JungDae-Han1
LeeKhwang-Sun1
ParkJun-Young1*
-
(Electronics Engineering, Chungbuk National University, Chungdae-ro 1, Cheongju 28644,
Korea.)
Copyright © The Institute of Electronics and Information Engineers(IEIE)
Index Terms
Back-biasing, data erase, flash memory, macaroni filler, 3-dimensional (3D) V-NAND
I. INTRODUCTION
As the pandemic accelerates the untact era, demand for mobile electronics has rapidly
increased. Especially, NAND flash storage, which consists of memory cells, enables
storage of data semi-permanently. Typically, memory cells contain a charge trap layer
(CTL) composed of Si3N4, as gate dielectric. The device structure of the cells in NAND flash has evolved
from 2-dimensional (2D) to 3-dimensional vertical NAND (V-NAND) for better density
and lower bit-cost.
In this context, recently, most NAND flash storage is fabricated based on the V-NAND
structure (1-3). Compared with the 2D based memory cell, V-NAND includes a poly-silicon channel,
as well as a buried dielectric layer underneath the channel. The buried dielectric
is called a macaroni oxide filler because of its geometry; it reduces variability
stemming from poly-silicon grains (4). For this reason, in contrast to back-biasing as applicable in 2D based memory cells
for better erase speed and operating configuration, back-biasing in V-NAND is impossible
due to the existence of the macaroni filler. Typically, there are several ways to
improve erase speed of V-NAND.
The first approach is gate dielectric engineering. For example, bandgap engineering
of tunneling oxide (e.g., BE-ONO) has already been applied for mass production (5,6). However, even though high-k dielectrics such as Al2O3 have been applied (7), further improvement of erase speed by gate dielectric engineering is difficult due
to uncontrollable gate leakage. The second approach is to use a novel erase configuration
such as thermal erase (8,9). The operation principle of the thermal erase is based on thermal excitation of electrons
under an intentionally-created high temperature environment. However, application
of thermal erase is difficult due to its complex operating configuration, high power
consumption, and thermal disturbance among memory cells.
The third approach involves bias configuration. For example, gate-indented-drain-leakage
(GIDL), a phenomenon in semiconductor physics, can be intentionally triggered (10). When high drain-to-gate bias (VDG) is applied. Then, excessive holes are generated
and drift from the drain to source through the poly-silicon channel. The holes increase
the channel potential and induce back-biasing in V-NAND. However, unfortunately, as
the number of V-NAND layers increases, the resistance of poly-silicon also increases.
Hence, control of hole injection and drift is difficult to improve. Although J. Jang
et al., (2) at Samsung Electronics Inc. demonstrated that back-biasing is available in TCATs
(Terabit Cell Array Transistor), back-biasing through a silicon substrate is only
applicable for cells in lower stories.
In this paper, we propose a novel V-NAND structure and fabrication process. Multi-layered
macaroni fillers composed of metallic core layers and dielectric outer layers are
proposed to maximize V-NAND erase speed. Through the metallic core layer, back-biasing
potential can be effectively transferred to all cells along the bit-line (BL) direction.
The back-biasing of gate-all-around (GAA) memory cells can improve erase efficiency.
All of the fabrication process and layout are compatible with the standard V-NAND
process. A comparison between the conventional V-NAND and the proposed structure will
be carried out under 3D simulations.
II. EXPERIMENTAL DETAILS
Fig. 1 shows the fabrication process flow of the proposed V-NAND structure for back-biasing.
SiO2 and Si3N4 are deposited iteratively on an Si-substrate, as shown in Fig. 1(a). After dry etching (Fig. 1(b)), O/N/O layers and a-Si (poly-Si) are deposited on the sidewall. The O/N/O can be
modified into BE-ONO, but no such layer was included in our simulation.
Then, barrier SiO2, which plays a role in isolation, is deposited underneath the poly-silicon channel.
An electrical conductive metallic (or metal) core layer fills the trench, as shown
in Fig. 1(c). Unlike conventional V-NAND strings that include macaroni fillers composed of only
SiO2, our proposed structure has a multi-layered macaroni filler composed of a metallic
core layer and barrier SiO2 (11). After that, etching of the top side and heavy doping of poly-Si deposition are performed
for drain region definition, as shown in Fig. 1(d). Then, dry etching, sacrificial Si3N4 removal, high-k blocking oxide deposition, and word-line (WL) formation are performed
(Fig. 1(e)-(g)). Finally, node separation and BL formation are performed (Fig. 1(g) and (h)).
The proposed fabrication processing and applied materials are fully compatible with
current NAND fabrication processing. Simulation studies to observe voltage distribution
through the metallic core layer were performed by aid of the 3D simulator COMSOL.
There are two reasons why we have used COMSOL as a simulator.
The first reason is for better simulation speed. Device structure in our proposed
structure is very complex as well as contains a lot of boundary conditions. Therefore,
the COMSOL can be preferred when using semiconductor models are not required. Considering,
this work focuses on voltage distribution through the metallic layer, applying semiconductor
simulator which requires lots of calculations are ineffective. The second reason is
for fair comparison with our previous work (11). Even though we have inferred that it is possible to apply back-biasing through the
metallic core layer, the evidence was not enough. In this context, we performed simulations
under the identical test vehicles such as simulator (i.e., COMSOL), back-bone structure,
and materials. It was also confirmed that potential distribution extracted by COMSOL,
was well matched with the measured data (12).
Fig. 2(a) shows the schematic geometry of the proposed V-NAND string for simulation. A V-NAND
string was designed with 10th floored WL for better simulation environment. Fig. 2(b) and (c) show cross-sectional view of the proposed NAND string cut along the WL and
BL directions. Compared to conventional V-NAND, the proposed V-NAND includes a metallic
core layer surrounded by barrier SiO2 and poly-silicon channel (Fig. 2(b)). Considering process compatibility with conventional fabrication processing, the
metallic layer was assumed to be identical to the WL material. Moreover, considering
that the electrical conductivity of thin film tungsten is lower than that of bulk
of 1.8 ˟ 107 S/m, the value was assumed to be 107 S/m (13). Other device geometry information was taken from previous papers (11,14,15). Detailed device dimensions and material information used for simulation are summarized
in Table 1.
Fig. 1. Fabrication process flow of V-NAND containing multi-layered macaroni filler
(a) and (b) Deposition of oxide and sacrificial silicon nitride layer, and dry etching
of hole, (c) Deposition of dielectric layers, poly-silicon channel, barrier oxide
isolation, and electrical conductive metallic core layer, (d) Etching of top layers
and deposition of oxide to avoid electrical short between BL and metallic core layer.
Then, heavily doped poly-silicon deposition for bit-line definition, (e) Selective
etching of sacrificial silicon nitride and oxide layer, (f) Deposition of blocking
oxide such as Al2O3 and WL metal, (g) and (h) Node separation, inter layer dielectric (ILD) deposition,
and BL metallization.
Fig. 2. (a) Tilted-view of proposed V-NAND string, (b) Cross-sectional image of the
proposed structure cut along the WL, (c) Cross-sectional image of the proposed V-NAND
cut along the BL.
Table 1. Parameters for simulation of multi-layered macaroni filler
|
Dimension [nm]
|
Material
|
WL thickness
|
20
|
W
|
Channel thickness
|
25
|
Poly-Si
|
Metallic core layer diameter
|
21
|
W
|
Barrier oxide thickness
|
4
|
SiO2
|
Tunneling oxide thickness
|
5
|
SiO2
|
Nitride thickness
|
8
|
Si3N4
|
Blocking oxide thickness
|
10
|
Al2O3
|
Si-substrate thickness
|
50
|
Si
|
BL thickness
|
100
|
W
|
Inter layer dielectric thickness
|
20
|
SiO2
|
III. RESULTS AND DISCUSSION
Fig. 3(a) shows a cross-sectional schematic image of a conventional V-NAND string. When back-bias
of 15 V is applied through the bottom silicon substrate, the voltage is gradually
distributed along the BL direction because of the low electrical conductivity of the
macaroni oxide and poly-silicon channel (Fig. 3(b)). The voltage distribution along the BL is not uniform; hence, the conventional V-NAND
structure is not suitable for back-biasing-assisted erase configuration.
Fig. 3. (a) Cross-sectional schematic of conventional V-NAND flash string along BL
direction, (b) Cross-sectional simulated potential distribution when positive voltage
(15 V) is applied to silicon substrate.
Fig. 4(a) shows a cross-sectional schematic image of the proposed V-NAND string. In contrast
to the conventional V-NAND, proposed structure includes multi-layered macaroni filler
composed of metallic core layer and the dielectric outer layer such as SiO
2. There is no structural difference between the conventional and the proposed V-NAND
structure except for metallic core layer. It has already been reported that the metallic
core layer shows better immunity against self-heating effect because of its superior
thermal conductivity
(11). When positive back-bias of 15 V is applied to the bottom silicon substrate, the
potential is effectively transferred from the bottom to the top layer owing to the
high electrical conductivity of the metallic layer. As back-biasing of V-NAND is possible,
there is no need to apply complicated erasing configurations such as those in the
GIDL method.
Fig. 4. (a) Cross-sectional schematic of proposed V-NAND flash string along BL direction,
(b) Cross-sectional simulated potential distribution when positive voltage (15 V)
is applied to silicon substrate.
Fig. 5 shows the extracted potential along the BL. The potentials of both the conventional
and the proposed structure were identically extracted at the surface of the metallic
core layer. In the case of the conventional 3D V-NAND, voltage drop along the BL was
1.4 V per WL due to the high resistance of SiO
2. Hence, actually, back-biasing is impossible under the conventional structure. However,
it was observed that the voltage drop was negligibly small under the proposed NAND
structure owing to the low resistance of the inserted metallic layer. In the case
of the proposed structure, extracted voltage drop at the 10th floor was only 20 mV.
Based on these results, it can be inferred that erasing of electrons by aid of back-biasing
can be further boosted if the back-biasing potential is higher than 15 V.
Fig. 5. Potential distribution extracted from Fig. 3 and 4. The potential of the proposed
structure was extracted at the surface of the metallic core layer. In the conventional
structure, identical point with the proposed structure was extracted for the fair
comparison.
However, time-dependent voltage characteristics should be confirmed to estimate the
minimum time required for back-biasing, as shown in
Fig. 6. The potential reached steady-state within 0.5 ps and was negligibly short compared
with the erasing speed as CTL is approximately hundreds of µs to ms. As a result,
even when the proposed structure and erasing configuration are applied for higher
stories of a NAND string (e.g., 512 floors), the time delay is not problematic.
Fig. 6. Time-dependent characteristic of proposed V-NAND string at surface of metallic
core layer.
Fig. 7 shows a simulated energy band diagram of the conventional and the proposed V-NAND
strings with respect to back-biasing. Sentaurus TCAD simulator was utilized for simulations.
In the conventional V-NAND string, voltage transfer from substrate to BL is difficult.
Hence, erasing configuration at high story cells (e.g., 10th floor) cannot be improved
by back-biasing, as shown in
Fig. 7(a). In contrast to the conventional V-NAND, the proposed structure contains a metallic
core layer in the middle of macaroni filler. Hence, voltage transfer from substrate
to BL is possible through the metallic layer. As a result, electrons stored at the
CTL can be effectively erased through the tunneling oxide, as shown in
Fig. 7(b).
Fig. 7. Simulated energy band diagram of (a) conventional, (b) proposed V-NAND string
during erasing configuration.
IV. CONCLUSIONS
Multi-layered macaroni filler was newly proposed for improvement of erase efficiency
in V-NAND. Potential distribution along the bit-line (BL) direction was investigated
based on simulation studies. It was confirmed that back-biasing is possible even with
the gate-all-around (GAA) device structure. The proposed V-NAND structure showed uniform
back-biasing potential, regardless of stories of word-lines (WL), because of the high
electrical conductivity of the metallic core layer. Stored electrons can be effectively
removed from the charge trap layer (CTL) by aid of applied back-biasing. As a result,
proposed multi-layered macaroni filler can improve erase efficiency in V-NAND without
large modification of fabrication process or layout. However, precise gap filling
during device fabrication, seems difficult even use of atomic layer deposition (ALD).
Hence, there might be a trade-off between erasing performance and fabrication cost.
ACKNOWLEDGMENTS
This research was supported by Chungbuk National University Korea National University
Development Project (2021).
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Author
Dae-Han Jung is currently pursuing the B.S. degree from the School of Electronics
Engineering, Chungbuk National University, Cheongju, Republic of Korea.
His current research interests include simulation of semiconductor devices.
Khwang-Sun Lee received the B.S. degree from the School of Electronics Engineering,
Chungbuk National University, Cheongju, Republic of Korea, in 2020, where he is currently
pursuing the M.S. degree.
His current research interests include simulation of semiconductor devices.
Jun-Young Park received the B.S. degree from the School of Electrical and Electronic
Engineering, Yonsei University, Seoul, South Korea, in 2014, and the M.S. & Ph.D.
degree from the Korea Advanced Institute of Science and Technology, Daejeon, South
Korea, in 2016 and 2020.
He is currently the Assistant Professor of School of Electronics Engineering, Chungbuk
National University, Cheongju, Republic of Korea.
His current research interests include reliability of semiconductor devices.