2020
DOI: 10.1021/acsnano.9b09828
|View full text |Cite
|
Sign up to set email alerts
|

Anisotropic Picosecond Spin-Photocurrent from Weyl Semimetal WTe2

Abstract: The generation and detection of ultrafast spin current, preferably reaching a frequency up to terahertz, is the core of spintronics. Studies have shown that the Weyl semimetal WTe 2 is of great potential in generating spin currents. However, the prior studies have been limited to the static measurements with the inplane spin orientation. In this work, we demonstrate a picosecond spin-photocurrent in a Td-WTe 2 thin film via a terahertz time domain spectroscopy with a circularly polarized laser excitation. The … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

3
34
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
7

Relationship

2
5

Authors

Journals

citations
Cited by 43 publications
(37 citation statements)
references
References 51 publications
3
34
0
Order By: Relevance
“…We also show that such giant Rashba effect can be used to generate spin-polarized photocurrents in terms of the circular photogalvanic effect. [18][19][20][21][22][23] Therefore, these giant Rashba phenomena may open a new door to promising spintronic and optoelectronic applications.…”
Section: Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…We also show that such giant Rashba effect can be used to generate spin-polarized photocurrents in terms of the circular photogalvanic effect. [18][19][20][21][22][23] Therefore, these giant Rashba phenomena may open a new door to promising spintronic and optoelectronic applications.…”
Section: Discussionmentioning
confidence: 99%
“…Because of the giant Rashba spin splitting, the KTO ultrathin lms can be used for achieving circular photogalvanic effect (CPGE) to generate spin-polarized photocurrents. [18][19][20][21][22][23] For the right-handed (le-handed) circularly polarized light, its photon has the angular momentum of +1 (À1), labeled by s + (s À ), and the selection rule for necessary transitions is that the allowed zcomponent change of the total angular momentum is DJ m ¼ +1 (À1). The valence band edge, originating from the J ¼ 3/2 states, has J m ¼ AE3/2, and the conduction band edge, from the Fig.…”
Section: Heterostructures and Photogalvanic Effectmentioning
confidence: 99%
See 1 more Smart Citation
“…4(e) and 4(f)], they both presented the same spectral shapes, strongly indicating that both C x and L 1x shared the same physical origin and are consistent with previous observation. 25,26,[35][36][37][38] However, the D x , L 2yz , and D yz terms also presented similar shapes in the frequency domain, and very few works pay attention to the underlying mechanism about these three terms. Ours is the first observation that all five terms resemble each other in nature, and we elucidate this phenomenon in a macroscopic phenomenological PGE-induced photocurrent framework.…”
Section: Chiral Terahertz Wave Emission and Manipulationmentioning
confidence: 99%
“…[ 11,12 ] Additionally, WTe 2 also shows controllable ferroelectric behavior [ 13,14 ] and spin relaxation within nanoseconds up to room temperature. [ 15 ] Thus, these rich features have endowed WTe 2 with tremendous potential applications such as all‐solid‐state flexible supercapacitors, [ 16 ] hydrogen evolution, [ 17 ] sodium ion batteries, [ 18 ] photodetectors, [ 19–21 ] and photothermoelectric transport. [ 22 ] Most notably, its Weyl semimetal and topological insulator behaviors have attracted tremendous research attention recently.…”
Section: Introductionmentioning
confidence: 99%