While carbon dioxide (CO
2) is the primary driver of anthropogenic climate change [
1], its role as a key C1 feedstock necessitates the capture and conversion of atmospheric CO
2 to value-added chemicals [
2–
4]. However, the inherent ultradilute atmospheric CO
2 concentration (~400 ppm) fundamentally limits the conversion efficiency [
1]. Carbon capture, utilization and storage (CCUS) technologies are critical to this effort [
5], with direct air capture (DAC) emerging as an essential negative emissions solution [
6–
9]. Among various conversion strategies, CO
2 photoreduction offers a promising solution with minimal carbon footprint and environmental compatibility
versus enzymatic, thermal, or electrochemical routes [
10–
12]. This challenge motivates the discovery of novel materials for integration of CO
2 DAC with photoreduction in one body for practical CCUS [
13].
Porous materials are pivotal to DAC advancement through their tunable structures and functionalities [
6,
7]. The porous material systems, including porous carbons [
14], zeolites [
15], metal-organic frameworks (MOFs) [
16–
24], covalent-organic frameworks (COFs) [
25,
26], and porous organic polymers (POPs) [
4,
8,
9], have been developed for integrated CO
2 capture-conversion [
2–
4]. Among them, the POPs exhibit exceptional structural diversity, featuring high surface areas, robust stability, tunable porosity, and facile functionalization [
27], establishing them as ideal atmospheric CO
2 capture platforms [
28]. Their customizable structures and pore environments further position POPs as scaffolds for integration of photocatalysts for CO
2 reduction [
29–
31]. To enhance CO
2 adsorption within POP materials, amine functionalization represents a key strategy where surface-grafted groups significantly boost CO
2 affinity [
32–
34]. The challenges in atmospheric CO
2 capture and conversion using POPs include [
2,
10,
35–
39]: (ⅰ) Intrinsically limited adsorption/conversion efficiency at ultradilute CO
2 concentrations due to poor interfacial contact; (ⅱ) Performance degradation from poor material stability hindering adsorption-conversion functionality; (ⅲ) System integration complexities involving adsorbent-catalyst coupling, CO
2 diffusion optimization, pore-blocking prevention, and incompatible operating conditions. Water-dispersible POPs, as an emerging class of porous materials [
39], offer exceptional aqueous dispersibility, robust structural stability, and facile postsynthetic modification, which may resolve the integration challenges of CO
2 capture and conversion.
Herein, we synthesized six novel water-dispersible POPs of POP-1~6 via polymerization of cyclen and tetrakis(4-(bromomethyl)phenyl)methane, followed by amine functionalization to enhance CO2 affinity. The POP-1~6 possessed excellent aqueous-phase dispersibility for efficient CO2 DAC, which can further integrate with an Fe-porphyrin catalyst (Fe-P) and Ru-photosensitizer for efficient atmospheric CO2 photoreduction to CO with a yield up to 93%. This work establishes a dual-function material platform for integrated atmospheric CO2 capture and photoreduction under ambient conditions.
The 1,4,7,10-tetraazacyclododecane (cyclen,
1) is one kind of microcyclic tetramine that can be used as an excellent node molecule for constructing POPs due to its inexpensiveness, good water solubility, and the amine groups of cyclen can potentially endow the POP with CO
2 adsorption properties [
40]. Aiming to achieve flexible adsorption due to the interaction of amine groups with CO
2 [
41], we employed
1 as an amine-based structural linker and tetrakis(4-(bromomethyl)phenyl)methane (
5) as a node molecule to synthesize the first cyclen-based
POP-1 (
Fig. 1, Figs. S1 and S2, and Method in Supporting information). As amine functionalization has been reported as an effective strategy to boost CO
2 affinity [
32–
34], we further introduced five selective primary and/or secondary amines to enhance the CO
2 adsorption capability. The
POP-2~6 were synthesized based on the post-modification of
POP-1 with a series of added amines (
Fig. 1 and Fig. S1). Specifically, we introduced cyclen to construct
POP-2,
N, N-di(2-aminoethyl)ethylenediamine (TETA) to construct
POP-3, polyamine N7 to construct
POP-4, PAMAM-G0 to construct
POP-5, and a cross-linked polymer derived from the polymerization reaction of PAMAM-G0 and 1,3-diiodopropane
in situ to construct
POP-6 (
Fig. 1 and Fig. S1). To the best of our knowledge, these are the first examples of construction of cyclen-based POPs, and the resulting
POP-1~6 exhibit excellent dispersibility in aqueous phase (Fig. S3 in Supporting information).
Fourier transform infrared (FT-IR) spectroscopy was executed to examine the chemical structure of
POP-1. As shown in Fig. S4 (Supporting information), no absorption band at 3327 and 3276 cm
−1 (N–H stretching vibration) manifests full conversion of secondary amine groups of
1. The absorption band at 1019 cm
−1 corresponding to C–N stretching vibration of tertiary amine group [
42] further confirmed the formation of the new C–N bond in
POP-1. Next, the absorption band at 2363 cm
−1 corresponding to N–H stretching vibration of tertiary ammonium salt (N
+-H) was also observed, while the absorption at ~1500 and 900 cm
−1 (C–N
+ stretching vibration) for quaternary ammonium salt was absent [
43–
45]. Consistently, solid-state
13C magic angle spinning nuclear magnetic resonance spectroscopy (
13C MAS NMR) of
POP-1 displayed a new peak assigned to the –CH
2– moieties at chemical shifts (δ) of 64.7 ppm, which further confirmed the formation of a new benzyl carbon (C–N) bond in
POP-1 (Fig. S11 in Supporting information) [
4,
46–
48]. The FTIR and
13C MAS NMR results confirmed the successful construction of
POP-1. Notably, a week absorption peak at 615 cm
−1 corresponding to C-Br stretching vibration in
POP-1 indicates that the residue of active benzyl bromide, which enables the post-modification with added amines (Fig. S4 in Supporting information). Next, elemental analysis was conducted to determine the residual amount of active benzyl bromide and the proportion of tertiary amine and tertiary ammonium salt in
POP-1 by ion exchange (Fig. S12 and Method in Supporting information). The result shows that
POP-1 contains 0.2% (mass fraction) of unreacted bromine residues (C-Br) and 11.8% (mass fraction) of ionic bond of bromine (Br
−), and the molar proportion of tertiary amine in
POP-1 is
ca. 74% and the cationic tertiary ammonium salts is
ca. 26% (Method in Supporting information). This cationic structure of
POP-1 enables the loading of anionic catalysts through electrostatic interaction [
49]. Nuclear magnetic resonance (NMR) spectroscopy was also used to analyze the structure of
POP-1 and polyamines post-modified POPs of
POP-2~6. Liquid-state
1H NMR spectroscopy showed only solvent peaks of POPs of
POP-1~6 (Figs. S5~S10 in Supporting information) due to their poor solubility, which is limited to structural verification of solid material, but
1H NMR further confirmed no starting materials and no depolymerization products of
1 and
5 existed in
POP-1 (Fig. S5) and no residual free amines from starting materials and no depolymerization products of
1 and
5 existed in POPs of
POP-2~6 (Figs. S6~10).
The predicted three-dimensional model of
POP-1 with ideally ordered structure suggests that the pore size is approximately 1.0 nm as calculated by Materials Studio 7.0 (
Fig. 1). Next, we performed the N
2 adsorption/desorption experiments to characterize the porosity of
POP-1. The N
2 sorption isotherms displayed steep gas uptake at low relative pressures (Fig. S13a in Supporting information) with an adsorption capacity of 67.8 mg/g. The Brunauer-Emmett-Teller (BET) surface area of
POP-1 was calculated to be 19.8 m
2/g. Pore size distribution (PSD) analysis revealed that the aperture distribution of
POP-1 is mostly at a range of 1–5 nm and contained both micropores (0.6–2 nm) and mesopores (2–35 nm) (Fig. S13b in Supporting information), the average pore width was calculated to be 1.8 nm with pore volume of 0.05 cm
3/g (Fig. S13). The hierarchical porous structure is expected to accelerate mass transport during CO
2 adsorption processes [
2,
4,
10]. The scanning electron microscopy (SEM) and transmission electron microscopy (TEM) images showed that
POP-1 has an irregular, cross-linked, sponge-like porous structure (
Fig. 2 and Fig. S14 in Supporting information). And the
POP-2~6 has the similar morphology as
POP-1 as revealed by TEM (Fig. S14 in Supporting information). Moreover, the scanning transmission electron microscopy (STEM) and energy dispersive X-ray (EDX) mapping analysis also certified the colocalization of C, N, and Br elements within of
POP-1~6 (
Fig. 2, Figs. S14 and S15 in Supporting information). Small-angle X-ray scattering (SAXS) profile indicated an amorphous morphology of
POP-1 (Fig. S16 in Supporting information). Thermal gravimetric analysis (TGA) suggested that
POP-1~6 exhibited high thermal endurance that maintained structural integrity below 200 ℃ under inert conditions (Fig. S17 in Supporting information).
We first studied the solid-phase CO
2 adsorption capacities of
POP-1~6 by collecting the CO
2 isothermals at 298 K. The solid-phase CO
2 adsorption capacities were determined to be 24.4, 31.2, 56.5, 71.4, 49.2, and 56.9 mg/g, respectively (
Fig. 3a, Fig. S18,
Table 1 and Table S1 in Supporting information). However, the CO
2 isothermals only reflect the adsorption capacity in solid phase; there is still a lack of methods to determine CO
2 adsorption capacity in solution [
27]. Given that the designed potential application of
POP-1~6 is to capture atmospheric CO
2 in aqueous phase, we developed a method to determine CO
2 adsorption capacity in water using gas chromatography (GC) (see Supporting information for details) [
50]. The capacities of CO
2 adsorption of
POP-1~6 were determined to be 263.9, 467.9, 527.2, 401.6, 505.1, and 569.1 mg/g, respectively (
Fig. 3a,
Table 1 and Table S1). We then explored the application of
POP-1~6 for CO
2 DAC by continuously pumping air into well-dispersed POPs in aqueous phase for 1–5 days. The CO
2 DAC capacities of
POP-1~6 over 5 days in aqueous phase were determined to be 10.8, 17.9, 19.5, 27.6, 34.3, and 48.5 mg g
−1 d
−1, respectively (
Fig. 3b,
Table 1, and Table S1). The significant difference in the ability of solid materials to adsorb CO
2 in air
versus in aqueous environments may primarily be attributed to the distinct roles of water molecules in the adsorption process. The fundamental cause lies in the inherent differences in the physical state, concentration, mass transfer kinetics, and adsorption or reaction mechanisms of CO
2 across different media. In air, adsorption involves the interaction between low-concentration gaseous CO
2 and solid materials; in contrast, in aqueous solutions, it entails the interaction between dissolved CO
2 species, including carbonic acid, bicarbonate, and carbonate ions, and the solid material within a hydrated environment [
51–
53]. The enhanced CO
2 adsorption capacities of
POP-2~6 compared to
POP-1 may be attributed to the successful post-modification of additional amines, which the activated amine sites at aperture would draw more CO
2 molecules into the pores [
54–
56]. The comparisons of CO
2 capture performance of
POP-1~6 with a range of benchmark materials are summarized in Tables S2 and S3 (Supporting information) [
57].
We then investigated the catalytic activity of
POP-1~
6 when integrated with catalysts by a series of photocatalytic experiments. The CO
2 photoreduction experiments were conducted using 5,10,15,20-tetrakis(4-sulfonatophenyl)porphyrin iron(III) chloride (
Fe-P) as a catalyst, Ru(bpy)
3Cl
2 as a photosensitizer, and TEOA as a sacrificial reagent in the POP system (
Fig. 4 and Fig. S19 and Table S4 in Supporting information for details). The
Fe-P and Ru(bpy)
3Cl
2 were integrated with
POP-1~
6 to achieve the photocatalytic CO
2 conversion. The density functional theory (DFT) calculations confirmed that the energy levels of the Ru(bpy)
3Cl
2 photosensitizer matched with those of the
Fe-P catalyst, and the electron transfer was allowed (Fig. S20 in Supporting information). The
13C isotope labelling experiment confirmed that the produced CO was from the photoreduction of CO
2 (Fig. S21 in Supporting information). The reaction conditions were then systematically studied and optimized for CO productivity and the turnover number (TON) using different contents of POP, the concentration of the Ru(bpy)
3Cl
2 photosensitizer, and the
Fe-P catalyst (Fig. S22 and Tables S5~S7 in Supporting information for details). Next, we studied the atmospheric CO
2 photoreduction of
POP-1~
6 (1 mg/mL) using 0.01 mmol/L of
Fe-P, 10 mmol/L of Ru(bpy)
3Cl
2, and 20 mmol/L TEOA, in water under an air atmosphere. The results showed that the
POP-1~
6 can achieved CO
2-to-CO conversion with a productivity of 1.4 µmol g
−1 h
−1 (TON = 335, yield = 29%), 2.6 µmol g
−1 h
−1 (TON = 622, yield = 53%), 3.9 µmol g
−1 h
−1 (TON = 928, yield = 80%), 3.9 µmol g
−1 h
−1 (TON = 927, yield = 79%), 4.2 µmol g
−1 h
−1 (TON = 1015, yield = 87%), and 4.5 µmol g
−1 h
−1 (TON = 1085, yield = 93%), respectively (
Fig. 5,
Table 2 and Table S8 in Supporting information). The high atmospheric CO
2 photoreduction performance of
POP-3~
6 may be owed to their high CO
2 adsorption capacities and the interactions, such as hydrophobic effect and electrostatic interactions, between the POP scaffolds and the
Fe-P catalyst [
58]. The cross-linked networks and hierarchical porous structure of POPs might also optimize the CO
2 mass transfer, electron transport, and the stability of intermediates [
58]. We further performed photocatalytic recycling experiments of
POP-1~6. The recycling results showed that these POPs have good recyclability with negligible activity loss after five catalytic cycles (Fig. S23 and Table S9 in Supporting information). The FT-IR experiments showed no obvious changes for
POP-1 before and after five photocatalytic cycles, which indicated that its structural integrity was maintained (Fig. S24 in Supporting information).
Meanwhile, the BET results showed that there is no obvious surface area loss in recycled
POP-1 after photocatalytic recycling, possibly due to no pore collapse or blockage (Fig. S13). XRD analysis showed that
POP-1~6 and recycled
POP-1~6 both are amorphous materials and have no obvious structure change (Fig. S25 in Supporting information). The scanning transmission electron microscopy (STEM) and energy dispersive X-ray (EDX) mapping analysis also certified the incorporation of heteroatoms of N and Br elements within of
POP-1~6 and of N, Br, Fe and Ru elements within recycled
POP-1~6 (
Fig. 2, Figs. S14, S15 and S26, and Table S10 in Supporting information). The quantitative EDS analysis (weight% and atomic%, Table S10) for all catalysts (
POP-1~6) also confirmed their stability after reuse since the element contents of C and N remain basically unchanged. XPS analysis of recycled
POP-1 confirmed the exist of C–C and C–N (Fig. S27 in Supporting information) [
59–
64], and there is no obvious signal of Fe and Ru may due to their trace amount (Figs. S15 and S26 and Table S10) [
59–
64]. The comparison of CO
2 reduction performance of these
POP-1~6 platforms with a range of benchmark materials for integrated CO
2 DAC and photoreduction are summarized in Table S11 (Supporting information).
In summary, we developed six amine-functionalized, water-dispersible cyclen-based POP platforms for atmospheric CO2 capture and photoreduction. The POP-1~6 exhibit exceptional aqueous-phase CO2 uptake 264–569 mg/g, with DAC capacities reaching 11–49 mg g−1 d−1 in water. When integrated with photocatalysts, the POP-1~6 can achieve atmospheric CO2-to-CO conversion with a productivity of 1.4–4.5 µmol g−1 h−1 and CO2 conversion rates up to 93% compared to free molecules while maintaining stability and recyclability (> 5 cycles). The design principles demonstrated herein provide insights for creating integrated capture-conversion systems based on POPs advancing carbon neutrality goals.