## Introduction

Electrocatalytic carbon dioxide reduction reaction (CO2RR), coupled to renewable energies, offers sustainable opportunities towards the production of value-added chemicals and carbon-based fuels1,2. Specifically, the electrochemical reduction of CO2 to C1 products (i.e., formic acid and CO) is of high relevance for the chemical industry3,4,5, which can also yield a mixture of CO as carbon-reduced product and H2 as byproduct. This so-called syngas mixture with varying molar ratios of H2/CO is commonly used as precursor for hydroformylation process (H2:CO = 1:1), methanol synthesis of Fischer−Tropsch process (H2:CO = 2:1) and methanation process (H2:CO = 3:1) to produce high-value/energy-dense hydrocarbons/alcohols5,6. However, the CO2-to-CO conversion, involving the transfer of two electrons and two protons, typically suffers from high kinetic barriers and low selectivity due to the high thermodynamic/kinetic stability of CO2 and the competing hydrogen evolution reaction (HER) in aqueous media, respectively7,8. Recently, great efforts have been dedicated to explore numerous electrocatalysts for catalytic CO2RR to CO, including noble metals (Au, Pd, Ag), transitional-metal-based materials (Fe, Co, Ni, Cu, Zn) and heteroatom-doped porous carbons2,7,9,10,11,12,13,14,15,16,17. Nevertheless, these single site catalysts still fail to meet the requirement of electrochemical syngas synthesis with tunable H2/CO ratio (from 1:1 to 3:1 or higher) at relatively low overpotential. Therefore, the development of electrocatalysts with high activity and selectivity that enables tuning the competitive reactivity between the CO2RR and HER at room temperature is imperative.

Metal-organic frameworks (MOFs) are one class of highly ordered crystalline coordination polymers, which are emerging as highly attractive catalytic systems due to the uniquely combining homogenous and heterogeneous features: First, the incorporation of well-defined and highly active sites into a defined and stable scaffold ensures excellent catalytic activity and selectivity; second, the porous metrics allow for sufficient and controllable mass transfer to and from the embedded active sites; finally, the molecularly defined catalytic environment around the active site allows for tuning the catalytic reaction by modifying the scaffold and facilitates deriving fundamental understanding of catalytic mechanism. For example, Co-PMOF and Al2(OH)2TCPP-Co MOFs have been developed for electrocatalytic CO2RR to CO with high selectivity (>70%)8,13,18. However, conventional MOFs suffer from certain drawbacks including their intrinsically low conductivity (electrical insulators) and the blockage of metal centers by organic ligands, which have greatly hampered their development for promoting CO2RR. Recent researches have demonstrated that layered 2D conjugated MOFs (2D c-MOFs)19,20,21,22,23 with fully in-plane π-delocalization along 2D directions and weak out-plane ππ stacking exhibit higher density of exposed metal centers and improved electron conductivity (up to 2500 S cm−1)24 apart from the inherited features of traditional MOFs, suggesting a great potential in high-performance electrocatalysis. For instance, the reported THT-Ni (THT = triphenylenehexathiol)25 and THT-Co26 2D c-MOFs with Ni(Co)S4 active sites afford superior HER electrocatalytic activity; Ni3(hexaiminotriphenylene)2 2D c-MOF with NiN4 active sites27 and phthalocyanine (Pc)-based 2D c-MOF with CoO4 active sites28 can efficiently catalyze oxygen reduction reaction with onset potential of 0.82 V and half-wave potential of 0.83 V vs. RHE (reversible hydrogen electrode) in alkaline media, respectively. Inspired by these successes, we anticipate that 2D c-MOFs should also act as promising electrocatalysts in enhancing CO2RR even though the related reports are rather limited29. Furthermore, the competitive reactivity between the CO2RR and HER can be presumably tuned by tailoring the structures and compositions of 2D c-MOFs. Therefore, as a proof-of-concept based on the above structural/property advantages, we rationally designed layered 2D c-MOFs with bimetallic centers to improve electrocatalytic CO2RR activity toward syngas synthesis; hereby one metal center will show high selectivity for CO2-to-CO conversion while the other metal center will be utilized for H2 generation due to its low binding energy of CO and high proton generation rate.

Herein, a 2D c-MOF electrocatalyst with bimetallic centers is synthesized by solvothermal approach for electrocatalytic CO2RR. This 2D c-MOF consists of phthalocyaninato copper as the ligand and zinc-bis(dihydroxy) complex (ZnO4) as the linkage, named as (PcCu-O8-Zn). The electrochemical measurements indicate that PcCu-O8-Zn exhibits highly selective catalytic activity for CO2-to-CO conversion (88%) and high turnover frequency (TOF) of 0.39 s−1 at −0.7 V vs. RHE and excellent stability. Syngas compositions with different molar H2/CO ratio (from 1:7 to 4:1) can be tuned via varying the metal centers (Cu and Zn) of ligand/linkage as well as applied potentials. Operando X-ray absorption spectroscopy (XAS) and surface-enhanced infrared absorption (SEIRA) spectroelectrochemistry are utilized to probe the catalytic sites and the reaction process. The spectroscopic studies combined with contrast experiments and density functional theory (DFT) calculation reveal that ZnO4 complexes in the linkages of PcCu-O8-Zn exhibit high catalytic activity for CO2-to-CO conversion, while CuN4 complexes in the Pc macrocycles act as the synergetic component to promote the protonation process and hydrogen generation along with the CO2RR. Thus, the bimetallic active sites contribute to a synergistic effect on the CO2RR. Our work highlights the bimetallic MOF electrocatalyst for highly selective CO2RR.

## Results

### Material design and reaction energetics

Density functional theory calculations were firstly employed to optimize the electrocatalyst design by simulating the reaction energetics of CO2RR and the competing HER on Pc-based 2D c-MOFs (PcM-O8-M1, M=Cu or Zn, M1=Cu or Zn) (Fig. 1 and Supplementary Figs. 14 and Tables 17). Typically, the electrochemical CO2-to-CO reduction steps include the first proton-coupled electron transfer to generate a carboxyl intermediate (*COOH), and subsequently the second charge transfer (one electron and one proton) for the formation of *CO intermediate, as well as the desorption of CO for the final CO product (Eqs. 1–3 in Supplementary Methods)30,31. On the other hand, HER goes through a proton (*H) intermediate. The results of calculations reveal that the formation of *COOH via protonation is the rate-limiting step for PcM-O8-M1 (Fig. 1a, c and Supplementary Figs. 3, 4). The calculated binding energy values of the intermediates (*COOH) and *H on PcM-O8-M1 manifest a stronger interaction of *COOH intermediate and a weaker interplay of *H with the linkages (M1O4 complexes) as compared with those of the phthalocyanine macrocycles (MN4 complexes, Supplementary Tables 25). It is thus proposed that M1O4 and MN4 complexes serve as the catalytic sites for CO2RR and HER, respectively. On the other hand, in the CO2RR process, the ZnO4 complexes of PcCu-O8-Zn display the lowest Gibbs free energy for *COOH formation and the lowest overpotential compared to other M1O4 complexes in PcM-O8-M1 (Fig. 1a, c and Supplementary Figs. 3, 4 and Supplementary Table 6), suggesting that the electrochemical CO2RR to CO is energetically preferred for PcCu-O8-Zn. In addition, the overpotential for CO2RR at M1O4 (Supplementary Table 6) has been found to be influenced by different MN4 complexes in the Pc ligand. For example, the overpotential of PcCu-O8-Zn is lower than that of PcZn-O8-Zn (while PcCu-O8-Cu < PcZn-O8-Cu), which reveals the important role of the Pc metal centers on promoting electrocatalytic CO2RR. To achieve more insight into the role of Pc metal centers, we further compare the free energy profiles of HER on MN4 and M1O4 complexes, which show that CuN4 complex in PcCu-O8-Zn exhibits the lowest HER energy barrier and the fastest proton/electron transfer kinetics among the different metal centers (Fig. 1b, d, Supplementary Table 7)32,33. Based on the above consideration, it is inferred that the presence of CuN4 complexes in the PcCu-O8-Zn MOF facilitates the protonation of adsorbed *CO2 on ZnO4 complexes, and thus accelerates the overall CO2RR kinetics. Therefore, a synergistic effect between CuN4 complexes and ZnO4 complexes is proposed for bimetallic MOF electrocatalysts.

### Synthesis and characterization

Inspired by the above theoretical calculation, PcCu-O8-Zn MOF comprising of 2,3,9,10,16,17,23,24-octahydroxy phthalocyaninato copper monomer linked by square planar ZnO4 linkages (Fig. 2a) was synthesized via solvothermal method (Supplementary Figs. 57), as confirmed by Fourier-transform IR (FT-IR) spectroscopy and powder X-ray diffraction (XRD) measurements. The disappearance of the ligand OH signals (3300 and 630 cm−1) and the peak shift from 1288 cm−1 (C-OH) to 1270 cm−1 (C-O-Zn) in the FT-IR spectra (Supplementary Fig. 8) demonstrate the successful coordination of O to Zn atoms34. The XRD pattern (Fig. 2b) shows intense peaks at 5.0°, 7.1° and 10.1°, assignable to (100), (110) and (200) plane, respectively, which indicates the long-range order within the ab plane35. The broad peak at 27.3° originates from the weak long-range stacking along the c direction with a layer distance of 0.33 nm, which is a typical feature of layered MOFs36. Compared to the calculated structures, the observed XRD pattern of PcCu-O8-Zn is in a good agreement with the AA staggered stacking geometry. Scanning electron microscopy (SEM, Supplementary Fig. 9) images indicate aggregated nanosheets in the resulting MOF samples. Transmission electron microscopy (TEM) images also present a mass of MOF nanosheets with an average size of 24 nm (Fig. 2c). The selected area electron diffraction pattern (SAED, inset image in Fig. 2c) and the high-resolution TEM (HR-TEM, Fig. 2d) images further manifest the crystalline structure of PcCu-O8-Zn based on a square lattice of 1.75 nm.

Element mapping images (Supplementary Fig. 10) disclose the homogenous distribution of Cu, Zn, C, N and O in the PcCu-O8-Zn sample. Furthermore, X-ray photoelectron spectroscopy (XPS) analysis also confirms the presence of Cu, Zn, C, N and O elements (Supplementary Fig. 11). In the high-resolution Cu 2p spectrum, the set of peaks at 936.7 and 953.8 eV is assigned to Cu 2p3/2 and Cu 2p1/2, respectively, which suggests one type of oxidized Cu (II) in the PcCu-O8-Zn37. The deconvolution of N1s spectra further verifies the coordination of Cu and N38. For the high-resolution scan of the Zn 2p region, the typical feature of Zn (II) is found39.

To further investigate the chemical state of the Cu and Zn atoms in the PcCu-O8-Zn sample, XAS and extended X-ray absorption fine structure (EXAFS) analyses were performed. The Cu K-edge X-ray absorption near-edge structure (XANES) spectra (Supplementary Fig. 12) show that both PcCu-O8-Zn and the monomer PcCu-(OH)8 exhibit a typical Cu(II) peak at 8985 eV (1s to 3d electron transition), which is similar to that of the reference copper(II) phthalocyanine (PcCu), thus confirming the presence of Cu-N in PcCu-O8-Zn40,41. Generally, two characteristic signals are observed in the Zn XANES spectra including the pre-edge peak at around 9660 eV and the main absorption peak at 9660−9680 eV, which correspond to the electron transition from 1s to 3d (typically found for the transition metal Zn) and the 1s to 4p electronic transition, respectively42. As shown in Fig. 2e, compared to Zn foil, the pre-edge peak signal at 9660 eV is not detected in the Zn K-edge spectrum of PcCu-O8-Zn due to the full occupied 3d orbital of Zn2+, therefore excluding the existence of Zn(0) in PcCu-O8-Zn. In addition, PcCu-O8-Zn also shows a main peak at 9665 eV similar to the ZnCO3 and ZnO (Fig. 2e), which suggests the oxidation valence of Zn atom as +2 in PcCu-O8-Zn42. Figure 2f displays the radial structure functions of PcCu-O8-Zn and clearly demonstrates the characteristic Zn-O coordination in PcCu-O8-Zn with intensive peak at around 1.55 Å. The absence of obvious structural peaks and the diminishment of the signal at 2.27 Å in Fig. 2f reveal that no heavy backscattering atoms (Zn) are bound to Zn sites in PcCu-O8-Zn43,44. Therefore, the XANES and EXAFS spectra of PcCu-O8-Zn together with the contrast experiments provide solid proof for the existence of square planar complexes via the coordination of PcCu(II)-(OH)8 to Zn(II) ions.

Low-pressure N2 sorption was measured to evaluate the porous properties of PcCu-O8-Zn (Supplementary Fig. 13). The Brunauer Emmett Teller surface area was measured to be 378 m2 g−1. The pore size distribution indicates its abundant micropores (1.4 nm) and mesopores (6 nm), which can be favorable for the mass transport during the catalytic process28.

### CO2RR activity evaluation

The electrocatalytic CO2RR activity of PcCu-O8-Zn was evaluated in a two-compartment electrochemical cell in 0.1 M KHCO3 aqueous electrolyte. The PcCu-O8-Zn/carbon nanotube (CNT) composite with a weight ratio of 2:1 (details provided in Methods section) was loaded on carbon paper, which was contacted as the working electrode. The contrast composite samples of 2D c-MOFs/CNT (PcZn-O8-Zn/CNT, PcZn-O8-Cu/CNT and PcCu-O8-Cu/CNT) were also synthesized (details in Supplementary Information, Supplementary Figs. 1417) and evaluated for electrocatalytic CO2RR activity. Cyclic voltammetry (CV) experiments revealed increased current densities for PcCu-O8-Zn/CNT in CO2-saturated media compared to Ar-saturated electrolyte (Supplementary Fig. 18), demonstrating its feasibility for CO2RR. To verify that the currents originate from the catalytic CO2RR, constant potential electrolysis was performed. The products were detected via gas chromatography (GC) and nuclear magnetic resonance (NMR) measurements. The results indicate that only gaseous (H2 and CO) products were generated at the applied potentials with total Faradaic efficiency of 99 ± 2.2% (Supplementary Figs. 1921). The resultant CO2RR catalytic performance including the maximum CO efficiency and the molar CO/H2 ratio suggested strong dependence on the type of metal centers and applied potential (Fig. 3a, b and Supplementary Fig. 20). Among the synthesized 2D c-MOFs/CNT hybrids, the PcCu-O8-Zn/CNT sample yielded the highest partial current density for CO (jCO) and the highest corresponding Faradic efficiency toward CO (FEco) over the investigated potential range (Fig. 3a, b), indicating superiority of the ZnO4 sites for selective conversion of CO2 to CO over ZnN4, CuN4 and CuO4 centers, which is also supported by the DFT calculations (Fig. 1). Notably, jCO for PcCu-O8-Zn/CNT showed a maximum value at −1.0 V vs. RHE, while H2 generation (jH2) displayed a steady rise with the increased overpotential (Supplementary Fig. 20a). This observation can be attributed to the competitive reactivity between the CO2RR and HER as well as the limitation of the transport of CO2 to the catalytic sites45. At −0.7 V vs. RHE, the FEco for PcCu-O8-Zn/CNT reached up to 88%, which is significantly higher than that of PcZn-O8-Zn/CNT (63%), PcZn-O8-Cu/CNT (6%), and PcCu-O8-Cu/CNT (10%) and the other reported Zn- and MOF-based electrocatalysts (up to ~80%, seen in Supplementary Table 8)13,18. Although CuN4 is more efficient for HER compared to ZnN4 based on theoretical calculations, PcCu-O8-Zn/CNT consisting of CuN4 and ZnO4 complexes still shows higher FEco than that of PcZn-O8-Zn/CNT comprising ZnN4 and ZnO4 complexes. This points to the synergistic catalytic effects between CuN4 and ZnO4 in selective electroreduction of CO2 to CO. In addition, PcCu-O8-Zn/CNT also shows a high TOF of 0.39 s−1, which is superior to other MOFs and Zn-related electrocatalysts (Supplementary Table 8). The molar ratio of the syngas CO/H2 catalytically generated by the 2D c-MOFs could be additionally controlled via the applied potentials. As shown in Fig. 3d, the molar H2/CO ratio for the PcCu-O8-Zn/CNT system could be tuned from around 1:7 to 4:1 by increasing the applied potential from −0.4 to −1.2 V vs. RHE.

To elucidate the kinetics of these MOFs toward the catalytic CO2RR, Tafel slopes were derived (Supplementary Fig. 22a). PcCu-O8-Zn/CNT exhibited the lowest Tafel slope (125 mV dec−1) toward the CO production compared to PcZn-O8-Zn/CNT (145 mV dec−1), PcZn-O8-Cu/CNT (223 mV dec−1) and PcCu-O8-Cu/CNT (280 mV dec−1), confirming its faster kinetics. Electrochemical impedance spectroscopy results indicate that PcCu-O8-Zn/CNT exhibits smaller resistance and faster electron kinetics than those of other as-synthesized 2D c-MOFs/CNT samples (Supplementary Fig. 22b). Besides, the PcCu-O8-Zn/CNT system presents long-term catalytic durability. The high FECO (86%) and current density were maintained over the course of 10 h of operation at −0.7 V vs. RHE (Fig. 3e). No obvious changes of morphology and structure (Supplementary Fig. 23) were observed in SEM image, XRD pattern, Raman and FR-IR spectra of PcCu-O8-Zn/CNT after the CO2RR long-term testing, demonstrating the high stability of PcCu-O8-Zn/CNT during electrocatalytic CO2 conversion.

### Unveiling the active sites

Operando XAS measurement was employed to gain insight into the valence state and coordination structure of Cu and Zn in the PcCu-O8-Zn/CNT under the CO2RR turnover condition (Fig. 4a–d and Supplementary Fig. 24). As shown in Fig. 4a, a typical pre-edge signal of Zn(0) at around 9660 eV is not observed in the Zn K-edge XANES spectra for all PcCu-O8-Zn/CNT samples42,43. This excludes the generation of metallic Zn in PcCu-O8-Zn/CNT electrocatalyst during the CO2RR process. Importantly, the main absorption peak at 9665 eV was not shifted in the Zn K-edge XANES spectra of PcCu-O8-Zn/CNT (Fig. 4a) as the applied potential was decreased to −0.4 (red circle dot curve) and −0.7 V (blue diamond dot curve) vs. RHE, respectively, and then increased back (indigo triangle dot curve) to the initial (black square dot curve) open circuit voltage (OCV). The results reveal that the oxidation state of Zn(II) in PcCu-O8-Zn/CNT was maintained throughout the catalytic process, which can be explained by the fact that the Zn(II) already has a full 3d electron shell46. In addition, the pre-edge peak at 8985 eV and the main absorption peak at 8998 eV in the Cu K-edge XANES spectra of PcCu-O8-Zn/CNT were not varied upon changing the applied potential, which indicates that the valence state of Cu(II) was not changed during the CO2RR process. Notably, the missing pre-edge peak at 8980 eV in Cu K-edge XANES spectra of all PcCu-O8-Zn/CNT samples further confirms that no metallic Cu was generated at the PcCu-O8-Zn/CNT electrode under electrolysis condition (Fig. 4b).

To monitor the local coordination environment changes, in situ EXAFS measurements were performend. As the applied potential was performed for one cycle, the peak at 1.55 Å assigned as Zn-O bond length in PcCu-O8-Zn/CNT was not shifted (Fig. 4c). Meanwhile, the peak intensity presents a negligible decrease (black square dot and indigo triangle dot curves in Fig. 4c), which is possibly due to the interaction of the reaction intermediates and the ZnO4 sites during the catalytic process, such as *H, *COOH, *CO and so on43. Therefore, the above in situ EXAFS results reveal no obvious change in Zn coordination number and bond length of Zn-O for PcCu-O8-Zn/CNT under the electrolysis condition. Furthermore, the characteristic signal of Zn−Zn bonding at 2.27 Å does not appear in the EXAFS spectra of all the PcCu-O8-Zn/CNT samples, again excluding the formation of metallic Zn or Zn cluster at PcCu-O8-Zn/CNT catalyst throughout CO2RR process. Regarding the CuN4 complexes, no obvious change of the Cu-N coordination peak at 1.54 Å was detected in the Cu K-edge EXAFS spectra of PcCu-O8-Zn/CNT (Fig. 4d) upon performing the potential in one cycle. Additionally, no obvious signal of Cu−Cu bonds was observed at 2.23 Å, which demonstrates that no heavy backscattering atoms (Cu) are bound to Cu sites in all PcCu-O8-Zn samples. Therefore, the operando XAS results fully prove that the well-defined sites (ZnO4 and CuN4) act as stable catalytic centers during the CO2RR process, while no metals or metal clusters form via the reduction of high-valence metal centers.

Next, operando SEIRA spectroelectrochemistry was employed to elucidate the electrocatalytic mechanism of the 2D c-MOF catalysts. The 2D c-MOFs were evenly deposited as a closed film onto a nanostructured Au surface, which acted as IR signal amplifier. SEIRA spectra were recorded at different potentials covering a broad potential window. SEIRA difference spectra taken under turnover conditions were derived using the spectrum of the respective system at −0.6 V vs. Ag/AgCl (Fig. 4e, f). The SEIRA difference spectra of PcZn-O8-Cu/CNT and PcCu-O8-Zn/CNT show distinct features that likely arise from their intrinsically different reactivities (Supplementary Fig. 25). Upon lowering the potential, a negative band at 2343 cm−1 assigned to dissolved CO2(g) was observed. This band was found to decrease with decreased potential indicating the consumption of CO2 near the surface in the catalytic process45. Strong positive bands in the region of 1660–1640 cm−1 were observed in both cases and attributed to the changes of the interfacial H2O, which accumulated in the MOFs due to catalysis or increasing negative polarization of the electrode. The high-frequency bands above 1800 cm−1 typically arise from metal bound species. Specifically, the bands located in the higher frequency region at 1933 and 2071 cm−1 were assigned to CO bound to the CuN4 and CuO4 centers, respectively (Fig. 4e, f)47. The shift of the ν(CO) mode could arise from the different electronic properties of Cu metal in the N4 and O4 frame, respectively. In this respect, CuN4 centers can stabilize the CO via π backbonding leading to drastically lowered ν(CO)s, while CO bound to Cu and oxide-derived Cu surfaces has been reported above 2000 cm−1,47,48. The strong band centered at 1851 cm−1 for the PcZn-O8-Cu/CNT system matches the frequency for (isolated) Cu-H and is thus assigned to the Cu-H intermediate formed at the CuO4 nodes in the HER cascade47,49. The particularly high intensity of this band suggests a dominating HER process over CO2RR at PcZn-O8-Cu/CNT in CO2-saturated solution. This interpretation is consistent with the electrocatalytic results (Supplementary Fig. 20), revealing that the PcZn-O8-Cu/CNT system shows high selectivity for H2 (>90%) over the complete potential range in CO2-saturated electrolyte. In contrast, Cu-H is not observed at the CuN4 units of the PcCu-O8-Zn/CNT systems. This may be due to low accumulation of the Cu-H species during catalysis, which could result from the fast proton transfer kinetics at CuN4 complexes to ZnO4 sites and yield H2. Interestingly, no indication for CO binding to the ZnO4 nodes was found due to its too low transient concentration to be observed with our current SEIRA spectro-electrochemical setup. This can be explained by the weak binding energy between ZnO4 and CO, which could facilitate a quick deliberation of the product and thus suggests fast CO2RR kinetics at the ZnO4 complexes in PcCu-O8-Zn/CNT.

## Discussion

To obtain further insight into the reactivity of 2D c-MOFs towards HER and CO2RR, the calculated free energy profiles on M1O4 site at U = 0.55 V were analyzed (Fig. 5a). For HER, the Gibbs free energy values of the key intermediates (*H) on M1O4 units are positive, with a minimum barrier of 0.7 eV, and therefore expected to be kinetically prohibited. However, the free energy values of CO2RR at the same equilibrium potential are negative, which reveals that the CO2RR at M1O4 site is thermodynamically downhill. It further verifies the favorable CO2RR process at M1O4 complexes of 2D c-MOFs. Although the CuN4 complexes show the lowest energy barriers for HER, PcCu-O8-Zn still exhibits the lowest free energy for the generation of rate-determining *COOH intermediate as compared to the other 2D c-MOFs during CO2RR catalysis. This establishes the synergetic effect of CuN4 and ZnO4 in enhancing the CO2RR activity. A proposed synergistic catalytic scheme is presented in Fig. 5b. CuN4 complexes attract numerous electrons and H2O toward producing abundant protons, wherein protons are partially transformed into molecular H2 and partially transferred to ZnO4 complexes. Simultaneously, the adsorbed CO2 on ZnO4 complexes is reduced to *COOH by coupling with these protons/electrons from the CuN4 sites and electrode/electrolyte, and subsequently the resultant *COOH will be transformed into *CO intermediate by a further charge transfer step (one electron and one proton). The desorption of *CO results in the final CO product. As a result, the kinetics of CO2RR on ZnO4 is greatly enhanced in PcCu-O8-Zn 2D c-MOF.

In summary, we have synthesized a layered 2D c-MOF (PcCu-O8-Zn) with bimetallic centers (ZnO4/CuN4) capable of synergistic electroreduction of CO2 to CO based on the theory-guided design. The electrocatalytic results indicated that PcCu-O8-Zn mixing with CNTs exhibited high CO2RR catalytic activity with high selectivity for CO conversion of 88%, TOF of 0.39 s−1 and long-term durability (>10 h), which is superior to the reported MOF- and Zn-based electrocatalysts. The molar H2/CO ratio could be rationally adjusted through varying the metal centers and applied catalytic potentials, beneficial for industrial applications. Theoretical calculation and the operando XAS and SEIRA analysis, as well as the control experiments suggested that the CO2RR takes place at the ZnO4 units while the CuN4 units promote the proton and electron transfer during the reaction process. Thus, the combination of ZnO4 and CuN4 complexes generates a synergetic effect, which contributes to the high CO2RR performance of PcCu-O8-Zn/CNT. Our work demonstrates the capability of bimetallic 2D c-MOFs as highly efficient electrocatalysts for promoting the CO2RR, which is of importance for conductive MOFs design and their electrocatalysis application and also sheds light on the development of high-performance bimetal-heteroatom doped carbon electrocatalysts.

## Methods

### Computational studies

The computational modeling of the reactants, intermediates and products, and reaction process involved in the reactions on 2D MOFs was performed by using DFT with the PBE exchange-correlation functional50, as implemented in the VASP code51,52. The total energies were converged within 10−6 eV/cell. The cut-off energy for plane wave basis was set at 500 eV. The Brillouin zone of the supercells was sampled using 4 × 4 × 1 Monkhorst–Pack grid of k-points. All calculations have been performed using the spin-polarized setup. Dispersion interactions were taken into account as proposed by Grimme within the DFT-D2 scheme53. More detail and relevant reference are provided in the Supplementary Information.

### Synthesis of PcCu-O8-Zn (Cu)

PcCu-(OH)8 (0.005 mmol) was well dispersed into DMF (N,N-Dimethyformamide, 25 ml). After adding 2.2 ml of NH3H2O (50%), the mixture solution was diluted by 30 ml of H2O. After sonication for 5 min, 5 ml of M(acac)2 (M=Cu, Zn, 0.01 mmol) solution was added into the above mixture. This mixture was transferred into the autoclave and heated at 120 °C for 40 h. Finally, the solid was obtained by filtration, washing with DMF, H2O and acetone, and vacuum drying at room temperature. PcM-O8-M1/CNT (M, M1=Cu or Zn) was synthesized with the similar procedure except that 15 mg of CNT was mixed with the PcCu-(OH)8 precursor, wherein the ratio of PcM-O8-M1 and CNT is around 2:1.

### Characterization

Powder XRD measurements were collected on a PW1820 powder diffractometer (Phillips) using Cu-Kα radiation (λ = 0.15418 nm, 40 kV, 30 mA). TEM images were obtained using a Cs-corrected TEM (Carl Zeiss Libra 200) operated at 200 kV. SEM was recorded on Zeiss Gemini S4 500. Raman spectra were collected with a Renishaw 2000 model confocal microscopy Raman spectrometer with a CCD detector and a holographic notch filter at ambient conditions. FT-IR tests were performed on a Bruker Optics ALPHA-E spectrometer equipped with Attenuated Total Reflectance (ATR) sample holder. The porosity was detected by nitrogen sorption using a micromeritics ASAP 2020 analyzer. XPS spectra were collected with an ESCALAB MK II X-ray photoelectron spectrometer using an Al Kα source. The rotating disk electrode (RDE) was performed on MSR electrode rotator (Pine Instrument Co.). The XAS and EXAFS data were collected at room temperature in transmission mode at beamline BL14W1 and BL15U1 of the Shanghai Synchrotron Radiation Facility (SSRF, China).

### Electrode preparation

One milligram of catalyst was added into 100 μl of ethanol containing 10 μl of Nafion solution (5% in ethanol) and ultrasonically treated for 30 min. And the catalyst ink was drop-casted onto carbon paper.

### Electrochemical test

Before testing, the Nafion membrane (115) was treated in H2O2 solution (5%) and pure water for 1 h. And the carbon paper with loading catalyst, Pt mesh and Ag/AgCl are used as the working, counter and reference electrode. Firstly, the electrolyte in the cathodic compartment was degassed by bubbling with Ar for at least 30 min for removal of oxygen, and then purged continuously with CO2. CO2 gas was delivered into the cathodic compartment at a rate of 30.00 sccm and was vented directly into the gas-sampling loop of a gas chromatograph. GC run was initiated every 20 min. All reference electrodes are converted to the RHE reference scale using E (vs. RHE) = E (vs. Ag/AgCl) + 0.197 V + 0.0591 V × pH.

The partial current densities of CO and H2 production were calculated from the GC peak areas as follows:

$$j_{{\mathrm{{CO}}}/{\mathrm{H}}_2} = v_{{\mathrm{{CO}}}/{\mathrm{H}}_2} \times {\mathrm{{flow}}}\;{\mathrm{{rate}}} \times \frac{{2FP_0}}{{RT}}A^{ - 1},$$
(1)

where VCO and VH2 are the volume concentration of CO and H2, respectively, P0 is the standard atmospheric pressure (1.013 bar), T is the absolute temperature (273.15 K), F is Faradaic constant (96,485 C mol−1), and A is the electrode area (1 cm2). Faradaic efficiencies for a given product were calculated by dividing these partial current densities by the total current density.

The liquid products were analyzed by NMR spectroscopy, in which 0.5 ml of the electrolyte was mixed with 0.1 ml D2O and 0.05 μl dimethyl sulfoxide (DMSO), wherein DMSO was serviced as an internal standard. The one-dimensional 1H spectrum was measured with water suppression using a pre-saturation method.

### Operando XAS measurement

Operando XANES and EXAFS experiments were carried out at the BL14W1 beamline of the Shanghai Synchrotron Radiation Facility (SSRF). All data were collected in fluorescence mode under applied potential controlled by CHI electrochemical workstation. A custom-designed cell (Supplementary Fig. 21) was used for the in situ XAS measurements, which was applied to the identical conditions as the real CO2RR testing. The X-ray energy was calibrated using a Cu metal foil and Zn metal foil.

### Operando SEIRA spectro-electrochemistry

All measurements were conducted in aqueous CO2 saturated 0.1 M KHCO3. An FT-IR spectrometer (Bruker IFSv66) equipped with a N2-cooled MCT detector was employed. The measurements were carried out in attenuated total reflection (ATR) mode in Kretschmann geometry using an Si prism as IR active waveguide. A thin and nano-scale rough Au layer was coated onto the prism for conductivity/contacting purposes prior to MOF deposition/drop-casting. Deposition of the Au film is described elsewhere54. MOF drop-casting followed procedures as described above. The Au layer acted as a signal amplifier giving rise to strong surface-enhancement of IR signals of compounds close to the Au surface. In this way, we achieve to record SEIRA spectra of the MOF layers close to the electrode surface, which should exhibit excellent electronic contact. For applying potentials, the MOF-coated prism was mounted into a customized three-electrode containing spectro-electrochemical cell as described elsewhere54. A hydrogen-flamed cleaned Pt wire and Ag/AgCl in 3 M KCl (DriRef, World Precision Instruments) acted as counter and reference electrode, respectively.