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AWAKE Electron Spectrometer Simon Jolly 7 th March 2013

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AWAKE Electron Spectrometer. Simon Jolly 7 th March 2013. Spectrometer Specifications. Wakefield accelerated electrons ejected collinear with proton beam: need to separate the 2 and measure energy of electron beam only. - PowerPoint PPT Presentation

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Page 1: AWAKE Electron Spectrometer

AWAKE Electron Spectrometer

Simon Jolly7th March 2013

Page 2: AWAKE Electron Spectrometer

Spectrometer Specifications

• Wakefield accelerated electrons ejected collinear with proton beam: need to separate the 2 and measure energy of electron beam only.

• Must be able to resolve energy spread as well as energy: spectrometer must accept a range of energies, probably 0-5 GeV.

• Current conceptual layout:– Dipole mounted ~2 m downstream of plasma exit

induces dispersion in electron beam.– Scintillator screen 1 m downstream of dipole

intercepts electron beam ONLY.– Dispersion gives energy-dependent position spread

on screen.– Scintillator imaged by intensified CCD camera

viewing upstream face of scintillator screen.

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 3: AWAKE Electron Spectrometer

Spectrometer Layout (Isometric View)

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Camera

Scintillator ScreenCERN 1 m dipole

Plasma cell

Protons

Electrons + Protons

• Edge of scintillator screen is aligned with dipole coils (position will depend on resolution).

• Screen mounted at 45 degrees to beam axis.• Camera is 4 m from centre of screen, mounted at

90 degrees to beam axis.• Camera shown in horizontal bending plane.• Camera can also be mounted vertically, directly

above screen, with screen tilted at 45 degrees to vertical as well as 45 degrees to beam axis. Dipole to screen distance remains unchanged (independent of screen-camera orientation).

Page 4: AWAKE Electron Spectrometer

Spectrometer Layout (Plan View)

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Electrons + Protons

Protons

Electrons

CERN 1 m MBPS dipole

Scintillator Screen

Camera

• For left-hand bend, beam enters at right-hand edge of dipole.

• Protons essentially unaffected; electrons bent in dipole field.

• Screen mounted at 45 degrees to beam axis.

• Camera is 4 m from centre of screen, mounted at 90 degrees to beam axis.

4 m

1.6 m

1 m

Page 5: AWAKE Electron Spectrometer

Spectrometer: Vacuum Vessel

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Electrons + Protons

Camera

• Screen mounted inside vacuum vessel, but camera outside.

• Light tight path from vacuum window to camera: doesn’t need to be permanent, just light tight…

Vacuum Window

Vacuum Vessel

Light Tight Path

Page 6: AWAKE Electron Spectrometer

Spectrometer: Shielding

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Electrons + Protons

• Most important item to shield is CCD Camera.

• Needs to be as far from beamline as possible (while still close enough to receive enough light).

• Maximise distance to beam axis.• More shielding required on

upstream side.

Vacuum Vessel

Shielding

Page 7: AWAKE Electron Spectrometer

CERN 1 m Dipole (Edda, Alexey)

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 8: AWAKE Electron Spectrometer

Spectrometer Simulations

• Initial simulations of Spectrometer layout carried out by Alexey:– Effects of upstream quadrupole doublet.– Quick check of fringe field effects.

• More detailed simulations by Dan Hall (UCL) including Spectrometer GUI for checking spectrometer layout parameters quickly.

• GPT simulations using beam parameters from K. Lotov (good and bad…) for design setup, with and without fringe fields.

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 9: AWAKE Electron Spectrometer

Spectrometer GUI: Assumptions

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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GUI and movies courtesy of Dan Hall (but don’t tell him…).

Page 10: AWAKE Electron Spectrometer

Good (“2 GeV”) Bad (“650 MeV”)

Electron Beam Distributions

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 11: AWAKE Electron Spectrometer

2 GeV, 1.86T: Trajectories

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 12: AWAKE Electron Spectrometer

2 GeV, 1.86T: Screen

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 13: AWAKE Electron Spectrometer

2 GeV, 1.86T: Screen (Zoom)

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 14: AWAKE Electron Spectrometer

2 GeV, 1.86T: Spectrometer Energies

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 15: AWAKE Electron Spectrometer

2 GeV, 1.86T: Energy Correlation

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 16: AWAKE Electron Spectrometer

2 GeV, 1.86T: Energy Correlation (2)

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 17: AWAKE Electron Spectrometer

2 GeV, 1.86T: Energy Resolution

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 18: AWAKE Electron Spectrometer

650 MeV, 1T: Screen

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 19: AWAKE Electron Spectrometer

650 MeV, 1.4T: Screen

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Page 20: AWAKE Electron Spectrometer

650 MeV, 1.86T: Screen

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 21: AWAKE Electron Spectrometer

650 MeV, 1T: Spectrometer Energies

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 22: AWAKE Electron Spectrometer

650 MeV, 1.4T: Spectrometer Energies

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 23: AWAKE Electron Spectrometer

650 MeV, 1.86T: Spectrometer Energies

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 24: AWAKE Electron Spectrometer

650 MeV, 1.86T: With Fringe Fields

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 25: AWAKE Electron Spectrometer

2 GeV, 1.86T: With Fringe Fields

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 26: AWAKE Electron Spectrometer

2 GeV, 1.86T: Spectrometer Energies

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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Page 27: AWAKE Electron Spectrometer

Conclusions

• Fundamental design hasn’t changed: it’s still simple!

• Already have camera (but not lens) and magnet (but not power supply).

• Some nice simulation results from Dan Hall using Konstantin Lotov’s beams:– Preliminary results show we can resolve the energy

distribution reasonably well.– With Konstantin’s parameters, energy spectrum not

washed out by emittance.– Fringe fields start to affect large angle beams at low

energy + high fields, but otherwise okay.– A note of caution:

• These are “idealised” fringe fields.• May have nonlinearities/nonuniformities in actual magnet field.• Definitely need magnetic field mapping + magnet “ramp” (hysteresis +

power supply).

• Onwards to finding a scintillator…07/03/13 Simon Jolly, UCL, AWAKE Collaboration

Meeting27

Page 28: AWAKE Electron Spectrometer

CDR/Technical Note Status

• Matt Wing looking after spectrometer text/figures for CDR:– Text written.– Will include 1 or 2 plots

I’ve just shown you.• Technical note is

somewhere between “draft” and “almost” done:– Have received

corrections from Matt Wing and Patric Muggli on Design + Layout sections.

– Simulations/Energy Reconstruction mostly plots: you’ve just seen them all…

07/03/13 Simon Jolly, UCL, AWAKE Collaboration Meeting

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