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A simple and effective cryogenic device was applied to the SHPB system to create the low-temperature field of the samples.
The maximum electric field is increased up to 1.8 × 106 and 2.4 × 106 for NP-1 and NP-2, respectively, compared to the value of 5.18 × 105 for Ref. The increased electric field of the samples with the Au and Ag NPs is mainly attributed to the reduction of barrier height as the effective barrier of the conduction band at the depletion region decreases.
The experimental results are in agreement with both analytic calulations based on Tung's model and physics-based two-dimensional numerical simulations, which confirm that the increased electric field of the samples with NPs is mainly attributed to the reduction of barrier height as the effective barrier of the conduction band at the depletion region of the surface decreases.
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By changing the thickness value of this second Co layer (X) by modifying the deposition time, the value of the anisotropy field of the sample could be controlled.
The analysis is shown in Fig. 6b e, for those three stripes that lie in the center of the spatial receptive field of the sample neuron.
When using the format "m_xxxx.txt" to name the Material files, the string "xxxx" should exactly match the string used in the Material Source Name field of the sample's Material file.
The values of the saturation magnetisation and the anisotropy field of these samples were larger in the samples that had a thicker ferromagnetic layer.
In the cation plot field most of the samples plot towards the Na + K corner and in the anion field the samples plot towards the Cl corner.
Fig. 6 Dark field images of the samples.
The electric field distributions of the samples were theoretical predicted using thin film design software (TFCalc).
The theoretical results of electric field distributions of the samples were calculate by thin film design software (TFCalc).
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