2018
DOI: 10.1002/advs.201801810
|View full text |Cite
|
Sign up to set email alerts
|

Weak Interlayer Interaction in 2D Anisotropic GeSe2

Abstract: Germanium diselenide (GeSe2) has recently emerged as a new member of in‐plane anisotropic 2D materials, notable for its wide bandgap of 2.74 eV, excellent air stability, and high performance in polarization‐sensitive photodetection. However, the interlayer interaction in GeSe2 has never been reported, which usually plays an important role in layer‐number‐dependent physical properties. Here, the interlayer coupling in GeSe2 is systematically investigated from theory to experiment. Unexpectedly, all of density f… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

1
28
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
10

Relationship

1
9

Authors

Journals

citations
Cited by 44 publications
(30 citation statements)
references
References 35 publications
1
28
0
Order By: Relevance
“…Due to the intrinsic indirect optical band gap, the PL intensity of SiP 2 was weak under 532 nm photoexcitation, and the PL peaks demonstrated an obvious redshift (decreasing band gap) from few-layers to bulk SiP 2 (Figure S5). Furthermore, the temperature-dependent PL and Raman spectra of 2D SiP 2 flake were also recorded to study the excitonic transitions, thermal quenching, phonon vibration, and interlayer coupling. The broad emission at ∼1.97 eV is the most efficient transition process (Figure d), which corresponds to the near-band-edge emission process. At temperatures from 80 to 300 K, the near-band-edge emission peak induced by the band-to-band transition demonstrated an obvious redshift due to the increased phonon interaction and lattice expansion .…”
Section: Resultsmentioning
confidence: 99%
“…Due to the intrinsic indirect optical band gap, the PL intensity of SiP 2 was weak under 532 nm photoexcitation, and the PL peaks demonstrated an obvious redshift (decreasing band gap) from few-layers to bulk SiP 2 (Figure S5). Furthermore, the temperature-dependent PL and Raman spectra of 2D SiP 2 flake were also recorded to study the excitonic transitions, thermal quenching, phonon vibration, and interlayer coupling. The broad emission at ∼1.97 eV is the most efficient transition process (Figure d), which corresponds to the near-band-edge emission process. At temperatures from 80 to 300 K, the near-band-edge emission peak induced by the band-to-band transition demonstrated an obvious redshift due to the increased phonon interaction and lattice expansion .…”
Section: Resultsmentioning
confidence: 99%
“…Raman spectroscopy is an effective tool to investigate the materials' characteristics including crystal structure, lattice symmetry, molecular vibration mode and relative interaction between layers [37][38][39]. The ternary BTS demonstrates similar vibration modes (A 1g…”
Section: Resultsmentioning
confidence: 99%
“…GeSe is a member of group-VI monochalcogenides (SnS, SnSe, GeS and GeSe), known as phosphorene analogues. [35][36][37][38] Recently, GeSe has been widely investigated in photodetectors, [39][40][41][42][43][44][45][46] ovonic threshold switching devices, [47][48][49][50] PEC water splitting, 51 gas sensors, 52 field effect transistors (FETs) [53][54][55] and photovoltaics. 33,56,57 Among these applications, GeSe displays great potential in the field of photovoltaics due to its excellent material, optical and electrical properties.…”
Section: Properties Of Gesementioning
confidence: 99%