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A Measurement of the Ultra-High Energy Cosmic Ray Spectrum with the HiRes FADC Detector

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Stereo observation of the cosmic ray flux yields a better resolution in geometry ... The analysis of stereo events is currently under way. ... – PowerPoint PPT presentation

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Title: A Measurement of the Ultra-High Energy Cosmic Ray Spectrum with the HiRes FADC Detector


1
A Measurement of the Ultra-High Energy
Cosmic Ray Spectrum with the HiRes FADC Detector
  • Andreas Zech
  • Rutgers University
  • for the HiRes Collaboration
  • CRIS 04 (May 31st , 2004)

2
Outline
  • Monocular vs. Stereoscopic Observation
  • HiRes FADC Event Reconstruction
  • Monte Carlo Simulation Programs
  • Data / Monte Carlo Comparisons
  • The HiRes-2 Energy Spectrum
  • Studies of Systematic Effects on the Aperture

3
  • The two HiRes Detectors
  • HiRes-1
  • taking data since 1997
  • 1 ring with 21 mirrors ( elev. 3o to 17o)
  • Sample Hold Electronics ( 5.6 ?s )
  • HiRes-2
  • started data taking in 1999
  • 2 rings with 42 mirrors (elev. 3o to 31o)
  • FADC electronics recording at 10 MHz.

4
Seeing more with one eye closed ?!?
5
Measuring the Energy Spectrum with HiRes
  • Analyzing our data in monocular mode has
    some advantages
  • better statistics at the high energy end due to
    longer lifetime of HiRes-1.
  • extension of the spectrum to lower energies due
    to greater elevation coverage and better time
    resolution of HiRes-2.
  • Stereo observation of the cosmic ray flux
    yields a better resolution in geometry and energy
    than monocular.
  • gt HiRes is a stereoscopic detector. The
    analysis of stereo events is currently under way.

6
Mono versus Stereo Energy Measurements
HiRes-1 mono vs. stereo
  • The HiRes monocular energy is in excellent
    agreement with stereoscopic measurements !

7
HiRes FADC Event Reconstruction
8
  • 1. Reconstruction of the
  • shower-detector-plane
  • project signal tubes onto the sky
  • fit tube positions to a line
  • reject tubes that are off-track (and off in
    time) as noise
  • gt the detector position and fitted line define
    the shower-detector-plane.

9
2. Reconstruction of the geometry within the
s-d-plane
10
Shower Profile Energy Reconstruction
  • Reconstruct charged particle profile from
    recorded p.e.
  • Subtract Cerenkov light.
  • Fit G.H. function to the profile.
  • Multiply by mean energy loss rate ? gt
    calorimetric energy
  • Add missing energy (muons, neutrinos, nuclear
    excitations 10) gt total energy

11
Monte Carlo Simulation Programs
12
The Role of Monte Carlo Simulations in the HiRes
Experiment
  • We need M.C. to calculate the acceptance of our
    detectors for the flux measurement
  • M.C. is also a powerful tool for resolution
    studies.
  • This requires a simulation program that
    describes the shower development and detector
    response as realistically as possible.

13
HiRes Monte Carlo Simulation
14
Varying Run Parameters
  • Trigger gains
  • Dead mirrors
  • Livetime
  • gt Nightly Database
  • Light pollution
  • gt Average for each data set
  • Atmospheric Density
  • gt Seasonal variations
  • Weather
  • gt strict cuts based on hourly observation
  • Aerosols
  • gt atmospheric database from laser shots
  • gt currently, we use average values

15
Data / Monte Carlo Comparisons Resolution
16
Photoelectrons per degree of track
  • black HiRes-2 data
  • red Monte Carlo
  • (5 x data statistics)
  • data
  • Monte Carlo

17
Distance to the shower axis (Rp)
18
? - Angle
19
Energy Resolution
  • (Erec - Etrue)
  • Etrue
  • ? 16

20
? Resolution
?rec. - ?true
? 5 deg
21
The HiRes-2 Energy Spectrum
22
HiRes-2 Exposure
fit to the exposure
Flux
23
HiRes-2 Energy Spectrum
  • statistics
  • 123 good nights,
  • 536 hours live time,
  • 6320 events with reconstructed geometry,
    2685 events after final cuts

24
The HiRes Mono Spectra
  • HiRes-1
  • 97 - 04
  • HiRes-2
  • 99 - 01

25
HiRes Mono and Flys Eye Stereo
  • HiRes-1
  • HiRes-2
  • Flys Eye stereo

26
Systematic Uncertainties
27
Systematic Uncertainties
  • Systematic uncertainties in the energy scale
  • absolute calibration of phototubes /- 10
  • fluorescence yield /- 10
  • correction for unobserved energy /- 5
  • aerosol concentration lt 9
  • atmospheric uncertainty in aperture
  • gt total uncertainty in the flux /- 31
  • What uncertainties in the aperture are
    introduced with our inputs to the Monte Carlo ?
    (i.e. input spectrum, composition, atmosphere)

28
Systematics due to the Input Energy Spectrum
  • A fit to the Flys Eye Stereo spectrum is used
    as an
  • input to the Monte Carlo.

29
Flys Eye vs. E-3 input spectrum
30
A bias that we are avoiding...
aperture using E-3 input spectrum aperture using
Flys Eye input spectrum
  • Assuming a wrong ( E-3 ) input spectrum would
    cause us a bias of 20 in the
    aperture.

31
Systematics due to the Input Composition
The input composition ( fraction of proton
and iron showers) is chosen from HiRes
Stereo and HiRes/MIA
measurements.
32
Exposures for pure proton / pure iron
  • lower acceptance for iron at low
    energies (lt 10 18.5 eV )
  • agreement at higher energies.

33
Systematic Uncertainty due to Input Composition
  • We assume a /- 20 uncertainty in the proton
    fraction from HiRes / MIA HiRes Stereo
    measurements.
  • This is a conservative estimate of the
    uncertainties in the composition.
  • A new composition measurement is needed !
  • gt HiRes , TA/TALE

black stat. errors red sys.
uncertainty
34
Systematics due to Aerosol
  • We are currently using a measurement of the
    average aerosol content of the atmosphere for our
    analysis.
  • What is the systematic effect on the energy
    resolution and aperture due to this assumption?
  • ( This is work in progress ... )

35
Atmospheric Database
09/00 - 03/01 clear nights
  • Aerosol VAOD measurement using vertical laser
    tracks.
  • Aerosol Horizontal Extinction Length from
    horizontal laser shots.

ltVAODgt 0.034
Preliminary
09/00 - 03/01 clear nights
lt1/hxlgt -1 20.8 km
36
Systematic Effect on Reconstructed Energies (MC
study)
? 17.5
  • Energy Resolution for
  • MC with atmos. database,
  • reconstructed with database

Energy Resolution for MC with atmos.
database, reconstructed with average
37
Systematic Effects on the Aperture
  • Ratio of Apertures
  • numerator using MC with atmos. db. ,
    reconstructed with atmos. db.
  • denominator using MC with atmos. db. ,
    reconstructed with average

38
Conclusions
  • Measurements of the Cosmic Ray Flux in monocular
    mode cover a wider energy range than in
    stereoscopic mode while providing very good
    energy resolution.
  • Our Monte Carlo Programs simulate all aspects of
    our experiment in a realistic way.
  • We have investigated systematic uncertainties
    related to the input spectrum, input composition
    and the aerosol content of the atmosphere.
    Further studies of atmospherics
    are under way.
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