Title: final state study
1final state study
- Jaewon Park
- University of Rochester
MINERvA/Jupiter Group Meeting, May 09, 2007
2Processes involving with final state
- Proton or muon tracks will determine primary
vertex - decays into two gammas
NC
CC
3Energy vector for gammas
Actual primary vertex position
- Gamma track is not good for reconstructing pi0
- Extrapolating long distance makes big uncertainty
- Instead, we used center of energy position with
respect to primary vertex, that is determined by
proton track
?
?
4Overview of calorimetry
lead
iron
ID
ECAL
HCAL
scintillator
particle
- After careful study of energy response in each
sub-detector with given energy of incoming
particle, then we can determine the energy of
particle
5Simple but fatal mistake on calorimetry
calculation
- While working on converting fortran analysis code
to c based code, couple of lines look weird.
Its turned out to be a big bug. - Separating ECAL region from ID was wrong. It
selected only half side of it. - The impact is making ECAL energy lower.
- This error propagates all the way to old
calibration calculation. - I believe that primary particle in old data was
pointed to the side that ECAL is selected
correctly.
6Resolution of proton, pi0, and each gammas before
correction
- Asymmetric energy distribution having lower side
tail.
7Resolution of proton, pi0, and each gammas after
correction
- Now it looks much better
- Also resolution gets smaller
8Reco E vs. True E of gamma
- Because lower energy gamma is shown to makes
resolution worse, I used event selection that
requires energy loss fraction in ID greater than
10 - But this doesnt make sense because earlier
calibration study shows such event election was
only useful for HCAL - Smart analysis technique cant beat up removable
systematic error
gamma1
gamma2
gamma1
gamma2
corrected
9Pi0 mass before correction
- Pi0 mass is determined from two gamma energies
and angle between them
10Pi0 mass after correction
- Lower-side tail has been reduced
11Enhance pi0 mass resolution using chi-squire
minimization with pi0 mass constraint
Guaranteed single solution
12Comparing Minuit solution with Mathematica
numerical solution
Mathematicas numerical solution
Minuit result
First and second run
13Chi-square minimization result gamma energy
resolution
are acquired from these plots
before
- True angle is used
- Chi-square minimization makes each gammas
resolution work - They become correlated with constraint
after
14Chi-square minimization result pi0 energy
resolution
- Pi0 resolution is enhanced
- We can apply chi-square cut to remove poor data
points
before
after
15W resolution this part didnt use chi-square fit
- W invariant mass of hadrons
- Didnt use E(id)/E gt 0.1, so efficiency
increased. - Reconstruced proton direction means using
reconstructed primary vertex - Pi0 mass cut m(pi0)90, 150
true proton dir
reco proton dir
true proton dir Pi0 mass cut
Reco proton dir Pi0 mass cut