Dispersion of Linear and Nonlinear Optical Susceptibilities in Calcium Neodymium Oxyborate Ca4NdO(BO3)3-LDA versus GGA

被引:16
作者
Reshak, Ali H. [1 ,2 ]
Auluck, S. [3 ]
Kityk, I. V. [4 ]
机构
[1] Univ S Bohemia, Inst Phys Biol, Nove Hrady 37333, Czech Republic
[2] Acad Sci Czech Republ, Inst Syst Biol & Ecol, Nove Hrady 37333, Czech Republic
[3] Indian Inst Technol, Dept Phys, Kanpur 208016, UP, India
[4] Czestochowa Tech Univ, Dept Elect Engn, Czestochowa, Poland
关键词
CRYSTAL-STRUCTURE;
D O I
10.1021/jp8098522
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We have performed ab inito theoretical calculations of the electronic structure and the linear and nonlinear optical susceptibilities for calcium neodymium oxyborate Ca4NdO(BO3)(3) using two approximations for the exchange correlation (XC) potentials, the local density approximation (LDA) and the generalized gradient approximation (GGA). Our calculations show that this compound is metallic-like, with density of states at the Fermi energy E-F, N(E-F), of 5.95 and 10.33 states/Ry-cell or bare electronic specific heat coefficients of 1.03 and 1.79 mJ/mol-K-2 for LDA and GGA, respectively. The overlap between the valence and conduction bands is strong, resulting in metallic behavior. We found that Nd-s/p/d, Ca-s/p. B-p, and O-s/p states controlled the overlapping around EF. The effect of LDA and GGA on the band structure, density of states, and linear optical properties is very small, while for the nonlinear optical properties, it is very pronounced. Our calculations show that chi((2))(111)(omega) is the dominant component for both LDA and GGA. We find opposite signs of the contributions of the 2 omega and 1 omega inter/intraband to the real and imaginary parts for the dominant component throughout the wide optical frequency range.
引用
收藏
页码:1614 / 1622
页数:9
相关论文
共 28 条
[1]  
ABDULLAYEV GK, 1982, KRISTALLOGRAFIYA+, V27, P795
[2]   OPTICAL-PROPERTIES OF PDO AND PTO [J].
AHUJA, R ;
AULUCK, S ;
JOHANSSON, B ;
KHAN, MA .
PHYSICAL REVIEW B, 1994, 50 (04) :2128-2132
[3]  
Blaha P, 2001, CALCULATING CRYSTAL, V60
[4]  
BOYD W, 1992, NONLINEAR OPTICS
[5]   DENSITY OF STATES, OPTICAL MASS, AND DC ELECTRICAL-RESISTANCE OF TA, W, NB, AND MO USING SLATER-KOSTER INTERPOLATION [J].
CHAKRABORTY, B ;
PICKETT, WE ;
ALLEN, PB .
PHYSICAL REVIEW B, 1976, 14 (08) :3227-3230
[6]   NEW DEVELOPMENT OF NONLINEAR-OPTICAL CRYSTALS FOR THE ULTRAVIOLET REGION WITH MOLECULAR ENGINEERING APPROACH [J].
CHEN, CT ;
WANG, YB ;
XIA, YN ;
WU, BC ;
TANG, DY ;
WU, KC ;
ZENG, WR ;
YU, LH ;
MEI, LF .
JOURNAL OF APPLIED PHYSICS, 1995, 77 (06) :2268-2272
[7]   INHOMOGENEOUS ELECTRON-GAS [J].
RAJAGOPAL, AK ;
CALLAWAY, J .
PHYSICAL REVIEW B, 1973, 7 (05) :1912-1919
[8]   Photoemission spectroscopy in metals:: band structure-Fermi surface-spectral function [J].
Hüfner, S ;
Claessen, R ;
Reinert, F ;
Straub, T ;
Strocov, VN ;
Steiner, P .
JOURNAL OF ELECTRON SPECTROSCOPY AND RELATED PHENOMENA, 1999, 100 :191-213
[9]   Electronic, linear, and nonlinear optical properties of III-V indium compound semiconductors [J].
Hussain Reshak, Ali .
JOURNAL OF CHEMICAL PHYSICS, 2006, 125 (03)
[10]   ELECTRONIC STRUCTURE OF HCP YTTERBIUM [J].
JEPSEN, O ;
ANDERSEN, OK .
SOLID STATE COMMUNICATIONS, 1971, 9 (20) :1763-+