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Green radicals of potassium poly(heptazine imide) using light and benzylamine

Yevheniia Markushyna a, Paolo Lamagni abc, Christian Teutloff d, Jacopo Catalano c, Nina Lock *bc, Guigang Zhang a, Markus Antonietti a and Aleksandr Savateev *a
aMax-Planck Institute of Colloids and Interfaces, Department of Colloid Chemistry, Research Campus Golm, 14476 Potsdam, Germany. E-mail: oleksandr.savatieiev@mpikg.mpg.de
bCarbon Dioxide Activation Center (CADIAC), Aarhus University, Interdisciplinary Nanoscience Center (iNANO), Department of Chemistry, DK-8000 Aarhus C, Denmark. E-mail: nlock@eng.au.dk
cSection of Biological and Chemical Engineering, Dept of Engineering, Aarhus University, Åbogade 40, DK-8200 Aarhus N, Denmark
dFreie Universität Berlin, Department of Physics, 14195 Berlin, Germany

Received 28th August 2019 , Accepted 7th October 2019

First published on 9th October 2019


Abstract

Tinted long-lived ionic carbon nitride radicals were recently introduced and applied in photocatalysis and energy storage. However, the reason for their higher activity in the photocatalytic reaction and optimal conditions for generating such radicals remain vague. Herein, we study the conditions for carbon nitride photocharging to achieve a higher charge density and validate a convenient method to quantify the number of electrons accumulated in carbon nitride semiconductors by quenching its radicals with methylviologen in the dark. In the presence of CO2, potassium poly(heptazine imide) (K-PHI) can be charged by up to 1000 μmol of electrons per gram of the material using benzylamine as an electron donor. Under the same conditions, mesoporous graphitic carbon nitride can accumulate only 50 μmol of electrons per gram. The products of the benzylamine oxidative coupling are imine and ammonia.


Introduction

Photocatalysis has become a topical field of research in organic chemistry starting from the beginning of 21st century due to its simple reaction conditions and omnitude.1 Indeed, the same photocatalyst can promote different chemical reactions.2,3 Due to their chemical stability, ease of preparation, structural tunability and availability, carbon nitrides became convenient catalysts in organic synthesis.4–7 Moreover, poly(heptazine imides) are capable of photocharging.8Fig. 1 sketches the mechanism of IDEAS (Illumination-Driven Electron Accumulation in Semiconductors) – a capacious acronym that we propose for this process in the present communication.
image file: c9ta09500d-f1.tif
Fig. 1 Schematic representation of IDEAS as exemplified for K-PHI. Image of K-PHI suspension in acetonitrile in the presence of benzylamine under a protective Ar atmosphere before light irradiation (yellow) and after light irradiation (green). Abbreviations: VB – valence band; CB – conduction band; ED – electron donor; EA – electron acceptor; and EAred – reduced electron acceptor.

On the energy scale, it can be schematically explained as follows. By absorbing a photon, potassium poly(heptazine imide) (K-PHI) is converted to the excited state (K-PHI*). Electron transfer from the HOMO of the electron donor (ED) lying above the valence band (VB) of K-PHI reduces K-PHI* and gives a negatively charged radical anion (K-PHI˙). IDEAS is accompanied by a distinct color change of K-PHI and related materials from yellow to green or blue.8–11 The energy stored in K-PHI is then released by exposing K-PHI˙ to the electron acceptors (EAs). This step leads to the recovery of K-PHI and formation of a reduced electron acceptor (EAred). K-PHI can accumulate up to several hundred μmol of electrons per gram of the material.9,12

Due to high reactivity of K-PHI˙, characterization of this material is a challenging task. Nevertheless, transient absorption spectroscopy has been used to characterize the green radicals of cyanamide-functionalized poly(heptazine imide).13,14

Earlier, we have shown superior activity of K-PHI in comparison with covalent carbon nitrides in reductive cyclocondensation of chalcones to cyclopentanoles,10 synthesis of N-fused pyrroles15 and oxidative thiolation of toluene.9 On the other hand, tinted long-lived carbon nitride radicals have been applied in H2 production8,16 and O2 reduction to H2O2.11,17 Based on cyanamide-functionalized poly(heptazine imide), Lotsch et al. designed a “solar battery” that combines in one device a light harvester and a charge storage reservoir.18

While already plentiful chemistry and unusual properties make K-PHI a promising material to address other synthetic challenges, a deeper understanding of the IDEAS mechanism is required to use carbon nitrides more efficiently in light-conversion applications.

It should be mentioned that the electron capacity of a relevant carbon nitride material, cyanamide-functionalized poly(heptazine imide), has been investigated electrochemically.18 However, related to the application in organic photocatalysis by suspending a semiconductor particulate in an organic solvent, a more convenient method for measuring the electron capacity of carbon nitride would comprise a redox indicator. Such a method would not require an electrolyte and a specialized electrochemical setup, while quenching of the reaction mixture with a suitable redox indicator would allow for quasi in situ quantification of IDEAS.

Herein, we develop and validate a convenient method to quantify IDEAS using benzylamine as a model electron donor and methylviologen as a redox indicator. We compare the capacity of K-PHI and covalent mesoporous graphitic carbon nitride (mpg-CN) under Ar and CO2.

Results and discussion

K-PHI was characterized using different techniques and the summary is given in Fig. S2 and S3.19 The number and position of diffraction peaks in the PXRD pattern are identical to the ones reported earlier (Fig. S2a).20,21 The valence band maximum (VBM) in K-PHI determined by ultraviolet photoelectron spectroscopy (UPS) is located at ∼2.5 V (Fig. S2e). K-PHI has the main onset of absorption at 460 nm related to π–π* transitions and a band of lower intensity with the edge at 650 nm (n–π* transitions) (Fig. S2f). By using the π–π* band, an optical band gap of 2.72 eV was determined. K-PHI shows maximum fluorescence at ∼500 nm upon sample excitation with 350 nm (Fig. S2g). K-PHI does not possess distinct porosity as evidenced by the N2 sorption isotherm (Fig. S2h). The specific surface area is 89 m2 g−1. FT-IR shows peaks typical for K-PHI and carbon nitrides in general: 800 cm−1 (heptazine out-of-plane bending), 916 cm−1 and 985 cm−1 (symmetric vibrations of the metal–NC2 moiety), 1116–1390 cm−1 (C–O stretch), 1574 cm−1 (secondary amine N–H bend), 1653 cm−1 (primary amine N–H bend), 2184 cm−1 (nitrile stretch), and 2500–3600 cm−1 (N–H stretch) (Fig. S2i).22 In water, K-PHI breaks into particles of ca. 50 to 200 nm in diameter with an average size of 94 nm (Fig. S2j). The ordered structure of the catalyst is readily observed in the high resolution transmission electron microscopy (HR-TEM) image of K-PHI (Fig. S2l). Relaxation of the excited state via a radiative path occurs within 0.66 ns (Fig. S3).

In order to quantify the number of electrons accumulated in K-PHI, we performed a series of experiments. K-PHI˙ was generated in situ using benzylamine as an electron donor followed by the addition of methylviologen dichloride (MV2+). The latter was reduced via a one-electron process to a radical cation (MV˙+) that has a pronounced blue colour. The amount of MV˙+ produced upon K-PHI˙ quenching with MV2+ was determined measuring the solution absorbance at 600 nm (Fig. S4). The amount of MV˙+ is therefore equal to the amount of electrons accumulated in the catalyst. Fig. 2a summarizes this procedure.


image file: c9ta09500d-f2.tif
Fig. 2 Insights into carbon nitride charge storage capacity. (a) Visual appearance of the reaction mixture – K-PHI, benzylamine, acetonitrile, under Ar (1 bar). From left to right: reaction mixture (under Ar) before light irradiation (yellow), after light irradiation (green), and methyl viologen (MV2+) addition (blue). Schematic representation of the procedure for measuring the absorption of a MV˙+ solution; (b) electron capacity of carbon nitrides and appearance of the reaction tubes after light was switched off under Ar (1 bar) and CO2 (1 bar). In the blank experiment, no carbon nitride catalyst was added. Conditions: benzylamine 50 μmol, MeCN 1 mL, time 24 h, T = 35 °C, gas pressure 1 bar; (c) capacity of K-PHI depending on the benzylamine concentration. Conditions for K-PHI˙ generation: MeCN 3 mL, CO2 1 bar, time 24 h, T = 35 °C. Conditions for K-PHI˙ quenching: MV2+ 0.1 mmol; (d) Number of electrons (y-axis) transferred from K-PHI˙ to MV2+versus K-PHI amount (x-axis) equal to the number of electrons accumulated in K-PHI˙. Conditions for K-PHI˙ preparation: initial benzylamine concentration 63 μmol mL−1, reaction temperature 35 °C, time 24 h, MeCN 3 mL, CO2 1 bar. K-PHI˙ quenching conditions: MV2+ 0.1 mmol. See the ESI for calculation details; (e) EPR spectra. EPR spectra of K-PHI suspension in MeCN in the dark (grey curves) and under 461 nm light (brown curves) irradiation (BA – benzylamine); (f) quenching of K-PHI˙ with AgOTf. Reaction was performed under CO2. Appearance of the reaction mixture and schematic representation of the quenching reaction.

Using the abovementioned methodology, the electron capacity of mpg-CN was determined to be 43 ± 5 μmol g−1, however no apparent colour change was observed (Fig. 2b). The higher surface area of mpg-CN compared to K-PHI, i.e. 180 m2 g−1versus 89 m2 g−1, apparently is not a decisive factor for efficient IDEAS. Instead, the crystalline structure and the ability of the material to stabilize negative charges observed for K-PHI are important. It has also been reported that cyanamide groups in poly(heptazine imide) are responsible for electron accumulation.8,21 In the case of K-PHI, a deeper reaction mixture colour was observed in the presence of CO2 (the interaction between CO2 and benzylamine is investigated below), which correlates with a higher electron capacity of 957 ± 82 μmol g−1 compared to 701 ± 46 μmol g−1 under Ar. Nevertheless, the electron capacity of K-PHI under Ar using benzylamine as an electron donor is still 5.8 times higher compared to that using benzyl alcohol as an electron donor.9 This illustrates the much better ability of amines to quench reductively the excited state of the carbon nitride photocatalyst. In the control experiment without the carbon nitride photocatalyst, MV2+ is not reduced by benzylamine alone.

Fig. 2c illustrates the effect of the benzylamine concentration, i.e. the electron donor concentration, on the number of electrons accumulated in K-PHI. K-PHI reaches saturation at a benzylamine concentration of 60 μmol mL−1, at which the electron capacity approaches 957 ± 82 μmol g−1. This number corresponds to 92 ± 8 C g−1 and is higher than that reported for cyanamide-functionalized poly(heptazine imide) determined from electrochemical discharge profiles (45 C g−1).18 Given that the molecular weight of a K-PHI monomer unit is 223 g mol−1 (Fig. S5),23 it can be concluded that every 4th heptazine unit in K-PHI bears an uncoupled electron, while for cyanamide-functionalized poly(heptazine imide) one electron is being stored on every 9th and 10th cyanamide-heptazine motif.8,18 Taking into account that K-PHI is represented by particles with an average diameter of 100 nm, the volume-to-surface ratio of heptazine units is 26. In other words, in order to achieve such a high density of trapped electrons, they must be stored not only on the surface of the material, but to be distributed in the bulk of the K-PHI particles. These results underline the similarity between the cathode of an electric battery and the K-PHI nanoparticle.

The plot of the number of trapped electrons versus K-PHI mass shows a linear trend, supporting the reproducibility of the method of IDEAS quantification in the range of K-PHI masses up to 10 mg per experiment, which is 787 ± 35 μmol g−1 (Fig. 2d).

Furthermore, we studied the suspension of K-PHI in acetonitrile by EPR (Fig. 2e). In the dark, a broad signal of low intensity at 3350 G (g = 2.016, after magnetic field calibration) was detected. The intensity of the signal remained almost the same when the EPR spectrum was acquired while the sample was irradiated with 461 nm (6 mW cm−2). Upon addition of benzyl amine to the sample in the dark, the broad signal at 3350 G disappeared and a narrow signal of low intensity appeared at 3370 G (g = 2.0048). Under light irradiation, the intensity of the signal increased drastically supporting that K-PHI* was quenched by benzylamine and the K-PHI˙ radical was formed.

Finally, K-PHI˙ can be quenched not only with MV2+, but also with AgOTf, necessarily under oxygen-free conditions. In this case, Ag+ is instantly reduced to Ag0 (Fig. 2f). Formation of Ag0 was confirmed by the presence of (111) and (200) diffraction peaks in the powder X-ray diffraction pattern of the resulting solid (Fig. S6). Upon the reaction mixture workup, benzylammonium triflate was isolated (Fig. S7). It suggests that the negative charge of K-PHI˙ is compensated by benzylammonium cations, similar to K+ when phosphate buffer is used.18 Taking into account the successful quenching of K-PHI˙ with AgOTf and MV2+ and their standard redox potentials, E(Ag/Ag+)0 = +0.80 V and E(MV2+/MV˙+)0 = −0.5 V vs. SHE, energetically the SOMO of K-PHI˙ lies at a potential more positive than −0.5 V vs. SHE.

In order to elucidate the path of benzylamine oxidation, we performed several experiments in CD3CN using (15N)-substituted benzylamine. In excess of CO2, (15N)benzylamine is quantitatively converted into benzylcarbamic acid as we deduced from the 15N, 1H and 13C NMR spectra (Fig. 3a). Therefore, benzylcarbamic acid is a more plausible electron donor than benzylamine itself, if the reaction is performed in the presence of CO2. In the 15N NMR spectrum of the reaction mixture obtained using (15N)benzylamine as a substrate, we registered a signal of (15N)imine at 329.3 ppm and a broad peak at −1.4 ppm that corresponds to either 15NH3 or 15NH4+ (Fig. 3b). In the control experiment using benzylcarbamic acid (50 μmol) as an electron donor, we also obtained imine in 40% yield as evidenced by 1H NMR (Fig. S8).


image file: c9ta09500d-f3.tif
Fig. 3 (a) 15N NMR spectrum of a (15N)benzylamine solution in CD3CN[thin space (1/6-em)]:[thin space (1/6-em)]DMSO-d6 (4[thin space (1/6-em)]:[thin space (1/6-em)]1) before (bottom) and after (top) saturation with CO2; (b) 15N NMR spectrum of the reaction mixture in CD3CN after the photocatalytic experiment. The up-field area was magnified and expanded for clarity.

The stoichiometry of benzylamine coupling to imine requires evolution of 1 equivalent of H2. However, the amount of H2 detected by GC-TCD (1.48 nmol, Fig. S9) was substantially lower than that expected from the reaction of benzylamine coupling (25 μmol). In order to comply with the mass balance of the reaction, hydrogen is presumably stored in K-PHI. Elemental analysis of the K-PHI after the photocatalytic reaction showed an increased content of hydrogen, 2.60 ± 0.01 wt% versus 2.23 ± 0.03 wt%, in the fresh K-PHI. The increased hydrogen content translates into 18.5 μmol of H+ (or 9.25 μmol of H2) that is close to the value obtained from the typical experiment of benzylamine coupling, i.e. 25 μmol (reagent loading as shown in Fig. 2b). These results suggest that not only electrons, but also protons from the reaction of benzylamine coupling are stored in K-PHI, which compensate the negative charge. The protons and electrons do not recombine spontaneously, but can be released in the dark by adding a Pt co-catalyst.8

Conclusions

The conditions for the carbon nitride radical anion generation by IDEAS were elaborated, and the number of accumulated electrons was measured by quenching the carbon nitride radical anion with a common redox indicator – methylviologen dichloride. This method is generally applicable for the characterization of semiconducting materials regarding their ability to accumulate electrons. Carbon nitride materials can be charged up to at least 957 ± 82 μmol g−1 (92 ± 8 C g−1) using benzylamine as a convenient electron donor in the presence of CO2. Every 4th heptazine unit in K-PHI thus holds an uncoupled electron. Optimization of the poly(heptazine imide) structure toward a higher capacity by IDEAS is one of the strategies to enhance further the photocatalytic performance of the material. Selection of stronger electron donors can also potentially increase the density of accumulated electrons in semiconductors.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

The authors are grateful to the Deutsche Forschungsgemeinschaft for the financial support (DFG-An 156 13–1). PL and NL acknowledge the Danish National Research Foundation (DNRF 118, CADIAC). PL, NL and JC thank the AU Synergic grant for partially supporting their work.

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Footnotes

Electronic supplementary information (ESI) available: Catalyst preparation procedure and characterization data; 1H, 13C and 15N NMR spectra; supplementary figures. See DOI: 10.1039/c9ta09500d
These authors contributed equally to this work.

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