Rokas Kondrotas, Chao Chen, XinXing Liu, Bo Yang, Jiang Tang. Low-dimensional materials for photovoltaic application[J]. Journal of Semiconductors, 2021, 42(3): 031701

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- Journal of Semiconductors
- Vol. 42, Issue 3, 031701 (2021)
![(Color online) The evolution of crystal structure and morphology of the grain as a function of structural dimensionality. CdTe, MoS2 and Sb2Se3 structures were selected as representative materials in each case. Grain morphology was calculated using Bravais−Friedel−Donnay−Harker (BFDH) theory[18].](/richHtml/jos/2021/42/3/031701/img_1.jpg)
Fig. 1. (Color online) The evolution of crystal structure and morphology of the grain as a function of structural dimensionality. CdTe, MoS2 and Sb2Se3 structures were selected as representative materials in each case. Grain morphology was calculated using Bravais−Friedel−Donnay−Harker (BFDH) theory[18 ].

Fig. 2. (Color online) (a) Photon absorption and carrier dynamics for a quasi-indirect band gap semiconductor. Photons are first absorbed via direct band gap (I) or indirect band gap (II), they then thermodynamically relax to the indirect band gap (III) and eventually recombine (IV). (b) The ratio of photons absorbed to the total number of photons (N total, photon number in AM 1.5 G spectrum with energy larger than E ind) as a function of ΔE and E ind. The blue-dashed line indicates a boundary of the 85%. A 1 and A 2 of dashed line 1 are 105 and 104 cm–1; A 1 and A 2 of dashed line 2 are 4 × 104 and 104 cm–1; A 1 and A 2 of dashed line 3 are 2 × 104 and 104 cm–1; A 1 and A 2 of dashed line 4 are 2 × 104 and 103 cm–1. (c) The ratio of electrons in indirect band (N ind) to the total number of electrons (N total) as a function of ΔE and temperature.
![(Color online) Point defects in Sb2Se3 taking into account, it contains two kinds of Sb and three kinds of Se. Reprinted from Chen et al.[27] with permission.](/Images/icon/loading.gif)
Fig. 3. (Color online) Point defects in Sb2Se3 taking into account, it contains two kinds of Sb and three kinds of Se. Reprinted from Chen et al .[27 ] with permission.
![(Color online) (a) Carrier movement in Sb2Se3 along [120] (red dashed arrows) and [221] (solid red arrow) directions. (b) Atomistic view of Sb2Se3 grain boundary oriented [001] direction perpendicular to substrate. All of the atoms at the edge of these ribbons are saturated (highlighted as red spheres) and introduce no recombination loss at the GBs. Reprinted from Tang et al. with permission[29].](/Images/icon/loading.gif)
Fig. 4. (Color online) (a) Carrier movement in Sb2Se3 along [120] (red dashed arrows) and [221] (solid red arrow) directions. (b) Atomistic view of Sb2Se3 grain boundary oriented [001] direction perpendicular to substrate. All of the atoms at the edge of these ribbons are saturated (highlighted as red spheres) and introduce no recombination loss at the GBs. Reprinted from Tang et al . with permission[29 ].
![(Color online) Layered crystal structure of SnS with Pnma space group and calculated morphology of the grain based on the surface energy. Surface energy (SE), EA and IP of various SnS facets. Printed with permission[61].](/Images/icon/loading.gif)
Fig. 5. (Color online) Layered crystal structure of SnS with Pnma space group and calculated morphology of the grain based on the surface energy. Surface energy (SE), EA and IP of various SnS facets. Printed with permission[61 ].
![(Color online) Schematics of growth process of 3D and 1D materials on (a, b) inert and (c, d) strongly interacting substrates. (a) represents an island-like growth mode, whereas (c) layer-by-layer[62].](/Images/icon/loading.gif)
Fig. 6. (Color online) Schematics of growth process of 3D and 1D materials on (a, b) inert and (c, d) strongly interacting substrates. (a) represents an island-like growth mode, whereas (c) layer-by-layer[62 ].
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Table 1. Summary of low-dimensional material characteristics and champion solar cell PCE.

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