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The bands at 450 and 468 nm can be attributed to free excitons, and emission peaks at longer wavelength of 481 and 492 nm can be attributed to the bound excitons [40, 41].
This theoretical model has been designed to illustrate the two emission bands in the UV region observed in our experimental Photoluminescence spectrum (PL), with the first emission band observed at 3.04 eV and attributed to the bound ionized acceptor exciton complexes, and the second one located at 3.5 and assigned to the free exciton.
Subsequent P proton-decoupled MAS-NMR studies of the R64L, R89L and the R64L/R89L double mutant showed the disappearance of the resonance attributed to the bound POPG at − 0.14 ppm.
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If these ΔδCα secondary shifts are entirely attributed to the 2% bound state, secondary shifts in the CR-bound state are ∼50-fold larger and therefore indicative of a high population of α-helical backbone ϕ and ψ angles, even while not rigidly anchored to the CR micelle.
In the PL spectra of In-doped ZnO NWs (#2 and #3); however, the DBE peak shifts to 3.357 eV, which is known as I9 line and is unambiguously attributed to the exciton bound to In donors [19, 20].
A relatively small decrease in the intensity of FT-IR signals in case of SP-HRG, when compared to CRG and also the presence of some additional bands in its IR spectrum, is attributed to the phytomolecules bound to the surface of SP-HRG post in-situ functionalization.
Notably the resonance at − 0.14 ppm that we have attributed to the POPG bound to the non-annular binding site is absent in the spectra of the three mutants.
The fast and efficient cells-hydrogel adhesion may be attributed to the specific binds between link N peptide and BMP-R II on BMSCs [ 22].
A small sideband at 1725 cm 1 is attributed to the ester bond of the surface bound initiator.
The decomposition of HDTMA within SMZ takes place in two phases; the first phase was attributed to the decomposition of surfactants bound to their adjoining molecules through hydrophobic interaction, while the second phase was due to the loss of surfactants bound to the surface of the zeolite through electrostatic interaction (Lin and Zhan 2012).
The difference between the QCM-D mass and the SPR mass can be attributed to the mass related to the bound and coupled mass of water.
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