Recent experiments at JET aimed at producing (4)He ions in the MeV range through third harmonic ion cyclotron resonance heating (ICRH) acceleration of (4)He beams in a (4)He dominated plasma. MeV range D was also present through parasitic ICRH absorption on residual D. In this contribution, we analyze TOFOR neutron spectrometer data from these experiments. A consistent description of the data is obtained with d(d, n)(3) He and (9)Be(alpha, n)(12)C neutron components calculated using Stix distributions for the fast D and (4)He, taking finite Larmor radius effects into account and with a ICRH power partition of P(D)(RF) = 0.01 X P(4He)(RF), in agreement with TOMCAT simulations. (C) 2010 American Institute of Physics. [doi:10.1063/1.3502316]
Neutron spectrometry of JET discharges with ICRH-acceleration of helium beam ions
Gorini G;Nocente M;Tardocchi M;
2010
Abstract
Recent experiments at JET aimed at producing (4)He ions in the MeV range through third harmonic ion cyclotron resonance heating (ICRH) acceleration of (4)He beams in a (4)He dominated plasma. MeV range D was also present through parasitic ICRH absorption on residual D. In this contribution, we analyze TOFOR neutron spectrometer data from these experiments. A consistent description of the data is obtained with d(d, n)(3) He and (9)Be(alpha, n)(12)C neutron components calculated using Stix distributions for the fast D and (4)He, taking finite Larmor radius effects into account and with a ICRH power partition of P(D)(RF) = 0.01 X P(4He)(RF), in agreement with TOMCAT simulations. (C) 2010 American Institute of Physics. [doi:10.1063/1.3502316]| File | Dimensione | Formato | |
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