Double-excitation manifold's effect on exciton transfer dynamics and the efficiency of coherent light harvesting

TL;DR

This paper investigates how double-excitation states influence exciton transfer and light harvesting efficiency, revealing that certain double-excitation states act as dynamical dark states that can enhance energy trapping and overall efficiency.

Contribution

It extends the dark state concept to the double-excitation manifold, demonstrating its impact on exciton dynamics and light harvesting efficiency in different geometries.

Findings

Double-excitation states can serve as dynamical dark states reducing radiative losses.

Topology and size of the antenna affect the dark state mechanism.

Exciton-exciton annihilation can both deplete double-excitation populations and enhance efficiency.

Abstract

The efficiency of natural light harvesting systems is largely determined by their ability to transfer excitations from the antenna to the energy trapping center before recombination. Exciton diffusion length similarly limits organic photovoltaics and demands bulk heterojunction architectures. Dark state protection, achieved by coherent coupling between subunits within the antenna, can significantly reduce radiative recombination and enhance the efficiency of energy trapping. In this work we extend the dark state concept to the double-excitation manifold by studying the dynamical flow of excitations. We show the lowest double-excitation state carries minimal oscillator strength but relaxation to this state from higher lying double excitations can be relatively rapid such that the lowest double excitation state can act as a dynamical dark state protecting excitation from radiative recombination. This mechanism is sensitive to topology and operates differently for chain and ring structures, while becoming more pronounced in both geometries when the size of the antenna increases. When the exciton-exciton annihilation (EEA) mechanism is considered, the double-excitation population is quickly depleted and the dynamics changes dramatically. However the efficiency and output power are still significantly different from those calculated using the single-excitation manifold alone, justifying the necessity of considering the double-excitation manifold. Remarkably, in certain scenarios, the EEA can even increase the overall light harvesting efficiency by bringing population down from the double-excitation dark states to the single-excitation manifold.