Science1 publisher3 min readPublished
Femtosecond photoemission catches an exciton shrinking by a quarter in an organic semiconductor
Physicists led by Graz's Peter Puschnig mapped an exciton's wavefunction and watched it shrink about 25% within 400 femtoseconds. Using that to design better solar-cell materials depends on ab-initio modelling of the data and on donor/acceptor measurements the team has not yet made.
The Scientist · Science desk

What happened
- The method, time-resolved photoemission orbital tomography, pairs pump-probe photoemission with momentum microscopy to record spatial and momentum spread together at femtosecond resolution.
- A 2.35 eV laser pulse created excitons in alpha-sexithiophene films, and a linearly polarized 21.7 eV pulse then ejected their electrons for measurement.
- At creation the exciton spread over about 1.5 nm, roughly the length of three sexithiophene molecules.
- The study is published in Physical Review X by groups at the University of Graz, Marburg University and Forschungszentrum Julich.
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Why it matters
- constraint The wavefunction is inferred from electron energies and directions through theory, so any material-design rule drawn from it depends on the ab-initio model used to interpret the data.
- capability Exciton calculations for organic semiconductors can now be checked against a measured size, spatial structure and phase, alongside energies and lifetimes.
- constraint Organic solar-cell groups cannot yet apply it where charge separates; until donor/acceptor blends are measured, the photovoltaic benefit remains the team's projection.
- cost Each result needs vacuum-transported films, ultrafast photoemission and heavy ab-initio computing across three sites, which for now suits close study of chosen materials over routine screening.
Excitons form when light lifts an electron into a higher energy band and the electron binds to the positively charged hole it leaves behind [18]. They decay within picoseconds. Standard spectroscopy is too slow to record their spatial extent and their momentum profile together inside that window [3]. Physics World describes the new study as the first experimental reconstruction of an exciton's quantum probability distribution [1].
The experiment uses two pulses. Puschnig, who led the work at the University of Graz with colleagues at Marburg University and Forschungszentrum Jülich [2], described the step after the second pulse ejects the electron. "If we then measure the energy and direction of the ejected electrons, theoretical models allow us to infer their quantum-mechanical state," he said [7]. Changing the gap between pulses gives a time series. "And by varying the time between the first and second laser pulses, we are able to obtain snapshots of the exciton at different times after its creation," he said [8].
Those snapshots show the exciton contracting by about 25% within 400 fs of its creation [10], to roughly 1.1 nm [1]. Four hundred femtoseconds is 0.4 ps [2], so the contraction is complete before the exciton reaches the end of a lifetime counted in picoseconds [3]. The Physics World report does not give error bars on either figure or say how many films were measured.
Calling this a direct measurement needs a qualification, and Puschnig's own account supplies it. The detector records the energies and directions of electrons. The wavefunction is what the models infer from them [7]. Interpreting the data required heavy ab-initio computation in Graz [13]. In my view the advance is that those calculations now have more to agree with. "What makes this particularly exciting is that we are not just measuring an energy or lifetime but are also gaining access to the quantum-mechanical wave function of the exciton itself, including its spatial structure and phase," Puschnig said [11].
For organic photovoltaics the case is still a forecast. Sexithiophene is used in solar cells [6], but these films hosted what the team calls a relatively simple exciton [16]. The step that matters for devices happens in donor/acceptor systems, where electron and hole begin to separate after photoexcitation. The researchers say the method could help explain how excited states evolve into those charge-separated states [15]. Those are the next experiments. "We want to observe how charge-separation processes are controlled by the molecular and electronic structure of a material," Puschnig told Physics World [17].
The procedure is demanding to run. "The main challenge was coordinating demanding experiments and theory: producing well-defined molecular films; transporting them under ultra-high vacuum from Jülich to Marburg in a vacuum suitcase; performing ultrafast photoemission measurements; and carrying out computationally intensive ab-initio calculations in Graz to interpret the data," Puschnig said [13].
What to watch
- trPOT measurements on a donor/acceptor blend showing how exciton size and phase change as electron and hole separate.
- Reproduction of the 1.5 nm starting size and 25% contraction, with stated uncertainties, on other films or by another group.
- Whether different theoretical models applied to the same photoemission data return the same wavefunction.