28 September 2026 to 2 October 2026
Lausanne, Switzerland
Europe/Paris timezone
Please register to the meeting through the LOC website: https://tmep26.epfl.ch/

Consistent workflow for evaluating beam-target fusion rate with the orbit-following code ASCOT5

Not scheduled
20m
Beaulieu Congress and Exhibition Center (Lausanne, Switzerland)

Beaulieu Congress and Exhibition Center

Lausanne, Switzerland

Local website: https://tmep26.epfl.ch/
Poster Poster session I

Speaker

Joona Sissonen

Description

Volumetric neutron sources (VNS) are being developed to produce 14 MeV DT neutrons for fusion materials testing. To limit the size and cost of such VNS, beam-driven systems utilising beam-target fusion reactions are widely studied [1]. Accurate prediction of the beam-target fusion rate is therefore essential for VNS design. Beam-target fusion rates are typically evaluated by first calculating the beam ionisation distribution, then following the ions as they slow down, and finally combining the resulting fast-ion density with the background plasma to obtain the fusion rate. This workflow neglects the depletion of fast ions by fusion reactions during slowing down, causing the steady-state fast-ion distribution—and consequently the fusion rate—to be systematically overestimated.

We implement a self-consistent treatment in ASCOT5 [2] by reducing marker weights at each time step according to the local fusion probability. This accounts for the loss of ions due to fusion during the slowing-down simulation. For a representative VNS spherical tokamak case with 150 keV NBI tritium, neglecting fusion depletion overestimates the fusion power by 0.2% and the steady-state fast-ion density by 0.3%. The latter error propagates into various moments that can be evaluated from the distribution, for instance, the power deposition.

The discrepancy increases with slowing-down time because ions have more opportunity to undergo fusion. In a homogeneous 20 keV plasma with 1 MeV deuterium ions, neglecting fusion depletion overestimates the fusion rate by 1.8%, while the total steady-state fast-ion probability mass differs by 1.5%. These results not only facilitate accounting for the fusion depletion in numerical calculations but also demonstrate the parameter space where such effects could potentially make a significant difference.

[1] C. Bachmann et al., ‘Progress in the concept development of the VNS—a beam-driven tokamak for component testing’, Nucl. Fusion, vol. 66, no. 4, p. 046015, Mar. 2026, doi: 10.1088/1741-4326/ae4e46.

[2] K. Särkimäki, ‘ASCOT5 5.6.3 documentation’. Accessed: May 27, 2026. [Online]. Available: https://ascot4fusion.github.io/ascot5/index.html

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