2017
DOI: 10.1038/ncomms14776
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Proposal for dark exciton based chemical sensors

Abstract: The rapidly increasing use of sensors throughout different research disciplines and the demand for more efficient devices with less power consumption depends critically on the emergence of new sensor materials and novel sensor concepts. Atomically thin transition metal dichalcogenides have a huge potential for sensor development within a wide range of applications. Their optimal surface-to-volume ratio combined with strong light–matter interaction results in a high sensitivity to changes in their surroundings.… Show more

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Cited by 88 publications
(83 citation statements)
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“…Recent theoretical studies have addressed dark excitons [20,22] using first-principles calculations, however, theory for dark and bright trions has so far exclusively been based on models [23][24][25]. We note that Feierabend et al [26] proposed further dark excitons with nonzero momenta. Here, we focus on excitation around ±K.…”
Section: Dark Excitations In Monolayer Transition Metal Dichalcogenidesmentioning
confidence: 99%
“…Recent theoretical studies have addressed dark excitons [20,22] using first-principles calculations, however, theory for dark and bright trions has so far exclusively been based on models [23][24][25]. We note that Feierabend et al [26] proposed further dark excitons with nonzero momenta. Here, we focus on excitation around ±K.…”
Section: Dark Excitations In Monolayer Transition Metal Dichalcogenidesmentioning
confidence: 99%
“…Now, we include excitonic effects and investigate how they change in presence of bi-and uniaxial strain. Excitons are integrated by solving the Wannier equation, providing access to eigenvalues and eigenfunctions for all available excitonic states [2,[20][21][22][23]. Furthermore, we derive the TMD Bloch equation for the microscopic polarization p…”
Section: Excitonic Effectsmentioning
confidence: 99%
“…Here, we have applied a separation ansatz decoupling the relative from the center-ofmass motion with the corresponding center-of-mass momentum Q and relative momentum q with Q = k 2 − k 1 and q = [18,59,60] and the electron (hole) occupations f e(h) q .In the next step, we solve the hybrid Bloch equations for the excitonic microscopic polarization p μ Q with the index μ = (K , ) denoting the K K and K exciton: [23] …”
Section: Functionalized Transition Metal Dichalcogenidesmentioning
confidence: 99%
“…The dark K exciton is only driven in the presence of molecules, which couple to the TMD excitons via the induced dipole field. The corresponding exciton-molecule coupling element reads in excitonic basis [23] …”
Section: Functionalized Transition Metal Dichalcogenidesmentioning
confidence: 99%
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