| Identifiers | |
|---|---|
3D model (JSmol) | |
| ChemSpider | |
PubChem CID | |
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| Properties | |
| C30H24Cl2FeN6 | |
| Molar mass | 595.31 g·mol−1 |
| Appearance | red solid |
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa). | |
Tris(bipyridine)iron(II) chloride is the chloride salt of the coordination complex tris(bipyridine)iron(II), [Fe(C10H8N2)3]2+ (often shortened to [Fe(bipy3]2+). It is a red, water soluble solid. It is one of the most studied transition metal complexes of 2,2'-bipyridine.
Tris(bipyridine)iron(II) center features an octahedral Fe(II) center bound to three bipyridine ligands. As confirmed many times by x-ray crystallography, the dication is octahedral, the Fe(II) center occupying a chiral pocket. The cation has idealized D3 symmetry, and as such both Δ and Λ are observed. The Fe-N distances are near 196 picometers, consistent with low spin complex. [1]
The complex has been isolated as salts with many anions. [2] The chloride salt is readily soluble in aqueous solution, and the hexafluorophosphate salt is soluble in organic solvents such as nitriles. [3]
The sulfate salt [Fe(bipy)3]SO4 is produced by combining ferrous sulfate with excess bipy in aqueous solution. [4] This result illustrates the preference of Fe(II) for bipyridine vs water. The potentials for |[Fe(bipy)3]2+/3+ and [Fe(phen)3]2+/3+ are very similar. [5]
Addition of cyanide to an aqueous solution of [Fe(bipy)3]SO4 precipitates Fe(bipy)2(CN)2. [6]
[Fe(bipy)3]2+ salts can also be prepared from Iron(II) tetrafluoroborate in the solid state via mechanochemistry. [7]
The electronic absorption spectrum of [Fe(bipy)3]2+ features a metal-to-ligand charge-transfer (MLCT) band at 540 nm (ε = 8,000‑14,000 M−1cm−1), a weak shoulder due to the spin-forbidden 3MLCT transition at 640 nm (ε < 50 M−1cm−1), a higher lying MLCT band at 350 nm (ε = 6,000‑10,500 M−1cm−1), and a bipy π‑π* transition at 290 nm (ε = 40,000‑70,000 M−1cm−1). [8] [9] [10]
In contrast to tris(bipyridine)ruthenium(II), this iron complex is not a useful photosensitizer because its excited states relax too rapidly, a consequence of the primogenic effect.
[Fe(bipy)3]2+ is a model system for photoinduced spin crossover/Light Induced Excited Spin State Trapping (LIESST). Upon photoexcitation of its 1MLCT band, the molecule undergoes intersystem crossing to the high-spin 5d–d state in less than 100 fs. [10] The lifetime of the high-spin state is 650 ps. The large changes in electronic structure, spin state, and Fe–N bond length in the high-spin state lead to strong transient signals in the time-resolved X-ray absorption spectra (XAS) and X-ray emission spectra (XES). Time-resolved Fe K-edge EXAFS has revealed a 0.203 ± 0.008 Å increase in Fe–N bond length in the high-spin state. [11] The large transient signals and ultrafast formation of the high-spin state has led to the application of [Fe(bipy)3]2+ as a reference compound used at many synchrotron beamlines to find temporal overlap of the laser pump and X-ray probe pulses and to measure the instrument response function (IRF). [12] The time resolution of these experiments is typically limited by the ~70 ps duration of the X-ray pulses, so the formation of the high-spin state is effectively instantaneous and the rise of the transient signal is IRF-limited. Since the advent of X-ray free-electron laser (XFEL) and high harmonic generation sources capable of producing sub-picosecond pulses of X-rays, the ultrafast spin-crossover dynamics of [Fe(bipy)3]2+ and related complexes have been a popular target for femtosecond X-ray spectroscopy experiments. The improved time resolution of these experiments enabled detection of the short-lived intermediate 3d–d state, whose lifetime was measured with Fe Kβ XES to be 58 fs in [Fe(bipy)3]2+ [13] and with Fe M2,3-edge XANES to be 39 fs in tris(o-phenanthroline)iron(II). [14]