Research paper
Experimental CharacterizationEach sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation5 characterizations6 properties6 figures
1 preparation2 characterizations1 property4 figures
1 preparation2 characterizations2 properties4 figures
1 preparation1 characterization1 figure
1 preparation1 characterization1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| PL Peak | X | 2.62eV | — | |||
| PL Peak | X₀/X- quenched in heterostructure | 2.33eV | — | |||
| PL Peak | IX | 1.89eV | — | |||
| Pl Peak Fwhm | IX | 130meV | — | |||
| Absorption Peak | X absorption peak | 2.37eV | — | |||
| Dr Feature Position | A exciton PLE resonance | 2.04eV | — | |||
| Dr Feature Position | X exciton PLE resonance | 2.42eV | — | |||
| Dr Feature Position | C exciton PLE resonance | 2.88eV | — | |||
| Pl Peak Shift | valley polarization ON/OFF ratio | 15.8 | — |
Related documents with shared materials, methods, properties, or citations.
Anomalous optical valley Hall dynamics of exciton-polaritions
Ultrafast Spatial Hole Burning Dynamics in Monolayer WS2: Insights from Time-resolved Photoluminescence Spectroscopy
Optical Control of Fluorescence Spatial Hole Burning Effect in Monolayer WS2
Gas pressure manipulation of exciton states in monolayer WS2
Strongly enhanced light-matter coupling of a monolayer WS2 from a bound state in the continuum
Floquet engineering of strongly-driven excitons in monolayer tungsten disulfide
Erbium-implanted WS2 flakes with room-temperature photon emission at telecom wavelengths
Large-Area Deterministic Stamping of 2D Materials on Arbitrarily Patterned Surfaces
Ultrathin Ga2O3 Tunneling Contact for 2D Transition-metal Dichalcogenides Transistor
Layered semiconductors integrated with polyimide thin films for high-quality valleytronic and quantum-photonic systems
High-Temperature Activation of Single-Photon Emitters in monolayer WS2
Electrical control of valley polarized charged biexcitons in monolayer WS2
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation5 characterizations6 properties6 figures
1 preparation2 characterizations1 property4 figures
1 preparation2 characterizations2 properties4 figures
1 preparation1 characterization1 figure
1 preparation1 characterization1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| PL Peak | X | 2.62eV | — | |||
| PL Peak | X₀/X- quenched in heterostructure | 2.33eV | — | |||
| PL Peak | IX | 1.89eV | — | |||
| Pl Peak Fwhm | IX | 130meV | — | |||
| Absorption Peak | X absorption peak | 2.37eV | — | |||
| Dr Feature Position | A exciton PLE resonance | 2.04eV | — | |||
| Dr Feature Position | X exciton PLE resonance | 2.42eV | — | |||
| Dr Feature Position | C exciton PLE resonance | 2.88eV | — | |||
| Pl Peak Shift | valley polarization ON/OFF ratio | 15.8 | — |
Related documents with shared materials, methods, properties, or citations.
Anomalous optical valley Hall dynamics of exciton-polaritions
Ultrafast Spatial Hole Burning Dynamics in Monolayer WS2: Insights from Time-resolved Photoluminescence Spectroscopy
Optical Control of Fluorescence Spatial Hole Burning Effect in Monolayer WS2
Gas pressure manipulation of exciton states in monolayer WS2
Strongly enhanced light-matter coupling of a monolayer WS2 from a bound state in the continuum
Floquet engineering of strongly-driven excitons in monolayer tungsten disulfide
Erbium-implanted WS2 flakes with room-temperature photon emission at telecom wavelengths
Large-Area Deterministic Stamping of 2D Materials on Arbitrarily Patterned Surfaces
Ultrathin Ga2O3 Tunneling Contact for 2D Transition-metal Dichalcogenides Transistor
Layered semiconductors integrated with polyimide thin films for high-quality valleytronic and quantum-photonic systems
High-Temperature Activation of Single-Photon Emitters in monolayer WS2
Electrical control of valley polarized charged biexcitons in monolayer WS2
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation5 characterizations6 properties6 figures
1 preparation2 characterizations1 property4 figures
1 preparation2 characterizations2 properties4 figures
1 preparation1 characterization1 figure
1 preparation1 characterization1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| PL Peak | X | 2.62eV | — | |||
| PL Peak | X₀/X- quenched in heterostructure | 2.33eV | — | |||
| PL Peak | IX | 1.89eV | — | |||
| Pl Peak Fwhm | IX | 130meV | — | |||
| Absorption Peak | X absorption peak | 2.37eV | — | |||
| Dr Feature Position | A exciton PLE resonance | 2.04eV | — | |||
| Dr Feature Position | X exciton PLE resonance | 2.42eV | — | |||
| Dr Feature Position | C exciton PLE resonance | 2.88eV | — | |||
| Pl Peak Shift | valley polarization ON/OFF ratio | 15.8 | — |
Related documents with shared materials, methods, properties, or citations.
Anomalous optical valley Hall dynamics of exciton-polaritions
Ultrafast Spatial Hole Burning Dynamics in Monolayer WS2: Insights from Time-resolved Photoluminescence Spectroscopy
Optical Control of Fluorescence Spatial Hole Burning Effect in Monolayer WS2
Gas pressure manipulation of exciton states in monolayer WS2
Strongly enhanced light-matter coupling of a monolayer WS2 from a bound state in the continuum
Floquet engineering of strongly-driven excitons in monolayer tungsten disulfide
Erbium-implanted WS2 flakes with room-temperature photon emission at telecom wavelengths
Large-Area Deterministic Stamping of 2D Materials on Arbitrarily Patterned Surfaces
Ultrathin Ga2O3 Tunneling Contact for 2D Transition-metal Dichalcogenides Transistor
Layered semiconductors integrated with polyimide thin films for high-quality valleytronic and quantum-photonic systems
High-Temperature Activation of Single-Photon Emitters in monolayer WS2
Electrical control of valley polarized charged biexcitons in monolayer WS2
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
1 preparation5 characterizations6 properties6 figures
1 preparation2 characterizations1 property4 figures
1 preparation2 characterizations2 properties4 figures
1 preparation1 characterization1 figure
1 preparation1 characterization1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| PL Peak | X | 2.62eV | — | |||
| PL Peak | X₀/X- quenched in heterostructure | 2.33eV | — | |||
| PL Peak | IX | 1.89eV | — | |||
| Pl Peak Fwhm | IX | 130meV | — | |||
| Absorption Peak | X absorption peak | 2.37eV | — | |||
| Dr Feature Position | A exciton PLE resonance | 2.04eV | — | |||
| Dr Feature Position | X exciton PLE resonance | 2.42eV | — | |||
| Dr Feature Position | C exciton PLE resonance | 2.88eV | — | |||
| Pl Peak Shift | valley polarization ON/OFF ratio | 15.8 | — |
Related documents with shared materials, methods, properties, or citations.
Anomalous optical valley Hall dynamics of exciton-polaritions
Ultrafast Spatial Hole Burning Dynamics in Monolayer WS2: Insights from Time-resolved Photoluminescence Spectroscopy
Optical Control of Fluorescence Spatial Hole Burning Effect in Monolayer WS2
Gas pressure manipulation of exciton states in monolayer WS2
Strongly enhanced light-matter coupling of a monolayer WS2 from a bound state in the continuum
Floquet engineering of strongly-driven excitons in monolayer tungsten disulfide
Erbium-implanted WS2 flakes with room-temperature photon emission at telecom wavelengths
Large-Area Deterministic Stamping of 2D Materials on Arbitrarily Patterned Surfaces
Ultrathin Ga2O3 Tunneling Contact for 2D Transition-metal Dichalcogenides Transistor
Layered semiconductors integrated with polyimide thin films for high-quality valleytronic and quantum-photonic systems
High-Temperature Activation of Single-Photon Emitters in monolayer WS2
Electrical control of valley polarized charged biexcitons in monolayer WS2