By Ashutosh Tiwari, Parameswar K. Iyer, Vijay Kumar, Hendrik Swart
Advanced Magnetic and OpticalMaterials bargains exact updated chapters at the useful optical and magnetic fabrics, engineering of quantum constructions, high-tech magnets, characterization and new applications. It brings jointly cutting edge methodologies and techniques followed within the study and improvement of the topic and all of the members are confirmed experts within the examine region. The 14 chapters are geared up 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 capability applications
- Strongly restricted quantum dots: Emission proscribing, photonic doping, and magneto-optical effects
- Microstructure characterization of a few quantum dots synthesized through mechanical alloying
- Advances in useful luminescent fabrics and phosphors
- Development in natural mild emitting fabrics and their capability applications
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Extra resources for Advanced magnetic and optical materials
3 Theoretical Framework One theoretical approach to examining heterostructures that combine superconducting and ferromagnetic materials is the Bogoliubov–de Gennes formalism . 3) where H0 is the Hamiltonian of a single electron, including both kinetic energy and all non-superconducting interactions; e and h are complex wave functions that describe electron-like and hole-like excitations respectively; E is the energy of the excitations; denotes complex conjugation; and Δ(x) is a complex field that describes superconductivity.
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.
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. Whenever the Thouless energy is much greater than the exchange field strength one expects to see a spectroscopic minigap, which closes when the resonant condition h ~ Eg is fulfilled, where Eg is the zero-field minigap [73, 74]. Beyond this a zero-energy peak emerges until the field strength overcomes all correlations and the density of states becomes essentially featureless .