Abstract

A feasibility study of fusion reactors based on accelerators is carried out. We consider a novel scheme where a beam from the accelerator hits the target plasma on the resonance of the fusion reaction and establish characteristic criteria for a workable reactor. We consider the reactions , and in this study. The critical temperature of the plasma is determined from overcoming the stopping power of the beam with the fusion energy gain. The needed plasma lifetime is determined from the width of the resonance, the beam velocity and the plasma density. We estimate the critical beam flux by balancing the energy of fusion production against the plasma thermo-energy and the loss due to stopping power for the case of an inert plasma. The product of critical flux and plasma lifetime is independent of plasma density and has a weak dependence on temperature. Even though the critical temperatures for these reactions are lower than those for the thermonuclear reactors, the critical flux is in the range of for the plasma density in the case of an inert plasma. Several approaches to control the growth of the two-stream instability are discussed. We have also considered several scenarios for practical implementation which will require further studies. Finally, we consider the case where the injected beam at the resonance energy maintains the plasma temperature and prolongs its lifetime to reach a steady state. The equations for power balance and particle number conservation are given for this case.

Highlights

  • Peak resonance energy of the d + t reaction with a center of mass energy of 64 keV

  • In the straightforward approach to the accelerator based fusion reactor (ABFR), where the beam from the acceleator is used as the fuel, there can be insurmountable difficulties

  • Neutral beam shields long range Coulomb interaction, but the cross section for ionization, such as σ(H2 + He → H2 + H+e + e)|100 keV = 5 × 10−17 cm2 is 7 orders of magnitude larger than that of the fusion cross section, so that the energy loss due to ionization is much larger than the fusion energy gain

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Summary

Introduction

Peak resonance energy of the d + t reaction with a center of mass energy of 64 keV. The critical temperature of the plasma is determined from overcoming the stopping power of the beam with the fusion energy gain.

Results
Conclusion
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