June 18-20, 2009 Detection of Askaryan radio pulses produced by cores of air showers. Suruj Seunarine, David Seckel, Pat Stengel, Amir Javaid, Shahid Hussain.

Slides:



Advertisements
Similar presentations
Ultrahigh Energy Cosmic Ray Nuclei and Neutrinos
Advertisements

July 29, 2003; M.Chiba1 Study of salt neutrino detector for GZK neutrinos.
The NuMoon experiment: first results Stijn Buitink for the NuMoon collaboration Radboud University Nijmegen 20 th Rencontres de Blois, 2008 May 19.
Radio detection of UHE neutrinos E. Zas, USC Leeds July 23 rd 2004.
TeVPA, July , SLAC 1 Cosmic rays at the knee and above with IceTop and IceCube Serap Tilav for The IceCube Collaboration South Pole 4 Feb 2009.
The presence of the South Pole Air Shower Experiment (SPASE) on the surface provides a set of externally tagged muon bundles that can be measured by AMANDA.
Sean Grullon For the IceCube Collaboration Searching for High Energy Diffuse Astrophysical Neutrinos with IceCube TeV Particle Astrophysics 2009 Stanford.
Shower & RF theory David Seckel, ANITA Collab. Mtg. Nov , /2002 Theory Notes on Shower and Radio Pulse.
SUSY06, June 14th, The IceCube Neutrino Telescope and its capability to search for EHE neutrinos Shigeru Yoshida The Chiba University (for the IceCube.
Apr 9, 2005 Scaling of Askaryan Pulses D. Seckel, Univ. of Delaware.
Jonathan Perkin ARENA May 05 Acoustic Cosmic Ray Neutrino Experiment FUTURE PROSPECTS simulation…
July 10, 2007 Detection of Askaryan radio pulses produced by cores of air showers. Suruj Seunarine, Amir Javaid, David Seckel, Philip Wahrlich, John Clem.
MP BACH MultiPixel Balloon-borne Air CHerenkov Detection of Iron Cosmic Rays Using Direct Cherenkov Radiation Imaged with a High Resolution Camera University.
EHE Search for EHE neutrinos with the IceCube detector Aya Ishihara for the IceCube collaboration Chiba University.
Simulation Issues for Radio Detection in Ice and Salt Amy Connolly UCLA May 18 th, 2005.
Steps towards a cosmogenic neutrino detector at the South Pole Summary of meeting on Sep 14 Opportunities - outer ring extension Acoustic & Radio technique,
Next Generation neutrino detector in the South Pole Hagar Landsman, University of Wisconsin, Madison Askaryan Under-Ice Radio Array.
Future Directions Radio A skaryan U nder ice R adio A rray Hagar Landsman Science Advisory Committee meeting March 1 st, Madison.
Why Neutrino ? High energy photons are absorbed beyond ~ 150Mpc   HE  LE  e - e + HE s are unique to probe HE processes in the vicinity of cosmic.
Contributions of the University of Bucharest to the study of high energy cosmic rays in the framework of the KASCADE-Grande experiment Octavian Sima Faculty.
Low frequency radio- emission associated with UHE cosmic rays KALYANEE BORUAH Physics Department, Gauhati University.
UCL Xmas 2006 : Dec 18 1 From the Tevatron to the Zevatron Mark Lancaster Simon Bevan, Amy Connolly, Ryan Nichol, Dave Waters.
Mar 9, 2005 GZK Neutrinos Theory and Observation D. Seckel, Univ. of Delaware.
March 02, Shahid Hussain for the ICECUBE collaboration University of Delaware, USA.
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Humberto Salazar (FCFM-BUAP) for the Pierre Auger Collaboration, CTEQ- Fermilab School Lima, Peru, August 2012 Ultrahigh Cosmic Rays: The highest energy.
1 Cosmic Rays in IceCube: Composition-Sensitive Observables Chihwa Song a, Peter Niessen b, Katherine Rawlins c for the IceCube collaboration a University.
Graduate Institute of Astrophysics, National Taiwan University Leung Center for Cosmology and Particle Astrophysics Chia-Yu Hu OSU Radio Simulation Workshop.
Detection of UHE Shower Cores by ANITA By Amir Javaid University Of Delaware.
Laboratory Particle- Astrophysics P. Sokolsky High Energy Astrophysics Institute, Univ. of Utah.
M.Chiba_ARENA20061 Measurement of Attenuation Length for Radio Wave in Natural Rock Salt and Performance of Detecting Ultra High- Energy Neutrinos M.Chiba,
RICE David Seckel, NeSS02, Washington DC, Sept ,/2002 R adio I ce C herenkov E xperiment PI presenter.
“The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra INFN and University, Torino, Italy For the EAS-TOP Collaboration.
ANtarctic Impulsive Transient Antenna University of Hawaii at Manoa Peter Gorham, PI John Learned and Gary S. Varner Ohio-State University Jim Beatty and.
June 6, 2006 CALOR 2006 E. Hays University of Chicago / Argonne National Lab VERITAS Imaging Calorimetry at Very High Energies.
Detection of UHE Shower Cores by ANITA By Amir Javaid University Of Delaware.
Cosmic ray physics in ALICE Katherin Shtejer Díaz For the ALICE Collaboration LatinoAmerican Workshop on High Energy Physics: Particles and Strings, Havana,
Simulation of a hybrid optical, radio, and acoustic neutrino detector Justin Vandenbroucke with D. Besson, S. Boeser, R. Nahnhauer, P. B. Price IceCube.
Steps towards a cosmogenic neutrino detector at the South Pole Summary of meeting on Sep 14 Opportunities - outer ring extension Acoustic & Radio technique,
Physical Description of IceTop 3 Nov IceTop Internal Review Madison, November 3-4, 2010 Physical Description of IceTop Paul Evenson, University.
RICE: ICRC 2001, Aug 13, Recent Results from RICE Analysis of August 2000 Data See also: HE228: Ice Properties (contribution) HE241: Shower Simulation.
Study of VHE Cosmic Ray Spectrum by means of Muon Density Measurements at Ground Level I.I. Yashin Moscow Engineering Physics Institute,
What we do know about cosmic rays at energies above eV? A.A.Petrukhin Contents 4 th Round Table, December , Introduction. 2. How these.
Studies of Askaryan Effect, 1 of 18 Status and Outlook of Experimental Studies of Askaryan RF Radiation Predrag Miocinovic (U. Hawaii) David Saltzberg.
25 June, 2006 UHE Neutrinos: II D. Seckel, Univ. of Delaware.
31/03/2008Lancaster University1 Ultra-High-Energy Neutrino Astronomy From Simon Bevan University College London.
NEVOD-DECOR experiment: results and future A.A.Petrukhin for Russian-Italian Collaboration Contents MSU, May 16, New method of EAS investigations.
June 19, 2009 Simulation of Askaryan Detectors and Events (SADE) David Seckel, Pat Stengel, Shahid Hussain D. Seckel, Univ. of Delaware.
Prospects of Identifying the Sources of the Galactic Cosmic Rays with IceCube Alexander Kappes Francis Halzen Aongus O’Murchadha University Wisconsin-Madison.
IceTop Design: 1 David Seckel – 3/11/2002 Berkeley, CA IceTop Overview David Seckel IceTop Group University of Delaware.
Lingling Ma IHEP China Measurement of Cosmic rays with LHAASO at 10PeV~100PeV 4th Workshop on Air Shower Detection at High Altitude Institute of High Energy.
Near-Field Effects of Cherenkov Radiation Induced by Ultra High Energy Cosmic Neutrinos Chih‐Ching Chen Collaboration with Chia-Yu Hu and Pisin Chen LeCosPA.
IceRay: an IceCube-Centered Radio GZK Array John Kelley University of Wisconsin, Madison for the IceRay working group ARENA08, Rome.
1 Cosmic Ray Physics with IceTop and IceCube Serap Tilav University of Delaware for The IceCube Collaboration ISVHECRI2010 June 28 - July 2, 2010 Fermilab.
Shih-Hao Wang 王士豪 Graduate Institute of Astrophysics & Leung Center for Cosmology and Particle Astrophysics (LeCosPA), National Taiwan University 1 This.
EHE Search for EHE neutrinos with the IceCube detector Aya Ishihara Chiba University.
Bergische Universität Wuppertal Jan Auffenberg et al. Rome, Arena ARENA 2008 A radio air shower detector to extend IceCube ● Three component air.
Simulation of a hybrid optical-radio-acoustic neutrino detector at South Pole D. Besson [1], R. Nahnhauer [2], P. B. Price [3], D. Tosi [2], J. Vandenbroucke.
SADE ANITA Monte Carlo(SAM) Test Results Amir Javaid University of Delaware.
SADE ANITA Monte Carlo(SAM) Test Results Amir Javaid University of Delaware.
Downgoing Muons in the IceCube experiment: Final presentation for Phys 735, Particle, Prof. Sridhara Dasu L.Gladstone 2008 Dec 3.
Cosmogenic Muon Background
L.L.Ma for LHAASO collaboration Beijing China
Expectation of Cosmic Ray Energy Spectrum with LHAASO
completed in austral season South Pole completed in austral season.
D. Seckel, Univ. of Delaware
Results on the Spectrum and Composition of Cosmic Rays
Event Rates vs Cross Sections
Karen Andeena, Katherine Rawlinsb, Chihwa Song*a
GZK Neutrino Spectrum. GZK Neutrino Spectrum How the detection scheme words.
Presentation transcript:

June 18-20, 2009 Detection of Askaryan radio pulses produced by cores of air showers. Suruj Seunarine, David Seckel, Pat Stengel, Amir Javaid, Shahid Hussain D. Seckel, Univ. of Delaware

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Topics Concept: –A source to test radio techniques –CR composition ? (not today) Askaryan pulses & air shower dimensions Air shower properties (AIRES & CORSIKA) –Particle content –Radial and energy distributions Calculation of RF signal –Coherent addition of subshowers –Issues: near zone/far zone, ray tracing Composition studies (not today) Detection –IceCube: shallow array, AURA –ANITA (not today)

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Theorist’s view of the UHE neutrino sky

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Recall how radio works 5 m 10 cm JC, SY: “How do you know when you haven’t seen anything?”

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Radio Goals & Staging 100 events/yr above eV >1000 km 3 sr Validation of design for field work Prototype projects – more than upper limits Detect Air Showers: Signal/Background/Calib

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Askaryan pulses from air shower core

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Critical dimensions

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) High energy ground level particles at SP CORSIKA/AIRES –Primary energy: 1,10,100,1000 PeV –Cutoff: 1,10,100,1000 GeV –Compositionp & Fe Explore –Particle content rad - meson - baryon - mu –Radial profilesE sh vs r –Shower development dN/dE, ancestry

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Ground level particles (above 10 GeV)  e-e-   n,p Radiation fraction increases with primary energy

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Radial distributions by particle ID radiating mesons baryons muons

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) E vs r (AIRES)

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) E vs r (CORSIKA) Fraction of available energy approaches 10% by 100 PeV Scaling allows use of high cutoff

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Synthesis of Askaryan pulses Many ground level particles –Superposition Individual RF pulses –Event: (id, t e, x e, n, E) –SubShower:(t s, x s, n, (r,l,s)) –Resolve geometry to antenna –Launch EM pulse(scaled AVZ) –Propagation effects (1/r, attenuation) –Adjust phase to common time basis Response –CoAdd spectra(t, n, pol, (complex spectrum)) –Antenna/DAQ

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) RF: (E p = 1 EeV, E cut = 1 TeV )

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) RF Cerenkov Rings

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) RF vs Core Size – (old)

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Characterization of Air Showers 40 10PeV Vertical CORSIKA showers. Hadrons cut. Looked at RF pattern on vertical string of 10 detectors every 10m starting at 200m deep, 150m from shower. A look at waveforms from single 1PeV and 10PeV events. Peaks taken from 10PeV waveforms to determine Cherenkov radiation pattern. Justification for raising the energy cuts.

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) 10PeV Waveforms on string

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Depth Profiles and Energy Cuts Waveform peaks at depth for 40 10PeV showers. Peak vmax values at different energy cuts.

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) RF vs core energy

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Parameterize Air Showers Use shower radius (R), shower length (L) and shower size (S) to fit shower radiation patterns. Peaks match up with some variation at the tails. Five event RF detection patterns (solid) with their parameterizations (dashed).

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Event Rate Calculation

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Shallow Array Concepts Drill 16 x 30m holes –1 dom per hole –4 antennas per dom 2 x 50m cables to each of four nearby strings & SJB 2 doms per cable

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) AURA geometry

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Summary Test beam for radio sure would be nice Air Shower Cores: E eff ~ 10% E p (at EeV) Synthetic RF looks usable CR Composition Measurement –Core energy anti-correlated with deep-  –p-Fe separation Three scenarios –Small subsurface array w/IceTop –AURA –ANITA

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) END

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Radial distributions by energy

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Sample the Cerenkov Ring

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Subshowers & Coherence of RF pulses

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Comparison of Fe/p

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Determining Cosmic Ray Composition AIRES showers (from S. Seunarine) E sh (r<20 cm) as proxy for radio High-lite: 10 PeV, True iron

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) Time Domain Waveforms

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) EeV/TeV again

Askaryan pulses from air shower cores, UMD Radio Mtg., June (Seckel) 1PeV Waveforms on String