Title: A Measurement of the Ultra-High Energy Cosmic Ray Spectrum with the HiRes FADC Detector
1A 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)
2Outline
- 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.
4Seeing more with one eye closed ?!?
5Measuring 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.
6Mono versus Stereo Energy Measurements
HiRes-1 mono vs. stereo
- The HiRes monocular energy is in excellent
agreement with stereoscopic measurements !
7HiRes 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.
92. Reconstruction of the geometry within the
s-d-plane
10Shower 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
11Monte Carlo Simulation Programs
12The 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.
13HiRes Monte Carlo Simulation
14Varying 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
15Data / Monte Carlo Comparisons Resolution
16Photoelectrons per degree of track
- black HiRes-2 data
- red Monte Carlo
- (5 x data statistics)
- data
- Monte Carlo
17Distance to the shower axis (Rp)
18? - Angle
19Energy Resolution
- (Erec - Etrue)
- Etrue
-
- ? 16
20? Resolution
?rec. - ?true
? 5 deg
21The HiRes-2 Energy Spectrum
22HiRes-2 Exposure
fit to the exposure
Flux
23HiRes-2 Energy Spectrum
- statistics
- 123 good nights,
- 536 hours live time,
- 6320 events with reconstructed geometry,
2685 events after final cuts
24The HiRes Mono Spectra
- HiRes-1
- 97 - 04
- HiRes-2
- 99 - 01
25HiRes Mono and Flys Eye Stereo
- HiRes-1
- HiRes-2
- Flys Eye stereo
-
26Systematic Uncertainties
27Systematic 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)
28Systematics due to the Input Energy Spectrum
- A fit to the Flys Eye Stereo spectrum is used
as an - input to the Monte Carlo.
29Flys Eye vs. E-3 input spectrum
30A 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.
31Systematics due to the Input Composition
The input composition ( fraction of proton
and iron showers) is chosen from HiRes
Stereo and HiRes/MIA
measurements.
32Exposures for pure proton / pure iron
- lower acceptance for iron at low
energies (lt 10 18.5 eV ) - agreement at higher energies.
33Systematic 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
34Systematics 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 ... )
35Atmospheric 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
36Systematic 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
37Systematic 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
38Conclusions
- 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.