2009
DOI: 10.1002/pssb.200844121
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Simulation of electronic density of states and optical properties of PbB4O7 by first‐principles DFT method

Abstract: First‐principles calculations based on the density functional theory and the generalized gradient approximation were carried out to systematically investigate the electronic structure and linear optical properties of lead tetraborate (PbB4O7; PTB) single crystals. An indirect band gap of 4.34 eV is obtained. The valence band top is at the X‐point and the conduction band is at the Γ‐point. The calculated total and partial densities of states indicate that the top valence band is constructed from O 2p states and… Show more

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Cited by 30 publications
(7 citation statements)
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“…The optical absorption series of the nanosheet system under pressure can be seen in Figure 4 (a). Scissor operation [23] was used to underestimate the optical band gap energy, but it is really uneasy to achieve the accurate optical energy band gap. This method is functioning for various organisms.…”
Section: Resultsmentioning
confidence: 99%
“…The optical absorption series of the nanosheet system under pressure can be seen in Figure 4 (a). Scissor operation [23] was used to underestimate the optical band gap energy, but it is really uneasy to achieve the accurate optical energy band gap. This method is functioning for various organisms.…”
Section: Resultsmentioning
confidence: 99%
“… where P implies the principal value of the integral. The knowledge of the real and imaginary parts of the dielectric function allows the calculation of other important optical functions such as the refractive index n (ω), reflectivity R ( ), extinction coefficient k (ω), energy loss function L (ω) and absorption coefficient α(ω) by using the following expressions [ 47 , 48 , 49 ]: …”
Section: Resultsmentioning
confidence: 99%
“…The optical parameters of these different phases of the CdTe material were obtained from the dielectric function expressed as ε(ω) = ε 1 (ω) + i ε 2 (ω); here, the first part represents a real and the second part represents an imaginary component of the frequency-dependent dielectric constant. The imaginary component is associated with the total absorbed energy by the material and is also related to the optical band gap of the materials. , These real and imaginary parts are most likely given as follows: ε 1 ( ω ) = 1 + 2 π true∫ 0 0.25em ε 2 ( ω ) ω 0.25em d ω true∫ 0 1 ώ 2 ω 2 d ώ ε 2 ( ω ) = 0.25em e 2 0.25em h π m 2 ω 2 normalv , normalc true∫ false| M cv ( k ) false| 2 δ [ ω cv false( k false) ω ] …”
Section: Computational Detailsmentioning
confidence: 99%