Research paper
Experimental CharacterizationEach sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation2 characterizations4 properties2 figures
2 preparations2 characterizations2 properties2 figures
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Optical Refractive Index | effective refractive index neff | 1.517 | — | |||
| Peak Energy | surface lattice resonance energy | 1.7eV | — | |||
| Peak Fwhm | surface lattice resonance linewidth | 27meV | — | |||
| Quality Factor | surface lattice resonance Q | 32 | — | |||
| Coupling Strength | light-matter coupling strength g | 25meV | — | |||
| Rabi Splitting | Rabi splitting Ω | 44meV | — | |||
| Pl Peak Fwhm | PL peak | 27meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 25meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 3.5meV | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Electrical Tuning of Neutral and Charged Excitons with 1-nm Gate
Proximity Induced Chiral Quantum Light Generation in Strain-Engineered WSe2/NiPS3 Heterostructures
Observation of Γ-valley moiré bands and emergent hexagonal lattice in twisted transition metal dichalcogenides
Tunable phononic coupling in excitonic quantum emitters
Spatial filtering of interlayer exciton ground state in WSe2/MoS2 heterobilayer
Ultra Localized Optoelectronic Properties of Nanobubbles in 2D Semiconductors
Voltage-Induced Oxidation for Enhanced Purity and Reproducibility of Quantum Emission in Monolayer 2D Materials
Programmable Nanowrinkle-Induced Room-Temperature Exciton Localization in Monolayer WSe2
Nanoscale confinement and control of excitonic complexes in a monolayer WSe2
Enhanced Polarizability and Tunable Diamagnetic Shifts from Charged Localized Emitters in WSe2 on a Relaxor Ferroelectric
Moiré-Engineered Excitonic Landscape and Phonon-Mediated Recombination in Twisted WSe2 Bilayers
Resonant exciton transfer in mixed-dimensional heterostructures for overcoming dimensional restrictions in optical processes
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation2 characterizations4 properties2 figures
2 preparations2 characterizations2 properties2 figures
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Optical Refractive Index | effective refractive index neff | 1.517 | — | |||
| Peak Energy | surface lattice resonance energy | 1.7eV | — | |||
| Peak Fwhm | surface lattice resonance linewidth | 27meV | — | |||
| Quality Factor | surface lattice resonance Q | 32 | — | |||
| Coupling Strength | light-matter coupling strength g | 25meV | — | |||
| Rabi Splitting | Rabi splitting Ω | 44meV | — | |||
| Pl Peak Fwhm | PL peak | 27meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 25meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 3.5meV | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Electrical Tuning of Neutral and Charged Excitons with 1-nm Gate
Proximity Induced Chiral Quantum Light Generation in Strain-Engineered WSe2/NiPS3 Heterostructures
Observation of Γ-valley moiré bands and emergent hexagonal lattice in twisted transition metal dichalcogenides
Tunable phononic coupling in excitonic quantum emitters
Spatial filtering of interlayer exciton ground state in WSe2/MoS2 heterobilayer
Ultra Localized Optoelectronic Properties of Nanobubbles in 2D Semiconductors
Voltage-Induced Oxidation for Enhanced Purity and Reproducibility of Quantum Emission in Monolayer 2D Materials
Programmable Nanowrinkle-Induced Room-Temperature Exciton Localization in Monolayer WSe2
Nanoscale confinement and control of excitonic complexes in a monolayer WSe2
Enhanced Polarizability and Tunable Diamagnetic Shifts from Charged Localized Emitters in WSe2 on a Relaxor Ferroelectric
Moiré-Engineered Excitonic Landscape and Phonon-Mediated Recombination in Twisted WSe2 Bilayers
Resonant exciton transfer in mixed-dimensional heterostructures for overcoming dimensional restrictions in optical processes
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation2 characterizations4 properties2 figures
2 preparations2 characterizations2 properties2 figures
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Optical Refractive Index | effective refractive index neff | 1.517 | — | |||
| Peak Energy | surface lattice resonance energy | 1.7eV | — | |||
| Peak Fwhm | surface lattice resonance linewidth | 27meV | — | |||
| Quality Factor | surface lattice resonance Q | 32 | — | |||
| Coupling Strength | light-matter coupling strength g | 25meV | — | |||
| Rabi Splitting | Rabi splitting Ω | 44meV | — | |||
| Pl Peak Fwhm | PL peak | 27meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 25meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 3.5meV | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Electrical Tuning of Neutral and Charged Excitons with 1-nm Gate
Proximity Induced Chiral Quantum Light Generation in Strain-Engineered WSe2/NiPS3 Heterostructures
Observation of Γ-valley moiré bands and emergent hexagonal lattice in twisted transition metal dichalcogenides
Tunable phononic coupling in excitonic quantum emitters
Spatial filtering of interlayer exciton ground state in WSe2/MoS2 heterobilayer
Ultra Localized Optoelectronic Properties of Nanobubbles in 2D Semiconductors
Voltage-Induced Oxidation for Enhanced Purity and Reproducibility of Quantum Emission in Monolayer 2D Materials
Programmable Nanowrinkle-Induced Room-Temperature Exciton Localization in Monolayer WSe2
Nanoscale confinement and control of excitonic complexes in a monolayer WSe2
Enhanced Polarizability and Tunable Diamagnetic Shifts from Charged Localized Emitters in WSe2 on a Relaxor Ferroelectric
Moiré-Engineered Excitonic Landscape and Phonon-Mediated Recombination in Twisted WSe2 Bilayers
Resonant exciton transfer in mixed-dimensional heterostructures for overcoming dimensional restrictions in optical processes
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation2 characterizations4 properties2 figures
2 preparations2 characterizations2 properties2 figures
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Optical Refractive Index | effective refractive index neff | 1.517 | — | |||
| Peak Energy | surface lattice resonance energy | 1.7eV | — | |||
| Peak Fwhm | surface lattice resonance linewidth | 27meV | — | |||
| Quality Factor | surface lattice resonance Q | 32 | — | |||
| Coupling Strength | light-matter coupling strength g | 25meV | — | |||
| Rabi Splitting | Rabi splitting Ω | 44meV | — | |||
| Pl Peak Fwhm | PL peak | 27meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 25meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 3.5meV | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Electrical Tuning of Neutral and Charged Excitons with 1-nm Gate
Proximity Induced Chiral Quantum Light Generation in Strain-Engineered WSe2/NiPS3 Heterostructures
Observation of Γ-valley moiré bands and emergent hexagonal lattice in twisted transition metal dichalcogenides
Tunable phononic coupling in excitonic quantum emitters
Spatial filtering of interlayer exciton ground state in WSe2/MoS2 heterobilayer
Ultra Localized Optoelectronic Properties of Nanobubbles in 2D Semiconductors
Voltage-Induced Oxidation for Enhanced Purity and Reproducibility of Quantum Emission in Monolayer 2D Materials
Programmable Nanowrinkle-Induced Room-Temperature Exciton Localization in Monolayer WSe2
Nanoscale confinement and control of excitonic complexes in a monolayer WSe2
Enhanced Polarizability and Tunable Diamagnetic Shifts from Charged Localized Emitters in WSe2 on a Relaxor Ferroelectric
Moiré-Engineered Excitonic Landscape and Phonon-Mediated Recombination in Twisted WSe2 Bilayers
Resonant exciton transfer in mixed-dimensional heterostructures for overcoming dimensional restrictions in optical processes
figure_digitization.json#Figure 3(a)figure_digitization.json#Figure 3(b)figure_digitization.json#Figure 3(c)figure_digitization.json#Figure 3(d)figure_digitization.json#Figure 3(f)figure_digitization.json#Figure 3(g)figure_digitization.json#Figure 3(h)figure_digitization.json#Figure 3(a)figure_digitization.json#Figure 3(b)figure_digitization.json#Figure 3(c)figure_digitization.json#Figure 3(d)figure_digitization.json#Figure 3(f)figure_digitization.json#Figure 3(g)figure_digitization.json#Figure 3(h)figure_digitization.json#Figure 3(a)figure_digitization.json#Figure 3(b)figure_digitization.json#Figure 3(c)figure_digitization.json#Figure 3(d)figure_digitization.json#Figure 3(f)figure_digitization.json#Figure 3(g)figure_digitization.json#Figure 3(h)figure_digitization.json#Figure 3(a)figure_digitization.json#Figure 3(b)figure_digitization.json#Figure 3(c)figure_digitization.json#Figure 3(d)figure_digitization.json#Figure 3(f)figure_digitization.json#Figure 3(g)figure_digitization.json#Figure 3(h)