Monte Carlo Studies for a Future Instrument. Stephen Fegan Vladimir Vassiliev UCLA

Similar documents
VERITAS Design. Vladimir Vassiliev Whipple Observatory Harvard-Smithsonian CfA

Monte Carlo Studies for CTA

Monte Carlo Simulation and System Layout

THE PATH TOWARDS THE CHERENKOV TELESCOPE ARRAY OBSERVATORY. Patrizia Caraveo

VHE Gamma-Ray Future Project: Beyond CANGAROO

Simulations for H.E.S.S.

Status and Future of the HESS experiment

GAMMA-RAY ASTRONOMY: IMAGING ATMOSPHERIC CHERENKOV TECHNIQUE FABIO ZANDANEL - SESIONES CCD

AGIS (Advanced Gamma-ray Imaging System)

THE PATH TOWARDS THE CHERENKOV TELESCOPE ARRAY OBSERVATORY. Patrizia Caraveo

The H.E.S.S. Standard Analysis Technique

Extreme high-energy variability of Markarian 421

Performance and Sensitivity of H.E.S.S.

VERITAS Observations of Starburst Galaxies. The Discovery of VHE Gamma Rays from a Starburst Galaxy

The TAIGA experiment - a hybrid detector for very high energy gamma-ray astronomy and cosmic ray physics in the Tunka valley

DATA ANALYSIS: EXTRACTING SCIENCE FROM MAGIC

The Cherenkov Telescope Array. Kevin Meagher Georgia Institute of Technology

Variable atmospheric transparency studies for the MAGIC telescopes

GRB observations at very high energies with the MAGIC telescopes

TenTen: A new IACT Array for Multi-TeV Gamma-Ray Astronomy

Feasibility of VHE gamma ray detection by an array of imaging atmospheric Cherenkov telescopes using the fluorescence technique

A Monte Carlo simulation study for cosmic-ray chemical composition measurement with Cherenkov Telescope Array

Cherenkov Telescope Arrays

arxiv: v1 [astro-ph.im] 7 Sep 2015

Ultra-High-Energy Cosmic Rays: A Tale of Two Observatories

The Cherenkov Telescope Array

Search for TeV Radiation from Pulsar Tails

Mirror Alignment and Optical Quality of the H.E.S.S. Imaging Atmospheric Cherenkov Telescopes

Recent Results from CANGAROO

REU Final Presentation: VERITAS Update. Summer 2011 Advisors: John Finley and Glenn Sembroski Purdue University By: Kara Ponder

Status of the MAGIC telescopes

Cosmic Ray Physics with the ARGO-YBJ experiment

Monte Carlo Studies of medium-size telescope designs for the Cherenkov Telescope Array

A Search for Point Sources of High Energy Neutrinos with AMANDA-B10

arxiv: v1 [astro-ph.im] 1 Sep 2015

Measurement of the CR e+/e- ratio with ground-based instruments

Primary CR Energy Spectrum and Mass Composition by the Data of Tunka-133 Array. by the Tunka-133 Collaboration

Cherenkov Telescope Array Status Report. Salvatore Mangano (CIEMAT) On behalf of the CTA consortium

Accurate Measurement of the Cosmic Ray Proton Spectrum from 100TeV to 10PeV with LHAASO

1 o.3. 0 o.5. Dec. 1 o.0 R.A. on 0. o 5 off 1. o 0 1. o

H.E.S.S. High Energy Stereoscopic System

Investigation of Observation Quality Parameters for H.E.S.S.-II

RECENT RESULTS FROM CANGAROO

arxiv: v1 [astro-ph.im] 24 Jun 2015

Stellar Intensity Interferometric Capabilities of IACT Arrays*

A model of the Earth's gamma-ray emission for GLAST derived from EGRET data. Dirk Petry (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29, 2005

The AUGER Experiment. D. Martello Department of Physics University of Salento & INFN Lecce. D. Martello Dep. of Physics Univ. of Salento & INFN LECCE

Kathrin Egberts Max-Planck-Institut für Kernphysik, Heidelberg for the H.E.S.S. Collaboration

Hadronic Interaction Studies with ARGO-YBJ

Very High-Energy Gamma- Ray Astrophysics

H.E.S.S. High Energy Stereoscopic System

arxiv: v1 [astro-ph] 26 Apr 2007

Gamma-ray Astrophysics

COSMIC RAY COMPOSITION.

The Whipple Collaboration

PoS(ICRC2017)945. In-ice self-veto techniques for IceCube-Gen2. The IceCube-Gen2 Collaboration

VERITAS Performance Gernot Maier

A METHOD TO ENHANCE THE SENSITIVITY OF PHOTOMULTIPLIERS FOR AIR CHERENKOV TELESCOPES

Comparing 2-Level and Time Next Neighbor Cleaning Protocols for Optimizing CTA Image Cleaning

X- & γ-ray Instrumentation

Status of the Small-Sized Telescopes of the Cherenkov Telescope Array

Advanced Stereoscopic Array Trigger. Frank Krennrich (Iowa State University)

Monte Carlo studies of CTA: an overview. Victor Stamatescu (University of Adelaide)

arxiv: v1 [astro-ph.im] 13 Sep 2017 Julian Sitarek University of Łódź, PL Lodz, Poland

The VERITAS Dark M atter and Astroparticle Programs. Benjamin Zitzer For The VERITAS Collaboration

The DISP analysis method for point-like or extended γ source searches/studies with the MAGIC Telescope

Cherenkov Telescopes for Gamma-Ray Astrophysics

The early days of ground-based gamma-ray astronomy in France. Gerard Fontaine - Hillas symposium Heidelberg December

CLASSIFICATION METHODS FOR MAGIC TELESCOPE IMAGES ON A PIXEL-BY-PIXEL BASE. 1 Introduction

Direct WIMP Detection in Double-Phase Xenon TPCs

arxiv: v1 [astro-ph.he] 28 Aug 2015

Improving H.E.S.S. cosmic-ray background rejection by means of a new Gamma-Ray Air Shower Parametrisation (GRASP)

The MAGIC gamma detector

VERITAS: exploring the high energy Universe

arxiv: v2 [astro-ph.im] 14 Mar 2016

Advanced Image Cleaning

VERITAS Observations of Supernova Remnants

Gamma-ray Astrophysics with VERITAS: Exploring the violent Universe

E. Caroli(1), R. M. Curado da Silva(2), J.B. Stephen(1), F. Frontera(1,3), A. Pisa (3), S. Del Sordo (4)

Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera

Detecting Gamma-Ray Bursts in the DC1 Data

Comparing Two-Level and Time Next Neighbor Cleaning Protocols for Optimizing CTA Image Cleaning

arxiv: v1 [astro-ph.im] 14 Sep 2017

arxiv: v1 [astro-ph.im] 26 Aug 2015

Application of an analysis method based on a semi-analytical shower model to the first H.E.S.S. telescope

Second large-scale Monte Carlo study for the Cherenkov Telescope Array

Observation of the Southern High Energy Peaked BL Lac Object PKS with CANGAROO-II Telescope

Study of Performance Improvement for Air Shower Array with Surface Water Cherenkov Detectors

The LHAASO-KM2A detector array and physical expectations. Reporter:Sha Wu Mentor: Huihai He and Songzhan Chen

Gamma/Proton separation study for the LHAASO-WCDA detector

arxiv:astro-ph/ v1 3 Dec 1997

The Gamma-ray Albedo of the Moon

Ultra-High Energy Particles Astronomy with a space-based experiment

arxiv:astro-ph/ v1 23 May 2000

Supernova Remnants as Cosmic Ray Accelerants. By Jamie Overbeek Advised by Prof. J. Finley

arxiv:astro-ph/ v1 4 Jul 2002

Analysis methods for Atmospheric Cerenkov Telescopes. Mathieu de Naurois

Measurement of a Cosmic-ray Electron Spectrum with VERITAS

CANGAROO-III: Status report

Rivelazione da terra di fotoni di alta energia

Transcription:

Monte Carlo Studies for a Future Instrument Stephen Fegan Vladimir Vassiliev UCLA

Approach to simulations CORSIKA 6200, 6500, 6502 w/bernlöhr Simulation of response of a single cell of an infinite array of telescopes Hexagonal layout, 3500m elevation Separation between telescopes 80-213m Perfect telescope optics Diameter of telescopes 5-15m Scale simulations to 1km 2, neglect boundary Trigger studies Pixelation and reconstruction of gamma-rays

Sample Design Distance From Center Of Array [m] Array 1. 217 telescopes 2. 8 hexagonal rings + 1 3. 80m separation Telescope and Detector 1. ø10m equivalent 2. QE = 0.25 (Bialkali) 3. 15º field of view Facts and Figures 1. Outer radius: 640m 2. Single cell area: 5543m 2 3. Total area: 1.06km 2 Distance From Center Of Array [m]

Cell effect Distance [m] Infinite Array Of Telescopes 1. 3500m ASL R Cherenk = 85m 2. D Scopes = 80m Geometry Dictates That 1. Impact point of every shower is in some cell 2. B Max = 47m 3. At least 3 telescopes contained in Cherenkov light pool Distance [m]

Cell effect Some Photoelectron threshold density [PE/m 2 ] 0.14 10 5 m 2 1.3 10 5 m 2 3.8 10 5 m 2 Distance from shower core [m] PE density after: 1. Atmosphere 2. Mirror reflection 3. Photocathode VERITAS-like Most of effective area comes from distant showers. Eff. area is strong function of energy. Cell Geometry Only interested in photons in within cell a distance of approx. L/ 3 from telescopes.

Trigger Efficiency vs Pixel Size I (Central Telescope) Central Telescope Trigger Efficiency El: 3.5 km QE: 1.0, D=7m QE: 0.5, D=10m QE: 0.5, D=7m QE: 0.25, D=10m Parameters: E γ =42 GeV FoV=15 o Rnsb=1kHz Optimum trigger sensor pixel size is 0.07 o -0.3 o Weak dependence on QE, D, El Trigger Pixel Size [degree]

Trigger Efficiency vs Pixel Size II (Full Array) Array Trigger Efficiency p=0.05 o p=0.08 o p=0.10 o p=0.13 o p=0.16 o p=0.20 o Array Trigger: Three telescopes above operational threshold Array Parameters: Elevation: 3.5 km QE: 0.25 Reflector: 10 m FoV: 15 o Photon Energy [GeV]

Performance vs. spacing (vary #, fix A) Cost $$$ 91 tel/km 2 61 tel/km 2 37 tel/km 2 (Ø=7m, 1kHz sustainable NSB trigger rate per telescope)

Performance vs. spacing (vary A, fix #) 37 tel/km 2 61 tel/km 2 91 tel/km 2 127 tel/km 2 (Ø=7m, 1kHz sustainable NSB trigger rate per telescope)

Performance vs. spacing (Ø=7m, 1kHz sustainable NSB trigger rate per telescope)

P.R.E. vs mirror area for 1km 2 array Cost $$$ Array configurations each with 1km 2 fiducial area. Hexagonal rings: 3 x 213m = 37 scope 4 x 160m = 61 scope 5 x 128m = 91 scope 6 x 106m = 127 scope 7 x 91m = 169 scope 8 x 80m = 217 scope Scope configuration: Ø = 5, 7, 10, 15m Ratio of mirror diameter to telescope separation, D/L [1]

Trigger Telescope Multiplicity Average Number of Telescopes in Trigger El=4.5km, QE: 1.0, D=7m El=4.5km, QE: 0.5, D=10m El=3.5km, QE: 1.0, D=7m El=3.5km, QE: 0.5, D=10m QE: 0.5 El: 4.5 km, D=7m QE: 0.25 El: 4.5 km, D=10m QE: 0.5 El: 3.5 km, D=7m QE: 0.25 El: 3.5 km, D=10m 40 GeV γ triggers 7 telescopes Photon Energy [GeV]

Cleaning Sample Event Photon direction [deg] Photon direction [deg] Event 1 (42 GeV) Photon direction [deg] Event 2 (42 GeV)

Cleaning Voronoi Diagram Photon direction [deg] 0.0-0.1-0.2-0.3-0.4-0.5 0.3 0.2 0.1 0.0-0.1-0.2-0.6-0.3-0.7-0.4-0.8-0.5-0.9-0.6-0.4-0.3-0.2-0.1 0.0 0.1 0.2 0.3 0.4-0.1 0.0 0.1 0.2 0.3 0.5 0.5 0.6 0.7 0.8 Photon direction [deg] Photon direction [deg] Event 1 (42 GeV) Event 2 (42 GeV)

Cleaning P.E. Separation Scales Diff. density [Arbitrary] γ: 21 GeV NSB: 150 γ/deg 2 γ: 42 GeV NSB: 150 γ/deg 2 P.E. separation [deg] QE: 0.25 Reflector Diameter: 10m Elevation: 3.5 km Trigger pixel size: 0.146 o Voronoi Diagram P.E.-P.E. separation scales in Image: 0.015 o -0.045 o γ: 100 GeV NSB: 150 γ/deg 2

Cleaning Sample Event Single 42 GeV event View from 4 telescopes Optimal cleaning (from consideration of angular reconstruction) keeps only photons near core Multiple cleaning schemes may be appropriate. Shower axis Shape cut Energy estimate

Performance of pixelated cameras dx Cleaning based on number of photons in neighborhood of each pixel. Cleaning scheme defined by two parameters: R radius of cleaning circle N number of photons Optimized for pixel size, dx, to give best reconstruction of gamma-rays. Almost degenerate: density

Sensitivity vs detector pixel size 40 GeV 100 GeV Simulations: 40, 100 GeV γ-rays with CORSIKA 7m telescopes 80m separation Perfect optics Pixellated cameras Analysis: 3D reconstruction Optimized cleaning based on density of PEs in image Results: 8 pixels 30-40% lower sensitivity 2-4 optimal

Lessons Cell Effect : operation in 40 GeV range possible with mid-sized telescopes Optimum trigger pixel size is ~0.1º (6 ) Optimum image pixel size is ~0.03º (2 ) Hard cleaning required to optimize reconstruction of shower axis Angular resolution of 6 (3 ) possible for 40GeV (100GeV) photons with 80m separation

What sensitivity might be achievable? Thought experiment: 1. 1km 2 effective area at all energies. 2. 0.1 ang. resolution at all energies. 3 4 1 2 Background: 1. Diffuse background extrapolated from EGRET. 2. Cosmic electrons. 3. 0.1% proton flux from π 0 interactions. 4. Higher fraction of proton events assuming increasing rejection with energy.