Phenolic glass based materials for the RPC electrodes RPC2016 Het Pand GENT R. Santonico INFN and University of Tor Vergata, Rome, Italy On behalf of the.

Slides:



Advertisements
Similar presentations
Dispersive property of a G-M tube HV - + In the proportional region a G-M tube has dispersive properties tube voltage.
Advertisements

Development of high rate RPCs Lei Xia Argonne National Laboratory.
1 MRPC detector as polarimeter for dEDM Characteristic of detector Time Resolution Electronics Possible R&D Plans D. Babusci, A. Ferrari, P. Levi Sandri,
1 Sep. 19, 2006Changguo Lu, Princeton University Induced signal in RPC, Configuration of the double gap RPC and Grouping of the strips Changguo Lu Princeton.
Progress report NeuLAND Outline Short reminder about NeuLAND Timing RPC concept Open questions - Impedance matching RPC prototype at GSI Next steps Collaboration.
CMS - PAVIA1 Engineering Design Review RPC - BAKELITE.
Development and study of Glass Resistive Plate Chambers Satyanarayana Bheesette Roll number: Supervisors Prof Raghava Varma, IIT Bombay Prof Naba.
Sandwich Construction Thin composite skins bonded to thicker, lightweight core. Large increase in second moment of area without weight penalty. Core needs.
Status of INO detector R&D B.Satyanarayana TIFR, Mumbai.
C.Shalem et al, IEEE 2004, Rome, October 18 R. Chechik et al. ________________RICH2004_____________ Playa del Carmen, Mexico 1 Thick GEM-like multipliers:
Atsuhiko Ochi Kobe University 25/06/2013 New Small Wheel MicroMegas Mechanics and layout Workshop.
The Resistive Plate Chamber detectors at the Large Hadron Collider experiments Roberto Guida Paolo Vitulo PH-DT-DI Univ. Pavia CERN EDIT school 2011.
ALICE-LHCC Review May 14, 2001 Thomas C. Meyer/EP-AIT1 TPC Field Cage Progress Report Project Schedule Technical Progress & Prototyping Contractual Matters.
Tariq J. Solaija, NCP Forward RPC EDR, Tariq Solaija Forward RPC EDR The Standard RPC for low  regions Tariq J. Solaija National Centre for.
Light Calibration System (LCS) Temperature & Voltage Dependence Option 2: Optical system Option 2: LED driver Calibration of the Hadronic Calorimeter Prototype.
RPC Development in Beijing and Potential for NO A Tianchi Zhao University of Washington May 16, 2005.
RPC detection rate capability ≈ 1/ρ Float-Glass ( Ω-cm) RPC rate capability < Bakelite( Ω-cm) one. New kind of doped glass was developed.
Test Beam the μ-RWELL Test Beam the μ-RWELL G. Bencivenni (a), R. de Oliveira (b), M. Gatta (a), G. Felici (a), G. Morello (a), M. Poli Lener (a) (a),
Design of a readout system for RPCs Olu Amoda2 The LODEN Group The group is an association of Fermilab scientists who teamed up to build a cosmic ray.
Towards a 1m 3 Glass RPC HCAL prototype with multi-threshold readout M. Vander Donckt for the CALICE - SDHCAL group.
Update on DHCAL and RPC progress Lei Xia ANL - HEP.
Development of Digital Hadron Calorimeter Using GEM Shahnoor Habib For HEP Group, UT Arlington Oct. 12, 2002 TSAPS Fall ’02, UT Brownsville Simulation.
Tests of RPCs (Resistive Plate Chambers) for the ARGO experiment at YBJ G. Aielli¹, P.Camarri¹, R. Cardarelli¹, M. Civardi², L. Di Stante¹, B. Liberti¹,
Slide 1Crispin Williams INFN BolognaALICE TOF The ALICE-TOF system 1. Quick overview of the TOF system that we are building 2. The Multigap Resistive Plate.
Test results of Multi-gap RPC Test Chambers for a Digital HCAL  Geometrical design  Test setup  Signal: avalanche mode and streamer mode  Comparison.
Marcello Abbrescia Muon general meeting, Mon 29-Apr p. 1 R&D on improved RPCs for phase 2 upgrade M. Abbrescia on behalf of the RPC upgrade group.
Marcello Abbrescia RPCs for CMS during Phase II RPC rate capability M. Abbrescia, The dynamic behaviour of Resistive Plate Chambers, NIM A 533 (2004) 7–10.
Academia meets Industry: RPC and TGC Vienna University of Technology March 25 th 2014 By R. Santonico.
Luigi Cosentino - n_TOF collaboration meeting - Bologna - 27  29 November New monitors for flux measurement and n-beam profile in EAR2 Luigi Cosentino,
Proposal of a digital-analog RPC front-end for synchronous density particle measure for DHCAL application R.Cardarelli and R.Santonico INFN and University.
1 Plannar Active Absorber Calorimeter Adam Para, Niki Saoulidou, Hans Wenzel, Shin-Shan Yu Fermialb Tianchi Zhao University of Washington ACFA Meeting.
For 2016 RPCWorkshop 1 Charge Distribution dependency on gap thickness of CMS endcap RPC Sung Park, KODEL, Korea Univ On behalf of the CMS RPC group 1.
Development of a Single Ion Detector for Radiation Track Structure Studies F. Vasi, M. Casiraghi, R. Schulte, V. Bashkirov.
An INTRODUCTION to RPC2016 Het Pand Gent 22 Feb 2016 By R. Santonico.
FEASIBILITY ANALYS OF AN MHD INDUCTIVE GENERATOR COUPLED WITH A THERMO - ACOUSTIC ENERGY CONVERSION SYSTEM S. Carcangiu 1, R. Forcinetti 1, A. Montisci.
NSS2006Shengli Huang1 The Time of Flight Detector Upgrade at PHENIX Shengli Huang PHENIX Collaboration Outlines: 1.Physics motivations 2.Multi-gap Resistive.
Updated Resistivity measurement on Mm-Batch-4 Bakelite & RPC Bakelite sample measurements Liang Guan TGRPC R&D Biweekly meeting
Displacement, Location or Position Sensor Muhajir Ab. Rahim School of Mechatronic Engineering, KUKUM.
Characteristic Impedance Measurement of Pickup Panel made up with a Suitable Dielectric Material, and Surface Resistivity (Automation) for large RPC electrodes.
R & D Status report on INO Naba K Mondal Tata Institute of Fundamental Research Tata Institute of Fundamental Research Mumbai, India.
First results from tests of gaseous detectors assembled from resistive meshes P. Martinengo 1, E. Nappi 2, R. Oliveira 1, V. Peskov 1, F. Pietropaola 3,
A high rate fast precision tracking trigger with RPCs
Large THGEM sampling elements for DHCAL status report
The ALICE-TOF system 1. Quick overview of the TOF system that we are building 2. The Multigap Resistive Plate Chamber -what is it? 3. Difference in.
An extension of Ramo's theorem to include resistive elements
Dipartimento di Fisica, Università del Salento
Results achieved so far to improve the RPC rate capability
An extensive aging study of bakelite RPC
Study on Surface Asperities
A proposal to equip the high eta muon stations with High Rate GRPC
SANDWICH CONSTRUCTION
An improved design of R-MSGC
THGEM: Introduction to discussion on UV-detector parameters for RICH
Multigap Resistive Plate Chambers (MRPC)
India-based Neutrino Observatory (INO)
Same geometry, but different size of the rim
News on second coordinate readout
Semi-Digital Hadronic CALorimeter
José Repond Argonne National Laboratory
TPC Field Cage Progress Report
Multigap Resistive Plate Chambers for EAS study in the EEE Project
Performance of a Multigap RPC prototype for the LHCb Muon System
A new type of RPC with very low resistive plates
MWPC’s, GEM’s or Micromegas for AD transfer and experimental lines
Muon Detector Jiawen ZHANG 16 September 2002.
Resistive Plate Chambers performance with Cosmic Rays
C. Lippmann, W. Riegler, A. Kalweit
Development of Resistive Plate Chamber for charge particle detection
A DLC μRWELL with 2-D Readout
Progress of DLC Resistive Electrode
Presentation transcript:

Phenolic glass based materials for the RPC electrodes RPC2016 Het Pand GENT R. Santonico INFN and University of Tor Vergata, Rome, Italy On behalf of the Rome2 RPC group

Abstract Pure phenolic glass and melamine coated phenolic glass. Optimal combination of electrical and mechanical properties Electrode thickness: the advantages of thin/very-thin electrodes Flexibility coupled to high mechanical performance

The phenolic glass The «phenolic glass» is a material made of glass fibers embedded inside the phenolic resin. This gives the advantage of coupling the low and well tunable electrical resistivity of the phenolic polymers with the high mechanical performance of the glass. Two types of materials suitable for the RPC electrodes have been studied so far: Pure phenolic glass plates Melamine coated phenolic glass plates, made with a phenolic glass core sandwiched between 20 micron thick melamine foils The mechanical performance of the phenolic glass offers the possibility of building RPCs with very thin electrodes that would be impossible, e.g. with the standard laminate where the phenolic resin impregnates a cellulose substrate The importance of thin electrodes has been already stressed and is one of the main points focused in this talk Thin phenolic glass electrodes show a good flexibility while keeping a high level of mechanical stability. This offers also the unprecedented possibility to fit cylindrical geometries

Thin electrodes vs the induced read out charge

Test of different phenolic materials The following tests were performed, at CR rates, on a few RPCs of sensitive area 10x50 cm 2. Melamine coated phenolic glass RPCs.8 mm thick electrodes of high resistivity and 1 mm gap Pure phenolic glass RPCs.5 mm electrodes of both high…and low…resistivity with 0.5 mm gap Pure phenolic glass bigap RPC 2x1 mm gas gaps 0.5 mm external electrodes 0.17 mm inner floating electrode

Melamine coated 0.8 mm phenolic glass electrodes vs standard 2 mm electrodes Efficiency vs voltage comparison

Melamine coated 0.8 mm phenolic glass electrodes vs standard 2 mm electrodes Prompt charge comparison Prompt charge (pC) HV(Volt)

Prompt signal amplitude comparison

Pure phenolic glass Efficiency vs HV 4 mm foam plates separates the gas volume from the readout stripe fraction of charge exceeding 5 pC

Prompt charge comparison vs HV 4 mm foam plates separates the gas volume from the readout stripe

0.5 gap – 0.5 electrode vs standard electrodes

Pure phenolic glass 1+1mm bigap 0.5mm external electrodes 0.17 mm floating inner electrode

Single vs bigap comparison

Comments on the multigap RPCs with floating inner electrodes An important achievement and the simplest RPC configuration to reach timing accuracies in the tens of picosecond range Based on the principle of the self-equipartition of the electric field among different gas gaps This principle makes the simplicity and the competitiveness of multigap RPCs This principle can work only when the current flowing in the gas prevails over any Ohmic term

Prompt charge vs voltage