Conversion of Magnetic Energy to Plasma Kinetic Energy During Guide Field Magnetic Reconnection in the Laboratory.

We present laboratory measurements showing the two-dimensional (2D) structure of energy conversion during magnetic reconnection with a guide field over the electron and ion diffusion regions, resolving the separate energy deposition on electrons and ions. We find that the electrons are energized by the parallel electric field at two locations, at the X line and around the separatrices. On the other hand, the ions are energized ballistically by the perpendicular electric field in the vicinity of the high-density separatrices. An energy balance calculation by evaluating the terms of the Poynting theorem shows that 40% of the magnetic energy is converted to particle energy, 2/3 of which is transferred to ions and 1/3 to electrons. Further analysis suggests that the energy deposited on particles manifests mostly in the form of thermal kinetic energy in the diffusion regions.

Anomalous Resistivity and Electron Heating by Lower Hybrid Drift Waves during Magnetic Reconnection with a Guide Field.

The lower hybrid drift wave (LHDW) has been a candidate for anomalous resistivity and electron heating inside the electron diffusion region of magnetic reconnection. In a laboratory reconnection layer with a finite guide field, quasielectrostatic LHDW (ES-LHDW) propagating along the direction nearly perpendicular to the local magnetic field is excited in the electron diffusion region. ES-LHDW generates large density fluctuations (δn_{e}, about 25% of the mean density) that are correlated with fluctuations in the out-of-plane electric field (δE_{Y}, about twice larger than the mean reconnection electric field). With a small phase difference (∼30°) between two fluctuating quantities, the anomalous resistivity associated with the observed ES-LHDW is twice larger than the classical resistivity and accounts for 20% of the mean reconnection electric field. After we verify the linear relationship between δn_{e} and δE_{Y}, anomalous electron heating by LHDW is estimated by a quasilinear analysis. The estimated electron heating is about 2.6±0.3 MW/m^{3}, which exceeds the classical Ohmic heating of about 2.0±0.2 MW/m^{3}. This LHDW-driven heating is consistent with the observed trend of higher electron temperatures when the wave amplitude is larger. Presented results provide the first direct estimate of anomalous resistivity and electron heating power by LHDW, which demonstrates the importance of wave-particle interactions in magnetic reconnection.

Two-dimensional plasma density evolution local to the inversion layer during sawtooth crash events using beam emission spectroscopy.

We present methods for analyzing Beam Emission Spectroscopy (BES) data to obtain the plasma density evolution associated with rapid sawtooth crash events at the DIII-D tokamak. BES allows coverage over a 2D spatial plane, inherently local measurements, with fast time responses, and, therefore, provides a valuable new channel for data during sawtooth events. A method is developed to remove sawtooth-induced edge-light pulses contained in the BES data. The edge light pulses appear to be from the Dα emission produced by edge recycling during sawtooth events, and are large enough that traditional spectroscopic filtering and data analysis techniques are insufficient to deduce physically meaningful quantities. A cross-calibration of 64 BES channels is performed by using a novel method to ensure accurate measurements. For the large-amplitude density oscillations observed, we discuss and use the non-linear relationship between the BES signal δI/I0 and the plasma density variation δne/ne0. The 2D BES images cover an 8 × 20 cm2 region around the sawtooth inversion layer and show large-amplitude density oscillations, with additional significant spatial variations across the inversion layer that grows and peaks near the time of the temperature crash. The edge light removal technique and method of converting large-amplitude δI/I0 to δne/ne0 presented here may help analyze other impulsive MHD phenomena in tokamaks.

Inverse mirror plasma experimental device­A new magnetized linear plasma device with wide operating range.

Inverse mirror plasma experimental device has been designed and fabricated for detailed experimental investigation of phase mixing and wave breaking of plasma oscillation/wave. The device produces quiescent magnetized plasma over a wide operating range using multifilamentary source with low filament spacing in cusp geometry along with a flexible transition magnetic field region between the plasma source chamber and the main chamber. Argon plasma has been produced in the device over a wide pressure range from 1.7 × 10(-5) mbar to 9 × 10(-4) mbar, achieving plasma densities in the range of ∼10(9) cm(-3)-10(12) cm(-3) and temperatures in the range of ∼1.7 eV-5 eV. To fulfill a desired prerequisite of having quiescent plasma (δn/n ≤ 1%) for realizing phase mixing of nonlinear plasma oscillation and other wave experiments, a quiescent magnetized plasma is obtained: typical quiescence, δn/n ∼ 0.5% at 10(-4) mbar and B(main) ∼ 1 kG. The potential of the multifilamentary plasma source has been experimentally explored using a flexible transition magnetic field and the usual control features of a filament discharge. Probe measurements reveal that the plasma to be axially and radially uniform, an excellent scenario for wave launching and studying its propagating and phase mixing characteristics.