• Journal of Semiconductors
  • Vol. 42, Issue 3, 031701 (2021)
Rokas Kondrotas1,2, Chao Chen1, XinXing Liu1, Bo Yang1, and Jiang Tang1
Author Affiliations
  • 1Sargent Joint Research Center, Wuhan National Laboratory for Optoelectronics and School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, China
  • 2Center for Physical Sciences and Technology, Sauletekio 3, Vilnius 10257, Lithuania
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    DOI: 10.1088/1674-4926/42/3/031701 Cite this Article
    Rokas Kondrotas, Chao Chen, XinXing Liu, Bo Yang, Jiang Tang. Low-dimensional materials for photovoltaic application[J]. Journal of Semiconductors, 2021, 42(3): 031701 Copy Citation Text show less
    (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. 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].
    (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 (Ntotal, photon number in AM 1.5 G spectrum with energy larger than Eind) as a function of ΔE and Eind. The blue-dashed line indicates a boundary of the 85%. A1 and A2 of dashed line 1 are 105 and 104 cm–1; A1 and A2 of dashed line 2 are 4 × 104 and 104 cm–1; A1 and A2 of dashed line 3 are 2 × 104 and 104 cm–1; A1 and A2 of dashed line 4 are 2 × 104 and 103 cm–1. (c) The ratio of electrons in indirect band (Nind) to the total number of electrons (Ntotal) as a function of ΔE and temperature.
    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 (Ntotal, photon number in AM 1.5 G spectrum with energy larger than Eind) as a function of ΔE and Eind. The blue-dashed line indicates a boundary of the 85%. A1 and A2 of dashed line 1 are 105 and 104 cm–1; A1 and A2 of dashed line 2 are 4 × 104 and 104 cm–1; A1 and A2 of dashed line 3 are 2 × 104 and 104 cm–1; A1 and A2 of dashed line 4 are 2 × 104 and 103 cm–1. (c) The ratio of electrons in indirect band (Nind) to the total number of electrons (Ntotal) 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.
    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].
    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].
    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].
    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].
    MaterialDimensionEgind (eV) ΔEg (eV) Anisotropy ratio*PV solar cell PCE (%)Application
    *Anisotropy ratio expressed in terms of: μ- mobility, m* - effective mass, σ - conductivity.
    (BA)2(MA)n–1 PbnI3n+12D1.5–2.300.28μ[34]12.53[35]LED, PV solar cells
    SnS2D1.070.150.08μ[36]4.36[37]Thermoelectrics, PV solar cells
    SnSe2D0.860.20.2σ[38]N/AThermoelectrics
    CuSbSe22D1.040.04N/A4.7[39]PV solar cells, thermoelectrics
    CuSbS22D1.40.050.15m*[40]3.22[41]PV solar cells, thermoelectrics
    MoSe22D1.060.40~0.001–0.01σ[42]1.29[43]PEC, HER, batteries, transistors, PV solar cells
    MoS22D1.290.300.006σ[44]2.8[45]PEC, HER, batteries, transistors, PV solar cells
    GeSe2D1.10.100.33σ[46]1.48[47]PV solar cells
    Sb2Se31D1.050.13~0.10σ[48]9.2[10]PV solar cells
    Sb2S31D1.70.08~0.10σ[49]7.5 [50]PV solar cells, HTL
    Sb2(S,Se)31D1.49N/AN/A10.5[51]PV solar cells
    Bi3S31D1.350.100.32μ[52]0.75[53]Thermoelectrics, PV solar cells
    SbSI1D2.150.200.31σ[54]3.05[55]PV solar cells, ferroelectric
    BiOI2D1.930.4N/A1.82[56]PV solar cells
    Se1D1.840N/A~6.5[57]PV solar cells
    Table 1. Summary of low-dimensional material characteristics and champion solar cell PCE.