Fundamental figures of merit for engineering Forster resonance energy transfer
arXiv:1807.06660 · doi:10.1364/OE.26.019371
Abstract
Over the past 15 years there has been an ongoing debate regarding the influence of the photonic environment on Forster resonance energy transfer (FRET). Disparate results corresponding to enhancement, suppression and null effect of the photonic environment have led to a lack of consensus between the traditional theory of FRET and experiments. Here we show that the quantum electrodynamic theory of FRET near an engineered nanophotonic environment is exactly equivalent to an effective near-field model describing electrostatic dipole-dipole interactions. This leads to an intuitive and rigorously exact description of FRET bridging the gap between experimental observations and theoretical interpretations. We show that the widely used concept of the Purcell factor is only important for understanding spontaneous emission and is an incorrect figure of merit for analyzing FRET. To this end, we analyze the figures of merit which characterize FRET in a photonic environment: (1) the FRET rate enhancement factor (), (2) the FRET efficiency enhancement factor () and (3) the two-point spectral density () governing FRET analogous to the local density of states that controls spontaneous emission. Counterintuitive to existing knowledge, we show that suppression of the Purcell factor is in fact necessary for enhancing the efficiency of the FRET process. We place fundamental bounds on the FRET figures of merit arising from material absorption in the photonic environment as well as key properties of emitters including intrinsic quantum efficiencies and orientational dependence. Finally, we use our approach to conclusively explain recent experiments and predict regimes where the FRET rate is expected to be enhanced, suppressed or remain the same. Our work paves for a complete theory of FRET with predictive power for designing the ideal photonic environment to control FRET.
18 pages, 6 figures
References in corpus (4)
- Theory of plasmon-enhanced Foerster energy transfer in optically-excited semiconductor and metal nanoparticles
- Nanophotonic enhancement of the Förster resonance energy transfer rate on single DNA molecules
- Super-Coulombic atom-atom interactions in hyperbolic media
- Nanoplasmonic Renormalization and Enhancement of Coulomb Interactions
Cited by in corpus (15)
- Plasmon-assisted Förster resonance energy transfer at the single-molecule level in the moderate quenching regime
- Resonance Energy Transfer and Quantum Entanglement Mediated by Epsilon-Near-Zero and Other Plasmonic Waveguide Systems
- Global operator bounds on electromagnetic scattering: Upper bounds on far-field cross sections
- Direct imaging of the energy transfer enhancement between two dipoles in a photonic cavity
- Overcoming the bottleneck for quantum computations of complex nanophotonic structures: Purcell and FRET calculations using a rigorous mode hybridization method
- Controlling exciton dynamics in two-dimensional MoS2 on hyperbolic metamaterial-based nanophotonic platform
- Long-range Single Molecule Förster Resonance Energy Transfer Between Alexa Dyes in Zero-Mode Waveguides
- Design of High-Performance Photon Number Resolving Photodetectors Based on Coherently Interacting Nanoscale Elements
- Understanding the Nature of Mean-Field Semiclassical Light-Matter Dynamics: An Investigation of Energy Transfer, Electron-Electron Correlations, External Driving and Long-Time Detailed Balance
- Plasmonic Waveguides to Enhance Quantum Electrodynamic Phenomena at the Nanoscale
- Long-Range Dipole-Dipole Interactions Enabled with Guided Plasmons of Matched Nanoparticle-on-Mirror Antenna Pairs
- Fluorescence decay enhancement and FRET inhibition in self-assembled hybrid gold CdSe/CdS/CdZnS colloidal nanocrystals supraparticles
- Purcell modification of Auger and interatomic Coulombic decay
- MQED-QD: An Open-Source Package for Quantum Dynamics Simulation in Complex Dielectric Environments
- Long-range mid-infrared energy transfer mediated by hyperbolic phonon polaritons