Pith. sign in

REVIEW 3 major objections 4 minor 1 cited by

Lanthanide L-Edge Spectroscopy of High-Entropy Oxides: Insights into Valence and Phase Stability

T0 review · 3 major / 4 minor · reviewed 2026-08-15 · deepseek-v4-flash

Pith's one-line read In Ceₓ(SmPrLaY)₁₋ₓO₂₋δ, raising cerium from 20% to 40% switches the crystal from bixbyite to fluorite while every cation keeps its oxidation state, so the phase change is compositional, not redox-driven.

desk verdict Solid valence measurements, overreached transition-mechanism claim; the XANES is the contribution. read the letter →

arxiv 2505.08055 v1 pith:HGM4HTYP submitted 2025-05-12 cond-mat.mtrl-sci

classification cond-mat.mtrl-sci
keywords high-entropyoxidesX-rayabsorptionspectroscopyXANESlanthanideL-edgebixbyite-fluoritetransitionceriumvalencepraseodymiummixedBaderchargeanalysis
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper asks why a five-cation rare-earth oxide changes crystal structure as its cerium fraction rises. It answers, using element-specific L3-edge X-ray absorption spectroscopy and DFT charge-partitioning analysis, that in $\mathrm{Ce}_x(\mathrm{SmPrLaY})_{1-x}\mathrm{O}_{2-\delta}$ the bixbyite-to-fluorite transition is not accompanied by any meaningful change in cation oxidation states: lanthanum and samarium stay trivalent, cerium stays mostly tetravalent with a constant ~10% Ce³⁺ fraction, and praseodymium stays mixed-valent near 3.5–3.6. The transition therefore appears driven by composition and its consequences for configurational entropy and anion-sublattice disorder, not by redox chemistry. If this holds, valence and crystal structure can be tuned independently in this high-entropy oxide family.

What carries the argument

The central probe is L3-edge X-ray absorption near-edge structure (XANES): a 2p core electron is excited into unoccupied 5d states, and the edge energy reports oxidation state while the white-line shape reports local coordination. The paper combines second-derivative white-line analysis for La, an L3-FWHM/L1 pre-edge correlation for Sm, a four-Gaussian fit for Ce that separates Ce³⁺ from Ce⁴⁺ final states, and a Lorentzian intensity-ratio fit for Pr, all calibrated against synthesized standards. On the computational side, the load-bearing object is Bader charge analysis of DFT charge densities from special quasi-random supercells, with identical cation configurations in both bixbyite and fluorite symmetry; the near-identical charge distributions across the two phases are what carry the inference that redox is not the driver.

What would settle it

Compute or measure the relative formation enthalpy (ideally free energy) of relaxed bixbyite and fluorite supercells of $\mathrm{Ce}_x(\mathrm{SmPrLaY})_{1-x}\mathrm{O}_{2-\delta}$ at $x = 0.20$, $0.325$, and $0.40$ at the 1400 °C synthesis temperature. If fluorite is not thermodynamically preferred at 40% Ce, or if the crossover composition does not match the observed transition, the compositional-entropy mechanism fails even though cation valences are unchanged.

Watch

Extended reading notes

Core claim

In $\mathrm{Ce}_x(\mathrm{SmPrLaY})_{1-x}\mathrm{O}_{2-\delta}$, as $x$ rises from 20 to 40 at.% Ce, X-ray diffraction shows a complete transformation from the bixbyite structure (Ia-3) to the fluorite structure (Fm-3m). L3-edge XANES of each lanthanide, benchmarked against standards, shows La and Sm remain 3+, Ce remains predominantly 4+ with a persistent ~10% Ce³⁺ component, and Pr remains mixed-valent with an estimated valence of 3.5–3.6; the Sm L3 white-line shape shifts toward the fluorite reference at 40% Ce. DFT with charge partitioning on disordered supercells of both phases yields essentially identical cation charge distributions between bixbyite and fluorite. The authors conclude that the structural transition is compositional in origin — the increasing tetravalent Ce fraction, configurational entropy, and anion-sublattice disorder — rather than a cation redox event, with oxygen vacancies maintaining electroneutrality.

Load-bearing premise

The mechanism claim — that configurational entropy and anion-sublattice disorder, not cation redox, drive the transition — rests on the invariance of measured and computed cation charges; the paper does not directly compare formation energies or free energies of the bixbyite and fluorite phases, so the driver is inferred from charge similarity rather than demonstrated energetically.

Editorial extensions

If this is right

  • Cerium fraction becomes a structural dial in this oxide family: raising it moves the material from bixbyite to fluorite without changing lanthanide valences, so phase and redox behavior can be selected separately.
  • The persistent ~10% Ce³⁺ component across all compositions implies a roughly constant oxygen-vacancy population, which should make ionic transport in these high-entropy oxides predictable from composition alone.
  • Element-specific L3-edge XANES can resolve oxidation states in multicomponent rare-earth oxides where XPS peak overlaps make deconvolution unreliable.
  • Stable trivalent La and Sm mean their L3 white-line shapes can serve as local coordination fingerprints for bixbyite-like versus fluorite-like environments in related high-entropy oxides.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Beyond the paper: if cation valences are truly pinned, substituting a redox-inactive tetravalent cation such as Zr⁴⁺ for Ce should reproduce the same bixbyite-to-fluorite crossover, confirming that the tetravalent fraction, not cerium's redox chemistry, is the controlling variable.
  • Beyond the paper: the roughly constant Ce³⁺ fraction implies the oxygen-vacancy concentration is also roughly composition-independent; a testable prediction is that oxygen diffusivity or ionic conductivity measured by isotope exchange or impedance spectroscopy will not jump discontinuously across the 20–40% Ce phase boundary.
  • Beyond the paper: the paper's mechanism is a correlation-based inference; direct free-energy comparisons or in situ high-temperature diffraction and XAS across the transition would turn it into a causal statement.
  • Beyond the paper: independent control of valence and structure could be exploited in devices such as ceria-based memristors, where Ce³⁺/Ce⁴⁺ polaron hopping sets the electronic behavior while the crystal structure could be pinned separately by composition.
Share X Bluesky LinkedIn Reddit HN

Signed reviews

No signed human review yet.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 4 minor

Summary. The manuscript reports an X-ray absorption spectroscopy (XANES) study of the high-entropy oxide series Ce_x(SmPrLaY)_(1-x)O_(2-δ) at x = 20, 32.5, and 40%, combined with DFT Bader charge analysis. XRD shows a bixbyite-to-fluorite transition as Ce increases. L3-edge XANES of La and Sm indicates stable trivalent states, Ce remains predominantly tetravalent with a minor ~10% Ce3+ component, and Pr maintains a mixed valence around 3.5–3.6 across all compositions. DFT Bader charge analysis on SQS supercells of both phases yields similar average cation charges between bixbyite and fluorite. The central claim is that the phase transition is driven by compositional effects rather than cation redox, with invariant cation valences allowing independent tuning of valence and structure.

Significance. If the result holds, this is a useful demonstration that element-specific XANES can quantify valence in multicomponent rare-earth oxides and that the bixbyite-to-fluorite transition in this HEO family occurs without significant cation redox activity. The use of external standards to anchor Ce, Pr, La, and Sm valences is a strength, as is the independent DFT Bader analysis, which does not calibrate to the XANES results. The conclusion that the transition mechanism is compositional, however, currently rests on charge similarity rather than on a direct phase-energetics comparison, so the mechanistic portion needs substantial support or tempering before the central claim is fully established.

major comments (3)
  1. [DFT Bader Analysis (p. 9, Fig. 7)] The conclusion that the bixbyite-to-fluorite transition 'does not arise from significant cation redox activity but is instead driven by configurational entropy and the evolution of anion sublattice disorder' does not follow from the Bader charge comparison alone. Bader charges are a charge-partitioning descriptor, not a thermodynamic potential, and the paper reports no total-energy or free-energy comparison between bixbyite and fluorite supercells at any composition. Without ΔE(x), or at least vacancy-formation enthalpies in both phases, the data support valence invariance but cannot distinguish a compositional/entropic driving force from a redox-related one. Please add direct phase-energetics calculations, or revise the claim to state that the results are consistent with, but do not prove, a compositional mechanism.
  2. [Results and Discussion, closing paragraph (p. 8–9)] The statement 'The relatively consistent Ce³⁺ content suggests that oxygen vacancy concentrations remain largely constant across the series' is arithmetically inconsistent with the reported valences. If La, Sm, and Y are fixed at 3+, Pr is approximately 3.5–3.6, and Ce is approximately 90% 4+ and 10% 3+, then increasing the Ce fraction x raises the average cation charge, so the charge-neutral oxygen content must increase and δ must decrease as x increases. A constant Ce³⁺ fraction therefore implies a changing oxygen-vacancy concentration, not a constant one. This claim needs to be corrected or replaced with a proper charge-balance equation, as it directly affects the paper's implications for ionic transport.
  3. [Sm Absorption Edge (p. 6, Fig. 4)] The inference that the 40% Ce sample adopts a fluorite-like Sm coordination is based on placement of the HEO samples relative to a line of best fit through standard compounds, but no fit parameters, residuals, uncertainties on the HEO FWHM values, or correlation statistics are reported. Given the acknowledged weak Sm L1 signal, this comparison is not quantitatively supported. Please report the FWHM values with uncertainties, the line-of-best-fit parameters and confidence intervals, or soften the coordination-environment conclusion.
minor comments (4)
  1. [DFT Bader Analysis (p. 9)] The text refers to 'Figure 4a' and 'Figure 4c' when discussing Bader charge distributions, but the actual figure is Figure 7; the figure citations should be corrected.
  2. [DFT Bader Analysis (p. 9)] The description that Pr 'shows a noticeable decrease in average Bader charge between 31% and 38% Ce content before stabilizing' appears to conflict with the earlier statement that Pr maintains a consistent mixed-valence state; please clarify whether this variation is within the expected scatter or a real trend.
  3. [Supplementary Table S1] The entry for LaCrO3 lists the powder formula as '0.4 La2O3+0.6CeO2', which appears to be a typo for the La2O3 + Cr2O3 mixture, and the La(OH)3 entry lists a mixed powder formula that does not correspond to the stated standard; please correct these entries.
  4. [Abstract and Conclusions] The phrasing 'driven by compositional effects' is stronger than what the current evidence supports; consider aligning the abstract and conclusions with the more measured statement that the measurements show invariant cation valences across the phase transition.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: valence assignments are anchored to external standards and DFT Bader analysis is independent of the XANES fits.

full rationale

The paper's derivation chain is self-contained. Ce and Pr valence estimates come from fitting L3-edge XANES with peak assignments and standards established in the literature (CeO2, CeF3, Pr6O11, Pr2O3), and La/Sm trivalence is judged against external standard spectra. The DFT Bader charge analysis is computed independently with r2SCAN, PAW pseudopotentials, and SQS supercells, and is used only to corroborate the experimentally measured valence invariance rather than to construct it. The bixbyite-to-fluorite transition is established by XRD and supported by Sm L1/L3 lineshape trends. The mechanistic assertion that the transition is 'driven by compositional effects rather than cation redox' is an inference drawn from the invariance of cation valences and Bader charges across the two structures; it lacks a direct phase-energy comparison, but underdetermination is not circularity. Similarly, the statement that consistent Ce3+ content 'suggests that oxygen vacancy concentrations remain largely constant' is an imperfect stoichiometric inference, not a reuse of fitted inputs as a prediction. The self-citations present ([4], [17], [31]) are background or methodological benchmarking references and are not load-bearing reductions of the central claim. No equation or fitted parameter is renamed as a prediction, and no result reduces by construction to its own input.

Assumptions & free parameters 2 free parameters · 6 assumptions · 0 invented entities

The paper introduces no new particles, forces, or conserved quantities. Its central claims rest on standard XANES peak-decomposition assignments from the literature, on the transferability of those assignments to the HEO environment, and on the assumption that Bader charge trends and air-quenched XRD phases reflect the thermodynamic state. The only fitted quantities are the Ce3+ percentages and Pr valence estimates derived from peak-area ratios.

free parameters (2)
  • Ce3+ fraction from Gaussian peak-area fitting = 9.2-11.7% (sample-dependent, Table 1)
    The central claim that Ce is predominantly 4+ with a minor Ce3+ component rests on the fitted areas of peaks A-D in the Ce L3 edge.
  • Pr average oxidation state from IC/IA ratio = 3.54-3.60 (Table 1)
    The mixed-valence claim for Pr rests on the Lorentzian fits and the ratio-intensity correlation calibrated with Pr6O11 and Pr2O3.
assumptions (6)
  • domain assumption Ce L3 XANES peaks A-D correspond to transitions 2p to delocalized d, 2p4f15d (Ce3+), 2p4f05d and 2p4f15dL (Ce4+).
    Invoked from Ref. [44] and used without re-validation for the HEO environment (Results, Ce Absorption Edge).
  • domain assumption Pr L3 peaks A-C correspond to Pr3+ 2p to 4f2 and Pr4+ 2p to 4f1 and 2p to 4f2L transitions.
    Invoked from Ref. [45] and applied to the HEO series (Results, Pr Absorption Edge).
  • domain assumption The first minimum in the second derivative of the La L3 edge reports the d-orbital ligand-field splitting energy.
    Used to conclude a consistent coordination environment for La across the series (Results, La Absorption Edge).
  • domain assumption Bader charge analysis trends reflect oxidation-state trends for rare-earth cations in oxides.
    The paper uses Bader charges to compare redox behavior across phases (Results, DFT Bader Analysis); Bader charges are known to be lower than formal oxidation states, which the paper acknowledges.
  • domain assumption Air-quenching from 1400 C preserves the high-temperature phase.
    Used to relate the room-temperature XRD phases to the sintered state (Experimental Methods).
  • domain assumption r2SCAN with PAW and f electrons in valence is accurate for these rare-earth oxides.
    Relied on the authors' own benchmark [31] and prior literature (Computational Methods).

how reviews work

0 comments
Cite this review

Pith. "Pith review of Lanthanide L-Edge Spectroscopy of High-Entropy Oxides: Insights into Valence and Phase Stability." pith.science (2026). https://pith.science/paper/HGM4HTYP

@misc{pith2026250508055,
  author       = {Pith},
  title        = {Pith review of: Lanthanide L-Edge Spectroscopy of High-Entropy Oxides: Insights into Valence and Phase Stability},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/HGM4HTYP}},
  note         = {Machine review of arXiv:2505.08055}
}
read the original abstract

High-entropy oxides (HEOs) are a promising class of multicomponent ceramics with tunable structural and electronic properties. In this study, we investigate the local electronic structure of rare-earth HEOs in the (Ce, Sm, Pr, La, Y)O2 system using X-ray absorption spectroscopy (XAS). By systematically increasing the Ce concentration, we observe a phase transition from bixbyite to fluorite, tracked by X-ray diffraction (XRD) and corroborated by L-edge XANES analysis of La, Sm, Ce, and Pr. The oxidation states of La and Sm remain trivalent, while Ce exhibits a minor Ce 3+ fraction and Pr shows a consistent mixed-valence state. Density functional theory (DFT) calculations with Bader charge analysis support these findings and reveal that the phase transition is driven by compositional effects rather than cation redox. Our combined experimental and computational approach provides new insights into structure-valence correlations in RE-HEOs and their implications for ionic transport and phase stability.

Discussion (0). Continue with ORCID to comment.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Disorder by Design: Unveiling Local Structure and Functional Insights in High Entropy Oxides

    cond-mat.mtrl-sci 2025-06 unverdicted novelty 1.0 of 10

    A synthesis of evidence that local structural disorder, not average crystallography, drives transport, catalytic, magnetic, and dielectric behavior in high entropy oxides, with a guide to the tools that reveal it.

Reference graph

Works this paper leans on

53 extracted references · 30 canonical work pages · cited by 1 Pith paper

  1. [5]

    In this study, we investigate the local electronic structure of rare-earth HEOs in the (Ce, Sm, Pr, La, Y)O₂ system using X -ray absorption spectroscopy (XAS)

    Institute for Computational and Data Science, The Pennsylvania State University, University Park, PA 16802, USA *Corresponding author: cmrost@vt.edu Abstract High-entropy oxides (HEOs) are a promising class of multicomponent ceramics with tunable structural and electronic properties. In this study, we investigate the local electronic structure of rare-ear...

  2. [6]

    Chemically-Disordered Transparent Conductive Perovskites with High Crystalline Fidelity

    S. S. I. Almishal et al. , “Transparent Correlated Metallic Perovskites with Conducive Chemical Disorder,” Jan. 15, 2025, arXiv: arXiv:2501.09193. doi: 10.48550/arXiv.2501.09193

  3. [7]

    All calculations assumed initial ferromagnetic spin alignment

    The pseudopotentials Ce, La, Pr, Sm, Y_sv, and O were selected from the PAW 64 dataset, with the f electrons of Ce, Pr, and Sm explicitly treated as valence electrons. All calculations assumed initial ferromagnetic spin alignment. To evaluate atomic charges, Bader charge analysis was performed. The program developed by Henkelman and co -workers [32], [33]...

  4. [8]

    High-entropy oxides: Harnessing crystalline disorder for emergent functionality,

    G. N. Kotsonis et al., “High-entropy oxides: Harnessing crystalline disorder for emergent functionality,” J. Am. Ceram. Soc., vol. 106, no. 10, pp. 5587– 5611, 2023, doi: 10.1111/jace.19252

  5. [9]

    Nanostructured High- Entropy Alloys with Multiple Principal Elements: Novel Alloy Design Concepts and Outcomes,

    J.-W. Yeh et al. , “Nanostructured High- Entropy Alloys with Multiple Principal Elements: Novel Alloy Design Concepts and Outcomes,” Adv. Eng. Mater., vol. 6, no. 5, pp. 299– 303, 2004, doi: 10.1002/adem.200300567. 11

  6. [10]

    Microstructural development in equiatomic multicomponent alloys,

    B. Cantor, I. T. H. Chang, P. Knight, and A. J. B. Vincent, “Microstructural development in equiatomic multicomponent alloys,” Mater. Sci. Eng. A , vol. 375–377, pp. 213–218, Jul. 2004, doi: 10.1016/j.msea.2003.10.257

  7. [11]

    Entropy-stabilized oxides,

    C. M. Rost et al., “Entropy-stabilized oxides,” Nat. Commun., vol. 6, no. 1, p. 8485, Sep. 2015, doi: 10.1038/ncomms9485

  8. [12]

    Colossal dielectric constant in high entropy oxides,

    D. Bérardan, S. Franger, D. Dragoe, A. K. Meena, and N. Dragoe, “Colossal dielectric constant in high entropy oxides,” Phys. Status Solidi RRL – Rapid Res. Lett., vol. 10, no. 4, pp. 328–333, 2016, doi: 10.1002/pssr.201600043

Show all 53 references
  1. [13]

    Multicomponent equiatomic rare earth oxides,

    R. Djenadic et al. , “Multicomponent equiatomic rare earth oxides,” Mater. Res. Lett., vol. 5, no. 2, pp. 102–109, Mar. 2017, doi: 10.1080/21663831.2016.1220433

  2. [14]

    Room temperature lithium superionic conductivity in high entropy oxides,

    D. Bérardan, S. Franger, A. K. Meena, and N. Dragoe, “Room temperature lithium superionic conductivity in high entropy oxides,” J. Mater. Chem. A, vol. 4, no. 24, pp. 9536–9541, Jun. 2016, doi: 10.1039/C6TA03249D

  3. [15]

    Charge-Induced Disorder Controls the Thermal Conductivity of Entropy-Stabilized Oxides,

    J. L. Braun et al. , “Charge-Induced Disorder Controls the Thermal Conductivity of Entropy-Stabilized Oxides,” Adv. Mater., vol. 30, no. 51, p. 1805004, 2018, doi: 10.1002/adma.201805004

  4. [16]

    Oxygen ion conductivity of the ceria - samarium oxide system with fluorite structure,

    H. Yahiro, Y . Eguchi, K. Eguchi, and H. Arai, “Oxygen ion conductivity of the ceria - samarium oxide system with fluorite structure,” J. Appl. Electrochem., vol. 18, no. 4, pp. 527–531, Jul. 1988, doi: 10.1007/BF01022246

  5. [17]

    Doped Ceria as a Solid Oxide Electrolyte,

    H. L. Tuller and A. S. Nowick, “Doped Ceria as a Solid Oxide Electrolyte,” J. Electrochem. Soc., vol. 122, no. 2, p. 255, Feb. 1975, doi: 10.1149/1.2134190

  6. [18]

    Polaronic Resistive Switching in Ceria‐Based Memory Devices,

    L. Sun, X. Hao, Q. Meng, L. Wang, F. Liu, and M. Zhou, “Polaronic Resistive Switching in Ceria‐Based Memory Devices,” Adv. Electron. Mater., vol. 5, no. 10, p. 1900271, Oct. 2019, doi: 10.1002/aelm.201900271

  7. [19]

    Oxygen level: the dominant of resistive switching characteristics in cerium oxide thin films,

    A. Younis, D. Chu, and S. Li, “Oxygen level: the dominant of resistive switching characteristics in cerium oxide thin films,” J. Phys. Appl. Phys., vol. 45, no. 35, p. 355101, Aug. 2012, doi: 10.1088/0022- 3727/45/35/355101

  8. [20]

    Multicomponent equiatomic rare earth oxides,

    R. Djenadic et al. , “Multicomponent equiatomic rare earth oxides,” Mater. Res. Lett., vol. 5, no. 2, pp. 102–109, 2017

  9. [21]

    High- Entropy Oxides: Epitaxial Growth, Kinetic Dependencies, and Linear Optical Properties,

    George Kotsonis, “High- Entropy Oxides: Epitaxial Growth, Kinetic Dependencies, and Linear Optical Properties,” The Pennsylvania State University, 2022

  10. [22]

    Multicomponent equiatomic rare earth oxides with a narrow band gap and associated praseodymium multivalency,

    A. Sarkar et al., “Multicomponent equiatomic rare earth oxides with a narrow band gap and associated praseodymium multivalency,” Dalton Trans., vol. 46, no. 36, pp. 12167– 12176, 2017, doi: 10.1039/C7DT02077E

  11. [24]

    Fluorite -structured high-entropy oxide sputtered thin films from bixbyite target,

    G. N. Kotsonis et al. , “Fluorite -structured high-entropy oxide sputtered thin films from bixbyite target,” Appl. Phys. Lett., vol. 124, no. 17, p. 171901, Apr. 2024, doi: 10.1063/5.0201419

  12. [25]

    Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides,

    R. D. Shannon, “Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides,” Acta Crystallogr. A, vol. 32, no. 5, pp. 751–767, Sep. 1976, doi: 10.1107/S0567739476001551

  13. [26]

    Muller and R

    O. Muller and R. Roy, The major ternary structural families . in Crystal chemistry of non-metallic materials, no. 4. Berlin Heidelberg: Springer, 1974

  14. [27]

    Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set,

    G. Kresse and J. Furthmüller, “Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set,” Comput. Mater. Sci., vol. 6, no. 1, pp. 15– 50, 1996, doi: 10.1016/0927- 0256(96)00008- 0

  15. [28]

    A High Entropy Oxide Designed to Catalyze CO Oxidation Without Precious Metals,

    C. Riley et al. , “A High Entropy Oxide Designed to Catalyze CO Oxidation Without Precious Metals,” ACS Appl. Mater. 12 Interfaces, vol. 13, no. 7, pp. 8120–8128, Feb. 2021, doi: 10.1021/acsami.0c17446

  16. [29]

    On the effect of kinetics on the formation of fluorite/bixbyite -structured Entropy-Stabilized Oxides,

    L. Spiridigliozzi, V . Monfreda, A. Marocco, and G. Dell’Agli, “On the effect of kinetics on the formation of fluorite/bixbyite -structured Entropy-Stabilized Oxides,” Ceram. Int., Apr. 2025, doi: 10.1016/j.ceramint.2025.04.261

  17. [30]

    A kinetic energy cutoff of 700 eV was applied for the plane -wave basis, and electronic self -consistency was achieved with an energy criterion of 10 -6 eV

    was used to treat exchange-correlation effects, as it has demonstrated strong performance for rare- earth oxide systems [31]. A kinetic energy cutoff of 700 eV was applied for the plane -wave basis, and electronic self -consistency was achieved with an energy criterion of 10 -...

  18. [31]

    Antimony substitution leading to structural transformation (Bixbyite→ Fluorite) and altering the optical band gap in Y2O3,

    R. Nagarajan and P. Kumari, “Antimony substitution leading to structural transformation (Bixbyite→ Fluorite) and altering the optical band gap in Y2O3,” J. Alloys Compd., vol. 863, p. 158733, May 2021, doi: 10.1016/j.jallcom.2021.158733

  19. [32]

    Newville et al

    M. Newville et al. , xraypy/XrayDB: 4.5.6. (Jan. 05, 2025). Zenodo. doi: 10.5281/zenodo.14601875

  20. [33]

    ATHENA, ARTEMIS, HEPHAESTUS: data analysis for X-ray absorption spectroscopy using IFEFFIT,

    B. Ravel and M. Newville, “ATHENA, ARTEMIS, HEPHAESTUS: data analysis for X-ray absorption spectroscopy using IFEFFIT,” J. Synchrotron Radiat., vol. 12, no. 4, pp. 537–541, Jul. 2005, doi: 10.1107/S0909049505012719

  21. [34]

    Larch: An Analysis Package for XAFS and Related Spectroscopies,

    M. Newville, “Larch: An Analysis Package for XAFS and Related Spectroscopies,” J. Phys. Conf. Ser., vol. 430, no. 1, p. 012007, Apr. 2013, doi: 10.1088/1742- 6596/430/1/012007

  22. [35]

    Efficient iterative schemes for ab initio total- energy calculations using a plane -wave basis set,

    G. Kresse and J. Furthmüller, “Efficient iterative schemes for ab initio total- energy calculations using a plane -wave basis set,” Phys. Rev. B , vol. 54, no. 16, pp. 11169– 11186, Oct. 1996, doi: 10.1103/PhysRevB.54.11169

  23. [36]

    Projector augmented -wave method,

    P. E. Blochl, “Projector augmented -wave method,” Phys. Rev. B, vol. 50, no. 24, 1994

  24. [37]

    Accurate and Numerically Efficient r2SCAN Meta - Generalized Gradient Approximation,

    J. W. Furness, A. D. Kaplan, J. Ning, J. P. Perdew, and J. Sun, “Accurate and Numerically Efficient r2SCAN Meta - Generalized Gradient Approximation,” J. Phys. Chem. Lett., vol. 11, no. 19, pp. 8208– 8215, Oct. 2020, doi: 10.1021/acs.jpclett.0c02405

  25. [38]

    Performance of exchange-correlation approximations to density functional theory for rare -earth oxides,

    M. K. Caucci et al. , “Performance of exchange-correlation approximations to density functional theory for rare -earth oxides,” Comput. Mater. Sci., vol. 253, p. 113837, May 2025, doi: 10.1016/j.commatsci.2025.113837

  26. [39]

    A fast and robust algorithm for Bader decomposition of charge density,

    G. Henkelman, A. Arnaldsson, and H. Jónsson, “A fast and robust algorithm for Bader decomposition of charge density,” Comput. Mater. Sci., vol. 36, no. 3, pp. 354– 360, Jun. 2006, doi: 10.1016/j.commatsci.2005.04.010

  27. [40]

    Improved grid- based algorithm for Bader charge allocation,

    E. Sanville, S. D. Kenny, R. Smith, and G. Henkelman, “Improved grid- based algorithm for Bader charge allocation,” J. Comput. Chem., vol. 28, no. 5, pp. 899–908, 2007, doi: 10.1002/jcc.20575

  28. [41]

    A grid-based Bader analysis algorithm without lattice bias,

    W. Tang, E. Sanville, and G. Henkelman, “A grid-based Bader analysis algorithm without lattice bias,” J. Phys. Condens. Matter , vol. 21, no. 8, 2009, doi: 10.1088/0953- 8984/21/8/084204

  29. [42]

    Special Quasirandom Structures,

    A. Zunger, S.-H. Wei, L. G. Ferreira, and J. E. Bernard, “Special Quasirandom Structures,” Phys. Rev. Lett., vol. 65, no. 3, pp. 353–356, 1990

  30. [43]

    ICET – A Python Library for Constructing and Sampling Alloy Cluster Expansions,

    M. Ångqvist et al., “ICET – A Python Library for Constructing and Sampling Alloy Cluster Expansions,” Adv. Theory Simul., vol. 2, no. 7, pp. 1–10, 2019, doi: 10.1002/adts.201900015

  31. [44]

    XANES study of Li-MgO and Li -La2O3-MgO catalysts for oxidative coupling of methane,

    H. Aritani, H. Yamada, T. Yamamoto, T. Tanaka, and S. Imamura, “XANES study of Li-MgO and Li -La2O3-MgO catalysts for oxidative coupling of methane,” J. Synchrotron Radiat., vol. 8, no. 2, pp. 593– 595, Mar. 2001, doi: 10.1107/S0909049500014448

  32. [45]

    Crystal field analysis of the 8- coordinated cubic environment in optical materials,

    F. Wen, “Crystal field analysis of the 8- coordinated cubic environment in optical materials,” Results Opt. , vol. 3, p. 100056, May 2021, doi: 10.1016/j.rio.2021.100056

  33. [46]

    Spectral-line-broadening study of the trivalent lanthanide -ion series.II. The variation of the electron- phonon coupling strength through the series,

    A. Ellens, H. Andres, M. L. H. ter Heerdt, R. T. Wegh, A. Meijerink, and G. Blasse, 13 “Spectral-line-broadening study of the trivalent lanthanide -ion series.II. The variation of the electron- phonon coupling strength through the series,” Phys. Rev. B, vol. 55, no. 1, pp. 180...

  34. [47]

    The Lanthanide Contraction Revisited,

    M. Seitz, A. G. Oliver, and K. N. Raymond, “The Lanthanide Contraction Revisited,” J. Am. Chem. Soc., vol. 129, no. 36, pp. 11153– 11160, Sep. 2007, doi: 10.1021/ja072750f

  35. [48]

    Local Structure of Pr, Nd, and Sm Complex Oxides and Their X- ray Absorption Near Edge Structure Spectra,

    H. Asakura, T. Shishido, S. Fuchi, K. Teramura, and T. Tanaka, “Local Structure of Pr, Nd, and Sm Complex Oxides and Their X- ray Absorption Near Edge Structure Spectra,” J. Phys. Chem. C, vol. 118, no. 36, pp. 20881– 20888, Sep. 2014, doi: 10.1021/jp504507c

  36. [49]

    Local Structure and La L1 and L3- Edge XANES Spectra of Lanthanum Complex Oxides,

    H. Asakura, T. Shishido, K. Teramura, and T. Tanaka, “Local Structure and La L1 and L3- Edge XANES Spectra of Lanthanum Complex Oxides,” Inorg. Chem., vol. 53, no. 12, pp. 6048–6053, Jun. 2014, doi: 10.1021/ic500381z

  37. [50]

    Concentration of Ce3+ and Oxygen Vacancies in Cerium Oxide Nanoparticles,

    P. Dutta, S. Pal, M. S. Seehra, Y . Shi, E. M. Eyring, and R. D. Ernst, “Concentration of Ce3+ and Oxygen Vacancies in Cerium Oxide Nanoparticles,” Chem. Mater., vol. 18, no. 21, pp. 5144–5146, Oct. 2006, doi: 10.1021/cm061580n

  38. [51]

    Room-temperature ferromagnetism in pure CeO2 nanoparticles prepared by a simple direct thermal decomposition,

    S. Phokha, E. Swatsitang, and S. Maensiri, “Room-temperature ferromagnetism in pure CeO2 nanoparticles prepared by a simple direct thermal decomposition,” Electron. Mater. Lett., vol. 11, no. 6, pp. 1012–1020, Nov. 2015, doi: 10.1007/s13391-015-4164-4

  39. [52]

    Simultaneous valence shift of Pr and Tb ions at the spin- state transition in (Pr${}_{1\ ensuremath{- }y}$Tb${}_{y}{)}_{0.7}$Ca${}_{0.3}$Co O${}_{3}$,

    H. Fujishiro et al. , “Simultaneous valence shift of Pr and Tb ions at the spin- state transition in (Pr${}_{1\ ensuremath{- }y}$Tb${}_{y}{)}_{0.7}$Ca${}_{0.3}$Co O${}_{3}$,” Phys. Rev. B, vol. 87, no. 15, p. 155153, Apr. 2013, doi: 10.1103/PhysRevB.87.155153

  40. [53]

    An improved laboratory- based x -ray absorption fine structure and x- ray emission spectrometer for analytical applications in materials chemistry research,

    E. P. Jahrman et al., “An improved laboratory- based x -ray absorption fine structure and x- ray emission spectrometer for analytical applications in materials chemistry research,” Rev. Sci. Instrum., vol. 90, no. 2, p. 024106, Feb. 2019, doi: 10.1063/1.5049383. Supplementary ...

  41. [54]

    Department of Materials Science and Engineering, Virginia Polytechnic Institute and State University, Blacksburg, V A 24060, USA

  42. [55]

    Department of Chemistry, The Pennsylvania State University, University Park, PA 16802, USA

  43. [56]

    Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA 16802, USA

  44. [57]

    Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USA

  45. [58]

    The standards that required a mixture of powders were milled in a Spex 8000M ball mill and quenched from the tabulated temperature

    Institute for Computational and Data Science, The Pennsylvania State University, University Park, PA 16802, USA *Corresponding author: cmrost@vt.edu Table S1: Details of the standards used in this work. The standards that required a mixture of powders were milled in a Spex 800...

Pith tools

Reviewed August 15, 2026 · model on record in the stance chip above.