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Figure 3(a) shows the geometry of the model.

Individual scans were cleaned, aligned and refined in order to yield the final geometry of the model.

If the spin polarization is constrained to be zero, the DFT equilibrium geometry of the model changes: both the tripled periodicity along the Si rows and the doubled periodicity along the Au rows are completely eliminated.

The geometry of the model, which includes the electrodes and skin composed of various layers, is shown in Fig. 6a.The electrical and thermal properties of the skin layers used for modeling appear in Table 333,34.

The geometry of the model is a complicated time-dependent two-dimensional configuration of flux contours analogous to a doublet.

These meso FE analyses are highly dependent on the quality of the initial geometry of the model.

X-ray images are taken to show the close similarity of the interior geometry of the models and the actual samples.

The geometry of the models considered in the study replicate the PCHEs that were fabricated using Alloy 617 plates for use in a High-Temperature Helium Facility (HTHF) at The Ohio State University.

The pore specific surface areas are similar between the reference model and the reconstructed model, reflecting that the pore geometry of the models are similar.

The geometries of the model systems (H3CSCH3 7 and A@(H3CSCH3 7 (A = Na+, K+, F−, Cl−, NO3 −) were optimized via constrained energy minimization at the level of density functional theory (DFT).

Using this method the geometry of the initial model is maintained in the final model.