference between revisions of "Mattione Update 09042013"

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(γp→π+π-p (ρ Mesons))
(γp→π+π-p (ρ Mesons))
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=== Protons ===
 
=== Protons ===
 
[[Image:Mattione_Update_09042013_Thrown_Proton_Rho.png|left|250px]]
 
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[[Image:Mattione_Update_09042013_EfficiencyDiffZoomed_TimeBased_Rho_Proton.png|thumb|left|250px]]
 
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=== Efficiencies ===
 
=== Efficiencies ===

Revision as of 18:20, 3 September 2013

CDC Track Finding

Single π+ Track

Single π+ Reconstruction: Current (Trunk) Code, trackeff_hists plugin

  • The below plots show the track reconstruction efficiency and resolution for the trunk using the single-track scripts plugin (trackeff_hists).
  • However, this efficiency is extremely misleading:
    • If a track is reconstructed using any of the hits that were on the thrown track it is considered "found."
    • This is regardless of whether the reconstructed track momentum is anywhere close to the thrown values.
Time-Based Tracks (trackeff_hists plugin)
Momentum Resolution (trackeff_hists plugin)

Single π+ Reconstruction: Current (Trunk) Code, NEW trackeffv2 plugin

  • The below plots show the track candidate and time-based track reconstruction efficiency for the trunk using a new plugin (trackeff_hists).
  • This plugin compares matches all of the thrown and reconstructed particles in the event, and requires that their momentum be "close."
    • "Close" for track candidates is defined as: Δp/p < 20%, Δθ < 40 degrees, Δφ < 40 degrees, ΔVertex-Z < 1 km
      • For thrown tracks with θ < 5 degrees, there is no cut on Δφ
    • "Close" for time-based tracks is defined as: Δp/p < 10%, Δθ < 15 degrees, Δφ < 15 degrees, ΔVertex-Z < 10 cm
Track Candidates (trackeffv2 plugin)
Time-Based Tracks (trackeffv2 plugin)
  • Note that the degradation of the efficiency at forward angles matches the track resolution plot in the previous section.
    • If I expand the requirements for the "Close" window, the efficiency increases, and the chosen parameters were somewhat arbitrary.

Single π+ Reconstruction: NEW Spiral Code

  • The below plots show the track candidate and time-based track reconstruction efficiencies for the new spiral code.
  • Note: The trackeffv2 plugin compares matches all of the thrown and reconstructed particles in the event, and requires that their momentum be "close."
    • "Close" for track candidates is defined as: Δp/p < 20%, Δθ < 40 degrees, Δφ < 40 degrees, ΔVertex-Z < 1 km
      • For thrown tracks with θ < 5 degrees, there is no cut on Δφ
    • "Close" for time-based tracks is defined as: Δp/p < 10%, Δθ < 15 degrees, Δφ < 15 degrees, ΔVertex-Z < 10 cm
Track Candidates Efficiency (Spiral Code)
Time-Based Track Efficiency (Spiral Code)
  • The below plots show the improvements in the track candidate and time-based track reconstruction efficiencies with the new spiral code.
Track Candidate Efficiency Improvement
Zoomed Track Candidate Efficiency Improvement
Time-Based Track Efficiency Improvement
Zoomed Time-Based Track Efficiency Improvement

γp→π+π-p (ρ Mesons)

Protons


Stage Efficiency - Current Code Efficiency - Spiral Code Improvement - Current Code Improvement - Spiral Code
Track Candidates
Track Candidates


Efficiencies

  • The below plots show the track candidate and time-based track reconstruction efficiencies for both track finding codes.
  • Note: The definition of closeness is the same as before (see the single-track section).
Track Candidates Efficiency (Spiral Code)
Time-Based Track Efficiency (Spiral Code)
  • The below plots show the improvements in the track candidate and time-based track reconstruction efficiencies with the new spiral code.
Track Candidate Efficiency Improvement
Zoomed Track Candidate Efficiency Improvement
Time-Based Track Efficiency Improvement
Zoomed Time-Based Track Efficiency Improvement

γp→π+π+π-(n)

γp→π+π+π-π-π0(p) (b1pi)

bggen (pythia)

γp→K+K+Ξ-