Geant4 Simulation of the Pierre Auger Fluorescence Detector

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Presentation transcript:

Geant4 Simulation of the Pierre Auger Fluorescence Detector Pedro Assis1, Patrícia Gonçalves1, Libor Nozka2, Mário Pimenta1, Bernardo Tomé1 1- Laboratório de Instrumentação e Física Experimental de Partículas (LIP), Lisboa, Portugal 2 - Institute of Physics of the Academy of Sciences of the Czech Republic, Praha, Czech Republic 11th Geant4 Collaboration Workshop and Users Conference 9-14 October 2006 LIP - Lisboa & IST - Lisboa

Ultra High Energy Cosmic Rays (UHECR) Charged Cosmic Rays Spectrum Many questions: Sources ? Acceleration mechanisms ? GZK cutoff ? Same physics laws ? A ver: Interesse de UHECR Interesse de Auger ; Futuro de Auger. EGRET (Energetic Gamma Ray Experiment Telescope) all sky map: Vela, Geminga & Crab pulsars ; AGN 3C279 ~300 sources @ the GeV scale, only a few @ the TeV; Ver INTEGRAL Arranjar plot de interaction length dos gammas que va ate 10^20 eV E > 1020 eV !

UHECR detection Extensive Air Showers (EAS) Light detection from space Fluorescence from air N2 molecules isotropic emission along the shower Cherenkov light collimated with the shower Fluorescence: 4-5 photons/m per ionizing particle. Direct detection of shower particles Scintillators, Cherenkov radiators (e.g. water),...

The Southern Pierre Auger Observatory A giant hybrid detector in Argentina FOV = 30o x 30o telescope building “Los Leones” LIDAR station communication tower Cherenkov water tank Surface Array 1600 detector stations; 1.5 Km spacing; 3000 Km2 . Representar o FOV em azimuth de um telescópio. Fluorescence Detectors 4 housings; 6 telescopes in each; Malargue, Argentina

Schmidt optics

Corrector ring Ring shaped lens to increase the telescope aperture (~2x); No significant degradation of optics performance. Toroidal profile

Corrector ring in Geant4 - G4Polycone; - Discretization of ring profile: Equidistant slices along Z ; Ri vs Zi from ring profile equation. R1 R2 RN Z1 Z2 ZN ... N - to be optimized...

Corrector ring in Geant4

Mirror 3.5 x 3.5 m2 spherical mirror; 3.4 m curvature radius; Made of square or hexagonal mirror segments (MS) with spherical curvature; Hexagonal MS mirror implemented in the simulation. 4 different MS shapes to fit the mirror curvature: Each mirror is made of 60 mirror segments.

Mirror segments (MS) in Geant4 Union of G4Trd solids ; Intersection of resulting boolean solid with a G4Sphere. (Rmin = Radius of curvature; Rmax = Rmin + thickness) The four MS types are described in the simulation. MS parameters (curvature, reflectivity, distance to camera) are read for each fluorescence telescope ; Access to a mirror segment DB is also possible.

Assembled mirror

Camera Camera frame Spherical focal surface; Hexagonal PMT´s; Reflecting light guides (“Mercedes”) to maximize light collection. 6 “Mercedes” light collectors

Mercedes light collectors in Geant4 Union of 3 G4Polyhedra solids

Assembled camera PMTs described as hexagonal volumes (shown in red) and defined as sensitive volumes.

Assembled telescope

Seeing light...

Some very preliminary results

Mirror “X-ray” Uniform illumination of the mirror (q=0o) ; Photon positions detected behind the mirror.

Camera “X-ray” Uniform illumination of the camera (q=0o); Average photon distribution over the PMT surface: Effect of non-uniformities of photocathodes can be introduced in the simulation.

PSF vs theta – an example 10 mm q=0o q=5o q=10o q=15o

Direction Scans Th=0º; Phi=0º

Direction Scans Th=15º; Phi=0º

Direction Scans Th=30º; Phi=0º

Position Scans Spots at Phi=0º; 90º; 180º; 270º Photons direction: Th=0º; Phi=0º

Position Scans Spots at Phi=0º; 90º; 180º; 270º Photons direction: Th=0º; Phi=0º

Position Scans Spots at Phi=0º; 90º; 180º; 270º Photons direction: Th=15º; Phi=0º

Position Scans Spots at Phi=0º; 90º; 180º; 270º Photons direction: Th=0º; Phi=0º

A SHOWER… 1000 Photons

A SHOWER… 100 Photons

A SHOWER… 100 Photons

A SHOWER… 100 Photons

A SHOWER… 1000 Photons

Summary A full Geant4-based simulation of the Auger fluorescence detectors was developed; Integration in the Auger simulation chain is being carried; Detailed comparisons with the ray-tracing software will be performed.

Optics of Auger Fluorescence Detectors Schmidt optics telescope. Mirror: f/1 spherical mirror ; 3.5 m x 3.5 m; PSF = 0.5o. Camera: 440 hexagonal pixels/PMT´s; 1.5o x 1.5o pixel FOV; Spherical focal surface. Diaphragm centered on the center of curvature of the mirror: - Ver que simulacoes do FD existem; - Ver a calibração do sistema óptico. Full Geant4 simulation will be implemented at LIP. Other LIP activities: Reconstruction and analysis of the Fluorescence Detectors data; Calibration at CERN testbeam facilities of a water tank using horizontal muons.