Classical Computing with Topological States: Coping with a post-Moore World

By Avik Ghosh

Electrical Engineering, University of Virginia, Charlottesville, VA

Published on

Abstract

As Moore?s Law grinds to a halt, we are entering a new world of software driven hardware, of ASICs and machine learning accelerators. This has opened up new opportunities for novel low-power electronics and emerging materials underpinning them. While quantum computing can end up being disruptive in algorithmic scale-up, there are many opportunities for classical computing with topological quantum states based on present day technology that can be quite disruptive as well. There are two examples I will focus on ? one is doing conventional Boolean logic at low power below the thermal Boltzmann limit, using the topological properties of Dirac fermions to control transmission across a gated interface. The other is doing collective computing using temporal state machines to solve certain graph theory problems efficiently. An example is skyrmions driven along racetracks, whose quasi-linear operation and topologically stabilized lifetimes at ultra-small sizes can potentially function as temporal memory in race logic for rapid pattern matching and intermittent-sensor processing applications. These two concepts ? topology driven lifetime and topology driven transmission, can be used to accomplish entirely different goals in low-power computing.

Bio

Avik Ghosh Avik Ghosh is Professor at the Charles Brown Dept of Electrical and Computing Engineering and the Dept of Physics at the University of Virginia. He did his PhD in condensed matter theory at the Ohio State University, and a postdoctoral fellowship in Electrical Engineering at Purdue University. He is the UVA site-director of the NSF-Industry University Cooperative Center on Multifunctional Integrated Systems Technology (MIST). Ghosh has authored 125+ refereed papers and a book (?Nanoelectronics ? a Molecular View?, World Scientific) in the area of computational nano-materials and devices. He has given over 125 invited lectures worldwide. He is Fellow of the Institute of Physics (IOP), senior member of the IEEE, and has received the IBM Faculty Award, the NSF CAREER Award, a 2006 best paper award from the Army Research Office, and UVA?s All University Teaching Award. His group?s work with Columbia University on negative index behavior in graphene was voted by the editors of Physics World as one of the top10 research breakthroughs of 2016.

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Researchers should cite this work as follows:

  • Avik Ghosh (2021), "Classical Computing with Topological States: Coping with a post-Moore World," https://nanohub.org/resources/35169.

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Classical Computing with Topological States: Coping with a post-Moore World
  • Classical Computing with Topological States: Coping with a post-Moore World 1. Classical Computing with Topol… 0
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  • ViNO group Grand Challenges 2. ViNO group Grand Challenges 132.1654988321655
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  • Topological Insulators… Topological Superconductors… Weyl Semi-Metals 3. Topological Insulators… Topo… 198.36503169836504
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  • Talk Outline: Topology in classical computing 4. Talk Outline: Topology in clas… 277.41074407741075
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  • Le roi est Moore, vive le roi 5. Le roi est Moore, vive le roi 380.68068068068072
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  • Alive? Dead? Dead-Alive? 6. Alive? Dead? Dead-Alive? 434.36770103436771
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  • Untitled: Slide 7 7. Untitled: Slide 7 507.640974307641
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  • Magnets can have low 8. Magnets can have low "Q" 626.32632632632635
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  • What sets 9. What sets "Q" ? 656.52318985652323
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  • Penalty for reducing Q  Reliability 10. Penalty for reducing Q  Rel… 816.61661661661662
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  • Small barrier not necessarily bad !! 11. Small barrier not necessarily … 891.82515849182516
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  • To create a large barrier in a scaled magnet  defect 12. To create a large barrier in a… 1000.1668335001668
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  • Smaller Q in all metallic Domain Walls 13. Smaller Q in all metallic Doma… 1048.5151818485151
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  • What happens if we add spatial inversion symmetry breaking? 14. What happens if we add spatial… 1085.7524190857525
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  • How much winding? 15. How much winding? 1165.7323990657324
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  • Winding of spins create a metastable state 16. Winding of spins create a meta… 1277.0770770770771
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  • How to get small and stable skyrmions? 17. How to get small and stable sk… 1408.742075408742
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  • Fast, Non-Volatile and static Skyrmions 18. Fast, Non-Volatile and static … 1499.5995995995997
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  • What can we use it for? HD memory and temporal memory 19. What can we use it for? HD mem… 1593.8271604938273
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  • Applications - Solving a MIN/MAX problem 20. Applications - Solving a MIN/M… 1686.353019686353
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  • How to store Temporal Information 21. How to store Temporal Informat… 1771.3713713713714
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  • How costly is this? 22. How costly is this? 1839.5061728395062
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  • Topology of spin winding in-real space 23. Topology of spin winding in-re… 1935.7023690357025
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  • Talk Outline: Topology in classical computing 24. Talk Outline: Topology in clas… 1981.8151484818152
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  • How to Reduce DV ? 25. How to Reduce DV ? 2011.544878211545
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  • Topology of emerging materials 26. Topology of emerging materials 2191.3246579913248
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  • Transmitting electrons at a graphene PN junction 27. Transmitting electrons at a gr… 2265.8324991658324
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  • Switching with geometry: Klein Tunnel Transistor 28. Switching with geometry: Klein… 2345.3453453453453
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  • Experimental switching 29. Experimental switching 2446.0460460460463
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  • A path towards higher performance KTFETs 30. A path towards higher performa… 2574.1741741741744
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  • Similar Dirac Fermions physics in other Q-Materials 31. Similar Dirac Fermions physics… 2652.0186853520186
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  • Topology  Universal Small Reflectivity 32. Topology  Universal Small R… 2720.7207207207207
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  • See this with spins in TIs/WSMs as well 33. See this with spins in TIs/WSM… 2906.6066066066069
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  • Topology 34. Topology 2936.9703036369706
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  • SPECIAL THANKS TO MY MENTORS ! 35. SPECIAL THANKS TO MY MENTORS ! 2999.1991991991995
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