4.8 Article

Triplet-pair spin signatures from macroscopically aligned heteroacenes in an oriented single crystal

Publisher

NATL ACAD SCIENCES
DOI: 10.1073/pnas.2201879119

Keywords

magnetic resonance; quantum information; singlet fission; triplet pair; photophysics

Funding

  1. US Department of Energy (DOE) [DE-AC36-08GO28308]
  2. US Department of Energy, Office of Basic Energy Sciences, Division of Chemical Sciences, Biosciences, and Geosciences
  3. DOE's Office of Energy Efficiency and Renewable Energy
  4. Office of Science of the US DOE [DE-AC02-05CH11231]

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The photo-driven process of singlet fission can generate coupled triplet pairs with intriguing properties. Among the sublevels, the quintet is particularly interesting for quantum information. Previous theoretical work has shown that this sublevel can be selectively populated under certain conditions.
The photo-driven process of singlet fission generates coupled triplet pairs (TT) with fundamentally intriguing and potentially useful properties. The quintet (TT0)-T-5 sublevel is particularly interesting for quantum information because it is highly entangled, is addressable with microwave pulses, and could be detected using optical techniques. Previous theoretical work on a model Hamiltonian and nonadiabatic transition theory, called the JDE model, has determined that this sublevel can be selectively populated if certain conditions are met. Among the most challenging, the molecules within the dimer undergoing singlet fission must have their principal magnetic axes parallel to one another and to an applied Zeeman field. Here, we present time-resolved electron paramagnetic resonance (TR-EPR) spectroscopy of a single crystal sample of a tetracenethiophene compound featuring arrays of dimers aligned in this manner, which were mounted so that the orientation of the field relative to the molecular axes could be controlled. The observed spin sublevel populations in the paired TT and unpaired (T+T) triplets are consistent with predictions from the JDE model, including preferential (TT0)-T-5 formation at z parallel to B-0, with one caveat-two (TT)-T-5 spin sublevels have little to no population. This may be due to crossings between the (TT)-T-5 and (TT)-T-3 manifolds in the field range investigated by TR-EPR, consistent with the intertriplet exchange energy determined by monitoring photoluminescence at varying magnetic fields.

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