研究目的
Investigating the photodetection performance of graphene–WS2–Si van der Waals heterostructure for application in high performance broadband photodetectors.
研究成果
The graphene–WS2–Si heterostructure photodetector exhibits high photoresponsivity, high specific detectivity, and fast response, making it suitable for high performance broadband photodetectors. The simple fabrication method also suggests potential for large scale device integration.
研究不足
The study is limited by the measurement system's capability to cover the full spectrum response, and the photoresponsivity decreases with the increase of the lateral size of the junction area due to increased recombination possibilities.
1:Experimental Design and Method Selection:
The study involves the fabrication and characterization of graphene–WS2–Si heterostructure photodetectors. The methodology includes photolithography, etching, sulfurization of WO3 film, transfer of graphene, and deposition of electrodes to realize the van der Waals heterostructure.
2:Sample Selection and Data Sources:
An n-type Si wafer with 285 nm thermally oxidized SiO2 was used as the substrate.
3:List of Experimental Equipment and Materials:
AFM (FM-Nanoview1000), SEM (VEGA3 SBH, TESCAN), Raman spectrometer (Andor, SR-5001-A-R), Agilent B2902A, supercontinuum source white light laser (SC-PRO, YSL Photonics), acousto-optic monochromator (AOTF-PRO, YSL Photonics), power meter (1935-C, Newport), mechanical chopper (SR540, Stanford Research Systems), oscilloscope (TDS 3054B, Tektronix), low-noise current amplifier (SR570, Stanford Research Systems), lock-in amplifier (SR830, Stanford Research Systems).
4:Experimental Procedures and Operational Workflow:
The fabrication process includes defining the contact region with WS2, depositing WO3 film, sulfurizing it into WS2, depositing Ag electrode, and transferring single layer graphene on the WS2 film. Electrical properties and photoresponse were measured in a probe station.
5:Data Analysis Methods:
The photocurrent and photoresponsivity were analyzed as functions of light intensity and wavelength. The response time was determined from time-resolved current measurements under modulated light irradiation.
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Oscilloscope
TDS 3054B
Tektronix
Tracing the fast variation of the voltage with time
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Low-noise current amplifier
SR570
Stanford Research Systems
Extracting the photocurrent during the scan
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Lock-in amplifier
SR830
Stanford Research Systems
Extracting the photocurrent during the scan
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Raman spectrometer
SR-5001-A-R
Andor
Measuring the Raman spectra of the heterostructure
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Source and measurement units
B2902A
Agilent
Measuring electrical properties and photoresponse
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Supercontinuum source white light laser
SC-PRO
YSL Photonics
Light source for measurements
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Acousto-optic monochromator
AOTF-PRO
YSL Photonics
Modulating light for measurements
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Mechanical chopper
SR540
Stanford Research Systems
Modulating incident light
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AFM
FM-Nanoview1000
Suzhou Flying Man Precision Instrument
Characterizing the surface roughness of heterostructure
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SEM
VEGA3 SBH
TESCAN
Measuring the morphology of the heterostructure
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Power meter
1935-C
Newport
Measuring light intensity
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