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The most negative interfaces (pure SA, S7A3, S5A5) showed significant fibrinogen adsorption, ascribed to the interactions of the αC domains of the protein with the gels, then correlated to considerable platelet adhesion; but low leukocyte/erythrocyte attachments were measured.
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The beneficial influence of GO may be attributed to its negative interface charge (or oxide charge).
In addition, the possible physical background of positive or negative interface stress is analyzed.
The shift of the GO curve as compared to the control curve may be due to the negative interface charge (or oxide charge) of GO.
The negative interface charge acts as a hole reservoir and thus confines the recombination zone near the emission layer (EML); 4,4′-bis N-carbazolyl -1,1′-biphenyl (CBP):4,4′-bis N-carbazolyl -1,1′-biphenyl
Displacement current measurement (DCM) data revealed the presence of negative interface charge originating from the spontaneous orientation polarization of the electron transport layer (ETL), 1,3,5-tris 1-phenyl-1H-benzimidazol-2-yl) benzene.
First principles calculation reveals that the W TiC interfaces with one overlayer possess high interface strength and are thermodynamically stable with negative interface energies, which could serve as the driving force for interdiffusion of W and TiC.
The results show that the threshold voltage shifts upward and approaches a maximum value with negative interface charges and shifts downward and reaches a minimum value with positive interface charges as the interface charge region length is increased from zero to the channel length.
It demonstrates that the electric field increases with the increase in the diameter of NC Ge at a stored charge in NC Ge layer of −1 × 1012 C. Similarly, we can prove that negative interface charge density will lead to a decrease in the electric field across the tunneling oxide layer.
The analyses were based on two aging mechanisms proposed in previous studies and the predictions showed consistency with the previous teardown observations that the sulfate formed at the negative interface is more difficult to be converted back than anywhere else in the electrodes.
Assuming vanishingly low, but clearly not negative interface tension, limitations to the droplet size can only be a consequence of a size-dependent term for the free energy of the aggregate bulk.
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