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At least 19 records

Efficient Self-Sensitized Photochemical CO 2 Reduction Using [Re(bpy 2+ )(CO) 3 (I)] 2+ and [Re(bpy 2+ )(CO) 3 (CH 3 CN)] 3+ Photocatalysts with Pendent Ammonium Cations

Rhenium(I) tricarbonyl complexes fac-[Re(bpy)(CO) 3 (L)]n + are the classical examples of self-sensitized photocatalysts capable of the dual roles of light absorption and catalysis. Here, in this work, a series of dicationic halido or tricationic solvento complexes fac-[Re(bpy 2+ )(CO) 3 X] n+ (PF 6 ) n (where X = Cl - or I - (n = 2), or CH 3 CN (n = 3) and bpy 2+ is bipyridine modified by two -CH 2 -(NMe3) + tetra-alkylammonium cations) have been investigated as self-sensitized and sensitized CO 2 reduction photocatalysts. Four structural isomers differing in the cation position have been tested in N,Nʹ-dimethylacetamide solvent (DMA) using 1,3-dimethyl-2-phenyl-2,3-dihydro-1H-benzimidazole (BIH) as the electron donor, and the position of the cationic pendants has a significant impact on the catalyst turnover number and quantum efficiency (ϕ). Up to 455 self-sensitized turnovers of CO and a high photon efficiency (ϕ CO ) of 22% have been achieved. Time-resolved infrared spectroscopy and theoretical calculations were used to characterize the catalytic cycle including the ligand exchange between one-electron reduced (OER) halido and solvento species as well as the binding of CO 2 to the putative two-electron reduced (TER) species. The CO 2 -reactive TER catalyst was formed by disproportionation or intramolecular electron transfer between two forms of the OER catalyst as indicated by the formation of the fully oxidized catalyst concurrent with CO 2 binding. When [Ru(bpy) 3 ] 2+ was used as a sensitizer, catalyst durability improved, and the selectivity toward formate increased as high as 3.3:1 over CO (total TON = 1370) due to acidification of the reaction, which promotes formation of the hydride intermediate, as BIH was consumed and deprotonated.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Stabilization Of The CN 3 5− Anion In Recoverable High‐pressure Ln 3 O 2 (CN 3 ) (Ln=La, Eu, Gd, Tb, Ho, Yb) Oxoguanidinates

Abstract A series of isostructural Ln 3 O 2 (CN 3 ) (Ln=La, Eu, Gd, Tb, Ho, Yb) oxoguanidinates was synthesized under high‐pressure (25–54 GPa) high‐temperature (2000–3000 K) conditions in laser‐heated diamond anvil cells. The crystal structure of this novel class of compounds was determined via synchrotron single‐crystal X‐ray diffraction (SCXRD) as well as corroborated by X‐ray absorption near edge structure (XANES) measurements and density functional theory (DFT) calculations. The Ln 3 O 2 (CN 3 ) solids are composed of the hitherto unknown CN 3 5− guanidinate anion—deprotonated guanidine. Changes in unit cell volumes and compressibility of Ln 3 O 2 (CN 3 ) (Ln=La, Eu, Gd, Tb, Ho, Yb) compounds are found to be dictated by the lanthanide contraction phenomenon. Decompression experiments show that Ln 3 O 2 (CN 3 ) compounds are recoverable to ambient conditions. The stabilization of the CN 3 5− guanidinate anion at ambient conditions provides new opportunities in inorganic and organic synthetic chemistry.

Chemistry↗

Materials Data on Ba3Rh(CN)3 by Materials Project

Ba3Rh(CN)3 crystallizes in the hexagonal P6_3/m space group. The structure is zero-dimensional and consists of two Ba3Rh(CN)3 clusters. Ba2+ is bonded in a 1-coordinate geometry to one N3- atom. The Ba–N bond length is 2.78 Å. Rh3+ is bonded in a trigonal planar geometry to three equivalent C atoms. All Rh–C bond lengths are 1.93 Å. C is bonded in a distorted linear geometry to one Rh3+ and one N3- atom. The C–N bond length is 1.23 Å. N3- is bonded in a distorted single-bond geometry to one Ba2+ and one C atom.

36 MATERIALS SCIENCE↗

Materials Data on Ba3Ir(CN)3 by Materials Project

Ba3Ir(CN)3 crystallizes in the hexagonal P6_3/m space group. The structure is zero-dimensional and consists of two Ba3Ir(CN)3 clusters. Ba2+ is bonded in a 1-coordinate geometry to one N3- atom. The Ba–N bond length is 2.78 Å. Ir5+ is bonded in a trigonal planar geometry to three equivalent C+0.67- atoms. All Ir–C bond lengths are 1.91 Å. C+0.67- is bonded in a 1-coordinate geometry to one Ir5+ and one N3- atom. The C–N bond length is 1.24 Å. N3- is bonded in a distorted single-bond geometry to one Ba2+ and one C+0.67- atom.

36 MATERIALS SCIENCE↗

Materials Data on BaTe3H15(CN)3 by Materials Project

BaH15Te3(CN)3 crystallizes in the monoclinic C2/c space group. The structure is two-dimensional and consists of two BaH15Te3(CN)3 sheets oriented in the (1, 0, 0) direction. Ba2+ is bonded in a 3-coordinate geometry to three N3- and five Te2- atoms. There are a spread of Ba–N bond distances ranging from 2.88–2.95 Å. There are a spread of Ba–Te bond distances ranging from 3.61–3.81 Å. There are three inequivalent C+0.67- sites. In the first C+0.67- site, C+0.67- is bonded in a tetrahedral geometry to one N3- and three H1+ atoms. The C–N bond length is 1.47 Å. All C–H bond lengths are 1.10 Å. In the second C+0.67- site, C+0.67- is bonded in a tetrahedral geometry to one N3- and three H1+ atoms. The C–N bond length is 1.47 Å. There is two shorter (1.10 Å) and one longer (1.11 Å) C–H bond length. In the third C+0.67- site, C+0.67- is bonded in a tetrahedral geometry to one N3- and three H1+ atoms. The C–N bond length is 1.47 Å. All C–H bond lengths are 1.10 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ba2+, one C+0.67-, and two H1+ atoms. Both N–H bond lengths are 1.03 Å. In the second N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ba2+, one C+0.67-, and two H1+ atoms. Both N–H bond lengths are 1.03 Å. In the third N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ba2+, one C+0.67-, and two H1+ atoms. There is one shorter (1.02 Å) and one longer (1.03 Å) N–H bond length. There are fifteen inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the ninth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the tenth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the eleventh H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the twelfth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the thirteenth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the fourteenth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. In the fifteenth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.67- atom. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 4-coordinate geometry to two equivalent Ba2+ and two Te2- atoms. There are one shorter (2.85 Å) and one longer (3.22 Å) Te–Te bond lengths. In the second Te2- site, Te2- is bonded in a 2-coordinate geometry to two Te2- atoms. The Te–Te bond length is 2.94 Å. In the third Te2- site, Te2- is bonded in a 5-coordinate geometry to three equivalent Ba2+ and two Te2- atoms.

36 MATERIALS SCIENCE↗

Materials Data on Al(CN)3 by Materials Project

Al(CN)3 is alpha Po structured and crystallizes in the trigonal R3m space group. The structure is zero-dimensional and consists of three Al(CN)3 clusters. Al3+ is bonded in a distorted T-shaped geometry to three equivalent N3- atoms. All Al–N bond lengths are 1.97 Å. C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.17 Å. N3- is bonded in a linear geometry to one Al3+ and one C2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Al(CN)3 by Materials Project

Al(CN)3 is Modderite-derived structured and crystallizes in the tetragonal P-42_1m space group. The structure is zero-dimensional and consists of two Al(CN)3 clusters. Al3+ is bonded in a T-shaped geometry to three N3- atoms. There is one shorter (1.96 Å) and two longer (1.97 Å) Al–N bond length. There are two inequivalent C2+ sites. In the first C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.16 Å. In the second C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.17 Å. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a linear geometry to one Al3+ and one C2+ atom. In the second N3- site, N3- is bonded in a linear geometry to one Al3+ and one C2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Ba3Co(CN)3 by Materials Project

Ba3Co(CN)3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Ba2+ is bonded in a 1-coordinate geometry to five equivalent N3- atoms. There are a spread of Ba–N bond distances ranging from 2.78–3.41 Å. Co1+ is bonded in a trigonal planar geometry to three equivalent C+0.67+ atoms. All Co–C bond lengths are 1.78 Å. C+0.67+ is bonded in a distorted linear geometry to one Co1+ and one N3- atom. The C–N bond length is 1.24 Å. N3- is bonded in a distorted single-bond geometry to five equivalent Ba2+ and one C+0.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Sr3Co(CN)3 by Materials Project

Sr3Co(CN)3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Sr2+ is bonded in a 1-coordinate geometry to four equivalent N3- atoms. There are a spread of Sr–N bond distances ranging from 2.56–3.00 Å. Co1+ is bonded in a trigonal planar geometry to three equivalent C+0.67+ atoms. All Co–C bond lengths are 1.76 Å. C+0.67+ is bonded in a distorted linear geometry to one Co1+ and one N3- atom. The C–N bond length is 1.25 Å. N3- is bonded in a 1-coordinate geometry to four equivalent Sr2+ and one C+0.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CsMn(CN)3 by Materials Project

CsMn(CN)3 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent N3- atoms to form distorted CsN12 cuboctahedra that share corners with twelve equivalent CsN12 cuboctahedra, faces with six equivalent CsN12 cuboctahedra, and faces with four equivalent MnN6 octahedra. All Cs–N bond lengths are 3.62 Å. There are two inequivalent Mn2+ sites. In the first Mn2+ site, Mn2+ is bonded to six equivalent N3- atoms to form MnN6 octahedra that share faces with eight equivalent CsN12 cuboctahedra. All Mn–N bond lengths are 1.95 Å. In the second Mn2+ site, Mn2+ is bonded in an octahedral geometry to six equivalent C2+ atoms. All Mn–C bond lengths are 1.92 Å. C2+ is bonded in a linear geometry to one Mn2+ and one N3- atom. The C–N bond length is 1.19 Å. N3- is bonded in a linear geometry to four equivalent Cs1+, one Mn2+, and one C2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on As(CN)3 by Materials Project

As(CN)3 crystallizes in the monoclinic C2 space group. The structure is zero-dimensional and consists of four arsenic cyanide molecules. there are three inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a linear geometry to one As3- and one N3- atom. The C–As bond length is 1.98 Å. The C–N bond length is 1.16 Å. In the second C4+ site, C4+ is bonded in a linear geometry to one As3- and one N3- atom. The C–As bond length is 1.97 Å. The C–N bond length is 1.17 Å. In the third C4+ site, C4+ is bonded in a linear geometry to one As3- and one N3- atom. The C–As bond length is 1.96 Å. The C–N bond length is 1.17 Å. As3- is bonded in a distorted T-shaped geometry to three C4+ atoms. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a single-bond geometry to one C4+ atom. In the second N3- site, N3- is bonded in a single-bond geometry to one C4+ atom. In the third N3- site, N3- is bonded in a single-bond geometry to one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on As(CN)3 by Materials Project

As(CN)3 crystallizes in the monoclinic C2 space group. The structure is zero-dimensional and consists of four arsenic cyanide molecules. there are three inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a distorted linear geometry to one As3- and one N3- atom. The C–As bond length is 1.95 Å. The C–N bond length is 1.17 Å. In the second C4+ site, C4+ is bonded in a linear geometry to one As3- and one N3- atom. The C–As bond length is 1.93 Å. The C–N bond length is 1.17 Å. In the third C4+ site, C4+ is bonded in a linear geometry to one As3- and one N3- atom. The C–As bond length is 1.95 Å. The C–N bond length is 1.17 Å. As3- is bonded in a distorted T-shaped geometry to three C4+ atoms. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a single-bond geometry to one C4+ atom. In the second N3- site, N3- is bonded in a single-bond geometry to one C4+ atom. In the third N3- site, N3- is bonded in a single-bond geometry to one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on KMn(CN)3 by Materials Project

KMn(CN)3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. K1+ is bonded in a 2-coordinate geometry to seven N3- atoms. There are a spread of K–N bond distances ranging from 2.96–3.34 Å. There are two inequivalent Mn2+ sites. In the first Mn2+ site, Mn2+ is bonded in an octahedral geometry to six C2+ atoms. All Mn–C bond lengths are 1.91 Å. In the second Mn2+ site, Mn2+ is bonded in an octahedral geometry to six N3- atoms. There is four shorter (1.96 Å) and two longer (1.97 Å) Mn–N bond length. There are three inequivalent C2+ sites. In the first C2+ site, C2+ is bonded in a linear geometry to one Mn2+ and one N3- atom. The C–N bond length is 1.19 Å. In the second C2+ site, C2+ is bonded in a linear geometry to one Mn2+ and one N3- atom. The C–N bond length is 1.19 Å. In the third C2+ site, C2+ is bonded in a linear geometry to one Mn2+ and one N3- atom. The C–N bond length is 1.19 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a bent 150 degrees geometry to three equivalent K1+, one Mn2+, and one C2+ atom. In the second N3- site, N3- is bonded in a distorted bent 150 degrees geometry to two equivalent K1+, one Mn2+, and one C2+ atom. In the third N3- site, N3- is bonded in a distorted bent 150 degrees geometry to two equivalent K1+, one Mn2+, and one C2+ atom.

36 MATERIALS SCIENCE↗

Performance Improvement of Lithium Metal Batteries Enabled By LiBF 3 CN as a New Electrolyte Additive

A newly synthesized electrolyte additive, lithium trifluoro(cyano) borate (LiBF 3 CN), has been investigated for electrochemical performance improvement of lithium metal batteries. The LiBF 3 CN has a structure where one fluorine atom of BF 4 – is substituted with a cyano group (–CN) prepared by the reaction of boron trifluoride etherate with lithium cyanide. The electrochemical performance in symmetric Li/Li cells and NCM523/Li cells is significantly improved upon the incorporation of LiBF 3 CN as an electrolyte additive into a carbonate-based electrolyte. Extensive characterization of the deposited lithium metal reveals that a thin (≈20 nm) and robust SEI composed of LiN x O y , Li 3 N and Li 2 O is formed by the reductive decomposition of the LiBF 3 CN additive, which plays an important role in decreasing the resistance and stabilizing lithium deposition/stripping. The insight into the substitution effect of a functional group obtained from this work provides guidance for the design of new electrolyte additives.

25 ENERGY STORAGE↗

Phase coexistence at the first-order Mott transition revealed by pressure-dependent dielectric spectroscopy of κ - (BEDT-TTF) 2 - Cu 2 (CN) 3

The dimer Mott insulator kappa - (BEDT-TTF) 2 - Cu 2 (CN) 3 can be tuned into metallic and superconducting states on applying pressure of 1.5 kbar and more. We have performed dielectric measurements (7.5 kHz to 5 MHz) on kappa - (BEDT-TTF) 2 - Cu 2 (CN) 3 single crystals as a function of temperature (down to T = 8 K) and pressure (up to p = 4.3 kbar). In addition to the relaxor-like dielectric behavior seen below 50 K at p = 0, that moves toward lower temperatures with pressure, a second peak emerges in ε 1 (T) around T = 15 K. When approaching the insulator-metal boundary, this peak diverges rapidly reaching ε 1 ≈ 10 5 . Our dynamical mean-field theory calculations substantiate that the dielectric catastrophe at the Mott transition is not caused by closing the energy gap, but due to the spatial coexistence of correlated metallic and insulating regions. We discuss the percolative nature of the first-order Mott insulator-to-metal transition in all details.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Materials Data on P(CN)3 by Materials Project

(CN)3P crystallizes in the tetragonal I-42d space group. The structure is zero-dimensional and consists of forty-eight hydrogen cyanide molecules and sixteen phosphine molecules.

36 MATERIALS SCIENCE↗