| کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
|---|---|---|---|---|
| 1336013 | 1500291 | 2011 | 4 صفحه PDF | دانلود رایگان |
On the basis of the experimentally synthesized [(PY5Me2)4Mn4Re(CN)7]5+, the theoretically modeled clusters of [(PY5Me2)4V4Re(CN)7]5+ and [(PY5Me2)4Ni4Re(CN)7]5+ both have strong magnetic anisotropy energy barriers.
Two theoretically modeled clusters of [(PY5Me2)4V4Re(CN)7]5+ and [(PY5Me2)4Ni4Re(CN)7]5+ both have strong magnetic anisotropy energy barriers on the basis of the experimentally synthesized [(PY5Me2)4Mn4Re(CN)7]5+.Figure optionsDownload as PowerPoint slideHighlights
► The couplings of Mn4Re and V4Re are antiferromagnetic and that of Ni4Re is ferromagnetic.
► Two modeled cyano-bridged magnets V4Re and Ni4Re both have strong anisotropy barriers.
► The more closely orthogonal hard axes may be responsible for the larger negative D values of the optimized V4Re and Ni4Re.
► The largest local D and the most closely orthogonal hard axes of [PY5Me2Ni(CN)]+ are responsible for the largest D of the optimized Ni4Re.
► The larger Mn–N≡C angle is responsible for the larger calculated D value of the optimized Mn4Re.
Journal: Polyhedron - Volume 30, Issue 18, 28 November 2011, Pages 3228–3231