2 research outputs found
Tuning of Photoluminescence by Cation Nanosegregation in the (CaMg)<sub><i>x</i></sub>(NaSc)<sub>1–<i>x</i></sub>Si<sub>2</sub>O<sub>6</sub> Solid Solution
Controlled
photoluminescence tuning is important for the optimization
and modification of phosphor materials. Herein we report an isostructural
solid solution of (CaMg)<sub><i>x</i></sub>(NaSc)<sub>1–<i>x</i></sub>Si<sub>2</sub>O<sub>6</sub> (0 < <i>x</i> < 1) in which cation nanosegregation leads to the presence of
two dilute Eu<sup>2+</sup> centers. The distinct nanodomains of isostructural
(CaMg)ÂSi<sub>2</sub>O<sub>6</sub> and (NaSc)ÂSi<sub>2</sub>O<sub>6</sub> contain a proportional number of Eu<sup>2+</sup> ions with unique,
independent spectroscopic signatures. Density functional theory calculations
provided a theoretical understanding of the nanosegregation and indicated
that the homogeneous solid solution is energetically unstable. It
is shown that nanosegregation allows predictive control of color rendering
and therefore provides a new method of phosphor development
Real-Space Observation of Nonvolatile Zero-Field Biskyrmion Lattice Generation in MnNiGa Magnet
Magnetic
skyrmions, particular those without the support of external
magnetic fields over a wide temperature region, are promising as alternative
spintronic units to overcome the fundamental size limitation of conventional
magnetic bits. In this study, we use in situ Lorentz microscope to
directly demonstrate the generation and sustainability of robust biskyrmion
lattice at zero magnetic field over a wide temperature range of 16–338
K in MnNiGa alloy. This procedure includes a simple field-cooling
manipulation from 360 K (higher than Curie temperature <i>T</i><sub>C</sub> ∼ 350 K), where topological transition easily
occurs by adapting the short-range magnetic clusters under a certain
magnetic field. The biskyrmion phase is favored upon cooling below <i>T</i><sub>C</sub>. Once they are generated, the robust high-density
biskyrmions persist even after removing the external magnetic field
due to the topological protection and the increased energy barrier