Luminescence Tuning, Thermal Quenching, and Electronic Structure of Narrow-Band Red-Emitting Nitride Phosphors

2017 ◽  
Vol 56 (19) ◽  
pp. 11837-11844 ◽  
Author(s):  
Dianpeng Cui ◽  
Zhen Song ◽  
Zhiguo Xia ◽  
Quanlin Liu
1993 ◽  
Vol 07 (22) ◽  
pp. 1449-1456
Author(s):  
G. A. R. LIMA ◽  
VITOR TORRES ◽  
A. FAZZIO

The electronic structure of the CuO chain and the CuO 2 plane in the superconductor YBa 2 Cu 3 O 7−δ doped with 3dn transition-metal (TM) atoms are investigated. The calculations were performed through the semiempirical INDO/S technique, where the correlation effects are taken into account by the Configuration Interaction (CI) procedure. We also calculated, for all 3dn impurities, the Hubbard parameters Udd corresponding to a narrow band. The results obtained demonstrate clear chemical trends in the electronic structure of the 3d's, from Ti to Ni, when they substitute Cu(1) and Cu(2) sites; the hybridization decreases when the atomic number Z decreases. Our work provides a picture which is important to understand the change in T c when the host is doped with TM atom.


2019 ◽  
Vol 7 (13) ◽  
pp. 3730-3734 ◽  
Author(s):  
Chao Li ◽  
Xiao-Ming Wang ◽  
Feng-Feng Chi ◽  
Zu-Pei Yang ◽  
Huan Jiao

Ca8Mg7Si9N22 crystallizes in a tetragonal space group P42/nmc (No. 137) with a unit cell of a = 7.3271(11) Å and c = 10.336(2) Å. Ca8Mg7Si9N22:Eu2+ shows a narrow-band blue emission peaking at 400 nm with an intriguing bandwidth ∼34 nm and shows remarkably high thermal quenching resistance, maintaining 92% photoluminescence emission intensity at 420 K and 75% at 700 K of that measured at room temperature.


2012 ◽  
Vol 134 (34) ◽  
pp. 14142-14157 ◽  
Author(s):  
Nils Leidel ◽  
Petko Chernev ◽  
Kajsa G. V. Havelius ◽  
Lennart Schwartz ◽  
Sascha Ott ◽  
...  

2019 ◽  
Author(s):  
Ya Zhuo ◽  
Jiyou Zhong ◽  
Jakoah Brgoch

Highly efficient, thermally stable, narrow-band phosphors that can be excited by a blue LED chip are crucial for energy-efficient light bulbs and display lighting. Here, a rare narrow-band, green-emitting phosphor based on the compound NaBaB<sub>9</sub>O<sub>15</sub>:Eu<sup>2+</sup> is demonstrated. The emission peak is centered at 515 nm with a full-width at half-maximum (fwhm) of 61 nm (2294 cm<sup>−1</sup>), and a photoluminescence quantum yield of >80% using blue or near-UV LED excitation. This borate’s remarkable green emission stems from Eu<sup>2+</sup> substituting on the smaller [NaO<sub>6</sub>] polyhedron instead of the larger and more favorable [BaO<sub>9</sub>] polyhedron. The phosphor also exhibits negligible thermal quenching up to 650 K owing to the wide band gap, high connectivity of the rigid NaBaB<sub>9</sub>O<sub>15</sub> crystal structure, and the depopulation of trap-states. This combination of optical properties and its straightforward synthesis conditions makes NaBaB<sub>9</sub>O<sub>15</sub>:Eu<sup>2+</sup> an ideal green phosphor for next-generation LED-based lighting or display systems.


1998 ◽  
Vol 545 ◽  
Author(s):  
J. O. Sofo ◽  
G. D. Mahan

AbstractWe report calculations which show that the band structure of CoSb3 is typical of a narrow band-gap semiconductor. The gap is strongly dependent on the relative position of the Sb atoms inside the unit cell. We obtain a band gap of 0.22 eV after minimization of these position. This value is more than four times larger than the result of a previous calculation which reported that the energy bands near the Fermi surface are unusual. The electronic states close to the Fermi level are properly described by a two-band Kane Model. The calculated effective masses and band gap are in excellent agreement with Shubnikov de Haas and Hall effect measurements. Recent measurements of the transport coefficients of this compound can be understood assuming it is a narrow band gap semiconductor, in agreement with our results.


2020 ◽  
Vol 7 (14) ◽  
pp. 2685-2691
Author(s):  
Tao Hu ◽  
Yan Gao ◽  
Xiaohong Ji ◽  
Zhiguo Xia ◽  
Qinyuan Zhang

Narrow-band blue-emitting MBe2(PO4)2:Eu2+ (M = Ca, Sr) phosphors were developed via selection of an ordered host with confined doping sites.


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