Abstract:Three-dimensional confinement allows semiconductor quantum dots to exhibit size-tunable electronic and optical properties that enable a wide range of opto-electronic applications from displays, solar cells and bio-medical imaging to single-electron devices. Additional modalities such as spin and valley properties in monolayer transition metal dichalcogenides provide further degrees of freedom requisite for information processing and spintronics. In nanostructures, however, spatial confinement can cause hybridi… Show more
“…35 This may be due to the limitation in the synthesis of TMD quantum dots. [37][38][39][40][41][42][43] The majority of the reports on TMD quantum dots have focused on the optical properties. [39][40][41]43 The phonon confinement effect manifests behavior similar to the shifting behavior of the phonon modes due to the layered effect, depending on the nature of the phonon dispersion.…”
Several phenomena can affect the phonon bands of low-dimensional systems, and their proper assignment and interpretation are essential in elucidating their effect on electronic, optical, and optoelectronic properties. Using an analytical approach, we investigate the similarities and differences of the layered effect, the phonon confinement effect, the Breit-Wigner-Fano effect, the inhomogeneous heating effect, and disorder-induced effects in the phonon line shapes of WS 2 and MoS 2. The subtle differences and similarities are critical in making proper assignments and interpretations of the phonon line shapes and are useful as guidance in the behavior of phonon bands, particularly in TMDs, and more generally in low-dimensional systems.
“…35 This may be due to the limitation in the synthesis of TMD quantum dots. [37][38][39][40][41][42][43] The majority of the reports on TMD quantum dots have focused on the optical properties. [39][40][41]43 The phonon confinement effect manifests behavior similar to the shifting behavior of the phonon modes due to the layered effect, depending on the nature of the phonon dispersion.…”
Several phenomena can affect the phonon bands of low-dimensional systems, and their proper assignment and interpretation are essential in elucidating their effect on electronic, optical, and optoelectronic properties. Using an analytical approach, we investigate the similarities and differences of the layered effect, the phonon confinement effect, the Breit-Wigner-Fano effect, the inhomogeneous heating effect, and disorder-induced effects in the phonon line shapes of WS 2 and MoS 2. The subtle differences and similarities are critical in making proper assignments and interpretations of the phonon line shapes and are useful as guidance in the behavior of phonon bands, particularly in TMDs, and more generally in low-dimensional systems.
“…Indeed, any disorder in 2D structures leads to the localization of the charge carrier wavefunction [33][34][35], which increases the spin and valley coherence times. In TMD MLs the charge carrier localization can be reached by means of the chemical exfoliation [36][37][38], lithographic nanopatterning [39], wrinkles [40], homojunctions [41], or defects [42][43][44].…”
Localization of charge carriers in monolayers (MLs) of transition metal dichalcogenides (TMDs) dramatically increases spin and valley coherence times, and, by analogy with other systems, the role of the hyperfine interaction should enhance. We perform theoretical analysis of the intervalley hyperfine interaction in TMD MLs based on the group representation theory. We demonstrate, that the spin-valley locking leads to the helical structure of the in-plane hyperfine interaction. In the upper valence band the hyperfine interaction is shown to be of the Ising type, which can be used for fabrication of the atomically thin quantum dots with the long spin and valley coherence times.
“…[4][5][6] The 2D host materials have the advantage of being cost efficient, with highly tunable properties 3,7 and optical access to the electron valley index in momentum space, 8,9 an additional degree of freedom compared to other solid state qubits in III-V quantum dots (QDs) or NV centres in diamond, for example. There are several approaches to achieve 3D quantum confinement, such as patterning TMD MLs, 10 chemically synthesized TMD nano-crystals, [11][12][13][14][15][16] and defect engineering. [17][18][19][20] In photoluminescence (PL) experiments at T ¼ 4 K, we observe QD-like, discrete emission lines (full width at half maximum (FWHM) typ.…”
Transition metal dichalcogenide monolayers such as MoSe2,MoS2 and WSe2 are direct bandgap semiconductors with original optoelectronic and spin-valley properties. Here we report spectrally sharp, spatially localized emission in monolayer MoSe2. We find this quantum dot like emission in samples exfoliated onto gold substrates and also suspended flakes. Spatial mapping shows a correlation between the location of emitters and the existence of wrinkles (strained regions) in the flake. We tune the emission properties in magnetic and electric fields applied perpendicular to the monolayer plane. We extract an exciton g-factor of the discrete emitters close to -4, as for 2D excitons in this material. In a charge tunable sample we record discrete jumps on the meV scale as charges are added to the emitter when changing the applied voltage.
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