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arxiv: 2605.17687 · v1 · pith:2GL4OAURnew · submitted 2026-05-17 · ⚛️ physics.chem-ph

Simulating Exciton Transport with Complex Absorbing Potentials

Pith reviewed 2026-05-19 21:52 UTC · model grok-4.3

classification ⚛️ physics.chem-ph
keywords exciton transportcomplex absorbing potentialsmolecular aggregatescyanine dyesvacancy defectsenergy transportnon-Hermitian systemsstochastic simulation
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The pith

A stochastic framework with complex absorbing potentials models exciton transport in large molecular aggregates.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper introduces a stochastic framework based on complex absorbing potentials to study exciton movement in large groups of molecules. These potentials act as non-Hermitian sinks that absorb the excitons and thereby measure how efficiently energy travels through the aggregate. The approach is applied to cyanine dye systems arranged as two-dimensional sheets or quasi-one-dimensional tubes, showing the effects of missing molecules and overall size on the dynamics. It also provides a classification scheme that connects the molecular packing arrangement in flat aggregates to their transport performance. A sympathetic reader would care because the results indicate that topology and disorder control energy flow and could inform the design of materials that move energy more effectively.

Core claim

We introduce a stochastic framework based on complex absorbing potentials (CAPs) to investigate exciton transport in large molecular aggregates. Within this approach, CAPs act as non-Hermitian reservoirs and sinks that enable effective measurement of transport efficiency. We apply this framework to cyanine dye aggregates and examine how vacancy defects and system size influence exciton dynamics in two-dimensional sheets and quasi-one-dimensional tubes. We also introduce a CAPs-based classification scheme that links molecular packing in 2D aggregates to transport behavior. Our results demonstrate how aggregate topology and structural disorder govern exciton dynamics and provide guidance for

What carries the argument

Complex absorbing potentials (CAPs) functioning as non-Hermitian reservoirs and sinks to measure transport efficiency in simulated exciton dynamics.

Load-bearing premise

Complex absorbing potentials can function as non-Hermitian reservoirs and sinks that enable effective measurement of transport efficiency in the simulated exciton dynamics.

What would settle it

A direct comparison between the transport efficiencies predicted by the CAPs framework and either exact quantum calculations on small aggregates or experimental exciton diffusion lengths measured in cyanine dye samples with controlled vacancy densities would settle the claim.

Figures

Figures reproduced from arXiv: 2605.17687 by Chern Chuang, Daniel Neuhauser, Dimitri Bazile, Justin Caram.

Figure 1
Figure 1. Figure 1: FIG. 1. Schematic representation of two brick-layer monomers showing the geometric parameters [PITH_FULL_IMAGE:figures/full_fig_p005_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Schematic representation of the complex absorbing potentials (CAPs) implemented in the [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Schematic of the 2D circular absorbing potentials applied to a 2D sheet geometry. The [PITH_FULL_IMAGE:figures/full_fig_p010_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: compares the PR with the average transmission computed using the 1D CAP potential as the energetic disorder strength (σ) increases. The transmission reproduces both the trend and overall shape of the PR. Thus, the average transmission predicts exciton delocalization and can serve as an alternative to PR/IPR(Inverse Participation ratio), with the additional advantage of providing directional information abo… view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (a) Plot of Average Transmission for 2D sheet aggregate with varying [PITH_FULL_IMAGE:figures/full_fig_p014_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Transmission calculated using angle-dependent CAPs with Aggregate Classification of H,J, [PITH_FULL_IMAGE:figures/full_fig_p015_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. k-state contribution of transmission for contour plots of TDBC under varying [PITH_FULL_IMAGE:figures/full_fig_p017_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. k-state contribution of transmission for contour plots of Cy7-DPA under varying [PITH_FULL_IMAGE:figures/full_fig_p018_8.png] view at source ↗
read the original abstract

We introduce a stochastic framework based on complex absorbing potentials (CAPs) to investigate exciton transport in large molecular aggregates. Within this approach, CAPs act as non-Hermitian reservoirs and sinks that enable effective measurement of transport efficiency. We apply this framework to cyanine dye aggregates and examine how vacancy defects and system size influence exciton dynamics in two-dimensional sheets and quasi-one-dimensional tubes. We also introduce a CAPs-based classification scheme that links molecular packing in 2D aggregates to transport behavior. Our results demonstrate how aggregate topology and structural disorder govern exciton dynamics and provide guidance for designing materials with enhanced energy transport.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The paper introduces a stochastic framework based on complex absorbing potentials (CAPs) to investigate exciton transport in large molecular aggregates. Within this approach, CAPs act as non-Hermitian reservoirs and sinks that enable effective measurement of transport efficiency. The framework is applied to cyanine dye aggregates to examine how vacancy defects and system size influence exciton dynamics in two-dimensional sheets and quasi-one-dimensional tubes. A CAPs-based classification scheme is introduced that links molecular packing in 2D aggregates to transport behavior. Results demonstrate how aggregate topology and structural disorder govern exciton dynamics.

Significance. If the central claims are validated, the work offers a potentially efficient stochastic alternative to full open-quantum-system simulations for studying exciton transport in large aggregates. The explicit applications to cyanine dyes, analysis of vacancies and topology, and the proposed classification scheme could provide practical guidance for material design. The approach's computational advantages for large systems would be a notable strength if benchmarks confirm consistency with established methods.

major comments (2)
  1. [Methods] Methods section: The manuscript does not supply an explicit mapping or benchmark demonstrating that the chosen CAP strength and spatial profile recover the correct long-time transport scaling (ballistic vs. diffusive) when compared to a Hermitian Lindblad or Redfield treatment on the same aggregate Hamiltonian. This mapping is load-bearing for the claim that CAP absorption rates directly quantify physical transport efficiency.
  2. [Results] Results section: No validation data, error analysis, or direct comparisons to benchmarks are reported for the claimed regimes of 2D sheets and quasi-1D tubes. Without these, the reported effects of vacancies and topology on dynamics cannot be distinguished from possible artifacts of the artificial non-Hermitian absorption.
minor comments (1)
  1. [Abstract] The abstract refers to a 'stochastic sampling scheme' but the precise implementation details (e.g., how survival probabilities are sampled and averaged) are not summarized with sufficient clarity for immediate reproducibility.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the thoughtful and constructive report. The comments highlight important points regarding validation of the CAP framework against established open-quantum-system methods. We address each major comment below and indicate the revisions we will make to strengthen the manuscript.

read point-by-point responses
  1. Referee: [Methods] Methods section: The manuscript does not supply an explicit mapping or benchmark demonstrating that the chosen CAP strength and spatial profile recover the correct long-time transport scaling (ballistic vs. diffusive) when compared to a Hermitian Lindblad or Redfield treatment on the same aggregate Hamiltonian. This mapping is load-bearing for the claim that CAP absorption rates directly quantify physical transport efficiency.

    Authors: We agree that an explicit benchmark is valuable for establishing the physical correspondence. The original manuscript provides a theoretical derivation linking CAP absorption to transport efficiency and selects parameters based on convergence tests and prior CAP literature for open systems. However, we acknowledge the absence of a direct side-by-side comparison to Lindblad/Redfield scaling on the same Hamiltonian. In the revised version we will add a dedicated benchmark subsection in Methods, using small aggregates (N ≤ 20) where both approaches are computationally feasible, demonstrating that the chosen CAP strength and profile reproduce the expected crossover from ballistic to diffusive scaling. revision: yes

  2. Referee: [Results] Results section: No validation data, error analysis, or direct comparisons to benchmarks are reported for the claimed regimes of 2D sheets and quasi-1D tubes. Without these, the reported effects of vacancies and topology on dynamics cannot be distinguished from possible artifacts of the artificial non-Hermitian absorption.

    Authors: We recognize that the lack of explicit error bars and cross-method validation leaves open the possibility of method-specific artifacts. The presented results already include averages over multiple stochastic trajectories for each configuration, but we did not report the associated standard deviations or perform limited-system comparisons. In the revision we will incorporate error analysis (standard deviation across realizations) for all reported transport efficiencies and add a supplementary figure comparing CAP and Redfield results on representative small 2D and tube geometries to confirm that vacancy and topology trends are preserved. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected; framework is introduced as a new simulation method.

full rationale

The paper presents an original stochastic framework that deploys complex absorbing potentials (CAPs) as non-Hermitian reservoirs and sinks to simulate exciton transport in molecular aggregates. The central steps consist of defining the CAP-augmented Hamiltonian, performing stochastic sampling on cyanine dye systems, and proposing a CAP-based classification that correlates packing geometry with observed dynamics. No load-bearing step reduces by construction to a prior fit or self-citation; the reported influences of vacancies, size, and topology are outputs of the new simulation rather than reparameterizations of its inputs. The derivation chain remains self-contained against external benchmarks because the method is benchmarked by direct application rather than by tautological re-derivation of its own assumptions.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Review is based on abstract only; no explicit free parameters, new entities, or additional axioms beyond the core modeling assumption are described.

axioms (1)
  • domain assumption CAPs act as non-Hermitian reservoirs and sinks that enable effective measurement of transport efficiency.
    Directly stated in the abstract as the foundation of the stochastic framework.

pith-pipeline@v0.9.0 · 5629 in / 1172 out tokens · 45313 ms · 2026-05-19T21:52:32.217425+00:00 · methodology

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Works this paper leans on

52 extracted references · 52 canonical work pages

  1. [1]

    Store the lattice coordinates and center them in thex–yplane A(xn, yn)→B=A−A mid. 9

  2. [2]

    Convert the centered coordinates to cylindrical coordinates B→C(R, θ), R= p x2 n +y 2 n, θ n = arctan yn xn

  3. [3]

    Select lattice points lying on a circle of radiusR a within a specified tolerance

  4. [4]

    VIL VIR Y(Å) X(Å) Brick Lattice with Angle Dependent 2D CAPs(VIL , VIR) 200 160 120 80 40 00 150 300 Ra FIG

    Construct the CAPs on the upper and lower arcs of the resulting circle of radiusR a. VIL VIR Y(Å) X(Å) Brick Lattice with Angle Dependent 2D CAPs(VIL , VIR) 200 160 120 80 40 00 150 300 Ra FIG. 3. Schematic of the 2D circular absorbing potentials applied to a 2D sheet geometry. The circular boundary defines the absorbing region of radiusR a. The angle-dep...

  5. [5]

    Exciton Transport in Molecu- lar Aggregates – From Natural Antennas to Synthetic Chromophore Systems.Advanced Energy Materials2017,7

    Brixner, T.; Hildner, R.; K¨ ohler, J.; Lambert, C.; W¨ urthner, F. Exciton Transport in Molecu- lar Aggregates – From Natural Antennas to Synthetic Chromophore Systems.Advanced Energy Materials2017,7

  6. [6]

    Barford, W.; Duffy, C. D. P. Role of quantum coherence and energetic disorder in exciton transport in polymer films.Physical Review B2006,74

  7. [7]

    Quantum Dynamics of Exciton Transport and Dissociation in Multichromophoric Systems.Annual Review of Physical Chemistry2021,72, 591–616

    Popp, W.; Brey, D.; Binder, R.; Burghardt, I. Quantum Dynamics of Exciton Transport and Dissociation in Multichromophoric Systems.Annual Review of Physical Chemistry2021,72, 591–616

  8. [8]

    Y.; Cotts, B

    Wong, C. Y.; Cotts, B. L.; Wu, H.; Ginsberg, N. S. Exciton dynamics reveal aggregates with intermolecular order at hidden interfaces in solution-cast organic semiconducting films.Nature Communications2015,6. 19

  9. [9]

    N.; Grynyov, R

    Lebedenko, A. N.; Grynyov, R. S.; Guralchuk, G. Y.; Sorokin, A. V.; Yefimova, S. L.; Ma- lyukin, Y. V. Coherent Mechanism of Exciton Transport in Disordered J-Aggregates.The Journal of Physical Chemistry C2009,113, 12883–12887

  10. [10]

    Kalinowski, J.Electrical and Related Properties of Organic Solids; Springer Netherlands, 1997; p 167–206

  11. [11]

    J.; Ruseckas, A.; Samuel, I

    Hedley, G. J.; Ruseckas, A.; Samuel, I. D. W. Light Harvesting for Organic Photovoltaics. Chemical Reviews2016,117, 796–837

  12. [12]

    K.; Eisfeld, A.; Valleau, S.; Aspuru-Guzik, A

    Saikin, S. K.; Eisfeld, A.; Valleau, S.; Aspuru-Guzik, A. Photonics meets excitonics: natural and artificial molecular aggregates.Nanophotonics2013,2, 21–38

  13. [13]

    Energy Transfer Mechanisms and the Molecular Exciton Model for Molecular Ag- gregates.Radiation Research1963,20, 55

    Kasha, M. Energy Transfer Mechanisms and the Molecular Exciton Model for Molecular Ag- gregates.Radiation Research1963,20, 55

  14. [14]

    Jelley, E. E. Molecular, Nematic and Crystal States of I: I-Diethyl–Cyanine Chloride.Nature 1937,139, 631–631

  15. [15]

    Jelley, E. E. Spectral Absorption and Fluorescence of Dyes in the Molecular State.Nature 1936,138, 1009–1010

  16. [16]

    P.; Geue, N.; Bradbury, N

    Deshmukh, A. P.; Geue, N.; Bradbury, N. C.; Atallah, T. L.; Chuang, C.; Pengshung, M.; Cao, J.; Sletten, E. M.; Neuhauser, D.; Caram, J. R. Bridging the gap between H- and J-aggregates: Classification and supramolecular tunability for excitonic band structures in two-dimensional molecular aggregates.Chemical Physics Reviews2022,3

  17. [17]

    E.; Saha-M¨ oller, C

    W¨ urthner, F.; Kaiser, T. E.; Saha-M¨ oller, C. R. J-Aggregates: From Serendipitous Discovery to Supramolecular Engineering of Functional Dye Materials.Angewandte Chemie Interna- tional Edition2011,50, 3376–3410

  18. [18]

    Efficient energy transfer between J-aggregates of thiamonomethinecyanine dyes.Chemical Physics Letters2015,621, 22–28

    Petrenko, V.; Dimitriev, O.; Slominskii, Y.; Smirnova, A. Efficient energy transfer between J-aggregates of thiamonomethinecyanine dyes.Chemical Physics Letters2015,621, 22–28

  19. [19]

    Anderson, P. W. Absence of Diffusion in Certain Random Lattices.Physical Review1958, 109, 1492–1505

  20. [20]

    A.; Scalettar, R

    Evensky, D. A.; Scalettar, R. T.; Wolynes, P. G. Localization and dephasing effects in a time- dependent Anderson Hamiltonian.The Journal of Physical Chemistry1990,94, 1149–1154

  21. [21]

    J.; Nemoto, K

    Uchiyama, C.; Munro, W. J.; Nemoto, K. Environmental engineering for quantum energy transport.npj Quantum Information2018,4

  22. [22]

    K.; Shi, L.; Willard, A

    Lee, C. K.; Shi, L.; Willard, A. P. Modeling the Influence of Correlated Molecular Disorder 20 on the Dynamics of Excitons in Organic Molecular Semiconductors.The Journal of Physical Chemistry C2018,123, 306–314

  23. [23]

    M.; Deotare, P

    Akselrod, G. M.; Deotare, P. B.; Thompson, N. J.; Lee, J.; Tisdale, W. A.; Baldo, M. A.; Menon, V. M.; Bulovi´ c, V. Visualization of exciton transport in ordered and disordered molec- ular solids.Nature Communications2014,5

  24. [24]

    Exciton transport in dynamically disordered molecular aggregates: influence on optical line shapes.Chemical Physics1993,177, 715–726

    Reineker, P.; Warns, C.; Neidlinger, T.; Barv´ ık, I. Exciton transport in dynamically disordered molecular aggregates: influence on optical line shapes.Chemical Physics1993,177, 715–726

  25. [25]

    Excitation transport in molecular aggregates with thermal motion.Phys- ical Chemistry Chemical Physics2020,22, 21169–21184

    Pant, R.; W¨ uster, S. Excitation transport in molecular aggregates with thermal motion.Phys- ical Chemistry Chemical Physics2020,22, 21169–21184

  26. [26]

    Frenkel excitons in one-dimensional systems with corre- lated disorder.Journal of Luminescence1999,83–84, 61–67

    Dom´ ınguez-Adame, F.; Malyshev, V. Frenkel excitons in one-dimensional systems with corre- lated disorder.Journal of Luminescence1999,83–84, 61–67

  27. [27]

    A single defect approximation for localized states on random lattices

    Biroli, G.; Monasson, R. A single defect approximation for localized states on random lattices. Journal of Physics A: Mathematical and General1999,32, L255–L261

  28. [28]

    S.; Klein, N

    Doria, S.; Sinclair, T. S.; Klein, N. D.; Bennett, D. I. G.; Chuang, C.; Freyria, F. S.; Steiner, C. P.; Foggi, P.; Nelson, K. A.; Cao, J.; Aspuru-Guzik, A.; Lloyd, S.; Caram, J. R.; Bawendi, M. G. Photochemical Control of Exciton Superradiance in Light-Harvesting Nan- otubes.ACS Nano2018,12, 4556–4564

  29. [29]

    Exciton trans- port in molecular organic semiconductors boosted by transient quantum delocalization.Nature Communications2022,13

    Giannini, S.; Peng, W.-T.; Cupellini, L.; Padula, D.; Carof, A.; Blumberger, J. Exciton trans- port in molecular organic semiconductors boosted by transient quantum delocalization.Nature Communications2022,13

  30. [30]

    Ishizaki, A.; Fleming, G. R. On the adequacy of the Redfield equation and related approaches to the study of quantum dynamics in electronic energy transfer.The Journal of Chemical Physics2009,130

  31. [31]

    Environment-assisted quantum transport and trapping in dimers

    M¨ ulken, O.; Schmid, T. Environment-assisted quantum transport and trapping in dimers. Physical Review E2010,82

  32. [32]

    Stochastic unraveling of Redfield master equa- tions and its application to electron transfer problems.The Journal of Chemical Physics2003, 119, 6635–6646

    Kondov, I.; Kleinekath¨ ofer, U.; Schreiber, M. Stochastic unraveling of Redfield master equa- tions and its application to electron transfer problems.The Journal of Chemical Physics2003, 119, 6635–6646

  33. [33]

    Stochastically Bundled Dissipators for the Quantum Master Equation

    Adhikari, S.; Baer, R. Stochastically Bundled Dissipators for the Quantum Master Equation. Journal of Chemical Theory and Computation2025,21, 4142–4150

  34. [34]

    L.; Belogolova, A

    Dempwolff, A. L.; Belogolova, A. M.; Sommerfeld, T.; Trofimov, A. B.; Dreuw, A. CAP/EA- 21 ADC method for metastable anions: Computational aspects and application toπ ∗ resonances resonances of norbornadiene and 1, 4-cyclohexadiene.The Journal of Chemical Physics2021, 155

  35. [35]

    A.; Jagau, T.-C

    Gyamfi, J. A.; Jagau, T.-C. Ab Initio Molecular Dynamics of Temporary Anions Using Com- plex Absorbing Potentials.The Journal of Physical Chemistry Letters2022,13, 8477–8483

  36. [36]

    Vibok, A.; Balint-Kurti, G. G. Parametrization of complex absorbing potentials for time- dependent quantum dynamics.The Journal of Physical Chemistry1992,96, 8712–8719

  37. [37]

    The time-dependent Schr¨ odinger equation: Application of absorbing boundary conditions.The Journal of Chemical Physics1989,90, 4351–4355

    Neuhasuer, D.; Baer, M. The time-dependent Schr¨ odinger equation: Application of absorbing boundary conditions.The Journal of Chemical Physics1989,90, 4351–4355

  38. [38]

    A H¨ uckel study of the effect of a molecular resonance cavity on the quantum conductance of an alkene wire.Chemical Physics Letters2004,393, 367–371

    Collepardo-Guevara, R.; Walter, D.; Neuhauser, D.; Baer, R. A H¨ uckel study of the effect of a molecular resonance cavity on the quantum conductance of an alkene wire.Chemical Physics Letters2004,393, 367–371

  39. [39]

    Conductance determined by transmission: probes and quantised constriction resistance.Journal of Physics: Condensed Matter1989,1, 8099–8110

    Landauer, R. Conductance determined by transmission: probes and quantised constriction resistance.Journal of Physics: Condensed Matter1989,1, 8099–8110

  40. [40]

    G.; Ferreira, A.; Bahamon, D

    de Castro, S. G.; Ferreira, A.; Bahamon, D. A. Efficient Chebyshev polynomial approach to quantum conductance calculations: Application to twisted bilayer graphene.Physical Review B2023,107

  41. [41]

    Press, 1999

    Datta, S.Electronic transport in Mesoscopic Systems; Cambridge Univ. Press, 1999

  42. [42]

    Non-Hermitian State-to-State Analysis of Transport in Aggregates with Multiple Endpoints.Journal of Chemical Theory and Computation2025,21, 5858–5866

    Sharma, D.; Bose, A. Non-Hermitian State-to-State Analysis of Transport in Aggregates with Multiple Endpoints.Journal of Chemical Theory and Computation2025,21, 5858–5866

  43. [43]

    A.; Taylor, H

    Mandelshtam, V. A.; Taylor, H. S. Spectral projection approach to the quantum scattering calculations.The Journal of Chemical Physics1995,102, 7390–7399

  44. [44]

    C.; Chuang, C.; Deshmukh, A

    Bradbury, N. C.; Chuang, C.; Deshmukh, A. P.; Rabani, E.; Baer, R.; Caram, J. R.; Neuhauser, D. Stochastically Realized Observables for Excitonic Molecular Aggregates.The Journal of Physical Chemistry A2020,124, 10111–10120

  45. [45]

    C.; Ribeiro, R

    Bradbury, N. C.; Ribeiro, R. F.; Caram, J. R.; Neuhauser, D. Stochastic methodology shows molecular interactions protect two-dimensional polaritons.Physical Review B2024,109

  46. [46]

    Quantum transport calculations using complex absorbing potentials.physica status solidi (b)2009,246, 1407–1412

    Varga, K. Quantum transport calculations using complex absorbing potentials.physica status solidi (b)2009,246, 1407–1412

  47. [47]

    Complex absorbing potential based Lorentzian fitting scheme and time dependent quantum transport.The Journal of Chemi- 22 cal Physics2014,141

    Xie, H.; Kwok, Y.; Jiang, F.; Zheng, X.; Chen, G. Complex absorbing potential based Lorentzian fitting scheme and time dependent quantum transport.The Journal of Chemi- 22 cal Physics2014,141

  48. [48]

    F.; Le´ on-Montiel, R

    Morales-Curiel, L. F.; Le´ on-Montiel, R. d. J. Photochemical dynamics under incoherent illu- mination: Light harvesting in self-assembled molecular J-aggregates.The Journal of Chemical Physics2020,152

  49. [49]

    A.; Knoester, J

    Didraga, C.; Klugkist, J. A.; Knoester, J. Optical Properties of Helical Cylindrical Molecu- lar Aggregates: The Homogeneous Limit.The Journal of Physical Chemistry B2002,106, 11474–11486

  50. [50]

    Seideman, T.; Miller, W. H. Calculation of the cumulative reaction probability via a discrete variable representation with absorbing boundary conditions.The Journal of Chemical Physics 1992,96, 4412–4422

  51. [51]

    Sneyd, A. J. et al. Efficient energy transport in an organic semiconductor mediated by transient exciton delocalization.Science Advances2021,7

  52. [52]

    K.; Moix, J

    Chuang, C.; Lee, C. K.; Moix, J. M.; Knoester, J.; Cao, J. Quantum Diffusion on Molecular Tubes: Universal Scaling of the 1D to 2D Transition.Physical Review Letters2016,116. 23