Maria Caporali

Synthesis and Characterization of Terminal [Re(XCO)(CO)2(triphos)] (X=N, P): Isocyanate versus Phosphaethynolate Complexes

The terminal rhenium(I) phosphaethynolate complex [Re(PCO)(CO)(2)(triphos)] has been prepared in a salt metathesis reaction from Na(OCP) and [Re(OTf)(CO)(2)(triphos)]. The analogous isocyanato complex [Re(NCO)(CO)(2)(triphos)] has been likewise prepared for comparison. The structure of both complexes was elucidated by X-ray diffraction studies. While the isocyanato complex is linear, the phosphaethynolate complex is strongly bent around the pnictogen center. Computations including natural bond orbital (NBO) theory, natural resonance theory (NRT), and natural population analysis (NPA) indicate that the isocyanato complex can be viewed as a classic Werner-type complex, that is, with an electrostatic interaction between the Re(I) and the NCO group. The phosphaethynolate complex [Re(P=C=O)(CO)(2)(triphos)] is best described as a metallaphosphaketene with a Re(I)-phosphorus bond of highly covalent character.

Water-Soluble, 1,3,5-Triaza-7-phosphaadamantane-Stabilized Palladium Nanoparticles and their Application in Biphasic Catalytic Hydrogenations at Room Temperature

Water‐dispersible Pd nanoparticles stabilized by the hydrophilic cage‐like aminophosphine ligand 1,3,5‐triaza‐7‐phosphaadamantane and its N‐methyl derivative were synthesized and fully characterized in the colloidal state by TEM, and NMR and UV spectroscopy and in the solid state by X‐ray photoelectron spectroscopy and powder XRD. The three different nanoparticles obtained showed a narrow distribution range with average core sizes of 2.8, 3.2, and 3.5u2005nm. The activity of some of these Pd nanoparticles as catalysts in the biphasic hydrogenation of organic substrates under mild conditions has been tested, and good results and excellent reusability (up to nine catalytic runs) were obtained.

Solution and Solid-State Dynamics of Metal-Coordinated White Phosphorus

The dynamic behavior in solution of eight mono-hapto tetraphosphorus transition metal-complexes, trans-[Ru(dppm)(2)(H)(η(1)-P(4))]BF(4) ([1]BF(4)), trans-[Ru(dppe)(2)(H)(η(1)-P(4))]BF(4) ([2]BF(4)), [CpRu(PPh(3))(2)(η(1)-P(4))]PF(6) ([3]PF(6)), [CpOs(PPh(3))(2)(η(1)-P(4))]PF(6) ([4]PF(6)), [Cp*Ru(PPh(3))(2)(η(1)-P(4))]PF(6) ([5]PF(6)), [Cp*Ru(dppe)(η(1)-P(4))]PF(6) ([6]PF(6)), [Cp*Fe(dppe)(η(1)-P(4))]PF(6) ([7]PF(6)), [(triphos)Re(CO)(2)(η(1)-P(4))]OTf ([8]OTf), and of three bimetallic Ru(μ,η(1:2)-P(4))Pt species [{Ru(dppm)(2)(H)}(μ,η(1:2)-P(4)){Pt(PPh(3))(2)}]BF(4) ([1-Pt]BF(4)), [{Ru(dppe)(2)(H)}(μ,η(1:2)-P(4)){Pt(PPh(3))(2)}]BF(4) ([2-Pt]BF(4)), [{CpRu(PPh(3))(2))}(μ,η(1:2)-P(4)){Pt(PPh(3))(2)}]BF(4) ([3-Pt]BF(4)), [dppm=bis(diphenylphosphanyl)methane; dppe=1,2-bis(diphenylphosphanyl)ethane; triphos=1,1,1-tris(diphenylphosphanylmethyl)ethane; Cp=η(5)-C(5)H(5); Cp*=η(5)-C(5)Me(5) ] was studied by variable-temperature (VT) NMR and (31)P{(1)H} exchange spectroscopy (EXSY). For most of the mononuclear species, NMR spectroscopy allowed to ascertain that the metal-coordinated P(4) molecule experiences a dynamic process consisting, apart from the free rotation about the M-P(4) axis, in a tumbling movement of the P(4) cage while remaining chemically coordinated to the central metal. EXSY and VT (31)P NMR experiments showed that also the binuclear complex cations [1-Pt](+)-[3-Pt](+) are subjected to molecular motions featured by the shift of each metal from one P to an adjacent one of the P(4) moiety. The relative mobility of the metal fragments (Ru vs. Pt) was found to depend on the co-ligands of the binuclear complexes. For complexes [2]BF(4) and [3]PF(6), MAS, (31)P NMR experiments revealed that the dynamic processes observed in solution (i.e., rotation and tumbling) may take place also in the solid state. The activation parameters for the dynamic processes of complexes 1(+), 2(+), 3(+), 4(+), 6(+), 8(+) in solution, as well as the X-ray structures of 2(+), 3(+), 5(+), 6(+) are also reported. The data collected suggest that metal-coordinated P(4) should not be considered as a static ligand in solution and in the solid state.

New diphosphine ligands based on diphenyl ether for the Pd-catalyzed CO/ethene copolymerization

The catalytic activity and selectivity of palladium(II) complexes of new, flexible bidentate ligands in the CO/ethene copolymerization reaction have been found to change considerably with the steric properties of the ligands.

Phosphorus oxide gate dielectric for black phosphorus field effect transistors

The environmental stability of the layered semiconductor black phosphorus (bP) remains a challenge. Passivation of the bP surface with phosphorus oxide, POx, grown by a reactive ion etch with oxygen plasma is known to improve photoluminescence efficiency of exfoliated bP flakes. We apply phosphorus oxide passivation in the fabrication of bP field effect transistors using a gate stack consisting of a POx layer grown by reactive ion etching followed by atomic layer deposition of Al2O3. We observe room temperature top-gate mobilities of 115 cm2/Vs in ambient conditions, which we attribute to the low defect density of the bP/POx interface.

Dephasing in strongly anisotropic black phosphorus

Weak localization was observed in a black phosphorus field-effect transistor 65 nm thick. The weak localization behavior was found to be in excellent agreement with the Hikami-Larkin-Nagaoka model for fields up to 1 T, from which characteristic scattering lengths could be inferred. The temperature dependence of the phase coherence length

Electronic effect of diphosphines on the regioselectivity of the palladium-catalyzed hydroesterification of styrene

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Long-lived palladium catalysts for CO/vinyl arene polyketones synthesis: a solution to deactivation problems.

was investigated, and above 1 K, it was found to decrease weaker than the

The Role of Water in the Preparation and Stabilization of High-Quality Phosphorene Flakes.

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Decoration of exfoliated black phosphorus with nickel nanoparticles and its application in catalysis

dependence characteristic of electron-electron scattering in the presence of elastic scattering in two dimensions. Rather, the observed power law was found to be close to that observed previously in quasi-one-dimensional systems such as metallic nanowires and carbon nanotubes.