Abstract:Four new quasi-1D Ni-lantern chain complexes of the form [Ni(SOCR)(L)] (R = Ph, L = DABCO (1); R = Ph, L = pyz (2); R = CH, L = DABCO (3); R = CH, L = pyz (4)) were prepared from the reaction of [Ni(SOCR)(EtOH)], R = CH or Ph, with the N,N'-donor bridging ligands pyrazine (pyz) or 1,4-diazabicyclo[2.2.2]octane (DABCO). Reaction of [Ni(tba)(EtOH)], (tba = thiobenzoate) with the mono-N donor ligand quinuclidine (quin) gave the discrete Ni-lantern complex [Ni(tba)(quin)] (5), whereas reaction with pyridine led to… Show more
“…In the present structural model, the transition metal in each lantern unit has a different coordination environment (see Figure 1), which leads to d-oribital energy levels of Ni(II) ions in two lantern units split in different manners, as shown in Figure 3. The [NiO 4 ] and [NiS 4 ] planes of the structures A and B are twisted about the Ni−Ni axis by 15.76°and 12.77°, respectively, which is slightly smaller than the experimental values reported by Doerrer et al 37 However, the Ni−Ni distances in optimized structure A were 0.770 and 0.764 Å larger than that in the experimental products ([Ni 2 (tba) 4 (EtOH)] and [Ni 2 (SAc) 4 (EtOH)]). 37 These difference can be ascribed to two reasons: One is a slight steric effect between coordinated Ni planes arising from the absence of substituted groups in thioformic acid backbone ligands.…”
contrasting
confidence: 62%
“…The [NiO 4 ] and [NiS 4 ] planes of the structures A and B are twisted about the Ni−Ni axis by 15.76°and 12.77°, respectively, which is slightly smaller than the experimental values reported by Doerrer et al 37 However, the Ni−Ni distances in optimized structure A were 0.770 and 0.764 Å larger than that in the experimental products ([Ni 2 (tba) 4 (EtOH)] and [Ni 2 (SAc) 4 (EtOH)]). 37 These difference can be ascribed to two reasons: One is a slight steric effect between coordinated Ni planes arising from the absence of substituted groups in thioformic acid backbone ligands. On the other hand, axial ligands in our model and experimental complexes have different coordination bonding characters.…”
contrasting
confidence: 62%
“…Comparing the solid-state magnetism of various dinickel lantern complexes, Doerrer et al found a change in coupling upon change of axial ligand. Dinickel lantern complex belongs to a mixed valence system, which possesses two Ni centers with different spin states, S = 0 and S = 1 . In the present complex, [Ni 2 (SOCH) 4 (NCS) 2 ], the distorted octahedral environment determines the d-level splitting ways.…”
In the theory of ligand fields, depending on the nature and field strength of the surrounding ligands, the central metal ion may exhibit different electronic configurations, low spin (LS) or high spin (HS). Realizing stable spin polarization is one of the main challenges in the field of molecular spintronic devices because of spin switching triggered by an external stimulus. Here, an asymmetric homobimetallic complex has been investigated using the nonequilibrium Green's function and spin density functional theory. Our calculations indicate that the homobimetallic complex can achieve negative differential resistance, rectification effect, and perfect spin filtering transport on the level of an individual molecule. Strikingly, when the molecule is stretched by 0.45 Å, the HS state is still the most stable because of the weak magnetic Ni−Ni interaction. Although its conductivity decreases by 30%, the efficiency of spin filtering remains 100%. These obtained theoretical findings suggest that the homobimetallic complexes hold great potential in molecular spintronics.
“…In the present structural model, the transition metal in each lantern unit has a different coordination environment (see Figure 1), which leads to d-oribital energy levels of Ni(II) ions in two lantern units split in different manners, as shown in Figure 3. The [NiO 4 ] and [NiS 4 ] planes of the structures A and B are twisted about the Ni−Ni axis by 15.76°and 12.77°, respectively, which is slightly smaller than the experimental values reported by Doerrer et al 37 However, the Ni−Ni distances in optimized structure A were 0.770 and 0.764 Å larger than that in the experimental products ([Ni 2 (tba) 4 (EtOH)] and [Ni 2 (SAc) 4 (EtOH)]). 37 These difference can be ascribed to two reasons: One is a slight steric effect between coordinated Ni planes arising from the absence of substituted groups in thioformic acid backbone ligands.…”
contrasting
confidence: 62%
“…The [NiO 4 ] and [NiS 4 ] planes of the structures A and B are twisted about the Ni−Ni axis by 15.76°and 12.77°, respectively, which is slightly smaller than the experimental values reported by Doerrer et al 37 However, the Ni−Ni distances in optimized structure A were 0.770 and 0.764 Å larger than that in the experimental products ([Ni 2 (tba) 4 (EtOH)] and [Ni 2 (SAc) 4 (EtOH)]). 37 These difference can be ascribed to two reasons: One is a slight steric effect between coordinated Ni planes arising from the absence of substituted groups in thioformic acid backbone ligands. On the other hand, axial ligands in our model and experimental complexes have different coordination bonding characters.…”
contrasting
confidence: 62%
“…Comparing the solid-state magnetism of various dinickel lantern complexes, Doerrer et al found a change in coupling upon change of axial ligand. Dinickel lantern complex belongs to a mixed valence system, which possesses two Ni centers with different spin states, S = 0 and S = 1 . In the present complex, [Ni 2 (SOCH) 4 (NCS) 2 ], the distorted octahedral environment determines the d-level splitting ways.…”
In the theory of ligand fields, depending on the nature and field strength of the surrounding ligands, the central metal ion may exhibit different electronic configurations, low spin (LS) or high spin (HS). Realizing stable spin polarization is one of the main challenges in the field of molecular spintronic devices because of spin switching triggered by an external stimulus. Here, an asymmetric homobimetallic complex has been investigated using the nonequilibrium Green's function and spin density functional theory. Our calculations indicate that the homobimetallic complex can achieve negative differential resistance, rectification effect, and perfect spin filtering transport on the level of an individual molecule. Strikingly, when the molecule is stretched by 0.45 Å, the HS state is still the most stable because of the weak magnetic Ni−Ni interaction. Although its conductivity decreases by 30%, the efficiency of spin filtering remains 100%. These obtained theoretical findings suggest that the homobimetallic complexes hold great potential in molecular spintronics.
“…[6-9, 11, 12] Theb inding of an axial ligand changes the coordination sphere at the metal site to square-pyramidal thus rendering such PW complexes paramagnetic.Asearch in the Cambridge Structural Database revealed that in O,O-, S,O-and S,S-bridged Ni 2 -PWs,the {NiO 4 }s ites are always coordinated by an axial ligand, while the {NiS 4 }a re not. [14] S,N-Bridged Ni 2 -PWs have been reported either with [11] or without [12,15] axially bound donor ligands.T ot he best of our knowledge,i nn one of those both situations have been realized within ag iven paddlewheel. However,t his would be highly interesting as it offers the possibility for molecular,m agnetic switching triggered by [*] Dr.K .M.F ürpaß, Dr.L.M.P eschel, Prof. Dr. 2021 The Authors.…”
Reaction of [NiCl 2 (PnH) 4 ](1)(PnH = 6-tert-butylpyridazine-3-thione) with NiCl 2 affords the binuclear paddlewheel (PW) complex [Ni 2 (Pn) 4 ](2). Diamagnetic complex 2 is the first example of aP Wc omplex capable of reversibly binding and releasing NH 3 .T he NH 3 ligand in [Ni 2 (Pn) 4 -(NH 3 )] (2•NH 3 )e nforces major spectroscopic and magnetic susceptibility changes,thus displaying vapochromic properties (l max (2) = 532 nm, l max (2•NH 3 ) = 518 nm) and magnetochemical switching (2:S = 0; 2•NH 3 :S = 1). Upon repeated adsorption/desorption cycles of NH 3 the PW core remains intact. Compound 2 can be embedded into thin polyurethane films (2 P )u nder retention of its sensing abilities.T herefore, 2 qualifies as reversible optical probe for ammonia. The magnetochemical switching of 2 and 2•NH 3 was studied in detail by SQUIDmeasurements showing that in 2•NH 3 ,solely the Ni atom coordinated the NH 3 molecule is responsible for the paramagnetic behavior.
“…[6-9, 11, 12] Theb inding of an axial ligand changes the coordination sphere at the metal site to square-pyramidal thus rendering such PW complexes paramagnetic.Asearch in the Cambridge Structural Database revealed that in O,O-, S,O-and S,S-bridged Ni 2 -PWs,the {NiO 4 }s ites are always coordinated by an axial ligand, while the {NiS 4 }a re not. [14] S,N-Bridged Ni 2 -PWs have been reported either with [11] or without [12,15] axially bound donor ligands.T ot he best of our knowledge,i nn one of those both situations have been realized within ag iven paddlewheel. However,t his would be highly interesting as it offers the possibility for molecular,m agnetic switching triggered by ad onor ligand.…”
Reaction of [NiCl 2 (PnH) 4 ](1)(PnH = 6-tert-butylpyridazine-3-thione) with NiCl 2 affords the binuclear paddlewheel (PW) complex [Ni 2 (Pn) 4 ](2). Diamagnetic complex 2 is the first example of aP Wc omplex capable of reversibly binding and releasing NH 3 .T he NH 3 ligand in [Ni 2 (Pn) 4 -(NH 3 )] (2•NH 3 )e nforces major spectroscopic and magnetic susceptibility changes,thus displaying vapochromic properties (l max (2) = 532 nm, l max (2•NH 3 ) = 518 nm) and magnetochemical switching (2:S = 0; 2•NH 3 :S = 1). Upon repeated adsorption/desorption cycles of NH 3 the PW core remains intact. Compound 2 can be embedded into thin polyurethane films (2 P )u nder retention of its sensing abilities.T herefore, 2 qualifies as reversible optical probe for ammonia. The magnetochemical switching of 2 and 2•NH 3 was studied in detail by SQUIDmeasurements showing that in 2•NH 3 ,solely the Ni atom coordinated the NH 3 molecule is responsible for the paramagnetic behavior.
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