Next linear collider test accelerator : conceptual design by Stanford Linear Accelerator Center

By Stanford Linear Accelerator Center

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First rule: Must have asymmetric emittances from the start of beam propagation (see theorem) - use asymmetric beams. charge dominated beam dynamics, rf design, laser and cathode design, etc. 53 LC93 - EIe~Ci-onGun Talk October 18, 1993 Mitigating Space Charge Because the electron trajectories am essemialily laminar, one can remove much of &e sjpace charge contribution to the emittance. "Focus+Drift"scheme (Carlsten and Sheffidd). Well understood theoretically for round beams. Model: and experimenta i X* CaC 7 \ X Focus X 0 X' Fruze space charge at this point by acceIention, prescrve the "collapse' of the bow-tie in phasespace.

I .. I I . - . 23 Cross checking the SLAC Mott polarimeters How: Use a standard polarized source Problem: There is NO standard polarized source Solution: Create a standard! How: Farm out thin (1oOnm) unstrained GaAs samples from a well characterized wafer to groups with 2% calibrated polarimeters. Have them measure P & QE at a given wavelength and temperature. Expect: 40 % < P < 50 % . , -. - 1993A new type photocathode for the polarized electron source with a distributed Bragg reflector Takashi S A K A Toshihiro KAT?

I .. I I . - . 23 Cross checking the SLAC Mott polarimeters How: Use a standard polarized source Problem: There is NO standard polarized source Solution: Create a standard! How: Farm out thin (1oOnm) unstrained GaAs samples from a well characterized wafer to groups with 2% calibrated polarimeters. Have them measure P & QE at a given wavelength and temperature. Expect: 40 % < P < 50 % . , -. - 1993A new type photocathode for the polarized electron source with a distributed Bragg reflector Takashi S A K A Toshihiro KAT?

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