2023
DOI: 10.1021/acsami.3c13004
|View full text |Cite
|
Sign up to set email alerts
|

SnS2/MoS2 van der Waals Heterostructure Photodetector with Ultrahigh Responsivity Realized by a Photogating Effect

Sufeng Quan,
Luyang Li,
Shuai Guo
et al.
Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2024
2024
2024
2024

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 6 publications
(2 citation statements)
references
References 50 publications
0
2
0
Order By: Relevance
“…The photoresponse performance of the 1D vdW Nb 2 Pd 1– x Se 5 photodetectors is further evaluated by several vital parameters, , including responsivity ( R ), detectivity ( D *), external quantum efficiency (EQE), and rising/decay time, which have been presented in detail in Note S1 in the Supporting Information. Figure (e) presents the calculated R and D * under a 638 nm laser with different power densities at a gate voltage of 40 V. A maximum R of ∼1 A/W is achieved at a gate voltage of 40 V because the photogating-effect-dominated photocurrent generation mechanism could extend the lifetime of photoexcited carriers . According to the measured noise power spectral density of the Nd 2 Pd 1– x Se 5 photodetector in Figure S7, the Nb 2 Pd 1– x Se 5 photodetector exhibits decreased R ( D *) from 1 A/W (4.23 × 10 8 Jones) to 0.2 A/W (8.95 × 10 7 Jones) when the power density increases from 0.45 μW/μm 2 to 6.93 μW/μm 2 , which is probably attributed to the decreased recombination of the photoexcited carriers under weak laser illumination. , As shown in Figure S8 in the Supporting Information, the maximum EQE of the Nb 2 Pd 1– x Se 5 photodetector reaches 196%, indicating the device has good photoelectric conversion efficiency .…”
Section: Resultsmentioning
confidence: 97%
“…The photoresponse performance of the 1D vdW Nb 2 Pd 1– x Se 5 photodetectors is further evaluated by several vital parameters, , including responsivity ( R ), detectivity ( D *), external quantum efficiency (EQE), and rising/decay time, which have been presented in detail in Note S1 in the Supporting Information. Figure (e) presents the calculated R and D * under a 638 nm laser with different power densities at a gate voltage of 40 V. A maximum R of ∼1 A/W is achieved at a gate voltage of 40 V because the photogating-effect-dominated photocurrent generation mechanism could extend the lifetime of photoexcited carriers . According to the measured noise power spectral density of the Nd 2 Pd 1– x Se 5 photodetector in Figure S7, the Nb 2 Pd 1– x Se 5 photodetector exhibits decreased R ( D *) from 1 A/W (4.23 × 10 8 Jones) to 0.2 A/W (8.95 × 10 7 Jones) when the power density increases from 0.45 μW/μm 2 to 6.93 μW/μm 2 , which is probably attributed to the decreased recombination of the photoexcited carriers under weak laser illumination. , As shown in Figure S8 in the Supporting Information, the maximum EQE of the Nb 2 Pd 1– x Se 5 photodetector reaches 196%, indicating the device has good photoelectric conversion efficiency .…”
Section: Resultsmentioning
confidence: 97%
“…27–29 Heterojunctions with type-II and type-III tunneling characteristics have garnered significant attention in research and development, which offer advantages such as the ability to efficiently separate photocarriers and the potential for achieving broadband optical absorption. 30–40 However, one of the key challenges in type-II and type-III optoelectronics is the need to address ultrafast switching speeds to keep pace with the rapid developments in optoelectronic devices with low photocurrent on/off ratio. Unlike type-II and type-III heterostructures, type-I heterostructures refer to heterostructures by having the minimum conduction band and the maximum valence band within the same semiconductor material.…”
Section: Introductionmentioning
confidence: 99%