CERN’s n_TOF neutron spallation target operating experience and future consolidation plans M. Calviani (CERN) 6 th High Power Targetry Workshop Oxford, April
Outline n_TOF facility and experiment History of target #1 and target #2 Operational feedback of target #3 Design of target #3 and ongoing R&D 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop2
n_TOF facility Neutron time-of-flight facility for high accuracy cross-section measurements Nuclear astrophysics & Nuclear technology EAR1 ~185 m EAR2 ~20 m Spallation neutrons generated by 20 GeV/c protons on a lead target 20 GeV/c protons 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop3
14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop4 Courtesy: F. Gunsing (CEA)
n_TOF measurements 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop5 Courtesy: F. Gunsing (CEA)
n_TOF neutron flux Extremely high instantaneous neutron flux 10 6 n/cm 2 /10 ms (EAR2) Unique for measurement of radioactive isotopes High resolution in energy (~10 -4 ) resonance studies Large energy range (~mev to 1 GeV) Low repetition rate (<0.8 Hz) no wrap-around 11 orders of magnitude! 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop6 Measurements Courtesy: M. Barbagallo (INFN)
n_TOF facility and requirements Due to the specific use of the facility, focus is not on average power on target, but to instantaneous flux 8.5*10 12 p+/pulse in 7 ns (27 kJ) 1.5x1.5 cm 2 1 Rep. rate ~4.8 sec ~5.5 kW average Instantaneous power ~4 GW Important dynamical effects during pulse in target Target material: since facility conception, focus was on Pb: Highest neutron yield (!) Low neutron capture cross-section improved background conditions 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop7
n_TOF spallation target #1 ( ) 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop8 Facility was conceived in 2000 and operated with a Pb target immersed in a pool with cooling water Design limitations: Insufficient cooling and the hot spot (proton/lead impact) Surface oxidation due to rupture of protective layer when flushing Mechanical instability Lack of water chemical stabilisation – pitting corrosion enhancement Facility stopped in 2004 due to water contamination
n_TOF spallation target #2 (2008-now) 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop9 Cope with limitations of target #2 Target embedded in a pressurized vessel Monolithic lead core, support and anticreep in AW5083 Water chemistry continuously monitored
Target #2 operational feedback Target #2 is not optimized for EAR2 (whilst compatible!) Beam power on target is presently limited by the need to maintain surface temperature low enough to avoid water boiling 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop10 EAR1 EAR2
n_TOF target material results Dedicated analyses quantified average of 6 m/y (~80 m/y for 10 B circuit) for AW5083-H111 Erosion/corrosion of 99.99% Pb significant ~900 m/y average (local max 3.2 mm/y) Severe environment Pb corrosion products unavoidable, lead dissolved in water or residues O 2 production by radiolysis Smooth run since April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop11
Target #2 operational feedback 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop12 Erosion/corrosion generates a significant contamination of the circuit Long-lived isotopes “coating” the pipes of the cooling water circuits EDMS
Target #2 operational feedback 6 years operation: Average conductivity <0.15 S/cm Oxygen content below 80 ppb Full continuous purification via redundant ion exchangers Purified N 2 flush via a Liqui-Cel ® membrane 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop LS1
Target #2 operational feedback In order to reduce photon background in EAR1, the target moderator is filled with 10 B enriched boric acid in saturation (1.28%) Dedicated circuit to guarantee constant concentration Conductivity ~60 S/cm 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop14 Courtesy: C. Domingo (IFCV
n_TOF target inspection April 2014 External inspection performed in April 2014 Only surface oxidation stains have been observed, due to humid atmosphere 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop15
Introduction of target #3 design 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop16 Main goal is to reduce circuit contamination by embedding the production core in a corrosion resistant envelope Dedicated moderator for EAR2 Target structure in low Co SS316L (waste) Water cooling maintained to guarantee excellent time-to- energy relation 1.Ta-cladded pure W core + PbSb4 multiplicator 2.Ti6Al4V-contained PbSb4 core 3.Back-up: optimised bare PbSb4 core
14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop17 Option 1 Ta-cladded W via HIPing – excellent heat transmission Al anticreep structure for PbSb4 mass Option 2 Ti6A/Pb contact critical for heat evacuation Container shall always behave elastically w/o plasticization Eliminates creep problem
Physics optimisation 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop18 All solutions improve fluxes in EAR2 (up to a factor of 3x) Small reduction in fluxes for EAR1 (as bare Pb is the absolute best)
Ongoing prototyping works – Ta-cladded W 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop19 Ongoing orders with external companies to validate quality of the surface bonding Non destructive + destructive tests Synchrotron x-ray tomography (ESRF) Possible development in-house at CERN at a later stage
Ongoing prototyping works – Ti6Al-Pb 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop20 Few Ti6A-contained Pb prototypes (1:4 and simplified geometry) are being developed to find the most adapted production method for the best thermal contact Pb casting into Ti6A cylinder (+metal pressing) Pb cryogenic shrink fitting into Ti6A cylinder PbSb4 prototype cylinder metrology Al prototype for fitting tests Ø150 mm 100 mm
Foreseen beam tests HiRadMat 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop21 To evaluate the effect of stresses/fatigue on the materials interface (Ta-W, Ti6A-Pb), it is foreseen to perform a beam test at HiRadMat facility during 2017 ~3000 pulses per target, ~1.5*10 11 p/pulse, 10 mm sigma Ta-cladded W Ti6A-contained PbSb4 ~40 cm ~10 cm Tank 440 GeV/c beam See C. Torregrosa’s talk on HRMT-27 (AD-target materials)
Conclusions and perspectives 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop22 Significant experience developed for the operation of bare Pb targets at CERN since 2000 (target #1 and #2) New generation target (#3) will have a corrosion resistant cladding Detailed design of target #3 will progress until end of 2017, production in 2018 R&D activities being carry out to validate technical choices
Thanks a lot
Ex. Exchange of ion exchangers During this winter shutdown we exchanged both cooling circuit ion exchangers High dose rate ~10 mSv/h High contamination levels of the circuit (200 kBq/l) Collective dose ~0.6 mSv Mixed bed exchangers: Nuclear grade (Purolite ® NRW3240) Industrial grade (Amberlite 200C Na and IRA900 Cl) 14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop24
14 April 2016M. Calviani - n_TOF - 6th High Power Targetry Workshop25