Experience with Insertion Device Photon Beam Position Monitors at the APS

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1 Experience with Insertion Device Photon Beam Position Monitors at the APS 27.6 meters (The APS has forty sectors meters total circumference)

2 Beam Position Monitors and Magnets in One Sector 18m X2 20m X2 11m X1 16m X1 Q FC BM x x x BM ID C C C C C C x C e - : Broad-band RF Beam Position Monitors (7) (Turn-by-Turn) x : Narrow-band RF Beam Position Monitors (4) (~ 300 Hz) : BM X-ray Beam Position Monitors (2 - Vertical Only) (~165 Hz) : ID X-ray Beam Position Monitors (2) (~165 Hz) FC : Fast Corrector Magnet (1) (~ 1000 Hz) C : Slow Corrector Magnets (7) (few Hz) Q : Quadrupole Magnets Bending Magnet and BPM Arrangement RFBPMs BM XBPMs #1 # (meters) (Source) Insertion Device and BPM Layout RFBPMs ID s XBPMs # 1 # (meters) (Source)

3 Insertion Device Photon Beam Position Monitor Blade Geometry Stray Radiation Sources X-ray BPMs (16, 20 meters from source) Insertion Device ID photons Main Dipole Bend Magnet 5 meters 78 mrad Legend Positron Trajectory Focusing Quadrupole Magnet Defocusing Quadrupole Magnet Sextupole Magnet Combined Function Horz./ Vert. Steering Corrector Magnet

4 Re-direction of Stray Photons by Girder Alignment* Stray radiation from upstream dipole, quadrupoles, sextupoles and correctors ID photons 77 mrad 1 mrad * Phys. Rev. ST Accel. Beams 2, (1999) Stray radiation from downstream dipole, quadrupoles, sextupoles and correctors Upstream X-ray BPM Downstream X-ray BPM P1 Blade Signal Sum Unmodified Sector 1ID Modified Sector P2 Blade Signal Sum Insertion device gap Insertion device gap

5 Raw Corrector Settings -136 Amps = -1 mrad Geometries of Canted Undulators and decker Distortions -78 mrad ID Undistorted Distorted -1 mrad mrad (= -78+1) -1 Canted, configuration mm Canted, configuration mm Canted, configuration 3

6 BPM Offset vs. Gap Lookup Tables (Vertical) Not distorted 200 m Not distorted BPM Offset vs. Gap Lookup Tables (Horizontal) Not distorted 400 m ID 20 Not distorted

7 Correction of Residual ID Photon BPM Gap-dependent Systematic Errors Background Subtraction Only Background + Exponent Corrections x (Absolute) x (Absolute) 100 microns ID 20 Gap (mm) ID 20 Gap (mm) x (Relative) x (Relative) approx. 40 microns ID 20 Gap (mm) ID 20 Gap (mm) Long Term Drift of BM and ID Photon BPM Readbacks BM ( m) Detectors 11 m from source ID ( m) Detectors 16.3 m from source

8 One-Week Angular Drift rad Local Steering Local Tunnel Air Temperature Impacts Pointing Stability Air Temp (deg. F) 8ID V. Angle ( rad) 8ID H. Angle ( rad)

9 Conceptual Design of Hard X-ray Beam Position Monitor (Top View) Cooled Cu X-ray Fluorescent Source Be. Filter Rectangular Beamline Photo-resistive Limiting Aperture Diamond Detectors (Approx. 3 x 2 mm) ~30 meters from source Side View

10 Summary An extensive accelerator re-alignment is near completion after a 6-year effort, resulting in reduced insertion device photon bpm stray radiation background signals. Correction of residual gap-dependent systematic errors is presently performed using lookup tables. Careful alignment, background subtraction, and algorithm refinement should further reduce systematic errors to the to 20 micron level (~0.5-1 rad). (but depend critically on assumptions / constraints) Development of a gold standard hard x-ray bpm located 30 meters from the source should allow achieving nrad-scale long-term pointing stability (perhaps the only way).

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