Fluorescence Measurements at ANL and the Auger Experiment

Similar documents
Precise Measurement of the Absolute Yield of Fluorescence Photons in Atmospheric Gases

The air fluorescence yield. Fernando Arqueros Universidad Complutense de Madrid Spain

John Ellison University of California, Riverside. Quarknet 2008 at UCR

AIRFLY: Measurement of the Air Fluorescence induced by electrons

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

RECENT RESULTS FROM THE PIERRE AUGER OBSERVATORY

The Pierre Auger Observatory Status - First Results - Plans

Particle Physics Beyond Laboratory Energies

7 th International Workshop on New Worlds in Astroparticle Physics São Tomé, September 2009 THE AMIGA PROJECT

arxiv: v1 [astro-ph] 30 Jul 2008

Ultra High Energy Cosmic Rays What we have learnt from. HiRes and Auger. Andreas Zech Observatoire de Paris (Meudon) / LUTh

TeV Particle Physics and Physics Beyond the Standard Model

Development of a prototype for Fluorescence detector Array of Single-pixel Telescopes (FAST)

Topic 7. Relevance to the course

The Cherenkov Telescope Array

UHE Cosmic Rays in the Auger Era

Cosmic Rays. M. Swartz. Tuesday, August 2, 2011

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

IceCube. francis halzen. why would you want to build a a kilometer scale neutrino detector? IceCube: a cubic kilometer detector

Ultrahigh Energy cosmic rays II

Modern Accelerators for High Energy Physics

Neutral particles energy spectra for 900 GeV and 7 TeV p-p collisions, measured by the LHCf experiment

Extensive Air Showers and Particle Physics Todor Stanev Bartol Research Institute Dept Physics and Astronomy University of Delaware

Dmitry Naumov. for Cosmotepetl Collaboration

Some Thoughts on Laboratory Astrophysics for UHE Cosmic Rays. Pierre Sokolsky University of Utah SABRE Workshop SLAC, March, 2006

GEANT4 simulation about the laboratory astrophysics in Taiwan

FLASH. FLuorescence in Air from SHowers (SLAC E-165) Pisin Chen SLAC. Report to DOE HEP Review SLAC, June 2-4, 2004

Air Fluorescence Photon Yield In Cosmic Ray Showers

arxiv:astro-ph/ v1 6 Mar 2007

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

Measurement of Muon Lifetime

MEASURING THE LIFETIME OF THE MUON

The Pierre Auger Project: Status and Recent Results. Pierre Auger Project. Astrophysical motivation

Results from the Pierre Auger Observatory. Paul Sommers, Penn State August 7, 2008, SSI

P. Tinyakov 1 TELESCOPE ARRAY: LATEST RESULTS. P. Tinyakov. for the Telescope Array Collaboration. Telescope Array detector. Spectrum.

Preliminary analysis of p-pb data update n. 6

The AMIGA detector of the Pierre Auger Observatory: an overview

Detectors for astroparticle physics

The Factors That Limit Time Resolution for Photon Detection in Large Cherenkov Detectors

LHC State of the Art and News

Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC

Beam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.

Searches for new Physics at HERA

arxiv:hep-ex/ v1 15 Aug 2006

Atmospheric Monitoring

Status and results from the Pierre Auger Observatory

Detecting High Energy Cosmic Rays with LOFAR

Black Holes and Extra Dimensions

Optic Detectors Calibration for Measuring Ultra-High Energy Extensive Air Showers Cherenkov Radiation by 532 nm Laser

Precision Tests of the Standard Model. Yury Kolomensky UC Berkeley Physics in Collision Boston, June 29, 2004

Updates on X 3872 production at Belle. K.Trabelsi QWG6 Workshop Nara, Dec 2-5, 2008

Cosmic Ray Physics with the Alpha Magnetic Spectrometer

High energy gamma production: analysis of LAL 4-mirror cavity data

Impact of the Fluorescence Yield selection on the reconstructed shower parameters

UHE Cosmic Rays and Neutrinos with the Pierre Auger Observatory

Indirect Dark Matter Detection

Ultra-High Energy Cosmic Rays & Neutrinos above the Terascale

2nd-Meeting. Ionization energy loss. Multiple Coulomb scattering (plural and single scattering, too) Tracking chambers

Exam Results. Force between charges. Electric field lines. Other particles and fields

KM3NeT. Astro-particle and Oscillations Research with Cosmics in the Abyss (ARCA & ORCA)

Dedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV

Results from the Telescope Array Experiment

Neutrino Radiography of the Earth with the IceCube Neutrino Observatory

MiniBooNE Progress and Little Muon Counter Overview

On the energy deposition by electrons in air and the accurate determination of the air-fluorescence yield

OVERVIEW OF THE RESULTS

Status and Perspectives for KM3NeT/ORCA

A gas-filled calorimeter for high intensity beam environments

Measurement of the pressure dependence of air fluorescence emission induced by electrons

Cosmic ray indirect detection. Valerio Vagelli I.N.F.N. Perugia, Università degli Studi di Perugia Corso di Fisica dei Raggi Cosmici A.A.

TeV energy physics at LHC and in cosmic rays

arxiv: v1 [physics.ins-det] 3 Feb 2011

Mass Composition Study at the Pierre Auger Observatory

Senior Design Proposal

A Gaussian Fitter for the CESR-c Fast Luminosity Monitor

Accelerator Based Particle Physics Experiments

Ultra-High Energy Cosmic Rays and Astrophysics. Hang Bae Kim Hanyang University Hangdang Workshop,

Cosmogenic neutrinos II

THE PIERRE AUGER OBSERVATORY: STATUS AND RECENT RESULTS

Ultra High Energy Cosmic Rays: Observations and Analysis

EEE4106Z Radiation Interactions & Detection

The ATLAS Experiment and the CERN Large Hadron Collider

COSMIC RAYS AND AGN's

An introduction to AERA. An Introduction to the Auger Engineering Radio Array (AERA)

Hadronic interactions of ultra-high energy cosmic rays

This presentation was created based on the slides by Vitor de Souza from his talk at the 4th

First Results from the Pierre Auger Project

COSMIC RAY COMPOSITION.

Ultra High Energy Cosmic Rays. Malina Kirn March 1, 2007 Experimental Gravitation & Astrophysics

Recent measurements of ultra-high energy cosmic rays and their impact on hadronic interaction modeling

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

Search for diffuse cosmic neutrino fluxes with the ANTARES detector

Searches for Exotica with CMS

High-energy cosmic rays

CHAPTER 3 Prelude to Quantum Theory. Observation of X Rays. Thomson s Cathode-Ray Experiment. Röntgen s X-Ray Tube

Universality (and its limitations) in Cosmic Ray shower development

Search for heavy neutrinos in kaon decays

IHEP-BINP CEPC accelerator collaboration workshop Beam energy calibration without polarization

Updated results of the OPERA neutrino-velocity analysis

SciBar and future K2K physics. F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies

Transcription:

Fluorescence Measurements at ANL and the Auger Experiment Motivation for Fluorescence Calibrations AIRFLY Fluorescence Experiment at ANL Auger Experiment Update

N 2 Molecule Vibrational Energy Levels 337nm transition

Main transitions are fast, nanoseconds

Many experiments use or will use Nitrogen Fluorescence Auger OWL and EUSO spacebased experiments

Scintillator Fluorescence

Due to smaller model dependence, Auger normalizes to its fluorescence detectors. Looks like HiRes. Water tank cross section lies right on top of AGASA until statistics run out. Only a 1σ discrepancy (25% in energy scale). Need to reduce σ 0.22 Augeryears of data

One example measurement of electron-induced fluorescence Not an absolute measurement Agrees with curve? 45% of Fluorescence Due to Electrons and Positrons < 10 MeV in 10 19 ev Shower

Much more information needed Pressure, Temperature, Humidity dependence Oxygen quenching More complete energy scan Absolute measurement to 5%

Much more information needed Complete Spectrum from 300-400 nm (Rayleigh scattering 1/Λ 4 ) Spectrum has been measured before but only piece-by-piece with 14 filters, each with different inefficiencies and acceptance from wrong wavelengths

Much more information needed Previous measurements differ by as much as x3 in various wavelengths Best measurements disagree with best models by as much as x5 in various wavelengths Usually in the smaller spectral lines so not a disaster, but still a problem

Fluorescence Calibration at Argonne Chemistry Division Van de Graaff Advanced Photon Source HEP Division Advanced Wakefield Accelerator Complementary machines: AWA only accelerator with enough energy to do absolute calibration with Cerenkov gas. Van de Graaff only machine with enough charge to measure spectrum.

Heroes AWA group notably Manoel Conde, Felipe Franchini, Zikri Yusof Chemistry staff notably Sergey Chemerisov and Bob Lowers

APS AWA Chemistry 45% of Fluorescence Due to Electrons and Positrons < 10 MeV in 10 19 ev Shower

Van de Graaff with cover removed Resistor plates step V down to zero Charged to 3 million volts Beam

AIRFLY Experiment, led by Paolo Privitera from INFN

AIRFLY Experiment, led by Paolo Privitera from INFN

AIRFLY Running Plan AWA Van de Graaff APS 2-day PMT X X X 1.5 week run 3 week run Depends on data needs Today s talk December Today s talk Just completed

Beam Pickup, used for all the PMT measurements Faraday Cup, mainly used to check Pickup Will fit slopes from PMT vs Pickup, an experiment with 2 electronics channels!

AWA PMT Fluorescence Data, 14 MeV electrons

AWA PMT Fluorescence Data, 14 MeV electrons

AWA PMT Fluorescence Data, 14 MeV electrons Oxygen quenching due to molecule collisions with N 2 *

0.5 MeV Run at Van de Graaff with beam halo

Cut ±2 sigma around main beam pickup peak for both AWA and Van de Graaff 5 minutes later, beam halo is gone

5 minutes of raw data!

Main goal for December running at AWA

Need ~5% measurement of Nmuons to maintain separation ANL may also play the key role in improving the water tank measurement

Basics of Current Design Scintillator strips are 200cm x 4.1cm, 64 strips per module, 5.2 m 2 6 modules per 31.2 m 2 unit, read out with 64-pixel PMTs Electronics counts number of strips over threshold every clock cycle and sends 9 bits per unit

What segmentation per 30 m 2 unit is needed? RMS of N μ / N Real μ 10 ns 25 ns 4% 5.5% For comparison CASA/MIA had 10 segments per 30 m 2 Segments: 192 384 Going from 384 segments to 192 saves $0.45M

Proposed Final Muon Layout Energy (E range) (EeV) Detector Spacing (m) Size (km 2 ) θ max (deg) #events/ Year Total Number of 30 m 2 Sites 0.4 (0.2-0.6) 375 2.5 45 (60) 700 (1150) 29 1.0 (0.6-3) 750 23 45 (60) 1050 (1750) 61 6.0 (3-10) 1500 250 45 (60) 310 (515) 127 Fluxes estimated from current Auger spectrum 6 * 127 = 762 modules, about a $1.5M project, but approval cannot come until Auger South is complete. Also depends on Airfly results.

Construction Progress 905 surface detector stations deployed Three fluorescence buildings complete each with 6 telescopes

Auger North Site Selected in June, Colorado site wins Hal, Rich, and I attended first organizational meeting last week. Plan is a R+D proposal in the spring then a full proposal writing workshop at UC in August-September.

ν Sensitivity of Large Cosmic Ray Air Shower Experiments for New Physics Searches M. C. Espírito Santo LIP - Lisboa HEP2005 Lisboa, July 2005

Besides the TeV-scale gravity signatures like Black Holes discussed in my previous seminar: Excited Lepton sensitivity to 100 TeV Leptoquark sensitivity to 100 TeV Heavy Gluinos in Split Supersymmetry But Tim/Carlos suggest the obvious one is Squarks in R-Parity Violating models, Tim is working on the cross section and UC group will simulate it

The End