TANAKA, Kenji

No ORCID on file · 74 papers in corpus · active 2024-2025

Study types

  • dataset 74
dataset 2025
·doi:10.57451/lhd.ctsfosc1.171957.1

A collective Thomson scattering (CTS) diagnostic with a ±3 GHz band around a 77 GHz gyrotron probe beam is to measure the velocity distribution of bulk and fast ions in high-temperature plasmas.

dataset 2025
·doi:10.57451/lhd.ctsfosc1.194921.1

A collective Thomson scattering (CTS) diagnostic with a ±3 GHz band around a 77 GHz gyrotron probe beam is to measure the velocity distribution of bulk and fast ions in high-temperature plasmas.

dataset 2025
·doi:10.57451/lhd.ctsfosc2.194700.1

A collective Thomson scattering (CTS) diagnostic with a ±3 GHz band around a 77 GHz gyrotron probe beam is to measure the velocity distribution of bulk and fast ions in high-temperature plasmas.

dataset 2025
·doi:10.57451/lhd.divtc3.131052.42

Divertor thermometers by using thermocouples (TCs) for divertor heat flux and temperature response analyses

dataset 2025
·doi:10.57451/lhd.divtc3.131059.217

Divertor thermometers by using thermocouples (TCs) for divertor heat flux and temperature response analyses

dataset 2025
·doi:10.57451/lhd.divtc3.164159.1

Divertor thermometers by using thermocouples (TCs) for divertor heat flux and temperature response analyses

dataset 2025
·doi:10.57451/lhd.divtc3.194653.1

Divertor thermometers by using thermocouples (TCs) for divertor heat flux and temperature response analyses

dataset 2025
·doi:10.57451/lhd.divtc3.939391.1

Divertor thermometers by using thermocouples (TCs) for divertor heat flux and temperature response analyses

dataset 2025
·doi:10.57451/lhd.fir2.194676.1

FIR laser interferometer measures the line averaged electron density and the electron density profile. Laser source: CH3OH laser (119um, 100mW) Michelson & Heterodyne interferometer (beat freq. 1 MHz). Time resolution: 10us.

dataset 2025
·doi:10.57451/lhd.firana.99330.1

Line integrated electron density (neL) and its profile calculated from raw data of FIR laser interferometers, FIR1, FIR2, and FIR3. Time resolution is basically 10 milli-second, and the time axis array is stored in the last, i.e. 14th chann…

dataset 2025
·doi:10.57451/lhd.a.firc.129531.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.134615.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.154760.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.16417.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.179909.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.38618.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.74622.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.8510.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.firc.97039.1

Line-integrated electron density at the central chord measured by FIR laser interferometer.

dataset 2025
·doi:10.57451/lhd.a.fir_fj.150946.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…

dataset 2025
·doi:10.57451/lhd.a.fir_fj.155673.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…

dataset 2025
·doi:10.57451/lhd.a.fir_fj.161386.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…

dataset 2025
·doi:10.57451/lhd.a.fir_fj.170390.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…

dataset 2025
·doi:10.57451/lhd.a.fir_fj.178026.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…

dataset 2025
·doi:10.57451/lhd.a.fir_fj.51851.1

The timing of the first fringe jump in the far-infrared (FIR) laser interferometer. When the phase change suddenly jumpes by more than one fringe (2π), the interferometer can no longer continuously track the phase shift value, and this phen…