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The suitable incorporation of Cd enables the band gap to be tuned for various potential applications [12].
Being coated on any surface and capability of the band gap to be tuned by changing the size and the shape of the particle are the potential advantages of colloidal QDs [5, 6].
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AlInN is a newly developed III-nitride for many promising applications due to its band gap being able to be tuned in a wide range of 0.70 ~ 6.14 eV with high spontaneous polarization[1 3].
No free parameters need to be tuned.
Computation results suggest that this gap can be tuned to a solar optimal ∼1.3 eV via systematic sulfur vacancy sites engineered into the crystal structure.
The optical band gap can then be tuned to the effective energy region for absorbing maximum intensity over the solar radiation spectrum.
The optical band gap can then be tuned to the effective energy region for absorbing the maximum intensity of the solar radiation spectrum.
The optical band gap can then be tuned to an effective energy region for absorbing the maximum intensity of the solar radiation spectrum.
Hence, a GSPC structure can be used for broadening as well as tuning the photonic band gap and the bandwidth of gaps can be tuned to a desired wavelength region by choosing appropriate value of γ (positive or negative).
Employing structural variations such as chalcogen/acceptor replacement, extension of the π-system, and the position of substitution along the pyran ring, the HOMO-LUMO gap can be tuned within the range of 2.18 to 1.41 eV.
Therefore the position of the unpaired electrons and the doublet quartet gap can be tuned by chemical methods, which opens the way to fine-tune the properties of the building blocks of organic magnets.
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