Simulations of various aspects of the PPS Various members of the collaboration, to be enumerated later.

Slides:



Advertisements
Similar presentations
General Characteristics of Gas Detectors
Advertisements

Radiation Detection ionization chambers (dosimeters, pulse chambers, particle track chambers) scintillation detectors semiconductor detectors photographic.
Geiger Counters. Higher Voltage As the voltage increases in a gas detector the ions collected increases. The proportional region ends. –Streamer mode.
Status of test beam data analysis … with emphasis on resistive coating studies Progress and questions 1Meeting at CEA Saclay, 25 Jan 2010Jörg Wotschack,
Drift velocity Adding polyatomic molecules (e.g. CH4 or CO2) to noble gases reduces electron instantaneous velocity; this cools electrons to a region where.
Micro MEsh GASeous Detectors (MicroMegas)
The performance of Strip-Fiber EM Calorimeter response uniformity, spatial resolution The 7th ACFA Workshop on Physics and Detector at Future Linear Collider.
Micromegas studies using cosmic rays Franck Sabatié May 7th 2009 Saclay cosmic ray bench Data acquisition system and analysis tools MIP detection Position.
Tracking detectors/1 F.Riggi.
Capacitors1 THE NATURE OF CAPACITANCE All passive components have three electrical properties Resistance, capacitance and inductance Capacitance is a measure.
1 Capacitance and Dielectrics Chapter 27 Physics chapter 27.
1 VCI, Werner Riegler RPCs and Wire Chambers for the LHCb Muon System  Overview  Principles  Performance Comparison: Timing, Efficiency,
PSSC Space Instrument Laboratory Plasma instrument calibration system provides an ion beam of energy range up to 130keV/charge in a clean room To develop.
Fusion Physics - Energy Boon or Nuclear Gloom? David Schilter and Shivani Sharma.
Proportional Counters
Lesson 17 Detectors. Introduction When radiation interacts with matter, result is the production of energetic electrons. (Neutrons lead to secondary processes.
Ionization. Measuring Ions A beam of charged particles will ionize gas. –Particle energy E –Chamber area A An applied field will cause ions and electrons.
1 Apr. 28, 2007 Test of the Pulse Height and Time Jitter for the IHEP Full-Size RPC’s with 8-m-Long Readout Strip Planes C. Lu, K. McDonald and W. Sands.
Detectors. Measuring Ions  A beam of charged particles will ionize gas. Particle energy E Chamber area A  An applied field will cause ions and electrons.
TOF at 10ps with SiGe BJT Amplifiers
UM PPS Lab Activities - HV Readout Long Run - Single Source Saturation Test PPS meeting April 30, 2012.
Definition & Determination of Capacitance
Chapter 6 Photodetectors.
Electrical Energy & Current. Introduction to Electric PE, Electric Potential, and Potential Difference Intro to Electric Potential.
Why silicon detectors? Main characteristics of silicon detectors: Small band gap (E g = 1.12 V)  good resolution in the deposited energy  3.6 eV of deposited.
TRIGGERING EXCIMER LASERS BY PHOTOIONIZATION FROM A CORONA DISCHARGE* Zhongmin Xiong and Mark J. Kushner University of Michigan Ann Arbor, MI USA.
Large-amplitude oscillations in a Townsend discharge in low- current limit Vladimir Khudik, Alex Shvydky (Plasma Dynamics Corp., MI) Abstract We have developed.
Chapter 13.
FISICA AMBIENTALE 1 Radioattività: misure 1 Lezioni Marie Curie.
Chapter 17 Electric Potential. Objectives: The students will be able to: Given the dimensions, distance between the plates, and the dielectric constant.
Monday, Mar. 7, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #12 Monday, Mar. 7, 2005 Dr. Jae Yu Particle Detection Ionization detectors MWPC.
CJ Barton Department of Physics INTAG Meeting – GSI – May 2007 Large Acceptance Bragg Detector at ISOLDE.
Paul Sellin, Radiation Imaging Group Time-Resolved Ion Beam Induced Charge Imaging at the Surrey Microbeam P.J. Sellin 1, A. Simon 2, A. Lohstroh 1, D.
Photos placed in horizontal position with even amount of white space between photos and header Sandia National Laboratories is a multi-program laboratory.
Measurements of several parameters of plasma panels October 2011.
Status of Beam loss Monitoring on CTF3 Results of Tests on LINAC and PETS as R&D for TBL Anne Dabrowski Northwestern University Thibaut Lefevre CERN CTF3.
1. DESY tests 2. Electronics developments 3. Optical developments 4. Outlook Casablanca J. Cvach, CALICE Coll. meeting.
Yosuke Watanabe….. University of Tokyo, RIKEN A, KEK C, Development of a GEM tracker for E16 J-PARC 1 Thanks to ???????????
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.
TPC R&D status in Japan T. Isobe, H. Hamagaki, K. Ozawa, and M. Inuzuka Center for Nuclear Study, University of Tokyo Contents 1.Development of a prototype.
1 Plasma Panel Sensors for Particle & Beam Detection (N31-7) Peter S. Friedman Integrated Sensors, LLC / Ottawa Hills, Ohio, USA /
IEEE 2011 NSS-MIC Valencia Yiftah Silver October 26 th 2011.
EPS-HEP 2015, Vienna. 1 Test of MPGD modules with a large prototype Time Projection Chamber Deb Sankar Bhattacharya On behalf of.
Yiftah Silver Tel Aviv University September 27 th 2012.
High voltage V = 300 Pixel capacitance C = 3 fF Embedded resistance R = 50K  Recovery time = 1 ns Pixel density = 10 4 cm -2 4 X estimated SLHC rate =
Experimental and Numerical studies on Bulk Micromegas SINP group in RD51 Applied Nuclear Physics Division Saha Institute of Nuclear Physics Kolkata, West.
M. Bianco On behalf of the ATLAS Collaboration
Using delay lines on a test station for the Muon Chambers Design considerations (A. F. Barbosa, Jul/2003)
GEM basic test and R&D plan Takuya Yamamoto ( Saga Univ. )
Wednesday, Oct. 18, 2006PHYS 3446, Fall 2006 Jae Yu 1 PHYS 3446 – Lecture #12 Wednesday, Oct. 18, 2006 Dr. Jae Yu 1.Particle Detection Ionization Detectors.
Techniques for Nuclear and Particle Physics Experiments By W.R. Leo Chapter Eight:
Development of a Plasma Panel, High Resolution Particle & Radiation Detector for Super LHC & Next Generation Colliders R. Ball 1, M. Ben-Moshe 2, J.W.
Hyper-Pure Germanium in Planar Configuration instrumentation examples1 A HP Ge is a cooled solid state detector LN2 Dewar HP Ge Charges Sensing Preamplifier.
Summer Student Session, 11/08/2015 Sofia Ferreira Teixeira Summer Student at ATLAS-PH-ADE-MU COMSOL simulation of the Micromegas Detector.
Chapter V Radiation Detectors.
MuTr Chamber properties K.Shoji Kyoto Univ.. Measurement of MuTr raw signal Use oscilloscope & LabView Read 1 strip HV 1850V Gas mixture Ar:CO 2 :CF 4.
Development of a Single Ion Detector for Radiation Track Structure Studies F. Vasi, M. Casiraghi, R. Schulte, V. Bashkirov.
Gas Electron Multiplier
Circuit Electricity. Electric Circuits The continuous flow of electrons in a circuit is called current electricity. Circuits involve… –Energy source,
An extension of Ramo's theorem to include resistive elements
Plan for Today (AP Physics I)
Simulation of Properties of COMPASS Drift-Chamber Prototypes
Dr: Mohamed Afifi By Lecturer Radiological Science
Photodetectors.
Radiation Detectors : Detection actually means measurement of the radiation with its energy content and other related properties. The detection system.
Capacitors Devices used to store charge.
(On Behalf of CMS Muon Group)
French Atomic and Alternative Energy Commission (CEA), FRANCE
PHYS 3446 – Lecture #16 Monday ,April 2, 2012 Dr. Brandt
Presentation transcript:

Simulations of various aspects of the PPS Various members of the collaboration, to be enumerated later

We Need to Know? Properties of the discharge – Voltage required – Current delivered – Development time – Decay time – Recovery time (deadtime) Properties of the device – Electric field distribution – Electric field uniformity in drift regions – Electric field intensity in discharge regions How to trigger the discharge – Minimum Number of electrons – Minimum Energy of the electrons How to produce the electrons – Energy loss from ions traversing the device – “Converters” Properties of the output pulses – Risetime – Decay time – Crosstalk

What to simulate Arriving particle spectrum Particle energy loss, multiple scattering Gas ionization Electric fields Output electrical signal Plasma discharge dynamics

Particle scattering Principal tool is GEANT4 – Widely used in nuclear physics – Gives event-by-event output for later analysis – Open source, easily available Example: 106 Ru (R. Varner)

106 Ru example

106 Ru Example

Electric Fields Y. Silver COMSOL has been the most used tool Examples:

Cell capacitance estimates

Electric Field Map Drift Region Dielectric 10  m  =10 Discharge (15 x 75  m) (1mm deep) 80 fF capacitance Sense (10 x 25  m) Applied HV (20 x 25  m) Resistive ( siemens/meter)

Modeling and simulation Initial geometry: two orthogonal copper strips separated by a 400 µm gas gap. One strip at ground, one at 1V. Initial strip dimensions: 1 cm X 1 mm X 25 µm. Initial two-strip capacitance: pF Incrementally changed dimensions Right: Electric potential plot of initial strip geometry

Capacitance v gas gap Right: Plot of capacitance vs. gas gap, keeping strip geometry constant Changed gas gap from 400 microns to 2000 microns, in 100 micron increments Data fitted with 4 th degree polynomial

Capacitance vs Electrode Width Right: capacitance plotted vs width of terminal electrode Width changed from 1 mm to 10 mm, in 1 mm increments

HV sensitivity of cells

Output electrical Signal Develop equivalent circuit Evaluate the circuit using SPICE to simulate the output pulse properties – Amplitude – Width – Ringing

Cell Schematic

Full Schematic

Plasma discharge Many approaches considered – None found to be practical or sufficient Possibilities – Fully dynamical (Y. Silver) Boltzmann equation Maxwell equation Atomic physics cross-sections Somewhat developed for Plasma Display Panels Expensive to run – Drift chamber models (C. Ferretti) CERN GARFIELD Electron production Gas amplification – Geiger counter models Semi-empirical – Require calibration “Rules of thumb”