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

rf cavities and dark currents mice
SMART_READER_LITE
LIVE PREVIEW

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


slide-1
SLIDE 1

Introduction RF Cavities Field Emissions The Problem The Solution

RF Cavities and Dark Currents MICE

Christopher Hunt

February 20, 2013

1 ,

slide-2
SLIDE 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 ,

slide-3
SLIDE 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 ,

slide-4
SLIDE 4

Introduction RF Cavities Field Emissions The Problem The Solution

Linear Acceleration

It started with Ising, built by Wider¨

  • e

and was improved by Alvarez

4 ,

slide-5
SLIDE 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 TM010 mode cavity

5 ,

slide-6
SLIDE 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 ,

slide-7
SLIDE 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 ,

slide-8
SLIDE 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) = Aβ2E 2 φ e−B φ3/2

βE

(1)

8 ,

slide-9
SLIDE 9

Introduction RF Cavities Field Emissions The Problem The Solution

Effects of Dark Currents

Dark currents produce X-Rays when the impact the opposite wall of the cavity Harmful to sensitive equipment, detectors and electronics Additional charge particles within cavity increase liklihood of RF breakdown Can damage the cavity, wastes a lot

  • f energy and inhibits the cavity’s

accelerating gradient Slowly leak energy from the electromagnetic field Wastes energy, requires more stress

  • n the RF system, increases

difficulty in construction

A MICE Tracker Module without outer casing

9 ,

slide-10
SLIDE 10

Introduction RF Cavities Field Emissions The Problem The Solution

Simulating Dark Currents

→ → Produce Particles using Fowler- Nordeim Inject Into Cavity Record Electron Spectra Run through G4 Based Front End → → → → → →

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 ,

slide-11
SLIDE 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 ,