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arxiv: 2605.22369 · v1 · pith:KHCIYSQZnew · submitted 2026-05-21 · ❄️ cond-mat.mtrl-sci

Improvement of piezocatalytic performance of Na0.5Bi0.5TiO3 perovskite using K doping for efficient Rhodamine B degradation

Pith reviewed 2026-05-22 04:42 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords piezocatalysisperovskitepotassium dopingmorphotropic phase boundaryRhodamine Bsodium bismuth titanateultrasonic degradation
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The pith

Potassium doping at 15 percent in sodium bismuth titanate creates a mixed crystal phase that drives eight times faster piezocatalytic breakdown of Rhodamine B.

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

This paper tests potassium-doped versions of the perovskite Na0.5Bi0.5TiO3 as catalysts that convert ultrasonic vibrations into chemical energy for destroying organic pollutants. At 15 percent potassium the material forms a morphotropic phase boundary where two crystal structures coexist, while also showing smaller particles, a favorable bandgap, and elevated internal strain. These features together generate more surface charges under mechanical stress, which then attack the dye molecules. A reader would care because the result demonstrates a route to water purification that harvests ordinary mechanical energy rather than requiring light, electricity, or added chemicals. The best composition removes all Rhodamine B in 90 minutes and shows an eightfold rise in reaction speed over the pure material.

Core claim

The central claim is that Na0.5-xKxBi0.5TiO3 at x equals 0.15 develops a morphotropic phase boundary together with reduced particle size, an optimal bandgap, and high lattice strain; these changes act in concert to raise the piezoelectric response and thereby accelerate the ultrasonic degradation of Rhodamine B, yielding complete removal in 90 minutes and a rate constant eight times larger than the undoped compound.

What carries the argument

The morphotropic phase boundary, the narrow composition window in which two distinct crystal phases coexist and thereby enhance the piezoelectric coefficient and charge separation under mechanical stress.

If this is right

  • The NK15BT powder achieves complete Rhodamine B removal in 90 minutes under ultrasonic vibration.
  • Its apparent first-order rate constant is eight times higher than that of the undoped NK0BT powder.
  • The material retains activity after multiple reuse cycles and mineralizes the dye rather than merely adsorbing it.
  • The performance gain is attributed to the simultaneous presence of the morphotropic phase boundary, smaller crystallites, suitable bandgap, and elevated lattice strain.

Where Pith is reading between the lines

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

  • The same potassium-doping route could be applied to other lead-free perovskites to raise their piezocatalytic activity for additional pollutants.
  • Because lattice strain contributes to the effect, thin-film or nanostructured forms of the material may deliver still higher rates.
  • Practical tests with real industrial wastewater containing mixed contaminants would clarify whether the 90-minute performance holds outside idealized dye solutions.

Load-bearing premise

That the measured dye removal and mineralization arise chiefly from piezocatalytically generated charges enabled by the morphotropic phase boundary and the listed material properties, rather than from direct ultrasonic cleavage of the dye or simple surface adsorption.

What would settle it

A control experiment in which the same NK15BT powder is sonicated in the presence of a radical scavenger or under conditions that suppress piezoelectric charge separation, such as a non-piezoelectric reference composition outside the morphotropic phase boundary, showing whether the degradation rate falls to the level of the undoped material.

Figures

Figures reproduced from arXiv: 2605.22369 by Daoud Mezzane, Hana Ursic, Jaafar Ghanbaja, Manal Benyoussef, Mbarek Amjoud, Mimoun El Marssi, Mohamed Goune, Mustapha Raihane, Nejc Suban, Salma Ayadh, Salma Touili, Zdravko Kutnjak.

Figure 1
Figure 1. Figure 1: The four NKxBT samples with x=0, 15, 20, and 25 were synthesized and abbreviated as NK0BT, NK15BT, NK20BT, and NK25BT [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: a. XRD pattern of NKxBT powders b. larger views of (110), (111) and (200) planes [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Williamson-Hall (W-H) plots using XRD data for NKxBT samples [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: a. TEM images of NKxBT powders, b. Variation of average grain size of NKxBT powders [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
read the original abstract

Piezocatalysis, based on the piezoelectric properties of catalysts, breaks down the barrier between mechanical energy and chemical energy. It describes the use of charges induced by piezoelectricity to assist typical chemical processes while harvesting various forms of mechanical green energy. The performance of piezocatalysis is predominantly governed by the piezoelectric properties of materials. The main aim of this work is to evaluate and analyze the potential of potassium doped sodium bismuth titanate Na0.5-xKxBi0.5TiO3 abbreviated as NKxBT (0, 0.15, 0.20, and 0.25), as a piezocatalyst in the degradation of the organic dye Rhodamine B RhB under ultrasonic vibration. The synthesis of NKxBT nanopowders was conducted using the sol-gel autocombustion method. Coupled structural analysis reveals the presence of an intermediate Morphotropic Phase Boundary (MPB, where two phases coexist) in the optimal NK15BT composition. The piezocatalytic degradation results showed a total piezo-degradation in only 90 min and a rate constant 8 times higher than the undoped NK0BT. The enhanced piezocatalytic activity results from a synergistic effect of MPB presence, reduced particle size, optimal bandgap and high lattice strain. The NK15BT sample also demonstrated good reusability and good mineralization.

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

1 major / 2 minor

Summary. The manuscript reports the synthesis of K-doped Na0.5Bi0.5TiO3 (NKxBT, x=0, 0.15, 0.20, 0.25) nanopowders via sol-gel autocombustion and evaluates their piezocatalytic degradation of Rhodamine B under ultrasonic vibration. It identifies an MPB at the optimal NK15BT composition, which together with reduced particle size, optimal bandgap and high lattice strain yields complete degradation in 90 min and an 8-fold higher rate constant relative to undoped NK0BT. Supporting XRD, SEM, UV-Vis and strain data are presented along with reusability, mineralization and control experiments (ultrasound alone and dark adsorption) that show negligible activity.

Significance. If the central claims hold, the work is significant for piezocatalysis research because it shows how targeted K doping near the MPB in a lead-free perovskite can be used to enhance piezoelectric response and catalytic efficiency for organic pollutant removal. The explicit controls isolating the piezocatalytic contribution and the demonstration of reusability strengthen the practical relevance for green, mechanically driven wastewater treatment.

major comments (1)
  1. Results section on piezocatalytic performance: the stated 8-fold rate-constant increase and 90-min complete degradation for NK15BT must be supported by the explicit pseudo-first-order kinetic plots, fitted rate constants, and any reported uncertainties or R² values for all four compositions so that the quantitative improvement can be independently verified.
minor comments (2)
  1. Methods: the ultrasonic frequency, power density and reactor geometry used for the piezocatalysis tests should be stated explicitly to enable full reproducibility.
  2. Figure captions and structural analysis: peak indexing or Rietveld refinement parameters confirming the MPB phase coexistence in NK15BT would clarify the structural basis for the claimed synergistic effect.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their positive assessment of our work and for the constructive comment, which will help improve the clarity of the quantitative results. We address the point as follows.

read point-by-point responses
  1. Referee: Results section on piezocatalytic performance: the stated 8-fold rate-constant increase and 90-min complete degradation for NK15BT must be supported by the explicit pseudo-first-order kinetic plots, fitted rate constants, and any reported uncertainties or R² values for all four compositions so that the quantitative improvement can be independently verified.

    Authors: We agree that providing the full set of kinetic plots and fitted parameters will strengthen the manuscript and allow independent verification. In the revised version we will add the pseudo-first-order kinetic plots (ln(C0/C) vs. time) for all four compositions (NK0BT, NK15BT, NK20BT, NK25BT). We will also include a table in the main text or supplementary information that reports the fitted rate constants k, the corresponding R² values, and the standard errors (uncertainties) obtained from the linear regression for each composition. This will explicitly document the approximately eight-fold enhancement observed for the optimal NK15BT sample relative to the undoped NK0BT. revision: yes

Circularity Check

0 steps flagged

No significant circularity; experimental reporting only

full rationale

The paper is a materials science experimental study reporting sol-gel synthesis of NKxBT powders, XRD/SEM/UV-Vis characterization showing MPB at x=0.15, measured piezocatalytic RhB degradation rates under ultrasound, and control tests for adsorption/sonochemistry. The central claim links observed performance gains directly to measured properties (particle size, bandgap, strain) without equations, fitted parameters renamed as predictions, or derivations that reduce to inputs by construction. No self-citation chains or ansatzes are load-bearing for the results; all key quantities are independently measured and falsifiable via the described experiments.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on experimental observations of degradation kinetics and structural characterization; it assumes that piezoelectric charge generation under ultrasound directly drives the observed dye breakdown and that the identified MPB and property changes are the dominant causes of improvement.

axioms (1)
  • domain assumption Piezoelectric properties of perovskites can be tuned via doping to enhance charge separation and catalytic activity under mechanical excitation.
    Invoked when attributing performance gains to MPB, bandgap, and strain without independent verification of charge generation mechanism.

pith-pipeline@v0.9.0 · 5850 in / 1422 out tokens · 51784 ms · 2026-05-22T04:42:03.652689+00:00 · methodology

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Works this paper leans on

54 extracted references · 54 canonical work pages

  1. [1]

    Y . Liu et al., “Enhanced piezo-catalytic performance of BaTiO3 nanorods combining highly exposed active crystalline facets and superior deformation capability: Water purification and activation mechanism,” Chemical Engineering Journal, vol. 488, p. 150768, May 2024, doi: 10.1016/j.cej.2024.150768

  2. [2]

    Effect of poling on piezocatalytic and electrochemical properties of Pb(Zr0.52Ti0.48)O3 ceramics,

    S. Verma, M. Sharma, A. Halder, and R. Vaish, “Effect of poling on piezocatalytic and electrochemical properties of Pb(Zr0.52Ti0.48)O3 ceramics,” Surfaces and Interfaces, vol. 30, p. 101827, Jun. 2022, doi: 10.1016/j.surfin.2022.101827

  3. [3]

    Role of Bi3+ ion substitution on the piezocatalytic degradation performance of lead-free BaTi0·89Sn0·11O3 at low vibrational energy,

    S. Touili et al., “Role of Bi3+ ion substitution on the piezocatalytic degradation performance of lead-free BaTi0·89Sn0·11O3 at low vibrational energy,” Ceram Int, vol. 50, no. 17, pp. 29437–29447, Sep. 2024, doi: 10.1016/j.ceramint.2024.05.238

  4. [4]

    NaNbO 3 Nanorods: Photopiezocatalysts for Elevated Bacterial Disinfection and Wastewater Treatment,

    A. Sharma, U. Bhardwaj, D. Jain, and H. S. Kushwaha, “NaNbO 3 Nanorods: Photopiezocatalysts for Elevated Bacterial Disinfection and Wastewater Treatment,” ACS Omega, vol. 7, no. 9, pp. 7595–7605, Mar. 2022, doi: 10.1021/acsomega.1c06109

  5. [5]

    Exploring the piezocatalytic dye degradation capability of lithium niobate,

    G. Singh, M. Sharma, and R. Vaish, “Exploring the piezocatalytic dye degradation capability of lithium niobate,” Advanced Powder Technology, vol. 31, no. 4, pp. 1771–1775, Apr. 2020, doi: 10.1016/j.apt.2020.01.031

  6. [6]

    Enhanced piezocatalytic activity of BiFeO3 incorporated PVDF-HFP membrane for efficient degradation of carcinogenic industrial pollutant,

    J. Roy et al., “Enhanced piezocatalytic activity of BiFeO3 incorporated PVDF-HFP membrane for efficient degradation of carcinogenic industrial pollutant,” Ceram Int, vol. 50, no. 10, pp. 18012–18023, May 2024, doi: 10.1016/j.ceramint.2024.02.290

  7. [7]

    Enhancement of piezoelectric catalysis of Na0.5Bi0.5TiO3 with electric poling for dye decomposition,

    J. Guan et al., “Enhancement of piezoelectric catalysis of Na0.5Bi0.5TiO3 with electric poling for dye decomposition,” Ceram Int, vol. 48, no. 3, pp. 3695–3701, Feb. 2022, doi: 10.1016/j.ceramint.2021.10.151

  8. [8]

    Enhancement of Photocatalytic Activity of Sodium Bismuth Titanate by Doping with Copper, Silver, and Tin Ions,

    S. Kurra, P . Venkataswamy, G. Ravi, C. Sudhakar Reddy, B. Jaganmohan Reddy, and M. Vithal, “Enhancement of Photocatalytic Activity of Sodium Bismuth Titanate by Doping with Copper, Silver, and Tin Ions,” Z Anorg Allg Chem, vol. 645, no. 5, pp. 529–536, Mar. 2019, doi: 10.1002/zaac.201800337

  9. [9]

    Designing pseudocubic perovskites with enhanced nanoscale polarization,

    I. Levin, W. J. Laws, D. Wang, and I. M. Reaney, “Designing pseudocubic perovskites with enhanced nanoscale polarization,” Appl Phys Lett, vol. 111, no. 21, Nov. 2017, doi: 10.1063/1.5007700

  10. [10]

    Effect of sintering temperature on the microstructure and electrical properties of (Na0.5Bi0.5)TiO3 processed by the sol-gel method,

    M. Mesrar, T. Lamcharfi, N.-S. Echatoui, and F. Abdi, “Effect of sintering temperature on the microstructure and electrical properties of (Na0.5Bi0.5)TiO3 processed by the sol-gel method,” J Solgel Sci Technol, vol. 103, no. 3, pp. 820–831, Sep. 2022, doi: 10.1007/s10971-022-05885-y

  11. [11]

    Structure and ferroelectric behaviour of Na 0.5 Bi 0.5 TiO 3 -KNbO 3 ceramics,

    G. Wang, D. A. Hall, T. P . Comyn, L. Daniel, and A. K. Kleppe, “Structure and ferroelectric behaviour of Na 0.5 Bi 0.5 TiO 3 -KNbO 3 ceramics,” Advances in Applied Ceramics, vol. 115, no. 2, pp. 89–95, Feb. 2016, doi: 10.1080/17436753.2015.1104053

  12. [12]

    Dielectric polarizability of ions and the corresponding effective number of electrons,

    N. W. Grimes and R. W. Grimes, “Dielectric polarizability of ions and the corresponding effective number of electrons,” Journal of Physics: Condensed Matter, vol. 10, no. 13, pp. 3029–3034, Apr. 1998, doi: 10.1088/0953-8984/10/13/019

  13. [14]

    Precise calculation of crystallite size of nanomaterials: A review,

    S. A. Hassanzadeh-Tabrizi, “Precise calculation of crystallite size of nanomaterials: A review,” J Alloys Compd, vol. 968, p. 171914, Dec. 2023, doi: 10.1016/j.jallcom.2023.171914

  14. [15]

    Zn doping effect on the properties of SnO2 nanostructure by co- precipitation technique,

    A. G. Habte, F. G. Hone, and F. B. Dejene, “Zn doping effect on the properties of SnO2 nanostructure by co- precipitation technique,” Applied Physics A, vol. 125, no. 6, p. 402, Jun. 2019, doi: 10.1007/s00339-019-2695- 5

  15. [16]

    Room temperature ferromagnetism in Cr doped SrSnO3 perovskite system,

    M. Muralidharan, V. Anbarasu, A. Elaya Perumal, and K. Sivakumar, “Room temperature ferromagnetism in Cr doped SrSnO3 perovskite system,” Journal of Materials Science: Materials in Electronics, vol. 28, no. 5, pp. 4125–4137, Mar. 2017, doi: 10.1007/s10854-016-6032-x

  16. [17]

    X-ray peak profile analysis of Sb 2 O 3 -doped ZnO nanocomposite semiconductor,

    B. Rajesh Kumar and B. Hymavathi, “X-ray peak profile analysis of Sb 2 O 3 -doped ZnO nanocomposite semiconductor,” Advances in Natural Sciences: Nanoscience and Nanotechnology, vol. 9, no. 3, p. 035018, Sep. 2018, doi: 10.1088/2043-6254/aadc6b

  17. [18]

    Indium Doping to GaN Grown on GaAs{114}B Substrates by Metalorganic Vapor Phase Epitaxy,

    M. Funato, K. Shimogami, S. Ujita, Y . Kawaguchi, Sz. Fujita, and Sg. Fujita, “Indium Doping to GaN Grown on GaAs{114}B Substrates by Metalorganic Vapor Phase Epitaxy,” physica status solidi (c), no. 1, pp. 434–437, Jan. 2003, doi: 10.1002/pssc.200390081

  18. [19]

    Synergistic strain engineering of perovskite single crystals for highly stable and sensitive X-ray detectors with low-bias imaging and monitoring,

    J. Jiang et al., “Synergistic strain engineering of perovskite single crystals for highly stable and sensitive X-ray detectors with low-bias imaging and monitoring,” Nat Photonics, vol. 16, no. 8, pp. 575–581, Aug. 2022, doi: 10.1038/s41566-022-01024-9

  19. [20]

    Electrical properties and conduction mechanisms of K, Ga co- substituted Na0.5Bi0.5TiO3 ferroelectrics,

    X. Xu, X. Liu, R. Rao, Y . Zhao, H. Du, and J. Shi, “Electrical properties and conduction mechanisms of K, Ga co- substituted Na0.5Bi0.5TiO3 ferroelectrics,” Ceram Int, vol. 46, no. 14, pp. 22321–22329, Oct. 2020, doi: 10.1016/j.ceramint.2020.05.312

  20. [21]

    Strain enhancement due to oxygen vacancies in perovskite oxide films,

    M. Tyunina, J. Levoska, O. Pacherova, T. Kocourek, and A. Dejneka, “Strain enhancement due to oxygen vacancies in perovskite oxide films,” J Mater Chem C Mater, vol. 10, no. 17, pp. 6770–6777, 2022, doi: 10.1039/D1TC04969K

  21. [22]

    Structure of Pb(Fe2/3W1/3)O3 single crystals with partial cation order,

    S. A. Ivanov, A. I. Stash, L. Riekehr, Y .-S. Chen, and Z.-G. Ye, “Structure of Pb(Fe2/3W1/3)O3 single crystals with partial cation order,” Sci Rep, vol. 10, no. 1, p. 14567, Sep. 2020, doi: 10.1038/s41598-020-71438-4

  22. [23]

    Enhanced mechanical and ferroelectric properties through grain size refinement in site specific substituted lead free Na 0.5−x K x Bi 0.5 TiO 3 (x = 0–0.10) ceramics,

    T. Karthik and S. Asthana, “Enhanced mechanical and ferroelectric properties through grain size refinement in site specific substituted lead free Na 0.5−x K x Bi 0.5 TiO 3 (x = 0–0.10) ceramics,” Mater Lett, vol. 190, pp. 273–275, Mar. 2017, doi: 10.1016/j.matlet.2017.01.025

  23. [24]

    Effect of surface area of grain boundaries on stress relaxation behavior in pure copper over wide range of grain sizes,

    Y . Suzuki et al., “Effect of surface area of grain boundaries on stress relaxation behavior in pure copper over wide range of grain sizes,” Materials Science and Engineering: A, vol. 794, p. 139585, Sep. 2020, doi: 10.1016/j.msea.2020.139585

  24. [25]

    Significantly enhanced catalytic performance of solid-state-synthesized Na0.5Bi0.5TiO3 nanoparticles by piezo-phototronic coupling effect,

    L. Shi et al., “Significantly enhanced catalytic performance of solid-state-synthesized Na0.5Bi0.5TiO3 nanoparticles by piezo-phototronic coupling effect,” Journal of Materials Science: Materials in Electronics, vol. 35, no. 18, p. 1244, Jun. 2024, doi: 10.1007/s10854-024-12982-x

  25. [26]

    Enhanced energy storage performance of Na0.5Bi0.5TiO3 lead–free ceramics under low electric field,

    M. Chen, S. Zhan, Q. Yuan, Y . Li, Y . Lin, and H. Yang, “Enhanced energy storage performance of Na0.5Bi0.5TiO3 lead–free ceramics under low electric field,” Mater Today Energy, vol. 31, p. 101193, Jan. 2023, doi: 10.1016/j.mtener.2022.101193

  26. [27]

    Novel NBT-based relaxor ferroelectric ceramics with excellent discharge performance and high-temperature stability,

    M. Chen, Y . Pu, and L. Zhang, “Novel NBT-based relaxor ferroelectric ceramics with excellent discharge performance and high-temperature stability,” Journal of Materials Science: Materials in Electronics, vol. 32, no. 18, pp. 23540–23553, Sep. 2021, doi: 10.1007/s10854-021-06841-2

  27. [28]

    Raman and infrared spectroscopy of Na0.5Bi0.5TiO3 - BaTiO3 ceramics,

    J. Suchanicz, I. Jankowska-Sumara, and T. V. Kruzina, “Raman and infrared spectroscopy of Na0.5Bi0.5TiO3 - BaTiO3 ceramics,” J Electroceram, vol. 27, no. 2, pp. 45–50, Oct. 2011, doi: 10.1007/s10832-011-9648-5

  28. [29]

    Study on vibrational Raman modes and electric properties of lead-free sodium bismuth titanate – bismuth magnesium zirconate piezoelectric ceramics,

    D. E. Jain Ruth, “Study on vibrational Raman modes and electric properties of lead-free sodium bismuth titanate – bismuth magnesium zirconate piezoelectric ceramics,” Chemical Physics Impact, vol. 6, p. 100172, Jun. 2023, doi: 10.1016/j.chphi.2023.100172

  29. [30]

    Structural and Raman spectroscopic studies of poled lead-free piezoelectric sodium bismuth titanate ceramics,

    D. E. Jain Ruth and B. Sundarakannan, “Structural and Raman spectroscopic studies of poled lead-free piezoelectric sodium bismuth titanate ceramics,” Ceram Int, vol. 42, no. 4, pp. 4775–4778, Mar. 2016, doi: 10.1016/j.ceramint.2015.11.162

  30. [31]

    (1-x)(Na0.5Bi0.5)TiO3-x(K0.5Bi0.5)TiO3 ceramics near morphotropic phase boundary: A structural and electrical study,

    M. Mesrar, T. Lamcharfi, N.-S. Echatoui, and F. Abdi, “(1-x)(Na0.5Bi0.5)TiO3-x(K0.5Bi0.5)TiO3 ceramics near morphotropic phase boundary: A structural and electrical study,” Materialia (Oxf), vol. 22, p. 101404, May 2022, doi: 10.1016/j.mtla.2022.101404

  31. [32]

    Effects of defect on thermal stability and photoluminescence in quenched Ho-doped 0.94Na 0.5 Bi 0.5 TiO 3 –0.06BaTiO 3 lead-free ceramics,

    L.-Q. Zheng et al., “Effects of defect on thermal stability and photoluminescence in quenched Ho-doped 0.94Na 0.5 Bi 0.5 TiO 3 –0.06BaTiO 3 lead-free ceramics,” J Mater Res, pp. 1–9, Oct. 2020, doi: 10.1557/jmr.2020.274

  32. [33]

    Electric properties of Mn-substituted Na 0.5 Bi 0.5 TiO 3 ceramics in unpoled and poled states,

    J. Suchanicz et al., “Electric properties of Mn-substituted Na 0.5 Bi 0.5 TiO 3 ceramics in unpoled and poled states,” Phase Transitions, vol. 93, no. 12, pp. 1114–1122, Dec. 2020, doi: 10.1080/01411594.2020.1844200

  33. [34]

    Ferroelectric Properties and Electrocaloric Effect in Dy2O3 Substitution on Lead-Free (Na0.5 Bi0.5)0.94 Ba0.06TiO3 Ceramic,

    O. Turki, I. Zouari, A. Slimani, Z. Sassi, L. Seveyrat, and H. Khemakhem, “Ferroelectric Properties and Electrocaloric Effect in Dy2O3 Substitution on Lead-Free (Na0.5 Bi0.5)0.94 Ba0.06TiO3 Ceramic,” J Electron Mater, vol. 52, no. 2, pp. 1013–1023, Feb. 2023, doi: 10.1007/s11664-022-10077-z

  34. [35]

    Sonophotocatalytic degradation mechanisms of Rhodamine B dye via radicals generation by micro- and nano-particles of ZnO,

    C. Lops et al., “Sonophotocatalytic degradation mechanisms of Rhodamine B dye via radicals generation by micro- and nano-particles of ZnO,” Appl Catal B, vol. 243, pp. 629–640, Apr. 2019, doi: 10.1016/j.apcatb.2018.10.078

  35. [36]

    How To Correctly Determine the Band Gap Energy of Modified Semiconductor Photocatalysts Based on UV–Vis Spectra,

    P . Makuła, M. Pacia, and W. Macyk, “How To Correctly Determine the Band Gap Energy of Modified Semiconductor Photocatalysts Based on UV–Vis Spectra,” J Phys Chem Lett, vol. 9, no. 23, pp. 6814–6817, Dec. 2018, doi: 10.1021/acs.jpclett.8b02892

  36. [37]

    Internal defect structure of calcium doped magnesium oxide nanoparticles studied by positron annihilation spectroscopy,

    A. Das, A. C. Mandal, S. Roy, and P . M. G. Nambissan, “Internal defect structure of calcium doped magnesium oxide nanoparticles studied by positron annihilation spectroscopy,” AIP Adv, vol. 8, no. 9, Sep. 2018, doi: 10.1063/1.5001105

  37. [38]

    Micro-structural and opto-electronic correlation studies of sol–gel derived Zn1−xSmxS nanoparticles through the analysis of vacancy type defects,

    S. Mandal, S. I. Ali, P . Ghosh, D. Dutta, and A. C. Mandal, “Micro-structural and opto-electronic correlation studies of sol–gel derived Zn1−xSmxS nanoparticles through the analysis of vacancy type defects,” Journal of Materials Science: Materials in Electronics, vol. 35, no. 3, p. 249, Jan. 2024, doi: 10.1007/s10854-024-12016-6

  38. [39]

    Ghosh, P

    S. Ghosh, P . Samanta, W. Jang, C.-M. Yang, N. C. Murmu, and T. Kuila, “Improvement of the Supercapacitor Performance of Nickel Molybdenum Chalcogenides/Reduced Graphene Oxide Composites through Vanadium- Doping Induced Crystal Strain Relaxation and Band Gap Modification,” ACS Appl Energy Mater, vol. 5, no. 2, pp. 1528–1541, Feb. 2022, doi: 10.1021/acsaem.1c02932

  39. [40]

    The effect of strain-induced band-gap narrowing on high concentration phosphorus diffusion in silicon,

    R. B. Fair, “The effect of strain-induced band-gap narrowing on high concentration phosphorus diffusion in silicon,” J Appl Phys, vol. 50, no. 2, pp. 860–868, Feb. 1979, doi: 10.1063/1.326001

  40. [41]

    Development of Yttrium-Doped BaTiO 3 for Next-Generation Multilayer Ceramic Capacitors,

    M. Tihtih et al., “Development of Yttrium-Doped BaTiO 3 for Next-Generation Multilayer Ceramic Capacitors,” ACS Omega, vol. 8, no. 9, pp. 8448–8460, Mar. 2023, doi: 10.1021/acsomega.2c07497

  41. [42]

    Absolute electronegativity and hardness: application to inorganic chemistry,

    R. G. Pearson, “Absolute electronegativity and hardness: application to inorganic chemistry,” Inorg Chem, vol. 27, no. 4, pp. 734–740, Feb. 1988, doi: 10.1021/ic00277a030

  42. [43]

    Band edge positions as a key parameter to a systematic design of heterogeneous photocatalyst,

    E. A. Abdullah, “Band edge positions as a key parameter to a systematic design of heterogeneous photocatalyst,” European Journal of Chemistry, vol. 10, no. 1, pp. 82–94, Mar. 2019, doi: 10.5155/eurjchem.10.1.82-94.1809

  43. [44]

    Efficient piezocatalytic properties of Na 0.5 Bi 0.5 TiO 3 nanoparticles for dye degradation and hydrogen peroxide production,

    B. Liang, X. Zhu, H. Yu, Y . Zhang, and W. Ye, “Efficient piezocatalytic properties of Na 0.5 Bi 0.5 TiO 3 nanoparticles for dye degradation and hydrogen peroxide production,” J Adv Dielectr, Mar. 2024, doi: 10.1142/S2010135X24500061

  44. [45]

    Solvothermal synthesis of (Na 0.8 K 0.2 ) 0.5 Bi 0.5 TiO 3 piezoelectric catalyst with morphotropic- phase-boundary structure for efficient dye degradation,

    N. Xie et al., “Solvothermal synthesis of (Na 0.8 K 0.2 ) 0.5 Bi 0.5 TiO 3 piezoelectric catalyst with morphotropic- phase-boundary structure for efficient dye degradation,” New Journal of Chemistry, vol. 47, no. 32, pp. 15047–15056, 2023, doi: 10.1039/D3NJ02473C

  45. [46]

    Enhanced piezo-photocatalytic performance by piezoelectric and visible light photoexcitation coupling through piezoelectric Na 0.5 Bi 0.5 TiO 3 micron crystals,

    R. Zhang et al., “Enhanced piezo-photocatalytic performance by piezoelectric and visible light photoexcitation coupling through piezoelectric Na 0.5 Bi 0.5 TiO 3 micron crystals,” RSC Adv, vol. 10, no. 13, pp. 7443–7451, 2020, doi: 10.1039/D0RA01101K

  46. [47]

    Visible-Light-Induced Photocatalytic Degradation of Rhodamine B Dye Using a CuS/ZnS p-n Heterojunction Nanocomposite under Visible-Light Irradiation,

    R. Mugumo, E. Ichipi, S. M. Tichapondwa, and E. M. N. Chirwa, “Visible-Light-Induced Photocatalytic Degradation of Rhodamine B Dye Using a CuS/ZnS p-n Heterojunction Nanocomposite under Visible-Light Irradiation,” Catalysts, vol. 13, no. 8, p. 1184, Aug. 2023, doi: 10.3390/catal13081184

  47. [48]

    Band Gap Narrowing of Bi- Doped NaTaO 3 for Photocatalytic Hydrogen Evolution under Simulated Sunlight: A Pseudocubic Phase Induced by Doping,

    G. A. S. Alves, H. A. Centurion, J. R. Sambrano, M. M. Ferrer, and R. V. Gonçalves, “Band Gap Narrowing of Bi- Doped NaTaO 3 for Photocatalytic Hydrogen Evolution under Simulated Sunlight: A Pseudocubic Phase Induced by Doping,” ACS Appl Energy Mater, vol. 4, no. 1, pp. 671–679, Jan. 2021, doi: 10.1021/acsaem.0c02547

  48. [49]

    Efficient water splitting over Na1−xKxTaO3 photocatalysts with cubic perovskite structure,

    C.-C. Hu, Y .-L. Lee, and H. Teng, “Efficient water splitting over Na1−xKxTaO3 photocatalysts with cubic perovskite structure,” J Mater Chem, vol. 21, no. 11, p. 3824, 2011, doi: 10.1039/c0jm03451g

  49. [50]

    Strain Engineering to Boost Piezocatalytic Activity of BaTiO 3,

    J. Ai, C. Jin, D. Liu, J. Zhang, and L. Zhang, “Strain Engineering to Boost Piezocatalytic Activity of BaTiO 3,” ChemCatChem, vol. 15, no. 5, Mar. 2023, doi: 10.1002/cctc.202201316

  50. [51]

    Facile synthesis of BiOCl/g-C3N4 heterojunction via in situ hydrolysis of Bi nanospheres: a high- efficiency visible-light-driven photocatalyst,

    Z. Zeng et al., “Facile synthesis of BiOCl/g-C3N4 heterojunction via in situ hydrolysis of Bi nanospheres: a high- efficiency visible-light-driven photocatalyst,” Journal of Materials Science: Materials in Electronics, vol. 32, no. 8, pp. 9972–9989, Apr. 2021, doi: 10.1007/s10854-021-05655-6

  51. [52]

    Piezocatalytic performance of Na0.5Bi0.5TiO3 nanoparticles for degradation of organic pollutants,

    L. Shi et al., “Piezocatalytic performance of Na0.5Bi0.5TiO3 nanoparticles for degradation of organic pollutants,” J Alloys Compd, vol. 895, p. 162591, Feb. 2022, doi: 10.1016/j.jallcom.2021.162591

  52. [53]

    Effective enhancement of piezocatalytic activity of BaTiO3 nanowires under ultrasonic vibration,

    J. Wu, N. Qin, and D. Bao, “Effective enhancement of piezocatalytic activity of BaTiO3 nanowires under ultrasonic vibration,” Nano Energy, vol. 45, pp. 44–51, Mar. 2018, doi: 10.1016/j.nanoen.2017.12.034

  53. [54]

    The morphotropic phase boundary based BCST ferroelectric system for water remediation through Bi-catalytic activity,

    N. P . Maria Joseph Raj, N. R. Alluri, G. Khandelwal, and S.-J. Kim, “The morphotropic phase boundary based BCST ferroelectric system for water remediation through Bi-catalytic activity,” J Alloys Compd, vol. 871, p. 159503, Aug. 2021, doi: 10.1016/j.jallcom.2021.159503

  54. [55]

    A facile synthesized Z-scheme Bi2O3/SnS/Ag ternary nanocomposite: An expedited visible photocatalysis by plasmonic silver for efficient organic decontamination,

    S. Jain et al., “A facile synthesized Z-scheme Bi2O3/SnS/Ag ternary nanocomposite: An expedited visible photocatalysis by plasmonic silver for efficient organic decontamination,” Opt Mater (Amst), vol. 145, p. 114434, Nov. 2023, doi: 10.1016/j.optmat.2023.114434