Publication | Open Access
A monometallic lanthanide bis(methanediide) single molecule magnet with a large energy barrier and complex spin relaxation behaviour
327
Citations
52
References
2015
Year
We report a dysprosium(iii) bis(methanediide) single molecule magnet (SMM) where stabilisation of the highly magnetic states and suppression of mixing of opposite magnetic projections is imposed by a linear arrangement of negatively-charged donor atoms supported by weak neutral donors. Treatment of [Ln(BIPM<sup>TMS</sup>)(BIPM<sup>TMS</sup>H)] [Ln = Dy, <b>1Dy</b>; Y, <b>1Y</b>; BIPM<sup>TMS</sup> = {C(PPh<sub>2</sub>NSiMe<sub>3</sub>)<sub>2</sub>}<sup>2-</sup>; BIPM<sup>TMS</sup>H = {HC(PPh<sub>2</sub>NSiMe<sub>3</sub>)<sub>2</sub>}<sup>-</sup>] with benzyl potassium/18-crown-6 ether (18C6) in THF afforded [Ln(BIPM<sup>TMS</sup>)<sub>2</sub>][K(18C6)(THF)<sub>2</sub>] [Ln = Dy, <b>2Dy</b>; Y, <b>2Y</b>]. AC magnetic measurements of <b>2Dy</b> in zero DC field show temperature- and frequency-dependent SMM behaviour. Orbach relaxation dominates at high temperature, but at lower temperatures a second-order Raman process dominates. Complex <b>2Dy</b> exhibits two thermally activated energy barriers (<i>U</i> <sub>eff</sub>) of 721 and 813 K, the largest <i>U</i> <sub>eff</sub> values for any monometallic dysprosium(iii) complex. Dilution experiments confirm the molecular origin of this phenomenon. Complex <b>2Dy</b> has rich magnetic dynamics; field-cooled (FC)/zero-field cooled (ZFC) susceptibility measurements show a clear divergence at 16 K, meaning the magnetic observables are out-of-equilibrium below this temperature, however the maximum in ZFC, which conventionally defines the blocking temperature, <i>T</i> <sub>B</sub>, is found at 10 K. Magnetic hysteresis is also observed in 10% <b>2Dy</b>@<b>2Y</b> at these temperatures. <i>Ab initio</i> calculations suggest the lowest three Kramers doublets of the ground <sup>6</sup>H<sub>15/2</sub> multiplet of <b>2Dy</b> are essentially pure, well-isolated |±15/2, |±13/2 and |±11/2 states quantised along the C[double bond, length as m-dash]Dy[double bond, length as m-dash]C axis. Thermal relaxation occurs <i>via</i> the 4<sup>th</sup> and 5<sup>th</sup> doublets, verified experimentally for the first time, and calculated <i>U</i> <sub>eff</sub> values of 742 and 810 K compare very well to experimental magnetism and luminescence data. This work validates a design strategy towards realising high-temperature SMMs and produces unusual spin relaxation behaviour where the magnetic observables are out-of-equilibrium some 6 K above the formal blocking temperature.
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