Abstract:Characteristics of the surface-wave plasma generated by a radial-line slot antenna (RLSA) have been studied by both direct plasma probe measurements and numerical simulations. Some unique characteristics have been found, including excellent critical radial plasma uniformity, low electron temperature under various pressure conditions, the main plasma generation area of RLSA being limited in the plasma surface, and few high-energy electrons existing in the wafer region. Numerical simulations are implemented to r… Show more
“…Thus, many researchers design the positions and number of slot antennas in order to ensure exciting the proper SW modes and further obtaining large-area even stable plasmas. 6,7,10,13 At the gas pressure of about 100 Pa, as shown in the present experiments, the wave energy absorbed by plasmas should be considered again. When the plasma density is in higher span ͑Ն10 18 m −3 ͒, the wavelength of SW will become almost constant, as shown in Fig.…”
Section: Discussionmentioning
confidence: 96%
“…Therefore, a possible way to control the discharge effectively is to utilize the plasmadielectric resonator, i.e., to apply the periodic slot antennas as the microwave energy excitation. [7][8][9][10][11][12][13][14] However, the SWP sources designed with the special wave-mode conversion device are not clearly described at the discharge pressure of about 100 Pa. Furthermore, the effect of wave-mode conversion device on the production of large-area uniform stable overdense plasmas has not been proposed.…”
Section: Introductionmentioning
confidence: 94%
“…Therefore, the development and application researches of the large-scale overdense SWP have attracted the unprecedented attention and the current study focus on the spatial uniformity and the temporal stability in large area. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] To address the above concerns, a lot of planar-type SWP sources have been optimized. As for these sources, the uniformity of plasma below the dielectric slab is one of the most important factors.…”
In this paper, the wave-mode conversion devices with three different structures have been devised for plasma heating. Surface-wave plasma ͑SWP͒ discharge analysis with or without considering the collision loss is presented theoretically. The comparative discharge experiments have been operated for obtaining the uniform stable microwave discharges. When a specially designed microwave appliance is selected as the proposed wave-mode conversion device, the discharges driven by resonant excitation with surface wave ͑SW͒ have yielded plasmas with density of about 10 18 m −3 at the gas pressure larger than 10 Pa. By comparing the results, the production of large-area uniform stable overdense SWP is attributed to the resonant excitation with SW evenly on the whole dielectric-plasma interface by the application of the specially designed wave-mode conversion device.
“…Thus, many researchers design the positions and number of slot antennas in order to ensure exciting the proper SW modes and further obtaining large-area even stable plasmas. 6,7,10,13 At the gas pressure of about 100 Pa, as shown in the present experiments, the wave energy absorbed by plasmas should be considered again. When the plasma density is in higher span ͑Ն10 18 m −3 ͒, the wavelength of SW will become almost constant, as shown in Fig.…”
Section: Discussionmentioning
confidence: 96%
“…Therefore, a possible way to control the discharge effectively is to utilize the plasmadielectric resonator, i.e., to apply the periodic slot antennas as the microwave energy excitation. [7][8][9][10][11][12][13][14] However, the SWP sources designed with the special wave-mode conversion device are not clearly described at the discharge pressure of about 100 Pa. Furthermore, the effect of wave-mode conversion device on the production of large-area uniform stable overdense plasmas has not been proposed.…”
Section: Introductionmentioning
confidence: 94%
“…Therefore, the development and application researches of the large-scale overdense SWP have attracted the unprecedented attention and the current study focus on the spatial uniformity and the temporal stability in large area. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] To address the above concerns, a lot of planar-type SWP sources have been optimized. As for these sources, the uniformity of plasma below the dielectric slab is one of the most important factors.…”
In this paper, the wave-mode conversion devices with three different structures have been devised for plasma heating. Surface-wave plasma ͑SWP͒ discharge analysis with or without considering the collision loss is presented theoretically. The comparative discharge experiments have been operated for obtaining the uniform stable microwave discharges. When a specially designed microwave appliance is selected as the proposed wave-mode conversion device, the discharges driven by resonant excitation with surface wave ͑SW͒ have yielded plasmas with density of about 10 18 m −3 at the gas pressure larger than 10 Pa. By comparing the results, the production of large-area uniform stable overdense SWP is attributed to the resonant excitation with SW evenly on the whole dielectric-plasma interface by the application of the specially designed wave-mode conversion device.
“…Therefore, SWP have been exhaustively investigated both theoretically and experimentally [1][2][3][4][5][6]. For example, M. Nagatsu et al [2] have yielded large-area surface-wave plasmas with an internally mounted planar cylindrical launcher, Y. Yasaka et al [7][8][9] have produced large-diameter uniformity plasma using multislotted planar antenna, and C. Tian et al [10] have studied characteristics of large-diameter plasma using a radial-line slot antenna. But most of the structure of chamber reported in the literature is circular cylinder; a rectangular cavity [11][12][13] is adopted in this article.…”
The theory of surface-wave discharge is introduced. A novel structure of the slot antenna array is designed in this paper, and its excitation is numerical analyzed using dipole-antenna array model and FDTD method, respectively. A microwave discharge experiment is operated with this slot-antenna array, and a numerical simulation is also done with FDTD code using the parameter of plasma from experimental measurement. It is found that the designed slot antenna array can excite effectively the microwave coupling into the cavity, and produce the stable large-area high-density plasma.
“…4,[11][12][13] The SPA process provides high density plasma (∼10 12 cm −3 ) at low electron temperature (0.7∼1.5 eV) with a wide process window (7∼1000 Pa) to enable a low damage plasma process compared to conventional inductively coupled plasma (ICP) or electron cyclotron resonance (ECR) plasma. 14 Recently, the use of slot-plane-antenna plasma oxidation (SPAO) has been studied for TiN/ZrO 2 /Al 2 O 3 /Ge MOS capacitors, where SPAO has been introduced in different stages (before Al 2 O 3 deposition, in between Al 2 O 3 and ZrO 2 deposition, and after the deposition of both Al 2 O 3 and ZrO 2 ) during the gate stack formation. 15 When SPAO was introduced after the deposition of both Al 2 O 3 and ZrO 2 , enhanced EOT downscaling with lower interface state den-sity, D it , behavior for the devices are reported.…”
This work investigates the dielectric quality and interface properties of TiN/Hf 1-x Zr x O 2 /Al 2 O 3 /Ge gate stacks with six different Zr content (0%, 25%, 33%, 50%, 75%, and 100%). The dielectrics were subjected to Slot-Plane Antenna Plasma Oxidation (SPAO) after the ALD deposition process prior to metal deposition. The equivalent oxide thickness (EOT), flat-band voltage (V FB ), interface state density (D it ), C-V hysteresis, and leakage current (I-V) behavior were analyzed. It was observed that EOT decreases with Zr addition in HfO 2 with up to 75% of Zr incorporation. While the devices with up to 75% of Zr demonstrated lower C-V hysteresis, flat-band voltage shift and mid-gap D it tend to increase with decrease in EOT. With 100% Zr incorporation EOT increased significantly while reducing the mid-gap D it . This behavior is mostly dependent on GeO x -like interfacial layer formation and defects at the interface. Weibull plots shows that charge to breakdown (Q BD ) increased with increase in the Zr percentage. However, the breakdown acceleration factor decreased with Zr percentage up to 75% and increased for 100% Zr content.
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