<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Gregson M</submitter><funding>European Research Council</funding><funding>University Of Manchester</funding><funding>European Cooperation in Science and Technology</funding><funding>Royal Society</funding><funding>University Of Nottingham</funding><funding>Engineering and Physical Sciences Research Council</funding><pagination>155-165</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC5950554</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>7(1)</volume><pubmed_abstract>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&lt;sup>TMS&lt;/sup>)(BIPM&lt;sup>TMS&lt;/sup>H)] [Ln = Dy, &lt;b>1Dy&lt;/b>; Y, &lt;b>1Y&lt;/b>; BIPM&lt;sup>TMS&lt;/sup> = {C(PPh&lt;sub>2&lt;/sub>NSiMe&lt;sub>3&lt;/sub>)&lt;sub>2&lt;/sub>}&lt;sup>2-&lt;/sup>; BIPM&lt;sup>TMS&lt;/sup>H = {HC(PPh&lt;sub>2&lt;/sub>NSiMe&lt;sub>3&lt;/sub>)&lt;sub>2&lt;/sub>}&lt;sup>-&lt;/sup>] with benzyl potassium/18-crown-6 ether (18C6) in THF afforded [Ln(BIPM&lt;sup>TMS&lt;/sup>)&lt;sub>2&lt;/sub>][K(18C6)(THF)&lt;sub>2&lt;/sub>] [Ln = Dy, &lt;b>2Dy&lt;/b>; Y, &lt;b>2Y&lt;/b>]. AC magnetic measurements of &lt;b>2Dy&lt;/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 &lt;b>2Dy&lt;/b> exhibits two thermally activated energy barriers (&lt;i>U&lt;/i> &lt;sub>eff&lt;/sub>) of 721 and 813 K, the largest &lt;i>U&lt;/i> &lt;sub>eff&lt;/sub> values for any monometallic dysprosium(iii) complex. Dilution experiments confirm the molecular origin of this phenomenon. Complex &lt;b>2Dy&lt;/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, &lt;i>T&lt;/i> &lt;sub>B&lt;/sub>, is found at 10 K. Magnetic hysteresis is also observed in 10% &lt;b>2Dy&lt;/b>@&lt;b>2Y&lt;/b> at these temperatures. &lt;i>Ab initio&lt;/i> calculations suggest the lowest three Kramers doublets of the ground &lt;sup>6&lt;/sup>H&lt;sub>15/2&lt;/sub> multiplet of &lt;b>2Dy&lt;/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 &lt;i>via&lt;/i> the 4&lt;sup>th&lt;/sup> and 5&lt;sup>th&lt;/sup> doublets, verified experimentally for the first time, and calculated &lt;i>U&lt;/i> &lt;sub>eff&lt;/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.</pubmed_abstract><journal>Chemical science</journal><pubmed_title>A monometallic lanthanide bis(methanediide) single molecule magnet with a large energy barrier and complex spin relaxation behaviour.</pubmed_title><pmcid>PMC5950554</pmcid><funding_grant_id>EP/K038869/1</funding_grant_id><funding_grant_id>EP/F030517/1</funding_grant_id><funding_grant_id>1069422</funding_grant_id><pubmed_authors>Tuna F</pubmed_authors><pubmed_authors>Gregson M</pubmed_authors><pubmed_authors>Collison D</pubmed_authors><pubmed_authors>Ariciu AM</pubmed_authors><pubmed_authors>Crowe IF</pubmed_authors><pubmed_authors>McInnes EJL</pubmed_authors><pubmed_authors>Winpenny REP</pubmed_authors><pubmed_authors>Liddle ST</pubmed_authors><pubmed_authors>Lewis W</pubmed_authors><pubmed_authors>Blake AJ</pubmed_authors><pubmed_authors>Chilton NF</pubmed_authors></additional><is_claimable>false</is_claimable><name>A monometallic lanthanide bis(methanediide) single molecule magnet with a large energy barrier and complex spin relaxation behaviour.</name><description>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&lt;sup>TMS&lt;/sup>)(BIPM&lt;sup>TMS&lt;/sup>H)] [Ln = Dy, &lt;b>1Dy&lt;/b>; Y, &lt;b>1Y&lt;/b>; BIPM&lt;sup>TMS&lt;/sup> = {C(PPh&lt;sub>2&lt;/sub>NSiMe&lt;sub>3&lt;/sub>)&lt;sub>2&lt;/sub>}&lt;sup>2-&lt;/sup>; BIPM&lt;sup>TMS&lt;/sup>H = {HC(PPh&lt;sub>2&lt;/sub>NSiMe&lt;sub>3&lt;/sub>)&lt;sub>2&lt;/sub>}&lt;sup>-&lt;/sup>] with benzyl potassium/18-crown-6 ether (18C6) in THF afforded [Ln(BIPM&lt;sup>TMS&lt;/sup>)&lt;sub>2&lt;/sub>][K(18C6)(THF)&lt;sub>2&lt;/sub>] [Ln = Dy, &lt;b>2Dy&lt;/b>; Y, &lt;b>2Y&lt;/b>]. AC magnetic measurements of &lt;b>2Dy&lt;/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 &lt;b>2Dy&lt;/b> exhibits two thermally activated energy barriers (&lt;i>U&lt;/i> &lt;sub>eff&lt;/sub>) of 721 and 813 K, the largest &lt;i>U&lt;/i> &lt;sub>eff&lt;/sub> values for any monometallic dysprosium(iii) complex. Dilution experiments confirm the molecular origin of this phenomenon. Complex &lt;b>2Dy&lt;/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, &lt;i>T&lt;/i> &lt;sub>B&lt;/sub>, is found at 10 K. Magnetic hysteresis is also observed in 10% &lt;b>2Dy&lt;/b>@&lt;b>2Y&lt;/b> at these temperatures. &lt;i>Ab initio&lt;/i> calculations suggest the lowest three Kramers doublets of the ground &lt;sup>6&lt;/sup>H&lt;sub>15/2&lt;/sub> multiplet of &lt;b>2Dy&lt;/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 &lt;i>via&lt;/i> the 4&lt;sup>th&lt;/sup> and 5&lt;sup>th&lt;/sup> doublets, verified experimentally for the first time, and calculated &lt;i>U&lt;/i> &lt;sub>eff&lt;/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.</description><dates><release>2016-01-01T00:00:00Z</release><publication>2016 Jan</publication><modification>2025-04-04T22:41:37.251Z</modification><creation>2025-04-04T22:41:37.251Z</creation></dates><accession>S-EPMC5950554</accession><cross_references><pubmed>29861976</pubmed><doi>10.1039/c5sc03111g</doi></cross_references></HashMap>