HiPoSpaNS High Power Spallation Neutron Source

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Presentation transcript:

HiPoSpaNS High Power Spallation Neutron Source Tobias Bär, Miriam Fitterer, Fernando Mirapeix, Robert Williamson

Why do we want a spallation neutron source?

Neutrons penetrate deep into matter Alpha Beta X-rays Neutron

Neutrons “see” the world in a unique way

HiPoSpaNS Site HiPoSpanNS site: about 10km west of San Sebastian (Spain) HiPoSpaNS

Schematic Layout Management and HR Injection Source, RFQ, Linac Tetrode gallery RF Extraction FIPPS Target & Experimental Hall

Injector Penning type H- ion source, 1ms 3 solenoid LEBT RFQ MEBT DTL CCL SCL 65 keV 3 MeV 50 MeV 200 MeV 400MeV Penning type H- ion source, 1ms 3 solenoid LEBT 4-vane RFQ, 324 MHz Fast chopper in MEBT Frequency jump at CCL to 648 MHz Superconducting linac to 400 MeV

Synchrotron 0.4 – 1.5 GeV RCS 700m, 3 superperiod doublet lattice Sinusoidal B field (0.27 – 0.6T) Ceramic vacuum chamber RF frequency sweep Magnetic alloy loaded cavities (304 – 415 kHz, 608 – 830 kHz) Gamma Transition 9.14 H- Charge exchange injection Carbon foil 1.25 x 1014 protons over 670 µs (~200 turns) Fast kicker extraction of 1µs pulse RCS

T-FIPPS Target Tunable Fully Integrated Power Powder Stream Target

T-FIPPS Target Parameters Powder material: W, Ni, Ti, (U) Beam-Powder interaction length: 2m (≈2.5 ∙ mean free path in W powder) Jet velocity: 5m/s Neutron flux: About 30n/p, -> 3∙1017 n/s

Summary High power microscope for the future Large neutron user community A steal at only €1bn Several upgrade paths Investment for the future