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Senate committee advances NRC nominee Matthew Marzano
Marzano
The U.S. Senate Environment and Public Works Committee voted 10–9 last week to advance the nomination of Matthew Marzano to serve on the Nuclear Regulatory Commission. It was a party-line vote, with all Democrats supporting Marzano and all Republicans voting “no.”
Marzano was nominated by President Biden in July to fill the open NRC seat, and the EPW Committee held a hearing in September on his nomination. His nomination will now go to the Senate for a vote, but it is not certain whether that will happen before the end of the year, in which case his nomination process would start over in 2025.
The five-member commission has been without a tiebreaker vote since June 2023 when Jeff Baran’s term expired.
O. Kaneko, Y. Takeiri, K. Tsumori, M. Osakabe, K. Ikeda, K. Nagaoka, H. Nakano, LHD Experiment Group
Fusion Science and Technology | Volume 58 | Number 1 | July-August 2010 | Pages 497-503
Chapter 9. Neutral Beam Interaction | Special Issue on Large Helical Device (LHD) | doi.org/10.13182/FST10-A10836
Articles are hosted by Taylor and Francis Online.
A unique and reliable method of plasma initiation has been established in the Large Helical Device (LHD) by using neutral beam (NB) injection into vacuum. Since LHD is a superconducting machine, the confining magnetic field exists unrelated to plasma. Under these circumstances it is demonstrated that the NB can initiate plasma by itself. A small fraction of injected NB is ionized by collision with the background neutral gas and is confined by the magnetic field. Although these high-energy ions are lost quickly by charge exchange, they work as the energy source for ionizing the background neutral particles and heating the produced plasma. As a result, very thin but hot "seed" plasma is generated, which ionizes puffed gas and makes dense target plasma that is sufficient for NB absorption. This process is simulated numerically and the results agree well with the experimental observations for both absolute values and temporal behavior of plasma parameters. The method does not depend on magnetic field strength strongly, and plasma can be initiated at the magnetic field strength as low as 0.4 T, although standard field strength of LHD is 2.75 T. The progress of high-beta studies in LHD owes this plasma production method much.