Abstract:Photoinduced dissociation of two Mo-CN bonds in [Mo(CN)8]4- affords the octahedral complex anion [Mo(CN)6]2-. This hexacyanomolybdate(IV) ion is also obtainable from tetracyanooxomolybdate via a thermal substitutional synthetic route. The anion represents the missing link in the ligand-field photolysis of octacyanomolybdate(IV); it is characterized by means of single-crystal X-ray diffraction, thermogravimetric analysis, and magnetic susceptibility measurements as well as IR, Raman, 1H and 13C NMR, and electro… Show more
“…In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state. The relative spin-state energetics of [Mo(CN) 6 ] 2À will be studied with a number of DFT and wave function theory methods. Finally, the magnetic properties will be theoretically simulated and compared with the experimental magnetic susceptibility data for a wide range of temperatures.…”
Section: Introductionmentioning
confidence: 77%
“…6 For the octahedral complex of Mo(IV) one would rather expect the triplet ground state ( 3 T 1g ; arising from two d electrons in the t 2g manifold) and thus, obviously, a paramagnetic character. The purpose of this paper is to elucidate this paradoxical result by means of quantum chemical calculations and interpretation of magnetic susceptibility measurements.…”
Section: Introductionmentioning
confidence: 99%
“…7,8 It is thus important to thoroughly understand their electronic properties and relation thereof to the molecular structure, particularly for cases as puzzling as the present one. Therefore, in this paper we shall consider various effects that might be responsible for the unexpected diamagnetism of [Mo(CN) 6 ] 2À , including a possibility of magnetic coupling between the neighboring anions in the crystal structure of 1, effects of the spin-orbit coupling, and distortions from the ideal octahedral geometry. In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, in this paper we shall consider various effects that might be responsible for the unexpected diamagnetism of [Mo(CN) 6 ] 2À , including a possibility of magnetic coupling between the neighboring anions in the crystal structure of 1, effects of the spin-orbit coupling, and distortions from the ideal octahedral geometry. In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state. The relative spin-state energetics of [Mo(CN) 6 ] 2À will be studied with a number of DFT and wave function theory methods.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, the magnetic properties will be theoretically simulated and compared with the experimental magnetic susceptibility data for a wide range of temperatures. 6 ] 2À were carried out using Turbomole 9 and Gaussian 09 10 packages. The structures were optimized and harmonic frequencies were computed (to verify the character of stationary points and to yield zero-point energies and thermal vibrational corrections to the Gibbs free energy) at the DFT:BP86/def2-TZVP 11 level in Turbomole.…”
Quantum chemical calculations are employed to elucidate the origin of a puzzling diamagnetism for a hexacyanomolybdate(IV) anion, [Mo(CN)6](2-), which was previously reported by Szklarzewicz et al. [Inorg. Chem., 2007, 46, 9531-9533]. The diamagnetism is surprising because for the octahedral (d)(2) complex one would rather expect a (paramagnetic) triplet ground state, clearly favored over a (diamagnetic) singlet state by an exchange interaction between two d electrons in the t2g orbitals. Nevertheless, the present calculations reveal that the minimum energy structure of isolated [Mo(CN)6](2-) is not an octahedron, but a trigonal prism; the latter geometry allows maximization of a σ-donation from the cyanides to the electron-deficient Mo(iv) center. Unlike for the octahedron, for the trigonal prism structure the singlet and triplet spin states are close in energy to within a few kcal mol(-1). Although the actual relative energy of the two spin states turns out to be method-dependent, the complete active space calculations (CASPT2; with the appropriate choice of the IPEA shift parameter) can reproduce the singlet ground state, in agreement with the experimentally observed diamagnetism. Moreover, magnetic measurements reveal a slight increase of the magnetic susceptibility with the increase of temperature from 100 to 300 K, suggesting an admixture of a thermally induced paramagnetism (possibly due to Boltzmann population of the low-energy triplet state) on top of the dominant diamagnetism. Our prediction that the geometry of [Mo(CN)6](2-) should significantly deviate from the ideal octahedron, not only in the gas phase, but also in a periodic DFT model of the crystalline phase, as well as the experimentally confirmed diamagnetic properties, does not agree with the previously reported ideal octahedral structure. We suggest that this crystal structure might have been determined incorrectly (e.g., due to overlooked merohedral twinning or superstructure properties) and it should be re-investigated.
“…In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state. The relative spin-state energetics of [Mo(CN) 6 ] 2À will be studied with a number of DFT and wave function theory methods. Finally, the magnetic properties will be theoretically simulated and compared with the experimental magnetic susceptibility data for a wide range of temperatures.…”
Section: Introductionmentioning
confidence: 77%
“…6 For the octahedral complex of Mo(IV) one would rather expect the triplet ground state ( 3 T 1g ; arising from two d electrons in the t 2g manifold) and thus, obviously, a paramagnetic character. The purpose of this paper is to elucidate this paradoxical result by means of quantum chemical calculations and interpretation of magnetic susceptibility measurements.…”
Section: Introductionmentioning
confidence: 99%
“…7,8 It is thus important to thoroughly understand their electronic properties and relation thereof to the molecular structure, particularly for cases as puzzling as the present one. Therefore, in this paper we shall consider various effects that might be responsible for the unexpected diamagnetism of [Mo(CN) 6 ] 2À , including a possibility of magnetic coupling between the neighboring anions in the crystal structure of 1, effects of the spin-orbit coupling, and distortions from the ideal octahedral geometry. In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, in this paper we shall consider various effects that might be responsible for the unexpected diamagnetism of [Mo(CN) 6 ] 2À , including a possibility of magnetic coupling between the neighboring anions in the crystal structure of 1, effects of the spin-orbit coupling, and distortions from the ideal octahedral geometry. In fact, our calculations will suggest that [Mo(CN) 6 ] 2À tends to adopt a non-octahedral, trigonalprismatic structure, which may be presumably the primary factor leading to stabilization of the low-spin state. The relative spin-state energetics of [Mo(CN) 6 ] 2À will be studied with a number of DFT and wave function theory methods.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, the magnetic properties will be theoretically simulated and compared with the experimental magnetic susceptibility data for a wide range of temperatures. 6 ] 2À were carried out using Turbomole 9 and Gaussian 09 10 packages. The structures were optimized and harmonic frequencies were computed (to verify the character of stationary points and to yield zero-point energies and thermal vibrational corrections to the Gibbs free energy) at the DFT:BP86/def2-TZVP 11 level in Turbomole.…”
Quantum chemical calculations are employed to elucidate the origin of a puzzling diamagnetism for a hexacyanomolybdate(IV) anion, [Mo(CN)6](2-), which was previously reported by Szklarzewicz et al. [Inorg. Chem., 2007, 46, 9531-9533]. The diamagnetism is surprising because for the octahedral (d)(2) complex one would rather expect a (paramagnetic) triplet ground state, clearly favored over a (diamagnetic) singlet state by an exchange interaction between two d electrons in the t2g orbitals. Nevertheless, the present calculations reveal that the minimum energy structure of isolated [Mo(CN)6](2-) is not an octahedron, but a trigonal prism; the latter geometry allows maximization of a σ-donation from the cyanides to the electron-deficient Mo(iv) center. Unlike for the octahedron, for the trigonal prism structure the singlet and triplet spin states are close in energy to within a few kcal mol(-1). Although the actual relative energy of the two spin states turns out to be method-dependent, the complete active space calculations (CASPT2; with the appropriate choice of the IPEA shift parameter) can reproduce the singlet ground state, in agreement with the experimentally observed diamagnetism. Moreover, magnetic measurements reveal a slight increase of the magnetic susceptibility with the increase of temperature from 100 to 300 K, suggesting an admixture of a thermally induced paramagnetism (possibly due to Boltzmann population of the low-energy triplet state) on top of the dominant diamagnetism. Our prediction that the geometry of [Mo(CN)6](2-) should significantly deviate from the ideal octahedron, not only in the gas phase, but also in a periodic DFT model of the crystalline phase, as well as the experimentally confirmed diamagnetic properties, does not agree with the previously reported ideal octahedral structure. We suggest that this crystal structure might have been determined incorrectly (e.g., due to overlooked merohedral twinning or superstructure properties) and it should be re-investigated.
The photoinduced properties of the octacoordinated complex K4MoIV(CN)8⋅2 H2O were studied by theoretical calculations, crystallography, and optical and magnetic measurements. The crystal structure recorded at 10 K after blue light irradiation reveals an heptacoordinated Mo(CN)7 species originating from the light‐induced cleavage of one Mo−CN bond, concomitant with the photoinduced formation of a paramagnetic signal. When this complex is heated to 70 K, it returns to its original diamagnetic ground state, demonstrating full reversibility. The photomagnetic properties show a partial conversion into a triplet state possessing significant magnetic anisotropy, which is in agreement with theoretical studies. Inspired by these results, we isolated the new compound [K(crypt‐222)]3[MoIV(CN)7]⋅3 CH3CN using a photochemical pathway, confirming that photodissociation leads to a stable heptacyanomolybdate(IV) species in solution.
The photoinduced properties of the octacoordinated complex K4MoIV(CN)8⋅2 H2O were studied by theoretical calculations, crystallography, and optical and magnetic measurements. The crystal structure recorded at 10 K after blue light irradiation reveals an heptacoordinated Mo(CN)7 species originating from the light‐induced cleavage of one Mo−CN bond, concomitant with the photoinduced formation of a paramagnetic signal. When this complex is heated to 70 K, it returns to its original diamagnetic ground state, demonstrating full reversibility. The photomagnetic properties show a partial conversion into a triplet state possessing significant magnetic anisotropy, which is in agreement with theoretical studies. Inspired by these results, we isolated the new compound [K(crypt‐222)]3[MoIV(CN)7]⋅3 CH3CN using a photochemical pathway, confirming that photodissociation leads to a stable heptacyanomolybdate(IV) species in solution.
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