Abstract:Exciton−polaritons�hybrid exciton−photon quasi-particles�have enabled exciting long-range coherent transport by taking advantage of the properties of their photonic component. However, most experimental demonstrations of strong coupling have been based on semiconductor Fabry−Peŕot microcavities. Here, we report an open and versatile exciton−polariton platform by integrating two-dimensional lead halide perovskites with plasmonic nanoparticle arrays, which support hybridization between excitons and surface latti… Show more
“…In the results Section , we choose the MNP and PC parameters to maximize the optical near-field of the PC, such that both resonances appear for the same frequency range. In this case, the collective interactions do not cause a narrow distinct peak, as focused on, e.g., in refs , , – , but rather amplify and sharpen the present MNP resonance.…”
Section: Theoretical Modelsupporting
confidence: 55%
“…Its distance dependency is depicted in the inset of Figure b, illustrating the (δ z ) −2 proportionality. To assign the hybrids to a particular coupling regime, the effective Rabi energy Ω eff ≠ 0 is compared with the line width γ ex and γ pl of the individual constituents. , A coupling strength leading to a peak splitting that is small compared to the line widths as, e.g., in the δ z = 17 nm , case is still assigned to weak coupling and has been observed in experiments with TMDCs coupled to a MNP or a PC in refs , , , and .…”
Section: Numerical Results and Discussionmentioning
Monolayers of transition
metal dichalcogenides (TMDCs)
are direct-gap
semiconductors with strong light–matter interactions featuring
tightly bound excitons, while plasmonic crystals (PCs), consisting
of metal nanoparticles that act as meta-atoms, exhibit collective
plasmon modes and allow one to tailor electric fields on the nanoscale.
Recent experiments show that TMDC-PC hybrids can reach the strong-coupling
limit between excitons and plasmons, forming new quasiparticles, so-called
plexcitons. To describe this coupling theoretically, we develop a
self-consistent Maxwell-Bloch theory for TMDC-PC hybrid structures,
which allows us to compute the scattered light in the near- and far-fields
explicitly and provide guidance for experimental studies. One of the
key findings of the developed theory is the necessity to differentiate
between bright and originally momentum-dark excitons. Our calculations
reveal a spectral splitting signature of strong coupling of more than
100 meV in gold-MoSe2 structures with 30 nm nanoparticles,
manifesting in a hybridization of the plasmon mode with momentum-dark
excitons into two effective plexcitonic bands. The semianalytical
theory allows us to directly infer the characteristic asymmetric line
shape of the hybrid spectra in the strong coupling regime from the
energy distribution of the momentum-dark excitons. In addition to
the hybridized states, we find a remaining excitonic mode with significantly
smaller coupling to the plasmonic near-field, emitting directly into
the far-field. Thus, hybrid spectra in the strong coupling regime
can contain three emission peaks.
“…In the results Section , we choose the MNP and PC parameters to maximize the optical near-field of the PC, such that both resonances appear for the same frequency range. In this case, the collective interactions do not cause a narrow distinct peak, as focused on, e.g., in refs , , – , but rather amplify and sharpen the present MNP resonance.…”
Section: Theoretical Modelsupporting
confidence: 55%
“…Its distance dependency is depicted in the inset of Figure b, illustrating the (δ z ) −2 proportionality. To assign the hybrids to a particular coupling regime, the effective Rabi energy Ω eff ≠ 0 is compared with the line width γ ex and γ pl of the individual constituents. , A coupling strength leading to a peak splitting that is small compared to the line widths as, e.g., in the δ z = 17 nm , case is still assigned to weak coupling and has been observed in experiments with TMDCs coupled to a MNP or a PC in refs , , , and .…”
Section: Numerical Results and Discussionmentioning
Monolayers of transition
metal dichalcogenides (TMDCs)
are direct-gap
semiconductors with strong light–matter interactions featuring
tightly bound excitons, while plasmonic crystals (PCs), consisting
of metal nanoparticles that act as meta-atoms, exhibit collective
plasmon modes and allow one to tailor electric fields on the nanoscale.
Recent experiments show that TMDC-PC hybrids can reach the strong-coupling
limit between excitons and plasmons, forming new quasiparticles, so-called
plexcitons. To describe this coupling theoretically, we develop a
self-consistent Maxwell-Bloch theory for TMDC-PC hybrid structures,
which allows us to compute the scattered light in the near- and far-fields
explicitly and provide guidance for experimental studies. One of the
key findings of the developed theory is the necessity to differentiate
between bright and originally momentum-dark excitons. Our calculations
reveal a spectral splitting signature of strong coupling of more than
100 meV in gold-MoSe2 structures with 30 nm nanoparticles,
manifesting in a hybridization of the plasmon mode with momentum-dark
excitons into two effective plexcitonic bands. The semianalytical
theory allows us to directly infer the characteristic asymmetric line
shape of the hybrid spectra in the strong coupling regime from the
energy distribution of the momentum-dark excitons. In addition to
the hybridized states, we find a remaining excitonic mode with significantly
smaller coupling to the plasmonic near-field, emitting directly into
the far-field. Thus, hybrid spectra in the strong coupling regime
can contain three emission peaks.
“…This has mostly been demonstrated in steady-state measurements, 119,153,156 though there are limited reports of time-resolved studies focusing on such energy transport in Fabry-P erot cavities, BSWPs, and even cavity-free polaritons. 104,139,147,[157][158][159] Yet, the choice of materials, methods of characterization, and cavity architectures are sufficiently scattered that it remains unclear how to control these effects, and the field is in need of systematic investigations to understand the mechanisms underpinning polariton transport. Numerous steady-state studies have highlighted the potential of polariton-assisted energy transfer, with reported distances reaching up to 100's of micrometers.…”
Section: A Lateral Transport: Diffusive To Ballisticmentioning
confidence: 99%
“…However, a recently published set of time-resolved studies reveals a much more complicated picture. 104,139,147,[157][158][159] In each case, the polariton-assisted energy transport was studied using some variation of pump-probe microscopy (Fig. 12).…”
Section: A Lateral Transport: Diffusive To Ballisticmentioning
confidence: 99%
“…152 Initial studies indicated, however, that the observed transport velocities are orders of magnitude below the expected group velocity and that polariton transport cannot occur through a simple ballistic process. 104,139,147,[157][158][159] In one case, the population was found to expand linearly in time and subsequent analysis suggested that the transport was diffusive in nature [Fig. 13(a)].…”
Section: A Lateral Transport: Diffusive To Ballisticmentioning
Organic polaritonics has emerged as a captivating interdisciplinary field that marries the complexities of organic photophysics with the fundamental principles of quantum optics. By harnessing strong light–matter coupling in organic materials, exciton–polaritons offer unique opportunities for advanced device performance, including enhanced energy transport and low-threshold lasing, as well as new functionalities like polariton chemistry. In this review, we delve into the foundational principles of exciton–polaritons from an experimental perspective, highlighting the key states, processes, and timescales that govern polariton phenomena. Our review centers on the spectroscopy of exciton–polaritons. We overview the primary spectroscopic approaches that reveal polariton phenomena, and we discuss the challenges in disentangling polaritonic signatures from spectral artifacts. We discuss how organic materials, due to their complex photophysics and disordered nature, not only present challenges to the conventional polariton models but also provide opportunities for new physics, like manipulating dark electronic states. As the research field continues to grow, with increasingly complex materials and devices, this review serves as a valuable introductory guide for researchers navigating the intricate landscape of organic polaritonics.
Dynamic
metasurfaces have emerged as a disruptive change in the
way the response of optical systems can be tailored by combining the
flexibility of flat optics in spatially engineering materials at the
nanoscale with the opportunity to reconfigure the metasurfaces’
properties reversibly upon external stimuli over time. In this context,
the far-reaching interest in pushing the tuning speed has driven the
development of ‘ultrafast all-optical metasurfaces’
in which transient nonlinearities photoinduced by femtosecond laser
pulses empower to achieve GHz modulation rates. While holding great
promises to unlock forefront applications, the future frontiers of
this class of spatiotemporal all-optical metasurfaces are accompanied
by formidable challenges. In this Perspective, alongside a brief panorama
of the state of the art, we spotlight some of the emerging frontiers
for ultrafast light-driven metasurfaces, with special emphasis on
the all-optical control of light, the enhancement of light–matter
interactions, and the time-variant frequency conversion, in the hope
our vision will prompt new ideas and horizons to explore.
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