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Information card for entry 7044858
Preview
| Coordinates | 7044858.cif |
|---|---|
| Original paper (by DOI) | HTML |
| External links | PubChem |
| Formula | C40 H112 I3 N8 O10 P4 Tb |
|---|---|
| Calculated formula | C40 H112 I3 N8 O10 P4 Tb |
| SMILES | C(C)(C)(C)P(NC(C)C)(NC(C)C)=[O][Tb]([O]=P(C(C)(C)C)(NC(C)C)NC(C)C)([OH2])([OH2])([OH2])([OH2])[OH2].C(C)(C)(C)P(=O)(NC(C)C)NC(C)C.C(C)(C)(C)P(=O)(NC(C)C)NC(C)C.[I-].[I-].[I-].O |
| Title of publication | Is a strong axial crystal-field the only essential condition for a large magnetic anisotropy barrier? The case of non-Kramers Ho(iii) versus Tb(iii ). |
| Authors of publication | Gupta, Sandeep K.; Rajeshkumar, Thayalan; Rajaraman, Gopalan; Murugavel, Ramaswamy |
| Journal of publication | Dalton transactions (Cambridge, England : 2003) |
| Year of publication | 2018 |
| Journal volume | 47 |
| Journal issue | 2 |
| Pages of publication | 357 - 366 |
| a | 13.789 ± 0.002 Å |
| b | 14.794 ± 0.002 Å |
| c | 20.679 ± 0.004 Å |
| α | 92.515 ± 0.015° |
| β | 108.184 ± 0.013° |
| γ | 115.182 ± 0.012° |
| Cell volume | 3549.4 ± 1.1 Å3 |
| Cell temperature | 120 ± 2 K |
| Ambient diffraction temperature | 120 ± 2 K |
| Number of distinct elements | 7 |
| Space group number | 2 |
| Hermann-Mauguin space group symbol | P -1 |
| Hall space group symbol | -P 1 |
| Residual factor for all reflections | 0.0497 |
| Residual factor for significantly intense reflections | 0.0462 |
| Weighted residual factors for significantly intense reflections | 0.1012 |
| Weighted residual factors for all reflections included in the refinement | 0.1047 |
| Goodness-of-fit parameter for all reflections included in the refinement | 1.054 |
| Diffraction radiation wavelength | 0.71075 Å |
| Diffraction radiation type | MoKα |
| Has coordinates | Yes |
| Has disorder | No |
| Has Fobs | No |
For the version history of this entry, please navigate to main COD server.
The link is: https://www.crystallography.net/7044858.html
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