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Combined energy spectrum of the Pierre Auger Observatory

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Title: Combined energy spectrum of the Pierre Auger Observatory


1
Combined energy spectrum of the Pierre Auger
Observatory
  • V. M. Olmos Gilbaja
  • Universidade de Santiago de Compostela
  • Instituto Galego de Física de Altas Enerxías

2
Differential flux
Energy reconstruction to count events in energy
bin Exposure at that energy
3
Introduction
  • 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

4
Energy 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

5
Energy 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

6
Exposure 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
7
Exposure 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
8
Individual spectra
  • Hybrid spectrum
  • SD spectrum

9
Energy 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

10
Combining 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

11
Combined spectrum of thePierre Auger Observatory
12
Conclusions
  • 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

13
BACK UP SLIDES
14
Event example
15
Spectrum
?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
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