Synthesis, Structure, and Magnetic Properties of Tetranuclear
Cubane-like and Chain-like Iron(II) Complexes Based on the N<sub>4</sub>O
Pentadentate Dinucleating Ligand
1,5-Bis[(2-pyridylmethyl)amino]pentan-3-ol
posted on 2002-02-20, 00:00authored byJuan M. Clemente-Juan, Christine Mackiewicz, Marc Verelst, Françoise Dahan, Azzedine Bousseksou, Yiannis Sanakis, Jean-Pierre Tuchagues
The tetranuclear complexes [Fe<sub>4</sub>(pypentO)(pym)<sub>3</sub>(Oac)(NCS)<sub>3</sub>]·1.5EtOH (<b>1</b>), [Fe<sub>4</sub>(pypentO)(pym)(Oac)<sub>2</sub>(NCS)<sub>2</sub>(MeO)<sub>2</sub>(H<sub>2</sub>O)]·H<sub>2</sub>O (<b>2</b>), [Fe<sub>2</sub>(pypentO)(NCO)<sub>3</sub>]<sub>2</sub> (<b>3</b>), and [Fe<sub>2</sub>(pypentO)(N<sub>3</sub>)<sub>3</sub>]<sub>2</sub> (<b>4</b>) have been prepared, and their structure
and magnetic properties have been studied (pypentOH = 1,5-bis[(2-pyridylmethyl)amino]pentan-3-ol, pymH =
2-pyridylmethanol). The X-ray diffraction analysis of <b>1</b> (C<sub>43</sub>H<sub>53</sub>N<sub>10</sub>O<sub>7.5</sub>S<sub>3</sub>Fe<sub>4</sub>, monoclinic, <i>P</i>2<sub>1</sub>/<i>n</i>, <i>a</i> = 11.6153(17) Å,
<i>b</i> = 34.391(17) Å, <i>c</i> = 14.2150(18) Å, β = 110.88(5)°, <i>V</i> = 5305(3) Å<sup>3</sup>, <i>Z</i> = 4) and <b>2</b> (C<sub>31</sub>H<sub>45</sub>N<sub>7</sub>O<sub>10</sub>S<sub>2</sub>Fe<sub>4</sub>,
monoclinic, <i>C</i>2/<i>c</i>, <i>a</i> = 19.9165(17) Å, <i>b</i> = 21.1001(12) Å, <i>c</i> = 21.2617(19) Å, β = 104.441(10)°, <i>V</i> = 8652.7(12)
Å<sup>3</sup>, <i>Z</i> = 8) showed a Fe<sub>4</sub>O<sub>4</sub> cubane-like arrangement of four iron(II) atoms, four μ<sub>3</sub>-O bridging ligands, one (<b>1</b>) or
two (<b>2</b>) syn<i>−</i>syn bridging acetates. The X-ray diffraction analysis of <b>3</b> (C<sub>40</sub>H<sub>46</sub>N<sub>14</sub>O<sub>8</sub>Fe<sub>4</sub>, monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i>, <i>a</i> =
11.7633(18) Å, <i>b</i> = 18.234(3) Å, <i>c</i> = 10.4792(16) Å, β = 99.359(18)°, <i>V</i> = 2217.7(6) Å<sup>3</sup>, <i>Z</i> = 2) and <b>4</b> (C<sub>34</sub>H<sub>46</sub>N<sub>26</sub>O<sub>2</sub>Fe<sub>4</sub>, monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i>, <i>V</i> = 4412.4(10) Å<sup>3</sup>, <i>a</i> = 23.534(3) Å, <i>b</i> = 18.046(2) Å, <i>c</i> = 10.4865(16) Å, β = 97.80(2)°,
<i>Z</i> = 4) showed a zigzag bis-dinuclear arrangement of four iron(II) cations, two μ<sub>2</sub>-O bridging pypentO ligands, four
μ<sub>2</sub>-N-cyanato bridging ligands (<b>3</b>) or four end-on azido bridging ligands (<b>4</b>): they are the first examples of cyanato
and azido bridged discrete polynuclear ferrous compounds, respectively. The Mössbauer spectra of <b>1</b> are consistent
with four different high-spin iron(II) sites in the Fe<sub>4</sub>O<sub>4</sub> cubane-type structure. The Mössbauer spectra of <b>3</b> are
consistent with two high-spin iron(II) sites (N<sub>5</sub>O and N<sub>4</sub>O). Below 190 K, the Mössbauer spectra of <b>4</b> are consistent
with one N<sub>5</sub>O and two N<sub>4</sub>O high-spin iron(II) sites. The temperature dependence of the magnetic susceptibility was
fitted with <i>J</i><sub>1</sub> ∼ 0 cm<sup>-1</sup>, <i>J</i><sub>2</sub> = −1.3 cm<sup>-1</sup>, <i>J</i><sub>3</sub> = 4.6 cm<sup>-1</sup>, <i>D</i> = 6.4 cm<sup>-1</sup>, and <i>g</i> = 2.21 for <b>1</b>; <i>J</i><sub>1</sub> = 2.6 cm<sup>-1</sup>, <i>J</i><sub>2</sub>
= 2.5 cm<sup>-1</sup>, <i>J</i><sub>3</sub> = − 5.6 cm<sup>-1</sup>, <i>D</i> = 4.5 cm<sup>-1</sup>, and <i>g</i> = 2.09 for <b>2</b>; <i>J</i><sub>1</sub> = 1.5 cm<sup>-1</sup>, <i>J</i><sub>2</sub> = 0.2 cm<sup>-1</sup>, <i>D</i> = − 5.6
cm<sup>-1</sup>, <i>D</i>‘ = 4.5 cm<sup>-1</sup>, and <i>g</i> = 2.14 for <b>3</b>; and <i>J</i><sub>1</sub> = − 2.6 cm<sup>-1</sup>, <i>J</i><sub>2</sub> = 0.8 cm<sup>-1</sup>, <i>D</i><i></i>= 6.3 cm<sup>-1</sup>, <i>D</i>‘ = 1.6 cm<sup>-1</sup>,
and <i>g</i> = 2.18 for <b>4</b>. The differences in sign among the <i>J</i><sub>1</sub>, <i>J</i><sub>2</sub>, and <i>J</i><sub>3</sub> super-exchange interactions indicate that the
faces including only μ<sub>3</sub>-OR bridges exhibit ferromagnetic interactions. The nature of the ground state in <b>1</b>−<b>3</b> is
confirmed by simulation of the magnetization curves at 2 and 5 K. In the bis-dinuclear iron(II) compounds <b>3</b> and
<b>4</b>, the <i>J</i><sub>2</sub> interaction resulting from the bridging of two Fe<sub>2</sub>(pypentO)X<sub>3</sub> units through two pseudo-halide anions is
ferromagnetic in <b>3</b> (X = μ<sub>2</sub>-N-cyanato) and may be either ferro- or antiferromagnetic in <b>4</b> (X = end-on azido). The
<i>J</i><sub>1</sub> interaction through the central O<sub>alkoxo</sub> and pseudo-halide bridges inside the dinuclear units is ferromagnetic in <b>3</b>
(X = μ<sub>2</sub>-N-cyanato) and antiferromagnetic in <b>4</b> (X = end-on azido). In agreement with the symmetry of the two Fe<sup>II</sup>
sites in complexes <b>3</b> and <b>4</b>, <i>D</i> (pentacoordinated sites) is larger than <i>D</i>‘ (octahedral sites).