LEMMA Test Beam Meeting

Slides:



Advertisements
Similar presentations
1 Pion beam tracker for HADES Jerzy Pietraszko CBM Collaboration Meeting, March 9-13, 2009, GSI, Darmstadt.
Advertisements

Status of DHCAL Slice Test Data Analysis Lei Xia ANL-HEP All results preliminary.
Simulation of the RPC Response José Repond Argonne National Laboratory CALICE Collaboration Meeting University Hassan II Casablanca, Morocco September.
SKS Minus Detectors in detail Tohoku Univ. K.Shirotori.
The Silicon Track Trigger (STT) at DØ Beauty 2005 in Assisi, June 2005 Sascha Caron for the DØ collaboration Tag beauty fast …
Status of Tracking at DESY Paul Dauncey, Michele Faucci Giannelli, Mike Green, Hakan Yilmaz, Anne Marie Magnan, George Mavromanolakis, Fabrizio Salvatore.
Status of  b Scan Jianchun Wang Syracuse University Representing L b scanners CLEO Meeting 05/11/02.
GLAST LAT Project Test Beam Meeting, June 6, 2006 S. Funk 1/6 PS Positron Simulations Stefan Funk June 6, 2006.
2/10/2000 CHEP2000 Padova Italy The BaBar Online Databases George Zioulas SLAC For the BaBar Computing Group.
PERFORMANCE OF THE MACRO LIMITED STREAMER TUBES IN DRIFT MODE FOR MEASUREMENTS OF MUON ENERGY - Use of the MACRO limited streamer tubes in drift mode -Use.
Simulation issue Y. Akiba. Main goals stated in LOI Measurement of charm and beauty using DCA in barrel –c  e + X –D  K , K , etc –b  e + X –B 
Geant4 Acceptance Suite for Key Observables CHEP06, T.I.F.R. Mumbai, February 2006 J. Apostolakis, I. MacLaren, J. Apostolakis, I. MacLaren, P. Mendez.
Monte Carlo Comparison of RPCs and Liquid Scintillator R. Ray 5/14/04  RPCs with 1-dimensional readout (generated by RR) and liquid scintillator with.
Thomas Jefferson National Accelerator Facility Page 1 EC / PCAL ENERGY CALIBRATION Cole Smith UVA PCAL EC Outline Why 2 calorimeters? Requirements Using.
1 Calorimeter in G4MICE Berkeley 10 Feb 2005 Rikard Sandström Geneva University.
August 26, 2003P. Nilsson, SPD Group Meeting1 Paul Nilsson, SPD Group Meeting, August 26, 2003 Test Beam 2002 Analysis Techniques for Estimating Intrinsic.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting Rutherford Appleton Lab Tuesday 25 th April 2006 M. Ellis.
David Adams ATLAS DIAL: Distributed Interactive Analysis of Large datasets David Adams BNL August 5, 2002 BNL OMEGA talk.
LM Feb SSD status and Plans for Year 5 Lilian Martin - SUBATECH STAR Collaboration Meeting BNL - February 2005.
1 A first look at the KEK tracker data with G4MICE Malcolm Ellis 2 nd December 2005.
Studying the efficiency and the space resolution of resistive strips MicroMegas Marco Villa – CERN MAMMA meeting Tuesday, 13 th December 2011 CERN, Geneva.
Interactions of hadrons in the SiW ECAL Towards paper Naomi van der Kolk.
Linda R. Coney – 5 November 2009 Online Reconstruction Linda R. Coney 5 November 2009.
Progress on the beam tracking instrumentation Position measurement device Tests performed and their resolution Decision on electronics Summary.
Start and Vertex Detector W. Boeglin, A.Klein Current Design: 3300 scintillating fibers 1mm diameter 3 double layers (1 axial, 2 stereo) cylindrical geometry.
Magnetized hadronic calorimeter and muon veto for the K +   +  experiment L. DiLella, May 25, 2004 Purpose:  Provide pion – muon separation (muon veto)
1 DT Local Reconstruction on CRAFT data Plots for approval CMS- Run meeting, 26/6/09 U.Gasparini, INFN & Univ.Padova on behalf of DT community [ n.b.:
TRANSMISSION LENGTH STATUS HAROLD YEPES-RAMIREZ IFIC, January 12 th
The Detector Performance Study for the Barrel Section of the ATLAS Semiconductor Tracker (SCT) with Cosmic Rays Yoshikazu Nagai (Univ. of Tsukuba) For.
Khaled Belkadhi (LLR-Ecole Polytechnique)1 DHCAL Test Beam Results using Full Train Reconstruction Khaled Belkadhi.
Mark Dorman Separation Of Charged Current And Neutral Current Events In The MINOS Far Detector Using The Hough Transform Mark Dorman 16/12/04.
Thomas Ruf, CERN EP Experience with C++ and ROOT used in the VX Beam Test Thomas Ruf, CERN, EP  Why? Event structure for VX-data rather complex: raw hits.
Can we detect a marble tomb with cosmic muons ? Corinne Goy, Max Chefdeville, Jean Jacquemier, Yannis Karyotakis 21 December 2015.
1 Simulations Purpose of the simulation codes Structure of the E866 simulation codes Issues of simulations for E906 Jen-Chieh Peng University of Illinois.
MAUS Status A. Dobbs CM43 29 th October Contents MAUS Overview Infrastructure Geometry and CDB Detector Updates CKOV EMR KL TOF Tracker Global Tracking.
Track Reconstruction in MUCH and TRD Andrey Lebedev 1,2 Gennady Ososkov 2 1 Gesellschaft für Schwerionenforschung, Darmstadt, Germany 2 Laboratory of Information.
Review and Perspective of Muon Studies Marco Destefanis Università degli Studi di Torino PANDA Collaboration Meeting GSI (Germany) September 5-9, 2011.
ΜTPC Reconstruction Status Report (…mostly a late night / weekend project … ) D. A. Jensen March 1, 2007.
Beam test Analysis Micromegas TPC by Wenxin Wang.
MUC Reconstruction status and GDML Management You Zhengyun School of Physics, PKU
Results with the RPC system of OPERA and perspectives
Background simulations: update and simulations of absorbed dose
Online Monitoring : Detector and Performance check
Neutrino factory near detector simulation
F2F Tracking Meeting, Prague 12/12/2013
MICE event viewer status - Mihailo Savic - CM 45
M. Kuhn, P. Hopchev, M. Ferro-Luzzi
P0D reconstruction/analysis update
Beam Gas Vertex – Beam monitor
Studies for Phase-II Muon Detector (|η| = ) – Plans
Bonn Test Station data analysis with PandaRoot
Interactions of hadrons in the Si-W ECAL
Tun Sheng Tan AUGUST UW Analysis Meeting Summer 2014
E. Barbuto, C. Bozza, A. Cioffi, M. Giorgini
DT Local Reconstruction on CRAFT data
ATLAS B-physics important periods
Slice Test: Preliminary Data Analysis The Ohio State University
Data Analysis in Particle Physics
The Silicon Track Trigger (STT) at DØ
VEPP-2000 plans for the study of the nucleon form factors
CMS Pixel Data Quality Monitoring
Imaging crystals with TKR
DQM for the RPC subdetector
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Search for coincidences and study of cosmic rays spectrum
Contents First section: pion and proton misidentification probabilities as Loose or Tight Muons. Measurements using Jet-triggered data (from run).
Quarkonium production, offline monitoring, alignment & calibration
Recent works on AMS TANG Zhi-Cheng.
Beam properties for run
Presentation transcript:

LEMMA Test Beam Meeting 28/6/2017 Report on recent software activities A. Bertolin, L. Sestini

Tuning of Fe-shield position rule for tuning: shielding should not intercept any of the mu- from annihilation if the muon chamber length exceed 2000 mm the x upper “corner” should not exceed + 1000 mm MCMC_v5_20k_FTFP_air_gun4cmq_shield50cm+390mm.root MCMC_v4_10k_FTFP_air.root x axis: from 0 mm to -1000 m y axis: 1 m z axis: 1 m cross checked with Marco D. x axis: from +390 mm to -1610 mm y axis: 1 m z axis: 0.5 m

Position pile-up per event Double_t positrons_x_spill=5.e+6; Double_t spill_delta_t=4.8; // sec Double_t time_integration=1.e-6; // sec i.e. 5 musec Double_t Poisson_mean=(positrons_x_spill*(time_integration/spill_delta_t)); cout << "positrons per spill = " << Poisson_mean << endl; positrons per spill = 1.04167 root [0] .x Poisson.C(1.04167) entries at 0 vetoed by the muon trigger outcome: 30 % of 2 positions 10 % of 3 positrons

Mu pairs per spill Run Summary: Number of events processed: 1M Time: 234632s = 2d 17h 10min 32s Dim: 5.1GB Mu pairs per spill generated: 1M cross section enhancement: 1e+3 402 (reco) / 516 (in acceptance) [integrated efficiency: 0.703869] 5 x 402 / 1e+3 = 2.00 reco pairs per spill 2 spill per minute -> 4 pairs per minute 1 hour (60 minutes) -> 240 pairs per hour 1 hour of data should be enough to get sufficiently filled “monitoring histograms” A. Lorenzon

Recent software work tupleTransformer.C applied to: MC tuple with one entry per HIT output: MC tuple with one entry per EVENT, content defined in tupla.h in addition subdetectors 50,51 and 55,56 are “defined” at: x = +70 (-70) mm for 50 (51) +- 50 mm with Z=17000 mm x = +170 (-170) mm for 55 (56) +- 50 mm with z=20000 mm https://github.com/svaninigit/LEMMA/blob/master/sw/Common/tupla.h /!\ “undefined” quantities should be set to -9999. for illustration purposes: yh[i] of an “X sensitive layer” = -9999. 2. xh[i] – zh[i] and yh[i] – zh[i] series belonging to the same muon track are identified by the same value of itrack[i] always assumes one incoming e+ per event

Recent software work (cont.) work has started in Padova to properly reconstruct and put the muon chamber data in the format defined by tuple.h (S. Vanini, A. Lorenzon) for the Si detectors we expect to have an ASCII file, with an AXIAL like format so to say, like the one circulated by Laura B., which can be “merged” in the muon data tuple at the offline level with a suitable script (some sort of event builder process)

Recent software work: alignment and monitoring tool tbanalysis.C, based on the format defined by tuple.h root 5.34.21 a few overall activity plots requires activity in 10 20 30 40 50 55 70, both x and y mu-: >= 8 x-hits && >= 4 y-hits backward propagation to 50/55 40 30 -> alignment mu+: backward propagation to 51/56 -> alignment to be added: hits plotting tool: x-z, y-z views (event display) output root file with computed information: n_x_hits_mum x_pos_mum[11] z_x_pos_mum[11] x_pos_mum_err[11] n_y_hits_mum y_pos_mum[11] y_x_pos_mum[11] y_pos_mum_err[11] n_x_hits_mup x_pos_mup[11] z_x_pos_mup[11] x_pos_mup_err[11] y_pos_mup[11] y_x_pos_mup[11] y_pos_mup_err[11] limited to subdet 51, 56 and 70 hits can be translated in a subdetector dependent way before any use copy of whatever is recorded in 10 and 20

is alive plot

mu- line, difference between the extrapolated and the MEASURED position 55 50 X Y 40 30 estimated p effect

mu+ line, difference between the extrapolated and the MEASURED position 56 51 X Y X coordinate in the mu+ case shows a very poor resolution: bug in the code we are trying to spot or due to multiple scattering in iron + air the RMS blows up to 40 mm (early studies on the mu+ line where made in vacuum using concrete as absorber)

Special beam requests mu- beam, as monochromatic as possible, at energies of 18, 20, 22, 24, 26, 28 GeV need 1 k mu- per point same reversing B or using mu+ x y distribution: ideally as for the e+ beam, flat over 2 cm x 2 cm MCMC_v5_10k_mumu_air_gun4cmq_shield50cm.root