Nufact09-IIT 107/24/2009 Project X and a Muon Facility at Fermilab Milorad Popovic FNAL.

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Presentation transcript:

Nufact09-IIT 107/24/2009 Project X and a Muon Facility at Fermilab Milorad Popovic FNAL

207/24/2009 Nufact09-IIT

307/24/2009 Proposed 8-GeV Implementation Plan Introduction Layouts and Beam Transfer Schemes – Booster Era – Project X Era (Beam Power = GeV) – Upgraded (4MW) Project X Experiments – Configurations – Proposed Locations – Beam Requirements – Providing the required proton time distributions

Nufact09-IIT 407/24/2009 Experiments and Their Requirements Various groups would like to do experiments made possible by intense 8-GeV proton beams: – Muon-to-electron conversion – Muon g-2 – K->  (with neutral and charged kaons) – Muon test beams – Neutrino factories based on muon storage rings – Muon colliders – Accelerator physics research and development We’ve been communicating with them to understand their needs. – Most want to start ASAP. – Many want a phased approach to high beam power. – Various time distributions are desired for proton beam.

Nufact09-IIT 507/24/2009 Advantages of the Proposed Plan It’s flexible. – Experiments can start with Booster beam, then transition to beam from Project X without relocating. – Beam time can be shared flexibly. It’s economical. – Existing infrastructure is intensely used. – Only one new tunnel for starters, a short one at that – Only one new high-power target station/exp’t hall – All (or most?) 1 st -round experiments located in one area It can be implemented rapidly. – The new tunnel could be built soon as an AIP project. It provides a path back to the energy frontier. – Target station is located in line with a long-term plan

Nufact09-IIT 607/24/2009 MI and RR time lines for NO A The Recycler is empty for as many as 8 Booster ticks.

Nufact09-IIT 707/24/2009 The proposed beam path, 8GeV Protons The cheapest route between two rings is via existing beam lines.

8 g-2 Beam Delivery Concept

Nufact09-IIT 907/24/2009 Take 2 cycles at time from Booster (thru Recycler) – stack in Accumulator – (~33ms) Form into 4 bunches – ~33ms – 1 bunch at time transfers to Debuncher Stretch Debuncher to slow extraction over 66ms – 2.4×10 12 / bunch (δν < 0.02) Use Recycler to accumulate Booster cycles – 12/20 to NuMI (1.33s) – 8/20 to mu2e (16/20)duty cycle Timing Diagram/Beam Delivery to mu2e

Nufact09-IIT 1007/24/2009 m 2e Beam Delivery Concept 20M$ 4M$

Jan-0811 Ankenbrandt and Popovic, Fermilab Recent documentation (note contributors)

Jan-0812 Ankenbrandt and Popovic, Fermilab Second Project X Physics Workshop Proposed Implementation Plan for Physics with Intense 8 GeV Proton Beams after the Tevatron Collider Era (A Tunnel Vision) Chuck Ankenbrandt and Milorad Popovic Fermilab January, 2008

Jan-0813 Ankenbrandt and Popovic, Fermilab 13  ->eg-2  Test Facility Booster-era Beam Transfer Scheme Rare Kaon Decays New 200-kW target station that can be upgraded to >2 MW

Nufact09-IIT 1407/24/ MW Target Station for Factory or Muon Collider

Jan-0815 Ankenbrandt and Popovic, Fermilab 15 2 MW Target Station for Factory or Muon Collider

Nufact09-IIT 1607/24/ MW Target Station for Factory or Muon Collider 14 m

Jan-0817 Ankenbrandt and Popovic, Fermilab 17 Beam Path to 200kW target station in Project X Era

18 Sitting of mu2e, g-2, Kaons,  test area, 4GeV Factory mu2e g-2  test area factory Rare Ks Nufact09-IIT 1807/24/2009

Jan-0819 Ankenbrandt and Popovic, Fermilab 19 Path of Beams to 4 GeV Factory in Project XLR8 Era

Neutrino Factory as 1 st Step Toward Muon Collider 1GeV H- Linac  <1 Structure 7GeV H- Linac  =1 Structure Proton Accumulation, Bunching Ring, 10 bunches 5x14GeV  Linac  =1, 50Hz 1 GeV,200MHz  Linac 4 GeV,400MHz DogBone  Linac 2-4MW-Target  Capture/Bunching/Cooling Proton Driver 2-4MW, 5Hz

8GeV H- Beam H-Striping&Proton Accumulation Bunching Targeting  CuptureBunchingCoolingAcceleration DUSEL 4 or 40GeV -Fact

80GeV Linac 80GeV Linac Collider Ring Muon Collider Stage

 80GeV Linac 80GeV Linac Collider Ring  m Acceleration m Collisions

Nufact09-IIT 2407/24/2009 Stop here

Jan-0825 Ankenbrandt and Popovic, Fermilab Jan Rare Kaon Decay Experiments Fermilab Milorad Popovic

Jan-0826 Ankenbrandt and Popovic, Fermilab Jan Collider Fermilab Milorad Popovic

Jan-0827 Ankenbrandt and Popovic, Fermilab Jan Collider Fermilab Milorad Popovic

Jan-0828 Ankenbrandt and Popovic, Fermilab Jan Collider Fermilab Milorad Popovic

Jan-0829 Ankenbrandt and Popovic, Fermilab Rare K Decay Experiment Requirements Beam Power – Booster era: ~ 25 kW – Project X era: 200 kW or even more Proton time distribution for KOPIO-like experiment – Slow spill with high duty cycle – Bunch length <~ 300 psec (the shorter the better) – Bunch separation ~ 40 nsec (Charged K exp’t can use KOPIO beam time structure) Creating the proton distribution in the Booster era – Momentum-stack three Booster batches in the Accumulator – Rebunch at ~26.4 MHz – Single-turn transfer all 42 bunches to the Debuncher – Add high-frequency rf harmonics of 26.4 MHz to ring voltage – Resonantly extract from the Debuncher – Repeat the above sequence twice per MI cycle

Jan-0830 Ankenbrandt and Popovic, Fermilab 30 Providing Proton Bunches for a Neutrino Factory or a Muon Collider

Nufact09-IIT 3107/24/2009 Booster-Era Beam Timelines for mu2e Experiment