The JET activation system has eight irradiation ends where samples may be i
rradiated in the neutron flux from the plasma. There is one end, re-entrant
into the top of the vessel, for which there is little intervening material
between it and the plasma; the other ends, including two beneath the diver
tor coils, have increasingly larger amounts of intervening structure. The l
ocal neutron spectrum at each irradiation end was measured by simultaneousl
y activating several elemental foils (Al, Au, Co, Fe, In, Mg, Nb, Ni, Ti, Z
r). There were 15 activation reactions in the energy range of 0.5-16 MeV wh
ich were used as input to the SNL-SAND-II code to determine the neutron ene
rgy spectrum. The results are compared with neutron transport calculations
both from the MCNP and FURNACE codes: the average standard deviation betwee
n measured to SNL-SAND-II calculated activity ratios was as low as 5%. The
results demonstrate the reliability of the neutronics calculations and have
implications for the design of diagnostics and blankets for the next gener
ation of large tokamaks such as ITER. The 377.9 keV line of the Fe-54(n, 2n
)Fe-53 reaction (threshold similar to 13.9 MeV, not a dosimetric standard)
has also been measured in different plasma conditions. The ratio of the sat
urated activity from this reaction to that from the Fe-56( n, p)Mn-56 react
ion (threshold similar to 4.5 MeV) provides information on the broadening o
f the 14 MeV fusion peak. (C) 1999 American Institute of Physics. [S0034-67
48(99)56401-0].