• Journal of Semiconductors
  • Vol. 41, Issue 5, 052201 (2020)
Zhongti Sun1、2, Xiwen Chen1、2, and Wanjian Yin1、2、3
Author Affiliations
  • 1College of Energy, Soochow Institute for Energy and Materials InnovationS (SIEMIS), Soochow University, Suzhou 215006, China
  • 2Jiangsu Provincial Key Laboratory for Advanced Carbon Materials and Wearable Energy Technologies, Soochow University, Suzhou 215006, China
  • 3Key Lab of Advanced Optical Manufacturing Technologies of Jiangsu Province & Key Lab of Modern Optical Technologies of Education Ministry of China, Soochow University, Suzhou 215006, China
  • show less
    DOI: 10.1088/1674-4926/41/5/052201 Cite this Article
    Zhongti Sun, Xiwen Chen, Wanjian Yin. Comprehensive first-principles studies on phase stability of copper-based halide perovskite derivatives AlCumXn (A = Rb and Cs; X = Cl, Br, and I)[J]. Journal of Semiconductors, 2020, 41(5): 052201 Copy Citation Text show less
    (Color online) (a) The optimized structure of CHPs with 325-type, they own the isostructural model with space group of Pnma, isolated [Cu2X5]3– anion unit is composed of two types of Cu+ sites, a trigonal site and a tetragonal site. (b) Calculated phase stability regions versus μCu and μX (referring to the chemical potential of Cu and X from that of their elementary substance) from left to right for the X site of I, Br, and Cl element and up to down for Cs and Rb element on A site, respectively. The cyan polygon region represents thermodynamic stability growth region, which is encircled by possible competing phases using colored line (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 1. (Color online) (a) The optimized structure of CHPs with 325-type, they own the isostructural model with space group of Pnma, isolated [Cu2X5]3– anion unit is composed of two types of Cu+ sites, a trigonal site and a tetragonal site. (b) Calculated phase stability regions versus μCu and μX (referring to the chemical potential of Cu and X from that of their elementary substance) from left to right for the X site of I, Br, and Cl element and up to down for Cs and Rb element on A site, respectively. The cyan polygon region represents thermodynamic stability growth region, which is encircled by possible competing phases using colored line (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of CHPs with 123-type, they all own octahedral structure with the space group of Cmcm (No. 63), composed of edge-sharing [CuX4] tetrahedron 1D chain. (b) Calculated thermodynamic stability regions of ACu2X3 (A = Rb and Cs; X = Cl, Br, and I) CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The above from left to right is the CHP for the X site of I, Br, and Cl element, and up to down is for Cs and Rb element on A site, respectively. The cyan polygon region represents thermodynamic stable interval, which is surrounded by competing phases using colored line (red, blue, orange, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 2. (Color online) (a) The structure model of CHPs with 123-type, they all own octahedral structure with the space group of Cmcm (No. 63), composed of edge-sharing [CuX4] tetrahedron 1D chain. (b) Calculated thermodynamic stability regions of ACu2X3 (A = Rb and Cs; X = Cl, Br, and I) CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The above from left to right is the CHP for the X site of I, Br, and Cl element, and up to down is for Cs and Rb element on A site, respectively. The cyan polygon region represents thermodynamic stable interval, which is surrounded by competing phases using colored line (red, blue, orange, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of CHPs with 213-type, they possess isostructural model with Pnma symmetry, which is composed of 1D [Cu–X] tetrahedron chain with isolated alkali metal cation (Rb+ , Cs+ ). (b) Calculated phase stability regions in cyan polygon of A2CuX3 (A = Cs and Rb; X = I, Br, and Cl) CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region indicates thermodynamic phase stability growth interval, which is encompassed by competing phases with colored line (red, blue, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 3. (Color online) (a) The structure model of CHPs with 213-type, they possess isostructural model with Pnma symmetry, which is composed of 1D [Cu–X] tetrahedron chain with isolated alkali metal cation (Rb+ , Cs+ ). (b) Calculated phase stability regions in cyan polygon of A2CuX3 (A = Cs and Rb; X = I, Br, and Cl) CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region indicates thermodynamic phase stability growth interval, which is encompassed by competing phases with colored line (red, blue, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of 459-type CHPs with space group of Pc, they own isolated [Cu5X9]4– anion with three types of Cu+ ions, a tetrahedral site, a trigonal site and a 2-fold coordination site. (b) Calculated thermodynamic stability regions of 459-type CHPs against μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region reveals thermodynamic stable growth interval and each colored line corresponds to one most probable competing phase. A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 4. (Color online) (a) The structure model of 459-type CHPs with space group of Pc, they own isolated [Cu5X9]4– anion with three types of Cu+ ions, a tetrahedral site, a trigonal site and a 2-fold coordination site. (b) Calculated thermodynamic stability regions of 459-type CHPs against μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region reveals thermodynamic stable growth interval and each colored line corresponds to one most probable competing phase. A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of 214-type CHPs, most of them possess octahedral space group Pnma with isolated [Cu–X] tetrahedron. But for Rb2CuCl4, it owns Cmca symmetry with 2D [Cu2Cl4]2– layers, induced by [Cu-Cl] octahedron Jahn-Teller distortion. (b) Calculated thermodynamic stability regions of A2CuX4 (A = Rb and Cs; X = Cl, Br, and I) halide perovskites versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The horizontal and vertical axis is from I to Cl element and from Cs to Rb element, respectively. The cyan polygon region shows thermodynamic stability growth interval, which is encircled by most probable competing phases with colored lines (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 5. (Color online) (a) The structure model of 214-type CHPs, most of them possess octahedral space group Pnma with isolated [Cu–X] tetrahedron. But for Rb2CuCl4, it owns Cmca symmetry with 2D [Cu2Cl4]2– layers, induced by [Cu-Cl] octahedron Jahn-Teller distortion. (b) Calculated thermodynamic stability regions of A2CuX4 (A = Rb and Cs; X = Cl, Br, and I) halide perovskites versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The horizontal and vertical axis is from I to Cl element and from Cs to Rb element, respectively. The cyan polygon region shows thermodynamic stability growth interval, which is encircled by most probable competing phases with colored lines (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of 113-type CHPs, even though they possess different structures, they all have the same [CuX6] octahedron unit via face- and corner-sharing. (b) Calculated thermodynamic stability regions of ACuX3 (A = Rb and Cs; X = Cl, Br, and I) versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The horizontal and vertical axis is from I to Cl element and from Cs to Rb element, respectively. The cyan polygon region represents thermodynamic stable growth interval, which is surrounded by most probable competing phases using colored line (red, blue, orange, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 6. (Color online) (a) The structure model of 113-type CHPs, even though they possess different structures, they all have the same [CuX6] octahedron unit via face- and corner-sharing. (b) Calculated thermodynamic stability regions of ACuX3 (A = Rb and Cs; X = Cl, Br, and I) versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The horizontal and vertical axis is from I to Cl element and from Cs to Rb element, respectively. The cyan polygon region represents thermodynamic stable growth interval, which is surrounded by most probable competing phases using colored line (red, blue, orange, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    (Color online) (a) The structure model of 327-type CHPs, they all own tetragonal space group Ccca with isolated [Cu2X7]3– anion composing of elongated [Cu–X] octahedron unit. (b) Calculated thermodynamic stability regions of 327-type CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region represents phase stability growth condition, which is encircled by competing phases using colored line (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    Fig. 7. (Color online) (a) The structure model of 327-type CHPs, they all own tetragonal space group Ccca with isolated [Cu2X7]3– anion composing of elongated [Cu–X] octahedron unit. (b) Calculated thermodynamic stability regions of 327-type CHPs versus μCu and μX (deviation of actual chemical potential of Cu and X from that of their elementary substance). The cyan polygon region represents phase stability growth condition, which is encircled by competing phases using colored line (red, blue, violet, and pink). A, Cu, and X atoms are in purple, coral and brown, respectively.
    TypeSpace group (No.)RbCs
    ClBrIClBrI
    325Pnma (62)
    123Cmcm (63)
    213Pnma (62)
    459Pc (7)
    214Pnma (62)
    Cmca (64)
    113P6122 (178)
    C2221 (20)
    Pbcn (60)
    327Ccca (68)
    Table 1. The Space group of existing CHPs with various types encompassing 325-, 123-, 213-, 459-, 214-, 113-, and 327-type from inorganic crystal structure database (ICSD). ‘√’ and blank grid symbol indicates the existing and non-existing phase in experiment, respectively.
    CompoundΔHd (meV/atom) Optimal decomposition pathway
    325-typeCs3Cu2I525Cs3Cu2I5 → 2CsI + CsCu2I3
    Cs3Cu2Br529Cs3Cu2Br5 → 2CsBr + CsCu2Br3
    Cs3Cu2Cl533Cs3Cu2Cl5 → Cu + CsCl + Cs2CuCl4
    Rb3Cu2I513Rb3Cu2I5 → 2RbI + RbCu2I3
    Rb3Cu2Br55Rb3Cu2Br5 → 4/3Rb2CuBr3 + 1/3RbCu2Br3
    Rb3Cu2Cl5–2Rb3Cu2Cl5 → 7/5RbCl + 2/5Rb4Cu5Cl9
    123-typeCsCu2I30CsCu2I3 → 4/3CuI + 1/3Cs3Cu2I5
    CsCu2Br322CsCu2Br3 → 4/3CuBr + 1/3Cs3Cu2Br5
    CsCu2Cl324CsCu2Cl3 → 4/3CuCl + 1/3Cu3Cu2Cl5
    RbCu2I323RbCu2I3 → RbI + 2CuI
    RbCu2Br328RbCu2Br3 → 3/2CuBr + 1/2Rb2CuBr3
    RbCu2Cl36RbCu2Cl3 → 3/4CuCl + 1/4Rb4Cu5Cl9
    213-typeCs2CuI3–22Cs2CuI3 → 1/2CsI + 1/2Cs3Cu2I5
    Cs2CuBr3–16Cs2CuBr3 → 1/2CsBr + 1/2Cs3Cu2Br5
    Cs2CuCl3–19Cs2CuCl3 → 1/2CsCl + 1/2Cs3Cu2Cl5
    Rb2CuI36Rb2CuI3 → 3/2RbI + 1/2RbCu2I3
    Rb2CuBr36Rb2CuBr3 → 3/2RbBr + 1/2RbCu2Br3
    Rb2CuCl38Rb2CuCl3 → 1/2Cu + RbCl + 1/2Rb2CuCl4
    459-typeCs4Cu5I9–20Cs4Cu5I9 → 3/4Cs3Cu2I5 + 7/4CsCu2I3
    Cs4Cu5Br9–9Cs4Cu5Br9 → 3/4Cs3Cu2Br5 + 7/4CsCu2Br3
    Cs4Cu5Cl98Cs4Cu5Cl9 → 3/4Cs3Cu2Cl5 + 7/4CsCu2Cl3
    Rb4Cu5I9–17Rb4Cu5I9 → 3/2RbI + 5/2RbCu2I3
    Rb4Cu5Br9–4Rb4Cu5Br9 → Rb2CuBr3 + 2RbCu2Br3
    Rb4Cu5Cl922Rb4Cu5Cl9 → 12/5Cu + 1/5Rb2CuCl3 + 6/5Rb3Cu2Cl7
    214-typeCs2CuI4–17Cs2CuI4 → 1/2CsI3 + 1/2Cs3Cu2I5
    Cs2CuBr414Cs2CuBr4 → 1/2CsBr + 1/4CsBr3 + 1/2CsCuBr3 + 1/4Cs3Cu2Br5
    Cs2CuCl434Cs2CuCl4 → CsCl + CsCuCl3
    Rb2CuI4–2Rb2CuI4 → RbI + 1/2RbI3 + 1/2RbCu2I3
    Rb2CuBr410Rb2CuBr4 → 2RbBr + CuBr2
    Rb2CuCl4–9Rb2CuCl4 → 1/2RbCl + 1/2Rb3Cu2Cl7
    113-typeCsCuI3–34CsCuI3 → 1/2CsI3 + 1/2CsCu2I3
    CsCuBr319CsCuBr3 → 1/2CuBr2 + 1/2Cs2CuBr4
    CsCuCl35CsCuCl3 → 1/2CuCl2 + 1/2Cs2CuCl4
    RbCuI3–42RbCuI3 → 1/2RbI3 + 1/2RbCu2I3
    RbCuBr321RbCuBr3 → RbBr + CuBr2
    RbCuCl3–10RbCuCl3 → 1/3CuCl2 + 1/3Rb3Cu2Cl7
    327-typeCs3Cu2I7–31Cs3Cu2I7 → CsI3 + 1/2Cs3Cu2I5 + 1/2CsCu2I3
    Cs3Cu2Br79Cs3Cu2Br7 → Cs2CuBr4 + CsCuBr3
    Cs3Cu2Cl79Cs3Cu2Cl7 → CsCuCl3 + Cs2CuCl4
    Rb3Cu2I7–31Rb3Cu2I7 → RbI + RbI3 + RbCu2I3
    Rb3Cu2Br723Rb3Cu2Br7 → 3RbBr + 2CuBr2
    Rb3Cu2Cl715Rb3Cu2Cl7 → Rb2CuCl4 + RbCuCl3
    Table 2. Calculated decomposition energies together with ODP in the CHPs AlCumXn (A = Rb and Cs; X = Cl, Br, and I; l, m, and n are integers).
    Space groupCs2CuI4Rb2CuI4Rb2CuBr4
    Pnma0.000.000.00
    Cmca0.290.330.04
    Table 3. The relative energy per formula unit (eV/f.u.) of 214-type CHPs including Cs2CuI4, Rb2CuI4, and Rb2CuBr4 in the different space group encompassing Pnma and Cmca, which are all non-existing phase in the ICSD.
    Space groupCsCuI3RbCuI3RbCuBr3
    C22210.000.000.00
    P6122 0.030.020.10
    Pbcn0.150.090.11
    Table 4. The relative energy per formula unit (eV/f.u.) of 113-type CHP including CsCuI3, RbCuI3, and RbCuBr3 in the different space group containing C2221, P6122, Pbcn, which are non-existing phase in the ICSD.
    ABX325123213459214113327
    Note: 1: Decomposition energy. 2: Stability region. √: Stable. × : Non-stable. : Exist.
    CsCuI××××××××××
    Br××××
    Cl××
    RbI××××××××
    Br××
    Cl×××××××
    Table 5. Summary for the stability region and decomposition energy of ODP in the different type CHPs AlBmXn (A = Rb and Cs; B = Cu; X = Cl, Br, and I; l, m, and n are integers; named as lmn-type). For each type CHP, number 1 and 2 represent decomposition energy and stability region, respectively. ‘√’ and ‘×’ symbols indicate ‘stable’ and ‘non-stable’ phase, respectively. Yellow square shows that this type is existing phase from inorganic Crystal Structure Database (ICSD).
    Zhongti Sun, Xiwen Chen, Wanjian Yin. Comprehensive first-principles studies on phase stability of copper-based halide perovskite derivatives AlCumXn (A = Rb and Cs; X = Cl, Br, and I)[J]. Journal of Semiconductors, 2020, 41(5): 052201
    Download Citation