3d charge trapping (ct) nand flash - sematech charge trapping (ct) nand flash. 2 outline why does...

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1 Yen-Hao Shih Macronix International Co., Ltd. Macronix International Co., Ltd. Hsinchu Hsinchu , Taiwan , Taiwan Email: Email: [email protected] [email protected] 3D Charge Trapping (CT) NAND Flash

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1

Yen-Hao Shih

Macronix International Co., Ltd.Macronix International Co., Ltd.HsinchuHsinchu, Taiwan, Taiwan

Email: Email: [email protected]@mxic.com.tw

3D Charge Trapping (CT) NAND Flash

2

Outline

� Why Does NAND Go to 3D?

� Design a 3D NAND Flash Memory

� Challenges and Opportunities in 3D CT NAND Flash Memory

� Summary

3

Floating Gate (FG) Flash Memory

Source

Oxide

Floating gate

Control gate

Drain

Single cell structure

ONO

~4F2~10F2

� 1967 FG Transistor invented by D. Kahng and S. M. Sz e (Bell Labs)� 1984 NOR Flash invented by Fujio Masuoka (Toshiba)� 1987 NAND Flash invented also by Fujio Masuoka (Toshi ba)

4

Flash Memory

NOR(Fast for Code Access)

NAND(High Density for Data Storage)

Flash Memory Applications

5

Scaling of FG NAND Memory (2D)

90nm D.C. Kim, et al., (Samsung)

IEDM 2002

0.25umK. Shimizu, et al.,

(Toshiba) IEDM 1997

25nm K. Prall, et al., (Micron)

IEDM 2010

1/100 of area in 13 years(~ 26.5 increase, or one node per 2 years)

6

Recent Scaling is Even Faster(at 1.5 Year/Gen)

YEAR

100

10

20

30

40

50

60

07Q1 Q2 Q3 Q4

08Q1 Q2 Q3 Q4

09Q1 Q2 Q3 Q4

10Q1 Q2 Q3 Q4

11Q1 Q2 Q3 Q4

IMFTSamsungToshibaHynix

Des

ign

Rul

e (n

m)

7

2D Scaling Fulfills Demands and 2D Scaling Fulfills Demands and Creates New Applications Creates New Applications

Kinam Kim (Samsung), IMW 2010

8

However, 2D Scaling is Running Out of Electrons

Number of electrons in FG device (~ 20 for 10nm device)

ONO and Tunnel Oxidecan’t be scaled.

For the same Vt window,

∆Q = C * ∆Vt,

the electron number decreases as NAND cells are scaled down.

Electron number of FG

Technology Node: F (nm)

10 100N

e: E

lect

ron

Num

ber

10

100

1000

GCR=0.7, Tono=15 nm, Tox=9nmGCR=0.65, Tono=13 nm, Tox=8nm

Source

Tunnel Oxide

Floating gate

Control gate

Drain

Single cell structure

ONO

9

Impact of the Small Number of ElectronsNumber of electrons per logic level

Node 45nm 32nm 22nm 16nm 11nm 8nm

SLC 400 200 100 50 25 13(2 levels)

MLC 140 70 35 18 10 5(4 levels)

TLC 60 30 15 8 4 2(8 levels)

QLC 30 15 8 4 2 1(16 levels)

OLC 2 1 0.5 0.2 0.1 0.05(256 levels)

Statistical fluctuation ~ √√√√N / N. N = 10 ���� 30%.

10

Solution is the 3D NAND Flash

Stack up 2D devices

Punch through multiple layers

2-layer TANOS NAND(Epitaxial Si growth)Samsung: IEDM 2006

2-layer BE-SONOS NAND (TFT device)Macronix: IEDM 2006

Bit-cost scalable (BiCS) TFT SONOSToshiba: VLSI 2007

C.Y. Lu (Macronix), Semicon Taiwan 2010

11

Difference between 3D Stacked NANDand BiCS

H. Tanaka, et al., (TOSHIBA), VLSI 2007

� Both types maintain the electron number at a reason able level.� 3D Stacked NAND can’t further reduce cost when laye r number >=4.� BiCS uses only one critical contact drill hole for m any layers so the bit cost is scalable, even when more than 16 layers are used.� Later 3D NAND technologies have followed the BiCS co ncept.

12

Outline

� Why Does NAND Go to 3D?

� Design a 3D NAND Flash Memory

� Challenges and Opportunities in 3D CT NAND Flash Memory

� Summary

13

To Build 3D NAND, Start from 2D

� Conventional structure� Charges stored in FG� Charges in/out through

the tunnel oxide.

� SONOS CT structure� Charges stored in nitride� Charges in/out through

the tunnel dielectric (ONO here).

14

How NAND Flash Works? Asymmetric E-fields and Jg On/Off Ratio

• P/E • High On/Off Ratio

CG

IPD/Blocking Oxide

ChargeStorage

TunnelOxide

Etunnel

EblockingSubstrate

e-

CG

IPD/Blocking Oxide

ChargeStorage

TunnelOxide

Etunnel

EblockingSubstrate

e- CG

IPD/Blocking Oxide

ChargeStorage

TunnelOxide

Etunnel

Eblocking

Substrate

e-

h+

CG

IPD/Blocking Oxide

ChargeStorage

TunnelOxide

Etunnel

Eblocking

Substrate

e-

h+

Program Erase

E-field

Jg (log scale)

Fast P/E

GoodRetention

� FG: GCR design� CT: high WF CG

high-K blockingONO tunnel dielectric

15

Glance over Various 2D CT Devices

Best reported reliability, no new process

Theoretically the highest

performance

H. T. Lue et al., (Macronix), TDMR 2010

16

Retention of 2D BE-SONOS NAND

� Retention is excellent, and there is no single tail bit.� The best reported CT reliability so far.� BE-SONOS fundamentally solves traditional CT erase- retention dilemma.

75nm BE-SONOS (Non-cut-ONO), P/E=1K

VT (V)

Bit

Cou

nts

100

101

102

103

104

105Before bake10min100min1100min5420min7230min10080min

PVDisturbed EV

150C Baking

C. C. Hsieh, et al., (Macronix), IEDM 2010H.T. Lue, et al.,

(Macronix), IEDM 2005

17

CT is Easier than FG for 3D

� 3D CT devices are simpler in topology.� 3D CT devices are smaller than 3D FG devices.� CT is more process-friendly.

C.H. Hung, et al., (Macronix), VLSI 2011

SungJin Whang, et al., (Hynix), IEDM 2010

18

~2006 2007 2008 2009 2010 2011

Stacked NANDIEDM 2006

Multi TFTIEDM 2006

BiCSVLSI Symp

P-BiCSVLSI Symp

VSATVLSI Symp

VG-NANDVLSI Symp

TCATVLSI Symp

VG TFTVLSI Symp

S-SGTIEDM 2001

Univ. of Tokyo DC -SFIEDM

Hybrid 3DIMW

SO

NO

S/T

AN

OS

FG

Stacking Devices:High Process Cost

BiCS Concept: Low Process Cost

Various 3D NAND Architectures

PNVG TFTVLSI Symp

19

In 2010, the Last of Several Crucial Elements Fell into Place for 3D NAND

2005, BE-SONOS, (Macronix)2007, BiCS (Toshiba)2009, Vertical Gate (VG) NAND (Samsung)2010, 3D Decoding (Macronix)

There are occasionally short windows in time when incredibly important things get invented that shape the lives of humans

– Steve Wozniak

20

Macronix’s BE-SONOS 3D NAND

� 75nm half-pitch, 8-layer device is fabricated.� Equivalent cell size = 0.001406 um 2 (MLC).� Each device is a double-gate TFT BE-SONOS device.

H. T. Lue et al., (Macronix), VLSI 2010

21

3D Decoding Method A —by Using Island Gate Devices

� The method uses self-boosting scheme.� Conventional WL, BL are grouped into “planes”.� One additional SSL’s device also grouped into “planes”.� Three planes select a memory cell.

H. T. Lue, et al., (Macronix), VLSI 2010

22

3D Decoding Method B —by Using P-N Polysilicon Diode � 1st phase, decodes a NAND vertical plane, by conventional self-

boosting.� 2nd phase, decodes a layer in the selected plane by source-side

biasing.

C.H. Hung et al., (Macronix), VLSI 2011

23

Comparison among the Architectures

[P-BiCS] R. Katsumata, et al, VLSI Symposia, pp. 136-137, 2009. [TCAT] J. Jang, et al, VLSI Symposia, pp. 192-193, 2009. [VSAT] J. Kim, et al, VLSI Symposia, pp. 186-187, 2009. [ VG] W. Kim, et al, VLSI Symposia, pp. 188-189, 2009.

24

Outline

� Why Does NAND Go to 3D?

� Design a 3D NAND Flash Memory

� Challenges and Opportunities in 3D CT NAND Flash Memory

� Summary

25

Process Integration for 3D CT NAND Flash Memory� 3D memory in FEOL or BEOL?� CMOS under or beside the memory array?� How to handle PL layers left on periphery area� Planarization between 3D memory and 2D CMOS� Thermal budget management

Takashi Maeda, et al., (Toshiba), VLSI 2009

26

HK-MG for Better Performance� HK can reduce the E-field and suppress the gate inj ection.� MG can reduce WL resistivity for faster R/W. � SEMATECH has been engaging HK-MG for years. The

experience should be very useful to 3D CT NAND community.

Jaehoon Jang, et al., (Samsung), VLSI 2009

27

Contact Holes for Layers� Contact holes for layers are very

area consuming. � Which approach is the most

compact and manufacturable?

Jaehoon Jang, et al., (Samsung), VLSI 2009

H. Tanaka, et al., (Toshiba), VLSI 2007

Jiyoung Jim, et al., (UCLA), VLSI 2008

28

Patterning and Etching

� At 5xnm node, 3D memory should be more than 32 layers, in order to compete with 1Z nm MLC NAND .

� For 30nm layer pitch, 32 layers gives a stack height of 960nm.

� The hole etching is challenging not only due to the high A/R but also due to different materials .

Jungdal Choi, et al., (Samsung), VLSI 2011

29

Scaling or Stacking or MLC

Number of Layer for 3D stacks

0 5 10 15 20 25 30

Rel

ativ

e B

it C

ost

Ref

. (25

nm M

LC F

G N

AN

D)

F=66nm, 6F2

F=50nm, 6F2

F=35nm, 4F2

F=25nm, 4F2

F=25nm, 6F2

VG possible

1

Log

scal

e

� In 3D VG NAND, there are 3 ways to shrink equivalent cell size.

� Pitch scaling� BL gap fill-in� WL bridging

� Layer stacking� Deep etching and profile control

� Multi-level cell� Device variation

� Which is the right way in terms of business?

30

Polysilicon TFT Channel Engineering

� The Worst-On-Current (WOC) of the NAND string is strongly affected by the electron mobility in polysilicon . It should be carefully engineered.

� Polysilicon uniformity on the same layer and layer-to-layer uniformity are both challenging.

Y. Fukuzumi, et al., (Toshiba), VLSI 2007

M. Mizukami, et al., (Toshiba), SSDM 2009

31

In 2D-to-3D Paradigm Shift, Challenges = Opportunities

� By 2013, 3D NAND Flash is going into commercialization. This will be the biggest paradigm shift in NVM business .

� To make 3D NAND Flashhappen, collaboration should be considered.

Jungdal Choi, et al., (Samsung), VLSI 2011

32

Summary� 2D FG NAND is running out of electrons. 3D is a must to meet demands.

� For 3D NAND Flash, CT type is more process-friendly, and VG is the most scalable architecture.

� Single deep etching (for realizing the BiCSconcept) and polysilicon TFT device uniformity are the most challenging topics.

� Macronix and other NAND giants are dedicated in this field for years. To accelerate the progress, collaboration is a good way, and should be considered.