Abstract
Exciton–exciton annihilation (EEA), an important loss channel in optoelectronic devices and photosynthetic complexes, has conventionally been assumed to be an incoherent, diffusion-limited process. Here we challenge this assumption by experimentally demonstrating the ability to control EEA in molecular aggregates using the quantum phase relationships of excitons. We employed time-resolved photoluminescence microscopy to independently determine exciton diffusion constants and annihilation rates in two substituted perylene diimide aggregates featuring contrasting excitonic phase envelopes. Low-temperature EEA rates were found to differ by more than two orders of magnitude for the two compounds, despite comparable diffusion constants. Simulated rates based on a microscopic theory, in excellent agreement with experiments, rationalize this EEA behaviour based on quantum interference arising from the presence or absence of spatial phase oscillations of delocalized excitons. These results offer an approach for designing molecular materials using quantum interference where low annihilation can coexist with high exciton concentrations and mobilities.
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Data availability
All of the data supporting this study can be found within the paper and its Supplementary Information. Source data are provided with this paper.
Code availability
Code that supports the findings of this study is available at https://github.com/Sarat1995/eea_pdi. This code includes scripts for data processing and theoretical modelling.
References
Jelly, E. E. Spectral absorption and fluorescence of dyes in the molecular state. Nature 138, 1009–1010 (1936).
Hestand, N. J., Tempelaar, R., Knoester, J., Jansen, T. L. C. & Spano, F. C. Exciton mobility control through sub-Å packing modifications in molecular crystals. Phys. Rev. B 91, 195315 (2015).
Tempelaar, R., Koster, L. J. A., Havenith, R. W. A., Knoester, J. & Jansen, T. L. C. Charge recombination suppressed by destructive quantum interference in heterojunction materials. J. Phys. Chem. Lett. 7, 198–203 (2016).
Castellanos, M. A. & Huo, P. Enhancing singlet fission dynamics by suppressing destructive interference between charge-transfer pathways. J. Phys. Chem. Lett. 8, 2480–2488 (2017).
Scholes, G. et al. Using coherence to enhance function in chemical and biophysical systems. Nature 543, 647–656 (2017).
Cao, J. et al. Quantum biology revisited. Sci. Adv. 6, eaaz4888 (2020).
Khairutdinov, R. F. & Serpone, N. Photophysics of cyanine dyes: subnanosecond relaxation dynamics in monomers, dimers, and H- and J-aggregates in solution. J. Phys. Chem. B 101, 2602–2610 (1997).
Scheblykin, I. G., Sliusarenko, O. Y., Lepnev, L. S., Vitukhnovsky, A. G. & Van der Auweraer, M. Strong nonmonotonous temperature dependence of exciton migration rate in J aggregates at temperatures from 5 to 300 K. J. Phys. Chem. B 104, 10950–10951 (2000).
King, S. M., Dai, D., Rothe, C. & Monkman, A. P. Exciton annihilation in a polyfluorene: low threshold for singlet–singlet annihilation and the absence of singlet–triplet annihilation. Phys. Rev. B Condens. Matter Mater. Phys. 76, 085204 (2007).
Ito, F., Inoue, T., Tomita, D. & Nagamura, T. Excited-state relaxation process of free-base and oxovanadium naphthalocyanine in near-infrared region. J. Phys. Chem. B 113, 5458–5463 (2009).
Völker, S. F. et al. Singlet–singlet exciton annihilation in an exciton-coupled squaraine–squaraine copolymer: a model toward hetero-J-aggregates. J. Phys. Chem. C 118, 17467–17482 (2014).
Dostál, J. et al. Direct observation of exciton–exciton interactions. Nat. Commun. 9, 2466 (2018).
Süß, J., Wehner, J., Dostál, J., Brixner, T. & Engel, V. Mapping of exciton–exciton annihilation in a molecular dimer via fifth-order femtosecond two-dimensional spectroscopy. J. Chem. Phys. 150, 104304 (2019).
Kriete, B. et al. Interplay between structural hierarchy and exciton diffusion in artificial light harvesting. Nat. Commun. 10, 4615 (2019).
Malý, P., Mueller, S., Lüttig, J., Lambert, C. & Brixner, T. Signatures of exciton dynamics and interaction in coherently and fluorescence-detected four- and six-wave-mixing two-dimensional electronic spectroscopy. J. Chem. Phys. 153, 144204 (2020).
Shaw, P. E., Ruseckas, A. & Samuel, I. D. W. Exciton diffusion measurements in poly(3-hexylthiophene). Adv. Mater. 20, 3516–3520 (2008).
Hedley, G. J. et al. Picosecond time-resolved photon antibunching measures nanoscale exciton motion and the true number of chromophores. Nat. Commun. 12, 1327 (2021).
Nguyen, D. T. et al. Elastic exciton–exciton scattering in photoexcited carbon nanotubes. Phys. Rev. Lett. 107, 127401 (2011).
Chmeliov, J., Narkeliunas, J., Graham, M. W., Fleming, G. R. & Valkunas, L. Exciton–exciton annihilation and relaxation pathways in semiconducting carbon nanotubes. Nanoscale 8, 1618–1626 (2016).
Yuan, L., Wang, T., Zhu, T., Zhou, M. & Huang, L. Exciton dynamics, transport, and annihilation in atomically thin two-dimensional semiconductors. J. Phys. Chem. Lett. 8, 3371–3379 (2017).
Deng, S. et al. Long-range exciton transport and slow annihilation in two-dimensional hybrid perovskites. Nat. Commun. 11, 664 (2020).
Tzabari, L., Zayats, V. & Tessler, N. Exciton annihilation as bimolecular loss in organic solar cells. J. Appl. Phys. 114, 154514 (2013).
Denton, G. J., Tessler, N., Harrison, N. T. & Friend, R. H. Factors influencing stimulated emission from poly(p-phenylenevinylene). Phys. Rev. Lett. 78, 733 (1997).
Baldo, M. A., Holmes, R. J. & Forrest, S. R. Prospects for electrically pumped organic lasers. Phys. Rev. B 66, 035321 (2002).
Akselrod, G. M., Tischler, Y. R., Young, E. R., Nocera, D. G. & Bulovic, V. Exciton–exciton annihilation in organic polariton microcavities. Phys. Rev. B 82, 113106 (2002).
Cunningham, P. D. et al. Delocalized two-exciton states in DNA scaffolded cyanine dimers. J. Phys. Chem. B 124, 8042–8049 (2020).
Giebink, N. C. et al. Intrinsic luminance loss in phosphorescent small-molecule organic light emitting devices due to bimolecular annihilation reactions. J. Appl. Phys. 103, 044509 (2008).
Nakanotani, H., Sasabe, H. & Adachi, C. Singlet–singlet and singlet–heat annihilations in fluorescence-based organic light-emitting diodes under steady-state high current density. Appl. Phys. Lett. 86, 213506 (2005).
Gélinas, S. et al. Recombination dynamics of charge pairs in a push–pull polyfluorene- derivative. J. Phys. Chem. B 117, 4649–4653 (2013).
Stevens, M. A., Silva, C., Russell, D. M. & Friend, R. H. Exciton dissociation mechanisms in the polymeric semiconductors poly(9,9-dioctylfluorene) and poly(9,9-dioctylfluorene-co-benzothiadiazole). Phys. Rev. B 63, 165213 (2001).
Tamai, Y., Matsuura, Y., Ohkita, H., Benten, H. & Ito, S. One-dimensional singlet exciton diffusion in poly(3-hexylthiophene) crystalline domains. J. Phys. Chem. Lett. 5, 399–403 (2014).
Chowdhury, M. et al. Tuning crystalline ordering by annealing and additives to study its effect on exciton diffusion in a polyalkylthiophene copolymer. Phys. Chem. Chem. Phys. 19, 12441–12451 (2017).
Engel, E., Leo, K. & Hoffmann, M. Ultrafast relaxation and exciton–exciton annihilation in PTCDA thin films at high excitation densities. Chem. Phys. 325, 170–177 (2006).
Smoluchowski, M. V. Versuch einer mathematischen theorie der koagulationskinetik kolloider lösnngen. Z. Phys. Chem. 92, 129–168 (1918).
Chandrasekhar, S. Stochastic problems in physics and astronomy. Rev. Mod. Phys. 15, 1–89 (1943).
Powell, R. C. & Soos, Z. G. Singlet exciton energy transfer in organic solids. J. Lumin. 11, 1–45 (1975).
Tempelaar, R., Jansen, T. L. C. & Knoester, J. Exciton–exciton annihilation is coherently suppressed in H-aggregates, but not in J-aggregates. J. Phys. Chem. Lett. 8, 6113–6117 (2017).
Süß, J. & Engel, V. A wave packet picture of exciton–exciton annihilation: molecular dimer dynamics. J. Chem. Phys. 152, 174305 (2020).
Oleson, A. et al. Perylene diimide-based Hj- and hJ-aggregates: the prospect of exciton band shape engineering in organic materials. J. Phys. Chem. C 123, 20567–20578 (2019).
Spano, F. C. & Mukamel, S.Superradiance in molecular aggregates. J. Chem. Phys. 91, 683–700 (1998).
Eaton, S. W. et al. Singlet exciton fission in polycrystalline thin films of a slip-stacked perylenediimide. J. Am. Chem. Soc. 135, 14701–14712 (2013).
Brown, K. E., Salamant, W. A., Shoer, L. E., Young, R. M. & Wasielewski, M. R. Direct observation of ultrafast excimer formation in covalent perylenediimide dimers using near-infrared transient absorption spectroscopy. J. Phys. Chem. Lett. 5, 2588–2593 (2014).
Pandya, R. et al. Exciton diffusion in highly-ordered one dimensional conjugated polymers: effects of back-bone torsion, electronic symmetry, phonons and annihilation. J. Phys. Chem. Lett. 12, 3669–3678 (2021).
Sneyd, A. J. et al. Efficient energy transport in an organic semiconductor mediated by transient exciton delocalization. Sci. Adv. 7, eabh4232 (2021).
Akselrod, G. M. et al. Visualization of exciton transport in ordered and disordered molecular solids. Nat. Commun. 5, 3646 (2014).
Akselrod, G. M. et al. Subdiffusive exciton transport in quantum dot solids. Nano Lett. 14, 3556–3562 (2014).
Seitz, M. et al. Exciton diffusion in two-dimensional metal-halide perovskites. Nat. Commun. 11, 2035 (2020).
Hybertsen, M. S. & Louie, S. G. Electron correlation in semiconductors and insulators: band gaps and quasiparticle energies. Phys. Rev. B 34, 5390 (1986).
Rehhagen, C. et al. Exciton migration in multistranded perylene bisimide J-aggregates. J. Phys. Chem. Lett. 11, 6612–6617 (2020).
Scheblykin, I. G., Sliusarenko, O. Y., Lepnev, L. S., Vitukhnovsky, A. G. & van der Auweraer, M. Excitons in molecular aggregates of 3,3′bis-[3-sulforpropyl]-5,5′-dichloro-9-ethylthiacarbocyanine (THIATS): temperature dependent properties. J. Phys. Chem. B 105, 4636–4646 (2001).
Mikhnenko, O. V., Blom, P. W. M. & Nguyen, T.-Q. Exciton diffusion in organic semiconductors. Energy Environ. Sci. 8, 1867–1888 (2015).
Caram, J. R. et al. Room-temperature micron-scale exciton migration in a stabilized emissive molecular aggregate. Nano Lett. 16, 6808–6815 (2016).
Marciniak, H., Li, X.-Q., Würthner, F. & Lochbrunner, S. One-dimensional exciton diffusion in perylene bisimide aggregates. J. Phys. Chem. A 115, 648–654 (2011).
Kreger, K. et al. Low temperature exciton dynamics and structural changes in perylene bisimide aggregates. J. Phys. B At. Mol. Opt. Phys. 50, 184005 (2017).
Jang, S., Cheng, Y.-C. & Reichman, D. R. Theory of coherent resonance energy transfer. J. Chem. Phys. 129, 101104 (2008).
Bakulin, A. A. et al. The role of driving energy and delocalized states for charge separation in organic semiconductors. Science 335, 1340–1344 (2012).
Malý, P. et al. Separating single- from multi-particle dynamics in nonlinear spectroscopy. Nature 616, 280–287 (2023).
Nakazono, S., Easwaramoorthi, S., Kim, D., Shinokubo, H. & Osuka, A. Synthesis of arylated perylene bisimides through C−H bond cleavage under ruthenium catalysis. Org. Lett. 11, 5426–5429 (2009).
Wan, Y. et al. Cooperative singlet and triplet exciton transport in tetracene crystals visualized by ultrafast microscopy. Nat. Chem. 7, 785–792 (2015).
Ryzhov, I. V., Kozlov, G. G., Malyshev, V. A. & Knoester, J. Low-temperature kinetics of exciton–exciton annihilation of weakly localized one-dimensional Frenkel excitons. J. Chem. Phys. 114, 5322–5329 (2001).
Hodge, P. G. On isotropic Cartesian tensors. Am. Math. Mon. 68, 793–795 (1961).
Schmidt, M. W. et al. General atomic and molecular electronic structure system. J. Comput. Chem. 14, 1347–1363 (1993).
Gordon, M. S. & Schmidt, M. W. Advances in electronic structure theory: GAMESS a decade later. Theory Appl. Comput. Chem. 2005, 1167–1189 (2005).
Yanai, T., Tew, D. P. & Handy, N. C. A new hybrid exchange–correlation functional using the Coulomb-attenuating method (CAM-B3LYP). Chem. Phys. Lett. 393, 51–57 (2004).
Dunning, T. H. & Hay, P. J. in Methods of Electronic Structure Theory. Modern Theoretical Chemistry Vol. 3 (ed. Schaefer, H. F.) 1–28 (Springer, 1977).
Spano, F. C. Absorption and emission in oligo-phenylene vinylene nanoaggregates: the role of disorder and structural defects. J. Chem. Phys. 116, 5877–5891 (2002).
Philpott, M. R. Theory of the coupling of electronic and vibrational excitations in molecular crystals and helical polymers. J. Chem. Phys. 55, 2039–2054 (2003).
Acknowledgements
The optical spectroscopy and microscopy work at Purdue University was supported by the US Department of Energy’s Office of Science’s Basic Energy Sciences programme through award DE-SC0019215 (to L.H). I.S.D. acknowledges support from the US Department of Energy through the Computational Science Graduate Fellowship under grant number DE-FG02-97ER25308. R.T. was supported by the Center for Molecular Quantum Transduction, an Energy Frontier Research Center funded by the US Department of Energy’s Office of Science’s Basic Energy Sciences programme under award DE-SC0021314. We thank M. Dai for the synthesis of 4Ph PDI.
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L.H. and R.T. conceived of the experiments. S.K., S.D., T.Z, Q.Z. and O.F.W. carried out the optical measurements. I.S.D. and R.T. carried out and analysed the theoretical calculations. S.K., I.S.D., R.T. and L.H. analysed the experimental data. S.K., I.S.D., R.T. and L.H. wrote the manuscript with input from all authors.
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Extended data
Extended Data Fig. 1 Atomic force microscopy images of PDI crystals.
Representative atomic force microscopy (AFM) images of (a) N-Ph PDI and (b) 4Ph PDI self-assembled microcrystals.
Extended Data Fig. 2 Photophysics of PDI monomer and single crystals.
(a) Normalized absorption and (b) Normalized emission spectra of N-Ph PDI and 4Ph PDI monomers dissolved in chloroform with concentrations of 10−5 M. (c) Absorption spectra of a single N-Ph PDI and 4Ph PDI crystals measured by micro-transmittance.
Extended Data Fig. 3 Temperature dependent EEA data of N-Ph PDI (1) and 4-Ph PDI (1).
Time resolved photoluminescence decay at different exciton densities for N-Ph PDI (1) (a-d) and 4Ph PDI (1) (e-h) crystals shown in main text at 30, 80, 120, and 240 K, respectively.
Extended Data Fig. 4 Temperature dependent EEA rate at 1015 cm−3.
(a) Temperature-dependent annihilation rate for N-Ph PDI-(1) crystal (green) and 4Ph PDI-(1) crystal (blue) for an initial exciton density of 1015 cm−3. EEA rate is suppressed by more than two orders of magnitude in N-Ph PDI at low temperature in contrast to a weak temperature dependence observed for 4Ph PDI. Data are presented as \(\gamma\) +/− SE, where the shaded areas indicate the standard error (SE) from the numerical fitting as described in the main text. (b) Comparing the experimentally determined ratio of EEA rates \(\frac{\gamma \left(N-{Ph\; PDI}\right)}{\gamma \left(4{Ph\; PDI}\right)}\) against the ratios predicted by the coherent microscopic theory and the incoherent diffusion-limited theory. Data are presented as the ratio of \(\gamma\) +/− SE, where shaded areas indicate the standard error (SE) of the ratio of EEA rates, propagating from those of γ.
Extended Data Fig. 5 Temperature dependent EEA data of N-Ph PDI (2) crystal.
Exciton density dependent time resolved photoluminescence decay for the N-Ph PDI (2) crystal at (a-h) 6 K, 12 K, 20 K, 30 K, 120 K, 180 K, 240 K, and 280 K, respectively.
Extended Data Fig. 6 Temperature dependent EEA data of N-Ph PDI (3) crystal.
Exciton density dependent time resolved photoluminescence decay for the N-Ph PDI (3) crystal at (a-e) 10 K, 30 K, 77 K, 130 K, and 280 K, respectively.
Extended Data Fig. 7 Temperature dependent EEA data of N-Ph PDI (3) crystal.
Exciton density dependent time resolved photoluminescence decay for the 4Ph PDI (2) crystal at (a-f) 10 K, 30 K, 80 K, 120 K, 240, and 280 K, respectively.
Extended Data Fig. 8 Summary of temperature dependent EEA rate of different N-Ph and 4-Ph PDI crystals.
Temperature-dependent EEA rate for three different N-Ph PDI crystals (blue) and two different 4Ph PDI (green) crystals, extracted based on the lowest and highest exciton intensities. Data are presented as \(\gamma\) +/− SE, where the shaded areas indicate the standard error (SE) from the numerical fitting as described in the main text. For all three N-Ph PDI crystals, the rate is suppressed by more than two orders of magnitude at low temperatures, contrasting the weak temperature dependence observed for the two 4Ph PDI crystals.
Extended Data Fig. 9 Transient Photoluminescence Microscopy.
(a) Schematic illustration of Transient Photoluminescence Microscopy setup. The initial excitation spot is magnified 150x by using a combination of a 50X objective and a 600 mm focal length imaging lens. A time-correlated single photon detector was scanned horizontally to obtain a spatially and temporally resolved emission profile. Abbreviations TCSPC, time-correlated single photon counter. (b) Spatial profile of the excitation laser shows a diffraction limited Gaussian.
Extended Data Fig. 10 Temperature dependence of exciton diffusion data.
Time evolution of spatial profile \({\sigma }^{2}\left(t\right)-{\sigma }_{0}^{2}\) for N-Ph PDI (a-d) and 4Ph PDI (e-h) at 30, 80, 120, 240 K, respectively. Data are presented as \({\sigma }_{t}^{2}\,\)+/− SE, which is the variance with the standard error (SE) estimated from a fitting of 41 spatial data points at time \(t\) to a Gaussian function. Solid black line is linear fit used to extract the diffusion constant D.
Supplementary information
Supplementary Information
Supplementary Note, Tables 1 and 2 and Figs. 1–5.
Source data
Source Data Fig. 2
Temperature-dependent photoluminescence spectra of N-Ph PDI and 4Ph PDI.
Source Data Fig. 3
TRPL decay at different exciton densities plus fitted data (for Fig. 3a–d) and numerically extracted EEA rates (for Fig. 3e).
Source Data Fig. 4
TRPL microscopy data as a function of time and space (for Fig. 4a), spatial slices from two-dimensional images at 0, 2 and 4 ns, along with Gaussian fits (for Fig. 4b), time evolution of spatial profile \({\sigma }^{2}\left(t\right)\) for 4Ph PDI and N-Ph PDI at 10 and 280 K (for Fig. 4c,d) and estimated diffusion constants as a function of temperature for both PDIs (for Fig. 4e).
Source Data Fig. 5
Experimentally determined ratios of the annihilation rates of N-Ph PDI and 4Ph PDI versus theoretically predicted ratios based on a microscopic, coherent model, as well as a model based on incoherent, diffusion-limited EEA using diffusion constants measured by photoluminescence microscopy (for Fig. 5a). The single exciton wavefunction coefficients for N-Ph PDI and 4Ph PDI (for Fig. 5b)
Source Data Extended Data Fig. 1
Atomic force microscopy data for both PDI crystals.
Source Data Extended Data Fig. 2
Normalized absorption and emission spectra (for Extended Data Figs. 2a,b, respectively) of the N-Ph PDI and 4Ph PDI monomers, as well as absorption spectra of single N-Ph PDI and 4Ph PDI crystals measured by micro-transmittance (for Extended Data Fig. 2c).
Source Data Extended Data Fig. 3
Temperature-dependent EEA data and fitted data of N-Ph PDI (1) and 4Ph PDI (1).
Source Data Extended Data Fig. 4
Temperature-dependent EEA data for both PDIs at 1015 cm−3.
Source Data Extended Data Fig. 5
Temperature-dependent EEA data and fitted data of N-Ph PDI (2).
Source Data Extended Data Fig. 6
Temperature-dependent EEA data and fitted data of N-Ph PDI (3).
Source Data Extended Data Fig. 7
Temperature-dependent EEA data and fitted data of 4Ph PDI (2).
Source Data Extended Data Fig. 8
Numerically estimated values of EEA rate for all N-Ph PDI and 4Ph PDI crystals.
Source Data Extended Data Fig. 9
Source data for the spatial profile of the excitation laser.
Source Data Extended Data Fig. 10
Temperature dependence of the exciton diffusion data for both PDIs.
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Kumar, S., Dunn, I.S., Deng, S. et al. Exciton annihilation in molecular aggregates suppressed through quantum interference. Nat. Chem. 15, 1118–1126 (2023). https://doi.org/10.1038/s41557-023-01233-x
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DOI: https://doi.org/10.1038/s41557-023-01233-x
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