Cartel de l'œuvreÉpoque/Dates

determined in second 2.2 and third 2.3 stages of proposed approach. Once relevant KC’s have been classified, they would indicate the required capability of inspection

Audsley’s algorithm (i.e., task critical scaling factors are used for braking ties), and since Audsley’s algorithm is optimal due to Theorem 1, we can conclude that Vestal’s

We define the manifold and field discretizations, provide a simplicial action, define the fermionic loop expansion, and finally perform the integrations in the discretized path

To leave its metastable state and reach the lateral surface of the wire, the screw dislocation (parallel to the cylindrical wire axis) must overcome an energy barrier whose maximum

Second, our calculations show that the adsorption of a NO molecule on an oxygen atom of the stoichiometric WO 3 (001) surface leads to an n-type doping, which is very similar to the

The band offsets between oxides and semiconductors (not shown here) are the same as in reference [20] except for Ge/GeO 2 interface [18]. Simulated and experimental data are in

Figure 8. Original VG ion source. This type of source has several drawbacks. - First, the source box is heated up to 600 K by the filament radiation and very

side of the gate sensibly enhances the collected charge and the bipolar gain of the device compared to the SMDG counterpart.. The difference between the two devices is