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. 2025 Apr 27;15(1):14706.
doi: 10.1038/s41598-025-96207-z.

Graphene-PbS quantum dot hybrid photodetectors from 200 mm wafer scale processing

Affiliations

Graphene-PbS quantum dot hybrid photodetectors from 200 mm wafer scale processing

Sha Li et al. Sci Rep. .

Abstract

A 200 mm processing platform for the large-scale production of graphene field-effect transistor-quantum dot (GFET-QD) hybrid photodetectors is demonstrated. A comprehensive statistical analysis of the electrical data revealed a high yield (96%) and low variation in the 200 mm scale fabrication. The GFET-QD devices deliver responsivities of 105 to 106 V/W in the wavelength range from 400 to 1800 nm with a response time of 10 ms. The spectral sensitivity compares well to that obtained via similar GFET-QD photodetectors. The device concept enables gate-tunable suppression or enhancement of the photovoltage, which may be exploited for electric shutter operation by toggling between the signal capture and shutter states. The devices show good stability over a wide operation range. Furthermore, an integration solution with complementary metal-oxide-semiconductor technology is presented to realize image-sensor-array chips and a proof-of-concept image system. This work demonstrates the potential for the volume manufacture of infrared photodetectors for a wide range of imaging applications.

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Conflict of interest statement

Competing interests: Z.W., B.R., D.N., and M.C.L. are employees of the non-profit company AMO GmbH. O.T., A.M., and A.Z. are employees of Graphenea S.A. C.B., A.R. Y.L. C.H., A.B., S.M. M.A. and I.M.-S. are employees of Emberion Limited. T.R. is an advisor of Emberion. The companies are working on the development and integration of electronic devices based on graphene and other nanomaterials.

Figures

Fig. 1
Fig. 1
(a) Schematic of the device architecture of the tandem GFET‒QD photodetector. (b) Schematic energy band diagram upon illumination. (c) Top-view optical microscope image of the tandem GFET‒QD photodetector device. (d) Fabrication flow of the GFET-QD photodetector, including the key steps of graphene transfer, patterning, contacting, QD deposition, encapsulation, and packaging. (e) As-fabricated 200 mm wafer (left) and later diced, wire-bonded, and packaged single-pixel photodetector in a hermetically sealed semiconductor package (right). (f–i) 200 mm wafer scale statistics of the electric metrics of encapsulated GFETs. Box-whisker plots of (f) Dirac points and hysteresis, (g) field effect mobility, (h) contact resistance, and (i) sheet resistance of the GFETs. Inset in (f): a photo of the 200 mm wafer after fabrication.
Fig. 2
Fig. 2
Electro-optical response of the GFET-QD photodetector. (a) Photovoltage emerging at the graphene‒QD junction shown against the Ids-Vgs curve of a GFET device (Vds = 0.5 V) with an irradiance level < 10–3 W/m2. (b) Photoresponse curves of the photodetector as a function of chopping frequency, with wavelengths of 520 and 1550 nm (Vds = 0.5 V, Vgs = -1.0 V). (c) Photoswitching behavior of the photodetector toward pulsed light illumination at a wavelength of 1550 nm, light intensity of 0.7 W/m2, Vgs = − 1.0 V and Vds = 0.5 V. (d) Photoresponse curves of the photodetector as a function of wavelength, with frequencies of 10 Hz and 100 Hz (Vds = 0.5 V, Vgs = − 1.0 V).
Fig. 3
Fig. 3
Tandem GFET-QD image sensor. (a) Schematic of a single-pixel photodetector device prior to hermetic sealing into a metal T0-8 semiconductor package with a sapphire window. (b) A single pixel photodetector after hermetic sealing of the sapphire window and connection to a dedicated readout electronics board. (c) Photograph of a few-pixel GFET array fabricated directly on an ASIC and subsequently wire bonded and hermetically sealed into a QFN package. Corresponding photoresponse of the few-pixel array measured through the ASIC at back gate voltages of Vgs = (d) − 1.4 V and (e) − 0.5 V, λ = 1550 nm, P = 0.7 W/m2, Vds = 0.5 V. Units are arbitrary digital values from the DAC output of the ROIC.

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