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RF Cavities and Dark Currents MICE Christopher Hunt February 20, - PowerPoint PPT Presentation

Introduction RF Cavities Field Emissions The Problem The Solution RF Cavities and Dark Currents MICE Christopher Hunt February 20, 2013 1 , Introduction RF Cavities Field Emissions The Problem The Solution Particle Acceleration RF


  1. Introduction RF Cavities Field Emissions The Problem The Solution RF Cavities and Dark Currents MICE Christopher Hunt February 20, 2013 1 ,

  2. Introduction RF Cavities Field Emissions The Problem The Solution Particle Acceleration RF Cavities are the work horse of High Energy Physics We’ve come a long way from using a simple potential difference! But it’s not just accelerators. . . 2 ,

  3. Introduction RF Cavities Field Emissions The Problem The Solution Muon Ionisation Cooling Experiment 3D Rendered CAD drawing of MICE Step VI Ionisation cooling concepts 3 ,

  4. Introduction RF Cavities Field Emissions The Problem The Solution Linear Acceleration It started with Ising, built by and was improved by Alvarez Wider¨ oe 4 ,

  5. Introduction RF Cavities Field Emissions The Problem The Solution Single Cavity Structures Solve Maxwell’s Equations to find the field structure Exists in modes dependent on geometry Example field structure for a TM 010 mode cavity 5 ,

  6. Introduction RF Cavities Field Emissions The Problem The Solution Multiple Cavity Structures The next step with a similar design is multicavity structure, either travelling wave or standing wave Characterized by the field phase shift per cavity A superconducting cavity CAD-Drawing 6 ,

  7. Introduction RF Cavities Field Emissions The Problem The Solution Field Emission Phenomena Very strong electric fields perpendicular to cavity surfaces: • Changes the work function potential barrier • Permits higher rates of quantum tunnelling • Amplified by local imperfections • Builds to form dark currents 7 ,

  8. Introduction RF Cavities Field Emissions The Problem The Solution Fowler-Nordheim Expected current density as a function of electric field Assumes a saw-toothed potential barrier j ( E ) = A β 2 E 2 e − B φ 3 / 2 (1) β E φ 8 ,

  9. Introduction RF Cavities Field Emissions The Problem The Solution Effects of Dark Currents Dark currents produce X-Rays when Harmful to sensitive equipment, the impact the opposite wall of the detectors and electronics cavity Additional charge particles within Can damage the cavity, wastes a lot cavity increase liklihood of RF of energy and inhibits the cavity’s breakdown accelerating gradient Slowly leak energy from the Wastes energy, requires more stress electromagnetic field on the RF system, increases difficulty in construction A MICE Tracker Module without outer casing 9 ,

  10. Introduction RF Cavities Field Emissions The Problem The Solution Simulating Dark Currents → → Produce Inject Into Record Run through Particles using Cavity Electron G4 Based Fowler- Spectra Front End Nordeim X-Ray Detector → - Monitoring the dose received by the → MICE tracker. → → - Can compare with simulation. → → - Predict X-Ray damage and Dark Current induced noise. 10 ,

  11. Introduction RF Cavities Field Emissions The Problem The Solution The Future First Finish the simulation and obtain quantitative predictions Second Start work on designing the tracker shielding detectors Then Consider the next part of my research: The RF phase control 11 ,

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