2023
DOI: 10.1109/tmtt.2022.3205612
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Design of a Simultaneous Information and Power Transfer System Based on a Modulating Feature of Magnetron

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Cited by 56 publications
(16 citation statements)
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“…When in the valence band electrons are provided with a sufficient amount of energy to jump into the conduction band, then the charge carriers are produced. Electron and hole‐effective masses can be visualized from CBM and VBM curvatures [67, 68]. Electron has positive effective mass in comparison with holes that have negative effective mass.…”
Section: Resultsmentioning
confidence: 99%
“…When in the valence band electrons are provided with a sufficient amount of energy to jump into the conduction band, then the charge carriers are produced. Electron and hole‐effective masses can be visualized from CBM and VBM curvatures [67, 68]. Electron has positive effective mass in comparison with holes that have negative effective mass.…”
Section: Resultsmentioning
confidence: 99%
“…The maximum efficiency of thermoelectric materials for an energy conversion process at a given temperature can be calculated using the figure of merit as follows [68]: ZTgoodbreak=S2goodbreak×σgoodbreak×T/κ.$$ \mathrm{ZT}={S}^2\times \sigma \times T/\kappa . $$ The figure of Merit (ZT) is one of the significant aspects of the thermoelectric property.…”
Section: Resultsmentioning
confidence: 99%
“…The plots of Power Factor (PF) against chemical potential are shown in Figure 7B that is derived from Seebeck coefficient and electrical conductivity. Another essential metric for assessing the effectiveness of real‐world thermoelectric devices is power factor (PF), which is the result of multiplying electrical conductivity by the Seebeck coefficient, which is found in [68–70]: Power factorgoodbreak=S2σ,$$ \mathrm{Power}\ \mathrm{factor}={S}^2\sigma, $$ where, σ is the electrical conductivity and S is the Seebeck coefficient.…”
Section: Resultsmentioning
confidence: 99%
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