Run 2 PMG 2/16/06 - McGinnis Run II PMG Stacking Rapid Response Team Report Dave McGinnis February 16, 2006.

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Presentation transcript:

Run 2 PMG 2/16/06 - McGinnis Run II PMG Stacking Rapid Response Team Report Dave McGinnis February 16, 2006

Run 2 PMG 2/16/06 - McGinnis January Antiproton Study Period  Quad Steering of the AP1 line  Not finished  Alignment of the Debuncher horizontal orbit and moveable devices.  Did not do arcs  Need to Energy align the AP2-Debuncher-Accumualtor  Horizontal Aperture up to 35  -mm-mrad!!!  Installation and commissioning of Debuncher lattice modifications  First round done  Vertical aperture up to 34  -mm-mrad  Removal of the Debuncher Schottkies  Completed  Obstruction search of the AP2 line.  Completed – none found  Installation of 4 additional AP2 trims  Two trims installed  Two trims staged  D/A Beam based alignment  Completed to the Q3-Q6 straight section  Accumulator orbit and aperture optimization  Underway  Backed out of orbit changes Need to update quad centering software Need to de-bug running wave software  Will only complete moveable devices

Run 2 PMG 2/16/06 - McGinnis Returning to Stacking After the Studies  Production into the Debuncher was good  Overall production was a function of the amount of beam on target.  Possible explanations  Spot size on target vs proton intensity  Bunch length on target vs proton intensity  Debuncher transverse cooling Far away from optimum gain Not tripping TWT’s  Accumulator Stacktail Flux  Measure production at various places along the chain as a function of intensity on target

Run 2 PMG 2/16/06 - McGinnis Antiproton Flux vs Intensity on Target

Run 2 PMG 2/16/06 - McGinnis Antiproton Stacking – Stacktail System  The time evolution of the antiproton phase space during cooling is best described by the Fokker-Plank Equation  Optimum profile that maximizes d  /dE for a constant stacking rate is exponential

Run 2 PMG 2/16/06 - McGinnis Antiproton Stacking – Stacktail System  The measured Accumulator 2-4 GHz Stacktail system can support a flux of 30mA/hr.  The currently used 2-4 GHz core momentum system is the same frequency as the Stacktail system  At a flux of 15mA/hr, the core 2-4 GHz system can support a exponential gain slope that is a factor of two larger than the gain slope of the Stacktail.  As the number of particles in the core increases, the factor of 2 gain slope is exceeded and the core pushes back on the Stacktail and the flux must be reduced.  For large fluxes into the Stacktail, the 2-4 GHz core momentum system cannot support a core.

Run 2 PMG 2/16/06 - McGinnis Antiproton Stacking – Stacktail System and the Core 4-8 GHz System  To support a core at high flux, the 4-8 GHz core momentum system must be used.  Because the 4-8 GHz core system runs at twice the frequency, the electrodes are ½ the size so the system has a factor of two smaller momentum reach.  Moving the core closer to Stacktail to accommodate the smaller reach resulted in system instabilities at moderate stacks.  We now :  Use the 2-4 GHz core momentum system to augment the hand-off between the Stacktail and the 4-8 GHz core momentum system  Run the 4-8 GHz core momentum system at MUCH larger gain.  Run the Stacktail during deposition debunching to pre- form the distribution to match the Stacktail profile

Run 2 PMG 2/16/06 - McGinnis Core 4-8 GHz Momentum Cooling System bandwidth  1 GHz of bandwidth at 7 GHz is ~3x more powerful than 1 GHz of bandwidth at 2.5 GHz  With simple redesign of the system equalizers, the 4-8 GHz system will be 5.7x more powerful than the 2-4 GHz system

Run 2 PMG 2/16/06 - McGinnis Stacking Performance

Run 2 PMG 2/16/06 - McGinnis Antiproton Parameters

Run 2 PMG 2/16/06 - McGinnis Future Pbar Work  Lithium Lens (0 – 25%)  Lens Gradient from 760T/m to 1000 T/m  Slip Stacking (7%)  Currently at 7.5x10 12 on average  Design 8.0x10 12 on average  AP2 Line (5-30%)  Lens Steering  AP2 Steer to apertures  AP2 Lattice  Debuncher Aperture (13%)  Currently at 30-32um  Design to 35um  DRF1 Voltage (5%)  Currently running on old tubes at 4.0 MEV  Need to be a t 5.3 MeV  Accumulator & D/A Aperture (20%)  Currently at 2.4 sec  Design to 2.0 sec  Stacktail Efficiency  Can improve core 4-8 GHz bandwidth by a factor of 2  Timeline Effects  SY120 eats 7% of the timeline

Run 2 PMG 2/16/06 - McGinnis Proposed Pbar Studies Review  Operational Issues (Drendel & Johnson)  Setup one-shots for circ beam in Deb  Setup Deb partial turn beam up AP2  Setup AP2 extraction of Deb circ beam  Setup for D/A orbit studies  Debuncher Orbit  Deb Orbit/BPM-Quad offset determination (Gollwitzer)  Deb Orbit Correction( Gollwitzer)  Deb Component Centering (Werkema)  Deb Electrical Centering ( Gollwitzer)  Deb Lattice Measurements (Nagaslaev)  AP2  Setting of the AP2-Deb Injection Region (McGinnis)  AP2 and Deb survey (Harms)  Lattice Design (Lebedev)  AP2 Orbit/BPM-Quad offset determination (Gollwitzer)  AP2 Orbit Correction (Gollwitzer)  AP2 Lattice Measurements (Nagaslaev)

Run 2 PMG 2/16/06 - McGinnis Proposed Pbar Studies Review  D/A Line  Acc Injection region (kicker & septa) (Derwent)  D/A Beam Based Alignment (Derwent)  Acc Injection channel and orbit Apertures (Derwent)  Deb Reverse Proton TBT system (Vander Meulen)  D/A Kicker time during stacking (Ashmanskas)  DRF2 timing (Ashmanskas)  Accumulator Aperture  Quad centers on the Accumulator (Werkema)  Orbit Correction in the Accumulator (McGinnis)  Moveable devices (Werkema)  Stacking  P1-P2-AP1 drift and auto-tune (McGinnis)  AP2 Orbit drift and correction (McGinnis)  Stacking Losses in AP50 (Werkema)