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A stackable cross point phase change memory
DerChang Kau, Stephen Tang§, Ilya V. Karpov, Rick Dodge§, Brett Klehn, Johannes A. Kalb, Jonathan Strand§,
Aleshandre Diaz§, Nelson Leung, Jack Wu§, Sean Lee, Tim Langtry§, Kuo-wei Chang, Christina Papagianni§,
Jinwook Lee, Jeremy Hirst§, Swetha Erra, Eddie Flores§, Nick Righos, Hernan Castro§ and Gianpaolo Spadini
Intel Corporation, Technology and Manufacturing Group, SC9-09, 2200 Mission College Blvd, Santa Clara, CA 95054 USA
§: Numonyx B.V. , R&D – Technology Development, 2550 N. 1st Street, Suite 250, San Jose, CA 95131
Tel:+1-408-765-0266 Fax:+1-408-653-8146 Email:DerChang.Kau@intel.com
Abstract
A novel scalable and stackable nonvolatile memory
technology suitable for building fast and dense memory
devices is discussed. The memory cell is built by layering
a storage element and a selector. The storage element is a
Phase Change Memory (PCM) cell [1] and the selector is
an Ovonic Threshold Switch (OTS) [2]. The vertically
integrated memory cell of one PCM and one OTS (PCMS)
is embedded in a true cross point array. Arrays are stacked
on top of CMOS circuits for decoding, sensing and logic
functions. A RESET speed of 9 nsec and endurance of 106
cycles are achieved. One volt of dynamic range
delineating SET vs. RESET is also demonstrated.
Introduction
PCM arrays with different selectors have been disclosed.
In a 0T1R configuration [3], the small read and write
windows pose a severe limitation to the size of the array.
In a 1T1R configuration [4], the paired MOS selector
limits the layout at 8λ2 or higher. Using a crystalline
bipolar selector [5, 6], cell sizes could approach ~5λ2;
however, decoding and selecting CMOS circuits share the
substrate with silicon selectors, resulting in reduced array
efficiency. Recent advances in thin film diode technology
improve layout efficiency and stack-ability [7] but the on-
off ratio of the thin film selectors will limit the size of each
array partition. In this work, a thin-film two-terminal
Ovonic Threshold Switch is deployed as the selector of a
memory cell. The symmetrical blocking or triggering
voltage, a.k.a. the threshold voltage, of the amorphous
alloy [8] provides the base for a robust inhibiting scheme
to isolate individual PCM cells in the cross point array.
OTS shares the matched physical and electrical properties
for PCM scaling. Given the compatibility of thin-film
PCMS with mainstream metallization schemes, multiple
layers of cross point memory arrays are feasible. Also,
this back-end technology is fully stackable over CMOS
circuits to achieve excellent array-efficiency and reduced
die size.
The Memory Cell
The physical construction of a memory cell is shown in
Fig. 1. The vertical stack of a PCMS cell consists of a top
electrode connecting to a column metal, an OTS and a
PCM interlinked by a middle electrode, and a bottom
electrode connecting to a row metal. The IV
characteristics are shown in Fig. 2. SET and RESET states
are delineated by the threshold voltages.
Fig. 2. The I-V Characteristics of a PCMS cell in SET and RESET.
Voltage is normalized to the threshold voltage of the SET state, Vt set.
Cell current is normalized to melting current, Imelt, the least current
required to amorphize the material. (see Fig. 4)
0.0
0.5
1.0
1.5
0.0 0.5 1. 0 1.5 2.0
Normalized Cell Voltage [V/Vt
SET
]
Normalized Cell Curren
t
●
SET
◊
RESET
Fig. 1. SEM cross section of a PCMS cell.
Bottom Electrode
PCM
Middle Electrode
OTS
Top Electrode
Column
Row
97-4244-5640-6/09/$26.00 ©2009 IEEE IEDM09-61727.1.1
The SET state exhibits lower threshold voltage than the
RESET state. The threshold switching characteristics of
OTS determine the threshold and sub-threshold of the SET
state. The higher threshold voltage of the RESET state is
attributed to the serial connection of two amorphous
alloys, OTS and amorphous PCM. These IV characteristics
shown in Fig. 3 are taken after a RESET pulse.
The programming transfer characteristics are illustrated in
Fig. 4. When current pulse amplitudes are lower than the
melting current level, Imelt, PCM is crystallized to a SET-
state (low resistance.) The SET-state threshold voltage,
Vtset, reflects OTS threshold switching characteristics. The
higher threshold voltage at RESET state is attributed to the
addition of amorphous PCM subject to electrical pulsing
amplitude higher than Imelt.
The Cross Point Array
With its low temperature processing, the thin-film PCMS
is inherently compatible with the present state of backend
metallization technologies. Therefore, the X/Y cross point
array does not require additional strapping for low
parasitic resistance. The strapless cross point topology
provides an ideal scaling path for 4λ2 implementation (Fig.
5.)
To electrically access a bit in a memory block, Vaccess is
applied to the selected column and 0V to the selected row.
The deselected row and column biases must be chosen so
that the voltage across each of the unselected cells is less
than the minimum threshold voltage in the block,
min(Vtset). This operating scheme can be modeled with an
inhibiting factor,
β
, where
β =
min(Vtset )/ Vaccess.
A. READ:
To ascertain the PCM state, a READ access bias is applied
to the selected cell to threshold switch SET but not
RESET. This access bias must be higher than the highest
SET threshold voltage, max(Vtset). Therefore, the READ
inhibiting factor is
β
R
=
min(Vtset )/ max(Vtset). Since the
SET threshold voltage is dominated by the OTS switching
mechanism, the OTS threshold distribution influences the
inhibiting latitude in READ.
B. WRITE:
To program a bit, a WRITE access bias is applied to the
selected cell. The access bias must be higher than the
highest RESET threshold voltage, max(Vtrst). Hence, the
WRITE inhibiting factor is
β
W
=
min(Vtset ) / max(Vtrst).
Consequently, the tradeoff between design latitude and
technology selection can be derived. The normalized
threshold voltage window between SET and RESET,
Fig. 5. The layout of PCMS array. The cross point array does not
require additional strapping to reduce wordline or bitline resistance.
The strapless cross point topology provides an ideal scaling path for
4λ2 implementation. CMOS circuit is placed under the memory array.
High area efficiency is thus achieved.
Fig. 4. Single cell PCMS electrical programming characteristics.
Current and voltage are normalized to Imelt and Vt set, respectively.
Each point is conditioned to the same initial states correspondingly.
0.5
1
1.5
2
2.5
00.511.5 2
Normalized Current Pulse Amplitude
Normalized Threshold Voltage
○ RESET-to-SET
■ SET-to-RESET
I
melt
Vt
set
Fig. 3 PCMS = PCM + OTS; The threshold behavior of a RESET
PCMS is equal to the additive result of the thresholds of OTS and
amorphous PCM in series. Voltage and current are normalized to
the threshold voltage and threshold current of OTS, Vtots and Itots
respectively.
0
1
012
V / Vt
ots
I / It
ots
OTS
PCM
PCMS
PCM+OTS
V
ots
V
p
cm
V
pcms
Threshold Snapback
IEDM09-618 27.1.2
Δ
Vtnorm, represents memory switching dynamic range. As
illustrated in Fig. 6, the inhibiting scheme stops working as
Δ
Vtnorm approaches 150% empirically. Moreover, a
smaller
Δ
Vtnorm yields a larger inhibiting factor. Larger
inhibiting factors provide wider design latitude for the
random access of a cross point array.
Experiments and Results
A. Physical construction:
A 64Mb PCMS cross point test chip is used as the
technology vehicle in this research. Cell sizes ranging
from 40nm to 230nm are explored. A 90nm CMOS
technology provides the base process flow for PCMS
integration. One memory layer is sandwiched between the
2nd and the 3rd levels of Cu interconnect (Fig. 7). The 3D
SEM image illustrates the compatibility of PCMS with
mainstream CMOS technology as well as the area efficient
topology in the vertical stack.
B. Operations:
Fig. 8 exhibits the programming transfer characteristics of
an array of 4096 independent, MOS-isolated bits. Each
group of the box plot represents the intrinsic program
distribution subject to each of pulse amplitudes.
No cross point operating disturbance is expected since
each of the bits in the array is MOS-isolated. However,
operating disturbances in a true cross point array can occur
and degrade distributions. For example, the program
distribution can be modulated by adjusting inhibiting bias
(Fig 9).
To eliminate the operating disturbance, inhibiting factor
optimization, such as device threshold targeting and
operating bias selection, must be deployed through proper
balance between technology and design.
C. Performance:
In addition to PCM’s non-volatility and cell-level
alterability, PCMS is also capable of high bandwidth and
Fig. 9 WRITE disturbances can occur in a PCMS cross point array.
The operating disturbance can be eliminated by bias optimization.
Inhibiting Bias 1
Inhibiting Bias 2
Optimized
Inhibiting Bias
Inhibiting Bias 1
Inhibiting Bias 2
Optimized
Inhibiting Bias
Fig. 8 Programming distribution of 4096 independent PCMS bits.
SET dist.
RESET dist.
Incomplete
SET/RESET dist.
synonymous with “disturb”
SET dist.
RESET dist.
Incomplete
SET/RESET dist.
synonymous with “disturb”
Metal 1
Metal 2
Row
C
olumn
Poly
Si-Substrate
Metal 1
Metal 2
Row
C
olumn
Poly
Si-Substrate
Fig. 7 One layer of the PCMS array fully integrated with a CMOS
technology. The memory cell stack, including rows and columns, is
shown sandwiched between M2 and M3. M3 is not shown.
Fi
g
. 6 Technolo
gy
choice of device
p
arameters vs. desi
g
n latitude.
30%
40%
50%
60%
70%
0% 50% 100% 150%
Normalized pgm Vt Window, [
Δ
Vt
norm
]
WRITE inhibiting factor [
β
W
]
≈
Δ
Vt
norm
Vt
rst
⎯
Vt
set
⎯
−
Vt
set
⎯
Vt
pcm
⎯
Vt
ots
⎯
β
w
min Vt
set
()
max Vt
rst
()
IEDM09-61927.1.3
long endurance. For example, shown in Fig. 10, PCM’s
high speed vitrification capability (RESET operation)
exhibits little or no degradation with OTS in series.
Cycling endurance of 106 cycles is demonstrated (Fig. 11).
More than 1 volt of dynamic range in a block of 2Mb
makes PCMS a good candidate for high density parts (Fig.
12).
Conclusion
The Ovonic Threshold Switch enables area efficient
memory layout and possesses compatible scaling attributes
with PCM for future random access memory and solid
state storage applications. Integrated with CMOS, PCMS
provides the most promising NVM technology in
scalability.
Acknowledgements
The authors gratefully acknowledge the valuable critiques
and continuous support from Al Fazio and Greg Atwood.
References
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Technical Digest, 36-5, p.803, 2001
[2] Stanford R. Ovshinsky, "Reversible electrical switching phenomena in disordered structures," Physical Review Letter Vol. 21, No. 20, pp.1450-1453,
Nov. 11, 1968
[3] Yi-Chou Chen, C.F. Chen, C.T. Chen, J.Y. Yu, S. Wu, S.L. Lung, Rich Liu and Chih-Yuan Lu, "An access-transistor-free (0T/1R) non-volatile
resistance random access memory (RRAM) using a novel threshold switching, self-rectifying chalcogenide device," IEDM Technical Digest, ’03, S37P4
[4] Y.N. Hwang, J.S. Hong, S.H. Lee, S.J. Ahn, G.T. Jeong, G.H. Koh, J.H. Oh, H.J. Kim, W.C. Jeong, S.Y. Lee, J.H. Park, K.C. Ryoo, H. Horii, Y.H. Ha,
J.H. Yi, W.Y. Cho, Y.T. Kim, K.H. Lee, S.H. Joo, S.O. Park, U.I. Chung, H.S. Jeong and Kinam Kim, "Full integration and reliability evaluation of
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[5] Fabio Pellizzer, Augusto Benvenuti, Robert Gleixner, Yudong Kim, Brian Johnson, Michele Magistretti, Tina Marangon, Agostino Pirovano, Roberto
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No.2 pp.209-220, 1978.
Fig. 12 RESET and SET distributions within a block of 2Mb. ΔVt
of x-axis is referenced to the mean Vt of SET state. This work
demonstrates more than 1V of window in memory array.
Fig. 11 PCMS cycling endurance: Cell SET Vt distribution vs. R/W
cycling counts. Degradation tails (3.5σ) developed after 1 million
cycles.
-100%
-80%
-60%
-40%
-20%
0%
1E+0 1E+2 1E+4 1E+6 1E+8
R/W Cycle Counts
% SET Vt change from fresh device
Fig. 10 PCMS is capable of high speed writes. Significant
programmed Vt window is achieved at pulse width as narrow as 9
nanoseconds. The pulse amplitude is the same for all pulse widths.
0%
25%
50%
75%
100%
1 10 100 1000
Pulse Width [ns ec ]
ΔVt [%]
IEDM09-620 27.1.4