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The Aperture and Precision of the Auger Observatory

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Title: The Aperture and Precision of the Auger Observatory


1
The Aperture and Precision of the Auger
Observatory
  • M. Ave, R. Cester, B.R. Dawson, J. Lloyd-Evans,
    P. Sommers and A.A. Watson
  • for the Pierre Auger Observatory Collaboration

2
Plan
  • The Pierre Auger Observatory is a hybrid
    detector
  • Surface Detectors
  • Surface Detector Aperture and Resolution
  • Fluorescence Detectors
  • Hybrid Reconstruction of Shower Axis
  • Hybrid Aperture and Resolution

3
Introduction
  • Mendoza Province, Argentina
  • 3000 km2, 875 g cm-2
  • 1600 water Cherenkov detectors 1.5 km grid
  • 4 fluorescence eyes -total of 30 telescopes each
    with 30o x 30o FOV

65 km
4
Introduction
  • The Pierre Auger Project is a Hybrid detector
  • Surface Detectors (SD) and Fluorescence Detectors
    (FD)
  • shower development Nch(X) recorded by FD
  • snapshot of shower front captured by SD
  • at depth where particle densities at large core
    distances are near their maximum values

5
Why a Hybrid Observatory?
  • Hybrid resolution of arrival directions, energies
    and masses is superior to that achieved by the SD
    or a single FD eye independently
  • Rich set of measurements on each hybrid EAS
  • SD and FD measure cosmic ray parameters using
    different methods with different systematic
    errors
  • Cross-checks and control of systematics.
  • while the FD only operates with a duty cycle
    of10, the Hybrid observations will allow
    confident analysis of SD data taken without FD
    coverage.

6
e.g. Measurements of Energy
  • SD alone E from estimates of water Cherenkov
    density 1000m from the shower core
  • requires conversion factor from EAS simulations
  • FD alone E from estimates of energy deposition
    in the atmosphere (light a dE/dX).
  • requires knowledge of atmospheric transmission.
  • two methods can be compared with Hybrid
  • Checks simulations and measurement systematics

7
Surface Detectors
  • for SD-only operation, typically will require 5
    stations at the 4 vem trigger level (lt 20 Hz per
    station)
  • standard techniques for direction and core
    finding. Several LDFs under study, including a
    modified Haverah Park function.
  • 10 m2, 1.2 m depth, 3 PMTs, 40 MHz FADC
  • Integrated signal expressed in units of vertical
    equivalent muons (1 vem 100 pe)

8
Surface Detectors
1019eV proton
  • SD water Cherenkov detectors measure muon,
    electron and gamma components of EAS, the latter
    especially important at large core distances

9
Surface Detector Resolution
  • SD Angular resolution E gt 1019eV

q (deg) Proton/Iron Proton/Iron Photon
Egt1019eV Egt1020eV Egt1019eV
20o 1.1o 0.6o 4.0o
40o 0.6o 0.5o 2.5o
60o 0.4o 0.3o 1.0o
80o 0.3o 0.2o 1.0o
10
Surface Detector Resolution
  • Energy determined from fitted density at 1000m,
    r(1000). Conversion factor from simulations
    averaged for p and Fe primaries. E gt 1019
    eV rms E resolution 12
    (assuming p/Fe mixture)

11
SD Aperture and Event Rate
Eo (eV) Trig Aperturekm2sr Rate per yeargt Eo
1018 0 0
3x1018 2200 15000
1019 7200 5150
2x1019 7350 1590
5x1019 7350 490
1020 7350 100
2x1020 7350 30
  • Zenith lt 60o, based on AGASA spectrum (Takeda et
    al 1998)
  • (Zenith gt 60o adds about 50 to event rate)

12
Auger Southern Site
  • Hybrid reconstruction works when a shower is
    recorded by the surface array and at least one
    eye
  • This multiple-eye design reduces our reliance on
    precise knowledge of atmospheric attenuation of
    light
  • Mean impact parameter at 1019eV is 13km

13
Fluorescence Detector
Schmidt aperture stop
3.8m x 3.8m prototype mirrorand camera
440 pixel camera 30ox30o
14
Fluorescence Detectors
2 equipped bayslooking over the engineering array
15
Hybrid Reconstruction of Axis
  • good determination of shower axis is vital for
    origin studies, but also vital as first step
    towards good energy and mass composition
    assignment
  • use eye pixel timing and amplitude data together
    with timing information from the SD.
  • GPS clocks in SD tanks and at FDs.
  • Hybrid methods using one eye give angular
    resolution comparable to stereo reconstruction

16
Hybrid Reconstruction (Cont.)
  • eye determines plane containing EAS axis and eye
  • plane normal vector known to an accuracy of
    0.2o
  • to extract Rp and y, eye needs to measure angular
    velocity w and its time derivative dw/dt
  • but difficult to get dw/dt, leads to degeneracy
    in (Rp,y)
  • degeneracy broken with measurement of shower
    front arrival time at one or more points on the
    ground
  • eg at SD water tank positions

17
Hybrid Reconstruction (Cont.)
  • Simulations at 1019eV
  • Reconstruct impact parameter Rp. Dramatic
    improvement with Hybrid reconstruction

18
Simulated Hybrid Aperture
Hybrid TriggerEfficiency
Stereo Efficiency
  • Note the significant aperture at 1018eV, and the
    stereo aperture at the higher energies
  • Trigger requirement at least one eye triggering
    on a track length of at least 6 degrees two
    surface detectors. q lt 60o
  • Hybrid Aperture Hybrid Trigger efficiency x
    7375 km2sr

19
Hybrid Reconstruction Quality
E(eV) Ddir (o) DCore (m) DE/E () DXmaxg/cm2
1018 0.7 60 13 38
1019 0.5 50 7 25
1020 0.5 50 6 24
statisticalerrors only
zenith angles lt 60O
  • 68 error bounds given
  • detector is optimized for 1019eV, but good Hybrid
    reconstruction quality at lower energy

20
Conclusions
  • the Hybrid nature of the Pierre Auger Observatory
    is a unique feature of the detector
  • it offers a large set of gold-plated events
    during the 10 of time when both fluorescence and
    surface detectors are operating
  • just as importantly, it provides cross-checks and
    justification to the collaboration and the
    community for the techniques used in analyzing
    the bulk of the data, that viewed by the surface
    array only
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