Optical absorption enhancement in slanted silicon nanocone hole arrays for solar photovoltaics
We investigate slanted silicon nanocone hole arrays as light absorbing structures for solar photovoltaics via simulation.With only 1-μm equivalent thickness, a maximum short-circuit current density of 34.9 m A/cm~2 is obtained. Moreover, by adding an Ag mirror under the whole structure, a short-circ...
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| Published in | Chinese physics B Vol. 25; no. 10; pp. 298 - 302 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
01.10.2016
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| Online Access | Get full text |
| ISSN | 1674-1056 2058-3834 |
| DOI | 10.1088/1674-1056/25/10/106802 |
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| Abstract | We investigate slanted silicon nanocone hole arrays as light absorbing structures for solar photovoltaics via simulation.With only 1-μm equivalent thickness, a maximum short-circuit current density of 34.9 m A/cm~2 is obtained. Moreover, by adding an Ag mirror under the whole structure, a short-circuit current density of 37.9 m A/cm~2 is attained. It is understood that the optical absorption enhancement mainly results from three aspects. First, the silicon nanocone holes provide a highly efficient antireflection effect. Second, after breaking the geometric symmetry, the slanted silicon nanocone hole supports more resonant absorption modes than vertical structures. Third, the Fabry–Perot resonance enhances the light absorption after adding an Ag mirror. |
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| AbstractList | We investigate slanted silicon nanocone hole arrays as light absorbing structures for solar photovoltaics via simulation.With only 1-μm equivalent thickness, a maximum short-circuit current density of 34.9 m A/cm~2 is obtained. Moreover, by adding an Ag mirror under the whole structure, a short-circuit current density of 37.9 m A/cm~2 is attained. It is understood that the optical absorption enhancement mainly results from three aspects. First, the silicon nanocone holes provide a highly efficient antireflection effect. Second, after breaking the geometric symmetry, the slanted silicon nanocone hole supports more resonant absorption modes than vertical structures. Third, the Fabry–Perot resonance enhances the light absorption after adding an Ag mirror. |
| Author | 张淑媛 刘雯 李兆峰 刘敏 刘雨生 王晓东 杨富华 |
| AuthorAffiliation | Engineering Research Center for Semiconductor Integrated Technology, Institute of Semiconductors,Chinese Academy of Sciences |
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| CitedBy_id | crossref_primary_10_1039_C8RA03730B crossref_primary_10_1063_1_5024052 crossref_primary_10_7498_aps_69_20200334 crossref_primary_10_1016_j_optcom_2019_125059 |
| Cites_doi | 10.1021/nl904187m 10.1063/1.4802442 10.1364/OE.21.018043 10.1038/srep07810 10.1021/nl204550q 10.1021/nl100161z 10.1016/j.egypro.2011.10.161 10.1364/OL.38.003973 10.1021/nl802886y 10.1364/OL.36.001713 10.1186/s11671-014-0718-x 10.1038/nmat2629 10.1016/S0038-092X(03)00065-3 10.1021/nn5023878 10.1002/pip.2355 10.1364/OE.21.00A872 10.1063/1.3292020 10.1016/j.solmat.2010.10.004 10.1063/1.4803676 10.1021/nl300713x 10.1146/annurev-matsci-062910-100434 10.1063/1.4901466 |
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| Notes | Shu-Yuan Zhang;Wen Liu;Zhao-Feng Li;Min Liu;Yu-Sheng Liu;Xiao-Dong Wang;Fu-Hua Yang;Engineering Research Center for Semiconductor Integrated Technology, Institute of Semiconductors,Chinese Academy of Sciences 11-5639/O4 |
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| References | 22 23 Shi Y P (3) 2014; 16 24 26 27 Shi Y P (2) 2014; 7 28 Yue H H (11) 2011; 32 Zhang X (29) 2015; 17 Zhang X (30) 2015; 17 31 10 32 33 13 14 15 17 Wang B M (21) 2012; 23 Qiu K (12) 2015; 36 1 4 5 Chen F X (18) 2013; 22 6 7 8 9 Chen L (19) 2015; 24 Wang W (25) 2013; 46 20 Xu R (16) 2012; 51 |
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