| Literature DB >> 28132505 |
Wilbert Mtangi1, Francesco Tassinari1, Kiran Vankayala1, Andreas Vargas Jentzsch2, Beatrice Adelizzi2, Anja R A Palmans2, Claudio Fontanesi3, E W Meijer2, Ron Naaman1.
Abstract
The production of hydrogen through water splitting in a photoelectrochemical cell suffers from an overpotential that limits the efficiencies. In addition, hydrogen-peroxide formation is identified as a competing process affecting the oxidative stability of photoelectrodes. We impose spin-selectivity by coating the anode with chiral organic semiconductors from helically aggregated dyes as sensitizers; Zn-porphyrins and triarylamines. Hydrogen peroxide formation is dramatically suppressed, while the overall current through the cell, correlating with the water splitting process, is enhanced. Evidence for a strong spin-selection in the chiral semiconductors is presented by magnetic conducting (mc-)AFM measurements, in which chiral and achiral Zn-porphyrins are compared. These findings contribute to our understanding of the underlying mechanism of spin selectivity in multiple electron-transfer reactions and pave the way toward better chiral dye-sensitized photoelectrochemical cells.Entities:
Year: 2017 PMID: 28132505 PMCID: PMC5330654 DOI: 10.1021/jacs.6b12971
Source DB: PubMed Journal: J Am Chem Soc ISSN: 0002-7863 Impact factor: 15.419
Figure 1Molecules used as photosensitizer and their supramolecular aggregation. (A) The chiral and achiral Zn porphyrins, (C and E) their absorption spectra and CD spectra of the aggregated state in solution (1.7 × 10–5 M in methylcyclohexane) and when adsorbed on the surface (inset C). (B) the chiral and achiral TPyA, (D and F) their absorption and CD spectra of the aggregated state in solution and when adsorbed on the surface (inset D). The red curves represent the chiral molecules, while the blue represent the achiral ones.
Figure 2Magnetic conducting atomic force microscopy (mc-AFM) measurements on stacks of chiral and achiral Zn-porphyrins. (A) The experimental setup. The current as a function of the applied voltage obtained from the chiral (B) and achiral (C) Zn-porphyrin molecules. The insets show corresponding histograms of currents obtained at 3 V for the two opposite magnetic orientations of the tip.
Figure 3Photoelectrochemical cell and the current density as a function of the potential. In A, a schematic representation of the photoelectochemical cell. The potential is given vs the Ag/AgCl electrode, when the TiO2 electrode is coated with self-assembled achiral (blue lines) or chiral (red lines) molecules. In (B) and (C), Zn-porphyrins were used while in (D) and (E), TPyA molecules were employed. The measurements were performed in the dark (solid lines) and under illumination (dotted lines). In (C) and (E) measurements were performed while chopping the light. All measurements were performed at a scan rate of 10 mVs–1. The flat-band potentials in the dark for Zn-porphyrin and TPyA molecules were obtained from Mott–Schottky plots (F and G, respectively) at a frequency of 1.99 kHz and oscillation voltage of 20 mV.
Figure 4Control of the hydrogen peroxide production. UV–vis absorption spectra from the titration of the used electrolyte (Na2SO4) with o-tolidine of bare TiO2 and TiO2 electrodes coated with (A) self-assembled Zn-porphyrins of either achiral (A-Zn) or chiral (S-Zn) and (B) TPyA molecules. The control refers to the titration of unused Na2SO4 with o-tolidine. (C) When the electrons transfer to the anodes is non spin specific the spins of the unpaired electrons on the two OH• are aligned antiparallel, hence the interaction between the two OH• is on a singlet surface that correlates with the production of hydrogen peroxide (H2O2). (D) When the electron transfer to the anode is spin specific, the spins of the two electrons are aligned parallel to each other, hence the two OH• interact on a triplet surface that forbids the formation of H2O2 and facilitates the production of oxygen in its ground state.