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Negative binding energy for the docked conformations (Figure 7A and 7C) indicates that the binding was thermodynamically favourable.
When the QD radius a increases, the electron binding energy for the superatom ground state also increases.
The binding energy for the different glymes reaches a maximum of ∼582 kJ mol−1 for the Li+ PEI pentaglyme (n=5, X=NH) complex.
Compared with g-C3N4/Ni/GO-2%, the binding energies of Ni 2p shifted to low binding energy for the g-C3N4/PtNi/GO-2% sample.
The slight higher binding energy for the O1s in C=O of the conjugate ring was due to the coordination of organic ligand [22].
The binding energy for the tested element was calibrated from the C 1 s peak (284.6 eV) of the surface adventitious carbon.
Similar(22)
The binding energies for the Ps in circular and spherical QDs are calculated.
The binding energies for the samples were calibrated by setting the measured binding energy of C 1s to 284.60 eV.
The binding energies for the sample were calibrated by setting the measured binding energy of C1s to 284.60 eV.
These values are in fairly good agreement with the reported exciton binding energies for the L1 line [24].
The binding energies for the species were all correlated to the binding energies determined from standards in the handbook of XPS [17] and earlier studies [18, 19].
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