Sensitivity of CNGS muon

Similar documents
The CNGS neutrino beam

Latest Results from the OPERA Experiment (and new Charge Reconstruction)

CNGS neutrino beam: from CERN to Gran Sasso

CNGS beam monitor with LVD

First neutrino beam and cosmic tracks. GDR neutrino

Results from the OPERA experiment in the CNGS beam

arxiv: v1 [hep-ex] 1 Oct 2015

Performance of the ICARUS T600 detector

Status and Results of the UA9 Crystal Collimation Experiment at the CERN-SPS

Particle Detectors A brief introduction with emphasis on high energy physics applications

The ICARUS Project FRONTIERS IN CONTEMPORARY PHYSICS II. Vanderbilt University, March 5-10, Sergio Navas (ETH Zürich) " Atmospheric neutrinos

Calorimetry in particle physics experiments

PoS(HEP2005)177. Status of the OPERA experiment. Francesco Di Capua. Universita Federico II and INFN.

Simulations and Measurements of Secondary Electron Emission Beam Loss Monitors for LHC

Theory English (Official)

Neutrino physics with the SHiP experiment at CERN

Application of GLoBES: GLACIER on conventional neutrino beams

Commissioning and Calibration of the Zero Degree Calorimeters for the ALICE experiment

ICARUS T600 experiment: latest results and perspectives

Study of possible opportunities for leptonic CP violation and mass hierarchy at LNGS


Tools of Particle Physics I Accelerators

CALICE Si-W EM Calorimeter: Preliminary Results of the Testbeams 2006

Horn R&D. S. Gilardoni. Speaker A. Fabich CERN AB

MINOS. Physics Program and Construction Status. Karol Lang The University of Texas at Austin. YITP: Neutrinos and Implications for Physics Beyond

The ATLAS Liquid Argon Calorimeter: Construction, Integration, Commissioning Ph. Schwemling on behalf of the ATLAS LAr Group

CNGS - CERN NEUTRINOS TO GRAN SASSO

Updated results of the OPERA long baseline neutrino experiment

Muon reconstruction performance in ATLAS at Run-2

Les Premières Données dans ATLAS et le Calorimètre à Argon Liquide

Design of Beam Halo Monitor for CMS

Long Baseline Neutrinos

Charge readout and double phase

Latest News On NuMI Beam Simulation

Results from the OPERA experiment in the CNGS beam

New Hadroproduction results from the HARP/PS214 experiment at CERN PS

Tracking properties of the ATLAS Transition Radiation Tracker (TRT)

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

Digital Imaging Calorimetry for Precision Electromagnetic and Hadronic Interaction Measurements

Calculation of the Dose Equivalent Rate from Induced Radioactivity Around the CNGS Target and Magnetic Horn

Today: Part I: Neutrino oscillations: beam experiments. Part II: Next tutorials: making distributions with histograms and ntuples

Commissioning of the ATLAS LAr Calorimeter

Status of ATLAS and Preparation for the Pb-Pb Run

ATLAS Tile Calorimeter Calibration and Monitoring Systems

Paolo Agnes Laboratoire APC, Université Paris 7 on behalf of the DarkSide Collaboration. Dark Matter 2016 UCLA 17th - 19th February 2016

Calibration and Performance of the ATLAS Tile Calorimeter During the LHC Run 2

HIRA CSI DETECTOR RESPONSE TO LOW ENERGY PROTONS

Test setup, APDs,, preamps Calibration procedure Gain monitoring with LED Beam test results Future R&D options

MINOS Flux Determination

The CNGS project. Pasquale Migliozzi INFN - Napoli

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Performance test of triple GEM detector at CERN n_tof facility

Muon Alignment at CMS

b Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program

Latest results of OPERA

BNL Very Long Baseline Neutrino Oscillation Expt.

The CERN-Gran Sasso Neutrino Program

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

PERFORMANCE OF THE ATLAS LIQUID ARGON FORWARD CALORIMETER IN BEAM TESTS

RECENT RESULTS FROM THE OPERA EXPERIMENT

RICH detectors for LHCb

Optimization of the Gas Flow in a GEM Tracker with COMSOL and TENDIGEM Development. Presented at the 2011 COMSOL Conference

Simulation and validation of the ATLAS Tile Calorimeter response

READINESS OF THE CMS DETECTOR FOR FIRST DATA

ATLAS New Small Wheel Phase I Upgrade: Detector and Electronics Performance Analysis

Equalisation of the PMT response to charge particles for the Lucid detector of the ATLAS experiment

Particle Identification Algorithms for the Medium Energy ( GeV) MINERνA Test Beam Experiment

Cross Section of Exclusive π Electro-production from Neutron. Jixie Zhang (CLAS Collaboration) Old Dominion University Sep. 2009

PoS(KAON13)012. R K Measurement with NA62 at CERN SPS. Giuseppe Ruggiero. CERN

ALICE Commissioning: Getting ready for Physics

HARP (Hadron Production) Experiment at CERN

Marcos Dracos IPHC-IN2P3/CNRS Strasbourg. 2 December 2008 M. Dracos, BENE 1

Bolometry. H. Kroegler Assciazione Euratom-ENEA sulla Fusione, Frascati (Italy)

Cavern background measurement with the ATLAS RPC system

Dario Barberis Evaluation of GEANT4 Electromagnetic and Hadronic Physics in ATLAS

Temperature Dependence Calibration and Correction of the DAMPE BGO Electromagnetic Calorimeter

Hadronic vs e + e - colliders

ALICE A Large Ion Collider Experiment

Experimental results on the atmospheric muon charge ratio

HARP a hadron production experiment. Emilio Radicioni, INFN for the HARP collaboration

PoS(HCP2009)042. Status of the ALICE Experiment. Werner Riegler. For the ALICE Collaboration. CERN

Studies of Hadron Calorimeter

High-energy neutrino detection with the ANTARES underwater erenkov telescope. Manuela Vecchi Supervisor: Prof. Antonio Capone

The HARP Experiment. G. Vidal-Sitjes (INFN-Ferrara) on behalf of the HARP Collaboration

Performance of New and Upgraded Detectors for Luminosity and Beam Condition Measurement at CMS

A. Chukanov On behalf of OPERA collaboration JINR, Dubna TAUP 2011, Munich, 5-9 september, 2011

Tracking at the LHC. Pippa Wells, CERN

Alignment of the ATLAS Inner Detector

Detecting ν τ s: the CHORUS and OPERA experience. Pasquale Migliozzi

Alignment of the ATLAS Inner Detector tracking system

CNGS beam monitor with the LVD detector

pp physics, RWTH, WS 2003/04, T.Hebbeker

What detectors measure

Particle Identification of the LHCb detector

Luminosity measurement in ATLAS with Diamond Beam Monitor

Particle Accelerators

Neutrino Oscillations Physics at DUNE

1. The ICARUS T600 detector

Results and Status from HARP and MIPP

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland

Transcription:

Sensitivity of CNGS muon detectors to beam-line misalignments q OUTLINE: Requirements for CNGS muon detectors Beam Loss Monitors as muon detectors Effects of beam-line alignment errors Sensitivity reach to mis-alignments 17 March 22 Francesco Pietropaolo, INFN/Padova 1

CNGS beam-line monitoring q CNGS main features: High energy beam (1-3 GeV) optimized for n t appearance No near detector envisaged n m beam normalization performed at LNGS: by experiments (OPERA/ICARUS) with large area muon detectors (n m interactions in up-stream rock) q Requirements for monitors along beam-line Detect mis-alignments of beam-line elements producing significant effects at LNGS: Proton beam wrt Target Horn / Reflector wrt beam axis Monitor beam intensity/stability (relative calibration only) 17 March 22 Francesco Pietropaolo, INFN/Padova 2

1 m 1m CNGS: location of beam monitors 7 m 67 m muons profile --> nm profile Francesco Pietropaolo, INFN/Padova 3 SEM foils Hadron profile monitors Proton wrt target Low energy m In principle alignments High energy m optics wrt p-beam alignment 17 March 22

Choice of detectors and layout for the muon monitoring stations q Detector: Choice based on results of studies on alignment errors negligible effects on n t rate with alignment errors within predicted accuracy (for all beam line elements) CERN-EP21-37; CERN-SL-21-16 EA Emphasis on reliability access to muon stations very restricted Muon pit 2 q Layout: Sample muon profile with sufficient accuracy to detect asymmetries # of detectors, spacing, Muon pit 1-3 -2-1 1 2 3 Radius (m) 17 March 22 Francesco Pietropaolo, INFN/Padova 4

BLM s as detectors for the muon monitoring stations m beam PRO: robust stable in time large signals (allow distant electronics ª 1 km) good S/N ready to use (with front-end electronics & DAQ) in modules of 36 (18x2 cables) V bias ª 1 kv CONTRA: poor linearity at highest muon flux (under investigation) gas filling (1 bar) N2 17 March 22 Francesco Pietropaolo, INFN/Padova 5

17 March 22 Francesco Pietropaolo, INFN/Padova 6 Fluka standalone Fast parametric simulation After 15 m Fe hadron dump ( 2 GeV range-out filter) After 67 m of molasse ( 5 GeV range-out filter) ª 2 m! r (m) r (m) -.5 -.25.25.5-2 -1 1 2-2 -1 1 2 p ±, p ±, K ±, m ± (1 13 pot cm 2 ) -1.4.5 1..8 1. 2. 1.5 1.2 2. 3. 1.6 un-collided proton peak m + (1 13 pot cm 2 ) -1 x 1 1 x 1 2.5 m + (1 13 pot cm 2 ) -1 Hadron monitor 7 x 1 5 4. first muon pit second muon pit BLM s characteristics: matching muon beam intensity and pit layout

17 March 22 Francesco Pietropaolo, INFN/Padova 7 Clear loss around Horn focused momenta Loss -2.8 ±.2 % First muon pit very sensitive to Horn focused particles Average displ. = 19.1 ±.5 cm Second muon pit sensitive to much higher energies Average displ. = -3.5 ± 1.2 cm E (GeV) r (m) r (m) 2 4 6-2 -1 1 2-2 -1 1 2.2.5 n t CC evts (GeV kt year) -1.4 1..4.8 1.5.6 1.2 2. 2.5.8 sin 2 2q = 1 1.6 3. Dm 2 = 2.5 1-3 ev 2 x 1-3 1. m + (1 13 pot cm 2 ) -1 n t evts at LNGS x 1 7 2. first muon pit x 1 5 second muon pit 3.5 m + (1 13 pot cm 2 ) -1 Mis-aligned case Aligned case Example 1: 6 mm horn lateral displacement (expected accuracy ª.1 mm!!) Effects of alignment errors

17 March 22 Francesco Pietropaolo, INFN/Padova 8 2 4 6-2 -1 1 2-2 -1 1 2 n t CC evts (GeV kt year) -1.2.5.4 1..4.6.8 x 1-3 1. m + (1 13 pot cm 2 ) -1.8 1.2 1.6 n t evts at LNGS x 1 7 2. first muon pit second muon pit m + (1 13 pot cm 2 ) -1 1.5 2. 2.5 3. 3.5 x 1 5 Example 2: 1 mm p-beam lateral displacement (expected accuracy ª.1 mm!!) Effects of alignment errors

Overall effects of CNGS beam-line misalignments n t CC interact. loss (%) 1 st muon chamber centroid displ. (cm) 2 nd muon chamber centroid displ. (cm) Proton beam lateral displacements (alignment accuracy ª.1mm).5 mm 1. mm. - 2.8 Proton beam angular displacements (alignment accuracy ª.1mr).5 mr 1. mr. -1.3 -.6-1.2-1.2-2.3 7.3 14.8 3.7 1.4 Small effects at LNGS Measurable along beam-line Horn lateral displacements (alignment accuracy ª.1mm) 3 mm 6 mm Reflector lateral displacements (alignment accuracy ª.1mm) 1 mm 3 mm -1. -2.8 -.4-3. 1.1 19.1 5.7 21.5 >>>> Statistical accuracy of the MC simulation <<<<.2.5 -.6-3.5-1.7-18.8 1.2 Muon monitors (complemented by SEM s at target) are sufficient to disentangle source of misalignment 17 March 22 Francesco Pietropaolo, INFN/Padova 9

Study of the layout of BLM s in the muon monitoring stations Working hypotheses: 18 BLM s per pit s meas 3% / full scale (mainly relative calibr.) max signal adjusted at full scale good linearity over full signal range Arrangements (17 BLM s): Centered on beam axis Left/Right symmetric Orthogonal Polar Estimator: Weighted sum of (L-R) differences Depends on s meas, DS, number of BLM s No need for absolute calibration! DS Goal: best arrangement best spacing (DS) minimal number of BLM s 17 March 22 Francesco Pietropaolo, INFN/Padova 1

Detecting asymmetries in muon profiles Estimators of projected displacements: depend on left/right differences along given direction Dx =  x i W i,j /  W i,j = DS  i cosq j [W i,j -W -i,j ] /  W i,j i,j i,j i>,j i,j y i q j x Dy =  y i W i,j /  W i,j = DS  i sinq j [W i,j -W -i,j ] /  W i,j i,j i,j i>,j (W ij = muon flux measurement in each detector) i,j DS Errors: s ª s DS 2 (i cosq x meas  j )2 /  W i,j i>,j i,j Estimator of sensitivity: Dr = Dx 2 +Dy 2 Dq = inv sin( Dy Dr ) s ª s DS 2 (i sinq y meas  j )2 /  W i,j i>,j i,j s q ª s r Dr = s x 2 + s y 2 Dr 17 March 22 Francesco Pietropaolo, INFN/Padova 11

Simulations q Extensive simulation of possible misalignments Proton beam wrt target - horn/reflector wrt beam-axis Focus on small displacements (sensitivity) Several displacement directions (x,y) q Wide variety of arrangements of 17 BLM s tested Orthogonal configuration 4 BML s per row Spacing for 1cm to 5cm Polar configuration 8 BLM s per circle Spacing from 2cm to 1cm Non-uniform spacing also tested Grouping BLM s where muon profiles vary rapidly x 1 7 2. q Double BLM s density (33 per muon station) also tested 1.6 1.2.8.4 muon pit 1-2 -1 1 2 x-slice (m) 17 March 22 Francesco Pietropaolo, INFN/Padova 12

17 March 22 Francesco Pietropaolo, INFN/Padova 13 4 8 12 2 7cm 2 4 6 Dr (cm) 8 Estimator Dr approaches muon profile average displacement when the full distribution is sampled Best sensitivity for minimum s r /Dr 1 Sensitivity to beam-line mis-alignments (I)

17 March 22 Francesco Pietropaolo, INFN/Padova 14 4 8 12 2.1.2 Relative error.5.4.3 7cm Best monitor spacing, DS, depends on muon profile width Polar/orthogonal configurations equivalent sensitivity Sensitivity to beam-line mis-alignments (II)

Sensitivity to beam-line mis-alignments (III) 1 st muon chamber (max spanned radius = 8 cm) Horn lateral displacements 3 mm 6 mm -1. -2.8 1.1 19.1 14% 8% 2 nd muon chamber (max spanned radius =12 cm) Proton beam lateral displacements.5 mm 1. mm s meas = 3% / full scale n t CC interact. Loss (%). -2.8 Centroid profile displ. (cm) 7.3 14.8 Relative error (%) 16 BLM s 32 BLM s 18% 1% 6% 3% 7% 4% wide variety of configurations (uniform/non-uniform spacing) give comparable sensitivity 16+1 BLM s allow detecting displ. with negligible effect at LNGS (assuming s meas = 3% / full scale) 32+1 BLM --> factor 2.5 better (more detailed description of muon profiles) 1 motorized BML for x-y scanning and cross-calibration 17 March 22 Francesco Pietropaolo, INFN/Padova 15

Summary Misalignments of the beam-line elements -within project values- will not affect n t event rate at Gran Sasso Muon monitoring arrays (based on BLM s) - located after the CNGS dump - should provide reliable information to control beam intensity and misalignments Optimization of BLM s design and layout is underway to match CNGS highest muon flux 17 March 22 Francesco Pietropaolo, INFN/Padova 16

BLM characteristics q Ionization camber Diameter 9.2cm Length 19cm Volume 1liter Filling N 2 (99.9%) Pressure 1bar Ionization energy 27eV Sensitivity 5 1-5 C/Gy Efficiency 4 1 3 pairs/part. Bias Voltage 8V (5-12V) Rise-time 3ns Dynamics > 1 6 q Electronics and DAQ Acquisition mode integration ADC full scale 1V Resolution 12bit Integrator capac. min 5pF max 5mF DAQ unit 36(+4) channels 1 CPU+Timinig Signal cables 18 channels Cable length max 15m Acqusition time 3ms (36ch.) q Performance (Cable <5m; C min = 1nF) Radiation resist. > 1 6 Gy q Calibration Single source (137Cs - 3mCi) --> few % cross-calibration & time stability Drift 1bit/s Noise 3bit Sens. 4 1 3 part./bit Full scale 1.6 17 part. 17 March 22 Francesco Pietropaolo, INFN/Padova 17