Interfacial electric field in Zr-MOF-grafted carbon nitride to boost H2O2 piezo-synthesis under ambient conditions

Jingyi Yang a, Zhi Li *ac, Huiru Chen a, Jie Leng a, Li Gong *b and Mingshan Zhu *ac
aGuangdong Engineering Technology Research Center of Water Treatment Processes and Materials, College of Environment and Climate, Jinan University, Guangzhou 511443, China. E-mail: zhili@jnu.edu.cn; zhumingshan@jnu.edu.cn
bInstrumental Analysis and Research Center, Sun Yat-Sen University, Guangzhou, 510275, China. E-mail: gongli2@mail.sysu.edu.cn
cGuangdong Provincial Key Laboratory of Spine and Spinal Cord Reconstruction, The Fifth Affiliated Hospital of Jinan University (Heyuan Shenhe People's Hospital), Heyuan 517465, China

Received 7th August 2025 , Accepted 11th September 2025

First published on 17th September 2025


Abstract

Harnessing interfacial electric fields offers a promising route to boost piezocatalytic efficiency. Here, we grafted Zr-MOF onto carbon nitride to construct an interfacial electric field, leading to a hydrogen peroxide production rate of 4.76 mmol g−1 h−1via water oxidation and the oxygen reduction reaction.


Hydrogen peroxide (H2O2) has emerged as a versatile and environmentally benign oxidant with wide-ranging applications in energy storage, water treatment, and green synthesis.1 Traditional H2O2 production relies on the energy-intensive anthraquinone process, which suffers from high carbon emissions and complex infrastructure.2 The direct synthesis of H2O2 from oxygen and water offers a sustainable alternative, but conventional thermostatic approaches often require noble metal catalysts and hazardous conditions.3 In this context, piezocatalysis, an emerging technology that converts mechanical energy into chemical energy, holds great promise for sustainable H2O2 production.4,5 Its mechanism relies on stress-induced charge separation within piezoelectric materials, which initiates redox reactions between O2 and H2O to generate H2O2. However, electrons and holes produced under piezoelectric excitation rapidly recombine, limiting the catalytic efficiency.6 Therefore, promoting effective charge separation remains a key challenge for advancing piezocatalytic systems.7–9

To overcome such rapid recombination of charge carriers, previous works have mainly focused on strategies such as elemental doping10 and introducing defect sites11 to improve charge-carrier–separation efficiency.12 In recent years, constructing an internal electric field (IEF) has been recognized as an effective method for improving the reactivity and selectivity of catalytic reactions in the energy and environmental fields.13 Zhang et al. prepared a step-scheme heterojunction ZnO/COF(TpPa-Cl) using a simple electrostatic self-assembly method and studied its photocatalytic H2O2 generation performance.14 However, research on using the IEF for enhancing charge carrier separation in piezocatalysis remains relatively scarce.

Carbon nitride (C3N4) was first reported in 2019 to have piezoelectrically catalyzed hydrogen-peroxide-producing activity, attributed to its excellent piezoelectric properties.15–17 However, the poor charge-carrier–separation ability of pure C3N4 limits the efficiency of its piezoelectric-catalyzed synthesis of H2O2, which may be due to its fast carrier complexation.18–21 To address this critical issue, we constructed the IEF to efficiently promote piezoelectric carrier separation by grafting MOFs22,23 onto the carbon nitride surface taking advantage of their tunable electronic structures and catalytic sites.24,25

We integrated C3N4 with UiO-66 through electrostatic self-assembly to create a composite exhibiting enhanced interfacial charge modulation. The optimized C3N4/UiO-66 system demonstrated exceptional piezocatalytic performance, achieving an H2O2 production rate of 4.76 mmol g−1 h−1 under ambient conditions, representing 12.1-fold and 11.5-fold improvements over pristine C3N4 and UiO-66, respectively. Electron paramagnetic resonance (EPR) spectra showed the simultaneous presence of *O2 and ˙OH radical species, indicating the cooperative use of oxygen reduction (ORR) and water oxidation (WOR) pathways. The IEF intensity of the C3N4/MOF was assessed by taking zeta potential measurements, and performing open-circuit voltage tests, and was found to be 1.17 times higher than that of pristine C3N4. This work has provided a generalizable strategy for developing advanced piezocatalytic WOR materials.

C3N4/UiO-66 composites were prepared via electrostatic self-assembly.14 Transmission electron microscopy (TEM) showed that UiO-66 indeed grafted onto the C3N4 surface (Fig. S1–S3) and XRD analysis revealed a shift in the (002) diffraction peak from 25.97° in C3N4 to 27.3° in the composite, indicating a reduced interlayer spacing (Fig. 1a). A shifted (100) peak at 12° and the retained (111) peak of UiO-66 at 7.2° suggested strong interfacial interactions and maintained structural integrity.26 Fourier-transform infrared spectroscopy (FT-IR) (Fig. 1b) showed characteristic peaks of triazine units at 810 cm−1 and 1200–1700 cm−1 for both C3N4 and the composite, with no evident COO signals, indicating a predominant C3N4 framework.27 Zeta potential analysis (Fig. 1c) confirmed the occurrence of electrostatic attraction between negatively charged C3N4 (−21.8 mV) and positively charged UiO-66 (+ 31.7 mV), promoting a stable composite formation, and demonstrating their spontaneous electrostatic self-assembly.14


image file: d5cc04517g-f1.tif
Fig. 1 (a) XRD patterns, (b) FT-IR spectra, and (c) zeta potential values of C3N4/UiO-66, UiO-66 and C3N4. (d) C 1s, (e) N 1s and (f) Zr 3d regions of the XPS spectrum of C3N4/UiO-66.

X-ray photoelectron spectroscopy (XPS) analysis further confirmed the formation of a strong electronic interface between C3N4 and UiO-66. Compare to the C 1s region of the spectrum (Fig. 1d and Fig. S4a and S5a), the composite yielded an intensified peak at 288.22 eV, attributed to C–N–Zr bonding, along with a shift in the C–N bond energy (286.49 eV), indicating interfacial charge redistribution. The N 1s region of the spectrum of the composite revealed an increased binding energy for N–H (400.31 eV) and decreased binding energy for C[double bond, length as m-dash]N–C (398.68 eV) compared to those of pure C3N4, as shown in Fig. 1e and Fig. S4b and S5b, suggesting coordination between nitrogen atoms and Zr–O clusters.28,29 These changes, together with the preserved pyrrole-N peak (401.35 eV), confirmed the structural integrity of the C3N4 framework and a modified electronic environment.30 Compare to the Zr 3d region of the spectrum of the composite (Fig. 1f and Fig. S4c and S5c), a slight downshift in Zr 3d5/2 (182.78 eV) and upshift in Zr 3d3/2 (185.24 eV) were observed, and further indicated electronic interactions at the interface, leading to increased electron density around Zr sites.31,32 These observations highlight the formation of a well-defined metal–semiconductor interface, which facilitates charge separation and enhances piezocatalytic activity.33

The piezocatalytic performance of the C3N4/UiO-66 composite showed a significant enhancement in H2O2 generation efficiency, demonstrating a production rate substantially surpassing those observed for the individual C3N4 and UiO-66 components under identical test conditions (Fig. 2a). As shown in Fig. 2b and c, the composite demonstrated remarkable stability, sustaining continuous operation over 6 h without significant activity loss and retaining over 90% of its initial performance after six cycles. Furthermore, the composite maintained good H2O2-generation capability in real water matrices such as tap water, seawater, river water, and rainwater, with only slight reductions in yield compared to pure water (Fig. 2d), primarily due to the presence of background organic and inorganic constituents that may have scavenged radicals or competed for active sites, highlighting its potential for practical applications. Mechanistic studies indicated the enhanced performance to be due to improved O2 activation and interfacial charge dynamics. The obtained O2 temperature-programmed desorption (O2-TPD) results (Fig. 2e) revealed a significantly higher capacity of the composite than of the components to adsorb oxygen, while piezoresponse force microscopy (PFM) yielded a pronounced butterfly-shaped amplitude loop with a peak amplitude of 182.04 pm (Fig. 2f), confirming strong piezoelectric activity. Electrochemical impedance spectroscopy showed the composite having displayed the lowest charge-transfer resistance (Fig. 2g),34 and piezoelectric current measurements indicated it to have the highest response (Fig. 2h) among all the samples.35 Linear sweep voltammetry (LSV) further demonstrated a strong current response in the 0.7–1 V range (Fig. 2i). Consistent with these results, the open-circuit voltage (OCV) of C3N4/UiO-66 (0.347 V) was significantly higher than those of the individual components (0.112 and 0.166 V) (Fig. S6), confirming a stronger charge-separation driving force. To further evaluate the performances of the three materials, their IEF strengths were quantified using the Gouy–Chapman formula (Eqn. S1–S5).36 The quantitative analysis demonstrated an IEF strength 1.17-times higher for the C3N4/UiO-66 composite than for C3N4 (Fig. S7)—with the strong IEF enhancing charge separation, as further evidenced by the poor performance of physically mixed samples (Fig. S8). These findings collectively confirmed that interface engineering can significantly enhance charge separation and transport, enabling efficient piezocatalytic H2O2 generation.


image file: d5cc04517g-f2.tif
Fig. 2 (a) Curves for piezoelectric H2O2 production in the presence of, respectively, C3N4/UiO-66, UiO-66 and C3N4. Experimental conditions: catalyst (0.1 g L−1) under ultrasound (Us), T = 25 °C. (b) Piezoelectric H2O2 production for 6 h. (c) and (d) H2O2 production in the presence of C3N4/UiO-66 (c) recycled every hour and (d) in different real water samples under Us. (e) Curves for O2-TPD of C3N4/UiO-66, UiO-66 and C3N4. (f) Phase hysteresis loop and amplitude butterfly loop when using C3N4/UiO-66. (g) Nyquist plots with the fitted equivalent circuit based on EIS simulation. (h) Transient current density time curves over time under periodic Us signals and (i) LSV for C3N4/UiO-66, UiO-66 and C3N4.

Electron paramagnetic resonance (EPR) spectroscopy was employed to investigate the surface electronic states of the catalysts. As shown in Fig. 3a, all samples exhibited a Lorentzian signal centered at g = 2.003, corresponding to unpaired, non-localized electrons in the heptazine ring structure of C3N4.37 Notably, the C3N4/UiO-66 composite showed a stronger signal intensity, which was not simply the sum of the individual contributions from C3N4 and UiO-66, indicating a higher content of localized unpaired electrons. This enhancement was attributed to interfacial ion-exchange interactions that promoted charge separation, thereby increasing the population of unpaired electrons and enhancing catalytic activity.


image file: d5cc04517g-f3.tif
Fig. 3 (a) Plots of EPR intensity versus g-factor. (b) Piezoelectric H2O2 generation under different atmospheres. (c) Values of piezocatalytic H2O2 production at 60 min when including indicated scavengers (p-BQ for *O2, TBA for ˙OH, NaOI3 for e, EDTA-2Na for h+). (d) and (e) Plots of EPR intensity versus G for the detection of (d) DMPO–*O2 and (e) DMPO-˙OH, each in the presence of C3N4/UiO-66, UiO-66 and C3N4, respectively.

A predominantly ORR mechanism for the function of C3N4/UiO-66 was further supported the higher yield of H2O2 in the presence of O2 and a significant decrease in H2O2 production in Ar (Fig. 3b).38 To elucidate the reactive species involved, sacrificial agent experiments were conducted.39 As shown in Fig. 3c, the addition of p-benzoquinone (p-BQ), a scavenger for superoxide radicals (*O2), led to a 94% decrease in H2O2 production, indicating *O2 to be the primary active species. The introduction of tert-butanol (TBA), a scavenger for hydroxyl radicals (˙OH), resulted in a 36.1% decrease, suggesting ˙OH to be a secondary contributor. Furthermore, introduction of sodium iodate (NaIO3), an electron scavenger, reduced the yield by 45.8%, whereas introducing the hole scavenger EDTA-2Na caused only a 7% reduction. These findings confirmed that H2O2 production proceeded predominantly via a 2e ORR pathway, with additional contributions from 2e and 4e WOR processes. EPR measurements using spin-trapping agents further validated the generation of *O2 and ˙OH radicals (Fig. 3d and e). The C3N4/UiO-66 composite exhibited stronger *O2 signals than did the individual components, highlighting its superior ability to activate O2 and produce reactive intermediates. These results were found to be consistent with those from atmospheric control and quenching experiments, collectively confirming that the enhanced piezocatalytic H2O2 production arose from efficient interfacial charge separation and a predominant *O2-driven ORR pathway.38,40

Based on the previous discussions, a plausible piezoelectric catalytic mechanism for the C3N4/UiO-66 composites was derived, and is outlined in Fig. 4. The C3N4/UiO-66 composite material was concluded to generate H2O2 through a piezoelectric-field-driven dual pathway.41 Under mechanical stress, such as ultrasound, the piezoelectric field generated by the piezoelectric material C3N4 interacts with the internal electric field at the interface, creating a coupled enhancement effect: the piezoelectric field drives the efficient separation of electron–hole pairs, with electrons (e) migrating directly to the Zr active sites of UiO-66 under the guidance of the IEF, generating H2O2 through the 2e ORR pathway; and holes (h+) accumulate on the C3N4 surface under the dual electric field, producing ˙OH through the WOR pathway, with ˙OH then indirectly converted into H2O2 through radical coupling. This synergistic effect not only continuously provides a driving force through the piezoelectric field to overcome charge recombination but also precisely regulates the spatial distribution of e/h+via the IEF, enabling the ORR and WOR pathways to proceed efficiently in parallel, ultimately achieving a significant increase in H2O2 yield.


image file: d5cc04517g-f4.tif
Fig. 4 Proposed reaction mechanism of H2O2 production piezocatalyzed by C3N4/UiO-66.

In summary, we successfully developed a C3N4/UiO-66 composite via electrostatic self-assembly, which exhibited a significantly enhanced IEF that promoted efficient piezocatalytic production of H2O2. The optimized composite achieved an outstanding H2O2-generation rate under ambient conditions, superior to those of C3N4 and UiO-66. The excellent performance was attributed to the strong IEF at the C3N4/UiO-66 interface, which promotes directional charge separation and facilitates carrier transport. Mechanistic studies revealed the engineered IEF not only facilitating effective charge separation but also simultaneously promoting both ORR and WOR pathways, as evidenced by EPR detection of *O2 and ˙OH radicals. This work presents a promising strategy for designing advanced piezocatalytic systems through interfacial engineering, paving the way for sustainable chemical synthesis using mechanical energy.

J. Y.: validation, investigation, writing – original draft. H. C.: formal analysis, methodology. J. L.: investigation, methodology. L.G.: writing – review & editing, supervision. Z. L.: conceptualization, writing – review & editing, supervision. M. Z.: resources, funding, writing – review & editing, supervision.

This work has been supported by the Science and Technology Program of Guangzhou (2024A04J6256). We are also grateful for the TEM and other technical support provided by Dr Xiang Yu of the Analytical and Testing Center of Jinan University.

Conflicts of interest

There are no conflicts to declare.

Data availability

The data supporting this article have been included as part of the supplementary information (SI). The experimental methods and characterisation data (TEM and XPS) supporting this article have been included in the SI. See DOI: https://doi.org/10.1039/d5cc04517g.

Notes and references

  1. C. Xia, J. Y. Kim and H. Wang, Nat. Catal., 2020, 3, 605–607 CrossRef CAS .
  2. J. M. Campos-Martin, G. Blanco-Brieva and J. L. Fierro, Angew. Chem., Int. Ed., 2006, 45, 6962–6984 CrossRef CAS PubMed .
  3. R. J. Lewis and G. J. Hutchings, ChemCatChem, 2019, 11, 298–308 CrossRef CAS .
  4. L. Zhao, M. Xu, S. Yang, Z. Zhu, J. Qi and F. Meng, ACS Sustainable Chem. Eng., 2025, 13, 8853–8869 CrossRef CAS .
  5. W. Qi, Y. Fu, E. Liu, Z. Cheng, Y. Sun, S. Liu and M. Yang, EES Catal., 2024, 2, 884–910 RSC .
  6. Y. Chen, S. Lan and M. Zhu, Chin. Chem. Lett., 2021, 32, 2052–2056 CrossRef CAS .
  7. Z. Li, S. Lan and M. Zhu, Environ. Sci. Ecotechnol., 2024, 18, 100329 CrossRef CAS PubMed .
  8. Y. Zhang, Y. Lin, R. Li, Z. Chen, D. Zeng, S. Chen, W. Wang, L. Zhang, W. Wang and H. Nie, Chem. Eng. J., 2023, 465, 143043 CrossRef CAS .
  9. M. Zhang, W. Guo, Y. Chen, D. He, A. B. Isaev and M. Zhu, Chin. Chem. Lett., 2023, 34, 108229 CrossRef CAS .
  10. G. Li, Q. Zhong, W. Wu, Y. Liu, H. Li, X. Li and T. Long, J. Colloid Interface Sci., 2025, 700, 138431 CrossRef CAS PubMed .
  11. J. Yang, M. Zhang, M. Chen, Y. Zhou and M. Zhu, Adv. Mater., 2023, 35, 2209885 CrossRef CAS .
  12. J. Xu, H. Che, C. Tang, B. Liu and Y. Ao, Adv. Mater., 2024, 36, 2404539 CrossRef CAS PubMed .
  13. L. Chen, J. T. Ren and Z. Y. Yuan, Adv. Energy Mater., 2023, 13, 220372 Search PubMed .
  14. Y. Zhang, J. Qiu, B. Zhu, M. Fedin, B. Cheng, J. Yu and L. Zhang, Chem. Eng. J., 2022, 444, 136584 CrossRef CAS .
  15. K. Wang, Z. Shu, J. Zhou, Z. Zhao, Y. Wen and S. Sun, J. Colloid Interface Sci., 2023, 648, 242–250 CrossRef CAS PubMed .
  16. K. Wang, D. Shao, L. Zhang, Y. Zhou, H. Wang and W. Wang, J. Mater. Chem. A, 2019, 7, 20383–20389 RSC .
  17. D. Li, Q. Wen, C. Gao, Y. Zhang, H. Zhu, J. Dang, F. Song and J. Zhou, Small, 2025, 21, 2500797 CrossRef CAS PubMed .
  18. H. Lv, Z. Li, P. Yin, P. Wan and M. Zhu, Chin. Chem. Lett., 2025, 36, 110457 CrossRef CAS .
  19. J. Chen, N. Kang, J. Fan, C. Lu and K. Lv, Mater. Today Chem., 2022, 26, 101028 CrossRef CAS .
  20. L. Tang, D. Zhou, Q. Chen and M. Zhu, Surf. Interfaces, 2025, 62, 106269 CrossRef CAS .
  21. Z. Li, Y. Zhou, Y. Zhou, K. Wang, Y. Yun, S. Chen, W. Jiao, L. Chen, B. Zou and M. Zhu, Nat. Commun., 2023, 14, 5742 CrossRef CAS PubMed .
  22. Z. Yu, D. Wang, T. Zheng, A. Zavabeti, Y. Wang, C. Wu, J. Yang, Y. Guo, P. A. Webley and G. K. Li, J. Mater. Chem. A, 2025, 13, 8368–8374 RSC .
  23. Y. Wang, P. Su, Z. Lin, X. Li, K. Chen, T. Ye, Y. Li, Y. Zou and W. Wang, Adv. Mater., 2025, 37, 2418207 CrossRef CAS PubMed .
  24. J. He, Z. Yi, Q. Chen, Z. Li, J. Hu and M. Zhu, Chem. Commun., 2022, 58, 10723–10726 RSC .
  25. Y. Li, Z. Li, X. Lin, H. Lv and M. Zhu, Chem. Commun., 2023, 59, 5749–5752 RSC .
  26. W. Wang, S. Song, P. Wang, M. He, Z. Fang, X. Yuan, H. Li, C. Li, X. Wang and Y. Wei, ACS Catal., 2023, 13, 4597–4610 CrossRef CAS .
  27. X.-H. Yi, S.-Q. Ma, X.-D. Du, C. Zhao, H. Fu, P. Wang and C.-C. Wang, Chem. Eng. J., 2019, 375, 121944 CrossRef CAS .
  28. H. Wang, E. Almatrafi, Z. Wang, Y. Yang, T. Xiong, H. Yu, H. Qin, H. Yang, Y. He and C. Zhou, J. Colloid Interface Sci., 2022, 608, 1051–1063 CrossRef CAS PubMed .
  29. Y. Wang, L. Guo, Y. Zeng, H. Guo, S. Wan, M. Ou, S. Zhang and Q. Zhong, ACS Appl. Mater. Interfaces, 2019, 11, 30673–30681 CrossRef CAS .
  30. R. Wang, L. Gu, J. Zhou, X. Liu, F. Teng, C. Li, Y. Shen and Y. Yuan, Adv. Mater. Interfaces, 2015, 2, 1500037 CrossRef .
  31. X. Zhang, Y. Yang, W. Huang, Y. Yang, Y. Wang, C. He, N. Liu, M. Wu and L. Tang, Mater. Res. Bull., 2018, 99, 349–358 CrossRef CAS .
  32. F. Yu, L. Chen, X. Shen, X. Li and C. Duan, APL Mater., 2019, 7, 101101 CrossRef .
  33. X. Lu, Y. Shi, D. Tang, X. Lu, Z. Wang, N. Sakai, Y. Ebina, T. Taniguchi, R. Ma and T. Sasaki, ACS Nano, 2022, 16, 4775–4785 CrossRef CAS PubMed .
  34. S. Wang, F. Chen, Z. Li, H. Tao, L. Qu, J. Li, M. Zhu and Q. Zha, Surf. Interfaces, 2023, 39, 102910 CrossRef CAS .
  35. T. Jia, L. Wang, Z. Zhu, B. Zhu, Y. Zhou, G. Zhu, M. Zhu and H. Tao, Chin. Chem. Lett., 2024, 35, 108692 CrossRef CAS .
  36. J. Ke, J. Liu, H. Sun, H. Zhang, X. Duan, P. Liang, X. Li, M. O. Tade, S. Liu and S. Wang, Appl. Catal., B, 2017, 200, 47–55 CrossRef CAS .
  37. Z. Li, H. Lv, K. Tong, Y. He, C. Zhai, Y. Yun and M. Zhu, Appl. Catal., B, 2024, 345, 123690 CrossRef CAS .
  38. M. Song, W. Liu, J. Zhang, C. Zhang, X. Huang and D. Wang, Adv. Funct. Mater., 2023, 33, 2212087 CrossRef CAS .
  39. Y. Zhang, C. Pan, J. Li and Y. Zhu, Acc. Mater. Res., 2023, 5, 76–88 CrossRef .
  40. C. Chen, K. Gu, P. Wang, Z. Q. Liu and Y. Ao, Angew. Chem., Int. Ed., 2025, 64, e202425656 CrossRef CAS PubMed .
  41. H. Chen, S. Gao, G. Huang, Q. Chen, Y. Gao and J. Bi, Appl. Catal., B, 2024, 343, 123545 CrossRef CAS .

This journal is © The Royal Society of Chemistry 2025
Click here to see how this site uses Cookies. View our privacy policy here.