research communications
Synthesis and
of cerium(IV) bis(phosphite)aDepartment of Chemistry, Creighton University, 2500 California Plaza, Omaha, Nebraska 68178, USA
*Correspondence e-mail: ericvilla@creighton.edu
The structure of cerium(IV) bis(phosphite), Ce(HPO3)2, has been solved by single-crystal X-ray diffraction and has trigonal (P-3m1) symmetry. The cerium(IV) cation exhibits -3m. and is octahedrally coordinated by O atoms of the phosphite ligands (point group symmetry 3m.). The highly symmetrical compound has a layered structure parallel to the ab plane, and is closely related to zirconium(IV) bis(phosphite) solved via powder X-ray diffraction with trigonal (P-3 symmetry. Structural details of the two compounds are comparatively discussed.
Keywords: crystal structure; cerium(IV); phosphite.
CCDC reference: 1565300
1. Chemical context
Phosphonates are commonly employed within the petroleum industry as antioxidants. Interactions between these antioxidants and possible metal impurities could potentially have unintended consequences in the processing of petroleum products. We are currently studying these interactions by exploring the crystalline materials formed via solvothermal syntheses of lanthanides with phosphorous acid.
Phosphorous acid (H3PO3) is a powerful reducing agent and is exceedingly water soluble. The anion HPO32− has many different names in the literature, including (but not limited to) phosphite, phosphonate, phosphorus(III) oxoanion, oxophosphate(III) and hydridotrioxidophosphate(2-). According to IUPAC, when the hydrogen atom is directly bonded to the phosphorus atom, it is to be named phosphonate; whereas when the anion tautomerizes to the PO2(OH)2− anion, it is named as phosphite. However, the latter ion is rarely identified in the solid state. While IUPAC prefers HPO32− to be named phosphonate, this name is also used for organophosphorus compounds with the general formula R-PO(OH)2 or R-PO(OR)2, where R = alkyl or To eliminate any confusion with organophosphorus compounds and to be consistent with the recent literature, we will herein refer to the HPO32− anion as phosphite.
The phosphite anion has many structural similarities to both phosphates and organophosphonates. In the phosphite anion, a hydrogen atom has replaced one of the oxygen atoms, which would be found in phosphate; also, the phosphite anion contains no P—C bonds that are found in phosphonates. Phosphite itself can be used as a precursor for making a vast array of phosphonates. In phosphite, the central phosphorus atom is PIII instead of the more air-stable PV, which provides the opportunity for redox chemistry. This ability to act as a reducing agent has led to several mixed-valent uranium compounds (Villa et al., 2012; Villa, Marr et al., 2013; Villa, Alekseev et al., 2013). Moving towards the lanthanides, lanthanide phosphite compounds have been synthesized in one of two main ways: hydrothermally (Cross et al., 2012; Ewald et al., 2003, 2005; Foulon et al., 1993a,b,1995; Loukili et al., 1988, 1991; Tijani et al., 1988; Xiong et al., 2006, 2009; Zhang et al., 1992) and phosphite reactions (Zakharova et al., 2003). We have expanded this chemistry by exploring solvothermal syntheses of lanthanide phosphites. Herein we will discuss the of the title compound, a new cerium(IV) bis(phosphite).
2. Structural commentary
The title compound Ce(HPO3)2 crystallizes in the Pm1. The smallest repeating unit contains one cerium(IV), one oxygen, one phosphorus(III) and one hydrogen atom. This simple structure contains slightly distorted octahedrally coordinated cerium(IV) cations (site symmetry m.; Fig. 1), which are linked together by corner-sharing phosphite ligands. These phosphite ligands have a slightly distorted tetrahedral configuration (point group symmetry 3m.). Each phosphorus(III) atom in the phosphite ligand is bonded to three oxygen atoms, comprising the bottom of the tetrahedron, and one hydrogen atom. The sheets of Ce(HPO3)2, which are located in the ab plane, contain alternating up–down phosphite ligands around the cerium(IV) metal cation, as indicated by the different directions of the hydrogen atoms (Figs. 2, 3). These sheets are layered down the c axis, where each cerium(IV) atom resides directly below the cerium above it at a distance of 5.6099 (3) Å, which corresponds to the length of the c axis; between the layers, the Ce—Ce—Ce angle is 180.0° (Fig. 3).
This structure is closely related to a known zirconium(IV) bis(phosphite), Zr(HPO3)2, which was isolated via a very different synthesis route involving refluxing in concentrated phosphorous acid and using HF to precipitate the desired compound (Millini et al., 1993). The structure was elucidated from powder X-ray diffraction data and has many similarities to the title structure shown above (Table 1). The main difference between the two is the metal–oxygen bond length, where the Ce—O bond length is unsurprisingly slightly longer. The zirconium coordination appears to be a bit closer to being octahedral than the cerium, but they are nearly the same after comparing the error of refinement.
3. Synthesis and crystallization
Cerium(IV) bis(phosphite) was synthesized solvothermally in acetonitrile (CH3CN). A stock solution of 1.00 M H3PO3 was prepared in acetonitrile. 0.0572 grams of ceric ammonium nitrate, (NH4)2Ce(NO3)6, was placed into a PTFE liner along with 2 ml of the 1.00 M phosphorous acid solution, yielding a solution 0.0522 M ceric ammonium nitrate. This gives an approximate molar ratio of cerium(IV) to phosphite of 1:20. After the cerium was completely dissolved, the PTFE liner was capped and sealed inside of a stainless steel autoclave. This was then placed into a programmable box furnace and heated to 363 K over a period of 30 minutes, held at 363 K for four h and then cooled for 975 minutes down to 298 K (or a rate of 4 K per hour).
The resulting mixture was washed with cold water and then placed into a plastic petri dish. The excess water was removed and the crystals were dispersed with acetonitrile. The large, hexagonal prisms of the title compound were light yellow in color. Many suitable crystals were present. A large crystal was isolated in immersion oil and broken perpendicular to the hexagonal face to yield a clean crystal for single-crystal X-ray diffraction.
4. Refinement
Crystal data, data collection and structure . The hydrogen-atom position was placed as a riding atom on the phosphorus position. The maximum electron density peaks are 0.330 e− Å−3 (located between P1 and O1 at 0.686 and 0.838 Å, respectively), 0.320 e− Å−3 (located adjacent to O1 at 0.608 Å) and 0.250 e Å−3 (located adjacent to Ce1 at 0.692 Å), which lead to nothing reasonable. All other maximum density peaks are under 0.2 e− Å−3. The minimum electron density is a very minimal at −0.609 e− Å−3. Two electron density holes of about the same magnitude reside around the phosphorus atom.
details are summarized in Table 2
|
Supporting information
CCDC reference: 1565300
Data collection: CrysAlis PRO (Rigaku OD, 2015); cell
CrysAlis PRO (Rigaku OD, 2015); data reduction: CrysAlis PRO (Rigaku OD, 2015); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009) and CrystalMaker (Palmer, 2014); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).Ce(HPO3)2 | Dx = 3.172 Mg m−3 |
Mr = 300.08 | Mo Kα radiation, λ = 0.71073 Å |
Trigonal, P3m1 | Cell parameters from 1912 reflections |
a = 5.6859 (3) Å | θ = 4.0–32.7° |
c = 5.6099 (3) Å | µ = 7.71 mm−1 |
V = 157.07 (2) Å3 | T = 293 K |
Z = 1 | Hexagonal, clear light yellow |
F(000) = 138 | 0.21 × 0.09 × 0.08 mm |
Rigaku SCX-Mini diffractometer | 197 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 197 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
ω scans | θmax = 30.5°, θmin = 5.5° |
Absorption correction: multi-scan (CrysAlis PRO; Rigaku OD, 2015) | h = −8→8 |
Tmin = 0.799, Tmax = 1.000 | k = −8→8 |
1852 measured reflections | l = −7→8 |
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.010 | Only H-atom coordinates refined |
wR(F2) = 0.029 | w = 1/[σ2(Fo2) + (0.0148P)2 + 0.0962P] where P = (Fo2 + 2Fc2)/3 |
S = 1.26 | (Δ/σ)max < 0.001 |
197 reflections | Δρmax = 0.51 e Å−3 |
13 parameters | Δρmin = −0.35 e Å−3 |
0 restraints |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. The structure was refined using SHELXT (Sheldrick, 2015) Intrinsic Phasing and SHELXL (Sheldrick, 2015). Olex2 (Dolomanov et al., 2009) was used as a graphical interface. Images of the above compound were made using CrystalMaker for Windows, version 9.2.8 (CrystalMaker, 2017). The refinement proceeded without any incidents and without any need for modelling disorder or twinning or restraints. The crystal was then mounted on MiTeGen Microloop with non-drying immersion oil. The crystal was then optically aligned on the Rigaku SCX-Mini diffractometer using a digital camera. Initial matrix images were collected to determine the unit cell, validity and proper exposure time. Three hemispheres (where φ= 0.0, 120.0 and 240.0) of data were collected with each consisting 180 images each with 1.00° widths and a 1.00° step. Refinement of the structure was based on F2 against all reflections. The R-factor R is based on F2>2σ(F2), but is not relevant to the choice of reflections for refinement; whereas the weighted R-factor wR and goodness of fit S are based on F2. Due to the presence of exclusively intense diffraction peaks, there is no observable difference between the R factors for all versus gt. |
x | y | z | Uiso*/Ueq | ||
Ce1 | 1.0000 | 1.0000 | 0.5000 | 0.01612 (11) | |
P1 | 0.6667 | 0.3333 | 0.19839 (17) | 0.01440 (18) | |
O1 | 0.81417 (19) | 0.6283 (4) | 0.2762 (4) | 0.0330 (4) | |
H1 | 0.6667 | 0.3333 | −0.059 (11) | 0.040* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ce1 | 0.00810 (11) | 0.00810 (11) | 0.03215 (17) | 0.00405 (6) | 0.000 | 0.000 |
P1 | 0.0114 (3) | 0.0114 (3) | 0.0204 (4) | 0.00569 (13) | 0.000 | 0.000 |
O1 | 0.0330 (8) | 0.0141 (8) | 0.0456 (9) | 0.0071 (4) | −0.0037 (4) | −0.0074 (7) |
Ce1—O1 | 2.2193 (19) | P1—H1 | 1.44 (6) |
P1—O1 | 1.5168 (19) | ||
O1i—Ce1—O1ii | 180.0 | O1ii—Ce1—O1 | 91.15 (8) |
O1iii—Ce1—O1iv | 88.85 (8) | O1i—Ce1—O1v | 91.15 (8) |
O1i—Ce1—O1iv | 88.85 (8) | O1ii—Ce1—O1iv | 91.15 (8) |
O1—Ce1—O1iv | 91.15 (8) | O1—Ce1—O1v | 88.85 (8) |
O1—Ce1—O1iii | 180.00 (9) | O1vi—P1—O1vii | 112.07 (8) |
O1iii—Ce1—O1v | 91.15 (8) | O1vi—P1—O1 | 112.07 (8) |
O1i—Ce1—O1iii | 91.15 (8) | O1vii—P1—O1 | 112.07 (8) |
O1i—Ce1—O1 | 88.85 (8) | O1—P1—H1 | 106.73 (9) |
O1ii—Ce1—O1iii | 88.85 (8) | O1vi—P1—H1 | 106.73 (9) |
O1ii—Ce1—O1v | 88.85 (8) | O1vii—P1—H1 | 106.73 (9) |
O1iv—Ce1—O1v | 180.0 | P1—O1—Ce1 | 162.28 (14) |
Symmetry codes: (i) x−y+1, x, −z+1; (ii) −x+y+1, −x+2, z; (iii) −x+2, −y+2, −z+1; (iv) −y+2, x−y+1, z; (v) y, −x+y+1, −z+1; (vi) −x+y+1, −x+1, z; (vii) −y+1, x−y, z. |
Bond lengths | Ce(HPO3)2 | Zr(HPO3)2 | bond angles | Ce(HPO3)2 | Zr(HPO3)2 |
Metal—O | 2.2193 (19) | 2.05 (2) | O—metal—O | 88.85 (8), 91.15 (8) | 89.2 (4), 90.8 (4) |
P—O | 1.5168 (19) | 1.52 (1) | metal—O—P | 162.28 (14) | 162.1 (3) |
P—H | 1.44 (6) | 1.43 (fixed) | O—P—O | 112.07 (8) | 111.2 (5) |
O—P—H | 106.73 (9) | 107.6 (6) |
Zr(HPO3)2 data from Millini et al. (1993). |
Acknowledgements
EMV and SHB would like to thank Creighton University, Creighton College of Arts and Sciences, and the Creighton University Chemistry Department for supporting undergraduate research. Funding for the project was graciously provided by Creighton University.
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