2018
DOI: 10.1038/s41467-018-04866-6
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Two-dimensional semiconductors in the regime of strong light-matter coupling

Abstract: The optical properties of transition metal dichalcogenide monolayers are widely dominated by excitons, Coulomb-bound electron–hole pairs. These quasi-particles exhibit giant oscillator strength and give rise to narrow-band, well-pronounced optical transitions, which can be brought into resonance with electromagnetic fields in microcavities and plasmonic nanostructures. Due to the atomic thinness and robustness of the monolayers, their integration in van der Waals heterostructures provides unique opportunities … Show more

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Cited by 334 publications
(309 citation statements)
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References 113 publications
(158 reference statements)
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“…Literature on optoelectronics based on TMDCs is growing rapidly every year with reports on single material and heterostructure devices. Enhanced light-matter interaction even at monolayer thickness along with a direct bandgap and mechanical flexibility gives clear advantage over silicon (Si) technology [6,26]. Optoelectronic devices such as photodetectors, photovoltaics, light-emitting devices and optical modulators have been demonstrated using TMDCs across a wide range of device architectures and measurement methodologies [4,27,28].…”
mentioning
confidence: 99%
“…Literature on optoelectronics based on TMDCs is growing rapidly every year with reports on single material and heterostructure devices. Enhanced light-matter interaction even at monolayer thickness along with a direct bandgap and mechanical flexibility gives clear advantage over silicon (Si) technology [6,26]. Optoelectronic devices such as photodetectors, photovoltaics, light-emitting devices and optical modulators have been demonstrated using TMDCs across a wide range of device architectures and measurement methodologies [4,27,28].…”
mentioning
confidence: 99%
“…Constructing a strong coupling system requires the quantum emitter with large transition momentum, which perfectly matches the advantage of strong excitonic effect in 2DLMs . Therefore, with the employment of 2DLMs, numbers of investigations with novel observations in the field of strong coupling are performed . Figure c illustrates the representative strong coupling systems constructed by 2DLMs and plasmonic nanocavities, where the TMDs together with a single plasmonic nanostructure or the nanoparticle on nanofilm structure are chosen .…”
Section: Outlook and Discussionmentioning
confidence: 99%
“…For more comprehensive reviews about various types of polaritons in the entire vdW and 2D material family, please refer to the following reviews . There is also an earlier review paper that focuses on the studies of strong light‐matter coupling in 2D semiconductors by 2017 . In the following sections of the paper, we will first discuss the generic dispersion properties of EPs and the experimental techniques that are used to probe EPs.…”
Section: Introductionmentioning
confidence: 99%
“…To understand the dispersion relations of the three polaritonic branches of the EPs, it is useful to write down the dielectric function of exciton resonance ε(ω,k) = ε1 + iε2 = ε + (ωL2 ωT2)εωT2 ω2 + ωTk2/Mx 2iωγex where ω T and ω L are the transverse and longitudinal resonance frequencies at zero momentum ( k = 0), ω is the angular frequency of the excitation optical beam, ε ∞ is the background dielectric constant, γ ex is exciton decay rate, the term ħω T k 2 /M x describes the spatial dispersion of excitons (exciton energies increases at higher momentum) that is normally quite small in the experiment accessible momentum regime, M x = m e + m h is the translation mass of exciton, and ħ is the reduced Planck constant. Note that the realistic dielectric function (Figure d) consists of multiple exciton resonances like Equation as well as a huge background contribution from interband transitions.…”
Section: Introductionmentioning
confidence: 99%