Jingwen Xu’s research while affiliated with Wuhan University of Technology and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (9)


Stochastic weighted particle control for electrostatic particle-in-cell Monte Carlo collision simulations in an axisymmetric coordinate system
  • Article

October 2024

·

23 Reads

Computer Physics Communications

·

Zhaoyu Chen

·

Yu Wang

·

[...]

·


Circuit diagram (containing the matching box and cables) used in this simulation. Vrf and Rrf represent the driving voltage provided by the rf power supply and its internal resistance, respectively. An L-type matching box is located between two cable sections. Cst, Lst and Rst are used to characterize the stray effects of the discharge chamber. The CCP itself is described by a PIC/MCC simulation and its impedance, ZCCP. P1-P5 represent five different positions in the circuit used for the analysis of the results.
Evolution of the electron density in the center of the plasma bulk (a), the effective/active power dissipated in the CCP (b) and the reflection coefficient at point P2 (c) as a function of time. Method (i) and Method (ii) refer to the two different methods of calculating the impedance at point P3 as pointed out in this section. The values of Cm1 and Cm2 are updated every 3000 RF cycles (about 221 µs). Conditions: 200 mTorr, two cables, cable I: 2 m, cable II: 1 m.
Temporal and spatial evolution of the electron density (a), average electron energy (b) and plasma potential (c). The values of Cm1 and Cm2 are updated every 3000 RF cycles (about 221 µs). Conditions: 200 mTorr, two cables, cable I: 2 m, cable II: 1 m.
Time evolution of the voltage (a) and current (b) amplitudes of the CCP and their corresponding Fourier spectrums (c) and (d) at 221 µs (solid black line) and 1326 µs (dashed red line). The values of Cm1 and Cm2 are updated every 3000 RF cycles (about 221 µs). Conditions: 200 mTorr, two cables, cable I: 2 m, cable II: 1 m.
Changes in Cm1 and Cm2 (a), ZP1 (b), ZP2 (c), ZP3 (d), ZP4 (e) and ZP5 (f) during the matching process. Conditions: 200 mTorr, two cables, cable I: 2 m, cable II: 1 m.

+8

Impedance matching design for capacitively coupled plasmas considering coaxial cables
  • Article
  • Publisher preview available

August 2024

·

80 Reads

Capacitively coupled plasmas (CCPs) are widely used in plasma processing applications, where efficient power coupling between the radio frequency (RF) source and the plasma is crucial. In practical CCP systems, impedance matching networks (IMNs) are employed to minimize power reflection. However, the presence of coaxial cables can significantly impact plasma impedance and matching performance. We develop a comprehensive simulation framework for the IMN design of CCPs, fully considering the effects of RF coaxial cables. The model self-consistently couples a distributed transmission line (TL) model, a lumped-element circuit model, and an electrostatic particle-in-cell model. This coupled model is used to investigate the impact of coaxial cables on matching performance under various discharge conditions and cable configurations. The simulation results indicate that the optimal power transmission efficiency was achieved after 6 matching iterations. The power coupled to the CCP increased from 2.7 W before matching to 180.9 W, and the reflection coefficient ultimately decreased to 0.003. The results also reveal that neglecting the cables will lead to a decrease in the power dissipated in the CCP. The proposed method demonstrates effectiveness in achieving impedance matching for different gas pressures (75–300 mTorr) and cable lengths. It can be concluded that the matching speed is faster for an appropriate cable length. This work provides valuable insights into the role of TLs in CCP impedance matching and offers a practical tool for optimizing power delivery in realistic CCP systems with RF coaxial cables.

View access options

Numerical characterization of capacitively coupled CF4 plasmas modulated by anion beam injection

In the study of electronegative CF4 capacitively coupled plasmas (CCP), plasma modulation is typically achieved by varying parameters such as pressure and voltage. In this work, the particle-in-cell/Monte Carlo (PIC/MC) method is used to simulate modulation of CF4 CCP with injection of anions (F⁻) ion beam (FB). The results demonstrate that FB injection effectively enhances the dissociation collision process between F⁻ ions and neutral molecules, thus altering the densities of electrons and ions. An effective modulation of the characteristic parameters of the plasma of CF4 can be achieved by controlling the current and energy of FB. Particularly noteworthy is the transition of the heating mode from the DA mode to the dissociation mode as the FB current increases to 0.038 A (energy fixed at 10 keV) or when the FB energy exceeds 10 keV (current fixed on 0.038 A). This transition is attributed to the generation of a substantial number of electrons through dissociative collisions. This approach provides insight into the controlled modulation of plasma characteristics in CF4 CCP, offering potential applications in various plasma-based technologies.



Numerical Impedance Matching via Extremum Seeking Control of Single-Frequency Capacitively Coupled Plasmas

January 2024

·

157 Reads

·

5 Citations

Impedance matching is a critical component of semiconductor plasma processing for minimizing the reflected power and maximizing the plasma absorption power. In this work, a more realistic plasma model is proposed that couples lumped element circuit, transmission line, and particle-in-cell (PIC) models, along with a modified gradient descent algorithm (GD), to study the impact of presets on the automatic matching process. The effectiveness of the proposed conceptual method is validated by using a single-frequency capacitively coupled plasma as an example. The optimization process with the electrode voltage and the reflection coefficient as the objective function and the optimized state, including plasma parameters, circuit waveforms, and voltage and current on transmission lines, is provided. These results show that the presets, such as initial conditions and objective functions, are closely related to the automatic matching process, resulting in different convergence speeds and optimization results, proving the existence of saddle points in the matching network parameter space. These findings provide valuable information for future experimental and numerical studies in this field.


Influence of external circuitry on CF4 breakdown process in capacitively coupled plasma

September 2023

·

64 Reads

·

1 Citation

Journal of Vacuum Science and Technology B: Nanotechnology and Microelectronics

Capacitively coupled plasma (CCP) tools are crucial for etching, deposition, and cleaning processes in the semiconductor industry. A comprehensive understanding of their discharge characteristics is vital for the advancement of chip processing technology. In this study, the influence of external circuitry on the breakdown process was investigated under the CF4 discharge system, with a particular focus on challenges presented by the nonlinear nature of the plasma. The results demonstrated that the external circuit significantly affects the discharge process by altering the electric field distribution as well as modifying the electron density and temperature of the plasma. By incorporating the matching circuit, stable discharge was achieved at reduced voltage levels. During breakdown, a substantial increase in the capacitance of the discharge chamber is induced by the formation of the sheath, which alters the amplitude of the electrical signal within the external circuit. The breakdown characteristics are significantly influenced by the capacitance of the matching network. Breakdowns with distinctive characteristics can be achieved by selectively choosing different capacitors. Furthermore, a shift in the CF4 discharge mode at different pressures under the external circuit model and the alteration in the discharge mode affect the electrical properties of the plasma in the matched circuit. These findings could be used to optimize the discharge of CCP and its applications, including surface treatment, material synthesis, and environmental remediation.


Numerical characterization of dual radio frequency micro-discharges

March 2023

·

106 Reads

·

1 Citation

Micro-discharges have many excellent characteristics, such as generation of high-density and non-equilibrium plasmas at atmospheric pressure. In this paper, we used an implicit particle-in-cell/Monte Carlo collision method for three-dimensional velocities in a one-dimensional space combined with the secondary electron emission model to study the characteristics of micro-discharges driven by dual radio frequency (RF) power. The effect on plasma parameters was observed by varying the voltage of the RF power, the frequency, and the gas pressure of the discharge. Since the electrode spacing is very small in micro-discharges, the voltage change will affect the characteristics of micro-discharges. In addition, the plasma density increases with the frequency and the discharge mode changes at different frequencies. Finally, the influence of gas pressure on the characteristics of micro-discharges cannot be ignored. When the air pressure decreases, the ion flux reaching the electrodes is significantly increased, and the energy distribution of ions increases in the high-energy portion.


Numerical simulations of the effects of radiofrequency cables on the single-frequency capacitively coupled plasma

November 2022

·

29 Reads

·

5 Citations

Radiofrequency (RF) coaxial cables are one of the vital components for the power sources of capacitively coupled plasmas (CCPs), by which the RF power is transferred to excite the plasma. Usually, the cables can be treated as transmission lines (TLs). However, few studies of TLs in CCP power sources were conducted due to the nonlinear coupling between TLs and the plasma. In this work, we developed a numerical scheme of TLs based on the Lax–Wendroff method and realized the nonlinear bidirectional coupling among the lumped-element model, transmission line model, and electrostatic particle-in-cell model. Based on the combined model, three discharge patterns were found, including weak matching state, normal state, and over matching state. The great differences among the three patterns indicated that the TLs could change the impedance matching of the device and significantly affect the plasma properties.


A Generalized External Circuit Model for Electrostatic Particle-In-Cell Simulations

August 2022

·

127 Reads

·

15 Citations

Computer Physics Communications

A fully self-consistent second order accuracy model for coupling a generalized external circuit and a one-dimensional bounded electrode-driven plasma was proposed in this paper. The plasma was embedded in the circuit as a non-linear element with a potential difference. Based on Kirchhoff's voltage law and the definition of current, the problem of solving the generalized external circuit was transformed into an initial value problem of a set of first-order ordinary differential equations which can be discretized numerically by the second-order backward differential formula. The charge conservation equation at the electrode plate was coupled to the above equation, and the voltage, current, and surface charge density at the next moment were solved by a differential equation solver. Dirichlet boundary conditions of Poisson's equation were obtained through the surface charge density σ0 of the generalized external circuit equation and the plasma density ρ of the Particle-in-Cell(PIC) model. The spatial distribution of plasma potential was solved by using the second-order central difference scheme. The obtained potential at the electrode plate can be used as the Robin boundary condition of the system of generalized external circuit equations. In this model, the loose coupling between the generalized external circuit and plasma was realized by the boundary condition, and the system was fully self-consistent based on the charge conservation law and energy conservation law. We simulated the capacitively coupled plasmas (CCP) under different external circuits as the example and verified the performance of the model. This model can be used to study the influence of different external circuit structures and parameters on plasma discharge, and can be used for any plasma sources driven by electrodes, like CCP, some vacuum electronic devices, and Z-Pinches.

Citations (5)


... A distributed circuit model, also known as TLM, can be solved numerically using the Lax-Wendroff two-step Method (LWM) with second order accuracy [19,29]. This LWM has the advantages of high stability and low computational costs. ...

Reference:

Impedance matching design for capacitively coupled plasmas considering coaxial cables
A Numerical Approach for Nonlinear Transmission Line Analysis with Bidirectional Coupling to Lumped-element and Particle-In-Cell Models
  • Citing Article
  • April 2024

Journal of Computational Physics

... The particle-in-cell/Monte Carlo collisions (PIC/MCC) method is an indispensable tool for investigating the physics in plasmas, especially in the conditions when kinetic effects prevail [1]. After 70 years of development, the PIC/MCC approach has been used in various discharge phenomena and plasma sources [2], e.g. the capacitively coupled plasma (CCP) sources [3][4][5][6][7], the inductively coupled plasma (ICP) sources [8][9][10], the magnetrons [11][12][13][14], the ion grid systems [15][16][17], plasma probes [18] and the electric thrusters [19][20][21][22][23][24]. Unlike the fluid approaches including nonlocal closure of the equations as an input, the PIC/MCC method is based on the first principle [25,26]. ...

Numerical Impedance Matching via Extremum Seeking Control of Single-Frequency Capacitively Coupled Plasmas

... The pressure and voltage in this work are relatively low, and the discharge of CCPs only exhibits significant secondary electron emission effects (SEEE) under high pressure and/or high RF voltage amplitude [12,[48][49][50][51][52], so the influence of SEEE is relatively small here. The secondary electron emission was not considered here, but it can easily be included in the model based on our previous work [53,54]. ...

Influence of external circuitry on CF4 breakdown process in capacitively coupled plasma
  • Citing Article
  • September 2023

Journal of Vacuum Science and Technology B: Nanotechnology and Microelectronics

... In this case, the voltage and current on the cable will not only change with time, but also with the spatial position along the cable, so that the coaxial cables need to be considered as transmission lines (TLs). Both experiments [16,17] and simulations [18,19] show that the cable has a significant impact on the voltage and current in the reactor, which will directly affect the design of the impedance matching. In many practical CCP systems, the IMN and RF power source are connected to the plasma reactor via RF coaxial cables. ...

Numerical simulations of the effects of radiofrequency cables on the single-frequency capacitively coupled plasma
  • Citing Article
  • November 2022

... In this work, a self-consistent coupling of a 1D3v direct implicit PIC/MCC code with an external circuit is used, which has been used successfully in the study of rf breakdown [29]. The external circuit coupling method comes from [47], which has been tested and improved successfully by our code [48,49]. The implicit PIC code allows for a larger time and space scale than the explicit one [50][51][52], which can finish the simulation more quickly. ...

A Generalized External Circuit Model for Electrostatic Particle-In-Cell Simulations
  • Citing Article
  • August 2022

Computer Physics Communications