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45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences.

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Presentation on theme: "45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences."— Presentation transcript:

1 45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences and Education LCWS11 27 September 2011 Baseline Damping Ring Lattice Design Status

2 27 September 2011 LCWS11 Baseline Damping Ring Lattice Design Status / J.A.Crittenden 2 / 4 Bunch Current Scan Analysis Disentangling the Photoelectron Production Kinetic Energy Distribution from the Beam Kick Strengths The early SPU signal from the leading bunch for a positron beam is largely due to photoelectrons produced on the bottom of the vacuum chamber. This is the closest production point where the beam kick attracts the photoelectrons toward the SPU. Thus the size and shape of the leading bunch signal is determined by the reflected photon rate, azimuthal distribution, the quantum efficiency for producing photoelectrons, and the kinetic energy distribution of the photoelectrons. In particular, the arrival time distribution determines the shape. By modeling the shape for different strengths of beam kick, we can determine the photoelectron energy distribution. An example of such an analysis is shown on the left. Note that the signal begins just a few nanoseconds after bunch passage even for weak beam kicks, indicating that high-energy photoelectrons were produced (hundreds of eV).

3 27 September 2011 LCWS11 Baseline Damping Ring Lattice Design Status / J.A.Crittenden 3 / 4 Example: 3 mA/bunch 5.3 GeV e+ 15E a-Carbon Two Power-Law Contributions F(E) = E P1 / ( 1 + E/E 0 ) P2 E 0 = E peak (P 2 -P 1 )/P 1 This level of modeling accuracy was achieved with the photoelectron energy distribution shown below, using a sum of two power law distributions. E peak = 80 eV P 1 = 4 P 2 = 8.4 The high-energy component (22%) has a peak energy of 80 eV and an asymptotic power of 4.4. Its contribution to the signal is shown as yellow circles in the lower left plot. E peak = 4 eV P 1 = 4 P 2 = 6 The low-energy component (78%) has a peak energy of 4 eV and an asymptotic power of 2. It's contribution to the signal is shown as pink triangles.

4 27 September 2011 LCWS11 Baseline Damping Ring Lattice Design Status / J.A.Crittenden 4 / 4 Photoelectron Energy Distribution 5.3 GeV e+ 15E a-Carbon

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