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        <identifier>oai:figshare.com:article/34034022</identifier>
        <datestamp>2026-09-30T16:28:12Z</datestamp>
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        <oai_dc:dc xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"  xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
          <dc:title>Quantum Mechanical
Insights into Magneto–Structural
Correlations Governing the Magnetic Relaxation of Non-Dysprosium Butterfly-Shaped
{Cr&lt;sup&gt;III&lt;/sup&gt;&lt;sub&gt;2&lt;/sub&gt;Ln&lt;sup&gt;III&lt;/sup&gt;&lt;sub&gt;2&lt;/sub&gt;} (Ln = Pr,
Nd, Tb, Ho, Er) Complexes</dc:title>
          <dc:creator>Amit Gharu (20427405)</dc:creator>
          <dc:creator>Keith S. Murray (1497661)</dc:creator>
          <dc:creator>Stuart K. Langley (1497673)</dc:creator>
          <dc:creator>Kuduva R. Vignesh (3715498)</dc:creator>
          <dc:subject>Biophysics</dc:subject>
          <dc:subject>Biochemistry</dc:subject>
          <dc:subject>Physical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Molecular Biology</dc:subject>
          <dc:subject>Physiology</dc:subject>
          <dc:subject>Chemical Sciences not elsewhere classified</dc:subject>
          <dc:subject>structural derivatives containing</dc:subject>
          <dc:subject>quantum mechanical insights</dc:subject>
          <dc:subject>large qtm rates</dc:subject>
          <dc:subject>field smm behavior</dc:subject>
          <dc:subject>ab initio &lt;/</dc:subject>
          <dc:subject>energy barriers (&lt;</dc:subject>
          <dc:subject>slow magnetic relaxation</dc:subject>
          <dc:subject>magnetic relaxation mechanism</dc:subject>
          <dc:subject>eff &lt;/ sub</dc:subject>
          <dc:subject>b &lt;/ sub</dc:subject>
          <dc:subject>2 &lt;/ sub</dc:subject>
          <dc:subject>synthesized several non</dc:subject>
          <dc:subject>iii &lt;/ sup</dc:subject>
          <dc:subject>understand smm characteristics</dc:subject>
          <dc:subject>best smm characteristics</dc:subject>
          <dc:subject>smm characteristics</dc:subject>
          <dc:subject>magnetic relaxation</dc:subject>
          <dc:subject>u &lt;/</dc:subject>
          <dc:subject>j &lt;/</dc:subject>
          <dc:subject>&gt;&lt; sub</dc:subject>
          <dc:subject>exchange (&lt;</dc:subject>
          <dc:subject>smms ).</dc:subject>
          <dc:subject>showed zero</dc:subject>
          <dc:subject>performing lanthanide</dc:subject>
          <dc:subject>mostly true</dc:subject>
          <dc:subject>molecule magnets</dc:subject>
          <dc:subject>loprop charges</dc:subject>
          <dc:subject>kramers ion</dc:subject>
          <dc:description>The Dy&lt;sup&gt;III&lt;/sup&gt; Kramers ion is generally found in
the best-performing
lanthanide-based single-molecule magnets (SMMs). Due to large QTM
rates, slow magnetic relaxation in non-Kramers ions like Tb&lt;sup&gt;III&lt;/sup&gt; and Ho&lt;sup&gt;III&lt;/sup&gt; is rare. Moreover, Ln&lt;sup&gt;III&lt;/sup&gt; ions coupled
with 3d ions often show enhanced SMM behavior due to significant 3d–4f
magnetic exchange, but this is mostly true for Dy&lt;sup&gt;III&lt;/sup&gt; analogues.
Despite this, we synthesized several non-Dy&lt;sup&gt;III&lt;/sup&gt;-based 3d–4f
tetranuclear butterfly-shaped complexes that showed zero-field SMM
behavior with energy barriers (&lt;i&gt;U&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt;) of
36–44 cm&lt;sup&gt;–1&lt;/sup&gt; and relatively long relaxation
times for the Tb&lt;sup&gt;III&lt;/sup&gt; and Ho&lt;sup&gt;III&lt;/sup&gt; examples. In this
work, &lt;i&gt;ab initio&lt;/i&gt; and DFT calculations on eight butterfly-type
{Cr&lt;sup&gt;III&lt;/sup&gt;&lt;sub&gt;2&lt;/sub&gt;Ln&lt;sup&gt;III&lt;/sup&gt;&lt;sub&gt;2&lt;/sub&gt;} complexes
were performed to understand the SMM characteristics of Tb&lt;sup&gt;III&lt;/sup&gt; and Ho&lt;sup&gt;III&lt;/sup&gt; analogues, and structural derivatives containing
other Ln&lt;sup&gt;III&lt;/sup&gt; ions (Pr, Nd, Gd, Er) that did not display
zero-field SMM behavior. The magnetic relaxation mechanism of individual
Ln&lt;sup&gt;III&lt;/sup&gt; ions, the Cr&lt;sup&gt;III&lt;/sup&gt;···Ln&lt;sup&gt;III&lt;/sup&gt; and Ln&lt;sup&gt;III&lt;/sup&gt;···Ln&lt;sup&gt;III&lt;/sup&gt; exchange
(&lt;i&gt;J&lt;/i&gt;) and the correlation between LoProp charges of
bridging and capping ligands, and &lt;i&gt;J&lt;/i&gt;s were analyzed
to understand SMM characteristics. Furthermore, the dependency of &lt;i&gt;U&lt;/i&gt;&lt;sub&gt;eff&lt;/sub&gt; and &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;B&lt;/sub&gt; on the
Cr&lt;sup&gt;III&lt;/sup&gt;···Ln&lt;sup&gt;III&lt;/sup&gt; &lt;i&gt;J&lt;/i&gt;s has been correlated, which suggests that the moderate Cr&lt;sup&gt;III&lt;/sup&gt;···Ln&lt;sup&gt;III&lt;/sup&gt; antiferromagnetic exchange with
support from ferromagnetic Ln&lt;sup&gt;III&lt;/sup&gt;···Ln&lt;sup&gt;III&lt;/sup&gt; exchange leads to the best SMM characteristics.</dc:description>
          <dc:date>2026-09-30T00:00:00Z</dc:date>
          <dc:type>Text</dc:type>
          <dc:type>Journal contribution</dc:type>
          <dc:identifier>10.1021/acs.inorgchem.6c03746.s001</dc:identifier>
          <dc:relation>https://figshare.com/articles/journal_contribution/Quantum_Mechanical_Insights_into_Magneto_Structural_Correlations_Governing_the_Magnetic_Relaxation_of_Non-Dysprosium_Butterfly-Shaped_Cr_sup_III_sup_sub_2_sub_Ln_sup_III_sup_sub_2_sub_Ln_Pr_Nd_Tb_Ho_Er_Complexes/34034022</dc:relation>
          <dc:rights>CC BY-NC 4.0</dc:rights>
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