Talks from the meetings of the European target and collector working group can be found on the ENG site
.
Neutrino Factory Targets
Current (2005) neutrino factory designs call for a 4 MW (mean) proton beam of 2–30 GeV energy impinging on a heavy element target. The beam is pulsed at 50 Hz with ~50 μs long macro-pulses consisting of one or more micro-pulses of ~1 ns length.
The target, 1–2 cm in diameter and 20 cm long, dissipates 1 MW (mean) and a dump target absorbs the remaining 3 MW of beam power. The high power density causes problems with cooling a static target and the high energy density per pulse gives rise to severe thermal shock effect.
At present three target solutions are proposed
- A mercury jet target which easily removes the heat. The target is blasted apart by each beam pulse but reforms before the next pulse, thereby overcoming the thermal shock problem.
- A solid target of small spheres to overcome the thermal shock problems, cooled by flowing helium or water.
- A rotating toroidal ring operating at 2000 K, dissipating the heat by thermal radiation to water cooled walls. The thermal shock is a problem which is presently being examined.
External links:
The Oxford–Princeton Workshops on High Power Targets:
- HPT1
(Oxford, May'08)
- HPT2
(Princeton, Nov'08)
- HPT3
(Oxford, Nov'09)
Two-yearly conferences on high power targets:
An excellent source of references to target studies is to be found at Kirk McDonald's web site
.
The nTOF11 'MERIT' target experiment
in the TT2A tunnel at CERN combines all elements for a true study of the mercury jet target option: an intense proton pulse hits the jet while enclosed in a 15T solenoid.
The European hadron production experiment, HARP
, will gather important data about the performance of materials for pion targets.
The Brookhaven targetry and phase rotation experiment, E951
, was in a way the predecessor to MERIT, testing the jet dispersal without the solenoid present.
File  | Title | Authors | Date | Published |
|---|
iwsmt8thermalshock.ppt | Thermal Shock Measurements and Modelling for Solid High-Power Targets at High Temperatures | J.R.J. Bennett, G. Skoro, S. Brooks, R. Brownsword, C.J. Densham, R. Edgecock, S. Gray, A.J. McFarland and D. Wilkins | 2006-10-16 | IWSMT-8 |
muoncollaboration.ppt | Thermal Shock Measurements and Modelling for Solid High-Power Targets at High Temperatures | J. R. J. Bennett, G. Skoro, J. Back, S. Brooks, R. Brownsword, C. J. Densham, R. Edgecock, S. Gray and A. J. McFarland | 2007-01-29 | Muon Collaboration Meeting, UCLA |
nufact06shocktests.ppt | Shock Tests on Tantalum and Tungsten | J.R.J. Bennett | 2006-08-18 | NuFact'06 |
thermalshock.ppt | Thermal Shock Measurements for Solid High-Power Targets at High Temperatures | J. R. J. Bennett, G. Skoro, J. Back, S. Brooks, R. Brownsword, C. J. Densham, R. Edgecock, S. Gray and A. J. McFarland | 2007-02-22 | Joint NF and EURISOL Target Meeting, CERN |
uknfnote_1.pdf | Considerations of Temperature Distribution in Heavy Metal Targets for the Neutrino Factory | C.Densham, P.Drumm, R.Bennett | 1999-08-15 | |
uknfnote_2.pdf | Some thoughts on a high power, radiation cooled, rotating toroidal target for neutrino production | R.Bennett | 1999-08-15 | |
uknfnote_9.doc | Target studies for a neutrino factory at the Rutherford Appleton Laboratory | P.Drumm, C.Densham, R.Bennett | 2000-07-28 | |
uknfnote_13.pdf | Plans for electron beam stress testing of target materials suitable for a neutrino factory | P.Drumm, C.Densham | 2001-01-03 | |
uknfnote_24.doc | A High Power Density Toroidal Target | R.Bennett et al. | 2001-09-10 | Basic Technology Bid |
uknfnote_30.pdf | Simulations of Pion Production in a Tantalum Rod Target using GEANT4 with comparison to MARS | K.A. Walaron | 2005-08-26 | |