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        <datestamp>2026-01-08T16:02:57Z</datestamp>
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          <dc:title>Magnetic Hysteresis at 31 K in a Four-Coordinate Dysprosium(III) Amide Complex</dc:title>
          <dc:creator>Benjamin Reant (9181130)</dc:creator>
          <dc:creator>John A. Seed (9181147)</dc:creator>
          <dc:creator>William J. A. Blackmore (11873154)</dc:creator>
          <dc:creator>Meagan Oakley (18246466)</dc:creator>
          <dc:creator>Conrad Goodwin (11850479)</dc:creator>
          <dc:creator>Nicolaj Kofod (6384143)</dc:creator>
          <dc:subject>Crystallography</dc:subject>
          <dc:subject>F-block chemistry</dc:subject>
          <dc:subject>Organometallic chemistry</dc:subject>
          <dc:subject>Dysprosium</dc:subject>
          <dc:subject>Single Molecule Magnet</dc:subject>
          <dc:subject>Amide</dc:subject>
          <dc:subject>Hysteresis</dc:subject>
          <dc:subject>Magnetic</dc:subject>
          <dc:description>&lt;p dir="ltr"&gt;Supporting data for: 10.1021/jacs.5c13255.&lt;/p&gt;&lt;p dir="ltr"&gt;Contains raw files for: ATR-IR, Luminescence, NMR, PXRD, SQUID magnetometry, UV-Vis-NIR data, and processed SC-XRD data.&lt;/p&gt;&lt;p dir="ltr"&gt;Manuscript abstract:&lt;/p&gt;&lt;p dir="ltr"&gt;The state-of-the-art in single-molecule magnet (SMM) design is dominated by charged dysprosium sandwich complexes with mono- or dianionic π-ligands and which exhibit some of the highest open-loop magnetic hysteresis temperatures (&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;H&lt;/sub&gt;), the highest 100 s blocking temperatures (&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;B100&lt;/sub&gt;) and some of the largest barriers to magnetic reversal (&lt;i&gt;U&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt;). Architectures that leverage more charge-dense ligands, such as amides or alkoxides, with axial coordination and weak equatorial interactions can generate larger crystal fields (CFs), and hence larger &lt;i&gt;U&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt; values; however, this is often not accompanied by correspondingly high &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;H&lt;/sub&gt; or &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;B100&lt;/sub&gt; values. Here we report a four-coordinate dysprosium(III) single-molecule magnet, [Dy{Me&lt;sub&gt;2&lt;/sub&gt;Si(NSi&lt;i&gt;i&lt;/i&gt;Pr&lt;sub&gt;3&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;}&lt;sub&gt;2&lt;/sub&gt;{K(toluene)&lt;sub&gt;2&lt;/sub&gt;}]&lt;sub&gt;n&lt;/sub&gt; (&lt;b&gt;1Dy&lt;/b&gt;), with charge-dense amide donors, but a coordination environment that is between axial and tetrahedral in structure. Nevertheless, &lt;b&gt;1Dy&lt;/b&gt; displays open-loop magnetic hysteresis up to 31 K using sweep rates of 22 Oe s&lt;sup&gt;–1&lt;/sup&gt;. The coercive field (&lt;i&gt;H&lt;/i&gt;&lt;sub&gt;C&lt;/sub&gt;) is 1.65 T at 1.8 K, and &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;B100&lt;/sub&gt; = 10.4 K. &lt;i&gt;Ab initio&lt;/i&gt; calculations show the four-coordinate geometry imparts a strong axial CF as the &lt;sup&gt;6&lt;/sup&gt;H&lt;sub&gt;15/2&lt;/sub&gt; spin-orbit multiplet is split over 1,958 K (1,361 cm&lt;sup&gt;–1&lt;/sup&gt;). The experimental &lt;i&gt;U&lt;/i&gt;eff (742 K, 516 cm–1) is smaller and resides near the energy of the third excited Kramers doublet. &lt;i&gt;Ab initio&lt;/i&gt; spin dynamics calculations show that the fitted barrier height at high T (&gt;45 K) is 559 cm&lt;sup&gt;–1&lt;/sup&gt;. Non-Kramers ion analogues &lt;b&gt;1Tb&lt;/b&gt; and &lt;b&gt;1Ho&lt;/b&gt; show waist-restricted hysteresis and short relaxation times at all temperatures. The magnetic properties of &lt;b&gt;1Dy&lt;/b&gt; place it highly amongst monometallic lanthanide SMMs using an alternative design strategy, which is synthetically simple and may be further refined.&lt;/p&gt;</dc:description>
          <dc:date>2026-01-08T16:02:57Z</dc:date>
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          <dc:identifier>10.48420/29673917.v1</dc:identifier>
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