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FLUKA for accelerator radiation protection –Indian perspective. Sunil C Accelerator Radiation Safety Section Radiation Safety Systems Division , Bhabha Atomic Research Centre. Accelerator Radiation Safety Section. Operational radiation protection Associated R&D
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FLUKA for accelerator radiation protection –Indian perspective Sunil C Accelerator Radiation Safety Section Radiation Safety Systems Division, Bhabha Atomic Research Centre
Accelerator Radiation Safety Section • Operational radiation protection • Associated R&D • Heavy Ion Accelerators (TIFR Bombay and VECC, Calcutta • ~5-7 MeV/amu Pelletron • ~10 MeV/amu with a superconducting linac booster • ~100 MeV/amu superconducting cyclotron • Electron accelerators (RRCAT Indore) • 20 MeV Microtron to 2.5 GeV electron synchrotron • High current industrial accelerators
Future plans • ADSS • Proton accelerators • 20 MeV to 1 GeV • Swimming poll critical reactor that can also be operated in sub critical mode with 600 MeV protons incident on LBE • 14 MeV neutron generators • Bare • Injectors for sub critical assemblies
Uses of FLUKA • Routine accelerator radiation protection • Source term calculations • Shielding • Induced activity • Synchrotron hutch shielding • Photoneutron estimation • ADSS • Proton accelerators • Secondary particle dose from heavy Ion reactions • Muon Transport and dose estimation • Spallation yields comparison with JQMD
Heavy Ion accelerators • Neutron source term calculations • EMPIRE, PACE (heavy ions) ALICE, PRECO (protons) • Transport using the source.f • BME! • 10 MeV/amu to 100 MeV/amu • Hauser-Feshbach for compound nucleus? • Induced activity calculations • Neutron spectrometry using passive techniques • ECR ion sources • Simulate electric fields?
Electron Accelerators • Photon (Bremsstrahlung) spectrometry • High energy • Detector response studies • neutrons and photons • Photoneutron spectrometry and dosimetry • Synchrotron dosimetry • Low energy (< 10 keV)
Photoneutrons • Contribution to the exposure in electron accelerators • A new technique to predict the neutron spectra using empirical relations • Spectra from FLUKA fitted to a Maxwellian • Temperature • Yield • Form a couple equation to predict the GDR part of the photoneutron spectrum
The procedure Sunil C, Sarkar P K, “Empirical estimation of photoneutron energy distribution in high energy electron accelerators”, Nuclear Instruments and Methods A 581, (2007), 844-849.
Independent FLUKA Calculation Experiment Our Calculation
Neutrons > 50 MeV • Experimental verification using Bi fission foils, track etch membranes shows higher values when compared to FLUKA calculations. • How much is photon induced fission? • The cross section is 1% of neutron fission (>200 MeV) • But at the experimental area, the photon fluence is expected to be several times higher than neutrons! • Calculate photon induced fission using FLUKA?
Photon Transmission • 30 cm diameter and 30 cm long cylindrical detector (approximating the upper trunk of a human body) is used to count the photons. • USRTRACK estimator tallies the photon fluence. • Deq99 (FLUSUW) subroutine used to fold the fluence with the dose conversion coefficients to obtain ambient dose equivalent
Residual activity • 2.5 GeV electron incident on 10 X0 -1Xm targets. • DPMJET activated using PHYSICS • LAM-BIAS at 100 • Photon transport cut off to 10 MeV
Residual Nuclei • In SS, 51Cr was reported by Fasso with a higher neutron cutoff energy. • Swanson’s technique and present calculation agree within a factor of 2; for example 57Co in Ni target, 63, 65Cu from Cu target. • 59Fe in SS (58Fe(n,)) target in this calculation was found to be four orders less compared to that obtained by Sato and Fasso • Most of the important nuclides formed are in the range of 200 -500 MBqW-1.
Synchrotron Hutch Shielding • Hutch design in INDUS (2.5 GeV, 1 mA) • Bremsstrahlung mixed with SR • Experiments claim existence of SR • Transportation tough - low energy at the edge of FLUKA capabilities. • Can it be simulated using FLUKA?
Heavy Ion reactions • Work done at PTB Germany • 200 MeV 12C ions on water phantom • Score neutron fluence and dose inside 5.7 cm spheres at different angles. • Compare with measurements done at GSI • Spectra from TOF (GSI measurements) • Dose using a TEPC (PTB measurements) • Dose using WENDI (GSI measurements)
Neutron Spectra 200 MeV/amu 12C incident on 15 cm diameter cylindrical water phantom
Charged particles Apply coincidence measurements
Response Matrices • Neutron attenuation through a target of finite thickness. • Response of Bonner sphere type passive techniques. • Response of liquid scintillators • Bismuth fission detectors • Neutron induced fission • Photon induced fission
ADSS • A sub critical assembly driven by 14 MeV neutrons • 256 nat.U rods inside water column, beam tube at center. • Analog mode • 36 hours for 106 histories ! • And still large errors (10%-30%)
Proton accelerators for ADSS • Plans to couple a sub critical reactor to a proton accelerator • Source term for lateral shielding of the accelerator tunnel, reactor pool top • Residual activity in LBE loop • Activation of magnets concrete wall • LBE window rupture due to heat load
ADSS problems • High beam current ;1-5 mA! • Proton energies varying from 100 MeV to 1GeV • Shielding calculations • Reduce dose by 9 orders:- ~7 meters! • Induced activity after several meters of water • Explicit Transport !? Or calculate neutrons at intermediate thicknesses? • Induced activity in magnets, concrete walls. • Induced activity in LBE after several combinations of irradiations.
Shielding • Attenuation length from IAEA 283 • n/p ratio from FLUKA • Multiply end result by the n/p ratio to get the transmitted dose after shield • Biasing!
Simplified view concrete 7 m water Window
Further work • Establish attenuation curves for different shield configurations. • Different types of concrete • Transport neutrons through several meters of water and calculate induced activity. • Irradiation profile, raddecay, dcytimes, usrbin