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.

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.
Gas Lasers This is what is inside. But how do they work ?
Geiger Counters. Higher Voltage As the voltage increases in a gas detector the ions collected increases. The proportional region ends. –Streamer mode.
GM COUNTER.
HEP Experiments Detectors and their Technologies Sascha Marc Schmeling CERN.
Detecting Radiation Oui! It is Friday apres-midi! Time for a bottle du vin avec ma petit fille. Oi Vay! The lab is une grande mess. Je will sweep tout.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (1/2) 3.Collider Experiments.
Drift velocity Adding polyatomic molecules (e.g. CH4 or CO2) to noble gases reduces electron instantaneous velocity; this cools electrons to a region where.
Geiger- Muller counter
Radiation Detectors / Particle Detectors
Photomultipliers. Measuring Light Radiant Measurement Flux (W) Energy (J) Irradiance (W/m 2 ) Emittance (W/m 2 ) Intensity (W/sr) Radiance (W/sr m 2 )
Tracking detectors/1 F.Riggi.
Time-of-Flight at CDF Matthew Jones August 19, 2004.
Principles of Radiation Detection
Proportional Counters
Detecting Cosmic Rays An inexpensive portable detector By: Danny Franke Quarknet 2004.
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.
Scintillators.
Characterization of Detectors NEP= noise equivalent power = noise current (A/  Hz)/Radiant sensitivity (A/W) D = detectivity =  area/NEP IR cut-off maximum.
Main detector types Multi Pixel Photon Counter (MPPC) and Charge Coupled Devices (CCDs) How does it work? 1. Photon hits a pixel producing electron hole.
Transducers Converts one type of energy into another. Light  Electrical (current, voltage, etc.) What characteristics should we look for in a transducer?
High Energy Detection. High Energy Spectrum High energy EM radiation:  (nm)E (eV) Soft x-rays X-rays K Soft gamma rays M Hard gamma.
Techniques for detecting X-rays and gamma-rays Pair production Creation of elementary particle and its antiparticle from a photon. Occurs only if enough.
Main detector types Scintillation Detector Spectrum.
GRAND Britni Bethune CROP 2002 G amma R ay A strophysics at N otre D ame The University of Notre Dame is located north of South Bend, Indiana The University.
Instruments for Radiation Detection and Measurement
Photomultiplier Tube. What is it? Extremely sensitive detector of light in the ultraviolet, visible and near infrared Multiplies the signal produced by.
Lecture 11  Production of Positron Emitters, Continued  The Positron Tomograph.
Instruments for Radiation Detection and Measurement Lab # 3 (1)
Lens ALens B Avg. Angular Resolution Best Angular Resolution (deg) Worst Angular Resolution (deg) Image Surface Area (mm 2 )
Type of Material: Instrumentation Review
1 Light Collection  Once light is produced in a scintillator it must collected, transported, and coupled to some device that can convert it into an electrical.
IONIZATION DETECTORS “High Energy Physics Phenomenology”
Photon detection Visible or near-visible wavelengths
Tanja Horn, CUA PHYS 575/675 Modern Detectors Phys 575/675, Spring 2012 Tools of High Energy and Nuclear Physics Detection of Individual Elementary Particles.
Why are low energy neutrons more dangerous than high energy neutrons?  Generally radiation causes damage to cells because it ionizes atoms. This can break.
Chapter 30: Nuclear Physics and Radioactivity. Radioactivity Radioactivity is the discentigration of an unstable nuclei. when the nuclei decays the nucleus.
FISICA AMBIENTALE 1 Radioattività: misure 1 Lezioni Marie Curie.
Tools for Nuclear & Particle Physics Experimental Background.
1 The GEM Readout Alternative for XENON Uwe Oberlack Rice University PMT Readout conversion to UV light and proportional multiplication conversion to charge.
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.
SCINTILLATION COUNTER. PRINCIPLE When light radiations strike fluorescent material it produces flashes of light called scintillations. These are detected.
Instrumentation Review. Direct and Indirect Ionization Direct - Charge particles that strip away electrons from atoms Indirect - uncharged that have to.
Calorimeters  A calorimeter is a detector that measures “energy” of the particles that pass through. Ideally it stops all particles of interest.  Usually.
GEM: A new concept for electron amplification in gas detectors Contents 1.Introduction 2.Two-step amplification: MWPC combined with GEM 3.Measurement of.
Ionization Detectors Basic operation
Seeing the Subatomic Stephen Miller Saturday Morning Physics October 11, 2003.
Medical Image Analysis Interaction of Electromagnetic Radiation with Matter in Medical Imaging Figures come from the textbook: Medical Image Analysis,
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:
Lecture 3-Building a Detector (cont’d) George K. Parks Space Sciences Laboratory UC Berkeley, Berkeley, CA.
Detection of Radiation Contents: Geiger tubes Photo-Multiplier tubes Cloud Chambers Solid State devices.
Ideal Detector Fast Cheap Rugged Responds to all wavelengths of light Can distinguish different wavelengths Sensitive Low LOD.
Chapter V Radiation Detectors.
Lecture 12  Last Week Summary  Sources of Image Degradation  Quality Control  The Sinogram  Introduction to Image Processing.
Thorsten Lux. Charged particles X-ray (UV) Photons Cathode Anode Amplification Provides: xy position Energy (z position) e- CsI coating 2 Gas (Mixture)
Radiation detectors Ion chamber 2. Geiger Muller counter (GM).
PAN-2013: Radiation detectors
Ion Detectors and The Proportional Detector
Ionization detectors ∆
Scintillation Counter
When this happens... We see this... 12/6/2018 Steve Wotton.
The Hall C Heavy Gas Cerenkov
NUCLEAR RADIATION DETECTORS
Radioactivity B. Sc. -III Feb Dr. Wagh G. S. M. Sc. M. Phil. Ph
Photomultiplier (PMT) Tubes
PARTICLE DETECTORS I recently joined the IAEA.
PHYS 3446 – Lecture #16 Monday ,April 2, 2012 Dr. Brandt
PHYS 3446 – Lecture #17 Wednesday ,April 4, 2012 Dr. Brandt
Presentation transcript:

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 to separate and move to charged plates. Applied voltage V Measured current I I V   A E

Cylindrical Chamber  Cylindrical geometry is common for counters. Grounded outer cathode High voltage anode  The avalanche is limited to a region near the wire. I V  

 A single track in a chamber creates many avalanches. All contribute to one pulse  Timing is based on first avalanche arrival. Usually nearest point in the field Single Track

Multiwire Proportional Chamber  An array of proportional readout wires can be placed in an array. Invented in 1968 by Georges CharpakInvented in 1968 by Georges Charpak Used in many discoveriesUsed in many discoveries Received the 1992 Nobel PrizeReceived the 1992 Nobel Prize  Provides excellent position resolution for charged particle tracks.

Uranium Cell  Liquid noble gases can be used in ionization chambers. Liquid argon, krypton, xenon  Uranium plates are alternated with readout pads. Separated by liquid argon  Readout on printed circuit boards. Outer readout pads Inner layer readout wires Ground planes to reduce crosstalk 4.0 mm 2.3 mm 4.3 mm depleted uranium liquid Ar gaps readout pad incident particle

Scintillation Detector  Scintillation detectors rely on the emission of photons from excited states. CountersCounters CalorimetersCalorimeters 1. An incident photon or particle ionizes the medium. 2. Ionized electrons slow down causing excitation. 3. Excited states immediately emit light. 4. Emitted photons strike a light- sensitive surface. 5. Electrons from the surface are amplified. 6. A pulse of electric current is measured.

Photomultiplier Tube  A photomultiplier tube (phototube, PMT) combines a photocathode and series of dynodes.  The high voltage is divided between the dynodes.  Output current is measured at the anode. Sometimes at the last dynodeSometimes at the last dynode

Multipart Detector  Multiple detectors are used to identify different particles.  Tracking chambers to measure position.  Calorimeters to measure energy.  Muon from top decay