By Ashutosh Tiwari, Parameswar K. Iyer, Vijay Kumar, Hendrik Swart
Advanced Magnetic and OpticalMaterials deals targeted updated chapters at the practical optical and magnetic fabrics, engineering of quantum buildings, high-tech magnets, characterization and new applications. It brings jointly cutting edge methodologies and methods followed within the study and improvement of the topic and the entire members are tested experts within the examine region. The 14 chapters are equipped in parts:
Part 1: Magnetic Materials
- Magnetic Heterostructures and superconducting order
- Magnetic Antiresonance in nanocomposites
- Magnetic bioactive glass-ceramics for bone therapeutic and hyperthermic therapy of reliable tumors
- Magnetic iron oxide nanoparticles
- Magnetic nanomaterial-based anticancer therapy
- Theoretical learn of strained carbon-based nanobelts: Structural, energetical, digital, and magnetic properties
- Room temperature molecular magnets – Modeling and applications
Part 2: Optical Materials
- Advances and way forward for white LED phosphors for solid-state lighting
- Design of luminescent fabrics with “Turn-on/off” reaction for anions and cations
- Recent developments in luminescent fabrics and their power applications
- Strongly constrained quantum dots: Emission restricting, photonic doping, and magneto-optical effects
- Microstructure characterization of a few quantum dots synthesized via mechanical alloying
- Advances in useful luminescent fabrics and phosphors
- Development in natural mild emitting fabrics and their capability applications
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Extra info for Advanced magnetic and optical materials
The inverse spin Hall effect causes scattering of the injected spin current and converts it to charge current, which below Tc is carried by quasiparticles. The electrical signatures of the inverse spin Hall effect thus manifest as a charge imbalance at the edges of the sample . Spin injection in conventional spintronics typically occurs as above, through diffusion of spins across a ferromagnet/non-ferromagnet interface. At a superconducting interface, a range of novel phenomena have been shown when spin-polarized currents are injected into superconductors, Superconducting Order in Magnetic Heterostructures 29 such as quasiparticle spin lifetimes close to one million times longer than the normal-state lifetime , which is a result of the unique properties of quasiparticles in superconductors.
Spin-polarized interfaces, multiple magnetic layers and conical-field magnets such as holmium (Ho), and enables the generation of triplet superconductivity from the wide variety of available singlet superconductors. The conversion from singlet pairing to spin-polarized triplet pairing can be understood as a two-step process. In the first step, spin-mixing  occurs from for instance spin-dependent scattering at interfaces . This generates the zero spin triplet projection which then coexists with the singlet component.
In agreement with theoretical prediction, it closes entirely at = π . When the material is magnetic, the oscillating order parameter leads to a corresponding oscillation in the density of states as a function of the penetration distance into the ferromagnet due to the alternating dominance of singlet and triplet pairing [64, 72]. The density of states in the ferromagnet is inverted compared with SN structures when the superconducting order parameter is negative (called the -phase) and triplet pairings dominate.
Advanced magnetic and optical materials by Ashutosh Tiwari, Parameswar K. Iyer, Vijay Kumar, Hendrik Swart