recent progress in resistance change memory€¦ · metal oxide: filament • set : voltage-induced...

36
AVS Thin-films User Group meeting, October 15, 2008 Recent Progress in Resistance Change Memory Yoshio Nishi Department of Electrical Engineering, Stanford University, Stanford, California 94305-4070

Upload: others

Post on 23-Jul-2020

2 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

AVS Thin-films User Group meeting, October 15, 2008

Recent Progress in Resistance Change Memory

Yoshio Nishi Department of Electrical Engineering,

Stanford University, Stanford, California 94305-4070

Page 2: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanisms• Scalability• Summary

Page 3: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Motivations for new nonvolatile memory research

• Scalability limit beyond 32nm nodes of existing memory both volatile memory and nonvolatile memory

• Increasing needs for less power consumption on chip

• Increasing demands for on-chip memory size• “Nano” materials evolution/revolutions have

stimulated exploration of new memory opportunities

• Logic coupled with memory

Page 4: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Memory area on a chip will increasePe

rcen

tage

of a

rea

in S

oC [%

]

2001 2004 2007 2010 2013 20160

20

40

60

80

100

Year

Memory

Logic

Due to design productivity, yield, and power

ITRS’ 2000

Page 5: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

The number of electrons stored in the floating gateA. Gibby, Stanford Univ Thesis, 2008

Page 6: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Year06 07 09 10 11 12 13 14 15 1608 17 18 19 20

65nm

45nm

32nm22nm

15nm10nm

7nm?

Flash

PRAM

CBRAM

MRAM

Strained channel

Nanowire devices/nanotubes

Molecular devices

New channel materials, Ge, III-V

Spintronics

FERAM

Organic/Molecular?

5nm?

193nm+liquid immersionEUV?

Self-assembly/bottom up?

2D chip+3D package3D chip

Emerging Bio/Medical Chips

Optimistic scenario (revised from 2007)

SOI , FD, UTB

Page 7: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Requirements for next generation NVM

NonNon--VolatilityVolatility

SpeedSpeed SRAM

DRAM

Flash

New Memory

CMOS Compatibility

Simple, Stable Process

Low Cost Material

Mass Productivity,

Uniformity: 300mm and beyond

R0~R1 Sensing Margin

Non-Destructive Reading

Non-volatility : > 10 years

Fast random access: tRead = 10ns

tWrite = 5ns ~ 100nsVirtually unlimited usage

: > 1012 cycles

New Functionalities

ITRSROADMAP 2005

Density Density

Hyunsang Hwang, Stanford, 07

Page 8: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

ITRS 2007

Page 9: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Resistance changes• Bulk material conduction changes depending

upon whether the bulk is crystalline or amorphous----phase change memory

• Formation of nanoscale conductive pass in solid which creates “on” state---nano-filament based resistance change memory

• Lowering or thinning of the barrier between electrode and solid which defines “on” state conduction---uniform switching resistance change memory

Page 10: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Conducting paths between the device’s two terminals in a reversible process that changes electrical resistance by orders of magnitude

– Filament effect (contributed by metal ions,charged defects, softbreakdown, storage/release of charge carriers, etc)

– small applied voltage levels and energy– large non-volatile resistance changes– simple, highly scalable structure

Resistance Change Memory

With Filament Formation-V

Ground

Metal

Metal

Insulator

IntroductionIntroduction

Page 11: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Source: Samsung

3D, Stackable Cross-Point Memory

SL

m-1

SL

m+1SL

m

WL

n-1

WL

n+1

WL

n

Memory element plus integrated diode

Wordline(W/L)

Bitline (B/L)

Source: Ho-Choel Kim (IBM)

Self-assembled pattern (18 nm half-pitch)

Page 12: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanisms• Scalability• Summary

Page 13: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

ZnXCd1-XS

100 / 1M ΩOn/Off Resistance106On/Off Ratio~ 50 nsRead/Write Time

Phillips Research Lab• P.W.M. Blom et al., Ferroelectric Schottky Diode, Phys.

Rev. Lett. 73, 2107 (1994)• P. van der Sluis, Non-volatile Memory Cell in ZnXCd1-XS,

Appl. Phys. Lett. 82, 4089 (2003)

NEC Corp.• T. Sakamoto et al., Nanometer-scale Switches Using Copper Sulfide,

Appl. Phys. Lett. 82, 3032 (2003)

Cu1-XS

50 / 100 M ΩOn/Off Resistance106On/Off Ratio~ 100 usRead/Write Time

Metal sulfide: Filament

Page 14: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

On-resistance is independent of contact size → filament conductionOff-resistance is proportional to contact size → bulk leakageOn/Off ratio improves with scaling

Small-scale devicesSmall-scale devices

AgSiO2

PtSiO2

Si

ZnCdS

ZnCdS resistance change memory characteristics

Z. Wang et al, IEEE Electron Device Letters Vol.28,(2007) pp14-16

Page 15: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Metal Oxide: Filament

• Set : voltage-induced partial dielectric breakdown

• Rest : disruption of conductive filament by high current density generated locally

※ e.g., TiO2, NiO, SrTiO3

Fuse / Anti-fuse type (Conductive Filament)

I. H. Inoue et al., Cond matter, 0702564v1 (2007)

Page 16: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanisms• Scalability• Summary

Page 17: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Compact “Non-volatile” Logic

Nonvolatile Flipflop Nonvolatile SRAM (latch)

S. Fujita*, K. Abe, T. H. Lee(3D conference 2004, Nanotech conference 2005)

Reference resistance

Q

R1CK R

D

CK

CKNV Memory

CK CK

CK

CK

CK

W. Wang, A. Gibby, Z. Wang, T. Chen, S. Fujita*, P. Griffin, Y. Nishi, and S. Wong (IEDM 2006), NMTRI review 2006.

NV Memory

NV memory Latchdatadata

Power Off Power On

Page 18: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

NVSRAM: No Area Overhead

W. Wang et al, 2006 IEDM

Page 19: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

2-terminal to 3 terminal devices

Page 20: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high
Page 21: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanisms• Scalability• Summary

Page 22: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Materials shown Resistance Switching

GexSe1-x(Ag,Cu,Te-doped), Ag2S, Cu2S, CdS, ZnS, CeO2

Others

La2-xSrxNiO4, La2CuO4+δ

…K2NiF4

PCMO(Pr0.7Ca0.3MnO3), LCMO(La1-xCaxMnO3)BSCFO(Ba0.5Sr0.5Co0.8Fe0.2O3-δ), YBCO(YBa2Cu3O7-x)(Ba,Sr)TiO3(Cr, Nb-doped), SrZrO3(Cr,V-doped), (La, Sr)MnO3

Sr1-xLaxTiO3, La1-xSrxFeO3, La1-xSrxCoO3, SrFeO2.7, LaCoO3, RuSr2GdCu2O3, YBa2Cu3O7

Perovskite

TiO2, NiO, CuxO, ZrO2, MnO2, HfO2, WO3, Ta2O5, Nb2O5, VO2, Fe3O4

…Binary Metal Oxide

Page 23: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Unipolar

Switching Operation Polarity

BipolarReset

(LRS HRS)

Set (HRS LRS)

Reset

Set

Reset

Set

• Depending on the materials and measurement, the curves could vary considerably.

Page 24: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

H. Hwang 2008

Page 25: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

N. Xu et al, 2008 VLSI Symposium, Honolulu

Page 26: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanism• Scalability• Summary

Page 27: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

• Set : - The oxidation of an electrochemically active electrode metal

- The drift of the mobile cations toward counter electrode

- Form a highly conductive filament

• Reset : An electrochemical dissolution of the conductive bridges

※ e.g., Ag+ in Ag2S, Ag+ in GeSe, Cu2+ in CuOx

Proposed Mechanism 1Ionic Transport and electrochemical redox reaction type

Xin Guo et al., Appl. Phys. Lett. 91, 133513 (2007)

Page 28: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Proposed mechanism 2Electronic Effect type (Charge trap & Schottky Contact)

• Charge injection by tunneling at high electric field

• Trapped at interface states in insulator

• Modification of the electrostatic schottky barrier and its resistance

※ e.g., Ti/PCMO/SRO

• Electronic charge injection acts like doping to induce an insulator-metal transition

※ e.g., PCMO, Cr-doped SrTiO3, Cu2O

Sawa et al., Appl. Phys. Lett. 85, 4073 (2004)T. Fuji et al., Apply. Phys. Lett. 86, 012107 (2005)Chen et al., Appl. Phys. Lett. 91, 123517 (2007)

Page 29: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

TiO2 Switching

• VO model of forming and switching in TiO2

• Evidence supporting VO model• Critical look at data:

Are vacancies really the whole story?• Evidence that H is origin of field-

programmable rectification• H + VO model of forming in TiO2 and related

oxidesYoshio Nishi & John Jameson, DRC 2008

Page 30: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Outline• Emerging nonvolatile memories• Switching behaviors

metal sulfides and metal oxides• Device applications

nonvolatile memory and nonvolatile logic• Phenomenological behaviors• Physical mechanisms• Scalability• Summary

Page 31: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Scalability questions

Can “on” resistance stays same or decrease?Can “off” resistance stays same of decrease?Retention characteristicsvs Programming speed ?Endurance?Programming voltage tunability?

Page 32: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

II--V CharacteristicsV Characteristics

Cu

Cu2-xS

Ti/Au

+

_

• Ron : ~150Ω

• Icomp. : 1mA

• Von : ~0.15V

• Consistent over 150 cycle sweeps

off→on

on→off

S. Kim and Y. Nishi, Non-Volatile Memory Technology Symposium, 2007, Albuquerque

Page 33: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

[email protected]@0.1V vs. Device Area (vs. Device Area (IIcompcomp. . =1mA)=1mA)

• Ron : ~150Ω, almost independent of device area.– Filament size (~5nm) much smaller than device area

• Roff : increasing with scaling down of device area.– Mainly determined by bulk properties

• Roff/Ron : improving with scaling down of devices

Ron

Roff

Roff/Ron

S-W Kim, Stanford Univ. Thesis, 2008

Page 34: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

CuCu22--xxS S NanopillarsNanopillars

~170nm

~25nm

Cu sub.

Cu2-xS nanopillar

Page 35: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Manipulation of characteristicsManipulation of characteristics• Simple structure : 2-terminal device• Scalability : ~40nm• Large on/off ratio : > 105 @ 3mA• Compatibility to CMOS process

• Low Von : < 0.3V• High operating current : mA range

25nm> 107 @ 2uA

~ 0.5V2uA

Page 36: Recent Progress in Resistance Change Memory€¦ · Metal Oxide: Filament • Set : voltage-induced partial dielectric breakdown • Rest : disruption of conductive filament by high

Summary• A variety of mechanisms for switching proposed

– Interface switching, filament, SCLC, Electrochemical reaction– Role of oxygen ion (O2-) or vacancy (Vo

2+)– Substantial role of hydrogen in the vacancy model delineated

• Materials oriented issues and opportunities– Reproducibility and uniformity depends on defects/structure– Unipolar vs. Bipolar: depend on structure/process temp.– Single crystal, pure-amorphous, polycrystalline– Improved device performance vs. Process complexity– uniform (atomic scale) distribution of doping element

• Potential for exciting applications-- Replacement of flash -- New functionality such as non-volatile latch, programmable

interconnect-- Ultimate universal memory embedded in logic VLSIs