2019
DOI: 10.1021/acsphotonics.8b01471
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Defect Reconstruction Triggered Full-Color Photodetection in Single Nanowire Phototransistor

Abstract: The coherent developments of high performance broadband photodetection and a discrimination technique are highly essential for multiscene imaging and optical communication applications. The integration of traditional bandpass filters or stacking other spectral absorber in photodetectors often complicates the device design and leads to asymmetric photogain for each waveband. Herein, we report on ultraviolet–visible (UV-vis) multispectral photodetection based on a single ZnO nanowire (NW) phototransistor, where … Show more

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Cited by 40 publications
(29 citation statements)
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“…The optimal D * is as large as 9.78 × 10 10 cm Hz 1/2 W −1 owing to the very small I d . The SnS photodetectors with large D * are suitable for detection within a broad wavelength range and for very weak optical signals 67…”
Section: Resultsmentioning
confidence: 99%
“…The optimal D * is as large as 9.78 × 10 10 cm Hz 1/2 W −1 owing to the very small I d . The SnS photodetectors with large D * are suitable for detection within a broad wavelength range and for very weak optical signals 67…”
Section: Resultsmentioning
confidence: 99%
“…All photodetectors exhibit a fast response toward all light with visible wavelengths. A response time down to 71 ns is obtained, several orders of magnitude lower when compared with that of other filterless color/spectrum‐sensitive photodetectors,5,9–14,16,19,45–47 (Table S5, Supporting Information), which can be further accelerated by reducing the device area. It should also notice that our device which works at the self‐powered mode shows higher responsivity than other color detectors based on perovskite, even all of them required additional voltage bias.…”
Section: Figurementioning
confidence: 95%
“…The well‐defined heterointerface is subjected to the type II band alignment, as shown by the band diagram in Figure a. This alignment is deduced from two facts: i) ZnO and conventional α‐C(:H) are naturally n‐type and p‐type, respectively; [ 19,34,35 ] ii) the type I (straddling gap) and type III (broken gap) alignments are precluded in our devices, as discussed in Figure S6 (Supporting Information). The interface staggering gap formed by the type II band alignment gives rise to a build‐in potential, efficiently separating and migrating the photogenerated carriers even under the sub‐band optical exposure.…”
Section: Resultsmentioning
confidence: 96%