Title: Combined energy spectrum of the Pierre Auger Observatory
1Combined energy spectrum of the Pierre Auger
Observatory
- V. M. Olmos Gilbaja
- Universidade de Santiago de Compostela
- Instituto Galego de FÃsica de Altas EnerxÃas
2Differential flux
Energy reconstruction to count events in energy
bin Exposure at that energy
3Introduction
- Two independent techniques are used in the Pierre
Auger Observatory - Ground array of more than 1600 detectors
- 24 fluorescence telescopes
- Ground array ? high duty cycle ? sensitive to
highest energies - Fluorescence detector ? using events detected in
coincidence with at least one surface detector ?
extension of the spectrum down to 1018 eV
4Energy reconstruction with FD
- Determine the shower geometry
- Account for the Cherenkov contribution and the
light scattering and attenuation - Obtain the energy deposit from the absolute
fluorescence yield - Fit of a Gaisser - Hillas to measured energy
deposit
5Energy reconstruction with SD
- Obtain the axis of the air shower from arrival
time measurements - Fit of a Lateral Distribution Function to
measured signals - Obtain signal at 1000 m S(1000)
- Account for the attenuation with zenith angle
using a CIC method obtaining S38º - Obtain the energy through a correlation of S38º
with the fluorescence measurement of energy using
hybrid events
6Exposure to hybrid events
- The calculation of the hybrid exposure requires
the knowledge of the detector on-time - Detection efficiency is influenced by external
(lightnings) or internal (data acquisition
failures) factors - A Monte Carlo method which reproduces the data
taking conditions including their time
variability has been used to derive the exposure
of the hybrid detection.
Corrected by 4 after validating the Monte Carlo
with air shower observations
systematic due to unknown primary composition
7Exposure to SD events
- Above saturation of trigger efficiency the
acceptance becomes purely geometrical - The exposure is obtained integrating over time
the unitary acceptance per detector - Monitoring information of active detectors
provide information to determine the exposure
with an uncertainty below 3 - Total exposure between Jan 2004 and Dec 2008 is
12790 km2 sr yr
? 4.59 km2 sr between 0º and 60º
8Individual spectra
9Energy Scale Systematics
- Absolute Fluorescence Yield 14
- Pressure dependence of Fluorescence Yield 1
- Humidity dependence of Fluorescence Yield 1
- Temperature dependence of Fluorescence Yield 5
- FD absolute calibration 11
- FD wavelength dependence response 3
- Rayleigh scattering in atmosphere 1
- Wavelength dependence of aerosol scattering 1
- FD reconstruction method 10
- Invisible energy 5
- Total 22
10Combining spectra
- Maximum likelihood method accounting for
systematic and statistical uncertainties - Flux scale parameters of kSD 1.01 and kFD
0.99 show the good agreement between independent
measurements - Systematic uncertainty of the combined flux below
4
11Combined spectrum of thePierre Auger Observatory
12Conclusions
- Two independent measurements of the cosmic ray
energy spectrum with the Pierre Auger Observatory
have been presented - Both measurements have the same systematic
uncertainty in the energy scale - Combining both spectra enables the measurement of
the ankle and the flux suppression at the highest
energies - Some comparisons with astrophysical models have
been performed
13BACK UP SLIDES
14Event example
15Spectrum
?1 3.26 log(E/eV) 18.61 ?2
2.59 18.61 log(E/eV) 19.46 ?3 4.3
19.46 log(E/eV) log(E1/2/eV)
19.61 log(Wc/eV) 0.16