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Information card for entry 4126200
Preview
Coordinates | 4126200.cif |
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Original paper (by DOI) | HTML |
Formula | C660 H570 Eu10 N90 O60 |
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Calculated formula | C660 H570 Eu10 N90 O60 |
SMILES | [Eu]12345678[n]9c(C(N[C@@H](c%10ccccc%10)C)=[O]2)cccc9C(Nc2ccc(cc2)C=Cc2ccc(cc2)NC2c9cccc%10C(N[C@@H](c%11ccccc%11)C)=[O][Eu]%11%12%13%14%15([n]9%10)([O]=2)[n]2c(C(Nc9ccc(C=Cc%10ccc(cc%10)NC%10c%16cccc%17C(N[C@@H](c%18ccccc%18)C)=[O][Eu]%18%19%20%21([n]%22c(C(Nc%23ccc(C=Cc%24ccc(cc%24)NC(c%24cccc([n]1%24)C(N[C@@H](c1ccccc1)C)=[O]3)=[O]5)cc%23)=[O]%18)cccc%22C(N[C@H](C)c1ccccc1)=[O]%19)([n]%16%17)([n]1c(C(N[C@@H](c3ccccc3)C)=[O]%20)cccc1C(Nc1ccc(cc1)C=Cc1ccc(cc1)NC1c3cccc5C(N[C@H](C)c%16ccccc%16)=[O][Eu]%16%17%18%19([n]%20c(C(N[C@@H](c%22ccccc%22)C)=[O]%16)cccc%20C(Nc%16ccc(cc%16)C=Cc%16ccc(cc%16)NC(c%16cccc(C(N[C@H](C)c%20ccccc%20)=[O]%15)[n]%11%16)=[O]%13)=[O]%18)([n]%11c(C(N[C@@H](c%13ccccc%13)C)=[O]%17)cccc%11C(Nc%11ccc(cc%11)C=Cc%11ccc(cc%11)NC(c%11cccc(C(N[C@H](C)c%13ccccc%13)=[O]8)[n]6%11)=[O]7)=[O]%19)([n]35)[O]=1)=[O]%21)[O]=%10)cc9)=[O]%12)cccc2C(N[C@H](C)c1ccccc1)=[O]%14)=[O]4.[Eu]12345678[n]9c(C(N[C@@H](c%10ccccc%10)C)=[O]3)cccc9C(Nc3ccc(cc3)C=Cc3ccc(cc3)NC3c9cccc%10C(N[C@H](C)c%11ccccc%11)=[O][Eu]%11%12%13%14([n]9%10)([n]9c(C(Nc%10ccc(C=Cc%15ccc(cc%15)NC(c%15cccc(C(N[C@@H](c%16ccccc%16)C)=[O]4)[n]1%15)=[O]7)cc%10)=[O]%11)cccc9C(N[C@H](C)c1ccccc1)=[O]%13)([n]1c(C(Nc4ccc(C=Cc7ccc(cc7)NC(c7cccc(C(N[C@@H](c9ccccc9)C)=[O]5)[n]27)=[O]8)cc4)=[O]%12)cccc1C(N[C@H](C)c1ccccc1)=[O]%14)[O]=3)=[O]6.[Eu]12345678[n]9c(C(N[C@@H](c%10ccccc%10)C)=[O]3)cccc9C(Nc3ccc(cc3)C=Cc3ccc(cc3)NC3c9cccc%10C(N[C@H](C)c%11ccccc%11)=[O][Eu]%11%12%13%14([n]9%10)([n]9c(C(Nc%10ccc(C=Cc%15ccc(cc%15)NC(c%15cccc(C(N[C@@H](c%16ccccc%16)C)=[O]4)[n]1%15)=[O]7)cc%10)=[O]%11)cccc9C(N[C@H](C)c1ccccc1)=[O]%13)([n]1c(C(Nc4ccc(C=Cc7ccc(cc7)NC(c7cccc(C(N[C@@H](c9ccccc9)C)=[O]5)[n]27)=[O]8)cc4)=[O]%12)cccc1C(N[C@H](C)c1ccccc1)=[O]%14)[O]=3)=[O]6.[Eu]12345678[n]9c(C(N[C@@H](c%10ccccc%10)C)=[O]3)cccc9C(Nc3ccc(cc3)C=Cc3ccc(cc3)NC3c9cccc%10C(N[C@H](C)c%11ccccc%11)=[O][Eu]%11%12%13%14([n]9%10)([n]9c(C(Nc%10ccc(C=Cc%15ccc(cc%15)NC(c%15cccc(C(N[C@@H](c%16ccccc%16)C)=[O]4)[n]1%15)=[O]7)cc%10)=[O]%11)cccc9C(N[C@H](C)c1ccccc1)=[O]%13)([n]1c(C(Nc4ccc(C=Cc7ccc(cc7)NC(c7cccc(C(N[C@@H](c9ccccc9)C)=[O]5)[n]27)=[O]8)cc4)=[O]%12)cccc1C(N[C@H](C)c1ccccc1)=[O]%14)[O]=3)=[O]6 |
Title of publication | Evolution of Luminescent Supramolecular Lanthanide M2nL3n Complexes from Helicates and Tetrahedra to Cubes. |
Authors of publication | Li, Xiao-Zhen; Zhou, Li-Peng; Yan, Liang-Liang; Yuan, Da-Qiang; Lin, Chen-Sheng; Sun, Qing-Fu |
Journal of publication | Journal of the American Chemical Society |
Year of publication | 2017 |
Journal volume | 139 |
Journal issue | 24 |
Pages of publication | 8237 - 8244 |
a | 61.483 ± 0.007 Å |
b | 61.483 ± 0.007 Å |
c | 61.483 ± 0.007 Å |
α | 90° |
β | 90° |
γ | 90° |
Cell volume | 232416 ± 5 Å3 |
Cell temperature | 293 ± 2 K |
Ambient diffraction temperature | 293 ± 2 K |
Number of distinct elements | 5 |
Space group number | 199 |
Hermann-Mauguin space group symbol | I 21 3 |
Hall space group symbol | I 2b 2c 3 |
Residual factor for all reflections | 0.1349 |
Residual factor for significantly intense reflections | 0.1308 |
Weighted residual factors for significantly intense reflections | 0.3287 |
Weighted residual factors for all reflections included in the refinement | 0.3421 |
Goodness-of-fit parameter for all reflections included in the refinement | 1.906 |
Diffraction radiation wavelength | 1 Å |
Diffraction radiation type | Synchrotron |
Has coordinates | Yes |
Has disorder | No |
Has Fobs | No |
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The link is: https://www.crystallography.net/4126200.html
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