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Qualification of the U.S. Conductors for ITER TF Magnet System
The U.S. Domestic Agency is one of the six suppliers of the toroidal field (TF) conductor for ITER. To qualify conductors per ITER requirements, we prepared or provided to the Swiss Plasma Center (SPC) eight test articles, sixteen conductors total, that were tested in the SULTAN facility at SPC in the ITER relevant conditions. The strands that were used in these SULTAN samples were fully characterized in the laboratories. In this paper, we report both test results and analysis of the conductors' performance against expected strand performance. The U.S. TF conductors showed a slightly better than average current sharing temperature and a relatively low sensitivity to warm up-cooldown cycles in comparison with other suppliers' conductors. However, the trend in current sharing temperature versus cycles and warm ups did not saturate, which means a continuing slow degradation of the conductor performance if the number of warm up and cooldown cycles will be significantly higher than expected. The ac losses in the U.S. TF conductors are in line with losses in the other TF conductor suppliers.
Fermiology and complex magnetism of RMn6Sn6 at high magnetic fields
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A Multi-Axial Time-Resolved Spectroscopic Technique for Magnetic Field, Electron Density, and Temperature Measurements in Dense Magnetized Plasmas, LO-001-16, Year 3 of 3
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Spectroscopic Studies of the Magnetic Excitation and Spin;#8208;Phonon Couplings in a Single;#8208;Molecule Magnet
Abstract not provided
Carbon deficiency-induced changes of structure and magnetism of Mn[subscript 3]SnC
Abstract not provided
Direct Detection of Pu-242 with a Metallic Magnetic Calorimeter Gamma-Ray Detector
Abstract not provided
Electron mass enhancement and magnetic phase separation near the Mott transition in double-layer ruthenates
Here, we present a detailed investigation of the specific heat of Ca 3 (Ru 1-x M x ) 2 O 7 (M = Ti, Fe, Mn) single crystals. Depending on the dopant and doping level, three distinct regions are present: a quasitwo-dimensional metallic state with antiferromagnetic (AFM) order formed by ferromagnetic bilayers (AFM-b), a Mott insulating state with G-type AFM order (G-AFM), and a localized state with a mixed AFM-b and G-AFM phase. Our specific heat data provide deep insights into the Mott transitions induced by Ti and Mn doping. We observed not only an anomalous large mass enhancement, but also an additional term in the specific heat, i.e., C ∝ T 2 , in the localized region. The C ∝ T 2 term is most likely due to long-wavelength excitations with both FM and AFM components. A decrease in the Debye temperature is observed in the G-type AFM region, indicating lattice softening associated with the Mott transition.
Magnetic and Nanostructured Materials from Lab to Fab: Chapter 12- Magnetically Doped Topological Insulator Thin Films
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Modern Permanent Magnets Chapter 10 Title: Critical materials for permanent magnets
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Architecture and magnetism of alnico
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Rapid-thermal-process pre-treatment promoted precipitation towards strengthening hard magnetism of Sm2Co17-type magnets
Not provided.
Tailoring structure and magnetic properties of NixCo1−x(N(CN)2)2 molecular magnets
Not Available
Searching for the nano effect in Cu-HCF (II) particles to improve Cs sorption efficiency: Highlighting the use of intrinsic magnetism
Not provided.