Progress in the ITER Physics Basis
By K. Ikeda. 2007
707 citations recorded by the source corpus.
Subfields: Biomedical Engineering, Materials Chemistry, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/c8fdab8cf1f863722537d3bbdbdccd8e999993ba
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Citations in the corpus
- Disruption mitigation by massive gas injection in JET (2011, background): “In particular, the product of halo current fraction Ihalo/IP and toroidal peaking factor (TPF) has to be limited to ensure the integrity of ITER wall components [23].”
- Physics Design of CFETR: Determination of the Device Engineering Parameters (2014, methodology): “Principally, ITER physics [5], [6] could be applied as physic basis for CFETR conceptual design in combination with special requirements of CFETR.”
- Energetic particle physics in fusion research in preparation for burning plasma experiments (2014, methodology): “It is planned that set of radial and vertical neutron cameras will be installed on ITER to measure the 2D EP density profile [29].”
- Physics and technology considerations for the deuterium–tritium fuel cycle and conditions for tritium fuel self sufficiency (2020, methodology): “Total heating power (Ptot), H-mode threshold power (PL–H), minimum edge power ow compatible with high con nement assuming a margin of 25% above PL–H (Psep ) and corresponding maximum radiated power in the plasma core (Prad ) for ITER [50] and the EU DEMO 1 design [81].”
- Chapter 3: MHD stability, operational limits and disruptions (2007, methodology): “This has allowed, for example a quasi-stationary equilibrium with qmin > 1 to be maintained at βN ∼ 3 for over 6 s in DIII-D (see [241] and chapter 6 of this issue [2]).”