TY - JOUR
T1 - First-principles calculations of the electronic structure and optical properties of and crystals
AU - Li, Jun
AU - Duan, Chun gang
AU - Gu, Zong quan
AU - Wang, Ding sheng
PY - 1998
Y1 - 1998
N2 - This paper reports the calculation of electronic structure and linear optical properties of (Formula presented) (LBO), (Formula presented) (CBO), and (Formula presented) (BBO) crystals using the linearized augmented plane-wave band method. It is found that the top of their valence bands consists of O orbitals, while the boron has almost no contribution. The linkage between ((Formula presented) anionic groups in the crystalline state is the main cause of making the gap of LBO and CBO larger than BBO’s. The near-edge interband transition contains the contribution of the trigonal coordinated B-O bands in the final state for LBO. For CBO and BBO, the final state consists mainly of cation states at the bottom of the conduction bands. In this case, however, the transition from the O derived valence states to these cation states is quite weak; strong transition only appears till about 1 eV above the absorption edge when B-O orbitals are also involved in the final states.
AB - This paper reports the calculation of electronic structure and linear optical properties of (Formula presented) (LBO), (Formula presented) (CBO), and (Formula presented) (BBO) crystals using the linearized augmented plane-wave band method. It is found that the top of their valence bands consists of O orbitals, while the boron has almost no contribution. The linkage between ((Formula presented) anionic groups in the crystalline state is the main cause of making the gap of LBO and CBO larger than BBO’s. The near-edge interband transition contains the contribution of the trigonal coordinated B-O bands in the final state for LBO. For CBO and BBO, the final state consists mainly of cation states at the bottom of the conduction bands. In this case, however, the transition from the O derived valence states to these cation states is quite weak; strong transition only appears till about 1 eV above the absorption edge when B-O orbitals are also involved in the final states.
UR - https://www.scopus.com/pages/publications/0000512480
U2 - 10.1103/PhysRevB.57.6925
DO - 10.1103/PhysRevB.57.6925
M3 - 文章
AN - SCOPUS:0000512480
SN - 1098-0121
VL - 57
SP - 6925
EP - 6932
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 12
ER -