Quantum coherent energy transport in the Fenna–Matthews–Olson complex at low temperature

Author:

Duan Hong-Guang1234ORCID,Jha Ajay256ORCID,Chen Lipeng78ORCID,Tiwari Vandana2910,Cogdell Richard J.11ORCID,Ashraf Khuram11,Prokhorenko Valentyn I.2ORCID,Thorwart Michael34ORCID,Miller R. J. Dwayne1213ORCID

Affiliation:

1. Department of Physics, School of Physical Science and Technology, Ningbo University, Ningbo 315211, People’s Republic of China

2. Max Planck Institute for the Structure and Dynamics of Matter, 22761 Hamburg, Germany

3. I. Institut für Theoretische Physik, Universität Hamburg, 22607 Hamburg, Germany

4. The Hamburg Center for Ultrafast Imaging, 22761 Hamburg, Germany

5. The Rosalind Franklin Institute, Rutherford Appleton Laboratory, Harwell Campus, Didcot, Oxfordshire OX11 OFA, United Kingdom

6. Research Complex at Harwell, Rutherford Appleton Laboratory, Didcot OX11 0QX, United Kingdom

7. Zhejiang Laboratory, Hangzhou 311100, P.R. China

8. Department of Chemistry, Technische Universität München, 85747 Garching, Germany

9. Department of Chemistry, Universität, 20146 Hamburg, Germany

10. European XFEL GmbH, 22869 Schenefeld, Germany

11. School of Molecular Biosciences, University of Glasgow, Glasgow G12 8QQ, United Kingdom

12. Department of Chemistry, University of Toronto, ON, Canada M5S 3H6

13. Department of Physics, University of Toronto, ON, Canada M5S 3H6

Abstract

In the primary step of natural light harvesting, the solar photon energy is captured in a photoexcited electron–hole pair, or an exciton, in chlorophyll. Its conversion to chemical potential occurs in the special pair reaction center, which is reached by downhill ultrafast excited-state energy transport through a network of chromophores. Being inherently quantum, transport could in principle occur via a matter wave, with vast implications for efficiency. How long a matter wave remains coherent is determined by the intensity by which the exciton is disturbed by the noisy biological environment. The stronger this is, the stronger the electronic coupling between chromophores must be to overcome the fluctuations and phase shifts. The current consensus is that under physiological conditions, quantum coherence vanishes on the 10-fs time scale, rendering it irrelevant for the observed picosecond transfer. Yet, at low-enough temperature, quantum coherence should in principle be present. Here, we reveal the onset of longer-lived electronic coherence at extremely low temperatures of ∼20 K. Using two-dimensional electronic spectroscopy, we determine the exciton coherence times in the Fenna–Matthew–Olson complex over an extensive temperature range. At 20 K, coherence persists out to 200 fs (close to the antenna) and marginally up to 500 fs at the reaction center. It decays markedly faster with modest increases in temperature to become irrelevant above 150 K. At low temperature, the fragile electronic coherence can be separated from the robust vibrational coherence, using a rigorous theoretical analysis. We believe that by this generic principle, light harvesting becomes robust against otherwise fragile quantum effects.

Funder

Deutsche Forschungsgemeinschaft

U.S. Department of Energy

Major Scientific Project of Zhejiang Laboratory

Publisher

Proceedings of the National Academy of Sciences

Subject

Multidisciplinary

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