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Wire scanners MDW chicane energy collimator 3 MPS collimators in this region end of linac Damage Simulation in MPS Collimators L. Keller Apr. 9, 2006.

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Presentation on theme: "Wire scanners MDW chicane energy collimator 3 MPS collimators in this region end of linac Damage Simulation in MPS Collimators L. Keller Apr. 9, 2006."— Presentation transcript:

1 wire scanners MDW chicane energy collimator 3 MPS collimators in this region end of linac Damage Simulation in MPS Collimators L. Keller Apr. 9, 2006

2 500 kW beam (0.65 MJ in 1.3 sec) Beam diameter ~ 2000 µ 30 cm Beam scraping the edge of a 30 cm long copper block SLAC Damage Test - 1971 It took about 1.3 sec to melt thru the 30 cm block, but for this relatively large beam, the front two radiation lengths remain intact.

3 MPS energy collimator ΔE/E = ±10% trajectories Diagnostic Chicane Use FLUKA to Model an Off-energy Beam Hitting the Sacrificial Energy Collimator MDW

4 X (cm) beam axis Z (cm) cm Al melting Beam into Edge of Two Meter Aluminum MPS Collimator FLUKA 200 bunches 1  from edge, E beam = 250 GeV 0.2 cm half-gap 250 GeV beam, 0.16 MJ in 60 µsec Al boiling Above Al melting GeV/e -

5 X (cm) Y (cm) beam axis into page FLUKA Aluminum melting Aluminum MPS Collimator Near Shower Maximum 200 bunches 1  from edge, E beam = 250 GeV 0.2 cm half-gap 250 GeV beam, 0.16 MJ in 60 µsec GeV/e -

6 X (cm) beam axis Z (cm) cm Beam into Body of Two Meter Aluminum MPS Collimator FLUKA 200 bunches E beam = 250 GeV 0.2 cm half-gap 250 GeV beam, 0.16 MJ in 60 µsec Al boiling Al melting GeV/e -

7 X (cm) beam axis Z (cm) cm Beam into Edge of Two Meter Aluminum MPS Collimator FLUKA 200 bunches 1  from edge, E beam = 500 GeV 0.2 cm half-gap 500 GeV beam, 0.32 MJ in 60 µsec Al boiling Al melting Above Al melting GeV/e -

8 X (cm) beam axis 200 bunches 1  from edge, E beam = 250 GeV Z (cm) cm C melting Beam into Edge of Two Meter Carbon MPS Collimator FLUKA C boiling 250 GeV beam, 0.16 MJ in 60 µsec GeV/e -

9 MPS Collimator Summary: 1. 200 full energy bunches hitting an aluminum block within 2 mm of the edge will eject molten and vaporized aluminum into the gap over a length of ~1 meter. 2. During accelerator tune up, the bunch intensity would need to be reduced by ~2 orders-of-magnitude and the emittance increased to avoid melting. (This is not new information.) 3. To avoid collimator damage, a spoiler/absorber combination would require a ≈0.5 rl consumable spoiler and many tens of meters of drift to the absorber (not simulated yet). 4. If the first part of the 200-bunch train vaporizes aluminum along the beam path, the longitudinal extent of the collimator damage may be considerably greater than one meter (not simulated). 5. A carbon collimator melts and vaporizes in a much smaller volume than in aluminum.


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