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A Cross Check of Atmospheric Attenuation for the High Resolution Fly’s Eye Astroparticle Experiment Chris Cannon Advisor: Lawrence Wiencke University of.

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Presentation on theme: "A Cross Check of Atmospheric Attenuation for the High Resolution Fly’s Eye Astroparticle Experiment Chris Cannon Advisor: Lawrence Wiencke University of."— Presentation transcript:

1 A Cross Check of Atmospheric Attenuation for the High Resolution Fly’s Eye Astroparticle Experiment Chris Cannon Advisor: Lawrence Wiencke University of Utah 1.Cosmic rays above 10 17 eV; the highest energy particles 2.Atmospheric attenuation plays a significant role in detector calibration. 3.Cross check atmospheric calibration 4.Results 5.Conclusion

2 At energies above 10 20 eV the flux is extremely low!!! Namely 1 particle/km 2 -steradian/century Flux E^3 Cosmic Ray Energy Spectrum Man-made accelerators

3 Using the Atmosphere as a Detector

4 Introducing High Resolution Fly’s Eye (HiRes)

5 Mirror PMT Cluster HiRes Camera

6 Display of a Sample Air Shower

7 The Atmosphere – Two Components Vertical Aerosol Optical Depth (VAOD) is the optical thickness of the aerosol component of the atmosphere. Transmission(aerosol) = e -VAOD Molecular Aerosols

8 Measuring VAOD with Atmospheric Lasers HiRes-1 detector HiRes-2 laser system 12.6 km Average VAOD: 0.04 +-.02

9 Measuring VAOD with Cosmic Rays Reality Erroneous Simulation - Overcorretion Erroneous Simulation - Undercorrection detector 1 detector 2 apparent shower 1 apparent shower 2 apparent shower 1 apparent shower 2

10 Data Selection Start with 2079 cosmic rays seen by both detectors. Require that: The two detectors see a common portion of the shower. Each detector must collect at least 1000 photons from the common track segment, which must be at least 5 degrees long. The probability that the event is noise based on a random walk model is less than 5%. The event is downward going. The opening angle between shower-detector planes is greater than 25 degrees. The scattering angle is at least 25 degrees. 1218 cosmic ray events remain. Purpose of Cuts: Remove noisy, dim events. Ensure good geometry. Remove Cherenkov dominated events.

11 Use the segment of the shower viewed by both detectors. Profile integration Luminosity (photons/m) Distance from Gound (m)

12 Plotting Data Difference in distance between detectors and shower Difference in shower brightness- 0 + Greater distance brighter shower. The atmosphere is over-corrected. Greater distance dimmer shower. The atmosphere is under-corrected.

13 Results Simulated Atmosphere Canonical Model Measured Average No Aerosols Comment Over-correction Under-correction

14 Conclusion: Using lasers.04 +-.02 Using cosmic rays.043 +-.001 (stat) VAOD Measurement

15 Effect of Atmospheric Calibration 1999 2003 With Model Atmosphere With Measured Atmosphere

16 Greisen-Zatsepin-Kuzmin (GZK) Cutoff Charged particles with E > 5 x 10 19 eV will travel at most 100 Mpc before their energy drops below the cutoff.

17 HiRes Atmospheric Works in Progress Improved atmospheric monitoring: Hourly aerosol corrections instead of average. Cloud monitoring.

18 Sources of Cosmic Rays êThe Sun êSolar Wind êLow Energy < 10 GeV êSupernovae Capable of accelerating particles to 10 15 eV êAGNs / GRBs … Possible sources for UHECRs

19 Requirements on acceleration size and field strength

20 Use Timing…. Depth Perception is Limited Need to measure a change in angular velocity Equal Angle Bins detector shower RpRp ψ Works best with Longer track Larger Rp Smaller ψ Geometry with One Eye


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