miniboone low energy analysis
DESCRIPTION
MiniBooNE Low Energy Analysis. H. Ray Los Alamos National Laboratory. Oscillation Fit Reporting. The final fit for e oscillations was performed using 2 different analyses Track Based : E QE 475 MeV to 3 GeV Boosting : E QE 300 MeV to 3 GeV - PowerPoint PPT PresentationTRANSCRIPT
MiniBooNE Low Energy Analysis
H. RayLos Alamos National Laboratory
H. Ray 2
Oscillation Fit Reporting
The final fit for e oscillations was performed using 2 different analysesTrack Based : E
QE 475 MeV to 3 GeVBoosting : E
QE 300 MeV to 3 GeV
Increased from 300 MeV due to 2 fit of 1% in Evis variable during 1st step of unblinding process
H. Ray 3
Oscillation Fit Reporting
We felt that we had checked everything to our full ability, and to our best knowledge could not further constrain processes in the low E region
MC studies of potential LSND oscillation signals indicated we could tighten the E requirement with a negligible loss in sensitivity
Prior to unblinding, we agreed to also examine events with E
QE > 300 MeV in the Track Based analysis
H. Ray 4
Observed Event Distribution
H. Ray 5
Observed Event Distribution
Counting Expt :300 MeV < E
QE< 1.250 GeV749 observed evts631 ± 25 ± 45 expected eventsExcess over background : 2.3
Background-subtracted
475 MeV to 3 GeV
H. Ray 6
Observed Event DistributionBackground-subtracted
475 MeV to 3 GeV
Counting Expt : 300 MeV < E
QE< 475 MeVExcess over background : 3.7
H. Ray 7
Observed Event DistributionBackground-subtracted
Best Fit (sin22, m2) = (1.0, 0.03 eV2)
300 MeV to 3 GeV
Only 4% Compatible w/LSND
Excluded by Bugey!
2 Probability: 18%, Null Hypothesis= 3%
H. Ray 8
What are the Low-E Events?
These low Energy events could be many things
We saw these events for the first time on Monday, March 26th (2007)
The following presents our very preliminary investigations to date
H. Ray 9
Fit Energy Event Composition
Boost Analysis 300 MeV to 3 GeV
Other12%
NCpi018%
Rad. Delta4%
K+26%
Ko6%
Mu+33%
Pi+1%
Other37%
Rad. Delta4%
K+10%
Ko3%
Mu+13%
Pi+0%
NCpi033%
Likelihood Analysis 475 MeV to 3 GeV
intrinsic e
mis-id
H. Ray 10
Low Energy Event Composition
Other30%
NCpi029%
Rad. Delta18%
K+5%
Ko1%
Mu+17%
Pi+0%
Other28%
Rad. Delta18%
K+7%
Ko2%
Mu+19%
Pi+0%
NCpi026%
Boost Analysis 300 MeV to 475 MeV
Likelihood Analysis 300 MeV to 475 MeV
intrinsic e
mis-id
H. Ray 11
Fundamental Information
Shutdowns
Low E events show no bias in event time
369 events 369 events
Not normalized to POT
H. Ray 12
Cosmic RaysMeasured from our strobe data
Cosmic events populateupper region of tank
Low E events show no bias in Y (vertical) position
2 expected evts in osc. analysis
369 events
H. Ray 13
Radiative Delta and NC0
Constrain our NC0
production rate using data from our detector Reduces error on mis-id 0 (<2%!)
This also constrains the radiative resonance rate, thus constraining rate of N
H. Ray 14
What we know so farLow E events pass EM Particle ID
Gamma or electronThe evts do not appear to be biased in
run range or event timeThe evts do not appear to be due to
cosmic ray backgroundRadiative Delta : unlikely = need x3
increase NC0 : unlikely = measure very well with
our data
H. Ray 15
SummaryA two-neutrino appearance only
model systematically disagrees with the shape of the excess as a function of E
Need to investigate non-oscillation explanations of the low E excess
Investigation of these low E events is underway
H. Ray 16
Final Results
Any conclusions drawn about the low E events will have no effect on our oscillation result