An ultrafast X-ray glance into photoacid electronic structure

Estimated charge distribution changes on the APTS photoacid and conjugate photobase forms, showing major changes in Mulliken charges and in the electric dipole moment upon electronic excitation.

Estimated charge distribution changes on the APTS photoacid and conjugate photobase forms, showing major changes in Mulliken charges and in the electric dipole moment upon electronic excitation. © MBI

F&ouml;rster cycle of an amine photoacid, showing electronic ground states S<sub>0</sub> and the first excited states S<sub>1</sub> of the acidic (left) and basic (right) species. There are the four stages of photoacid behaviour in aqueous solution, as shown by the cartoons. In the centre transient soft-X-ray spectra are shown, measured on 8-aminopyrene-1,3,6-trisulfonate (APTS).

Förster cycle of an amine photoacid, showing electronic ground states S0 and the first excited states S1 of the acidic (left) and basic (right) species. There are the four stages of photoacid behaviour in aqueous solution, as shown by the cartoons. In the centre transient soft-X-ray spectra are shown, measured on 8-aminopyrene-1,3,6-trisulfonate (APTS). © MBI

Photoacids are molecules that release a proton upon electronic excitation, thus enhancing the acidity of a liquid. Pioneering work by Theodor Förster has shown the direct relationship between the wavelength position of optical absorption and acidity properties with which the increase in acidity  in the first electronic excited state can be quantified. However, underlying full microscopic explanations for the photoacidity phenomenon have remained sparse. With ultrafast X-ray spectroscopy, locally probing the electronic structure of a proton donating group of an amine aromatic photoacid has now provided direct insight in the changes of electronic structure. The long standing open question for photoacidity has now finally been resolved: major electronic structure changes occur on the base side of the so-called Förster cycle, whereas the acid side plays a minor role. 

Photoacids have been known for more than 70 years. Theodor Förster has been the first to correctly describe the observations of absorption and fluorescence spectra of photoacids, and connect positions of the electronic transitions giving rise to optical absorption bands to the increased acidity properties of photoacids in the electronic excited state. Many research activities have been pursued in the following decades, but apart from quantum chemical calculations of photoacid molecules of medium size, focussing on the intramolecular electronic charge distribution changes of the proton donating moieties of photoacids, microscopic insight have remained limited. Some of these studies have indicated – in line with previous suggestions based on physical organic principles – that the effects of electronic excitation are much more pronounced on the conjugate photobase side of the Förster cycle.

Scientists from the Max-Born-Institute in Berlin, Stockholm University, the University of Hamburg, Helmholtz-Zentrum Berlin, Ben-Gurion University of the Negev in Beersheva and Uppsala University, have now successfully pursued a novel combined experimental and theoretical approach to study the electronic charge distributions of photoacids along the four stages of photoacids provide direct microscopic insight into the electronic structural changes of the proton donating amine group of an aminopyrene derivative in aqueous solution. The K-edge X-ray absorption spectra of nitrogen atoms in the molecular structure were measured at the synchrotron BESSY II in transmission mode to locally probe electronic structure on ultrafast time scales. Together with quantum chemical calculations, such results provide a consistent picture of photoacid behaviour (Fig. 1): electronic charge distributions of the proton donating group are only minor on the photoacid side, but substantial on the conjugate photobase side. Yet the overall dipole moment change of the whole molecule is as important as the local charge distribution changes, hence solvation dynamics by the solvent water is the second important factor governing photoacidity.

MBI

  • Copy link

You might also be interested in

  • BESSY II is back in operation after maintenance shutdown
    News
    10.09.2026
    BESSY II is back in operation after maintenance shutdown
    On 7 September 2026, BESSY II was set into operation after a four-week shutdown. BESSY II is scheduled to resume full user operation on 22 September.
  • 3D magnetic field experiment at BESSY II takes spintronics a step further
    Science Highlight
    07.09.2026
    3D magnetic field experiment at BESSY II takes spintronics a step further
    (Fe0.63Ni0.3Pd0.07)3P or FNPP is a magnetic material that exhibits complex magnetic structures even at room temperature. This makes the material of interest for spintronics, a field that could enable data processing with significantly lower energy consumption. One potential application is novel magnetic memory devices. However, generating and modifying the desired structures in a controlled manner remains a challenge to date. A new study led by HZB has now taken a step forward in this regard. They demonstrated at the worldwide unique VEKMAG-Station at BESSY II, that a tiny external B-field in the plane of the magnetic patterns is sufficient to change them.
  • Confirmed figures for the first time: Investments in BESSY are worthwhile for Berlin and Germany
    News
    03.09.2026
    Confirmed figures for the first time: Investments in BESSY are worthwhile for Berlin and Germany
    An impact analysis by DIW Econ demonstrates the scientific and economic value of BESSY II. Every euro invested yields three euros for Germany and as much as ten euros for the State of Berlin. Furthermore, the study provides an economic forecast for the construction of BESSY III.
    The impact analysis was presented on 3 September 2026 to Dr Henry Marx, State Secretary for Science and Research in the Berlin Senate. He supports the investment and is a strong advocate for BESSY III.