4.6 Article

PtSe2 Field-Effect Phototransistor with Positive and Negative Photoconductivity

Journal

ACS APPLIED ELECTRONIC MATERIALS
Volume 4, Issue 11, Pages 5177-5183

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsaelm.2c00552

Keywords

PtSe2 FEPT; negative photoconductivity; photoinduced desorption; positive photoconductivity; photogating effects; high carrier mobility

Funding

  1. National Key R&D Program of China
  2. National NaturalScience Foundation of China
  3. Natural Science Foundation of Jiangsu Province
  4. Natural Science Research Project of Higher Education Institutions of Jiangsu Province
  5. China Postdoctoral Science Founda-tion
  6. [2019YFA0705204]
  7. [62005107]
  8. [62005074]
  9. [BK20180862]
  10. [BK20190839]
  11. [20KJB140007]
  12. [2019M651725]

Ask authors/readers for more resources

By investigating the photoconductive mechanism of a few-layer PtSe2 field-effect phototransistor (FEPT), we found that both positive and negative photoconductivity can be observed. The changes in photoconductivity are attributed to the photoinduced desorption of oxygen molecules, photoinduced carriers, and the photogating effects caused by photoinduced electrons at the PtSe2/SiO2 interface.
Platinum diselenide (PtSe2) has been exploited for visible and infrared photodetectors due to its tunable electrical and photoelectric properties determined by a layer-dependent band gap. We investigated the photoconductive mechanism of the few layer (3 nm) PtSe2 field-effect phototransistor (FEPT) under illumination of visible and infrared lasers. The few-layer PtSe2 FEPT shows ambipolar characteristics modulated by a gate voltage with a mobility of 1496.7 cm2 v-1 s-1 (electron) and 1410 cm2 v-1 s-1 (hole) at VDS = 0.16 V. Both positive photoconductivity (PPC) and negative photoconductivity (NPC) were observed in the PtSe2 photodetector. The responsivity (R) of the device at VG = 4 V was 0.14 A/W, 0.63 A/W, and 0.086 A/W, and the specific detectivity (D*) was 4.34 x 108 Jones, 1.95 x 109 Jones, and 2.4 x 108 Jones under 532, 808, and 405 nm laser irradiation, respectively. The R of the device at VG = -2.4 V was 0.525 A/W, 0.34 A/W, and 0.087 A/W, and theD* was 1.84 x 109 Jones 1.06 x 109 Jones, and 2.19 x 108 Jones. The change of the photoconductivity is attributed to a combination of three mechanisms: (1) photoinduced desorption of oxygen molecules from the surface, which is related to the NPC; (2) the photoinduced carriers, which leads to PPC; and (3) the photogating effects related to the photoinduced electrons in the interface of PtSe2/SiO2. NPC dominates in the device at a high gate voltage due to the photogating effect. Through the study of the P/NPC mechanism in PtSe2, understanding of the photoconductive mechanism in the field of photoelectric detection is further deepened.

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