Quantum simulation of Singlet Fission in a trapped ion platform
POSTER
Abstract
Trapped ions provide a pristine platform for quantum simulation of spin and spin–boson models, enabling high-fidelity unitary control and dissipative dynamics relevant to chemical and biological systems [1]. Singlet fission is a multi-excitonic process that converts one photoexcited singlet excitation on a molecular or ionic site into two triplet excitations [2]. In principle, singlet fission could enable surpassing conventional photovoltaic efficiency limits, but predictive design rules are still elusive because the conversion yield depends on a delicate balance of coherence, vibronic resonance, exchange, and environmental relaxation [3].
Here, we model singlet fission in an ion crystal by engineering an effective spin-1 Hamiltonian using the ground-state hyperfine and Zeeman sublevels of the manifold to encode the singlet ground, singlet excited, and triplet states. We analyze the motional-mode couplings required to generate effective singlet fission interaction and to transport excitation across lattice sites. We present an experimental configuration that enables both on-site interactions and inter-site couplings, allowing singlet fission and delocalization of singlet and triplet excitations across the ion crystal.
[1] V. So et al., Sci. Adv.10, eads8011(2024)
[2] Smith. M. B., Michl. J., Annu.Rev.Phys.Chem.64.361–386 (2013)
[3] Campaioli. F, et al., PRXEnergy.3.043003 (2024)
Here, we model singlet fission in an ion crystal by engineering an effective spin-1 Hamiltonian using the ground-state hyperfine and Zeeman sublevels of the manifold to encode the singlet ground, singlet excited, and triplet states. We analyze the motional-mode couplings required to generate effective singlet fission interaction and to transport excitation across lattice sites. We present an experimental configuration that enables both on-site interactions and inter-site couplings, allowing singlet fission and delocalization of singlet and triplet excitations across the ion crystal.
[1] V. So et al., Sci. Adv.10, eads8011(2024)
[2] Smith. M. B., Michl. J., Annu.Rev.Phys.Chem.64.361–386 (2013)
[3] Campaioli. F, et al., PRXEnergy.3.043003 (2024)
*This work is supported by the Welch Foundation Award (grant no. C-2154), the Office of Naval Research Young Investigator Program (grant no. N00014-22-1-2282), the NSF CAREER Award (grant no. PHY-2144910), and the Office of Naval Research (grant no. N00014-23-1-2665 and N00014-24-1-2593). We acknowledge that this material is based on work supported by the U.S Department of Energy, Office of Science, Office of Nuclear Physics under the Early Career Award (grant no. DE-SC0023806).
Presenters
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Midhuna Suganthi Duraisamy
- Rice University