“…Similarly, the emission peaks excited by an exciting light at 397 nm are the characteristic emissions of Eu 3+ ions, and they are assigned to the high-energy transition 5 D 2 → 7 F 3 at 515 nm and 5 D 1 → 7 F J (J = 0–2) at 530 nm, 541 nm, and 561 nm; low-energy transition 5 D 0 → 7 F J (J = 1–4) at 598 nm, 622 nm, 657 nm, and 702 nm, respectively [8,35]. The weaker emission peak at 598 nm corresponding to 5 D 0 → 7 F 1 is allowed by the magnetic dipole transitions due to Eu 3+ ions, located at a site with inversion symmetry, while the stronger emission peak at 622 nm, corresponding to 5 D 0 → 7 F 2 , is allowed by the electric dipole transitions that are a result of absence of inversion symmetry at the Eu 3+ lattice site [36,37,38,39].…”