5 mev mott measurement
DESCRIPTION
5 MeV Mott Measurement. Overview: polarized electrons Mott scattering injector polarimeter training & qualification. for CEBAF Operations group Joe Grames, Marcy Stutzman February 14 th , 2007. Sir Nevill F. Mott at the ceremony with his Nobel Prize for Physics, 1977. ( N + - N - ). - PowerPoint PPT PresentationTRANSCRIPT
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5 MeV Mott Measurement
for CEBAF Operations group
Joe Grames, Marcy Stutzman
February 14th, 2007
Sir Nevill F. Mott at the ceremony with his Nobel Prize for Physics, 1977
Overview:• polarized electrons• Mott scattering• injector polarimeter• training & qualification
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What is a polarized beam?A beam is polarized in a specific direction if the average value of all the spins along that direction is not zero.
Polarization =(N+ - N-)
(N+ + N-)
(9 - 1)
(9 + 1)= 80%
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Polarized electron beam
• Circularly polarized laser light on GaAs• Polarized electrons generated• Polarization is longitudinal
– Parallel or anti-parallel to direction of beam motion (this is called the helicity)
• Wien filter used to change direction of polarization– Polarization direction changes, but beam
orbit unchanged (use injector steer script)
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What is a polarimeter?A polarimeter is a tool which analyzes the polarized beam in a way that an observer (you) may physically detect and measure.
= Aexp
(R1 – R2)
(R1 + R2)Analyzer • Pbeam =
Beam
R1
R2
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Mott scattering
• “Low” energy electrons (20 kV- 10 MeV)
• Heavy nucleus atoms (e.g., gold Z=79)• “Spin-orbit” interaction
– Interaction of orbital angular momentum of electron (L) and its magnetic moment (µs)
– VSO~ L· µs
• Sensitive to electron polarization direction transverse to beam motion
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Sherman function
• Scattering asymmetry
• Sherman function– Depends on electron
energy, target material, scattering angle
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• Targets– Ideal target: single heavy
nucleus, e.g., Au, Ag or Cu– Real target: thick foils (nm or
m), diluted Sherman function, extrapolation to zero thickness
Polarimeter targets
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Vacuum Valve
SetupViewer
Target Corrector
Dump Dipole
Detector Hut
TargetChamber
Target/ViewerLadder
Start with beam to FC2.A script reliably steps you through Mott setup.Perform measurement of beam polarization.The script restores conditions when finished.
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Why flip the helicity?We reverse the sign (+ or -) of the beam polarization at ~30 Hz to cancel differences between the two detectors (R1 or R2).
For each detector we measure an asymmetry:
AR1exp =
(R1+ - R1-)
(R1+ + R1-)
We combine asymmetries for the two detectors (AR1exp AR2
exp) to arrive at a “super asymmetry” Aexp is proportional to the polarization.
Aexp = S • Pbeam
measured
unknown
Analyzer (known)
AR2exp =
(R2+ - R2-)
(R2+ + R2-)
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Detector Spectra
• Detector package– E (energy)– E (discriminates
photons)
• Mott data analysis automated
• Looks for asymmetry between up and down counts
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Detector Asymmetryelectronicthreshold inelastic elastic
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Mott operation• Spin must be rotated transverse to get a
Mott asymmetry (Wien filter ~70° or more)• Target
– We routinely use our 1 m gold foil– Extrapolated Sherman function well known– Beam current 0.5 to 1 A sufficient for 5 min run
• Use FC1 to ensure <1uA• FC2 is downstream of the Mott dipole – won’t help
during measurement
• Backgrounds– Field emission from 0L03/0L04 cryomodules
• “Auto-Joan” disabled so that we can turn off injector cryomodules
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Qualification – means sitting w/ expert to watch & learn, then you do w/ expert present & finally “signed off”:
• Preparing for Mott• Delivering beam to polarimeter• Changing the Wien angle• Beam setup troubleshooting• Adjusting detector HV• Making a measurement• Logging the data• Backing out of Mott
Training
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Okay, Sir Nevill Mott says,
“ let’s measure the beam polarization!”