Research paper
Experimental CharacterizationComputational DFTEach sample groups how it was prepared, characterized, and measured. Click a card to expand.
2 preparations2 characterizations5 properties1 figure
1 preparation1 characterization4 properties1 figure
2 preparations2 characterizations3 properties1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Xrd Space Group | band alignment | type II hetero-interface | — | |||
| Fet Threshold Voltage | VB onset | -1.3V | — | |||
| Fet Threshold Voltage | CB onset | 1.7V | — | |||
| Fet Threshold Voltage | VB onset | -1.9V | — | |||
| Fet Threshold Voltage | CB onset | 1.4V | — | |||
| Pl Peak Intensity | trion contribution | 85% | — | |||
| PL Peak | exciton peak | not stated | — | |||
| PL Peak | trion peak | not stated | — | |||
| PL Peak | trion/charged-complex emission | shifts to lower energies upon hBN capping | — | |||
| Optical Band Gap | absorption strength | substantial oscillator strength in charged complexes | — | |||
| Raman Intensity Ratio | lineshape | trion emission broader than Gaussian or Lorentzian | — | |||
| Pl Peak Fwhm | PL peak | 8.3meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.8meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 6meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 0.5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 11.31meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 1.6meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 8.36meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.76meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.95meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.76meV | — | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Sub-nm range momentum-dependent exciton transfer from a 2D semiconductor to graphene
Optimizing strong light-matter coupling of plasmonic lattices and monolayer semiconductors
Non-linear and negative effective diffusivity of optical excitations in moiré-free heterobilayers
Dipolar interlayer excitons in transition metal dichalcogenide alloy heterobilayers
Twist-dependent intra- and interlayer excitons in moiré MoSe2 homobilayers
Förster energy transfer boosts indirect anisotropic interlayer excitons in 2L-MoSe2/perovskite heterostructures
Electrically Controlled Interfacial Charge Transfer Induced Excitons in MoSe2-WSe2 Lateral Heterostructure
Twisted MoSe2 Homobilayer Behaving as a Heterobilayer
Customising radiative decay dynamics of two-dimensional excitons via position- and polarisation-dependent vacuum-field interference
Strongly nonlinear nanocavity exciton-polaritons in gate-tunable monolayer semiconductors
Rydberg exciton states and near-infrared light-emitting diode in monolayer MoTe2 devices
Stacking Polarity–Controlled Interlayer Photocarrier Dynamics in MoSe2/MoS2 Heterostructures
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
2 preparations2 characterizations5 properties1 figure
1 preparation1 characterization4 properties1 figure
2 preparations2 characterizations3 properties1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Xrd Space Group | band alignment | type II hetero-interface | — | |||
| Fet Threshold Voltage | VB onset | -1.3V | — | |||
| Fet Threshold Voltage | CB onset | 1.7V | — | |||
| Fet Threshold Voltage | VB onset | -1.9V | — | |||
| Fet Threshold Voltage | CB onset | 1.4V | — | |||
| Pl Peak Intensity | trion contribution | 85% | — | |||
| PL Peak | exciton peak | not stated | — | |||
| PL Peak | trion peak | not stated | — | |||
| PL Peak | trion/charged-complex emission | shifts to lower energies upon hBN capping | — | |||
| Optical Band Gap | absorption strength | substantial oscillator strength in charged complexes | — | |||
| Raman Intensity Ratio | lineshape | trion emission broader than Gaussian or Lorentzian | — | |||
| Pl Peak Fwhm | PL peak | 8.3meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.8meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 6meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 0.5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 11.31meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 1.6meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 8.36meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.76meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.95meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.76meV | — | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Sub-nm range momentum-dependent exciton transfer from a 2D semiconductor to graphene
Optimizing strong light-matter coupling of plasmonic lattices and monolayer semiconductors
Non-linear and negative effective diffusivity of optical excitations in moiré-free heterobilayers
Dipolar interlayer excitons in transition metal dichalcogenide alloy heterobilayers
Twist-dependent intra- and interlayer excitons in moiré MoSe2 homobilayers
Förster energy transfer boosts indirect anisotropic interlayer excitons in 2L-MoSe2/perovskite heterostructures
Electrically Controlled Interfacial Charge Transfer Induced Excitons in MoSe2-WSe2 Lateral Heterostructure
Twisted MoSe2 Homobilayer Behaving as a Heterobilayer
Customising radiative decay dynamics of two-dimensional excitons via position- and polarisation-dependent vacuum-field interference
Strongly nonlinear nanocavity exciton-polaritons in gate-tunable monolayer semiconductors
Rydberg exciton states and near-infrared light-emitting diode in monolayer MoTe2 devices
Stacking Polarity–Controlled Interlayer Photocarrier Dynamics in MoSe2/MoS2 Heterostructures
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
2 preparations2 characterizations5 properties1 figure
1 preparation1 characterization4 properties1 figure
2 preparations2 characterizations3 properties1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Xrd Space Group | band alignment | type II hetero-interface | — | |||
| Fet Threshold Voltage | VB onset | -1.3V | — | |||
| Fet Threshold Voltage | CB onset | 1.7V | — | |||
| Fet Threshold Voltage | VB onset | -1.9V | — | |||
| Fet Threshold Voltage | CB onset | 1.4V | — | |||
| Pl Peak Intensity | trion contribution | 85% | — | |||
| PL Peak | exciton peak | not stated | — | |||
| PL Peak | trion peak | not stated | — | |||
| PL Peak | trion/charged-complex emission | shifts to lower energies upon hBN capping | — | |||
| Optical Band Gap | absorption strength | substantial oscillator strength in charged complexes | — | |||
| Raman Intensity Ratio | lineshape | trion emission broader than Gaussian or Lorentzian | — | |||
| Pl Peak Fwhm | PL peak | 8.3meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.8meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 6meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 0.5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 11.31meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 1.6meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 8.36meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.76meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.95meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.76meV | — | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Sub-nm range momentum-dependent exciton transfer from a 2D semiconductor to graphene
Optimizing strong light-matter coupling of plasmonic lattices and monolayer semiconductors
Non-linear and negative effective diffusivity of optical excitations in moiré-free heterobilayers
Dipolar interlayer excitons in transition metal dichalcogenide alloy heterobilayers
Twist-dependent intra- and interlayer excitons in moiré MoSe2 homobilayers
Förster energy transfer boosts indirect anisotropic interlayer excitons in 2L-MoSe2/perovskite heterostructures
Electrically Controlled Interfacial Charge Transfer Induced Excitons in MoSe2-WSe2 Lateral Heterostructure
Twisted MoSe2 Homobilayer Behaving as a Heterobilayer
Customising radiative decay dynamics of two-dimensional excitons via position- and polarisation-dependent vacuum-field interference
Strongly nonlinear nanocavity exciton-polaritons in gate-tunable monolayer semiconductors
Rydberg exciton states and near-infrared light-emitting diode in monolayer MoTe2 devices
Stacking Polarity–Controlled Interlayer Photocarrier Dynamics in MoSe2/MoS2 Heterostructures
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
2 preparations2 characterizations5 properties1 figure
1 preparation1 characterization4 properties1 figure
2 preparations2 characterizations3 properties1 figure
| Type | Label | Value | Material | Sample | Condition | Source |
|---|---|---|---|---|---|---|
| Xrd Space Group | band alignment | type II hetero-interface | — | |||
| Fet Threshold Voltage | VB onset | -1.3V | — | |||
| Fet Threshold Voltage | CB onset | 1.7V | — | |||
| Fet Threshold Voltage | VB onset | -1.9V | — | |||
| Fet Threshold Voltage | CB onset | 1.4V | — | |||
| Pl Peak Intensity | trion contribution | 85% | — | |||
| PL Peak | exciton peak | not stated | — | |||
| PL Peak | trion peak | not stated | — | |||
| PL Peak | trion/charged-complex emission | shifts to lower energies upon hBN capping | — | |||
| Optical Band Gap | absorption strength | substantial oscillator strength in charged complexes | — | |||
| Raman Intensity Ratio | lineshape | trion emission broader than Gaussian or Lorentzian | — | |||
| Pl Peak Fwhm | PL peak | 8.3meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.8meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 6meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 0.5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 11.31meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 5meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 1.6meV | — | — | — | |
| Pl Peak Fwhm | PL peak | 8.36meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.76meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 5.95meV | — | — | — | — |
| Pl Peak Fwhm | PL peak | 3.76meV | — | — | — | — |
Related documents with shared materials, methods, properties, or citations.
Sub-nm range momentum-dependent exciton transfer from a 2D semiconductor to graphene
Optimizing strong light-matter coupling of plasmonic lattices and monolayer semiconductors
Non-linear and negative effective diffusivity of optical excitations in moiré-free heterobilayers
Dipolar interlayer excitons in transition metal dichalcogenide alloy heterobilayers
Twist-dependent intra- and interlayer excitons in moiré MoSe2 homobilayers
Förster energy transfer boosts indirect anisotropic interlayer excitons in 2L-MoSe2/perovskite heterostructures
Electrically Controlled Interfacial Charge Transfer Induced Excitons in MoSe2-WSe2 Lateral Heterostructure
Twisted MoSe2 Homobilayer Behaving as a Heterobilayer
Customising radiative decay dynamics of two-dimensional excitons via position- and polarisation-dependent vacuum-field interference
Strongly nonlinear nanocavity exciton-polaritons in gate-tunable monolayer semiconductors
Rydberg exciton states and near-infrared light-emitting diode in monolayer MoTe2 devices
Stacking Polarity–Controlled Interlayer Photocarrier Dynamics in MoSe2/MoS2 Heterostructures