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arxiv: 2603.14642 · v4 · pith:4UHB3HI5new · submitted 2026-03-15 · ❄️ cond-mat.mtrl-sci

Role of Oxygen Vacancies in Stabilizing the Orthorhombic Phases of Hf0.5Zr0.5O2 Nanoparticles

Pith reviewed 2026-05-21 11:19 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords oxygen vacanciesHf0.5Zr0.5O2 nanoparticlesorthorhombic phaseferroelectric orderingchemical strainLandau-Ginzburg-Devonshire theoryphase stabilizationdielectric response
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The pith

Oxygen vacancies stabilize the ferroelectric orthorhombic phase in small Hf0.5Zr0.5O2 nanoparticles via chemical strain.

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

The paper establishes that the concentration of oxygen vacancies, tuned by annealing under different oxygen partial pressures, directly controls the fraction of orthorhombic phases in approximately 7 nm Hf0.5Zr0.5O2 nanoparticles. Experiments using EPR, XPS, XRD and NMR link higher vacancy levels to more orthorhombic content, while Landau-Ginzburg-Devonshire calculations show that the resulting chemical strain, together with trilinear coupling of nonpolar, antipolar and polar phonon modes, stabilizes the o-III phase that carries long-range ferroelectric order. A sympathetic reader would care because the mechanism enables ferroelectric-like behavior and enhanced dielectric response in isolated nanoparticles dispersed in a polymer matrix, without requiring epitaxial substrates or large grain sizes. The work also ties the vacancy-induced elastic dipoles and ionic conductivity to reduced depolarization fields and possible negative capacitance states at interfaces.

Core claim

Phenomenological calculations based on Landau-Ginzburg-Devonshire theory considering trilinear coupling between nonpolar, antipolar and polar phonon modes indicate that chemical strain induced by oxygen vacancies can stabilize the orthorhombic phase o-III with the ferroelectric long-range ordering in small Hf0.5Zr0.5O2 nanoparticles. The theory confirms the stability of ferroelectric polarization in the vacancy-enriched Hf0.5Zr0.5O2 nanoparticles.

What carries the argument

Landau-Ginzburg-Devonshire theory with trilinear coupling between nonpolar, antipolar and polar phonon modes, which incorporates chemical strain from oxygen vacancies to determine phase stability.

If this is right

  • The fraction of orthorhombic phases rises with oxygen vacancy concentration as measured by EPR, XPS, XRD and NMR.
  • Dielectric permittivity maximum intensifies near 350-380 K in PVDF composites containing vacancy-enriched nanoparticles.
  • Defect-induced elastic dipoles and higher ionic conductivity reduce the depolarization field and support ferroelectric-like ordering.
  • Interfacial effects in weakly screened, spatially isolated nanoparticles embedded in PVDF may produce negative capacitance states.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Controlling oxygen partial pressure during annealing offers a general route to induce ferroelectric order in other oxide nanoparticles without substrate strain.
  • The same vacancy-driven elastic and screening effects could be tested in pure HfO2 or ZrO2 particles to broaden the materials scope.
  • Combining vacancy engineering with external electric fields or additional dopants might further tune the trilinear coupling strength.
  • The approach may enable flexible, polymer-hosted ferroelectric devices where traditional epitaxial stabilization is impractical.

Load-bearing premise

Chemical strain from oxygen vacancies is the dominant mechanism that stabilizes the o-III orthorhombic phase and overcomes size and interface effects in these 7 nm particles.

What would settle it

If controlled annealing experiments produce no measurable increase in orthorhombic phase fraction when oxygen vacancy concentration is raised, or if the LGD model without chemical strain predicts equivalent o-III stability, the central claim would be refuted.

Figures

Figures reproduced from arXiv: 2603.14642 by Anna N. Morozovska, Anna O. Diachenko, Dean R. Evans, Eugene A. Eliseev, Jana Houdkova, Lesya D. Demchenko, Lesya P. Yurchenko, Michail D. Volnyanskii, Mikhail P. Trubitsyn, Myroslav V. Karpets, Oksana V. Leshchenko, Oleksandr S. Pylypchuk, Petr Jiricek, Valentin V. Laguta, Victor N. Pavlikov, Yuriy O. Zagorodniy.

Figure 1
Figure 1. Figure 1: TEM images of Hf0.5Zr0.5O2 nanoparticles annealed in an air atmosphere, sample N1 (a, b) and in CO + CO₂ atmosphere, sample N2 (c, d). X-ray diffraction (XRD) measurements of the samples are presented in Fig. S3 (see Supplementary Materials). Despite the high crystallinity of the nanoparticles, their XRD spectra exhibit broad diffraction lines arising from significant surface effects, thereby complicating … view at source ↗
Figure 6
Figure 6. Figure 6: (a) Experimental 91Zr NMR spectrum of Hf0.5Zr0.5O2 nanoparticles annealed in a CO+CO2 atmosphere along with the best fit, where the dashed curve presenting a Gaussian component; (b) the line shape corresponding [PITH_FULL_IMAGE:figures/full_fig_p016_6.png] view at source ↗
read the original abstract

In this work we study the stabilization of the orthorhombic phases in small Hf0.5Zr0.5O2 nanoparticles (average size ~ 7 nm) annealed under different oxygen partial pressures. Concentration of the oxygen vacancies, which is determined by annealing conditions, was estimated from the electron paramagnetic resonance spectra and X-ray photoelectron spectroscopy. The fraction of the orthorhombic phases, that is determined by the X-ray diffraction and nuclear magnetic resonance, depends on the concentration of oxygen vacancies. Phenomenological calculations based on Landau-Ginzburg-Devonshire theory considering trilinear coupling between nonpolar, antipolar and polar phonon modes, indicate that chemical strain induced by oxygen vacancies can stabilize the orthorhombic phase o-III with the ferroelectric long-range ordering in small Hf0.5Zr0.5O2 nanoparticles. The theory confirms the stability of ferroelectric polarization in the vacancy-enriched Hf0.5Zr0.5O2 nanoparticles. The increase in the intensity of the dielectric permittivity maximum, observed near 350 - 380 K in the PVDF matrix with the Hf0.5Zr0.5O2 nanoparticles annealed in the CO+CO2 atmosphere, is clearly associated with the increase in oxygen vacancies concentration. The vacancies lead to the defect-induced elastic dipole formation and to the increase in ionic conductivity, which decreases the depolarization field and may induce the ferroelectric-like phase transition in the vacancy-enriched Hf0.5Zr0.5O2 nanoparticles. Due to the interfacial effects the negative capacitance states may be realized in weakly screened and spatially isolated Hf0.5Zr0.5O2 nanoparticles embedded in the PVDF matrix.The present approach based on oxygen-vacancy-induced elastic and screening effects may provide a route for engineering ferroelectric-like states in other nanoscale ferroic oxides.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The paper examines stabilization of orthorhombic phases (particularly ferroelectric o-III) in ~7 nm Hf0.5Zr0.5O2 nanoparticles by controlling oxygen vacancy concentration through annealing under varying oxygen partial pressures. Vacancy levels are quantified via EPR and XPS, while orthorhombic phase fractions are assessed by XRD and NMR, showing a correlation with vacancy density. Phenomenological LGD theory incorporating trilinear coupling between nonpolar, antipolar, and polar modes is invoked to argue that chemical strain from vacancies stabilizes the o-III phase with long-range ferroelectric order; dielectric measurements in a PVDF matrix link increased permittivity maxima near 350-380 K to vacancy-induced elastic dipoles and reduced depolarization fields, with implications for negative capacitance.

Significance. If the central stabilization mechanism holds with quantitative validation, the work would be significant for defect engineering of ferroelectricity in nanoscale fluorite oxides, offering a route to ferroelectric-like states in particles too small for conventional size-effect suppression. The experimental linkage of vacancy concentration to phase fraction via multiple spectroscopies provides a solid empirical foundation, while the LGD approach with trilinear terms could generalize to other nanoscale ferroics if the parameters and size corrections are made explicit.

major comments (3)
  1. [Theory / LGD calculations] Theory section (phenomenological LGD calculations): The central claim that chemical strain ε_chem(v) from measured oxygen-vacancy concentrations stabilizes the o-III phase with ferroelectric ordering requires explicit values for the Landau coefficients and the functional mapping from vacancy density (EPR/XPS) to strain; without these, it cannot be verified whether the trilinear coupling produces a sufficient negative shift in the polar-mode quadratic term to overcome depolarization and surface penalties in 7 nm particles.
  2. [Theory / Finite-size effects] Finite-size modeling: The LGD expansion lacks explicit size-dependent electrostatic (depolarization field ~1/R) and surface-energy terms for R ≈ 7 nm, which are load-bearing for the long-range ferroelectric ordering conclusion; their omission leaves the quantitative sufficiency of vacancy-induced stabilization untested against standard nanoparticle penalties.
  3. [Dielectric measurements] Dielectric interpretation (§ on permittivity measurements): The post-hoc attribution of the 350-380 K permittivity maximum to a vacancy-driven ferroelectric-like transition would be strengthened by direct evidence such as temperature-dependent structural data or P-E hysteresis; the current link to reduced depolarization via ionic conductivity remains interpretive.
minor comments (2)
  1. [Abstract and introduction] The abstract and main text use 'o-III' without a brief definition or reference to standard HfO2 orthorhombic phase labeling (e.g., Pca21 or Pmn21), which would aid readers unfamiliar with the nomenclature.
  2. [Figures and captions] Figure captions for XRD/NMR data should explicitly state the quantitative phase fractions extracted for each annealing condition to allow direct comparison with the vacancy concentrations reported in the text.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which help clarify the presentation of our theoretical modeling and experimental interpretations. We respond point by point to the major comments and indicate planned revisions.

read point-by-point responses
  1. Referee: [Theory / LGD calculations] Theory section (phenomenological LGD calculations): The central claim that chemical strain ε_chem(v) from measured oxygen-vacancy concentrations stabilizes the o-III phase with ferroelectric ordering requires explicit values for the Landau coefficients and the functional mapping from vacancy density (EPR/XPS) to strain; without these, it cannot be verified whether the trilinear coupling produces a sufficient negative shift in the polar-mode quadratic term to overcome depolarization and surface penalties in 7 nm particles.

    Authors: We agree that explicit values improve verifiability. In the revised manuscript we will list the Landau coefficients (taken from established HfO2/ZrO2 literature), specify the linear mapping ε_chem(v) = α·v calibrated to our EPR/XPS vacancy densities and XRD lattice expansion, and show the resulting negative shift in the polar-mode quadratic term together with a direct numerical comparison to the depolarization and surface penalties estimated for 7 nm particles. revision: yes

  2. Referee: [Theory / Finite-size effects] Finite-size modeling: The LGD expansion lacks explicit size-dependent electrostatic (depolarization field ~1/R) and surface-energy terms for R ≈ 7 nm, which are load-bearing for the long-range ferroelectric ordering conclusion; their omission leaves the quantitative sufficiency of vacancy-induced stabilization untested against standard nanoparticle penalties.

    Authors: We accept that explicit size-dependent terms are needed for quantitative rigor. The revised theory section will add the depolarization-field term (scaled as 1/R with a dielectric-environment prefactor) and a surface-energy penalty (proportional to surface-to-volume ratio for R ≈ 7 nm). Updated stability diagrams will demonstrate that the vacancy-induced chemical strain still overcomes these penalties to stabilize long-range ferroelectric order in the o-III phase. revision: yes

  3. Referee: [Dielectric measurements] Dielectric interpretation (§ on permittivity measurements): The post-hoc attribution of the 350-380 K permittivity maximum to a vacancy-driven ferroelectric-like transition would be strengthened by direct evidence such as temperature-dependent structural data or P-E hysteresis; the current link to reduced depolarization via ionic conductivity remains interpretive.

    Authors: We agree that direct structural or hysteresis data would strengthen the claim. However, temperature-dependent XRD on the low-volume-fraction nanoparticles inside the PVDF matrix is hindered by matrix scattering, and reliable P-E loops are precluded by leakage and electrode geometry in the composite. We will therefore expand the discussion with quantitative estimates of ionic-conductivity screening, additional conductivity measurements, and explicit caveats on the interpretive nature of the ferroelectric-like assignment while preserving the observed correlation with vacancy concentration. revision: partial

Circularity Check

0 steps flagged

LGD phenomenological model remains independent of the nanoparticle data

full rationale

The paper reports experimental measurements of oxygen-vacancy concentration (EPR/XPS), orthorhombic phase fractions (XRD/NMR), and dielectric response, then separately states that LGD calculations with trilinear coupling indicate chemical-strain stabilization of the o-III phase. No quoted equation or section shows that the Landau coefficients, the vacancy-to-strain mapping, or the trilinear terms are fitted to the same 7 nm particle data set; the theory is presented as a consistency check rather than a self-referential derivation. The derivation chain therefore does not reduce to its inputs by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim depends on the validity of the LGD phenomenological expansion and the interpretation that measured vacancy levels produce sufficient chemical strain; no independent first-principles derivation or machine-checked proof is referenced.

free parameters (1)
  • LGD Landau coefficients and trilinear coupling strength
    Phenomenological theory requires these coefficients to be chosen or fitted to reproduce the observed phase stability and polarization.
axioms (1)
  • domain assumption Trilinear coupling between nonpolar, antipolar and polar phonon modes is the dominant interaction that, together with vacancy-induced chemical strain, stabilizes the o-III phase.
    Invoked directly in the description of the phenomenological calculations.

pith-pipeline@v0.9.0 · 5979 in / 1454 out tokens · 68752 ms · 2026-05-21T11:19:01.405500+00:00 · methodology

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Works this paper leans on

87 extracted references · 87 canonical work pages · 1 internal anchor

  1. [1]

    Müller, T

    J. Müller, T. S. Boscke, U . Schroder, S. Mueller, D. Brauhaus, U. Bottger, L. Frey, and T. Mikolajic, Ferroelectricity in Simple Binary ZrO2 and HfO2. Nano Lett. 12, 4318, (2012); https://doi.org/10.1021/nl302049k

  2. [2]

    T. S. Boscke, J. Muller, D. Brauhaus, U. Schroder, and U. Bottger, Ferroelectricity in hafnium oxide thin films, Appl. Phys. Lett. 99, 102903 (2011); https://doi.org/10.1063/1.3634052

  3. [3]

    Muller, T

    J. Muller, T. S. Boscke, D. Brauhaus, U. Schroder, U. Bottger, J. Sundqvist, P. Kucher, T. Mikolajick, and L. Frey, Ferroelectric Zr0.5Hf0.5O2 thin films for nonvolatile memory applications, Appl. Phys. Lett. 99, 112901 (2011); https://doi.org/10.1063/1.3636417 34

  4. [4]

    J. P. B. Silva et al. Roadmap on ferroelectric hafnia and zirconia-based materials and devices, APL Mater. 11, 089201 (2023); https://doi.org/10.1063/5.0148068

  5. [5]

    K.-H. Kim, I. Karpov, R. H. Olsson III, D. Jariwala. Wurtzite and fluorite ferroelectric materials for electronic memory, Nature Nanotechnology 18, 422 (2023); https://doi.org/10.1038/s41565-023-01361-y

  6. [6]

    A. Paul, G. Kumar, A. Das, G. Larrieu, and S. De. Hafnium oxide-based ferroelectric field effect transistors: From materials and reliability to applications in storage-class memory and in-memory computing. J. Appl. Phys. 138, 010701 (2025); https://doi.org/10.1063/5.0278057

  7. [7]

    Afroze, H

    N. Afroze, H. Fahrvandi, G. Ren, P. Kumar, C. Nelson, S. Lombardo, M. Tian, et al. Atomic-scale confinement of strongly charged 180° domain wall pairs in ZrO2. arXiv.2507.18920 (2025); https://doi.org/10.48550/arXiv.2507.18920

  8. [8]

    Mukherjee, N

    B. Mukherjee, N. S. Fedorova, J. Íñiguez-González. Extrinsic nature of the polarization in hafnia ferroelectrics, arXiv.2508.00372 (2025); https://doi.org/10.48550/arXiv.2508.00372

  9. [9]

    Hafnia and hafnia-toughened ceramics,

    J. Wang, H. P. Li, and R. Stevens, “Hafnia and hafnia-toughened ceramics,” J. Mater. Sci. 27 (20), 5397 (1992); https://doi.org/10.1007/BF00541601

  10. [10]

    Monoclinic to tetragonal transformations in hafnia and zirconia: A combined calorimetric and density functional study,

    X. Luo, W. Zhou, S. Ushakov, A. Navrotsky, and A. Demkov, “Monoclinic to tetragonal transformations in hafnia and zirconia: A combined calorimetric and density functional study,” Phys. Rev. B 80 (13), 134119 (2009); https://doi.org/10.1103/PhysRevB.80.134119

  11. [11]

    Phase diagram up to 105 GPa and mechanical strength of HfO2,

    Y. Al-Khatatbeh, K. K. M. Lee, and B. Kiefer, “Phase diagram up to 105 GPa and mechanical strength of HfO2,” Phys. Rev. B 82(14), 144106 (2010), https://doi.org/10.1103/PhysRevB.82.144106

  12. [12]

    Ohtaka, H

    O. Ohtaka, H. Fukui, T. Kunisada, T. Fujisawa, K. Funakoshi, W. Utsumi, T. Irifune, K. Kuroda, and T. Kikegawa. Phase relations and equations of state of ZrO2 under high temperature and high pressure, Phys. Rev. B 63, 174108 (2001); https://doi.org/10.1103/PhysRevB.63.174108

  13. [13]

    Estandìa, N

    S. Estandìa, N. Dix, J. Gazquez, I. Fina, J. Lyu, M. F. Chisholm, J. Fontcuberta, and F. Sánchez, Engineering ferroelectric Hf0.5Zr0.5O2 thin films by epitaxial stress, ACS Appl. Electron. Mater. 1, 1449 (2019); https://doi.org/10.1021/acsaelm.9b00256

  14. [14]

    Estandìa, N

    S. Estandìa, N. Dix, M. F. Chisholm, I. Fina, and F. Sánchez, Domain-matching epitaxy of ferroelectric Hf0.5Zr0.5O2(111) on La2/3Sr1/3MnO3(001), Cryst. Growth Des. 20, 3801 (2020); https://dx.doi.org/10.1021/acs.cgd.0c00095

  15. [16]

    Richter, T

    C. Richter, T. Schenk, M. H. Park et al, Si Doped Hafnium Oxide —A “Fragile” Ferroelectric System, Adv. Electron. Mater. 3, 1700131 (2017), https://doi.org/10.1002/aelm.201700131

  16. [17]

    Shimizu, T., Katayama, K., Kiguchi, T. et al. The demonstration of significant ferroelectricity in epitaxial Y-doped HfO2 film. Sci Rep 6, 32931 (2016); https://doi.org/10.1038/srep32931

  17. [18]

    Mueller, J

    S. Mueller, J. Mueller, A . Singh, S . Riedel, J . Sundqvist, U . Schroeder, T . Mikolajick. Incipient ferroelectricity in Al‐doped HfO 2 thin films. Advanced Functional Materials. 22, 2412 -2417 (2012); https://doi.org/10.1002/adfm.201103119

  18. [19]

    Pešic´, F

    M. Pešic´, F. P. G. Fengler, T. Schenk et. al. Physical Mechanisms behind the Field-Cycling Behavior of 35 HfO2-Based Ferroelectric Capacitors , Adv. Func. Mater. 26, 4601 (2016). https://doi.org/10.1002/adfm.201600590

  19. [20]

    M. H. Park, Y. H. Lee, H. J. Kim, T. Schenk, W. Lee, K. Do Kim, F. P. G. Fengler, T. Mikolajick, U. Schroeder, and C. S. Hwang. Surface and grain boundary energy as the key enabler of ferroelectricity in nanoscale hafnia-zirconia: a comparison of model and experiment. Nanoscale 9, 9973 (2017); https://doi.org/10.1039/C7NR02121F

  20. [21]

    A. N. Morozovska, E. A. Eliseev, S. V. Kalinin, and M. V. Strikha. Sizes of Ferroelectricity Appearance and Disappearance in Nanosized Hafnia-Zirconia: Landau-type Theory (2026); https://doi.org/10.48550/arXiv.2601.06267

  21. [22]

    S. Lim, Y . Ahn, B . Won, S . Lee, H . Park, M . Kumar, H. Seo, Effects of Substrate and Annealing Conditions on the Ferroelectric Properties of Non-Doped HfO2 Deposited by RF Plasma Sputter. Nanomaterials, 14, 1386 (2024); https://doi.org/10.3390/nano14171386

  22. [23]

    Hoffmann, U

    M. Hoffmann, U. Schroeder, T. Schen et al., Stabilizing the ferroelectric phase in doped hafnium oxide, J. Appl. Phys. 118, 072006 (2015); https://doi.org/10.1063/1.4927805

  23. [24]

    M. D. Glinchuk, A.N. Morozovska, A. Lukowiak, W. Stręk, M. V. Silibin, D. V. Karpinsky, Y. Kim, S. V. Kalinin, Possible Electrochemical Origin of Ferroelectricity in HfO 2 Thin Films, Journal of Alloys and Compounds. 830, 153628 (2020), https://doi.org/10.1016/j.jallcom.2019.153628

  24. [25]

    E. A. Eliseev, Y. O. Zagorodniy, V. N. Pavlikov, O. V. Leshchenko, H. V. Shevilakova, M. V. Karpec, A. D. Yaremkevych, O. M. Fesenko, S. V. Kalinin, and A. N. Morozovska. Phase diagrams and polarization reversal in nanosized HfxZr1-xO2-y, AIP Advances, 14, 055224 (2024); https://doi.org/10.1063/5.0209123

  25. [26]

    E. A. Eliseev, I. V. Kondakova, Y. O. Zagorodniy, H. V. Shevliakova, O. V. Leshchenko, V. N. Pavlikov, M. V. Karpets, L. P. Yurchenko, and A. N. Morozovska, The origin of the ferroelectric-like orthorhombic phase in oxygen-deficient HfO2-y nanoparticles. Semiconductor Physics, Optoelectronics and Quantum Electronics, 28, 134 (2025); https://doi.org/10.154...

  26. [27]

    O. S. Pylypchuk, V. V. Vainberg, V. N. Poroshin, O. V. Leshchenko, V. N. Pavlikov, I. V. Kondakova, S. E. Ivanchenko, L. P. Yurchenko, L. Demchenko, A. O. Diachenko, M. V. Karpets, M. P. Trubitsyn, E. A. Eliseev, and A. N. Morozovska. A colossal dielectric response of HfxZr1-xO2 nanoparticles. Physical Review Materials 9, 114412 (2025); https://doi.org/10...

  27. [28]

    O. S. Pylypchuk, I. V. Fesych, V. V. Vainberg, Y. O. Zagorodniy, V. I. Styopkin, J. M. Gudenko, I. V. Kondakova, L. P. Yurchenko, V. N. Pavlikov, A. O. Diachenko, M. M. Koptiev, M. D. Volnyanskii, V. V. Laguta, E. A. Eliseev, M. P. Trubitsyn, and A. N. Morozovska. Resistive switching and charge accumulation in Hf0.5Zr0.5O2 nanoparticles. Journal of Physic...

  28. [29]

    Ernst, G

    R.R. Ernst, G. Bodenhausen, A. Wokaun, Principles of Nuclear Magnetic Resonance in One and Two Dimensions, Oxford university press, New York, 1990

  29. [30]

    Srivastava, M

    D.J. Srivastava, M. Giammar, M.C. Venetos, L. McCarthy-Carney, and P.J. Grandinetti MRSimulator: A cross-platform, object-oriented software package for rapid solid -state NMR spectral simulation and analysis. J. Chem. Phys. 161, 212501 (2024); https://doi.org/10.1063/5.0237608 36

  30. [31]

    Stoll, A

    S. Stoll, A. Schweiger, EasySpin, a comprehensive software package for spectral simulation and analysis in EPR. J. Magn. Reson. 178 (1), 42 (2006); https://doi.org/10.1016/j.jmr.2005.08.013

  31. [32]

    Fujimoto, Y

    K. Fujimoto, Y. Sato, Y. Fuchikami, R. Teranishi, K. Kaneko, Orthorhombic-like atomic arrangement in hafnium-oxide-based nanoparticle, J Am Ceram Soc. 105, 2823 (2022), https://doi.org/10.1111/jace.18242

  32. [33]

    Materlik, C

    R. Materlik, C. Künneth, and A. Kersch, The origin of ferroelectricity in Hf1−xZrxO2 A computational investigation and a surface energy model, Journal of Applied Physics 117, 134109 (2015); https://doi.org/10.1063/1.4916707

  33. [34]

    Mirenghi, A

    L. Mirenghi, A. Rizzo, An Accurate Quantitative X -ray Photoelectron Spectroscopy Study of Pure and Homogeneous ZrN Thin Films Deposited Using BPDMS . Appl. Sci. 13, 1271 (2023); https://doi.org/10.3390/app13031271

  34. [35]

    Greczynski, D

    G. Greczynski, D. Primetzhofer, J. Lu, L. Hultman, Core-level spectra and binding energies of transition metal nitrides by non -destructive x -ray photoelectron spectroscopy through capping layers, Applied Surface Science, 396, 347 (2017); https://doi.org/10.1016/j.apsusc.2016.10.152

  35. [36]

    Sarma, C.N.R

    D.D. Sarma, C.N.R. Rao. XPES studies of oxides of second -and third-row transition metals including rare earths. J. Electron Spectrosc. Relat. Phenom. 20, 25 (1980); https://doi.org/10.1016/0368-2048(80)85003-1

  36. [37]

    Clinical correlations of photoparoxysmal responses,

    S. Ardizzone, M.G. Cattania, P. Lugo. Interfacial electrostatic behaviour of oxides: correlations with structural and surface parameters of the phase. Electrochim. Acta 39, 1509 (1994); https://doi.org/10.1016/0013- 4686(94)85128-X

  37. [38]

    R Shah, B

    L. R Shah, B. Ali, H. Zhu, W. G. Wang, Y. Q. Song, H. W. Zhang, S. I. Shah, and J. Q. Xiao. Detailed study on the role of oxygen vacancies in structural, magnetic and transport behavior of magnetic insulator: Co– CeO2. J. Phys.: Condens. Matter 21, 486004 (2009); http://doi.org/10.1088/0953-8984/21/48/486004

  38. [39]

    Grover, R

    V. Grover, R. Shukla, R. Kumari, B. P. Mandal, P. K. Kulriya, S. K. Srivastava, S. Ghosh, A. K. Tyagi, and D. K. Avasthi. Effect of grain size and microstructure on radiation stability of CeO 2: an extensive study. Phys.Chem. Chem. Phys., 16, 27065 (2014); http://doi.org/0.1039/c4cp04215h

  39. [40]

    K. Wang, Y. Chang, L. Lv, Y. Long, Effect of annealing temperature on oxygen vacancy concentrations of nanocrystalline CeO2 film. Applied Surface Science 351, 164 (2015); http://doi.org/10.1016/j.apsusc.2015.05.122

  40. [41]

    Mehmood et al, Surface, Subsurface, and Bulk Oxygen Vacancies Quantified by Decoupling and Deconvolution of the Defect Structure of Redox -Active Nanoceria, Inorganic Chemistry

    R. Mehmood et al, Surface, Subsurface, and Bulk Oxygen Vacancies Quantified by Decoupling and Deconvolution of the Defect Structure of Redox -Active Nanoceria, Inorganic Chemistry. 58 (9), 6016 (2019); https://doi.org/10.1021/acs.inorgchem.9b00330

  41. [42]

    Huang, T.-L

    C.-Y. Huang, T.-L. Tsai, C.-A. Lin, and T.-Y. Tseng. Switching mechanism of double forming process phenomenon in ZrOx/HfOy bilayer resistive switching memory structure with large endurance. Applied Physics Letters 104, 062901 (2014); http://doi.org/10.1063/1.4864396

  42. [43]

    Liu, H., Zheng, S., Chen, Q. et al. Structural and ferroelectric properties of Pr doped HfO 2 thin films fabricated by chemical solution method. J Mater Sci: Mater Electron 30, 5771 (2019). https://doi.org/10.1007/s10854-019-00874-4

  43. [44]

    H. Idriss, On the wrong assignment of the XPS O1s signal at 531–532 eV attributed to oxygen vacancies in photo- and electro-catalysts for water splitting and other materials applications, Surface Science 712, 121894 37 (2021); https://doi.org/10.1016/j.susc.2021.121894

  44. [45]

    Posada-Borbon et al,, On the signatures of oxygen vacancies in O1s core level shifts, Surface Science, 705, 121761 (2021); https://doi.org/10.1016/j.susc.2020.121761

    A. Posada-Borbon et al,, On the signatures of oxygen vacancies in O1s core level shifts, Surface Science, 705, 121761 (2021); https://doi.org/10.1016/j.susc.2020.121761

  45. [46]

    K. Ye, K. Li, Y. Lu et al, An overview of advanced methods for the characterization of oxygen vacancies in materials, TrAC Trends in Analytical Chemistry, 116, 102 (2019); https://doi.org/10.1016/j.trac.2019.05.002

  46. [47]

    Q. Zhao, X. Wang, T. Cai, The study of surface properties of ZrO2, Applied Surface Science, 225, Issues 1–4, 7 (2004); https://doi.org/10.1016/S0169-4332(03)00832-8

  47. [48]

    Kliava, EPR of impurity ions in disordered solids

    J. Kliava, EPR of impurity ions in disordered solids. Distributions of the spin Hamiltonian parameters. Phys. Stat. Sol. (b) 134, 411 (1986); https://doi.org/10.1002/pssb.2221340202

  48. [49]

    Wright, R.C

    S. Wright, R.C. Barklie, EPR characterization of defects in monoclinic powders of ZrO2 and HfO2, Materials Science in Semiconductor Processing, 9 (6), 892 (2006); https://doi.org/10.1016/j.mssp.2006.10.006

  49. [50]

    V. V. Laguta, C. Elissalde, M. Maglione, A. M. Artemenko, V. Chlan, H. Štěpánková, Yu. Zagorodniy,. Crystal structure transformations induced by surface stresses in BaTiO3 and BaTiO3@SiO2 nanoparticles and ceramics. Phase Transitions, 88 (8), 761 (2015); https://doi.org/10.1080/01411594.2014.996852

  50. [51]

    Bastow, M.E

    T.J. Bastow, M.E. Smith, 91Zr NMR characterisation of phases in transformation toughened zirconia, Solid State Nucl. Magn. Reson. 1 (4), 165 (1992); https://doi.org/10.1016/S0926-2040(10)80001-3

  51. [52]

    Abragam, Principles of NuclearMagnetism (Oxford University Press, New York, 1961)

    A. Abragam, Principles of NuclearMagnetism (Oxford University Press, New York, 1961)

  52. [53]

    J. F. Baugher, P. C. Taylor, T. Oja, P. J. Bray, Nuclear magnetic resonance powder patterns in the presence of completely asymmetric quadrupole and chemical shift effects: application to matavanadates. J. Chem. Phys., 50, 4914 (1969); https://doi.org/10.1063/1.1670988

  53. [54]

    Bastow, M.E

    T.J. Bastow, M.E. Smith, S.N. Stuart, Observation of 91Zr NMR in zirconium-based metals and oxides, Chemical Physics Letters, 191, Issues 1–2, 125 (1992); https://doi.org/10.1016/0009-2614(92)85380-S

  54. [55]

    Thermal conductivity of superconducting MgB 2

    F. Vasconcelos et al, Extended Czjzek model applied to NMR parameter distributions in sodium metaphosphate glass, J. Phys.: Condens. Matter. 25, 255402 (2013); https://doi.org/10.1088/0953- 8984/25/25/255402

  55. [56]

    G. Le Caër et al, An extension of the Czjzek model for the distributions of electric field gradients in disordered solids and an application to NMR spectra of 71Ga in chalcogenide glasses, J. Phys.: Condens. Matter, 22, 065402 (2010), https://doi.org/10.1088/0953-8984/22/6/065402

  56. [57]

    T. Zhu, L. Ma, S. Deng & S. Liu, Computational materials, Progress in computational understanding of ferroelectric mechanisms in HfO2, npj Comput Mater 10, 188 (2024); https://doi.org/10.1038/s41524-024- 01352-0

  57. [58]

    Dutta, P

    S. Dutta, P. Buragohain, S. Glinsek, C. Richter, H. Aramberri, H. Lu, U. Schroeder, E. Defay, A. Gruverman, J. Íñiguez. Piezoelectricity in hafnia. Nature Communications 12, 7301 (2021); https://doi.org/10.1038/s41467-021-27480-5

  58. [59]

    S. Zhou, J. Zhang, A. M. Rappe, Strain-induced antipolar phase in hafnia stabilizes robust thin-film ferroelectricity. Science Advances 8 (47), eadd5953 (2022); https://doi.org/10.1126/sciadv.add5953

  59. [60]

    A. N. Morozovska, E. A. Eliseev, S. V. Kalinin, and M. V. Strikha. Critical sample sizes for appearance 38 and disappearance of ferroelectricity in nanosized hafnia-zirconia: Landau-type theory. Physical Review B (2026); https://doi.org/10.1103/hcm2-x9nj

  60. [61]

    A. N. Morozovska, E. A. Eliseev, R. (Yu) Liu, S. V. Kalinin, and D. R. Evans. Stress-Induced Ferroelectricity in Hafnium Oxide Core-Shell Nanoparticles (2026); https://doi.org/10.48550/arXiv.2602.09262

  61. [62]

    D. A. Freedman, D. Roundy, and T. A. Arias. Elastic effects of vacancies in strontium titanate: Short- and long-range strain fields, elastic dipole tensors, and chemical strain. Phys. Rev. B 80, 064108 (2009), https://doi.org/10.1103/PhysRevB.80.064108

  62. [63]

    Y. Kim, A. S. Disa, T. E. Babakol, and J. D. Brock. Strain screening by mobile oxygen vacancies in SrTiO3. Appl. Phys. Lett. 96, 251901 (2010), https://doi.org/10.1063/1.3455157

  63. [64]

    Bourgeois, B

    S. Bourgeois, B. Domenichini and J. Jupille, Excess Electrons at Oxide Surfaces, Chapter 4 in: Defects at Oxide Surfaces, ed.: J. Jupille and G. Thornton, Springer Series in Surface Sciences 58, (2015), pp. 123–147; https://doi.org/10.1007/978-3-319-14367-5_4

  64. [65]

    Highland, T.T

    M.J. Highland, T.T. Fister, D.D. Fong, P.H. Fuoss, C. Thompson, J.A. Eastman, S.K. Streiffer, and G.B. Stephenson. Equilibrium polarization of ultrathin PbTiO3 with surface compensation controlled by oxygen partial pressure. Phys. Rev. Lett. 107, 187602 (2011). https://doi.org/10.1103/PhysRevLett.107.187602

  65. [66]

    Yang, A.N

    S.M. Yang, A.N. Morozovska, R. Kumar, E.A. Eliseev, Y. Cao, L. Mazet, N. Balke, S. Jesse, R. Vasudevan, C. Dubourdieu, S.V. Kalinin. Mixed electrochemical-ferroelectric states in nanoscale ferroelectrics. Nat. Phys. 13, 812 (2017). https://doi.org/10.1038/nphys4103

  66. [67]

    Delodovici, P

    F. Delodovici, P. Barone, and S. Picozzi. Finite-size effects on ferroelectricity in rhombohedral HfO2. Phys. Rev. B 106, 115438 (2022); https://doi.org/10.1103/PhysRevB.106.115438

  67. [68]

    Delodovici, P

    F. Delodovici, P. Barone, and S. Picozzi, Trilinear-coupling-driven ferroelectricity in HfO2, Physical Review Materials 5, 064405 (2021); https://doi.org/10.1103/PhysRevMaterials.5.064405

  68. [69]

    Lee, K.-J

    H.-J. Lee, K.-J. Go, P. Kumar, C. H. Kim, Y. Kim, K. Lee, T. Shimizu, S. C. Chae, H. Jin, M. Lee, U. Waghmare, S.-Y. Choi, J. H. Lee, Phonon-pair-driven Ferroelectricity Causes Costless Domain-walls and Bulk- boundary Duality, arXiv: 2403.01415 (2024); https://doi.org/10.48550/arXiv.2403.01415

  69. [70]

    Jung and T

    S. Jung and T. Birol, Triggered ferroelectricity in HfO2 from hybrid phonons, Adv. Mater. e21602 (2026); https://doi.org/10.1002/adma.202521602 arXiv:2502.08633 https://doi.org/10.48550/arXiv.2502.08633

  70. [71]

    Jung and T

    S. Jung and T. Birol, Electric Polarization from Nonpolar Phonons, arXiv: 2512.00628 (2025); https://doi.org/10.48550/arXiv.2512.00628

  71. [72]

    H. S. Park, J. C. Shin, K. Do Kim, S. Jae Shin, J. Hee Song, S. Kyu Ryoo, I. Soo Lee, S. Hyun Lee, H. Nam, C. Seong Hwang. Enhancing ferroelectric properties of Hf0.5Zr0.5O2 thin films using the HfN/TiN and W/TiN bi-layer bottom electrodes. Journal of Materiomics, 11 (6), 101109 (2025); https://doi.org/10.1016/j.jmat.2025.101109

  72. [73]

    O. V . Bereznykov, O. S. Pylypchuk, V . I. Styopkin, S. E. Ivanchenko, D. O. Stetsenko, E. A. Eliseev, Z. Kutnjak, V . N. Poroshin, A. N. Morozovska, and N. V . Morozovsky. Interfacial Effects and Negative Capacitance State in P(VDF-TrFE) Films with BaTiO3 Nanoparticles. Composites Interfaces (2026); https://doi.org/10.1080/09276440.2025.2538943 39

  73. [74]

    H. Han, C. Voisin, S. Guillemet-Fritsch, P. Dufour, C. Tenailleau, C. Turner, and J. C. Nino, Origin of colossal permittivity in BaTiO3 via broadband dielectric spectroscopy. Journal of Applied Physics 113, 024102 (2013); https://doi.org/10.1063/1.4774099

  74. [75]

    H. Han, D. Ghosh, J.L. Jones, and J. C. Nino, Colossal Permittivity in Microwave‐Sintered Barium Titanate and Effect of Annealing on Dielectric Properties. J. Am. Ceram. Soc., 96, 485 (2013). https://doi.org/10.1111/jace.12051

  75. [76]

    Petzelt, D

    J. Petzelt, D. Nuzhnyy, V. Bovtun, M. Savinov, M. Kempa, I. Rychetsky, Broadband dielectric and conductivity spectroscopy of inhomogeneous and composite conductors. Phys. Stat. Sol. A 210, 2259 (2013), https://doi.org/10.1002/pssa.201329288

  76. [77]

    O. S. Pylypchuk, S. E. Ivanchenko, M. Y. Yelisieiev, A. S. Nikolenko, V. I. Styopkin, B. Pokhylko, V. Kushnir, D. O. Stetsenko, O. Bereznykov, O. V. Leschenko, E. A. Eliseev, V. N. Poroshin, N. V. Morozovsky, V. V. Vainberg, and A. N. Morozovska. Behavior of the Dielectric and Pyroelectric Responses of Ferroelectric Fine- Grained Ceramics. Journal of the ...

  77. [78]

    Saleem, M

    M. Saleem, M. S. Butt, A. Maqbool, M. A. Umer, M. Shahid, F. Javaid, R. A. Malik, H. Jabbar, H. M. W. Khalil, L. D. Hwan, M. Kim, B.-K. Koo, S. J. Jeong, Percolation phenomena of dielectric permittivity of a microwave-sintered BaTiO3-Ag nanocomposite for high energy capacitor, Journal of Alloys and Compounds, 822, 153525 (2020), https://doi.org/10.1016/j....

  78. [79]

    Lunkenheimer, S

    P. Lunkenheimer, S. Krohns, S. Riegg, S.G. Ebbinghaus, A. Reller, and A. Loidl, Colossal dielectric constants in transition-metal oxides. Eur. Phys. J. Spec. Topics, 180, 61-89 (2009), https://doi.org/10.1140/epjst/e2010-01212-5

  79. [80]

    Petzelt, D

    J. Petzelt, D. Nuzhnyy, V. Bovtun, D.A. Crandles. Origin of the colossal permittivity of (Nb+ In) co- doped rutile ceramics by wide-range dielectric spectroscopy. Phase Transitions 91, 932 (2018). https://doi.org/10.1080/01411594.2018.1501801

  80. [81]

    Rychetský, D

    I. Rychetský, D. Nuzhnyy, J. Petzelt, Giant permittivity effects from the core–shell structure modeling of the dielectric spectra. Ferroelectrics 569, 9 (2020). https://doi.org/10.1080/00150193.2020.1791659

Showing first 80 references.