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The results are similar to the negative band as reported earlier for single macrodomains.
CIGS thin films form positively charged GBs which is related to negative band bending.
As the frequency goes up, the permittivity in both directions turns negative (band 2).
Ultrasonic pre-irradiation enhanced the negative band intensity, indicating slight perturbation of the tertiary structure [24].
The surface potential near GBs shows negative band bending behaviors with about 300 meV of energy shift.
In water, the CD curves show a strong negative band below 200 nm as a sign of the presence of unfolded conformers.
It is noted that alkaline environment leads to a negative band edge of TiO2 microsphere and promotes the interfacial charge transfer.
On the other hand, the CD spectra of refolded ABF-2 showed a significant negative band in the region between 208 and 220 nm.
However, a negative band around 200 nm from the random coil structure was dominantly observed for the egg white-templated metal clusters.
The AlxGa1 − xN nanotubes exhibit direct band gaps for the whole range of Al compositions, with band gaps varying from 3.45 to 4.85 eV, and a negative band gap bowing coefficient of −0.14 eV.
Importantly, while normal leaf tissue shows a typical split signal with both a negative and a positive peak in the induced fractional circular polarization and circular dichroism, the signals close to the veins only display a negative band.
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