Accelerator Instrumentation and Technology for High Energy Physics

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Presentation transcript:

Accelerator Instrumentation and Technology for High Energy Physics John Byrd Center for Beam Physics LBNL

PEP-II Electron Cloud Diagnostics Question: How to get a more global view of the low energy electrons in the beam pipe? Initial idea: Measure electron induced modulation of first TE waveguide modes transmitted in the beam pipe. (Caspers and Kroyer, 2004) The results should be directly related to the averaged electron cloud density. The phase shift for an angular frequency w is given by with the plasma frequency For re=1012/m3, Df~ 1 degree PM sidebands at ±f0 A similar effect can be observed in the ionosphere, limiting the accuracy of GPS.

PEP-II Beam Pipe Transmission Expt Hardware installed in Region 12 straight solenoid field available to vary electron density initial tests can run parasitically with operations 2.84GHz, -25dBm John Byrd, LBL Uli Wienands, SLAC Ron Akre, SLAC Alan Fisher,SLAC Fritz Caspers, CERN Tom Kroyer, CERN ~ Digital Scope Agilent 54621A Spectrum Analyser HP 8560A Long coax cable down to tunnel PEP Tunnel High Pass 0º 180º 1 dB High Pass 180º 1 dB 0º Pmax = 15dBm beam TE wave Solenoid windings to control re PEP-II LER »30m

Initial observations An initial test shows some effect. Further studies starting now. No beam Beam pipe TE cutoff With beam 1.5 GHz 3 GHz 2 GHz 4 GHz