Air Shower Simulations for NAHSA
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High Energy and Prompt Neutrino Production in the Atmosphere P
High Energy and Prompt Neutrino Production in the Atmosphere P. Berghaus, R. Birdsall, P. Desiati, T. Montaruli (1) and J. Ranft (2) (berghaus, rbirdsall, desiati, tmontaruli @icecube.wisc.edu, [email protected]) (1) University of Wisconsin, Madison (2) UGH Siegen Abstract: Atmospheric neutrinos and muons have been extensively measured by underground experiments in the region below 10GeV. The AMANDA neutrino telescope has measured the spectrum of atmospheric neutrinos up to 100 TeV and IceCube, which has about 100 times higher acceptance, is expected to collect unprecedented statistics at even higher energies in the near future. Since high energy atmospheric neutrinos are the foreground for extraterrestrial events, their study is of fundamental importance. With IceCube it will be possible to investigate the high energy tail above 1TeV, where kaon and charm physics become relevant. We are working on understanding high energy hadronic models and compare Monte-Carlo data generated with the CORSIKA air shower simulation package to results from particle physics experiments. We also show the effect of improving the simulation of charm production within CORSIKA after calibrating the hadronic model DPMJET against experimental data. The main goal of Neutrino Telescopes is the detection of high energy neutrinos from extraterrestrial sources such as Supernova Remnants, Active Galactic Nuclei (AGN), and Gamma Ray Bursts (GRB) [1]. However, extraterrestrial neutrinos are concealed by the intense flux of neutrinos produced through interactions of cosmic rays in the Earth©s atmosphere via decays of π and K mesons. This foreground has to be understood In order to allow its separation from a potential extraterrestrial neutrino signal. -
Extensive Air Shower Simulations with Corsika and the Influence of High-Energy Hadronic Interaction Models
EXTENSIVE AIR SHOWER SIMULATIONS WITH CORSIKA AND THE INFLUENCE OF HIGH-ENERGY HADRONIC INTERACTION MODELS D. HECK FOR THE KASCADE COLLABORATION Institut f¨ur Kernphysik, Forschungszentrum Karlsruhe, D-76021 Karlsruhe, Germany E-mail:[email protected] When high-energy cosmic rays (γ’s, protons, or heavy nuclei) impinge onto the Earth’s atmosphere, they interact at high altitude with the air nuclei as targets. By repeated interaction of the secondaries an ‘extensive air shower’ (EAS) is gen- erated with huge particle numbers in the maximum of the shower development. Such cascades are quantitatively simulated by the Monte Carlo computer program CORSIKA. The most important uncertainties in simulations arise from modeling of high-energy hadronic interactions: a) The inelastic hadron-air cross sections. b) The energies occurring in EAS may extend far above the energies available in man-made accelerators, and when extrapolating towards higher energies one has to rely on theoretical guidelines. c) In collider experiments which are used to ad- just the interaction models the very forward particles are not accessible, but just those particles carry most of the hadronic energy, and in the EAS development they transport a large energy fraction down into the atmosphere. CORSIKA is coupled alternatively with 6 high-energy hadronic interaction codes (DPMJET, HDPM, neXus, QGSJET, SIBYLL, VENUS). The influence of those interaction models on observables of simulated EAS is discussed. 1 Introduction CORSIKA (COsmic Ray SImulation for KAscade) is a detailed Monte Carlo program to study the evolution of extensive air showers (EAS) in the atmo- sphere initiated by various cosmic ray particles. -
Approximating the Lateral Distribution Function of Cherenkov Radiation As a Function of the Particle Type for Tunka-133 Array
Approximating the Lateral Distribution Function of Cherenkov Radiation as a Function of the Particle Type for Tunka-133 Array Zena Fadhel Khadhum1, Hassan Abdullah Mahdi2, A.A. Al-Rubaiee2,* 1College of science, Department of astronomy and space, Baghdad University, Baghdad, Iraq 2College of Science, Department of Physics, Al-Mustansiriyah University, Baghdad, Iraq *Email: [email protected] Abstract The main interest of the present work is in analyzing the lateral distribution function (LDF) of Cherenkov radiation from particles that produced in Extensive Air Showers (EAS). The simulation of LDF of Cherenkov radiation is fulfilled by utilizing the CORSIKA program at 3∙1015 eV of the primary energy around the knee region for many primaries for vertical showers for Tunka-133 array conditions. Depending on the numerical simulation results of Cherenkov light LDF, sets of parameterized polynomial functions are resetted for several particles as a function of primary particle type. The comparison between the approximated LDF of Cherenkov radiation with the LDF which has been simulated using CORSIKA program for Tunka-133 array is verified for several primary particles for vertical EAS cascade. Keywords: Cherenkov light, lateral distribution function, Extensive Air Showers. 1. Introduction Primary cosmic rays (PCRs) of energy spectrum and mass composition in EAS have been studied around the knee region. This approach has a main significant for getting information about PCR acceleration mechanisms and origin [1, 2]. Generally, LDF of Cherenkov radiation depends on the type and energy of the produced primary particle, observation level, distance from EAS core R, height of the first interaction and the direction of shower axis [3, 4]. -
A Branching Model for Hadronic Air Showers Vladimir Novotny
A branching model for hadronic air showers Vladimir Novotny∗ Charles University, Faculty of Mathematics and Physics, Institute of Particle and Nuclear Physics, Prague, Czech Republic E-mail: [email protected] Dalibor Nosek Charles University, Faculty of Mathematics and Physics, Institute of Particle and Nuclear Physics, Prague, Czech Republic E-mail: [email protected] Jan Ebr Institute of Physics of the Academy of Sciences of the Czech Republic, Prague, Czech Republic E-mail: [email protected] We introduce a simple branching model for the development of hadronic showers in the Earth’s atmosphere. Based on this model, we show how the size of the pionic component followed by muons can be estimated. Several aspects of the subsequent muonic component are also discussed. We focus on the energy evolution of the muon production depth. We also estimate the impact of the primary particle mass on the size of the hadronic component. Even though a precise calcu- lation of the development of air showers must be left to complex Monte Carlo simulations, the proposed model can reveal qualitative insight into the air shower physics. arXiv:1509.00364v1 [astro-ph.HE] 1 Sep 2015 The 34th International Cosmic Ray Conference, 30 July- 6 August, 2015 The Hague, The Netherlands ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it/ A branching model for hadronic air showers Vladimir Novotny 1. Introduction We study a hadronic component of extensive air showers. Key parameters that we want to determine are a shape of a muonic subshower profile and an atmospheric depth of its maximum µ µ (Xmax). -
Air Shower Simulation with New Hadronic Interaction Models in CORSIKA
33RD INTERNATIONAL COSMIC RAY CONFERENCE, RIO DE JANEIRO 2013 THE ASTROPARTICLE PHYSICS CONFERENCE Air Shower Simulation with new Hadronic Interaction Models in CORSIKA T. PIEROG1 D. HECK1 1 Karlsruhe Institute of Technology (KIT), IKP, D-76021 Karlsruhe, Germany [email protected] Abstract: The interpretation of EAS measurements strongly depends on detailed air shower simulations. COR- SIKA is one of the most commonly used air shower Monte Carlo programs. The main source of uncertainty in the prediction of shower observables for different primary particles and energies being currently dominated by differences between hadronic interaction models, two models, EPOS and QGSJETII, have been updated taking into account LHC data. After briefly reviewing major technical improvements implemented in the latest release, version 7.37, such as optional hybrid or massively parallel simulation, the impact of the improved hadronic inter- action models on shower predictions will be presented. The performance of the new EPOS LHC and QGSJETII- 04 models in comparison to LHC data is discussed and the impact on standard air shower observables derived. As a direct consequence of the tuning of the model to LHC data, the predictions obtained with these two models show small differences on the full energy range. Keywords: EAS, LHC, CORSIKA, CONEX, EPOS, QGSJETII, Simulations. 1 Introduction Then the main new options available in the last release of The experimental method of studying ultra-high energy CORSIKA v7.37 and CONEX v4.37 will be reviewed. Fi- cosmic rays is an indirect one. Typically, one investigates nally using detailed Monte Carlo simulations done with various characteristics of extensive air showers (EAS), a these air shower simulation models, the new predictions huge nuclear-electromagnetic cascade induced by a pri- for Xmax and for the number of muons will be presented. -
Investigation on Gamma-Electron Air Shower Separation for CTA
Taras Shevchenko National University of Kyiv The Faculty of Physics Astronomy and Space Physics Department Investigation on gamma-electron air shower separation for CTA Field of study: 0701 { physics Speciality: 8.04020601 { astronomy Specialisation: astrophysics Master's thesis the second year master student Iryna Lypova Supervisor: Dr. Gernot Maier leader of Helmholtz-University Young Investigator Group at DESY and Humboldt University (Berlin) Kyiv, 2013 Contents Introduction 2 1 Extensive air showers 3 1.1 Electromagnetic showers . 3 1.2 Hadronic showers . 7 1.3 Cherenkov radiation . 11 2 Cherenkov technique 13 2.1 Cherenkov telescopes . 13 2.2 Cherenkov Telescope Array . 18 2.3 Air shower reconstruction . 24 3 γ-electron separation with telescope arrays 31 3.1 Hybrid array . 31 3.2 The Cherenkov Telescope Array . 39 Summary 42 Reference 44 Appendix A 47 Appendix B 50 Introduction Very high energy (VHE) ground-based γ-ray astrophysics is a quite young science. The earth atmosphere absorbs gamma-rays and direct detection is possible only with satellite or balloon experiments. The flux of gamma rays falls rapidly with increasing energy and satellite detectors become not effective anymore due to the limited collection area. Another possibility for gamma- ray detection is usage of Imaging Atmospheric Cherenkov telescopes. The primary γ-ray creates a cascade of the secondary particles which move through the atmosphere. The charged component of the cascade which moves with velocities faster the light in the air, emits Cherenkov light which can be detected by the ground based optical detectors. The ground based gamma astronomy was pioneered by the 10 m single Cherenkov telescope WHIPPLE (1968) [1] in Arizona. -
Astro-Particle Physics: Imaging Air Cherenkov Telescopes (Iacts)
IceAct: Cosmic Ray Air Cherenkov telescopes as an upgrade to the IceCube Neutrino Observatory at the South Pole Larissa Paul, Anna AbadSantos, Antonio Banda, Aine Grady, Sean McLaughlin, Matthias Plum and Karen Andeen Department of Physics, Marquette University, Milwaukee WI, USA Student researchers Astro-particle physics: Imaging Air Cherenkov Telescopes (IACTs): Testing epoxy for the use at the South Pole: at work • Cosmic rays - Particles Source? IACTs detect Cherenkov light produced in the atmosphere by air showers: this The IceAct cameras consist of 61 PMMA Winston cones (WCs) glued onto the with the highest known allows us to study the purely electromagnetic component of the air shower with glass of 61 SiPMs with epoxy. The epoxy used in previous versions of the energy in the universe excellent energy and mass resolution prototype was not cold-rated, causing rapid degradation of the camera at Polar • Discovered in 1912, still a • technique is complementary to the particle detectors already in place at the temperatures. A reliable cold-rated epoxy is vital to ensure many years South Pole of successful data taking. the IceAct lot of unknowns: camera • What are cosmic rays? • will allow us to significantly improve several measurements that we are • What are the astrophysical sources of cosmic interested in through: We are testing two different cold-rated epoxies for rays? • cross-calibrations of the different detector components against each other long-term reliability and reproducibility: • How are they accelerated? • reconstruction of events with different detector configurations • Goal #1: release equal amounts of epoxy drops • Air showers onto each SiPM. Cascades of secondary particles generated by cosmic IceAct: • Problem: viscosity of epoxy changes with time exposed to air, causing the ray particles interacting with the earth's atmosphere. -
Systematic Differences Due to High Energy Hadronic Interaction Models
Systematic Differences due to High Energy Hadronic Interaction Models in Air Shower Simulations in the 100 GeV-100 TeV Range R.D. Parsons1, ∗ and H. Schoorlemmer1 1Max-Planck-Institut f¨urKernphysik P.O. Box 103980; D 69029 Heidelberg; Germany The predictions of hadronic interaction models for cosmic-ray induced air showers contain inherent uncertainties due to limitations of available accelerator data and theoretical understanding in the required energy and rapidity regime. Differences between models are typically evaluated in the range appropriate for cosmic-ray air shower arrays (1015- 1020 eV). However, accurate modelling of charged cosmic-ray measurements with ground based gamma-ray observatories is becoming more and more important. We assess the model predictions on the gross behaviour of measurable air shower parameters in the energy (0.1-100 TeV) and altitude ranges most appropriate for detection by ground-based gamma- ray observatories. We go on to investigate the particle distributions just after the first interaction point, to examine how differences in the micro-physics of the models may compound into differences in the gross air shower behaviour. Differences between the models above 1 TeV are typically less than 10%. However, we find the largest variation in particle densities at ground at the lowest energy tested (100 GeV), resulting from striking differences in the early stages of shower development. INTRODUCTION vations, as most pointedly seen in the measurement of the cosmic ray electron spectrum [8{11] where the back- Ground based gamma-ray astronomy uses the particle ground contamination must be estimated from compar- shower initiated when a very high energy (> 100 GeV) ison to Monte Carlo simulations, in which case the sys- gamma-ray interacts with an atom in the Earth's atmo- tematic uncertainties in the hadronic interactions quickly sphere, to detect and reconstruct the primary particles become the dominant form of uncertainty in the measure- of the primary gamma-rays. -
Extensive Air Showers and Ultra High-Energy Cosmic Rays: a Historical Review
EPJ manuscript No. (will be inserted by the editor) Extensive Air Showers and Ultra High-Energy Cosmic Rays: A Historical Review Karl-Heinz Kampert1;a and Alan A Watson2;b 1 Department of Physics, University Wuppertal, Germany 2 School of Physics and Astronomy, University of Leeds, UK Abstract. The discovery of extensive air showers by Rossi, Schmeiser, Bothe, Kolh¨orsterand Auger at the end of the 1930s, facilitated by the coincidence technique of Bothe and Rossi, led to fundamental con- tributions in the field of cosmic ray physics and laid the foundation for high-energy particle physics. Soon after World War II a cosmic ray group at MIT in the USA pioneered detailed investigations of air shower phenomena and their experimental skill laid the foundation for many of the methods and much of the instrumentation used today. Soon in- terests focussed on the highest energies requiring much larger detectors to be operated. The first detection of air fluorescence light by Japanese and US groups in the early 1970s marked an important experimental breakthrough towards this end as it allowed huge volumes of atmo- sphere to be monitored by optical telescopes. Radio observations of air showers, pioneered in the 1960s, are presently experiencing a renais- sance and may revolutionise the field again. In the last 7 decades the research has seen many ups but also a few downs. However, the exam- ple of the Cygnus X-3 story demonstrated that even non-confirmable observations can have a huge impact by boosting new instrumentation to make discoveries and shape an entire scientific community. -
Detection Techniques of Radio Emission from Ultra High Energy Cosmic Rays
Detection Techniques of Radio Emission from Ultra High Energy Cosmic Rays DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Chad M. Morris, B.S. Graduate Program in Physics The Ohio State University 2009 Dissertation Committee: Prof. James J. Beatty, Adviser Prof. John F. Beacom Prof. Richard J. Furnstahl Prof. Richard E. Hughes c Copyright by Chad M. Morris 2009 Abstract We discuss recent and future efforts to detect radio signals from extended air showers at the Pierre Auger Observatory in Malarg¨ue, Argentina. With the advent of low-cost, high-performance digitizers and robust digital signal processing software techniques, radio detection of cosmic rays has resurfaced as a promising measure- ment system. The inexpensive nature of the detector media (metallic wires, rods or parabolic dishes) and economies of scale working in our favor (inexpensive high- quality C-band amplifiers and receivers) make an array of radio antennas an appealing alternative to the expense of deploying an array of Cherenkov detector water tanks or ‘fly’s eye’ optical telescopes for fluorescence detection. The calorimetric nature of the detection and the near 100% duty cycle gives the best of both traditional detection techniques. The history of cosmic ray detection detection will be discussed. A short review on the astrophysical properties of cosmic rays and atmospheric interactions will lead into a discussion of two radio emission channels that are currently being investigated. ii This dissertation is dedicated to my wife, Nichole, who has tolerated and even encouraged my ramblings for longer than I can remember. -
Pos(ICRC2019)270 B † 15%
Air-Shower Reconstruction at the Pierre Auger Observatory based on Deep Learning PoS(ICRC2019)270 Jonas Glombitza∗a for the Pierre Auger Collaboration yb aRWTH Aachen University, Aachen, Germany bObservatorio Pierre Auger, Av. San Martín Norte 304, 5613 Malargüe, Argentina E-mail: [email protected] Full author list: http://www.auger.org/archive/authors_icrc_2019.html The surface detector array of the Pierre Auger Observatory measures the footprint of air show- ers induced by ultra-high energy cosmic rays. The reconstruction of event-by-event information sensitive to the cosmic-ray mass, is a challenging task and so far mainly based on fluorescence detector observations with their duty cycle of ≈ 15%. Recently, great progress has been made in multiple fields of machine learning using deep neural networks and associated techniques. Apply- ing these new techniques to air-shower physics opens up possibilities for improved reconstruction, including an estimation of the cosmic-ray composition. In this contribution, we show that deep convolutional neural networks can be used for air-shower reconstruction, using surface-detector data. The focus of the machine-learning algorithm is to reconstruct depths of shower maximum. In contrast to traditional reconstruction methods, the algorithm learns to extract the essential in- formation from the signal and arrival-time distributions of the secondary particles. We present the neural-network architecture, describe the training, and assess the performance using simulated air showers. 36th International Cosmic Ray Conference — ICRC2019 24 July – 1 August, 2019 Madison, Wisconsin, USA ∗Speaker. yfor collaboration list see PoS(ICRC2019)1177 c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0). -
A Tool for Air-Shower Simulations
CORSIKA A tool for air-shower simulations Pierpaolo Savina OUTLINE INTRODUCTION Energy range of astroparticle physics: High energy cosmic rays detection techniques: From few GeV up to ~100 EeV. Indirect measurement (Extensive Air Showers). Extensive Air Showers (EAS): result of many inter-dependent Identify the primary particle by measuring the shower: sub processes. Energy shower size Direction arrival timing Type shape and particle contents difficult to detect multi-messengers astophysics: CR, gamma and neutrinos likely from same sources. Neutral particle point back to sources but huge background. easy to detect 2 OUTLINE SIMULATIONS Computer simulation: reproduction Mathematical model: description of a of the behavior of a system using a system using mathematical concept computer to simulate the outcomes and language. using a model associated to the system. used when is impractical to do a full simulation. Models are based on simplifications, assumptions and approximations. Complex problems (EAS simulations) broken down in smaller sub-problems. More simplifications lead to smaller “confidence level” (more verification needed). Monte Carlo Techniques: algorithms that rely on repeated random sampling to obtain numerical results. Their essential idea is using randomness to solve problems. 3 KASKADE: experiment to measure OUTLINE CORSIKA cosmic rays composition in Karlsruhe Cosmic Ray Simulation for KASCADE consistent results in different experiments. Models: e.m. : EGS4 low-E hadronic: FLUKA references: UrQMD CORSIKA GHEISHA physics manual user guide high-E hadronic: QGSJET EPOS-LHC DPMJET SIBILL recommended Models tuned at collider energies then extrapolated in the energy range considered Fair agreement from 1012 to 1020 eV. much better agreement at low energies where data constrains extrapolations.