2D Valley-Spin Transport in Transition Metal Dichalcogenides

By Zhihong Chen

Electrical and Computer Engineering, Purdue University, West Lafayette, IN

Published on

Abstract

Electronic devices exploring carrier transport with spin and valley degree of freedom have emerged as promising candidates for next-generation information storage and transport, since pure spin and valley currents do not accompany energy dissipation associated with Joule heating. The spin and valley degree of freedom of electrons in two-dimensional (2D) transition metal dichalcogenides (TMDs) have been extensively studied by theory, optical and optoelectronic experiments. The ability to electrically generate and detect such pure spin and valley currents in these materials is of particular importance. In this talk, we first report that valley current can be electrically induced and detected through the valley Hall effect and inverse valley Hall effect, respectively, in monolayer molybdenum disulfide. We compare temperature and channel length dependence of non-local electrical signals in monolayer and multi-layer samples to distinguish the valley Hall effect from classical Ohmic contributions. Significantly, valley transport is observed over four-micron distance in monolayer samples at room temperature. We then study the valley coupled spin generation in monolayer tungsten disulfide and spin diffusion in a 2D stack device. Our device design approach provides a unique way to integrate charge, spin and valley degrees of freedom, which can be useful for emerging valleytronic applications.

Bio

Zhihong Chen Zhihong Chen received her B.S. degree in physics from Fudan University in 1998, and her Ph.D. degree in physics from the University of Florida in 2003. After two years of postdoctoral research at IBM T.J. Watson research center, she became a research staff member in the Physical Science Department. Her research focused on design and fabrication of high performance carbon based devices and circuits. In 2008, she was appointed as the manager of the Carbon Technology Group at IBM, where she was in charge of evaluating the potential of carbon materials and the development of novel carbon based technologies for commercial applications. She joined the School of Electrical and Computer Engineering at Purdue University in 2010 as an Associate Professor, and has become a Full Professor since 2017. Her research interests focus on device and circuit designs for beyond-CMOS applications. She has become the Director of the SRC nCORE NEW LIMITS Center since 2018, and Associated Director of Research for Birck Nanotechnology Center in 2019. She is an Associate Editor of IEEE Electron Device Letters.

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Cite this work

Researchers should cite this work as follows:

  • Zhihong Chen (2020), "2D Valley-Spin Transport in Transition Metal Dichalcogenides," https://nanohub.org/resources/33422.

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Time

Location

Burton Morgan, Room 121, Purdue University, West Lafayette, IN

Tags

2D Valley-Spin Transport in Transition Metal Dichalcogenides
  • 2D Valley-Spin Transport in Transition Metal Dichalcogenides 1. 2D Valley-Spin Transport in Tr… 0
    00:00/00:00
  • Spin Hall Effect 2. Spin Hall Effect 45.812479145812482
    00:00/00:00
  • Switching Current of SOT Switching Based Write Unit 3. Switching Current of SOT Switc… 138.83883883883885
    00:00/00:00
  • Transition Metal Dichalcogenides (2H – MX2) 4. Transition Metal Dichalcogenid… 355.98932265598933
    00:00/00:00
  • Valley Dependent Spin Splitting in TMDs 5. Valley Dependent Spin Splittin… 513.14647981314647
    00:00/00:00
  • Monolayer and Multilayer MoS2 Characterization 6. Monolayer and Multilayer MoS2 … 710.54387721054388
    00:00/00:00
  • Non-local Measurement Set-up for Valley Current Detection 7. Non-local Measurement Set-up f… 824.95829162495829
    00:00/00:00
  • Non-local Measurements of Monolayer and Multi-layer MoS2 8. Non-local Measurements of Mono… 897.8311644978312
    00:00/00:00
  • Non-local Measurements of Monolayer and Multi-layer MoS2 9. Non-local Measurements of Mono… 980.613947280614
    00:00/00:00
  • Temperature Dependence of Non-local Signals 10. Temperature Dependence of Non-… 1018.1181181181181
    00:00/00:00
  • Temperature Dependence of Non-local Signals 11. Temperature Dependence of Non-… 1049.2826159492827
    00:00/00:00
  • Valley Hall Effect Induced Non-local Resistance 12. Valley Hall Effect Induced Non… 1074.1074407741075
    00:00/00:00
  • Valley Hall Effect Induced Non-local Resistance 13. Valley Hall Effect Induced Non… 1138.6052719386053
    00:00/00:00
  • Valley Hall Effect Induced Non-local Resistance 14. Valley Hall Effect Induced Non… 1144.0774107440775
    00:00/00:00
  • Large Spin Splitting in WSe2 Valence Band 15. Large Spin Splitting in WSe2 V… 1172.8395061728395
    00:00/00:00
  • Large Spin Splitting in WSe2 Valence Band 16. Large Spin Splitting in WSe2 V… 1190.2902902902904
    00:00/00:00
  • Air Stable P-type Doping for WSe2 FETs 17. Air Stable P-type Doping for W… 1223.0897564230897
    00:00/00:00
  • Air Stable P-type Doping for WSe2 FETs 18. Air Stable P-type Doping for W… 1279.9466132799466
    00:00/00:00
  • Electrical Detection of Valley Coupled Spin Currents in WSe2 19. Electrical Detection of Valley… 1288.9556222889557
    00:00/00:00
  • Nonlocal Spin Valve Measurements for Out-of-Plane Spins 20. Nonlocal Spin Valve Measuremen… 1324.9582916249583
    00:00/00:00
  • Nonlocal Spin Valve Measurements for Out-of-Plane Spins 21. Nonlocal Spin Valve Measuremen… 1335.7691024357691
    00:00/00:00
  • Nonlocal Spin Valve Measurements for Out-of-Plane Spins 22. Nonlocal Spin Valve Measuremen… 1352.4858191524859
    00:00/00:00
  • Acknowledgement 23. Acknowledgement 1366.8001334668002
    00:00/00:00
  • Thank you! 24. Thank you! 1370.4371037704373
    00:00/00:00