Chunlong Li’s research while affiliated with Chinese Academy of Sciences and other places

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Publications (11)


Fig. 1 (a) The schematic diagram of Co 2 MnSi/GaAs/PZT heterostructures controlled by piezo-voltages. When the piezo-voltages were applied, the direction of the strain is parallel to the z-axis. The [1À10] and [110] directions are parallel to the z-axis in samples I and II, respectively. The inset figures are the schematic of an axially acting multilayer piezo-stack and the structure of the magnetic film. (b) The magnetic hysteresis loops of the Co 2 MnSi thin film in the initial state along the in-plane [110], [1À10], and [100] directions. The inset shows the saturated magnetization in the [100] direction with 420 Oe magnetic field.
Fig. 2 The magnetic hysteresis loops under different piezo-voltages (from À60 V to 50 V; step is 10 V) along the in-plane [1À10] and [110] directions. (a) The magnetic hysteresis loops in the [1À10] direction are square curves with U PZT > À10 V. (b) Contrary to (a), the square curve changed to two-step curves with U PZT < À30 V and the saturated field increased with the increase of U PZT absolute value. (c) The magnetic hysteresis loops in the [110] direction are changed to two-step curves from square curves with U PZT > 0 V. (d) The magnetic hysteresis loops keep the square curve with U PZT < À30 V (compressed states).
Fig. 3 The magnetic properties of the Co 2 MnSi film under different piezo-voltages. (a) Compared with the Co 2 MnSi film under different piezovoltages, the magnetic hysteresis loops of [1À10] and [110] directions keep square and two-step curves with U PZT ¼ 40 V (stretched states), respectively. (b) The two-step axis and the square axis are exchanged with U PZT ¼ À40 V (compressed states). (c) The piezo-voltage dependence of the saturation field in the [1À10] and [110] directions; the voltage step is 5 V. (d) The magnetic hysteresis loops maintain the hard axis in the [100] direction under different piezo voltages.
Fig. 4 The magnetic hysteresis loops under different piezo-voltages (from À40 V to 90 V, step is 10 V) along the in-plane [110] and [1À10] directions of the sample II. (a) The magnetic hysteresis loops in the [110] direction change to square curves from two-step curves with U PZT > 20 V (stretched states). (b) The magnetic hysteresis loops in the [110] direction keep the two-step curves with U PZT < À20 V and the saturation field increase with the negative piezo-voltage increase. (c) The magnetic hysteresis loops in the [1À10] direction are changed to two-step curves from square curves with U PZT > 40 V. (d) The magnetic hysteresis loops keep the square curve with U PZT < À20 V in the [1À10] direction.
Fig. 5 The magnetic properties of the Co 2 MnSi film under different piezo-voltages. (a) The piezo-voltage dependence of the saturation field in the [1À10] and [110] directions; the voltage step is 10 V. (b) The magnetic hysteresis loops maintain the hard axis in the [100] direction under different piezo-voltages. The inset is the definition of the q and a. q(a) is the angle between the magnetization (magnetic field) and [1À10] direction.

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Dual-axis control of magnetic anisotropy in single crystal Co 2 MnSi thin film through piezo-voltage-induced strain
  • Article
  • Full-text available

May 2022

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79 Reads

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siwei Mao

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Chunlong Li

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[...]

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Voltage controlled magnetic anisotropy (VCMA) has been considered as an effective method in traditional magnetic devices with lower power consumption. In this article, we have investigated the dual-axis control of magnetic anisotropy in Co2MnSi/GaAs/PZT hybrid heterostructures through piezo-voltage-induced strain using longitudinal magneto-optical Kerr effect (LMOKE) microscopy. The major modification of in-plane magnetic anisotropy of the Co2MnSi thin film is controlled obviously by the piezo-voltages of the lead zirconate titanate (PZT) piezotransducer, accompanied by the coercivity field and magnetocrystalline anisotropy significantly manipulated. Because in-plane cubic magnetic anisotropy and uniaxial magnetic anisotropy coexist in the Co2MnSi thin film, the initial double easy axes of cubic split to an easiest axis (square loop) and an easier axis (two-step loop). While the stress direction is parallel to the [1-10] easiest axis (sample I), the square loop of the [1-10] direction could transform to a two-step loop under the negative piezo-voltages (compressed state). At the same time, the initial two-step loop of the [110] axis simultaneously changes to a square loop (the easiest axis). Otherwise, we designed and fabricated the sample II in which the PZT stress is parallel to the [110] two-step axis. The phenomenon of VCMA was also obtained along the [110] and [1-10] directions. However, the manipulated results of sample II were in contrast to those of the sample I under the piezo-voltages. Thus, an effective dual-axis regulation of the in-plane magnetization rotation was demonstrated in this work. Such a finding proposes a more optimized method for the magnetic logic gates and memories based on voltage-controlled magnetic anisotropy in the future.

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Pre-metal dielectric PE TEOS oxide pitting in 3D NAND: mechanism and solutions

December 2021

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120 Reads

In 3D NAND, as the stack number increases, the process cost becomes higher and higher, and the stress problem becomes more and more serious. Therefore, the low cost and low stress plasma enhanced tetraethyl orthosilicate (PE TEOS), compared to high density plasma (HDP) oxide, shows its superiority as pre-metal dielectric (PMD) oxide layer in 3D NAND. This paper explores the challenges in the application of PE TEOS in 3D NAND PMD oxide layer. In our experiment both PE TEOS and HDP are employed as the PMD oxide for 3D NAND staircase protection. There is not any void found in the two oxide structures. However, oxide pitting is spotted in the subsequent diluted hydrofluoric acid wet etching in the PE TEOS split. Moreover, we observe that the top silicon nitride corrodes in hot phosphoric acid. We study the mechanism of PE TEOS oxide pitting and silicon nitride corroding, propose two solutions: (1) HDP oxide + PE TEOS, and (2) PE TEOS + dry etching. Experimental results demonstrate that our solutions can well address the issue of PE TEOS oxide pitting and effectively protect the staircase structure. This work extends the application of PE TEOS oxide of which the cost and the stress are both low in 3D NAND.


FIG. 1. (a) Measurement configurations for the VCMA in the TiN/HZO/PtCoRu structure. HZO is the ferroelectric layer, and TiN is the bottom electrode of the FM/FE structure. The magnetic hysteresis loop of the PtCoRu magnetic layer with perpendicular magnetic anisotropy (PMA) is measured using the MOKE under different polarized voltages (U HZO ). (b) Cross-sectional TEM image of the Si/SiO 2 /TiN/HZO-stacked sample. The 10 nm HZO was etched away and stopped on the 100 nm-thick TiN of the bottom electrode. The inset is the schematic diagram of metal/ferroelectric/metal used for C-V and P-V measurements. The magnetic hysteresis loops with the magnetic field in the perpendicular direction with different (c) positive and (d) negative polarized voltages.
FIG. 2. The coercive field (H c ) and remnant magnetization (M r ) of the PtCoRu magnetic layer as a function of the polarized voltage (U HZO ) applied to the HZO ferroelectric layer.
FIG. 3. (a) The polarization-voltage (P-V) curves of 10 nm HZO with different sweep voltages range. (b) Capacitance-voltage (C-V) curves of 10 nm HZO with a 3 V sweep voltage. The inset is the amplitude variation (DS) of HZO vs U HZO amplitude in the TiN/HZO/TiN structure. (c) The HZO ferroelectric layer is positive polarized with 3 V voltage, and a stress is induced. The black arrows represent the strain states. The light green arrows represent the polarization of HZO. (d) Ferroelectric thin film returns to its original state with a stress release. Due to the remnant polarization (P r ) of HZO, the HZO cannot return to the original state with a residual stress.
FIG. 4. (a) The schematic diagrams for measurements of anomalous Hall effect and application of polarized voltages. The applied polarized voltage U HZO , the measured Hall voltage, and the channel current (red arrow) are indicated. (b) The anomalous Hall voltages are measured with out-of-plane magnetic field under different polarized voltages, 0, 2, 3, and 4 V. A 50 lA constant current is applied in the Hall bar device. The changes in the V H in the PtCoRu Hall bar device under 0, 61, and 63 V periodic polarized voltage (U HZO ) without the external magnetic field. The distinct high and low Hall voltages states are shown depending on the 63 V polarized voltage.
Ferroelectric control of the perpendicular magnetic anisotropy in PtCoRu/Hf 0.5 Zr 0.5 O 2 heterostructure

July 2021

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214 Reads

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9 Citations

The magneto-electric coupling (MEC) effect has been considered an effective method for the voltages controlled magnetic anisotropy in traditional ferroelectric/ferromagnetic structures. Unlike traditional perovskite ferroelectrics, the ferroelectric hafnium-based oxides hold great potential for use in the complementary metal oxide semiconductors (CMOS) circuit with the advantages of CMOS compatibility and easy scaled-down and lower leakage current. In this article, the MEC effects in the PtCoRu/Hf0.5Zr0.5O2 (HZO) heterostructure have been investigated using the polar magneto-optical Kerr effect microscopy and anomalous Hall effect. The major modification of perpendicular magnetic anisotropy of the PtCoRu thin film was controlled obviously within the ±4 V polarized voltages of the Hf0.5Zr0.5O2 (HZO) film, accompanying with the coercivity field and remnant magnetization significantly decreased. The Hall voltages of PtCoRu in Hall bar devices were also controlled effectively under ±3 V polarized voltages. Such a finding proposes a more optimized method for the magnetic logic gates and memories based on voltage-controlled magnetic anisotropy in future.


FIGURE 10. Layout of staircase, channel hole and contact holes
An Improved Dimensional Measurement Method of Staircase Patterns With Higher Precision in 3D NAND

July 2020

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992 Reads

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3 Citations

IEEE Access

3D NAND is a great architectural innovation in the field of flash memory. The staircase for control gate is a unique and important process in the manufacturing of 3D NAND. The staircase is employed to form the electrical connection between the control gate and contact. The current method used to measure the dimension of staircase patterns is, however, not precise enough for the development of state-of-the-art 3D NAND. In this circumstance, an accurate measurement of dimension for as-formed staircase patterns is of great importance and technical interest. In this paper, an improved measurement method is proposed to meet the requirement for higher precision. By taking the overlay into account, a calculation formula for measuring the dimensional error of as-formed staircase is derived for the first time. Two kinds of anchor design (convex SS0 and concave SS0) are put forward to perform dedicated experiments. Achieved results show that the measurement error of as-formed staircase using this improved method is improved from 31.6 nm for normal measurement method to 14.1 nm. The dimensional uniformity of as-formed staircase is therefore improved significantly which in turn leads to well controlled word line leakage. Furthermore, in advanced staircase structure of stair divided scheme (SDS), the convex SS0 shows an advantage in cost compared to the concave SS0.


FIGURE 1. Schematic diagrams of (a) conventional and (b) Xtacking 3D NAND structures where CMOS is not shown, and corresponding samples: (1) Sample A following conventional flow, (2) Sample B and C following Xtacking flow with only BEOL passivation, and (3) Sample D and E following Xtacking flow with only final passivation.
FIGURE 2. Comparison of cell SS (columns) and standard deviation s (dots) in samples with only BEOL passivation. Sample A was conventional as the control group. Sample B was only passivated in anneal ambience without an BEOL SiN as H source. Sample C was passivated with an BEOL SiN as H source.
FIGURE 3. Comparison of cell SS (columns) and standard deviation σ (dots) in different structures. Sample A is the conventional sample with BEOL passivation as the control group. Sample D and sample E are Xtacking samples with final passivation but with different metal via densities.
FIGURE 4. Schematic diagrams of H diffusion paths during final passivation in (a) conventional sample and (b) Xtacking samples. Path I represents for the H direct diffusion through the array Si substrate. Path II describes H diffusing along metal via and metal lines to channel holes.
FIGURE 5. By-tier cell SS difference as a function of passivation time. The lower and upper WLs corresponds to the cells close to the Si substrate and interconnections, respectively.
Hydrogen Source and Diffusion Path for Poly-Si Channel Passivation in Xtacking 3D NAND Flash Memory

January 2020

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1,372 Reads

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12 Citations

IEEE Journal of the Electron Devices Society

Poly-Si channels need well passivated by using hydrogen passivation process in 3D NAND flash memories for better poly-Si quality with low trap density. It is believed that Xtacking 3D NAND flash memory has the advantage of flexible arranging the passivation process. In this article, two different passivation locations were compared in Xtacking structure to achieve better trap passivation. An optimized passivation process conducted at wafer backside with passivation SiN as hydrogen diffusion source was found to have an improved trap passivation result. This benefit was attributed to the sufficient H diffusion paths in Xtacking. These results also indicated the advantage of trap passivation for future higher stacked Xtacking 3D NAND flash memory.


A High Density and Low Cost Staircase Scheme for 3D NAND Flash Memory: SDS(Stair Divided Scheme)

September 2019

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599 Reads

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12 Citations

We propose and implement Stair Divided Scheme (SDS), a novel high density and low cost staircase scheme for 3D NAND. In SDS, the stairs are divided into m zones in Y direction, and thus only N/m stairs are needed in X direction for N control gates. We further present the photoresist (PR) consume model. The PR consume model fits the result well. Based on the PR consume model, we are able to prove the process efficiency and low cost of SDS. We also show that SDS can improve the integration for higher bit density. Finally, we find that the critical dimension (CD) of stair divided zone shifts post stair etching. We investigate the reason and point out that, it is necessary to make compensation in layout to ensure the precise alignment of stairs.


An effective process to remove etch damage prior to selective epitaxial growth in 3D NAND flash memory

July 2019

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88 Reads

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4 Citations

An effective post etch treatment (PET) process was proposed to eliminate etch damage in the channel hole, of which the depth and the aspect ratio is beyond 3 μm and 30:1 respectively, prior to selective epitaxial growth (SEG) in three dimensions (3D) NAND flash memory. In this work, it is demonstrated that the damaged layer both at the channel hole bottom and sidewall induced by capacitively coupled plasma (CCP) was effectively eliminated using low energy plasma of CL2 + NF3/CH2F2 in PET, and then obtaining an excellent surface condition in channel hole and fabricating a void-free SEG epitaxial layer.




Investigation of Threshold Voltage Distribution Temperature Dependence in 3D NAND Flash

December 2018

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227 Reads

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22 Citations

IEEE Electron Device Letters

The impact of temperature on array Vth distribution was investigated in 3D NAND flash. Cell Vth distributions were obtained under different program and read temperature splits. After the page is programmed under high temperature, it is found that the high tail of Vth distribution exhibits a larger shift than the low tail, during read at different temperatures (85°C and –25°C). On the contrary, the low tail of Vth distribution shows a larger shift than the high tail during cross temperature read, after the page programmed under low temperature. The temperature coefficient (Tco) of cell Vth shows cell to cell variations, which can be categorized into two types. For type 1, the Tco is correlated with the selected cell Vth due to polysilicon channel; For type 2, the Tco is independent of the selected cell Vth. The corresponding impacts on Vth distribution are studied via array Monte Carlo simulation. Based on the simulation results, the above temperature dependent observations can be well modeled by the combination of both Tco variation type 1 and 2. Furthermore, two optimization approaches are proposed to alleviate the Vth distribution broadening and are validated by experiments.


Citations (8)


... The spin dynamics and spin transport parameters obtained from the ST-FMR platform further demonstrate the stability and accuracy of the system. It is worth noting that by replacing the semiconductor heating element with other stimuli, such as a top gate made from high-k materials, 40 a bottom polarized electric field from ferroelectric materials, 5,33,41 or stress-strain excitation using piezoelectric ceramics, 42 the system can achieve either volatile or non-volatile in situ control. ...

Reference:

A radio frequency/direct current hybrid rotatable spin torque ferromagnetic resonance platform
Ferroelectric control of the perpendicular magnetic anisotropy in PtCoRu/Hf 0.5 Zr 0.5 O 2 heterostructure

... Therefore, the peripheral-under-cell (PUC) structure has been adopted for the NAND device, which can effectively reduce the total area by stacking the periphery and NAND cell, compared to the conventional structure where the periphery is located around the NAND cell [4]- [6]. However, the PUC structure is created by manufacturing NAND cell on the periphery sequentially, which affects the performance and reliability of the peripheral transistor [7], [8]. In particular, the cell alloy process is an essential thermal process for passivation and metal stabilization when manufacturing NAND cells, but it significantly influences peripheral transistors [8]- [10]. ...

Hydrogen Source and Diffusion Path for Poly-Si Channel Passivation in Xtacking 3D NAND Flash Memory

IEEE Journal of the Electron Devices Society

... Fortunately, several types of the two-directional-staircase-forming method have been developed, where staircases are made not only in the direction along a WLy but also in the direction perpendicular to the WL. [97,98] By using this method, both the lithography cost and WLy contact area could be remarkably reduced. ...

An Improved Dimensional Measurement Method of Staircase Patterns With Higher Precision in 3D NAND

IEEE Access

... In order to solve this problem, methods of etching multiple ON layers at once by increasing the dimensions of the staircase, through the formation of maskless ONON stack feature in advance, have been studied (see supplementary information Figure S1). [1,7] These methods have more complex shapes than the existing process, so the maskless ONON stack feature etch pro le through the passivation of the sidewall has become important, and, for this, uorocarbon rich gases such as C 4 F 8 and C 4 F 6 -based gases have been actively studied. [8][9][10][11][12] In addition, many studies have been conducted on the selectivity etching of O/N or N/O for pro le improvement and accurate etch stop. ...

A High Density and Low Cost Staircase Scheme for 3D NAND Flash Memory: SDS(Stair Divided Scheme)

... S ince memory devices based on MOSFET have been scaled down to its physical limitations, most of them have needed to expand their array architecture in 3-dimensional structure to increase their array density. [1][2][3][4][5][6][7][8][9] Resistive-switching random access memory (ReRAM) is a potential candidate as next-generation memory device using memristor materials owing to its simple 2-terminal structure, fast switching speed, and low-power consumption. [10][11][12][13][14][15][16][17] Especially, InGaZnO (IGZO) has been studied as a memristor device with analog and digital switching properties in virtue of CMOS fabrication compatibility and the co-integration with IGZO TFTs on flexible substrates for wearable electronics and reconfigurable logic systems. ...

An effective process to remove etch damage prior to selective epitaxial growth in 3D NAND flash memory

... In order to simplify the simulation, we just chose the 64 WL layer; Table 1 shows the detailed device structure parameters of the simulation. For simplification, the three TSG/BSG layers and two top/bottom dummy (DMY) layers are not depicted in detail in Figure 1, and the simulation setting is almost the same as in our previous work [10,11]. The electric potential and electron density along the channel of the conventional scheme and novel scheme were simulated using the Synopsys Sentaurus Sdevice simulator. ...

Cycling Induced Trap Generation and Recovery Near the Top Select Gate Transistor in 3D NAND
  • Citing Conference Paper
  • March 2019

... Temperature (T ) dependence of NAND string parameters has been investigated in several works [10], [32], [33], where the role of GBs has been discussed in a CT frame. Fig. 8 reports the T dependence of the average and rms V T , showing that the reduction in such quantities after a DT approach is more evident at low T , reaching about 20% for T = 198 K. ...

Investigation of Threshold Voltage Distribution Temperature Dependence in 3D NAND Flash
  • Citing Article
  • December 2018

IEEE Electron Device Letters

... The models used in TCAD device simulation were as follows: the Shockly-Read-Hall (SRH) model, the non-local tunneling (NLT) model, the Poole-Frenkel model, the thermal emission model, and the drift-diffusion model. These models can effectively reflect physical characteristics and have proven to be useful in explaining many phenomena of 3D NAND flash [11,12], and the specific simulation parameters used can be referenced in article [13], which is a previous research study by the research group. ...

The Influence of Grain Boundary Interface Traps on Electrical Characteristics of Top Select Gate Transistor in 3D NAND Flash Memory
  • Citing Article
  • December 2018

Solid-State Electronics