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Published byBertram Melvyn Houston Modified over 9 years ago
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Exploring Laser Light Ruben Conceição
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Pierre Auger Observatory Ultra High Energy Cosmic Rays Pierre Auger Observatory – Fluorescence Detector Longitudinal Profile Fluorescence light – Surface Detector Ground charged lateral distribution Ruben Conceição2Sesimbra, IDPASC 2010
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Following the light FD Point Spread Function Multiple Scattering Ruben Conceição3Sesimbra, IDPASC 2010
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Zeta Measuring the differential light profiles Angular distance to spot center: – Zeta ( ) Evaluate – By using – Measured in each pixel i Average many profiles to reduce statistical fluctuations – Need to control Event similarity Clouds Undershooting Applicable in full camera acquisition or in a band! CLF shot seen at LL with full camera aquisition Ruben Conceição4Sesimbra, IDPASC 2010
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CLF @ Coihueco Light lateral profile vs. angular distance to spot center (zeta) Direct light Detector PSF Multiple Scattering
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CLF @ Coihueco Total light vs. elevation angle (several millions CLF shots) Mie Rayleigh The shape of the light profile is sensitive to VAOD
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Geant4 Laser Simulation Photon tracking in the atmosphere done with Geant4: – Rayleigh scattering – Mie scattering Layers with constant depth (20 g/cm2) Different atmospheric profiles Detectors implemented as cone sections, 2 m height to simulate camera aperture and inclination. Can suffer any number of Mie or Rayleigh scatterings Comparison between data and simulation Ruben Conceição7Sesimbra, IDPASC 2010
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Conclusions Powerful tools for understanding the multiscattered light – Further studies to check the dependency with altitude, time of arrival and distance can be done First data/MC comparison results are encouraging – Reasonable agreement The detector PSF can be acquired up to 10 -4 of maximum signal
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BACKUP Ruben Conceição9Sesimbra, IDPASC 2010
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CLF @ Los Leones Ruben Conceição10Sesimbra, IDPASC 2010
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