Matteo Atzori (1428118)Elisa Sessini (1300539)Flavia Artizzu (1300536)Luca Pilia (1813777)Angela Serpe (1300533)CarlosJ. Gómez-García (1493068)Carlos Giménez-Saiz (1431718)Paola Deplano (1300542)Maria Laura Mercuri (1587808)
The reaction of the croconate dianion (C<sub>5</sub>O<sub>5</sub>)<sup>2–</sup> with a Fe(III) salt has led, unexpectedly,\nto the formation of the first example of a discrete Fe(II)–croconate\ncomplex without additional coligands, K<sub>4</sub>[Fe(C<sub>5</sub>O<sub>5</sub>)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>](HC<sub>5</sub>O<sub>5</sub>)<sub>2</sub>·4H<sub>2</sub>O (<b>1</b>). <b>1</b> crystallizes in the monoclinic <i>P</i>2<sub>1</sub>/<i>c</i> space group and presents discrete octahedral\nFe(II) complexes coordinated by two chelating C<sub>5</sub>O<sub>5</sub><sup>2–</sup> anions in the equatorial plane and two trans\naxial water molecules. The structure can be viewed as formed by alternating\nlayers of <i>trans</i>-diaquabis(croconato)ferrate(II) complexes\nand layers containing the monoprotonated croconate anions, HC<sub>5</sub>O<sub>5</sub><sup>–</sup>, and noncoordinated water\nmolecules. Both kinds of layers are directly connected through a hydrogen\nbond between an oxygen atom of the coordinated dianion and the protonated\noxygen atom of the noncoordinated croconate monoanion. A H-bond network\nis also formed between the coordinated water molecule and one oxygen\natom of the coordinated croconate. This H-bond can be classified as\nstrong–moderate being the O···O bond distance\n(2.771(2) Å) typical of moderate H-bonds and the O–H···O\nbond angle (174(3)°) typical of strong ones. This H-bond interaction\nleads to a quadratic regular layer where each [Fe(C<sub>5</sub>O<sub>5</sub>)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>]<sup>2–</sup> anion is connected to its four neighbors in the plane through four\nequivalent H-bonds. From the magnetic point of view, these connections\nlead to an <i>S</i> = 2 quadratic layer. The magnetic properties\nof <b>1</b> have been reproduced with a 2D square lattice model\nfor <i>S</i> = 2 ions with <i>g</i> = 2.027(2)\nand <i>J</i> = 4.59(3) cm<sup>–1</sup>. This model\nreproduces quite satisfactorily its magnetic properties but only above\nthe maximum. A better fit is obtained by considering an additional\nantiferromagnetic weak interlayer coupling constant (<i>j</i>) through a molecular field approximation with <i>g</i> = 2.071(7), <i>J</i> = 2.94(7) cm<sup>–1</sup>,\nand <i>j</i> = −0.045(2) cm<sup>–1</sup> (the\nHamiltonian is written as <i>H</i> = –<i>JS<sub>i</sub>S<sub>j</sub></i>). Although this second model might\nstill be improved since there is also an extra contribution due to\nthe presence of ZFS in the Fe(II) ions, it confirms the presence of\nweak ferromagnetic Fe–Fe interactions through H-bonds in compound <b>1</b> which represents one of the rare examples of ferromagnetic\ncoupling via H-bonds.
Hua Gui Yang (1440067)Hua Chun Zeng (1441510)
William J. Evans (529233)Kevin A. Miller (2102332)Stosh A. Kozimor (1615057)Joseph W. Ziller (1340067)Antonio G. DiPasquale (1274730)Arnold L. Rheingold (1274736)
Junghwan Do (2102317)Ranko P. Bontchev (2425492)Allan J. Jacobson (1644922)
Jeongho Yeon (1406326)Sang-Hwan Kim (527119)Sau Doan Nguyen (1985821)Hana Lee (445860)P. Shiv Halasyamani (1261704)
IrinaV. Kalinina (2064703)Natalya V. Izarova (2012452)Ulrich Kortz (1290630)