C.Distefano Catania, 9 th – 11 th January 2006 LNS Gilda applications: NEMO and ANTARES NA4 Generic Application Meeting Carla Distefano for the NEMO Collaboration.

Slides:



Advertisements
Similar presentations
P. Sapienza, Laboratori Nazionali del Sud (INFN)NOW2004, sept A km 3 detector in the Mediterranean: status of NEMO Motivation for a km 3 detector.
Advertisements

R.Shanidze, B. Herold, Th. Seitz ECAP, University of Erlangen (for the KM3NeT consortium) 15 October 2009 Athens, Greece Study of data filtering algorithms.
Trigger issues for KM3NeT the large scale underwater neutrino telescope the project objectives design aspects from the KM3NeT TDR trigger issues outlook.
Antonis Leisos KM3NeT Collaboration Meeting the calibration principle using atmospheric showers the calibration principle using atmospheric showers Monte.
Consorzio COMETA - Progetto PI2S2 UNIONE EUROPEA NEMO Monte Carlo Application on the Grid R. Calcagno for the NEMO Collaboration.
Jan 2009 U. Katz: Astroparticle Physics 1 What is KM3NeT – the Vision  Future cubic-kilometre sized neutrino telescope in the Mediterranean Sea  Exceeds.
ANTARES and KM3NeT John Carr Centre de Physique de Particules de Marseille IN2P3 / MICINN meeting Madrid, 12 Jan 2009.
10/7/2003C.Spiering, VLVNT Workshop1. 10/7/2003C.Spiering, VLVNT Workshop2  With the aim of constructing a detector of km3 scale in the Northern hemisphere,
Antonis Leisos KM3NeT Design Study the calibration principle using atmospheric showers the calibration principle using atmospheric showers construction.
Use of floating surface detector stations for the calibration of a deep-sea neutrino telescope G. Bourlis, N. A. B. Gizani, A. Leisos, A. G. Tsirigotis,
Kay Graf University of Erlangen for the ANTARES Collaboration 13th Lomonosov Conference on Elementary Particle Physics Moscow, August 23 – 29, 2007 Acoustic.
ANTARES aims, status and prospects Susan Cartwright University of Sheffield.
Energy Reconstruction Algorithms for the ANTARES Neutrino Telescope J.D. Zornoza 1, A. Romeyer 2, R. Bruijn 3 on Behalf of the ANTARES Collaboration 1.
P. Sapienza, NOW 2010 The KM3NeT project  Introduction & Main objectives  The KM3NeT Technical Design Report  Telescope physics performance  New developments.
The ANTARES Neutrino Telescope Mieke Bouwhuis 27/03/2006.
Antares/KM3NeT M. de Jong. neutrinos  p Scientific motivation: – origin cosmic rays – birth & composition relativistic jets – mechanism of cosmic particle.
C.Distefano Barcelona July 4 – 7, 2006 LNS Detection of point-like neutrino sources with the NEMO-km 3 telescope THE MULTI-MESSENGER APPROACH TO UNIDENTIFIED.
Paolo Piattelli - KM3NeTIAPS - Golden, 6-8 may 2008 KM3NeT: a deep-sea neutrino telescope in the Mediterranean Sea Paolo Piattelli - INFN/LNS Catania (Italy)
KM3NeT The Birth of a Giant V. Popa, KM3NeT Collaboration Institute for Space Sciences, Magurele-Bucharest, Romania.
Hanoi, Aug. 6-12, 2006 Pascal Vernin 1 Antares Status report P.Vernin CEA Saclay, Dapnia On behalf of the Antares collaboration P.Vernin
Coincidence analysis in ANTARES: Potassium-40 and muons  Brief overview of ANTARES experiment  Potassium-40 calibration technique  Adjacent floor coincidences.
P. Piattelli, CRNT meeting, Paris december 2004 High Energy Neutrino Astronomy Status and perspectives of the high energy neutrino observatories.
C.DistefanoCRIS 2008 – Salina, September The KM3Net Consortium Istituto Nazionale di Fisica Nucleare Laboratori Nazionali del Sud Towards a km3-scale.
Exploring the Cosmos with Neutrinos Aart Heijboer …all of them. nm
Apostolos Tsirigotis Simulation Studies of km3 Architectures KM3NeT Collaboration Meeting April 2007, Pylos, Greece The project is co-funded by the.
Status of KM3NeT (Detector Design Optimisations) Christopher Naumann, CEA Saclay – IRFU / SPP for the KM3NeT consortium 44 th Reconcontres de Moriond,
Petten 29/10/99 ANTARES an underwater neutrino observatory Contents: – Introduction – Neutrino Astronomy and Physics the cosmic ray spectrum sources of.
Antoine Kouchner Université Paris 7 Laboratoire APC - CEA/Saclay for the ANTARES collaboration Neutrino Astronomy: a new look at the Galaxy Astronomy Neutrino.
CEA DSM Irfu The ANTARES Neutrino Telescope A status report Niccolò Cottini on behalf of the ANTARES Collaboration 44 th Rencontres de Moriond February.
Piera Sapienza – VLVNT Workshop, 5-8 october 2003, Amsterdam Introduction and framework Simulation of atmospheric  (HEMAS and MUSIC) Response of a km.
V.Bertin CPPM / ANTARES Coll. - Moriond ANTARES : A deep-sea 0.1 km² neutrino telescope Vincent Bertin - CPPM-Marseille on behalf of the Antares.
SINP MSU, July 7, 2012 I.Belolaptikov behalf BAIKAL collaboration.
Agustín Sánchez-Losa IFIC (CSIC-Universitat de València) Transient sources, like AGNs or Gamma Ray Bursters, are among.
ANTARES  Physics motivation  Recent results  Outlook 4 senior physicists, ~5 PhD students, ~5 technicians M. de Jong RECFA 23 September 2005.
KM3NeT International Solvay Institutes 27  29 May 2015, Brussels, Belgium. Maarten de Jong Astro-particle and Oscillations Research with Cosmics in the.
The NEMO Project: Toward a km 3 Neutrino Telescope in the Mediterranean Sea M. Circella, INFN Bari NUPPAC-05, Nov The NEMO Project (NEutrino Mediterranean.
 NEMO The NEMO Status Report M.Taiuti on behalf of the NEMO Collaboration Merida, Yucatan, Mexico 30th International Cosmic Ray Conference.
G. RiccobeneIFAE, Pavia 19-21Aprile 2006 Astronomia a neutrini con km 3 sott’acqua e ghiaccio.
Ronald Bruijn – 10 th APP Symposium Antares results and status Ronald Bruijn.
Isabella Amore Laboratori Nazionali del Sud - INFN, Catania International School of Cosmic Ray Astrophysics 15th Course: "Astrophysics at Ultra-high Energies"
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
Alexander Kappes Erlangen Centre for Astroparticle Physics for the ANTARES collaboration IAU GA, SpS 10, Rio de Janeiro, Aug Status of Neutrino.
The ANTARES detector: background sources and effects on detector performance S. Escoffier CNRS Centre de Physique des Particules de Marseille on behalf.
R. Coniglione, VLVnT08, Toulon April ‘08 KM3NeT: optimization studies for a cubic kilometer neutrino detector R. Coniglione P. Sapienza Istituto.
PHY418 Particle Astrophysics
June 6, 2006 CALOR 2006 E. Hays University of Chicago / Argonne National Lab VERITAS Imaging Calorimetry at Very High Energies.
Astroparticle physics with large neutrino detectors  Existing detectors  Physics motivation  Antares project  KM3NeT proposal M. de Jong.
Status report on the Antares project Luciano Moscoso (DSM/DAPNIA, CEA/Saclay F Gif-sur-Yvette) (On behalf of the ANTARES collaboration)
Sebastian Kuch, Rezo Shanidze Preliminary Studies of the KM3NeT Physics Sensitivity KM3NeT Collaboration Meeting Pylos, Greece, April 2007.
KM 3 Neutrino Telescope European deep-sea research infrastructure DANS – symposium Maarten de Jong.
Search for diffuse cosmic neutrino fluxes with the ANTARES detector Vladimir Kulikovskiy The ANTARES Collaboration 3-9 August 2014ANTARES diffuse flux.
31/03/2008Lancaster University1 Ultra-High-Energy Neutrino Astronomy From Simon Bevan University College London.
C.Distefano KM3NET ‘Physics and Simulation (WP2)’ Oct 24 – 25, 2006 LNS NEMO software Carla Distefano for the NEMO Collaboration KM3NET ‘Physics and Simulation.
STATUS AND PHYSICS GOALS OF KM3NET Paolo Piattelli P. Piattelli, ICHEP14 Valencia INFN – LNS, Catania (Italy)
Antares status and plans  Reminder  Project status  Plans M. de Jong.
Isabella Amore VLV T08, Toulon, France April 2008 International Workshop on a Very Large Volume Neutrino Telescope for the Mediterranean Sea Results.
Status and Perspectives of the BAIKAL-GVD Project Zh.-A. Dzhilkibaev, INR (Moscow), for the Baikal Collaboration for the Baikal Collaboration September.
Geant4 Simulation for KM3 Georgios Stavropoulos NESTOR Institute WP2 meeting, Paris December 2008.
1 Cosmic Ray Physics with IceTop and IceCube Serap Tilav University of Delaware for The IceCube Collaboration ISVHECRI2010 June 28 - July 2, 2010 Fermilab.
Search for Ultra-High Energy Tau Neutrinos in IceCube Dawn Williams University of Alabama For the IceCube Collaboration The 12 th International Workshop.
KM3NeT Neutrino conference 2-7 June 2014, Boston, U.S.A. Maarten de Jong on behalf of the KM3NeT collaboration The next generation neutrino telescope in.
KM3NeT P.Kooijman Universities of Amsterdam & Utrecht for the consortium.
The Antares Neutrino Telescope
Corso di Calcolo Parallelo Grid Computing
Systematic uncertainties in MonteCarlo simulations of the atmospheric muon flux in the 5-lines ANTARES detector VLVnT08 - Toulon April 2008 Annarita.
discovery potential of Galactic sources
Instrumentation and Methods in Astroparticle Physics Physics 801
MUPAGE: A fast muon generator
on behalf of the NEMO Collaboration
ICRC2011, 32ND INTERNATIONAL COSMIC RAY CONFERENCE, BEIJING 2011
Presentation transcript:

C.Distefano Catania, 9 th – 11 th January 2006 LNS Gilda applications: NEMO and ANTARES NA4 Generic Application Meeting Carla Distefano for the NEMO Collaboration

C.Distefano Catania, 9 th – 11 th January 2006 LNS Why neutrino astronomy? The detection of high energy cosmic rays (up to eV) are milestones in modern astrophysics but there are still several open questions: Particle acceleration mechanism in astrophysical sources Identification of high energy CR sources Solution of UHECR puzzle The detection of high energy cosmic rays (up to eV) are milestones in modern astrophysics but there are still several open questions: Particle acceleration mechanism in astrophysical sources Identification of high energy CR sources Solution of UHECR puzzle Neutrinos traverse space without being deflected or attenuated –They point back to their sources –They allow to view into dense environments Neutrinos are produced in high energy hadronic processes –They can allow distinction between hadronic and leptonic acceleration mechanisms Neutrinos traverse space without being deflected or attenuated –They point back to their sources –They allow to view into dense environments Neutrinos are produced in high energy hadronic processes –They can allow distinction between hadronic and leptonic acceleration mechanisms

C.Distefano Catania, 9 th – 11 th January 2006 LNS Neutrino production in cosmic accelerators Halzen Proton acceleration Fermi mechanism proton spectrum dN p /dE ~E -2 Neutrino production Proton interactions p  p (SNR,X-Ray Binaries) p   (AGN, GRB, microQSO) decay of pions and muons Astrophysical jet Particle accelerator Electrons are responsible for lower energy gamma fluxes (synchrotron, IC)

C.Distefano Catania, 9 th – 11 th January 2006 LNS Candidate sources of UHE (> TeV) neutrinos Jets and cores of Active Galactic NucleiGamma Ray Bursts Galactic Centre Galactic Microquasars Galactic SuperNova Remnants

C.Distefano Catania, 9 th – 11 th January 2006 LNS The observation of TeV neutrino fluxes require km 3 scale detectors neutrino muon Cherenkov light ~5000 PMTs Connection to the shore neutrino atmospheric muon depth >3000m

C.Distefano Catania, 9 th – 11 th January 2006 LNS Neutrino telescopes brief history 80’s:DUMAND R&D 90’s:BAIKAL, AMANDA, NESTOR 2k’s:ANTARES, NEMO R&D 2010:IceCube Mediterranean KM3... AMANDA IceCube Mediterranean km 3 BAIKAL DUMAND Pylos La Seyne Capo Passero

C.Distefano Catania, 9 th – 11 th January 2006 LNS ANTARES ANTARES is installing a 0.1 km 2 demonstrator detector close to Toulon at D=2400 m. 12 strings 25 stories / string 3 PMTs / storey 900 PMTs ~70 m 350 m 100 m 14.5 m Submarine links Junction Box 40 km to shore Anchor/line socket to be deployed by ANTARES deployed Line0 and Milom, underwater connection Apr

C.Distefano Catania, 9 th – 11 th January 2006 LNS L a = 66  5 m pure seawater 3500 m Capo Passero NEMO The NEMO Collaboration is dedicating special efforts to: search, characterization and monitoring of a deep sea site adequate for the installation of the Mediterranean km 3. The NEMO Collaboration is dedicating special efforts to: search, characterization and monitoring of a deep sea site adequate for the installation of the Mediterranean km 3. development of technologies for the km 3 (technical solutions chosen by small scale demostrators are not directly scalable to a km 3 )

C.Distefano Catania, 9 th – 11 th January 2006 LNS Proposed NEMO km 3 architecture Proposed NEMO detector : 5000: 6000 PMTs 80:100 towers arranged in a lattice ~140 m between towers The NEMO km3 architecture is based on the NEMO-tower module. 1.2 km Height: compacted15:20 m total750 m instrumented600 m n. beams16 to 20 n. PMT64 to 80 Beams: length20m spacing40 m The tower is a semi-rigid 3D structure designed to allow easy deployment and recovery. High local PMT density is designed to perform local trigger. 750 m 10’’ PMTs

C.Distefano Catania, 9 th – 11 th January 2006 LNS The NEMO test site in Catania: phase 1 The NEMO Collaboration is undergoing the Phase 1 of the project, installing a fully equipped Deep-Sea facility to test prototypes and develop new technologies for the detector. Shore laboratory port of Catania Underwater test site: 25 km E offshore Catania at 2000 m depth e.o. cable from shore TSS Frame + acoustic detectors To be completed in 2006 Junction Box NEMO mini-tower (4 floors) Deployed on Jan 2005 An electro-optical cable (10 fibres, 4 conductors) was deployed on It connects the shore laboratory, in the Port of Catania, with the underwater test site

C.Distefano Catania, 9 th – 11 th January 2006 LNS NEMO: Find the most efficient displacement of PMTs (effective area > 1 km 2 and angular resolution ~0.1°) taking into account technological constraints (mechanics, deployment, electronics)... and budget ! NEMO: Find the most efficient displacement of PMTs (effective area > 1 km 2 and angular resolution ~0.1°) taking into account technological constraints (mechanics, deployment, electronics)... and budget ! ANTARES: Study detector response to neutrino fluxes Optimization of analysis procedures (noise rejection,…) ANTARES: Study detector response to neutrino fluxes Optimization of analysis procedures (noise rejection,…) Present goals of Monte Carlo simulations

C.Distefano Catania, 9 th – 11 th January 2006 LNS ANTARES Monte Carlo Simulation Tools parameters detector geometry file input event parameters initial tracks hits signal and 40 K hits reconstructed tracks gendet generator code km3 modk40 reco muon propagation and light simulation noise and electronics simulation track reconstruction code I/O event generator event generator: astrophysical signal atmospheric bkg

C.Distefano Catania, 9 th – 11 th January 2006 LNS Atmospheric neutrino and muon background Atmospheric neutrinos: upward tracks are good neutrino candidates; direction and energy criteria can be used to discriminate background from astrophysical signals. Atmospheric muons: installation at Depth > 3000 m downward looking telescope but background due to mis- reconstructed muons; rejection of atmospheric muons background: quality cuts. Bugaev, E.V., 1998, Phys. ReV., D58,

C.Distefano Catania, 9 th – 11 th January 2006 LNS Simulation of muon background Background due to atmospheric muon flux is several orders of magnitude larger than the expected signal. We need to optimize reconstruction algorithms in order to minimize the number of mis-reconstructed tracks (up-going tracks). These algorithms have to be tested and applied on a muon sample as large as the expected one in 1 year (mass production), simulation of multi muon events with complete simultation are also mandatory. The NEMO and ANTARES Collaborations have chosen to use the CORSIKA and MUSIC codes to simulate the muon background reaching the detector. Official CORSIKA page MUSIC: Antonioli et al, 1997, Astrop. Phys. 7, 375.

C.Distefano Catania, 9 th – 11 th January 2006 LNS Mass production of atmospheric muons with CORSIKA CORSIKA is a program for detailed simulation of extensive air showers initiated by high energy cosmic ray particles: the particles are tracked through the atmosphere until they undergo reactions with the air nuclei or decay; atmospheric muons reaching the sea level are written in the output file. Muons are then propagated in sea water up to the detectors (MUSIC): the number of muons reaching the detectors depends on their geometrical surfaces and on site depth (muon energy loss in sea water) ANTARES A geom ~0.1 km 2 D=2400 m NEMO A geom ~ km 2 D=3500 m Mass production of Corsika events is conducted jointly by NEMO and ANTARES

C.Distefano Catania, 9 th – 11 th January 2006 LNS Hardware tools for mass production Atmospheric muons mass production requires intensive use of CPU and storage.  NEMO Collaboration decided to use GRID First Step: GILDA-CT GILDA is an excellent tutorial for GRID. Easy access to the CPU resources (and less burocracy!) Close interaction with GILDA team Second Step: GRID Mass Production requires a larger number of CPUs with fast processors

C.Distefano Catania, 9 th – 11 th January 2006 LNS Open Problems Monte Carlo simulations with a sufficient number of events (10 6 primaries) require large CPU Time  job CPU time limit 48 h in GRID. CPU time limits depend on CPU speed. We need to require the attribute: GlueHostProcessorClockSpeed>1800 This attribute is not published in some CEs. The migration to VOMS led problems due to the short (default 12 h) duration of the VOMS credential: see talk of E. Giorgio. A crash error is often LRC endpoint not found RMC endpoint not found The Local Replica Catalog end point not published by the CE The Replica Metadata Catalog end point not published by the CE Job crash: sometimes it is not clear or understood  poor diagnostics (at least for us!)

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Running CORSIKA in the GRID: CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run

C.Distefano Catania, 9 th – 11 th January 2006 LNS The Corsika JDL script: corsika_0.jdl Type = "Job"; JobType = "Normal"; Executable = "run-corsika.sh" ; StdOutput = "std.out"; StdError = "std.err"; Requirements = (other.GlueCEPolicyMaxCPUTime>2800)&&(other.GlueHostProcessorClockSpeed>1800); RetryCount = 2; MyProxyServer = "grid014.ct.infn.it"; InputSandbox = {"run-corsika.sh", "corsika.exe", "EGSDAT4_.05", "EGSDAT4_.15", "EGSDAT4_.4", "EGSDAT4_1.", "EGSDAT4_3.", EGSDAT4_.25", "NUCNUCCS", "SECTNU", "QGSDAT01", "inputs_h2_0"}; OutputSandbox = {"std.out","std.err","corsika_p_h2_0.log"}; OutputData = { [ OutputFile = "corsika_p_h2_0.evt.gz"; LogicalFileName = "lfn:p_h2_0.out"; StorageElement = "grid005.ct.infn.it"; ] };

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Running CORSIKA in the GRID: CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) Job retrieving (edg-job-get-output) CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) Job retrieving (edg-job-get-output) Download the output file from SE (~200 MB zipped file) lcg-cp --vo gridit lfn:p_h2_0.out file:corsika_p_h2_0.evt.gz

C.Distefano Catania, 9 th – 11 th January 2006 LNS Used CPU times on GRID  Tutorial on GILDA (October 2004)  Mass production on INFN-GRID (since March 2005) GRID Italia CPU time for the statistics already collected in Catania: ~ 6 years Disk space for the statistics already collected in Catania: ~ 220 GB (zipped files)

C.Distefano Catania, 9 th – 11 th January 2006 LNS Future applications on the GRID CORSIKA events initial tracks at the detector hits signal and 40 K hits reconstructed tracks MUSIC km3 modk40 reco muon propagation and light simulation noise and electronics simulation track reconstruction code I/O muon propagation up to the detector atm. muon events at the sealevel We would like to run the whole simulation chain on the GRID. Many codes linked with several libraries and that handle big I/O files (~ 1 GB). Codes are already compiled and a trial job was successful run.

C.Distefano Catania, 9 th – 11 th January 2006 LNS Summary and Outlook Simulation of neutrino telescope response requires a mass production of atmospheric muon background events; ANTARES and NEMO are jointly conducting a mass production of Corsika events  since March 2005, the NEMO Collaboration uses GRID for mass production; The next step is to implement the whole simulation chain in GRID  many different programs linked with several libraries and with big file to handle. The first attempt has been successful; At the LNS in Catania, a new GRID CE and SE will be soon available.

C.Distefano Catania, 9 th – 11 th January 2006 LNS

C.Distefano Catania, 9 th – 11 th January 2006 LNS Generation of atmospheric muons with CORSIKA Corsika is a program for detailed simulation of extensive air showers initiated by high energy cosmic ray particles: the particles are tracked through the atmosphere until they undergo reactions with the air nuclei or decay; atmospheric muons reaching the sea level are written in the output file.  Primary ions -> p, He, N, Mg, Fe  Primary energy -> TeV/nucleone  Primary zenith angles –> 0°  85°  Energy threshold for muons at sea level -> 0.5 TeV for ions between 0° and 60° and 1 TeV for ions between 60° and 85°  Slope primary spectrum  E -2 Simulation inputs:

C.Distefano Catania, 9 th – 11 th January 2006 LNS Candidate sites for the km 3 ANTARES APpEC Meeting, January :4000 m 2400 m 3400 m NEMO NESTOR

C.Distefano Catania, 9 th – 11 th January 2006 LNS # # This file /opt/edg/etc/alice/edg_wl_ui.conf is managed by LCFG. Do not modify! # [ VirtualOrganisation = "gridit"; NSAddresses = "grid014.ct.infn.it:7772"; LBAddresses = "grid014.ct.infn.it:9000"; ] CT-vo.conf # # Autogenerated by LCFG cliconfig component. Do not modify! # [ rank = - other.GlueCEStateEstimatedResponseTime; requirements = other.GlueCEStateStatus == "Production"; RetryCount = 3; ErrorStorage = "/tmp"; OutputStorage = "/tmp/jobOutput"; ListenerPort = 44000; ListenerStorage = "/tmp"; LoggingTimeout = 30; LoggingSyncTimeout = 30; LoggingDestination = "grid014.ct.infn.it:9002"; # Default NS logger level is set to 0 (null) # max value is 6 (very ugly) NSLoggerLevel = 0; DefaultLogInfoLevel = 0; DefaultStatusLevel = 0; DefaultVo = "atlas"; ] CT.conf

C.Distefano Catania, 9 th – 11 th January 2006 LNS run-corsika_0.sh #!/bin/bash export ION=p export range=h2 nrun=0 ln -s inputs_${range}_${nrun} inputs chmod +x corsika.exe time./corsika.exe > corsika_${ION}_${range}_${nrun}.log gzip corsika_${ION}_${range}_${nrun}.evt

C.Distefano Catania, 9 th – 11 th January 2006 LNS submit-job.sh #!/bin/bash nrun=1 NLIMIT=10 export range=h2 while [ $nrun -le "$NLIMIT" ] do sed "s/160/16${nrun}/g" inputs_${range}_0 > temp1 sed "s/170/17${nrun}/g" temp1 > temp2 sed "s/180/18${nrun}/g" temp2 > temp3 sed "s/aaaa/${nrun}/g" temp3 > inputs_${range}_${nrun} sed "s/nrun=0/nrun=${nrun}/g" run-corsika_0.sh > run-corsika.sh sed "s/${range}_0/${range}_${nrun}/g" corsika_0.jdl > corsika.jdl edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl nrun=$(($nrun+1)) done

C.Distefano Catania, 9 th – 11 th January 2006 LNS Results: present event statistics Primary = 0°-60° = 60°- 85° TeV/nucleon V TeV/nucleon V2* TeV/nucleon V3** TeV/nucleon h TeV/nucleon h2* TeV/nucleon h3** p (10 8 ) (10 8 ) 10 8 (10 7 ) He 10 8 (10 8 ) 10 8 (10 8 ) 10 8 (10 7 ) N 10 8 (10 8 ) (10 8 ) (10 6 ) Mg 10 8 (10 8 ) (10 8 ) (10 6 ) Fe (3·10 7 ) (3·10 7 ) 10 6 (10 6 ) * NEMO in charge for production ** ANTARES in charge for production Done Done Done Done Done Done Done Done

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) Job retrieving (edg-job-get-output) Running CORSIKA in the GRID:

C.Distefano Catania, 9 th – 11 th January 2006 LNS GRID applications details CORSIKA compiled and linked in “USER INTERFACE” on GRID-CT Produce a script for launching the code Produce the jdl file for a specific run Submit the jdl file using VO GRIDIT (edg-job-submit) edg-job-submit --config CT.conf --config-vo CT-vo.conf -o job_run.name corsika.jdl Status inquire (edg-job-status) Job retrieving (edg-job-get-output) Download the output files from SE (~200 MB zipped file) lcg-cp --vo gridit lfn:p_h2_0.out file:corsika_p_h2_0.evt.gz Running CORSIKA in the GRID: