In 1957 John Lawson at Harwell pointed out a crucial minimum requirement for the achievement of net power output from a deuterium–tritium plasma in any fusion device. No matter what the temperature, Lawson showed, a thermalized D–T plasma cannot put out more fusion power than the input power required to keep it hot unless the product of the ion density and the energy confinement time (often refered to as the confinement parameter or Lawson parameter), exceeds
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© 1984 American Institute of Physics.
1984
American Institute of Physics
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