Abstract. The Lower Hybrid Current Drive (LHCD) system on Alcator C-Mod can produce spectra with a wide range of peak parallel refractive index (n || ). An experiment in which LH power is square-wave modulated on a time scale much faster than the current relaxation time does not significantly alter the poloidal magnetic field inside the plasma and thus allows for realistic modeling and consistent plasma conditions for different n || spectra. Boxcar binning of hard x-rays during LH power modulation allows for time resolution sufficient to resolve the build-up, steady-state, and slowing-down of fast electrons. A transport model built in Matlab has been used to determine a fast electron pinch velocity for a high-n || case of 1-2 m/s.
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LOWER HYBRID POWER MODULATION EXPERIMENTSIn order to control the location of LH-driven current, it is important to understand where in the plasma the LH power is deposited as well as the transport properties of the current-carrying fast electrons. To this end, there have been several studies of fast electron diffusion in LHCD tokamak plasmas 1,2 which have determined an upper bound on fast electron diffusion in the range of 0.2-2 m 2 /s. Recent experiments on Alcator C-Mod have revealed the build-up of a radial electric field in the core of the plasma during LHCD operation, 3,4 speculated to be caused by an inward pinch of LHdriven fast electrons.In this experiment, designed to measure transport properties of the LH-driven fast electrons, LH power was square-wave modulated with a 25 ms period and a 50% duty cycle. Bremsstralung radiation from the resulting fast electrons was measured with Alcator C-Mod's 32 spatial chord hard x-ray (HXR) camera.5 The camera's pulse trains are digitized and post-processed for flexible time and energy binning. The resulting HXR emission was boxcar binned in time for high signal-to-noise, high timeresolution x-ray time traces. This signal was Fourier decomposed, spatially inverted, and fit to a transport model to determine the magnitude of fast electron pinch velocity. Peak coupled LH power was approximately 400 kW. In the case analyzed in this paper, n || =3.1, n e =8.3×10 19 m -3 , T e0 =2.3 keV, and I p =800 kA.