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It is also observed that the spin anisotropy of the edge states is attributed to the reconstruction of the edge.
The change of the VBT states is attributed to the confinement of charge carriers which results in the quasi-continuous energy bands of the bulk semiconductors becoming discretized.
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The scale and time dependent wavelet coherence variations observed for CO2 and meteorological data over three different states were attributed to mesoscale variability including variations in the type of vegetation, topography, land-vegetation contrast, cloud cover, and overall landscape heterogeneity.
By comparing the band structures of H-covered 3 BLs calculated with (Fig. 3a) and without SOC (Fig. 3b), we note that the topological surface states are attributed to the SOC.
In our model, differences between active and passive states are attributed to the rate of the uncorrelated external drives.
Most significantly, the interconversion of the OF and IF states was attributed mostly to the rocking of the TM1 TM2/TM6 TM7 bundle as a rigid body with respect to the rest of the protein.
The suppression of carrier transmission in the OFF state is attributed to the finite bandgap of the ∼15 nm wide graphene nanoribbon channel.
According to our previous prediction based on a theoretical model, the occurrence of the nonmagnetic ground state is attributed to a spin frustration effect inherent in organic molecular assemblages.
Much of this state is attributed to the minor crop status of this crop coupled with the specialized nature of use for flavoring and the need to maintain end-product consistency from year to year.
Significant red shifting of absorption onset (Δλabsonset ≈ 85 210 nm) and emission peak maxima (Δλem.max ≈ 175 nm) at solid state is attributed to the formation of more rigid planar interdigited π-stack 3D structure.
Occurrence of the superferromagnetic state is attributed to interaction between nanoparticles leading to correlation between orientations of their magnetic moments.
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