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    L. Curchod

    EPFL, Physics, Graduate Student
    The unique flexibility of TCV in plasma shaping has been exploited to address different aspects of tokamak physics, for which the plasma shape may play a role. This paper summarizes the experiments undertaken in the TCV tokamak... more
    The unique flexibility of TCV in plasma shaping has been exploited to address different aspects of tokamak physics, for which the plasma shape may play a role. This paper summarizes the experiments undertaken in the TCV tokamak ("Tokamak à Configuration Variable") over the last decade essentially in stability and transport. This paper enables a comprehensive and integrated view of the
    The unique flexibility of TCV in plasma shaping has been exploited to address different aspects of tokamak physics, for which the plasma shape may play a role. This paper summarizes the experiments undertaken in the TCV tokamak... more
    The unique flexibility of TCV in plasma shaping has been exploited to address different aspects of tokamak physics, for which the plasma shape may play a role. This paper summarizes the experiments undertaken in the TCV tokamak ("Tokamak à Configuration Variable") over the last decade essentially in stability and transport. This paper enables a comprehensive and integrated view of the
    Scenarios with different electron cyclotron heating power profile distributions and widths were compared for the first time in experiments on the Tokamak `a Configuration Variable (TCV). The heating profile was changed from shot to shot... more
    Scenarios with different electron cyclotron heating power profile distributions and widths were compared for the first time in experiments on the Tokamak `a Configuration Variable (TCV). The heating profile was changed from shot to shot over a wide range from localized on-axis, with normalized minor radius half-width at half maximum σ1/2 ∼ 0.1, up to a widely distributed heating power profile with σ1/2 ∼ 0.4 and finally to a profile peaked far off-axis. The global confinement, MHD activity, density, temperature and electron pressure profile evolution were compared. In particular, the energy confinement properties of discharges with localized on-axis heating and distributed on-axis heating were very similar, with degradation close to that predicted by the ITER L-mode scaling; in the case of off-axis heating, on the other hand, the confinement degradation was even stronger.
    The first demonstration of electron-Bernstein-wave heating by double-mode conversion from the O to the X mode in an overdense H-mode tokamak plasma has been achieved in the Tokamak a Configuration Variable device. This technique overcomes... more
    The first demonstration of electron-Bernstein-wave heating by double-mode conversion from the O to the X mode in an overdense H-mode tokamak plasma has been achieved in the Tokamak a Configuration Variable device. This technique overcomes the upper density limit experienced by conventional microwave heating. The sensitive dependence of the O-X mode conversion on the microwave launching direction has been verified experimentally, and localized power deposition consistent with theoretical predictions has been observed at densities well above the conventional cutoff.