Overview of Future Memory Devices - from Stacked Memory...
Transcript of Overview of Future Memory Devices - from Stacked Memory...
IFST 200519-21 June 2005, Yokohama, Japan
Overview of Future Memory Devices - from Stacked Memory, Gain Memory,
SEM to Molecular Memory
Kazuo Nakazato
Nagoya University
SRAM DRAM FLASHhigh-speed low cost
high-densitylow cost
high-density
server, CPUcache memory
computermain memory replacement of hard disk
ROMmobile equipment
high-speed
Memory
Feature
Application
Memory Cell
low power
Semiconductor Memories
6 - 8 F2 4 - 10 F2130 F2
10 ns 40 ns 10 μs
Cell Size
Access Time
Source/Drain
substrate MOSFET
Gate
Stacked Vertical
MOSFET
insulator
Via
Stacked Vertical MOSFET
Stacked Vertical MOSFET
substrate MOSFET
no PWELL-NWELL isolation
pMOSFET
nMOSFETStacked Vertical
MOSFET
polycrystalline silicon channel
performance degradation when carriers transport across grain boundaries
columnar or disc-shaped grains
vertical carrier flow mainly without crossing any grain boundaries
stacked
Why Stacked Vertical ?
グレイン
バンダリ
グレイン
バンダリ
伝導帯
価電子帯
深い準位
ΨB= 8εs pqNST
2
ΨB : barrier height of grain boundaryNST : trap density at grain boundaryεs : silicon permittivityp : carrier density
3-d Memory Cell
grain boundary
EC
EV
deep level
gate oxide
source
drain
gate
gate
SiO2
polycrystalline silicon
channel
ON current [μA]0 50 100
3μm
3σ
2σ
σ
0
-σ
-2σ
-3σCum
ulat
ive
Pro
babi
lity
Example of Distribution of Grain-boundaries
measuredanalysis from the distribution of grain boundaries
Distribution of ON currents of SV-MOSFET
transistor size(0.2μmx0.2μm)
plan view
cross sectional view
300n
m
pMOS 1.2VW=2μm
show very similar to single-crystal MOSFET
1.E-15
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
-4 -3 -2 -1 0 1 2 30.E+00
1.E-04
2.E-04
3.E-04
4.E-04
5.E-04
0 1 2 3
1V0.1V
VDS=2V
VGS [V]
I DS
[A/μ
m]
VDS [V]I D
S[A
/μm
]
3V
2V
1V
VGS=
measureddevice simulation with 300 cm2/Vs
Idealsubthreshold slope~ 60 mV/dec.
Low OFF current
High ON current ~300μA/μm
Characteristics of SV-MOSFET
NMOS
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
-1.5-1.0-0.50.00.5
Vg[V]-Id[A/cell]
Characteristics of p-type SV-MOSFET stacked on substrate MOSFET
substrate MOSFETsubstrate MOSFET
0.0 0.1 0.2 0.3 0.4 0.5.01
.1
1
5102030
50
70809095
99
99.9
99.99
Vth [V]
累積頻度 (%)
SVMOSFET
substrate MOSFET
0.06 0.07 0.08 0.09 0.10 0.11.01
.1
1
5102030
50
70809095
99
99.9
99.99
subthreshold voltage slope [V/dec]
累積頻度 (%)
SVMOSFET
substrate MOSFET
SVSV--MOSFETMOSFET
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
1.E-04
1.E-03
-1.5-1.0-0.50.00.5
Vg[V]
-Id[A/cell]
SVMOSFET
substrate MOSFET
VDS=-1.2V, RT
VDS=-1.2V, RTH Matsuoka, T Mine, K Nakazato, M Moniwa, Y Takahashi, M Matsuoka, H Chakihara, A Fujimoto, and K Okuyama, Symp. VLSI Technol. Dig. Papers 2004
PMOS
533MHz 64Mbit SRAM9kbit deficit
T Kikuchi, S Moriya, H Matsuoka, K Nakazato, A Nishida, H Chakihara, M Matsuoka, and M Moniwa, IEDM Dec. 2004
2.0
1.5
1.0
0.5
90 130 [nm]
32Mb
64Mb
128Mb
[μm2]
SRAM Cell Size vs Process Node
Conventional
SVMOS
Cell size of next generation can be achieved by the present process node
Huge investment is required for setting up next process node.Memory with minimum cell size may become standard cell finally.
Cel
l Siz
e
Process Node
Semiconductor Memories
SRAM DRAM FLASHhigh-speed low cost
high-densitylow cost
high-density
server, CPUcache memory
computermain memory replacement of hard disk
ROMmobile equipment
high-speed
Memory
Feature
Application
Memory Cell
low power
6 - 8 F2 4 - 10 F2130 F2
10 ns 40 ns 10 μs
Cell Size
Access Time
CL
(fF),
CS
(fF),
A(μ
m2 )
, VS
(V) 104
103
102
101
100
10-1
10-2
16K 256K 4M 64M 1G 16G
Memory Capacity (bits/chip)
CL
CS
AVS
DRAM 1-T cell
memory node(VDD, 0)
CS
CL
VSVDD2
bit line
word line
HM52Y64165FTT-75
cell area
VS ~ VDDCS
2CL
0
10
20
0.3 0.2 0.1 0.07 0.05minimum feature size (μm)
post DRAM
capacitor-lessFabrication Limit
aspe
ct ra
tio
1T cell
teff =0.5nm CS=30fF
post DRAM cell
J.M.Park et alIEDM 2002
VS
CS
VS
Gain Cell
memory node
large capacitor
memory node
large capacitor
100fF
0.1fF100fF
30fC 0.1fC
bit line
MOSFET
memorynode
word line
Minimum sized gain cell (~ half of DRAM 1-T cell)Stacked structure
Tunnel transistorhigh ON/OFF current ratio (high speed/long retention time)
PLEDM - memory cell
Si substrate
MOSFET
verticaltunnel
transistor
GND
word line
bit line
senseline
built-in coupling capacitor
Si Sii-Si
n+-Si
i-Si
n+-Si
gate
source
drain
barrier
insulator
(a) (b)
source
barrierdrain
shutter
gate
Conduction band energy diagramSchematic cross-sectional viewshowing device operating principle
energy
source
drain
modulationby gate bias
OFF
ON
Stacked Tunnel Transistor - PLEDTR
50nmDark field TEM
Source-barrier
Drain-barrier
SOURCE
DRAIN
GATE
Source/Drain Barriers
Impurity Diffusion Barrier from heavily doped source/drain
SOURCE
DRAIN
Diffusion constantthrough grain boundaries ismore than 100 times higherthan the diffusion constant in grain.
graingrain
741369
Effect of Source and Drain Barriers
without tunnel barrier
with tunnel barrier
Si3N4~0.8nm
CO
NC
EN
TRA
TIO
N
(ato
ms/
cc)
DEPTH(μm)0 0.5 1
intrinsic-Si
tunnel barrier
n+ -Si n+ -Si
CO
NC
EN
TRA
TIO
N
(ato
ms/
cc)
1021
1020
1019
1018
1017
1016
1015
1021
1020
1019
1018
1017
1016
1015
0
10
20
Vth (V)-1 0 1 2
Num
ber
0
10
20
30
40
50
60
Vth (V)-1 0 1 2
Num
ber
distribution of threshold voltage
μ= 43.3 cm2/Vsμ= 100 cm2/Vs
limited limitedmobility tunnel barrier
ON
cur
rent
(arb
. uni
t)
0 1 2
ON current
thickness of Si3N4 tunnel barrier (nm)
1
0.1
0.01
0.001
0.0001
0.00001
10
low pressure rapid thermal nitridation
1time (min.)
thic
knes
s (n
m)
0.8
direct nitridation of silicon
<< 1min.
>> 1min.
source barrier
drain barriershutter barrier
self-limiting growth
Formation of Stable Thin Tunnel Barriers
VDS =1.5V1μ
1n
1p
1f0 1 2
VGS (V)
I DS
(A)
3
source
drain
gate
barriers
45nm
60nm
0 1 2VDS (V)
301
234
I DS
(μA)
VGS =3V2.8V2.6V2.4V2.2V2V
60 nm channel PLEDTR
K Nakazato, K Ito, H Mizuta, and H AhmedElectron. Lett., 35 (1999), pp.848-850
I/O
VDD
φp
φY
φRW
VW1
VW2
VN1VN2
VDW
VDR
100fF100fF
VW
1φ p
φ RW
I/Oφ Y
VN
1 (V
)V
N2
(V)
VD
R (V
)V
DW
(V)
0 100 200
t (nsec)
high
low
WH WL
S R r S R rS R S R
Vth
0
0
0
0
0
0
1
0
1
01
-1-2
01
-1-2
Operation of PLEDM device
MOSFET
PLEDTR
VDS =1.5V1m
1μ
1n
1p
1f-1 0 1 2
VGS (V)
I DS
(A)
Vth
MOSFET
PLEDTR
VDS =1.5V1m
1μ
1n
1p
1f-1 0 1 2
VGS (V)
I DS
(A)
Vth
plan view cross sectional view
SiO 2
metal
n+
bit lineword line
p+-Si
Si substrate
Memory Cell Layout
DRAM 1-T cell 6-8F2
Unit cell2.5F x 2F = 5F2
1M 4M 16M 64MDRAM 1-T
256M
1G
PLEDM
SEM: single-electronmemory
107
Electron Number / bit
106
105
104
103
102
10
1
high-εcapacitor
1990 2000 2010 2020
Year
4G 16G 64G
3DCapacitor
withoutcapacitor
1T
gaincell
chargingenergy
SEM
Electron Number Stored in a Memory Cell
2Ce2
energy
eV
V
electron flow rate
Coulombblockade region
zero voltage
voltage applied
0
EC
E =C
Charging energy by one electron
VC
Coulomb gapvoltageV ~ E /eC C
Coulomb Blockadetunnel barrier
small island
memory node Cg
Vg
CSmultiple-tunnel-junction
V
I
0 VC
-VC
Coulomb blockade
eVC = 2Ce 2
Single-electron Memory
Cou
lom
b bl
ocka
deVg
memory-node voltage V
constant electron-number on memory node
V =Cg Vg – e n
C
C + Cg + CS
tunnel barriersmall island
T = 4.2K
Cur
rent
(nA)
offset 10nA per 0.1V gate step
VDS (V)
T = 4.2K
Cur
rent
(nA)
offset 10nA per 0.1V gate step
VDS (V)
SiO2Si substrate
Single-crystal Si, doped with P 1019cm-3
30nm
Silicon In-plane Gate Multiple-Tunnel-Junction
40nm
Electron islands Tunnel
junctions
Ionized donor
10 nm
20 nm400 nm
Naturally formed Electron Islands
• heavily doped silicon nanowire• Randomly distributed dopants• Self-consistent calculation with
Thomas-Fermi approximation
G. J. Evans, H. Mizuta, and H. Ahmed, Jpn. J. Appl. Phys. 40, pp. 5837-5840 (2001)
R. J. Blaikie, K. Nakazato, R. B. S. Oakeshott, J. R. A. Cleaver, and H. Ahmed, Appl. Phys. Lett. 64, pp. 118-120 (1994)
VDT
IDD
VG
IDD
VGVDT
electron storage node
VDT (Volts)
I DD
(nA)
-0.12 0.120
1
0
VG (Volts)
I DD
(nA)
-3.3 -3.2 -3.1 -3
1
0-2.9
Si Single-electron Memory
< 30nm
N. J. Stone and H. Ahmed, Appl. Phys. Lett. 77, pp. 744-746 (2000)
0.1
0.3
0.5
0.7
-0.03 0 0.03
Ele
ctro
met
er o
utpu
t I D
D(n
A)
Write line Voltage VDT (V)
0.2
0.3
0.4
-0.02 0 0.02
Ele
ctro
met
er o
utpu
t I D
D(n
A)Write line Voltage VDT (V)
one bit = one electron
bit l
ine,
VB
word line, VW
memory node
IS
bit l
ine,
VB
word line, VW
memory node
ISVB - VW
VW
VB
write “0” write “1”
VB - VW
VW
VB
write “0” write “1”
4.2K
70
80
90
100
0.4 0.6 0.8 1 1.2
time (sec)
I S(n
A)
VW
VB
4.2K
70
80
90
100
0.4 0.6 0.8 1 1.2
time (sec)
I S(n
A)
VW
VB
124
126
128
130
0 100 200 300
I S(n
A)
time (sec)
124
126
128
130
0 100 200 300
I S(n
A)
time (sec)
Random Write to Single-electron Memory Cell Array
write pulse width = 5ns
N J Stone, H Ahmed, and K Nakazato,IEEE EDL 20, pp. 583-585, 1999
3x3 bit L-SEM array0 0.5 1 1.5 2 2.5
time (s)
-0.2
0
0.2
0.4
0.6
0.8
'0''1'
'0'
1.01.5
2.0
2.5
3.0
5.0
Volta
ge (V
) 4.0
3.0
2.0
1.0
0
'0'Vo
ltage
(V)
IDS
(μA
)IDS0
VRWL
VWWL
VD
VSVD0
VS0
IDS
Single-electron Transistor – CMOS Hybrid Memory Array
high-drivability
single-electron control
Z. A. K. Durrani, A. C. Irvine, H. Ahmed, and K. Nakazato, Appl. Phys. Lett. 74, pp. 1293-1295 (1999)
109
106
103
100
10-3
10-6
10-9
0 0.5 1.0island size [nm]
rete
ntio
n tim
e [s
ec]
0.5nm
110C
1.5
Molecular Single-electron Memory
Molecular single-electron memory
Self-assembled monolayerdonor-(π-bridge)-acceptor dye
Collaboration with Cranfield University, U.K.
S(CH2)10
N
HCN
NCN
C
(CH2)n
S(CH2)10N
HCN
N
CN
(CH2)n
Au
Au
Au
C
Current–voltage characteristics of a self-assembled monolayer on a gold-coated substrate and investigated using a decanethiol-coated gold tip.
PLEDM
(1993)
multiple-tunneljunction
(2001)
0.2μm
2nm
commercialsingle-electron
memory
commercialsingle-electron
memory
First-demonstratedexperimental
single-electron memory
First-demonstratedexperimental
single-electron memory
sense transistor
precise controlof electrons
+large drivability
Summary
gate oxide
source
drain
gate
gatechannel
SVMOS
(2004)
molecularsingle-electron memory
tunnelbarrier