Manganese, nitrogen co-doped porous carbon with high-loading active sites as the oxygen reduction catalyst for Zn–air batteries

Hao Xu *a, Yuxuan Gao a, Ruopeng Li *b, Weiyan Sun a, Xiangyu Lu b, Jie Bai a and Peixia Yang b
aCollege of Chemical Engineering, Inner Mongolia University of Technology, Hohhot, 010051, China. E-mail: xuhao@imut.edu.cn
bMIIT Key Laboratory of Critical Materials Technology for New Energy Conversion and Storage, School of Chemistry and Chemical Engineering, Harbin Institute of Technology, Harbin, 150001, China. E-mail: liruopeng630@163.com

Received 9th June 2024 , Accepted 20th June 2024

First published on 21st June 2024


Abstract

Manganese–nitrogen–carbon (Mn–N–C) materials have been considered ideal catalysts for the oxygen reduction reaction (ORR). However, avoiding metal agglomeration during pyrolysis while ensuring the construction of Mn–Nx active centers is still difficult. Furthermore, the influence of pyrolysis temperature on structures of Mn–N–C is controversial, and needs an in-depth understanding. Herein, we prepare single atom Mn–N–C via a spatial confinement method. This is achieved through the pyrolysis of the ZIF precursor, where single Mn(acac)3 molecules are trapped within its cavities. Compared with 800 °C and 1000 °C, 900 °C is the optimal pyrolysis temperature for the synthesis of ZIF-derived Mn–N–C, which promotes the formation of the porous framework and dense Mn–Nx centers (27.47%). As a result, Mn–N–C-900 possesses an outstanding performance with a half-wave potential (E1/2) of 0.882 V in alkaline media. Impressively, the Zn–air battery using Mn–N–C-900 delivers a high peak power density of 84 mW cm−2.


Introduction

In order to achieve carbon neutrality goals and accelerate the development of an environment-friendly society, the next generation of clean energy devices, including Zn–air batteries (ZABs), has garnered significant attention because of low pollution features.1–12 However, the actual performance of ZABs is limited by the slow ORR kinetics.13–19 As benchmark catalysts for the ORR, Pt-based catalysts are costly and prone to instability, making them unsuitable for widespread commercial applications.20–23 Therefore, there is a pressing demand for the application of non-precious metal materials.24–28

Mn–N–C has emerged as a hopeful alternative to Pt/C.29,30 The atomically dispersed Mn–Nx site is recognized as the main active center, while the porous structure can enhance the accessibility of Mn–Nx centers.31,32 However, the manganese species in precursors are often aggregated into low-activity nanoparticles during pyrolysis, which hinders the construction of Mn–Nx centers.33 Moreover, the influence of pyrolysis temperature on the Mn–Nx center loading and pore framework of Mn–N–C catalysts is still unclear, and needs further study. Hence, exploiting a facile approach to achieve the controllable construction of single atom Mn–Nx sites and studying the correlation between pyrolysis temperature and the structure of catalysts are necessary for the development of Mn–N–C.

Herein, we report a spatial confinement method to prepare Mn–N–C by pyrolyzing the zeolitic imidazolate framework (ZIF) with single Mn(acac)3 molecules trapped within its cavities. The spatial confinement effect of ZIF-8 nanocavities on Mn(acac)3 molecules can avoid the appearance of manganese-based nanoparticles. Compared with 800 and 1000 °C, 900 °C is the optimal pyrolysis temperature for the synthesis of ZIF-derived Mn–N–C. The Mn–N–C-900 synthesized at 900 °C exhibits a more prominent porous structure and a higher loading of Mn–Nx active sites than those of reference samples. As a result, the optimized Mn–N–C-900 possesses outstanding activity and durability with an E1/2 of 0.882 V in an alkaline solution. Impressively, the solid-state ZAB utilizing Mn–N–C-900 reveals an eminent peak power density.

Experimental

Synthesis of the catalysts

Preparation of the ZIF-8@Mn(acac)3 precursor: in a typical procedure, solution A was obtained by dissolving 10 mg Mn(acac)3 and 576 mg Zn(NO3)2·6H2O in 20 mL CH3OH. Simultaneously, solution B was obtained by dissolving 4.5 g 2-methylimidazole (2-MeIM) in 80 mL CH3OH. Finally, solution A was rapidly combined with solution B, and the mixed solution was stirred at 23 °C for 24 h. The precipitate obtained was then washed 3 times with CH3OH and dried at 60 °C for twelve hours.

Preparation of Mn–N–C-900: ZIF-8@Mn(acac)3 was pyrolyzed at 900 °C in an Ar/H2 (95%:5%) atmosphere for 2 h at 5 °C min−1.

To reveal the influence of pyrolysis temperature on Mn–Nx loading and the pore structure, reference Mn–N–C-800 and Mn–N–C-1000 catalysts were prepared using a similar process to Mn–N–C-900, except for choosing 800 °C and 1000 °C as the pyrolysis temperature, respectively.

Physicochemical characterization

A scanning electron microscope (SEM, Zeiss) and transmission electron microscope (TEM, JEOL JEM 2100) were employed to study the morphology. The X-ray diffraction (XRD) patterns and Raman spectra were collected on a Bruker D8 and a HR800, respectively. X-ray photoelectron spectroscopy (XPS) and the N2 adsorption–desorption test were conducted on a Physical Electronics PHI model 5700 instrument and 3H–2000PS1 analyzer, respectively.

Electrochemical measurements

The mass loading of Mn–N–C and Pt/C on the working electrode was 0.459 and 0.255 mg cm−2, respectively. The preparation method of catalyst ink is provided in our previous reports.34

Solid state Zn–air battery test: Zn foil, PVA polymer and nickel foam coated with the catalyst (2 mg cm−2) were chosen as the anode, solid-state electrolyte and cathode, respectively. The preparation method of polyvinyl alcohol (PVA) electrolyte is provided in previous reports.34

Results and discussion

Structural characterization

The synthetic process of the ZIF-8@Mn(acac)3 precursor and its resulting Mn–N–C is exhibited in Scheme 1. Initially, the ZIF-8@Mn(acac)3 precursor is synthesized through the self-assembly of Zn2+, 2-MeIM, and Mn(acac)3 in a methanol solution. The spatial confinement effect of ZIF-8 nanocavities on Mn(acac)3 effectively prevents the aggregation of metal species during the pyrolysis process. After pyrolysis of precursors under H2/Ar at various temperatures (800, 900 and 1000 °C), Mn–N–C materials with different active center loadings and pore structures are synthesized. The final mass yield of Mn–N–C-900 is 0.0721 g (Fig. S1).
image file: d4se00771a-s1.tif
Scheme 1 Synthetic process of Mn–N–C-900.

The morphology of the ZIF-8@Mn(acac)3 precursor and the obtained Mn–N–C catalysts are detected by SEM images. As shown in Fig. 1a, ZIF-8@Mn(acac)3 presents a coral-like structure consisting of abundant nano-polyhedra. After the pyrolysis treatment, the surface of the obtained catalysts becomes rougher (Fig. 1b–d), which is due to the decomposition of nitrogen sources. As shown in TEM and HRTEM images, no nanoparticles are observed in Mn–N–C-900 catalysts (Fig. 1e–f), proving that the size of manganese species may be at the atomic level.


image file: d4se00771a-f1.tif
Fig. 1 SEM images of (a) the precursor and the obtained Mn–N–C at (b) 800 °C, (c) 900 °C and (d) 1000 °C; (e) TEM and (f) HRTEM images of Mn–N–C-900.

XRD is employed to detect the crystal structure of the catalysts (Fig. 2a). Two peaks corresponding to the C (002) and C (101) planes are detected in all samples.34 No diffraction peaks corresponding to crystalline manganese-based species are detected. The above results indicate that there is no significant metal agglomeration during the pyrolysis process, and the size of Mn species may be at the atomic level. Raman spectra are employed to investigate the influence of pyrolysis temperature on the graphitization degree of the catalysts. As shown in Fig. 2b, two peaks are observed in the synthesized samples, corresponding to the D-band (carbon defects) and G-band (graphitization), respectively.35,36 As the pyrolysis temperature increases from 800 °C to 1000 °C, the ID/IG values of Mn–N–C catalysts decrease gradually from 0.89 to 0.87. This trend indicates that high pyrolysis temperatures can increase the graphitization degree, thereby improving the conductivity of the catalysts. In addition, compared with the reference samples, Mn–N–C-900 possesses higher specific surface area (SBET, 1062 m2 g−1) and pore volume (Vpore, 0.158 cm3 g−1) (Fig. 2c–d), leading to enhanced accessibility of active sites within the catalyst.


image file: d4se00771a-f2.tif
Fig. 2 (a) XRD patterns; (b) Raman spectra; (c) N2 adsorption–desorption curves; and (d) SBET and Vpore.

The evaporation of Zn at 900 °C leads to the formation of a large number of micropores,37 so the obtained Mn–N–C-900 exhibits larger SBET and Vpore than those of Mn–N–C-800. Nevertheless, when the temperature is increased to 1000 °C, the pore structure of Mn–N–C-1000 undergoes significant collapse, resulting in poor SBET and Vpore. The above results indicate that 900 °C is the optimal pyrolysis temperature for the synthesis of ZIF-derived Mn–N–C, which is conducive to the construction of a porous structure and large specific surface area.

The influence of pyrolysis temperature on the chemical composition of Mn–N–C is verified by XPS. The C 1s spectra of the obtained catalysts exhibit three peaks, attributed to C–C (284.8 ± 0.3 eV), C–N (285.4 ± 0.3 eV) and C–O (286.5 ± 0.3 eV) (Fig. S3).15 The presence of a C–N bond proves the introduction of N species into the carbon substrate. In addition, there are three peaks in the Mn 2p spectrum of the Mn–N–C-900 catalyst at 641.6 ± 0.3, 653.6 ± 0.3 and 646.0 ± 0.3 eV, attributed to Mn 2p3/2 and Mn 2p1/2 and the satellite peak, respectively (Fig. S4).38 The N 1s spectra of the obtained Mn–N–C exhibit five nitrogen species, oxidized-N (402–405 eV), graphitic-N (401.5 ± 0.3 eV), pyrrole-N (400.7 ± 0.3 eV), Mn–N (399.3 ± 0.3 eV) and pyridinic-N (398.4 ± 0.3 eV) (Fig. 3a–c).15 Previous work has demonstrated the importance of pyridinic-N in capturing manganese atoms to construct the Mn–Nx site and enhancing the adsorption of O2 molecules on the catalysts.39 The relative content of pyridinic-N in Mn–N–C-900 (44.8%) is higher than that in Mn–N–C-800 (27.82%) and Mn–N–C-1000 (25.31%) (Fig. 3d and Table S1). Meanwhile, it is generally accepted that the atomically dispersed Mn–Nx site is the main active center. Compared with the reference samples, Mn–N–C-900 has a higher relative content of Mn–Nx sites (27.47%) (Fig. 3d and Table S1).


image file: d4se00771a-f3.tif
Fig. 3 (a–c) N 1s spectra of Mn–N–C catalysts. (d) The relative content of N species.

Obviously, as the temperature increases from 800 °C to 900 °C, more Mn–Nx and pyridinic-N are formed in catalysts. However, at an excessive temperature of 1000 °C, there is a notable decomposition of nitrogen species, resulting in a decrease in the relative content of Mn–Nx and pyridinic-N. The above results indicate that the optimal pyrolysis temperature for the synthesis of ZIF-derived Mn–N–C is 900 °C. 900 °C promotes the formation of pyridinic-N and Mn–Nx active sites, potentially leading to higher catalytic activity compared to reference catalysts. The following electrochemical tests strongly support the above viewpoint.

Oxygen reduction performance evaluation

The performance of Mn–N–C is assessed in 0.1 M KOH. The E1/2 of Mn–N–C-900 reaches 0.882 V (Fig. 4a), which is superior to that of reference Mn–N–C samples, confirming the satisfactory activity of Mn–N–C-900. Moreover, among the synthesized ZIF-derived materials, Mn–N–C-900 demonstrates the highest kinetic current density (Fig. 4b). Furthermore, Mn–N–C-900 possess the lowest Tafel slope of 19.21 mV dec−1, suggesting the outstanding reaction kinetics (Fig. 4c).18,20 On the other hand, the accelerated durability test is employed to assess the stability of Mn–N–C-900. The decay in E1/2 (only 3 mV) for Mn–N–C-900 is almost negligible after 5000 cycles (Fig. 4d). Obviously, the obtained Mn–N–C-900 possesses remarkable activity and stability, which is attributed to abundant Mn–Nx sites and a significant porous structure. 900 °C is the optimal pyrolysis temperature for the preparation of ZIF-derived Mn–N–C.
image file: d4se00771a-f4.tif
Fig. 4 ORR measurements in 0.1 M KOH: (a) LSV curves; (b) kinetic current density; (c) Tafel plots; and (d) results of the accelerated durability test.

Furthermore, we assemble and test the primary ZAB utilizing Mn–N–C-900. The detailed structure of the primary ZAB is shown in Fig. 5a. This study does not involve the installation and testing of rechargeable ZABs. As demonstrated in Fig. 5b, the open circuit voltage of a battery utilizing Mn–N–C-900 is found to be approximately 1.5 V. Additionally, the peak power density of the Mn–N–C-900-based battery (84 mW cm−2) is higher than that of Pt/C (Fig. 5c). Moreover, the Mn–N–C-900 based battery has the capability to power a timer successfully (Fig. 5d). Therefore, the ZABs using Mn–N–C-900 as catalysts exhibit great potential for practical application.


image file: d4se00771a-f5.tif
Fig. 5 (a) The structure of the solid-state ZAB. (b) Voltage-time curves. (c) Polarization curves. (d) Photograph of a timer powered by a solid-state battery using Mn–N–C-900.

Conclusions

In summary, our work utilizes the spatial confinement method to prepare the single atom Mn–N–C. This is achieved through the pyrolysis of the ZIF precursor, where single Mn(acac)3 molecules are trapped within its cavities. Benefiting from the porous structure and the high loading of Mn-Nx, the resulting Mn–N–C-900, synthesized at 900 °C, shows outstanding catalytic activity and stability with an E1/2 of 0.882 V in 0.1 M KOH, which surpasses those of the reference samples synthesized at 800 °C and 1000 °C. Furthermore, the peak power density of the ZAB utilizing Mn–N–C-900 can reach 84 mW cm−2. Our work provides insights into the synthesis of Mn–N–C, and revealing the impact of pyrolysis temperature on the structure of catalysts.

Data availability

The data supporting this article have been included as part of the ESI.

Author contributions

Hao Xu: data curation, writing – original draft; Yuxuan Gao: data curation, writing – original draft; Ruopeng Li: conceptualization, writing – review & editing; Weiyan Sun: investigation, software; Xiangyu Lu: writing – review & editing; Jie Bai: investigation, software; Peixia Yang: writing – review & editing.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work was supported by the Shiyanjia Lab (http://www.shiyanjia.com), (GZC20233449) Postdoctoral Fellowship Program of CPSF, (52163029) National Natural Science Foundation of China, and (LBH-Z23156) Postdoctoral Fellowship of Heilongjiang.

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Footnotes

Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4se00771a
These authors contributed equally to this work.

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