Room-temperature adjustable sub-Terahertz wave detector and preparation method
A hertz wave and detector technology, applied in the field of light guide-like and photovoltaic-like detection, can solve the problems of limiting device bandwidth and speed, high noise, low sensitivity, etc., and achieve the effect of improving miniaturization, improving integration, and avoiding strong reflection
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Embodiment 1
[0052] The thickness of the sapphire substrate is 1mm, when the outer radius of the logarithmic periodic antenna is 1mm, the arc is 50°, the line width of the split gate is 1μm, the line spacing is 500nm, the thickness of the aluminum oxide gate dielectric layer is 30nm, and the conductive channel CVD graphene with a length of 5μm (concentration about 10 13 cm -2 , the mobility is about 1000~5000cm 2 V -1 the s -1 ). Such as image 3 As shown, the electrical performance of the graphene field effect tube is good, and the gate control realizes the doping of graphene P and N types, and the voltage of the Dirac point is around 1.8-2V; from image 3 It can be seen from the inset that the graphene and the log-periodic antenna form a good ohmic contact, laying the foundation for the device for sub-terahertz wave detection.
Embodiment 2
[0054] The thickness of the sapphire substrate is 1mm, when the outer radius of the logarithmic periodic antenna is 2mm, the arc is 50°, the line width of the split grid is 2μm, the line spacing is 600nm, the thickness of the aluminum oxide gate dielectric layer is 50nm, and the conductive channel CVD graphene with a length of 6μm (concentration about 10 13 cm -2 , the mobility is about 1000~5000cm 2 V -1 the s -1 ),Such as Figure 4 As shown, the change of photocurrent was observed in real time under the irradiation of sub-sub-Hz wave of 0.02-0.4 THz by semiconductor analyzer. It can also be seen that the gate voltage control realizes different doping types of graphene. Compared with the dark current, the resistance of P-type doped graphene becomes larger and the photocurrent becomes smaller, while the resistance of N-type doped graphene is small and the current becomes smaller. large; and the change trend of the photocurrent amplitude of the two types of doped graphene ...
Embodiment 3
[0056] The thickness of the sapphire substrate is 0.5mm, when the outer radius of the logarithmic periodic antenna is 1mm, the arc is 50°, the line width of the split gate is 2.2μm, the line spacing is 600nm, the thickness of the aluminum oxide gate dielectric layer is 30nm, and the conductive channel CVD with a length of 10μm Graphene (concentration about 10 13 cm -2 , the mobility is about 1000~5000cm 2 V -1 the s -1 ), under zero bias voltage and sub-terahertz irradiation, the device generates photocurrent, which is similar to a photovoltaic device and has a high signal-to-noise ratio; as the bias voltage increases, it is similar to a photoconductive device, and the photoresponse also increases. It is consistent with the photoconductive type results of the detectors at both ends of the graphene antenna.
[0057] Various parameters in the detector structure change within a certain range. A room temperature-adjustable sub-terahertz wave detector in the present invention h...
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