Upload
others
View
9
Download
0
Embed Size (px)
Citation preview
Shockwaves in RRAM (memristive) systems Marcelo J. Rozenberg
LPS CNRS/Universite Paris-‐Sud (Orsay, France)
collaborators: Vlad Dobrosavljevic (Magnet Lab – FSU) Shao Tang Pablo Levy (CNEA-‐Buenos Aires) Fernando Marlasca Federico Tesler (UBA-‐Buenos Aires) Carlos Acha Pablo Stoliar (Nanogune San SebasMan– AIST Tsukuba)
Neuromorphic circuits and computaMon is a very hot topic
• DARPA’s Synapse Program • EU Human Brain Project • Facebook • Google (DeepMind, AlphaGo)
Bio-‐chips (CMOS hardware) Deep neural networks (soWware)
Park et al Nanotechnology ‘13
Novel electronic devices for neuromorphic systems
Neurons: volaMle ResisMve Switching
n°PCT/EP2015/058873
A Leaky-‐Integrate-‐and-‐Fire Neuron Analogue realized with a Mob insulator (submibed)
(2013)
Synapses: Non-‐volaMle ResisMve Switching
A Sawa, Mat Today (2008)
non-‐polar bi-‐polar
HP’s memristor
TiO2, NiO, TaOx, HfO2, CuO, FeO, VO, STO, LSCO, YBCO, LCMO, etc, etc, etc
Introductory review: MR Scholarpedia 6(4):11414 (2011)
Universal funcMonality of TMOs
Park et al Nanotechnology ‘13
Neurons and Synapses: Great oportunity for oxyde electronics !
Novel electronic devices for neuromorphic systems
Voltage-enhanced Oxygen difussion model (bi-polar)
Top electrode
Bobom electrode
Key ingredients Inhomogeneitites Oxygen vacancy Interfaces
Voltage-enhanced Oxygen diffusion (VEOD) model
b a
Ra Rb
Higly resistive interfaces (Schottky) Oxygen difussion (enhanced by V)
Inhomogeneity 1-d channels
(see also Jeong,Schroeder and Waser et al PRB’09 and R. Meyer et al NVMTS2008)
MR, Sanchez, Weht, Levy, Acha PRB ’10
V
I
V
R Rhi
Rlow
PLCMO YBCO
experiments
Non-trivial test: “Table with legs” MR, Sanchez, Weht, Levy, Acha PRB ’10
V
R Rhi
Rlow
model simulaMons
Chen Ignatiev, APL’05
R vs V data on LCMO
Sum of two symmetric interface contributions
R
V 0
RL RR RT
Panasonic MN101LR05D 8-‐bit MCU with Embedded ReRAM
Crossbar’s integrated device RRAM product
Some new theoreMcal insight
Shock Waves and Commuta=on Speed of Memristors Phys. Rev. X 6, 011028 (2016) Synopsis: Waves That Shock Resistance
Recalling shock waves. Key noMon is the speed of the propagaMon vs speed of source
standard wave equaMon, velocity is c, solve for u(x,t)
right and leW propagaMng
Wave propagaMon
iniMal condiMon
so, the propagaMon speed depends on the perturbaMon
one we may add a difussive term
conservaMon law in acousMcs and fluid mechanics, gas dynamics, etc
These last two are Burger’s equaMons
right propagaMng perturbaMon
Burger’s eq can develop shockwaves Key feature is: The propagaMon velocity increases with the magnitude of the perturbaMon
Method of characterisMcs
Ionic (oxygen vacancies) moMon under an electric field E
conservaMon law:
ion concentraMon
is a generalized Burger’s equaMon
resisMvity
Burger’s
Then, need jdrift faster than linear in u
is a generalized Burger’s equaMon
resisMvity
Burger’s
Then, need jdrift faster than linear in u
What is this relaMon in the VEOD model? predicts shockwaves:
So it predicts shockwaves
experiments PLCMO VEOD model simulaMons
I
Rankine – Hugoniot condiMon
xint
Scaling law is realized!
experiments PLCMO VEOD model simulaMons
xint width of Schobky barrier RHI resistance of HI-‐R state
xint
Summary
• We now have arMficial synapses (and neurons) made of simple 2 terminal oxides
whose physics is based on the physical phenomenon of resisMve switching
• The way is open for neuromorphic aplicaMons
• TheoreMcal modeling may provide useful guidance for experiments