Front End Technologies Harold Kirk Brookhaven National Laboratory February 19, 2014.

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Presentation transcript:

Front End Technologies Harold Kirk Brookhaven National Laboratory February 19, 2014

The Front End Technology Challenges Target Chicane RF for Buncher/Rotator Ionization cooling (MICE/Cooling talks to follow) Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Technology Challenges Target and Capture –3 GJ (15T, 2.4m ID ) superconducting solenoid –Shielding for SC coils surrounding the target –Replaceable Target Module (Solid or Liquid) –Beam dump (splash mitigation if liquid target) Chicane –Field requirements (B ≥ 2T) –Shielding for SC coils RF for Buncher/Rotator –325 MHz with 20 MV/m in B ≥ 2T field Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Liquid Target System Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19, MW Candidate materials: Hg, Ga, PbBi Use of Ga results in ~15% loss in muon production

A Solid Target System February 19, 2014 Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014)5 He-cooled W-balls shielding Target Module

Solid Target Module February 19, 2014 Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014)6 75 cm Carbon Rod 75 cm Carbon Beam Dump 1 MW Candidate material: Carbon 4 Interaction Lengths 1% unspent primary proton beam

Drive Beam Energy Budget The primary beam energy goes to: ~10% into the Target Module ~15% conduced downstream ~ 75 % into the volume immediately surrounding the target module February 19, 2014 Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014)7

He Cooled Shielding 75% of beam power absorbed in target shield Shielding concept: 97% pure Tungsten balls 60% packing fraction He gas flow cooled –W and H 2 O are incompatible –Reduce activation products (e.g., tritium) Thermal engineering required to establish feasibility Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Liquid Target Issues Jet delivery (Nozzle Design) Splash Mitigation –20 m/s could cause significant disruption of the liquid in the collection system –Potential to disrupt particle production –Chosen solution will need to be bench tested Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Chicane Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) Push toward higher decay channel B fields (≥2T) will require SC coils A credible shielding solution will be needed P. Snopok, IIT,FNAL C. Rogers, RAL February 19,

Buncher/Phase Rotator Require 325MHz, 20 MV/m, B ≥ 2T Gradient corresponds to: – 201MHz: 16 MV/m – 805 MHz : 32 MV/m MTA rso far: 805 MHZ, 20 MV/m, B=5T Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Summary Front End technical challenges include: Shielding for the target and capture solenoids Shielding solution for the chicane. The liquid delivery system –An improved jet stream –Splash mitigation of the 20-m/s jet in the liquid collector Operation of high-gradient 325 MHz cavities in fields B ≥ 2T Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Backup Slides Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

15T Liquid Target Solution Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Utility Connections for 15T System Shielding Helium Remote Handling Features Nozzle Supply Beam Entrance Vent Mercury Drains Mercury Vessel Helium Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Liquid Target System Core Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) He-cooled W-balls shielding Splash mitigation Hg delivery system February 19,

MERIT Beam Pipe Simulations Y. Zhan, Stony Brook Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) February 19,

Free Jet Simulations Harold Kirk, BNL | DOE Review of MAP (FNAL, February 19-20, 2014) T = 16 ms T = 111 ms T = 180 ms 20 m/s Hg Jet in air Results encouraging, but: Nozzle is simple circular orifice 2D simulation—need 3D February 19,