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Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University
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Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

Dec 23, 2015

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Page 1: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

Fabrication and Characterization of Ultra-narrow RRAM Cells

Byoungil Lee and H.-S. Philip WongElectrical Engineering,

Stanford University

Page 2: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

• Motivations• AlOx RRAM typical cell characteristics• Fabrication of ultra-narrow RRAM

cells• Characterization of ultra-narrow cells• Summary and discussion

Outline

Page 3: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

• Motivations– Issues with RRAM

• Over-SET by over-shoot current.• Poor LRS uniformity, large reset current, and

device failure.• Current-limiting devices are required.• Implementation of ‘Within-A-Cell-Current-

Limiter’.

– Study of scaling

Ultra-narrow RRAM Cells

Page 4: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

– Bipolar switching.– Large variation in LRS and IRESET.

AlOx RRAM Large Cell

AlOx

Pt

PtTiN

10nm

W

w

w

-2 -1 0 1 2-400

-200

0

200

400

Voltage (V)

Cu

rre

nt (

A) W = 10m

Page 5: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

AlOx RRAM Large Cell

0 500 1000 1500

103

104

105

Cycles

Re

sis

tan

ce(Ω

)

10m 0.5m

1k 10k0

0.2

0.4

0.6

0.8

1

Partial SETCurrent Overshoot

LRS (Ω)C

um

ula

tive

Fre

qu

en

cy

4.5kΩ

10m0.5m

– Filamentary conduction property. – Does not scale with the size.

Page 6: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

AlOx RRAM Large Cell

1k 10k0

0.2

0.4

0.6

0.8

1

Partial SETCurrent Overshoot

LRS (Ω)C

um

ula

tive

Fre

qu

en

cy

4.5kΩ

10m0.5m

– Filamentary conduction property. – Does not scale with the size.– LRS and IRESET are determined by Ilimit

0 2k 4k 6k0

50

100

1500 2k 4k 6k0

50

100

150

Current Overshoot

Partial SET

LRS (Ω)

10m

0.5m

Page 7: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

0.1 1 10 100

1

10

100

Limited SET current (mA)

Rese

t Cur

rent

( mA

) [Seo 04]

[Kinoshita 08]

I(RESET) = I(SET)

IRESET ISET in RRAM

Page 8: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

1

0.1

0.01 0.1 1 10 100Cell Area (m2)

Rese

t Cur

rent

( mA

) [Lee 08]

This work

1k

Cell Area (m2)LR

S ( Ω

)0.01 0.1 1 10 100

10k

100k [Lee 08]This work

Scaling Trend of RRAM

– Filamentary conduction property. – No scaling with the size in the previous works.– LRS of our RRAM cell does scale with the size!

Page 9: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

Ultra-narrow RRAM Cell using ALD AlOx

w

w

100nm

– Top-view SEM of the fabricated devices. – Smallest cell size: 50nm X 50nm

Page 10: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

- Top Pt: 40nm, TiN: 40nm- Oxides thickness: 7.4 nm- Bottom Pt: 40nm- Metal width: 100nm- AlOx width: 10nm

TiN

Pt

Pt

10nm

AlOx

SiO2

20nm

Ultra-narrow RRAM Cell using ALD AlOx

Page 11: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

Pattern bottom Pt lines

Deposit PECVD SiO2

Deposit reactively sputtered TiN at room temperature

Pattern top Pt lines

Dry-etch TiN and SiO2 usingthe top Pt lines as a mask

Wet-etch 10nm of SiO2

Deposit ALD AlOx at 300C

Dry-etch AlOx

PtSiO2

PtTiN

PtSiO2

PtTiN

PtSiO2

PtTiN

PtPtSiO2

PtTiN

d

w

tAlOx

Process Flow

Page 12: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

-4 -2 0 2-600

-400

-200

0

200

400

600

Voltage (V)

Curr

ent (

A) 4.7kΩ 14kΩ

26kΩ

400nm100nm50nm

DC I-V Characteristics

– SET current is limited without any external cur-rent-limiters.

– Due to resistive TiN layer and small contact area.

Page 13: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

0 0.01 0.02 0.030

200

400

600

800

1/Line width (1/nm)

100nm

50nm

Resi

stan

ce (Ω

)

300nm

Line Resistance

– Current-limiting is not a result of the long electrode line.

– New device features ‘Within-A-Cell-Current-Limiter.’

Page 14: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

0 200 400 600 800 1000

10k

1M

0.1G

Cycles

Resi

stan

ce ( Ω

)

50nm100nm

400nm

1k 10k 100k0

0.2

0.4

0.6

0.8

1

LRS (Ω)C

um

ula

tive

Fre

qu

en

cy

500nmRef. cell 400nm 100nm 50nm

Programming Cycle Test

– 500nm standard cell shows a broad tail in LRS distribu-tion.

– Ultra-narrow cells truncate lower-end of LRS distribution.

Page 15: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

1

0.1

0.01 0.1 1 10 100Cell Area (m2)

Rese

t Cur

rent

( mA

) [Lee 08]

This work

1k

Cell Area (m2)LR

S ( Ω

)0.01 0.1 1 10 100

10k

100k [Lee 08]This work

Scaling Trend of Ultra-narrow Cells

– Filamentary conduction property. – IRESET and LRS does scale with the size!

Page 16: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

0 50 100 150 200 250 300

10k

1M

100M0 50 100 150 200 250 300

10k

1M

100M

Cycles

Resi

stan

ce ( Ω

)Re

sist

ance

( Ω)

22

7

- SET/RESET: 30ns/1us

- SET/RESET: 4ns/20ns

Programming Speed

Page 17: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

0 4000 8000 12000

10k

1M

100M

Cycles

Resi

stan

ce ( Ω

)

Programming Endurance

– 104 programming cycles.

Page 18: Fabrication and Characterization of Ultra-narrow RRAM Cells Byoungil Lee and H.-S. Philip Wong Electrical Engineering, Stanford University.

Summary

• Demonstrated fabrication and char-acterization of ultra-narrow RRAM cells.

• Established new aspect of scaling trend of filamentary conduction de-vices.

• Within-A-Cell-Current-Limiter im-proves LRS distribution without inte-grating TRs.