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Evaporated Se x Te 1‐ x Thin Films with Tunable Bandgaps for Short‐Wave Infrared Photodetectors
Author(s) -
Tan Chaoliang,
Amani Matin,
Zhao Chunsong,
Hettick Mark,
Song Xiaohui,
Lien DerHsien,
Li Hao,
Yeh Matthew,
Shrestha Vivek Raj,
Crozier Kenneth B.,
Scott Mary C.,
Javey Ali
Publication year - 2020
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.202001329
Subject(s) - responsivity , materials science , photodetector , optoelectronics , specific detectivity , fabrication , thin film , infrared , band gap , absorption edge , optics , substrate (aquarium) , absorption (acoustics) , semiconductor , nanotechnology , medicine , oceanography , alternative medicine , physics , pathology , geology , composite material
Abstract Semiconducting absorbers in high‐performance short‐wave infrared (SWIR) photodetectors and imaging sensor arrays are dominated by single‐crystalline germanium and III–V semiconductors. However, these materials require complex growth and device fabrication procedures. Here, thermally evaporated Se x Te 1‐ x alloy thin films with tunable bandgaps for the fabrication of high‐performance SWIR photodetectors are reported. From absorption measurements, it is shown that the bandgaps of Se x Te 1‐ x films can be tuned continuously from 0.31 eV (Te) to 1.87 eV (Se). Owing to their tunable bandgaps, the peak responsivity position and photoresponse edge of Se x Te 1‐ x film‐based photoconductors can be tuned in the SWIR regime. By using an optical cavity substrate consisting of Au/Al 2 O 3 to enhance its absorption near the bandgap edge, the Se 0.32 Te 0.68 film (an optical bandgap of ≈0.8 eV)‐based photoconductor exhibits a cut‐off wavelength at ≈1.7 μm and gives a responsivity of 1.5 AW −1 and implied detectivity of 6.5 × 10 10 cm Hz 1/2 W −1 at 1.55 μm at room temperature. Importantly, the nature of the thermal evaporation process enables the fabrication of Se 0.32 Te 0.68 ‐based 42 × 42 focal plane arrays with good pixel uniformity, demonstrating the potential of this unique material system used for infrared imaging sensor systems.