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Materials Data on TiOF by Materials Project

TiOF crystallizes in the orthorhombic Pmmn space group. The structure is two-dimensional and consists of one TiOF sheet oriented in the (0, 0, 1) direction. Ti3+ is bonded to four equivalent O2- and two equivalent F1- atoms to form a mixture of edge and corner-sharing TiO4F2 octahedra. The corner-sharing octahedral tilt angles are 4°. There are two shorter (2.02 Å) and two longer (2.07 Å) Ti–O bond lengths. Both Ti–F bond lengths are 2.01 Å. O2- is bonded in a rectangular see-saw-like geometry to four equivalent Ti3+ atoms. F1- is bonded in a water-like geometry to two equivalent Ti3+ atoms.

36 MATERIALS SCIENCE↗

Correlated Anion Disorder in Heteroanionic Cubic TiOF 2

Resolving anion configurations in heteroanionic materials is crucial for understanding and controlling their properties. For anion-disordered oxyfluorides, conventional Bragg diffraction cannot fully resolve the anionic structure, necessitating alternative structure determination methods. We have investigated the anionic structure of anion-disordered cubic (ReO 3 -type) TiOF 2 using X-ray pair distribution function (PDF), 19 F MAS NMR analysis, density functional theory (DFT), cluster expansion modeling, and genetic-algorithm structure prediction. Our computational data predict short-range anion ordering in TiOF 2 , characterized by predominant cis-[O 2 F 4 ] titanium coordination, resulting in correlated anion disorder at longer ranges. To validate our predictions, we generated partially disordered supercells using genetic-algorithm structure prediction and computed simulated X-ray PDF data and 19 F MAS NMR spectra, which we compared directly to experimental data. To construct our simulated 19 F NMR spectra, we derived new transformation functions for mapping calculated magnetic shieldings to predicted magnetic chemical shifts in titanium (oxy)fluorides, obtained by fitting DFT-calculated magnetic shieldings to previously published experimental chemical shift data for TiF 4 . We find good agreement between our simulated and experimental data, which supports our computationally predicted structural model and demonstrates the effectiveness of complementary experimental and computational techniques in resolving anionic structure in anion-disordered oxyfluorides. From additional DFT calculations, we predict that increasing anion disorder makes lithium intercalation more favorable by, on average, up to 2 eV, highlighting the significant effect of variations in short-range order on the intercalation properties of anion-disordered materials.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Materials Data on TiOF by Materials Project

TiOF crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ti3+ is bonded to four equivalent O2- and two equivalent F1- atoms to form a mixture of edge and corner-sharing TiO4F2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ti–O bond lengths are 2.04 Å. Both Ti–F bond lengths are 1.98 Å. O2- is bonded in a square co-planar geometry to four equivalent Ti3+ atoms. F1- is bonded in a linear geometry to two equivalent Ti3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on TiOF by Materials Project

TiOF is zeta iron carbide-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ti3+ is bonded to three equivalent O2- and three equivalent F1- atoms to form a mixture of edge and corner-sharing TiO3F3 octahedra. The corner-sharing octahedra tilt angles range from 40–58°. There are a spread of Ti–O bond distances ranging from 1.90–1.97 Å. There are two shorter (2.17 Å) and one longer (2.20 Å) Ti–F bond lengths. O2- is bonded in a 3-coordinate geometry to three equivalent Ti3+ atoms. F1- is bonded in a distorted trigonal planar geometry to three equivalent Ti3+ atoms.

36 MATERIALS SCIENCE↗

Etching-Chemistry-Driven Ruthenium Doping on Ti 3 C 2 T x MXene for Optimizing Electrochemical Performance

We demonstrate that the etching chemistry used during MXene synthesis from Ti 3 AlC 2 MAX phase significantly influences surface functionalization and structural vacancies, which in turn affect ruthenium (Ru) ion interactions. Using hydrofluoric acid (HF) and ammonium bifluoride (NH 4 HF 2 ) as etchants, we obtained MXene surfaces with distinct functional groups and Ti vacancies that impact Ru ion interactions and electrochemical performance. Both MXene variants (labeled MX(H) and MX(N), respectively) exhibited negative zeta potentials in their pristine state, but upon the addition of Ru the zeta potential for MX(H) reached 12.9 mV while that for MX(N) remained negative at −6.4 mV. This adsorption resulted in a 14.4-fold increase in the specific capacitance of MX(H)/Ru compared to pristine MX(H), whereas MX(N)/Ru exhibited only a 4.4-fold increase over its pristine counterpart. X-ray diffraction analysis identified the formation of ammonium titanium oxide fluoride, (NH 4 ) 3 TiOF 5 , on MX(N), which likely contributed to its reduced Ru adsorption. X-ray photoelectron spectroscopy suggested the presence of Ti vacancies in both MXene variants; however, their behavior toward Ru accommodation differed markedly, with MX(H) showing the most obvious shift in the Ti 2p peak in the XPS survey spectrum, while MX(N) showed the most obvious shift in the C 1s peak. Electron paramagnetic resonance spectroscopy further demonstrated a distinct alteration in the spectral signatures of MX(H) upon Ru addition, in contrast to the negligible changes in MX(N), indicating effective passivation of the Ti defect sites in MX(H) via vacancy-assisted Ru doping. Cyclic voltammetry showed that Ru-incorporated MX(H) nanocomposites exhibit more efficient redox-active sites, as reflected in their higher capacitance values. These findings highlight the pivotal role of MXene surface chemistry in controlling cation adsorption, providing valuable insights for the rational design of high-performance electrodes.

2D surface engineering↗