2021
DOI: 10.1039/d1tc03359j
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Reinforcement of double built-in electric fields in spiro-MeOTAD/Ga2O3/Si p–i–n structure for a high-sensitivity solar-blind UV photovoltaic detector

Abstract: Novel p-i-n self-powered solar-blind UV photodetector based on p-type spiro-MeOTAD (spiro), Ga2O3, and n-type Si is fabricated. The p-type spiro film is spin-coated on the surface of Ga2O3 film deposited...

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Cited by 30 publications
(29 citation statements)
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“…Simultaneously, these photogenerated carriers are immediately separated by two built-in electric potentials: the holes and electrons drift into the spiro and Si, respectively. Finally, carriers flow into the external circuit, resulting in a high photocurrent. , …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Simultaneously, these photogenerated carriers are immediately separated by two built-in electric potentials: the holes and electrons drift into the spiro and Si, respectively. Finally, carriers flow into the external circuit, resulting in a high photocurrent. , …”
Section: Resultsmentioning
confidence: 99%
“…Finally, carriers flow into the external circuit, resulting in a high photocurrent. 29,30 To analyze the influence of spiro thickness on the photoelectric response performance, Figure 3b depicts the I− V curves of D1−D5 in linear coordinate under SBUV illumination with an intensity of 1 mW/cm 2 . Meanwhile, the key parameters such as thickness and transmittance of spiro layers, V oc , and I sc data of devices are compared and summarized in Table S1.…”
Section: Resultsmentioning
confidence: 99%
“…Here, we propose a substitution method by using spiro-OMeTAD as an organic p-type hole transporting layer (HTL) to fabricate graphene/spiro-OMeTAD/Si heterostructure-based PDs because of its various advantages as mentioned below. Benefiting from its high solubility and amorphous nature, the spiro-OMeTAD HTL can be prepared by simple spin coating. Also, due to its large band gap (∼2.9 eV), the spiro-OMeTAD is an ideal transparent material for graphene–Si PDs .…”
Section: Introductionmentioning
confidence: 99%
“…Because of the advantages of high sensitivity, low background noise, and low false alarm rate, solar-blind ultraviolet photodetectors have significant applications in civil, industrial, and military fields. Ultrawide-bandgap semiconductors, such as diamond, Al x Ga 1– x N, Mg x Zn 1– x O, and Ga 2 O 3 , have been utilized to develop such photodetectors because of their strong absorption in the solar-blind region. Among the above materials, Ga 2 O 3 with an intrinsic bandgap of 4.2–5.3 eV has absorption cutoff wavelengths in the solar-blind region without the need of bandgap tuning through alloying or doping, making it an ideal candidate for solar-blind detection. Recently, with the rapid development of optical measurement techniques, there is an increasing demand for solar-blind precision measurement, which has been demonstrated using photodetector arrays. However, the measurement accuracy of these photodetector arrays was limited by the spacing and size of the photodetector pixels.…”
mentioning
confidence: 99%
“…Figure h briefly illustrates the zero-bias performance parameters of state-of-the-art UV photodetectors developed from various wide-bandgap semiconductors. It is obvious that the responsivity as well as the response time of the PSD are superior to most UV photodetectors. ,,,,,,, , The excellent performances of the device benefit from the enhanced absorption efficiency and shortened transport path in the nanometer-thick Ga 2 O 3 .…”
mentioning
confidence: 99%