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| 1 | +============================================ |
| 2 | +Parametrization for metal halide perovskites |
| 3 | +============================================ |
| 4 | + |
| 5 | +(c) 2017, Marcus Elstner, Karlsruher Institut für Technologie |
| 6 | +[original mio set] |
| 7 | + |
| 8 | +(c) 2024, Junke Jiang, INSA Rennes |
| 9 | +[extension with I, Cs, Pb, recalculating all tables for consistency] |
| 10 | + |
| 11 | +All rights reserved |
| 12 | + |
| 13 | +This work is licensed under the Creative Commons Attribution-ShareAlike 4.0 |
| 14 | +International License. To view a copy of this license, consult the LICENSE file |
| 15 | +or visit http://creativecommons.org/licenses/by-sa/4.0/ . |
| 16 | + |
| 17 | +NOTE: The rights holder(s) for this work explicitly require that the attribution |
| 18 | +conditions of this license are enforced. Use in part or in whole of this data is |
| 19 | +permitted only under the condition that the scientific background of the |
| 20 | +Licensed Material will be CITED IN ANY PUBLICATIONS ARISING FROM ITS USE. The |
| 21 | +required references are specified in this file and must be included in resulting |
| 22 | +works. |
| 23 | + |
| 24 | + |
| 25 | +General information |
| 26 | +=================== |
| 27 | + |
| 28 | +This set was designed to describe the electronic structure of 2D and 3D metal |
| 29 | +halide perovskites. The parameters of H, C, and N may slightly deviate from mio-1-1. |
| 30 | +We refer to the detailed documentation in the Slater-Koster files for further |
| 31 | +information. The compression radii of Cs have been taken from Ref.[JCTC13], the |
| 32 | +power of the confinement potential, however, is slightly different. |
| 33 | + |
| 34 | +Note: This set assumes that you use shell-resolved SCC in DFTB. In case you use |
| 35 | +the DFTB+ code, you can achieve it by setting `OrbitalResolvedSCC = Yes`. |
| 36 | + |
| 37 | + |
| 38 | +Maximal angular momenta |
| 39 | +----------------------- |
| 40 | +H: s |
| 41 | +C: p |
| 42 | +N: p |
| 43 | +I: p |
| 44 | +Cs: s |
| 45 | +Pb: p |
| 46 | + |
| 47 | + |
| 48 | +Spin constants |
| 49 | +-------------- |
| 50 | + |
| 51 | +Note, the calculation of the spin constants follows here for all elements the |
| 52 | +convention as used for the Hubbard U values: For non-occupied atomic orbitals |
| 53 | +(orbitals above HOMO), the corresponding value of the HOMO is used. |
| 54 | + |
| 55 | +H: |
| 56 | + -0.07174 |
| 57 | +C: |
| 58 | + -0.03062 -0.02505 |
| 59 | + -0.02505 -0.02265 |
| 60 | +N: |
| 61 | + -0.03318 -0.02755 |
| 62 | + -0.02755 -0.02545 |
| 63 | +Cs: |
| 64 | + -0.00949 |
| 65 | +I: |
| 66 | + -0.01445 -0.01132 |
| 67 | + -0.01132 -0.01145 |
| 68 | +Pb: |
| 69 | + -0.01335 -0.00932 |
| 70 | + -0.00932 -0.01097 |
| 71 | + |
| 72 | + |
| 73 | +Repulsive energy: |
| 74 | +======================================== |
| 75 | + |
| 76 | +NOTABENE: NO REPULSIVE potential is provided; there is a dummy spline only. |
| 77 | + The SKFs CANNOT be used to do structural relaxation. |
| 78 | + |
| 79 | + |
| 80 | +Relevant publications |
| 81 | +===================== |
| 82 | + |
| 83 | +[PRMat25] J. Jiang et al., Phys. Rev. Materials 9, 023803 (2025). |
| 84 | + |
| 85 | +[JCTC13] M. Wahiduzzaman et al., J. Chem. Theory Comput. 9, 9, 4006 (2013). |
| 86 | + |
| 87 | +[PRB98] M. Elstner, D. Porezag, G. Jungnickel, J. Elsner, M. Haugk, |
| 88 | +Th. Frauenheim, S. Suhai, and G. Seifert, Phys. Rev. B 58, 7260 (1998). |
| 89 | + |
| 90 | + |
| 91 | +Required references |
| 92 | +=================== |
| 93 | + |
| 94 | +H,C,N - H,C,N: [PRMat25,PRB98] |
| 95 | +H,C,N,I,Cs,Pb - I: [PRMat25] |
| 96 | +H,C,N,I,Cs,Pb - Cs: [PRMat25,JCTC13] |
| 97 | +H,C,N,I,Cs,Pb - Pb: [PRMat25] |
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