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Program - Brookhaven National Laboratory

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The European Activation SYstem has been re-engineered and re-written in modern programming languages<br />

so as to answer today’s and tomorrow’s needs in terms of activation, transmutation, depletion, decay and<br />

processing of radioactive materials. The new FISPACT-II inventory code development project has allowed<br />

us to embed many more features in terms of energy range: up to GeV; incident particles: alpha, gamma,<br />

proton, deuteron and neutron; and neutron physics: self-shielding effects, temperature dependence and<br />

covariance, so as to cover all anticipated application needs: nuclear fission and fusion, accelerator physics,<br />

isotope production, stockpile and fuel cycle stewardship, materials characterization and life, and storage<br />

cycle management. In parallel, the maturity of modern, truly general purpose libraries encompassing<br />

thousands of target isotopes such as TENDL-2012, the evolution of the ENDF-6 format and the capabilities<br />

of the latest generation of processing codes PREPRO, NJOY and CALENDF have allowed the activation<br />

code to be fed with more robust, complete and appropriate data: cross sections with covariance, probability<br />

tables in the resonance ranges, kerma, dpa, gas and radionuclide production and 23 decay types. All such<br />

data for the five most important incident particles (n, p, d, α, γ) are placed in evaluated data files up<br />

to an incident energy of 200 MeV. The resulting code system, EASY-II(12) is designed as a functional<br />

replacement for the previous European Activation System, EASY-2010. It includes many new features<br />

and enhancements, but also benefits already from the feedback from extensive validation and verification<br />

activities performed with its predecessor. This work was funded by the RCUK Energy <strong>Program</strong>me under<br />

grant EP/I501045.<br />

PR 49<br />

’List-Mode’ Data Acquisition and Analysis for a Compton Suppression System<br />

R. Britton, P.H. Regan, Centre for Nuclear and Radiation Physics, Department of Physics, University of<br />

Surrey, Guildford, GU2 7XH, UK.<br />

Compton Suppression techniques have been widely used [1] to reduce the Minimum Detectable Activity<br />

(MDA) of various radionuclides when performing gamma spectroscopy of environmental samples. This is<br />

achieved by utilising multiple detectors to reduce the contribution of photons that Compton Scatter out<br />

the detector crystal, only partially depositing their energy. Photons that are Compton Scattered out of<br />

the primary detector are captured by a surrounding detector, and the corresponding events vetoed from<br />

the final dataset using coincidence based fast-timing electronics. The current work presents the use of<br />

a Lynx T M data acquisition module from Canberra UK (Harwell, Oxfordshire) to collect data in ‘List-<br />

Mode’ [2], where each event is time stamped for offline analysis. A post-processor developed to analyse<br />

such datasets [3] allows the optimisation of the coincidence delay, and then identifies and supresses events<br />

within this time window. This is the same process used in conventional systems with fast-timing electronics,<br />

however in the work presented, data can be re-analysed using multiple time and energy windows. All data<br />

is also preserved and recorded (in traditional systems, coincident events are lost as they are vetoed in real<br />

time), and the results are achieved with a greatly simplified experimental setup. Monte-Carlo simulations<br />

of Compton Suppression systems have been completed to support the optimisation work, and are also<br />

presented here. This work is supported by grants from the Engineering and Physical Sciences Research<br />

Council (EPSRC-UK).<br />

[1] Britton R (2011) J Radioanal Nucl Chem 292(1):33-39 [2] Burnett J, Davies A (2011) J Radioanal Nucl<br />

Chem 288(3):699-703 [3] Britton R (2012) J Radioanal Nucl Chem, DOI 10.1007/s10967-012-1811-1<br />

PR 50<br />

288

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