Title: Unfolding atmospheric neutrino spectrum with IC9 data (second update)
1Unfolding atmospheric neutrino spectrum with IC9
data (second update)
4 / 4 / 2007
2Upgrades
- Use of the energy estimate of Rime
- Smearing matrix build with a distribution closer
to what we expect to measure
3Reminder How to choose the best variable?
- Criteria
- As much linear as possible with energy
- With the least spread
- Possible candidates nchan, tot_charge, energy
estimator
4log10 of Total charge
delta
log10 Charge (pe)
log10 Charge (pe)
log10 Enu GeV
log10 Enu GeV
RMS 0.42
RMS is related with the quality of the fit
deviation from fit / delta
Y-projection
log10 Enu GeV
5log10 of estimator
log10 estimator
log10 estimator
log10 Nchan
log10 Enu GeV
log10 Enu GeV
log10 Nchan
deviation from fit / delta
log10 Nchan
log10 Enu GeV
6MC samples
- Neutrino events 50 x 106 (?-2)
- (dataset 437)
- CORSIKA 1000 x 106
- (dataset 296)
- Coincident muons 3000 x 106
- (dataset 394)
(files had to be reprocess to include the energy
estimator)
7Spectral index for simulation
- It is convenient to generate the MC sample in
such a way that generated/expected is flat (more
efficient smearing matrix calculation, smoother
distribution to unfold)
dataset 437 (?-2)
dataset 390 (?-1)
With ?-2, we avoid to generate too many useless
high energy events
8Generated / expected
dataset 437 (?-2)
dataset 390 (?-1)
Flatter ratio between generated and
expected Still, statistics could be not enough
(factor 10 more)
9Processing
- First guess with line fit
- The result is used to feed the LLH
- Quality cuts are applied after processing
10Ndir ? 8, Ldir gt 200 m, ? gt 92?
atmospheric neutrinos 671 corsika events
13 coincident muons 2.6
purity 98
11Unfolding initial distribution
- In unfolding problems, it is usually very useful
to have an idea of the distribution we want to
unfold. - BUT the robustness of our method against our
choice of the initial distribution has to be
checked.
12Smearing matrix
Maybe more statistics are still needed
13Measured distribution
(background from single and double atmospheric
muons already included)
14Unfolded spectrum
Using Singular Value Decomposition
15Deviation from the true spectrum
16New initial spectrum
- We have to make things harder to the algorithm,
to check its robustness
17The unfolded spectrum follows well the true
spectrum A more systematic way of robustness
check is underway
18Difference between true and unfolded
19Summary and Prospects
- Energy estimate shows better behavior as energy
correlated variable - The new MC (gamma-2) offers flatter generate /
expected distribution - Good quality of unfolding even when the initial
spectrum is different from the true one - To do list
- More statistics for smearing matrix
- Combine different variables (?)
- Continue on optimization of cuts
- Tuning of regularization constant and other
internal parameters