2023
DOI: 10.1039/d2na00552b
|View full text |Cite
|
Sign up to set email alerts
|

Integration of photovoltaic and photogating effects in a WSe2/WS2/p-Si dual junction photodetector featuring high-sensitivity and fast-response

Abstract: Two-dimensional (2D) materials-based van der Waals (vdW) heterostructures with exotic semiconducting properties have shown tremendous potential in next-generation photovoltaic photodetectors. Nevertheless, these vdW heterostructure devices inevitably suffer a compromise between...

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

0
10
0

Year Published

2023
2023
2024
2024

Publication Types

Select...
6

Relationship

4
2

Authors

Journals

citations
Cited by 10 publications
(11 citation statements)
references
References 59 publications
0
10
0
Order By: Relevance
“…Additionally, Figure c displays the Raman spectra of the dual junction device at four different positions. The red and yellow curves represent the Raman spectra of the WS 2 and WS 2 /GaN regions, respectively, where two prominent peaks of E 2g and A 1g consistently appear, aligning with the typical Raman modes of WS 2 . The green curve illustrates the Raman spectrum of the ReS 2 region, exhibiting a strong A g characteristic peak at 158.04 cm –1 along with other weaker Raman peaks. , The purple curve corresponds to the Raman spectrum of the ReS 2 /WS 2 /GaN region, demonstrating a combined peak of WS 2 and ReS 2 , indicating the successful production of high-quality vdWs heterostructures through the transfer process. High-resolution transmission electron microscopy (HRTEM) images in Figure S2 confirm the highly crystalline nature of the WS 2 and ReS 2 nanosheets.…”
Section: Resultsmentioning
confidence: 90%
See 2 more Smart Citations
“…Additionally, Figure c displays the Raman spectra of the dual junction device at four different positions. The red and yellow curves represent the Raman spectra of the WS 2 and WS 2 /GaN regions, respectively, where two prominent peaks of E 2g and A 1g consistently appear, aligning with the typical Raman modes of WS 2 . The green curve illustrates the Raman spectrum of the ReS 2 region, exhibiting a strong A g characteristic peak at 158.04 cm –1 along with other weaker Raman peaks. , The purple curve corresponds to the Raman spectrum of the ReS 2 /WS 2 /GaN region, demonstrating a combined peak of WS 2 and ReS 2 , indicating the successful production of high-quality vdWs heterostructures through the transfer process. High-resolution transmission electron microscopy (HRTEM) images in Figure S2 confirm the highly crystalline nature of the WS 2 and ReS 2 nanosheets.…”
Section: Resultsmentioning
confidence: 90%
“…Furthermore, the relationship between I ph and P follows a power-law function (I ph ∝ P α ), where a high α (0.88) signifies minimal loss of photoexcited carriers and an effective reduction in the compounding rate of photoexcited carriers due to the dual vdWs heterojunction structure. 47,48 Then, photodetection metrics such as responsivity (R), detection (D*), external quantum efficiency (EQE), and light on/off ratio (I on /I off ) were evaluated based on the 31 ITO/GaN, 52 MoS 2 /AlN, 53 W/GaN, 54 GaN/β-Ga 2 O 3 , 55 WSe 2 /WS 2 /p-Si, 41 Ni/GaN, 56 WS 2 /Si, 30 graphene/Si, 57 MoS 2 /p-GaN, 58 WS 2 /GaN, 35 PtSe 2 /GaN, 36 and MoS 2 /WS 2 . 59 extracted I ph in Figure 3c.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…As a result, Figure 1c displays the SPD image and the extracted potential profile. The averaged SPD of WTe 2 and WS 2 can be measured and calculated using the following equations: [36] eSPD WTe 2 = W tip − W WTe 2…”
Section: Resultsmentioning
confidence: 99%
“…As a result, Figure 1c displays the SPD image and the extracted potential profile. The averaged SPD of WTe 2 and WS 2 can be measured and calculated using the following equations: [ 36 ] eSPDWTe2badbreak=Wtip0.33emgoodbreak−WWTe2$$\begin{equation}eSP{D}_{WT{e}_2} = {W}_{tip}\ - {W}_{WT{e}_2}\end{equation}$$ eSPDWS2badbreak=Wtip0.33emgoodbreak−WWS2$$\begin{equation}eSP{D}_{W{S}_2} = {W}_{tip}\ - {W}_{W{S}_2}\end{equation}$$Where e is the electron charge, W tip , WWTe2${W}_{WT{e}_2}$ and WWS2${W}_{W{S}_2}$ represent the work functions of KPFM tip, WTe 2 and WS 2, respectively. Therefore, after contact, the built‐in electric field points from WS 2 to the WTe 2 side.…”
Section: Resultsmentioning
confidence: 99%