Search NASASearch

DOE OSTI · 3391613

Experimental observation and integrated modelling of proton-beryllium fusion in He and D plasmas at JET

Štancar, Žiga [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Eriksson, J. [Uppsala University (Sweden)]·Oliver, H.J.C. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Kiptily, V.G. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Conroy, S. [Uppsala University (Sweden)]·Čufar, A. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)]·Hjalmarsson, A. [Uppsala University (Sweden)]·Kazakov, Ye.O. [Ecole Royale Militaire, Brussels (Belgium)]·Ghani, Z. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Gorelenkova, M. [Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)] (ORCID:0000000184871396)·Boboc, A. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Carvalho, P. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Chomiczewska, A. [Institute of Plasma Physics and Laser Microfusion (IPPLM) Warsaw (Poland)]·Delabie, E. [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)]·Dreval, M. [Kharkiv Institute of Physics and Technology (KIPT) (Ukraine)]·Garzotti, L. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Kirov, K. K. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Kos, D. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Lawson, K. D. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Lengar, I. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)]·Lennholm, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Lerche, E. [Ecole Royale Militaire, Brussels (Belgium)]·Litaudon, X. [Alternative Energies and Atomic Energy Commission (CEA), Cadarache (France)]·Litherland-Smith, E. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Maslov, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Menmuir, S. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·O’Mullane, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Parr, E. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Patel, A. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Snoj, L. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)]·Sydenham, R. [University of Portsmouth (United Kingdom)]·Sun, H. J. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)]·Villari, R. [ENEA Frascati Research Center (Italy)]·Wang, V. T. [Queen Mary University of London (United Kingdom)]·Zotta, V. K. [Sapienza University of Rome (Italy)]

Abstract

Validated integrated modelling of JET ITER-like wall experiments in which fusion performance is driven by reactions between fast ions and intrinsically present metal wall impurities is presented. A steady-state L-mode plasma with dominant proton-beryllium fusion and neutron yields of up to ≈ 6·10 13 s -1 is developed in He and D, via radiofrequency heating of a H minority. The fusion drive is unambiguously confirmed by the neutral particle analyser, fast ion loss detector, and γ-ray diagnostics. Experiments are analysed via an integrated modelling framework, developed to model the two-stage proton beryllium-fusion chain and produce high-fidelity fusion product source terms. The modelling chain comprises TRANSP and JETTO for plasma core modelling, LOCUST for full orbit product tracking and collisional slowing-down, DRESS to resolve two- and three-body fusion kinematics, and MCNP for neutron transport calculations. Modelling shows that the primary 9 Be(p,n) 9 B reaction is the dominant neutron emitter at naturally present concentrations of beryllium in these experiments. The yield contribution of secondary reactions between fusion products and beryllium, 9 Be(d,n) 10 B and 9 Be(α,n) 12 C, is found to be negligible. The proton-deuteron knock-on effect in D plasmas is modelled, which is calculated to contribute ≈ 25% to the total neutron yield. For both He and D discharges the total computed neutron rates match fission chamber (FC) measurements within the combined experimental and computational uncertainty, with an average discrepancy of ≈ ± 20%. Realistic proton-beryllium neutron sources are propagated through JET’s MCNP neutron transport model which shows that 235 U FCs’ response is sensitive to p–Be source changes, with up to ≈ 10% variation compared to a D–D neutron source. We show that the high-energy tail of the fast proton minority can be studied with multi-foil neutron activation. The framework is also applied to the study of interactions between fast protons and boron impurities, of relevance to ITER. We calculate that in JET conditions a significant alpha source with DT-like energies could be generated through 11 B(p, α)2α fusion, and detected via γ-emission in secondary interactions between fast alphas and boron. The work represents an important step towards validating predictive integrated modelling capabilities for non-standard fusion reactions.

Explore related subjects

Keep this discovery

BibTeXRIS

Štancar, Žiga [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Eriksson, J. [Uppsala University (Sweden)], Oliver, H.J.C. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Kiptily, V.G. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Conroy, S. [Uppsala University (Sweden)], Čufar, A. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)], Hjalmarsson, A. [Uppsala University (Sweden)], Kazakov, Ye.O. [Ecole Royale Militaire, Brussels (Belgium)], Ghani, Z. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Gorelenkova, M. [Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)] (ORCID:0000000184871396), Boboc, A. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Carvalho, P. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Chomiczewska, A. [Institute of Plasma Physics and Laser Microfusion (IPPLM) Warsaw (Poland)], Delabie, E. [Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)], Dreval, M. [Kharkiv Institute of Physics and Technology (KIPT) (Ukraine)], Garzotti, L. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Kirov, K. K. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Kos, D. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Lawson, K. D. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Lengar, I. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)], Lennholm, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Lerche, E. [Ecole Royale Militaire, Brussels (Belgium)], Litaudon, X. [Alternative Energies and Atomic Energy Commission (CEA), Cadarache (France)], Litherland-Smith, E. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Maslov, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Menmuir, S. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], O’Mullane, M. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Parr, E. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Patel, A. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Snoj, L. [Jozef Stefan Institute (IJS), Ljubljana (Slovenia)], Sydenham, R. [University of Portsmouth (United Kingdom)], Sun, H. J. [United Kingdom Atomic Energy Authority (UKAEA), Abingdon (United Kingdom)], Villari, R. [ENEA Frascati Research Center (Italy)], Wang, V. T. [Queen Mary University of London (United Kingdom)], Zotta, V. K. [Sapienza University of Rome (Italy)]. 2026-07-21. Experimental observation and integrated modelling of proton-beryllium fusion in He and D plasmas at JET. https://doi.org/10.1088/1741-4326/ae870b

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related discoveries

Integrated Neutronics Modeling for Inertial Fusion Energy Systems: Development and Application to LD-FIRST

Lawrence Livermore National Laboratory (LLNL) is proposing a new Laser Driven Fusion Integration Research and Science Test Facility (LD-FIRST) with the goal of providing an experimental testbed for future Inertial Fusion Energy (IFE) systems. However, IFE systems require detailed and accurate multiphysics modeling to quantify material damage, thermal loading, and tritium breeding within complex chamber environments. This article presents the first step in an integrated multiphysics framework that couples meshed CAD-based geometry within Monte Carlo neutronic simulations to enable high-fidelity analysis of IFE chamber concepts, with future coupling to external codes. The neutronics workflow utilizes OpenMC and its third-party capability to use CAD-based geometries through DAGMC and tally on unstructured meshes with Libmesh to evaluate neutron transport behavior, geometric fidelity, and material performance under reactor-relevant conditions. The use of tailored tallies on unstructured meshes in this framework allows direct transfer without interpolating to CFD simulation tools. Two IFE chambers were evaluated, both conceived by LLNL: HYLIFE-II and Laser IFE (LIFE). This work produced high-fidelity conformal surface and volumetric meshes of the HYLIFE-II and LIFE chambers with mapped spatial insight into material damage, thermal loading, and tritium breeding. The HYLIFE-II model was built utilizing available resources and used as a test case to verify that the neutronics framework can handle complex geometries. The LIFE chamber CAD was provided by LLNL and was the main focus of this work. This work analyzes multiple ternary alloy breeding materials for the LIFE chamber, across different 6 Li enrichments to produce data relevant to the LD-FIRST project. This work also investigates the level of model fidelity for the LIFE chamber, and results show that inclusion of detailed first wall and coolant structures increased the predicted tritium breeding ratio (TBR) by ~30%, highlighting the sensitivity of tritium breeding and the need for a high-fidelity simulation framework for IFE chambers. These developments provide a scalable toolset for the design and optimization of next-generation IFE chambers, forming a solid foundation for future coupled multiphysics analysis.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY

Extending mARC II Arc-Jet Test Duration via Design and Implementation of Model System Cooling Sleeve

The mARC II is a 30 kW arc-jet facility at NASA Ames Research Center used to generate high-enthalpy flows for low-cost thermal protection system (TPS) technology development. Sustained operation of downstream instrumentation and material samples is constrained by thermal loading transmitted through the arc-jet test environment, limiting achievable run times and experimental throughput. This work presents the design, integration, and validation of a cooling sleeve implemented on the sweep arm drive motor feedthrough to mitigate thermal accumulation during testing. The addition of the cooling sleeve is a simple, robust upgrade that translates directly into enhanced facility capability by supporting longer run durations, reduced turnaround time, and higher throughput.

numerical simulations

Comparing Thermal Neutron Scintillators for Use With SiPM-Readout Detectors

Scintillator-based thermal neutron detectors for scientific scattering facilities offer an effective combination of large-area coverage and good spatial resolution. At Oak Ridge National Laboratory, silicon photomultiplier (SiPM)-readout Anger cameras using 6 Li glass scintillators have been developed, but the spatial resolution of these detectors is limited by the relatively low light yield of the glass. Recently, several brighter scintillator compositions with sufficient 6 Li concentration have emerged as promising candidates for higher-resolution imaging. Here, in this work, we evaluate five scintillator materials: GS20, LiF/ZnS:Ag, LiF/ZnO:Zn, LiI:Eu, and Cs 2 LiYCl 6 :Ce, each mounted on a SiPM Anger camera. For each scintillator, the neutron detection efficiency, spatial resolution, and count rate capabilities were measured and compared. Each of the new compositions achieved a spatial resolution better than 0.5 mm, compared to 0.66 mm for GS20, with LiI:Eu reaching the best value of 0.32 mm. Although these compositions improve the spatial resolution of the Anger camera, their longer pulse decay times limit their use in high count rate applications, and the camera’s hardware must be optimized for the different properties of the new scintillators.

Neutron detectors