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In transition: Commercializing fusion power
Commercial fusion power is closer than ever. There are now around 30 U.S. fusion companies, several of which claim to be on track to connect to the grid as early as the 2030s.
Tokamak and laser inertial confinement approaches benefit from decades of research at facilities such as the National Ignition Facility (NIF) at Lawrence Livermore National Laboratory and ITER, with alternative concepts including stellarator, magnetic mirror, and Z-pinch confinement also making notable progress as private and government funding for fusion increases.
R. W. Stoughton, J. Halperin, C. E. Bemis, H. W. Schmitt
Nuclear Science and Engineering | Volume 50 | Number 2 | February 1973 | Pages 169-171
Technical Note | doi.org/10.13182/NSE73-A23241
Articles are hosted by Taylor and Francis Online.
The neutron multiplicities P(n) in the spontaneous fission of 246Cm, 248Cm, and 252Cf have been measured in a 3He neutron counter assembly. The efficiency ∈ for detection of a single neutron was measured to be 0.360, based on (average number of neutrons per fission) = 3.73 for 252Cf spontaneous fission. Using this value of ∈ and assuming a Gaussian distribution p(v) for the emitted neutrons, we fitted our observed P(n), corrected for small background and pile-up effects, to the model by the method of least squares in which the Gaussian width σv and were the parameters of fit. Values of p(v) were then calculated from the resulting Gaussian function. In the case of 252Cf, our values of p(v) agree well with literature values; the p(v) values for the curium isotopes have not been measured previously as far as we know. The values of for both 246 Cm and 248Cm fall on a straight line through existing experimental values for the nuclides 242Cm, 244Cm, and 250Cm in a plot of versus mass number; our values were 2.86 ± 0.06 and 3.14 ± 0.06 for 246Cm and 248Cm, respectively.