<p>Symmetry-breaking structural phase transitions in spin crossover (SCO) complexes play a pivotal role in the development of multifunctional SCO materials. In this work, the influence of counter anions on the symmetry-breaking behavior and SCO properties was investigated in three mononuclear Fe<sup>III</sup>-qsal type complexes, [Fe(qsal-4-Me)<sub>2</sub>]A (Hqsal-4-Me = 4-methyl-<i>N</i>-(8-quinolyl)salicylaldimine; A = BF<Stack> <sub>4</sub> <sup>−</sup> </Stack> (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">B</mi> <mi mathvariant="bold">F</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation>), ClO<Stack> <sub>4</sub> <sup>−</sup> </Stack> (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation>), and OTf<sup>−</sup> (<b>3</b><sub><b>OTf</b></sub>)). All complexes exhibit a typical “Chain-Layer” structural motif. Single-crystal structural analysis at varying temperatures (50–400 K for <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">B</mi> <mi mathvariant="bold">F</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> and 120–300 K for <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation>) revealed distinct symmetry-breaking behaviors in <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">B</mi> <mi mathvariant="bold">F</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation>. Notably, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">B</mi> <mi mathvariant="bold">F</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> undergoes complete symmetry-breaking and re-entrant behavior, coupled with a three-step SCO, while <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> shows only symmetry-breaking incomplete SCO without re-entrance. Structure analyses indicated that the more compact crystal packing in <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> strengthens the elastic interactions between the high-spin Fe<sup>III</sup> centers. This stabilizes the low-spin/high-spin [LS-HS] intermediate phase, thereby inhibiting the reentrant behavior. Compound <b>3</b><sub><b>OTf</b></sub> with the largest OTf<sup>−</sup> anion remains in the HS state below 400 K. While <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">1</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">B</mi> <mi mathvariant="bold">F</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> showed no LIESST effect, <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <msub> <mrow> <mn mathvariant="bold">2</mn> </mrow> <mrow> <msub> <mrow> <mi mathvariant="bold">C</mi> <mi mathvariant="bold">l</mi> <mi mathvariant="bold">O</mi> </mrow> <mrow> <mrow> <mn mathvariant="bold">4</mn> </mrow> </mrow> </msub> </mrow> </msub> </math></EquationSource> </InlineEquation> displayed a rare reverse-LIESST effect upon irradiation with 980 nm light. The findings reported here demonstrate that subtle variations in anion type can dramatically modulate SCO behavior, offering valuable insights for the design of functional materials with tailored spin transitions.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Unveiling the role of counter-anions in symmetry breaking and spin crossover in mononuclear FeIII complexes

  • Xin-Yu Zhang,
  • Zhen Shao,
  • Ming-Yuan Zhang,
  • Du-Yong Chen,
  • Qi Liu,
  • Cheng-Cheng Zhang,
  • Yin-Shan Meng,
  • Tao Liu,
  • Xin-Yi Wang

摘要

Symmetry-breaking structural phase transitions in spin crossover (SCO) complexes play a pivotal role in the development of multifunctional SCO materials. In this work, the influence of counter anions on the symmetry-breaking behavior and SCO properties was investigated in three mononuclear FeIII-qsal type complexes, [Fe(qsal-4-Me)2]A (Hqsal-4-Me = 4-methyl-N-(8-quinolyl)salicylaldimine; A = BF 4 ( \(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\) 1 B F 4 ), ClO 4 ( \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 ), and OTf (3OTf)). All complexes exhibit a typical “Chain-Layer” structural motif. Single-crystal structural analysis at varying temperatures (50–400 K for \(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\) 1 B F 4 and 120–300 K for \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 ) revealed distinct symmetry-breaking behaviors in \(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\) 1 B F 4 and \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 . Notably, \(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\) 1 B F 4 undergoes complete symmetry-breaking and re-entrant behavior, coupled with a three-step SCO, while \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 shows only symmetry-breaking incomplete SCO without re-entrance. Structure analyses indicated that the more compact crystal packing in \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 strengthens the elastic interactions between the high-spin FeIII centers. This stabilizes the low-spin/high-spin [LS-HS] intermediate phase, thereby inhibiting the reentrant behavior. Compound 3OTf with the largest OTf anion remains in the HS state below 400 K. While \(\mathbf{1}_{\mathbf{BF}_{\mathbf{4}}}\) 1 B F 4 showed no LIESST effect, \(\mathbf{2}_{\mathbf{ClO}_{\mathbf{4}}}\) 2 C l O 4 displayed a rare reverse-LIESST effect upon irradiation with 980 nm light. The findings reported here demonstrate that subtle variations in anion type can dramatically modulate SCO behavior, offering valuable insights for the design of functional materials with tailored spin transitions.