RICH 2007Dirk Wiedner / LHCb1 The Usage of N-Perflourcarbons as RICH Radiators.

Slides:



Advertisements
Similar presentations
Lecture 8b Gas Chromatography.
Advertisements

1.1 INFRARED RADIATION 1.2 SURFACES AND RADIATION 1.3 STATES OF MATTER 1.4 CONDUCTION 1.5 CONVECTION 1.6 EVAPORATION AND CONDENSATION 1.7 ENERGY TRANSFER.
1 Ann Van Lysebetten CO 2 cooling experience in the LHCb Vertex Locator Vertex 2007 Lake Placid 24/09/2007.
Properties of Matter 2.1 Matter has observable properties. 2.2
Qualifications: BSc (Hons) Chemistry, Jordan PhD (Env Chemistry), Aberdeen, United Kingdom MRSC, CChem, IEMA DR AHMED AYOUB Technical Manager Work Experience:
USE OF GEANT4 FOR LHCB RICH SIMULATION S. Easo, RAL, LHCB AND ITS RICH DETECTORS. TESTBEAM DATA FOR LHCB-RICH. OVERVIEW OF GEANT4 SIMULATION.
Cherenkov Detectors. Index of Refraction When light passes through matter its velocity decreases. –Index of refraction n. The index depends on the medium.
Phase Changes.
The Nature of Liquids 13.2.
PERFORMANCE OF THE DELPHI REFRACTOMETER IN MONITORING THE RICH RADIATORS A. Filippas 1, E. Fokitis 1, S. Maltezos 1, K. Patrinos 1, and M. Davenport 2.
Cherenkov Radiation (and other shocking waves). Perhaps also the ones of the fish?
Advanced Thermodynamics Note 8 Refrigeration and Liquefaction
Atomic Matter.
CsI Photocathode Production and Testing
What is spectroscopy? It is the study of how matter interacts with electromagnetic radiation (gamma rays down to radio waves) Matter can interact with.
The HERMES Dual-Radiator Ring Imaging Cerenkov Detector N.Akopov et al., Nucl. Instrum. Meth. A479 (2002) 511 Shibata Lab 11R50047 Jennifer Newsham YSEP.
Unit 2 Test Review.
A RICH Detector for strangeness physics A RICH Detector for strangeness physics in Hall A at Jefferson Lab in Hall A at Jefferson Lab. Why. How. Main Characteristics/Expected.
Modelling of Electron Air Showers and Cherenkov Light A.Mishev J. Stamenov Institute for Nuclear Research and Nuclear Energy Bulgarian Academy of Sciences.
Position Sensitive SiPMs for Ring Imaging Cherenkov Counters C.Woody BNL January 17, 2012.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
6 June 2002Andrea Bressan University-INFN Trieste1 COMPASS RICH-1 on behalf of the COMPASS RICH Group.
Read Sections 6.1 and 6.2 before viewing the slide show.
EIC Detector – JLab – 04/June/2010 Cisbani / HERMES RICH 1 HERMES: Forward RICH Detector Evaristo Cisbani / INFN-Rome Sanità Group Most of the slides from.
Heat and States of Matter
Changing State Mixing Materials Water Cycle Heating and Cooling Separating Solids Burning Materials Evaporation.
A RICH with Aerogel for a hadron machine On behalf of the LHCb RICH group Some results and considerations on: Cerenkov angle resolution from aerogel Index.
Matter Key Questions: What’s the difference between an element, compound, and mixture? What’s the difference between an element, compound, and mixture?
Boiling, Freezing, and Melting 5.5B. Boiling—Descriptive When water boils (100ºC), it is changing from a liquid to a gas. Every liquid has its own boiling.
Phases of Matter What distinguishes the forms of matter?
J. Direito - M. Battistin – 28 th May 2010EN/CV/DC J. Direito, M. Battistin (EN/CV/DC) 28 th May 2010 Detector Cooling Project III Thermosiphon Workshop.
CLAUDIO BORTOLIN SPD Cooling Status INFN – PD / CERN.
HBD CDR Gas System and Monitoring Craig Woody BNL DC Upgrades/EC Meeting March 9, 2005.
STATES OF MATTER.
HW Review 1.35 A tank of gas with a total pressure of 12.0 atm contains a mixture of oxygen, nitrogen and argon. If the partial pressure of nitrogen.
States of Matter and Intermolecular Forces Chapter States and State Changes.
 The Four States of Matter  Solid  Liquid  Gas  Plasma.
International RICH-Workshop of the CBM Experiment at FAIR Gesellschaft für Schwerionenforschung Darmstadt, GERMANY March Radiator Gases { s.
Mauro Iodice INFN Roma (Italy) Hall A Collaboration Meeting - JLAB May 18, 2004.
Heat Transfer Equations For “thin walled” tubes, A i = A o.
Chapter 5: States of Matter Solids, Liquids, and Gases.
Matter & Energy. States of Matter  Solid- Definite volume and shape Particles are tightly packed Slight expansion when heated Incompressible.
Scan ~100 bar entry positions with laser diode measures transmitted intensity (relative to reference intensity) determine attenuation length (Λ) by aiming.
Status of the ATLAS ID Evaporative cooling system JCOV 25 Nov P. Bonneau TS/CV/Detector Cooling CONTENTS Overall statusOverall status Cooling plant.
Chapter #12 States of Matter Inter-particle Forces.
Liquids Chemistry Mrs. Coyle. Liquids Intermolecular attractions hold molecules of liquids together. Intermolecular attractions hold molecules of liquids.
Gas for World wide RPCs Ian Crotty12 Feb Contents The problem Sourcing the gases Storing Mixing Exhaust Safety Gas Bottle Is simple Chamber.
Quality-evaluation of Cesium Iodide photocathodes for the ALICE/High Momentum Particle Identification detector by means of a VUV-Scanner system Herbert.
P HOTON Y IELD DUE TO S CINTILLATION IN CF4 Bob Azmoun, Craig Woody ( BNL ) Nikolai Smirnov ( Yale University )
Second run with the Copper filter WA104 technical meeting – 23/03/2016.
Chapter 13 and 14. Essential Question: What are three units for pressure and how do you convert units? Warm-Up: What are the three states of matter? List.
TRD Gas System Layouts Production Readiness Review 03 – Nov F. Hahn.
PSA PLANT OXYGEN GENERATION SYSTEMS. 1. PSA Description 2. Molecular Sieves 3. Process ( Adsorption and Desorption) 4. Application for PSA process 5.
ANLEC R&D COMMUNICATION PACK ( ). While mercury can be removed from Oxy-Fuel flue gas, further work is required to understand its form and removal.
Creating a reliable source of pure low-radioactivity argon Henning O. Back – Princeton University Fermilab Detector R&D Review.
Low radioactivity argon from underground sources Henning O. Back – Princeton University LIDINE 2013.
STATES OF MATTER The Three States of Matter The Three States of Matter Solid Solid Liquid Liquid Gas Gas.
UV/VIS SPECTROSCOPY.
Refrigeration & air conditioning
Particle Identification (PID) at HIEPA Experiment
Natural Gas Processing I Chapter 2 In-feed System
Rosario Turrisi INFN Padova
Introduction to Food Engineering
Gas for World wide RPCs Ian Crotty 12 Feb 2015.
Follow-up of the tests with the copper filter
Production of Cesium Iodide Photocathodes for
Recirculating CO2 System
Particle Identification in LHCb
Revision States of Matter.
Mass Balance- in Non-Reactive System Multi unit system
Presentation transcript:

RICH 2007Dirk Wiedner / LHCb1 The Usage of N-Perflourcarbons as RICH Radiators

RICH 2007Dirk Wiedner / LHCb2 The specifications Little chromatic dispersion Refractive index sufficient O(1.001) Good UV transmittance (CsI) Long radiation length Non flammable Easy to use  N-perflourcarbons fulfill these specs

RICH 2007Dirk Wiedner / LHCb3 Refractive index FROM: Gas Cherenkov detectors for high momentum charged particle identification in ALICE G. Volpe et. altera n = 7eV Gas(n-1)x10 CF nm C4F nm C5F nm C6F14 Fluid! nm Refractive index can be tuned by choosing the appropriate Perflourcarbon Very moderate chromatic dispersion, at 177 nm dn/dE [eV −1 ] = 53 × 10−6* *Dissertation von Peter Fauland Universit¨at Bielefeld

RICH 2007Dirk Wiedner / LHCb4 Transparency Good transparency for clean C n F m Extinction in far UV ok for light gas as C3F8 –Photon detector should be sensitive above 180nm molar extinction coefficient,  (1/cm/mol) Chemical Physics Letters, volume 3, number 8, 1969,

RICH 2007Dirk Wiedner / LHCb5 Watch contaminations Benzene kills transparancy Water and Oxygen should be kept low 150nm 200 nm Water

RICH 2007Dirk Wiedner / LHCb6 Membrane cleaning Membranes allow selection of kinetic diameter CF 4 and C 4 F 10 can be well separated from Oxygen, Argon and Nitrogen UBE Industries, Specialty Chemicals and Products Division, High Purity Chemicals Business Unit, Ube Europe GmbH, Duseldorf, Germany.

RICH 2007Dirk Wiedner / LHCb7 C 4 F 10 recovery C 4 F 10 is a good Čerenkov radiator Widely used: Compass, Delphi, Hera-B, Hermes, LHCb Expensive gas: must be recovered before opening detector Example: LHCb Rich1

RICH 2007Dirk Wiedner / LHCb8 LHCb RICH1 C 4 F 10 recovery Twofold membrane filters –Eliminates light gases –Exit can be used for recovery or direct recycling Fridge –Separates C 4 F 10 from Argon, Nitrogen etc. –Outputs liquid C 4 F 10 to container

RICH 2007Dirk Wiedner / LHCb9 The test setup

RICH 2007Dirk Wiedner / LHCb10 The test setup

RICH 2007Dirk Wiedner / LHCb11 The test setup

RICH 2007Dirk Wiedner / LHCb12 The test setup N 2Out

RICH 2007Dirk Wiedner / LHCb13 The test setup

RICH 2007Dirk Wiedner / LHCb14 The test setup

RICH 2007Dirk Wiedner / LHCb15 Vapor pressure of C n F m

RICH 2007Dirk Wiedner / LHCb16 Tests 20 recovery test with C4F10 13 runs with evaporation in source bottle 7 runs with external evaporation

RICH 2007Dirk Wiedner / LHCb17 Obstacles Mixture of different C n F m, O(5%) non C 4 F 10 Ice built up in compressor electronic box Up to 6.6 kg can stay in recovery rack Corrosion of 63 l bottles in lab –Liquid extraction line in bottle not gas tight C 4 F 10 condensates at 1.2 bar overpressure –Compression must go along with heating Liquid loss at >200l/h waste gas flow

RICH 2007Dirk Wiedner / LHCb18 Summary of recovery tests System works stable Efficiency in first 5 tests 81.5% av. Efficiency in next 15 tests 90.4% av. External evaporator works reliably 24 h for 4 m 3 of LHCb max. flow Next steps –Installation of recovery system –commissioning

RICH 2007Dirk Wiedner / LHCb19 Backup Slides