Description of the dataset

List of files

| Name | Description | |------------------------------------------|-------------------------------------------------------------------------------| | Figures_for_paper_1_normal_state.ipynb | Notebook containing theoretical plots for the normal state | | Figures_for_paper_2_BdG.ipynb | Notebook containing theoretical plots for the superconducting state | | util.py | Python function used in plotting of theoretical results | | export.aiida | AiiDA archive containing full provenance of the DFT calculations | | struct_PdTe2Bi.xsf | Relaxed structure of PdTe2/Bi2/Bi2Te3 | | struct_PtTe2Bi.xsf | Relaxed structure of PtTe2/Bi2/Bi2Te3 | | struct_TiTe2Bi.xsf | Relaxed structure of TiTe2/Bi2/Bi2Te3 | | struct_NbTe2Bi.xsf | Relaxed structure of NbTe2/Bi2/Bi2Te3 | | struct_PdTe2.xsf | Relaxed structure of PdTe2/Bi2Te3 | | struct_PtTe2.xsf | Relaxed structure of PtTe2/Bi2Te3 | | struct_TiTe2.xsf | Relaxed structure of TiTe2/Bi2Te3 | | struct_NbTe2.xsf | Relaxed structure of NbTe2/Bi2Te3 | | requirements.txt | Requirements file for used python environment | | Transport_data.zip | Compressed folder containing the data from transport experiments of this work |

Additional information for the theory data

UUID of calculations

The 'nTI' addition means the calculation was done for n-doped TI, and the 'Bi2' part of the name indicates the additional Bi2 layer between XTe2 and Bi2Te3.

bandstructure calculations used in normal state figures

| Name | UUID | |---------------|----------------------------------------| | PtTe2_nTI | c67fce15-86e0-4c58-81e5-4da458f1c1e0 | | PdTe2_nTI | a6b6dbba-eed1-480d-a369-8e7af3d9f995 | | NbTe2_nTI | 5fd81c50-e443-441d-8d4f-8e1f3637b23e | | TiTe2_nTI | 259cd110-ced1-4aa0-b6d8-fb6a098b8faa | | PtTe2_Bi2_nTI | 41d27e83-fe60-4193-9871-705b228a8388 | | PdTe2_Bi2_nTI | cbde254c-be3e-4bcc-bdfa-d2806dfb3338 | | NbTe2_Bi2_nTI | 5330ed92-302f-4034-800f-a0078f45867e | | TiTe2_Bi2_nTI | bf6fa45f-eb97-4ae6-b3af-a8c8c568c38d | | PtTe2 | 780b6d97-abad-45a7-9f9e-a319b8598470 | | PdTe2 | e40d257f-3ab7-4aea-8f9d-77d2ab7ade8d | | NbTe2 | 3add16cb-a62c-4938-b3aa-06ecf6bbd72f | | TiTe2 | 6c3c8752-d12a-44af-b3b9-fe05f74b689e | | PtTe2_Bi2 | 41d27e83-fe60-4193-9871-705b228a8388 | | PdTe2_Bi2 | cbde254c-be3e-4bcc-bdfa-d2806dfb3338 | | NbTe2_Bi2 | 6c0dd5a5-2c20-4315-bd56-320ec772e06c | | TiTe2_Bi2 | 744fe188-dcea-448c-9bd2-3117356a5fbe |

$\overline{\chi}$ calculations for the SC state

| Name | UUID | |---------------|----------------------------------------| | PtTe2 | 5d1c6b7c-8063-4c7c-8303-b019375441ac | | PtTe2_nTI | b819aa78-e0d8-4d34-9c51-e443bc935a6b | | PdTe2 | 4625f596-713a-4bf0-91ac-135dfadfcdce | | PdTe2_nTI | 687c84d4-b95d-4e47-911a-7a4e75439df1 | | NbTe2 | bcd6f4bf-cd5e-44cb-a92f-7ab43950895b | | NbTe2_nTI | 3d6ba41c-59e6-407d-b77b-d80184fbe956 | | TiTe2 | 119c6cf4-f405-44ba-a7ca-04bea0ac0a3f | | TiTe2_nTI | 86145f11-305a-4641-84e9-fdc1fa13eba1 | | PtTe2_Bi2 | 1e2b9d7e-ee41-43e4-a898-8ac68b2c378f | | PdTe2_Bi2 | c2360b63-a9ea-4cc8-86e6-ea0a7d4e8682 | | NbTe2_Bi2 | 4ef2a45f-0c76-480e-8758-fb349760f0c1 | | NbTe2_Bi2_nTI | 1f4df7aa-189a-43b3-a2c2-9a2b11831882 | | TiTe2_Bi2 | 0995c730-564a-46cb-a17a-343918272b1c | | TiTe2_Bi2_nTI | d95c59ed-e239-4f58-bc7e-3e78b26fafe1 |

SC DOS calculations

| Name | UUID | |---------------|----------------------------------------| | PtTe2_nTI | 402aa788-569a-4102-953d-051efb2210ff | | PdTe2_nTI | 139f9031-28f2-4226-8895-cb000b28954c | | NbTe2_Bi2_nTI | 2b3d73e8-23be-4cd3-ad29-15dacd90231e | | TiTe2_Bi2_nTI | 837e0f21-7304-40e3-9615-d3dedcdeaf08 |