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High Brightness Electron Beam Diagnostics and their ... - CASA

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Parabolic<br />

off-axis<br />

reflector<br />

~ 300 mm<br />

Wire Grid Polarizer<br />

Figure5.11:Overviewoftheopticstoguidethecoherenttransitionradiationemittedfroman aluminumfoiltotheentranceoftheinterferometer.<br />

Air Actuator<br />

to insert TR radiator<br />

Plano-convex<br />

into the beam path<br />

Light shield<br />

lens (f<br />

IR<br />

=125 mm)<br />

mirror(M1)ismountedonamicropositionerthatcantranslateby1msteps.Twopicomo-<br />

<strong>Beam</strong><br />

direction<br />

optical port<br />

Aluminum Foil<br />

sitivearea.Itisan-oaxisgold-sputteredreectorwithafocallengthof10cm. Theplanarmirrorsarest<strong>and</strong>ardopticalcircularmirrorsof50:8mmdiameter.Themovable Theparabolicreectorisusedtofocusanincomingcollimatedbeamontothedetectorsentorsarealsomountedonthemirrorgimbalmountsthatcanbeusedremotelytoadjustthe horizontal<strong>and</strong>verticalinclinationofthemirrortomakesureitiscoplanarwiththeimageof thexedmirror(M2)throughthebeamsplitter.<br />

"Switcher" Mirror<br />

~ 600 mm 125 mm<br />

ThepolarizinginterferometerisdepictedinFig5.12:Let'srstanalyzehowapolarizinginterfer- 5.5.2TheoryofOperation ometerworksinthesimplistic(usual)caseofaplaneTEMwave.Afterward,wewillrenethis TheGolaycell(seeFig.5.7)<strong>and</strong>itsacquisitionsystemhavebeendescribedpreviously.<br />

analysisincludingtheeectduetoTRelectriceld. Let!E(t)betheelectriceldincomingintotheinterferometer.Whenthiseldentersthe<br />

~ 400 mm<br />

~ 300 mm<br />

Fixed Mirror<br />

Wire Grid Polarizer<br />

Movable Mirror<br />

Golay Cell Detector

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