H. van Cong, K. C. Ho-Huynh Thi, C. T. Huynh-Pivet, A. Pivet, C. V. Huynh, A. L. Pivet, I. Pivet
{"title":"29.58%(31.26) %效率获得最高限制 \\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {n }^+(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {p }^+)-\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\ mathbf {p }(\\\\\\\\\\\\\\\\\\\\","authors":"H. van Cong, K. C. Ho-Huynh Thi, C. T. Huynh-Pivet, A. Pivet, C. V. Huynh, A. L. Pivet, I. Pivet","doi":"10.54647/physics14491","DOIUrl":null,"url":null,"abstract":"In the n+(p+) − p(n) crystalline InP-junction solar cells, by basing on a same treatment method, and for a same heavy (low) doping effect, as those investigate in our recent papers [1, 2], but using now a new expression, obtained for the static relative dielectric constant ε rd a , determined exactly in the effective Bohr model, as that given in Eq. (1c), representing the donor (acceptor) d(a)-radius rd a − effect, or the ε rd a − effect, suggesting further that, for an increasing rd a , ε rd a decreases, as showed in Table 1, according to the increase in photovoltaic efficiency η, as that observed in Tables 2 and 3, we finally get, in our present paper, for highest values of rd a , the limiting highest efficiency results of such n+(p+) − p(n) crystalline InP-junction solar cells, η=29.58% (31.26%), respectively. SCIREA Journal of Physics ISSN: 2706-8862 http://www.scirea.org/journal/Physics October 23, 2022 Volume 7, Issue 5, October 2022 https://doi.org/10.54647/physics14491","PeriodicalId":194720,"journal":{"name":"SCIREA Journal of Physics","volume":"16 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-10-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"29.58% (31.26)% -Limiting Highest Efficiencies obtained in the \\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{n}^+(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}^+)-\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\",\"authors\":\"H. van Cong, K. C. Ho-Huynh Thi, C. T. Huynh-Pivet, A. Pivet, C. V. Huynh, A. L. Pivet, I. Pivet\",\"doi\":\"10.54647/physics14491\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In the n+(p+) − p(n) crystalline InP-junction solar cells, by basing on a same treatment method, and for a same heavy (low) doping effect, as those investigate in our recent papers [1, 2], but using now a new expression, obtained for the static relative dielectric constant ε rd a , determined exactly in the effective Bohr model, as that given in Eq. (1c), representing the donor (acceptor) d(a)-radius rd a − effect, or the ε rd a − effect, suggesting further that, for an increasing rd a , ε rd a decreases, as showed in Table 1, according to the increase in photovoltaic efficiency η, as that observed in Tables 2 and 3, we finally get, in our present paper, for highest values of rd a , the limiting highest efficiency results of such n+(p+) − p(n) crystalline InP-junction solar cells, η=29.58% (31.26%), respectively. 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29.58% (31.26)% -Limiting Highest Efficiencies obtained in the \\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{n}^+(\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}^+)-\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\\mathbf{p}(\\\\\\\\\\
In the n+(p+) − p(n) crystalline InP-junction solar cells, by basing on a same treatment method, and for a same heavy (low) doping effect, as those investigate in our recent papers [1, 2], but using now a new expression, obtained for the static relative dielectric constant ε rd a , determined exactly in the effective Bohr model, as that given in Eq. (1c), representing the donor (acceptor) d(a)-radius rd a − effect, or the ε rd a − effect, suggesting further that, for an increasing rd a , ε rd a decreases, as showed in Table 1, according to the increase in photovoltaic efficiency η, as that observed in Tables 2 and 3, we finally get, in our present paper, for highest values of rd a , the limiting highest efficiency results of such n+(p+) − p(n) crystalline InP-junction solar cells, η=29.58% (31.26%), respectively. SCIREA Journal of Physics ISSN: 2706-8862 http://www.scirea.org/journal/Physics October 23, 2022 Volume 7, Issue 5, October 2022 https://doi.org/10.54647/physics14491