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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.
I. Yamada, K. Narihara, H. Funaba, T. Minami, H. Hayashi, T. Kohmoto, LHD Experiment Group
Fusion Science and Technology | Volume 58 | Number 1 | July-August 2010 | Pages 345-351
Chapter 8. Diagnostics | Special Issue on Large Helical Device (LHD) | doi.org/10.13182/FST10-A10820
Articles are hosted by Taylor and Francis Online.
The Large Helical Device (LHD) Thomson scattering system measures electron temperature and density profiles of LHD plasmas along the LHD major radius at a horizontally elongated section. The LHD Thomson scattering system has an oblique backward-scattering configuration. The number of observation points and typical spatial resolution are 144 and 17 mm, respectively. The temporal sampling frequency is 10 to 100 Hz. Measurable temperature and density ranges are Te = 5 eV to 20 keV and ne 1018 m-3 , respectively. The LHD Thomson scattering system consists of several subsystems: laser system, light collection optics, polychromators, and data acquisition system. In the past decade, we have continued our efforts to improve the performance and reliability of the LHD Thomson scattering system through extension of measurable temperature and density ranges, Raman and Rayleigh calibrations for absolute density measurements, new laser beam positioning system, and plasma light monitor system for increasing data reliability. In this paper, we describe the recent progress of the LHD Thomson scattering system in detail.
