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High-current density and high-asymmetry MIIM diode based on oxygen-non-stoichiometry controlled homointerface structure for optical rectenna
Optical rectennas are expected to be applied as power sources for energy harvesting because they can convert a wide range of electromagnetic waves, from visible light to infrared. The critical element in these systems is a diode, which can respond to the changes in electrical polarity in the optical...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6928205/ https://www.ncbi.nlm.nih.gov/pubmed/31873112 http://dx.doi.org/10.1038/s41598-019-55898-x |
Sumario: | Optical rectennas are expected to be applied as power sources for energy harvesting because they can convert a wide range of electromagnetic waves, from visible light to infrared. The critical element in these systems is a diode, which can respond to the changes in electrical polarity in the optical frequency. By considering trade-off relationship between current density and asymmetry of IV characteristic, we reveal the efficiency limitations of MIM diodes for the optical rectenna and suggest a novel tunnel diode using a double insulator with an oxygen-non-stoichiometry controlled homointerface structure (MO(x)/MO(x−y)). A double-insulator diode composed of Pt/TiO(2)/TiO(1.4)/Ti, in which a natural oxide layer of TiO(1.4) is formed by annealing under atmosphere. The diode has as high-current-density of 4.6 × 10(6) A/m(2), which is 400 times higher than the theoretical one obtained using Pt/TiO(2)/Ti MIM diodes. In addition, a high-asymmetry of 7.3 is realized simultaneously. These are expected to increase the optical rectenna efficiency by more than 1,000 times, compared to the state-of-the art system. Further, by optimizing the thickness of the double insulator layer, it is demonstrated that this diode can attain a current density of 10(8) A/m(2) and asymmetry of 9.0, which are expected to increase the optical rectenna efficiency by 10,000. |
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