Brookhaven Science Associates U.S. Department of Energy AGS Upgrade and Super Neutrino Beam DOE Annual HEP Program Review April 27-28, 2005 Derek I. Lowenstein.

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Presentation transcript:

Brookhaven Science Associates U.S. Department of Energy AGS Upgrade and Super Neutrino Beam DOE Annual HEP Program Review April 27-28, 2005 Derek I. Lowenstein

Brookhaven Science Associates U.S. Department of Energy 2 R&D Plan  Long baseline neutrino experiments are a compelling next high energy physics initiative in the US.  BNL (AGS) and Fermilab (MI) are the two possible sources of neutrinos that could satisfy the neutrino intensity and energy spectrum.  The R&D effort focuses on a phase 1 delivery of 9 x protons / 0.4 sec (1.0 MW); 2.3 x protons/10 7 sec The AGS has previously delivered 7 x protons/ 2 sec (.14 MW); 3.5 x protons / 10 7 sec Ultimate possibility of 1.8 x protons /0.2 sec (4 MW); 9 x protons / 10 7 sec.

Brookhaven Science Associates U.S. Department of Energy 3 AGS Intensity History 1 MW AGS

Brookhaven Science Associates U.S. Department of Energy 4 High Beam Power Proton Machines 1 MW AGS 10 MW 4 MW AGS

Brookhaven Science Associates U.S. Department of Energy AGS Alternative Intensity Enhancement Paths  Linac upgrade Conceptual design in 2004 neutrino experiment proposal  FFAG An old concept with a new twist Under investigation

Brookhaven Science Associates U.S. Department of Energy 6 Path to increased intensity  Minimize space charge at injection to the Booster and the AGS  Maximize AGS repetition rate

Brookhaven Science Associates U.S. Department of Energy 7

8 AGS Proton Driver Parameters present AGS1 MW AGS4 MW AGSJ-PARC Total beam power [MW] Beam energy [GeV] Average current [  A] Cycle time [s] No. of protons per fill0.7     Average circulating current [A] No. of bunches at extraction No. of protons per bunch1     No. of protons per 10 7 sec.3.5     10 20

Brookhaven Science Associates U.S. Department of Energy 9 AGS Upgrade to 1 MW 200 MeV Drift Tube Linac BOOSTER High Intensity Source plus RFQ Superconducting Linacs To RHIC 400 MeV 800 MeV 1.2 GeV To Target Station AGS 1.2 GeV  28 GeV 0.4 s cycle time (2.5 Hz) 0.2 s 200 MeV l 1.2 GeV superconducting linac extension for direct injection of ~ 1  protons low beam loss at injection; high repetition rate possible further upgrade to 1.5 GeV and 2  protons per pulse possible (x 2) l 2.5 Hz AGS repetition rate triple existing main magnet power supply and magnet current feeds double rf power and accelerating gradient further upgrade to 5 Hz possible (x 2)

Brookhaven Science Associates U.S. Department of Energy 10 Several of the items that were discussed in the October 2004 CDR will require R&D support. A second approach has developed since the CDR. Not everything has to be reinvented by a particular laboratory, so we will take full advantage of Fermilab’s NuMi experience and future R&D efforts, BNL’s and JLab’s experience with the SNS.

Brookhaven Science Associates U.S. Department of Energy GeV Superconducting Linac Beam energy 0.2  0.4 GeV0.4  0.8 GeV0.8  1.2 GeV Rf frequency805 MHz1610 MHz1610 MHz Accelerating gradient10.8 MeV/m23.5 MeV/m23.4 MeV/m Length37.8 m41.4 m38.3 m Beam power, linac exit17 kW34 kW50 kW

Brookhaven Science Associates U.S. Department of Energy 12 Some other areas that require further study

Brookhaven Science Associates U.S. Department of Energy 13 Beam Loss at H - Injection Energy AGS PSR SNS1 MW AGS BoosterLANL Beam power, Linac exit, kW Kinetic Energy, MeV Number of Protons N P, Vertical Acceptance A,   m  2  N P /  2  3 A),   m Total Beam Losses, % Total Loss Power, W Circumference, m Loss Power per Meter, W/m

Brookhaven Science Associates U.S. Department of Energy 14 AGS Injection Simulation RF voltage450kV Injection parameters: Injection turns360 Repetition rate2.5 Hz Pulse length1.08 ms Chopping rate0.65 Linac average/peak current20 / 30 mA Momentum spread  0.15 % Inj. beam emittance (95 %)  m Bunch length85 ns Longitudinal emittance1.2 eVs Momentum spread  0.48 % Circ. beam emittance (95 %) 100  m

Brookhaven Science Associates U.S. Department of Energy 15 New AGS Main Magnet Power Supply UpgradePresent Repetition rate2.5 Hz1 Hz Peak power110 MW 50 MW Average power4 MW 4 MW Peak current5 kA 5 kA Peak total voltage  25 kV  10 kV Number of power converters / feeds62

Brookhaven Science Associates U.S. Department of Energy 16 Eddy Current Losses in AGS Magnets For 2.5 (5.0) Hz: In pipe: 65 (260) W/m In coil: 225 (900) W/m

Brookhaven Science Associates U.S. Department of Energy 17 AGS RF System Upgrade Use present cavities with upgraded power supplies (two 300 kW tetrodes/cavity) UpgradePresent Rf voltage/turn0.8 MV0.4 MV harmonic number Rf frequency~ 9 MHz MHz Rf peak power2 MW Rf magnetic field18 mT

Brookhaven Science Associates U.S. Department of Energy 18 Beam line to your favorite western mine W

Brookhaven Science Associates U.S. Department of Energy 19 Neutrino Beam Production 1 MW He gas-cooled Carbon- carbon target New horn design Target on down-hill slope for long baseline experiment Beam dump well above ground water table to avoid water activation

Brookhaven Science Associates U.S. Department of Energy 20 Costs  The October 2004 proposal has an initial estimated direct construction cost of $273M. TEC of $407M (FY04$), including a 30% contingency and 14.5% overhead.  The incremental AGS operations costs to HEP, concurrent with RHIC, is estimated to be the order of $25M (FY05$) for a 35 week per year operation. Cost is dependent upon sharing beam time with other programs using the AGS at the time.

Brookhaven Science Associates U.S. Department of Energy 21

Brookhaven Science Associates U.S. Department of Energy 22 Path Towards >1 MW Upgrade IUpgrade IIUpgrade III Linac intensity/pulse1.0    Linac rep. rate2.5 Hz2.5 Hz5.0 Hz Linac extraction energy1.2 GeV1.5 GeV1.5 GeV  2  Beam power54 kW144 kW288 kW AGS intensity/pulse0.9    AGS rep. rate2.5 Hz2.5 Hz5.0 Hz Rf peak power2 MW4 MW8 MW Rf gap volts/turn0.8 MV0.8 MV1.5 MV AGS extraction energy 28 GeV28 GeV28 GeV Beam power1 MW2 MW4 MW

Brookhaven Science Associates U.S. Department of Energy 23 4 MW AGS Proton Driver Layout 200 MeV Drift Tube Linac BOOSTER High Intensity Source plus RFQ Superconducting Linacs To RHIC 400 MeV 800 MeV 1.5 GeV To Target Station AGS 1.2 GeV  28 GeV 0.2 s cycle time (5 Hz) 0.1 s 200 MeV

Brookhaven Science Associates U.S. Department of Energy 24 A new use of an old idea. An FFAG injector to the AGS.

Brookhaven Science Associates U.S. Department of Energy 25 FFAG proton drivers  Renewed interest in Fixed Field Alternate Gradient (FFAG) accelerators [F. Meot (Saclay)]  Advantages: High repetition rate (~ kHz), final energy > 1 GeV  Successful demonstration of scaling (fixed tune) FFAG [Y. Mori/S. Machida (KEK)]  Non-scaling designs with small tune variation are being developed  Example: Idea of a 10 MW proton driver: [A. G. Ruggiero (BNL)]  1 GeV, 10 mA, 10 MW, 1 kHz  After FFAG: DF: ~ 3 x 10 -4, I peak ~ 30 A  Issues: High rf power, fast frequency tuning, complicated magnetic field profile Target 200-MeV DTL 1.0-GeV FFAG H – Stripping Foil DFF SS gg x, cm 200 MeV 1.0 GeV s, m

Brookhaven Science Associates U.S. Department of Energy 26 AGS Upgrade with 1.5-GeV FFAG Performance Rep. Rate 0.4 -> 2.5 Hz Top Energy 28 GeV Intensity > 1.0 x ppp Ave. Power > 1.0 MW 1.5-GeV Booster 400-MeV DTL 28-GeV AGS HI Tandem 1.5-GeV FFAG AGS Cycle with 1.5-GeV FFAG 0.4 sec DTL cycle for Protons with 1.5-GeV FFAG 1 x mA (H – ) 1.2-GeV SCL

Brookhaven Science Associates U.S. Department of Energy 27 R&D funding request  We are preparing an accelerator R&D funding request (FY06) to investigate cost saving and performance enhancing alternatives for the development of a next generation neutrino source, directed towards a long baseline experiment. Simulating the space charge effects of high intensity beams. Reducing the costs and improving the reliabilty of the proton source and the neutrino production target station. Study the FFAG as an alternative to a high energy linac.

Brookhaven Science Associates U.S. Department of Energy 28 Conclusion An upgraded AGS with 1 MW (further upgradeable to 2 and 4 MW) beam power is a cost effective and competitive proton driver for a neutrino super-beam long baseline experiment.