Abstract:The time dependence of the ion composition in pulse-modulated dual-frequency capacitively coupled plasma with Ar/C4F8/O2 was measured using a quadrupole mass spectrometer with an electrostatic energy analyzer. After turning on the pulse, Ar+ ions were preferentially generated, and then, the composition of CxFy
+ ions, such as C2F4
+ and C3F5
+ ions, increased. This phenomenon was discussed on the basis of the time variation of electron temperature and the r… Show more
“…Signal time delay due to ion transit time through the QMS was considered. Our previous study 12) has confirmed the proportional relationship between the square root of ion mass number and the ion transit time, from light ions (CF + ) to heavy ions (C 3 F 5 + ). Hereafter, the delay time when the pulse is turned on is determined as T .…”
Section: Experimental Methodssupporting
confidence: 54%
“…In our previous work, 12) the ion species produced from a pulsed Ar/C 4 F 8 /O 2 plasma were Ar , and C 3 F 5 + were the dominant ions in this study. This is consistent with the calculated ionization rates based on ionization cross sections, 13) and hereafter, we focus on these five ion species.…”
Section: Experimental Methodsmentioning
confidence: 57%
“…The experimental setup used in this study was reported in our previous work 12) and is briefly described here. In this study, a RF electrode (diameter: 10 cm) and an opposing ground electrode (electrode spacing: 3 cm) were installed in a cylindrical vacuum chamber (diameter: 16 cm; height: 18 cm) which was evacuated by a turbomolecular pump at a base pressure less than 10 −4 Pa.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…However, the pulse operation of the plasma induces time-dependent behavior of positive ions, and this behavior might influence the etching performance. In our previous work, 12) the temporal variation of positive-ion (hereinafter simply referred to as "ions") composition was found in a pulse-operated Ar/C 4 F 8 /O 2 DF-CCP which is used to fabricate HAR features in silicon dielectric films. This phenomenon was studied based on the temporal variation of the ion production rates, which depend on gas flow ratio and timevarying electron temperature (T e ).…”
The time-varying mechanism of the positive-ion composition in a pulse-modulated Ar/C4F8/O2 dual-frequency capacitively coupled plasma was investigated in detail using a quadrupole mass spectrometer equipped with an electrostatic energy analyzer. Time-resolved measurements of the ion composition with respect to the pulse-off period (
T
off
) revealed that the electron temperature (
T
e
) just after turning on the pulse is an important factor in determining the ratio of the ionization rates of the Ar+ and C
x
F
y
+ ions. The time-varying phenomenon of the ion composition was also investigated through a numerical analysis based on the particle balance model, considering the production and loss rates of ions, ion–ion recombination processes, and ion–molecule reactions. When the VHF power (
P
VHF
) was increased, a decrease in the ambipolar diffusion loss time constants of the ions (
τ
loss
i
) was observed, and the change in electronegativity was pointed out as the cause of this phenomenon.
“…Signal time delay due to ion transit time through the QMS was considered. Our previous study 12) has confirmed the proportional relationship between the square root of ion mass number and the ion transit time, from light ions (CF + ) to heavy ions (C 3 F 5 + ). Hereafter, the delay time when the pulse is turned on is determined as T .…”
Section: Experimental Methodssupporting
confidence: 54%
“…In our previous work, 12) the ion species produced from a pulsed Ar/C 4 F 8 /O 2 plasma were Ar , and C 3 F 5 + were the dominant ions in this study. This is consistent with the calculated ionization rates based on ionization cross sections, 13) and hereafter, we focus on these five ion species.…”
Section: Experimental Methodsmentioning
confidence: 57%
“…The experimental setup used in this study was reported in our previous work 12) and is briefly described here. In this study, a RF electrode (diameter: 10 cm) and an opposing ground electrode (electrode spacing: 3 cm) were installed in a cylindrical vacuum chamber (diameter: 16 cm; height: 18 cm) which was evacuated by a turbomolecular pump at a base pressure less than 10 −4 Pa.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…However, the pulse operation of the plasma induces time-dependent behavior of positive ions, and this behavior might influence the etching performance. In our previous work, 12) the temporal variation of positive-ion (hereinafter simply referred to as "ions") composition was found in a pulse-operated Ar/C 4 F 8 /O 2 DF-CCP which is used to fabricate HAR features in silicon dielectric films. This phenomenon was studied based on the temporal variation of the ion production rates, which depend on gas flow ratio and timevarying electron temperature (T e ).…”
The time-varying mechanism of the positive-ion composition in a pulse-modulated Ar/C4F8/O2 dual-frequency capacitively coupled plasma was investigated in detail using a quadrupole mass spectrometer equipped with an electrostatic energy analyzer. Time-resolved measurements of the ion composition with respect to the pulse-off period (
T
off
) revealed that the electron temperature (
T
e
) just after turning on the pulse is an important factor in determining the ratio of the ionization rates of the Ar+ and C
x
F
y
+ ions. The time-varying phenomenon of the ion composition was also investigated through a numerical analysis based on the particle balance model, considering the production and loss rates of ions, ion–ion recombination processes, and ion–molecule reactions. When the VHF power (
P
VHF
) was increased, a decrease in the ambipolar diffusion loss time constants of the ions (
τ
loss
i
) was observed, and the change in electronegativity was pointed out as the cause of this phenomenon.
“…Furthermore, plasma light intensity is linearly proportional to ion density. [25][26][27] Since the ion density at the SWP near the quartz disk is higher than that of the bulk region by more than 10 times, the light intensity would surpass that from the bulk by at least 10 times, leading to the SWP being the dominant light source for the image. In this sense, it is reasonable to think the measurement results reflect the inhomogeneous distribution of the SWP.…”
Microwave surface-wave plasma (SWP) provides relatively higher ion density and radical species density than RF plasma, making it a promising plasma source for semiconductor fabrication. However, its plasma uniformity is compromised due to the non-uniform field distribution as the microwave wavelength is typically shorter than chamber dimensions. This could be a bottleneck as to the practical application of SWP in semiconductor fabrication demanding a large-area plasma with a high uniformity. In this work, we propose field agitation by applying the phase difference of 0° and 180° between two input microwaves in the chamber to enhance the plasma uniformity. The chamber, optimized for the TM_130 mode at 2.458 GHz, successfully produces a large-area SWP with a diameter of 450 mm with 800 W absorption power and 200 mTorr argon pressure. The measurement results show that the system is capable of yielding enhanced uniformity of large-area SWP while maintaining high ion density.
Capacitively coupled plasma (CCP) discharges working at low pressure are widely used for the synthesis of thin films and the modification of the surface properties of materials. Due to their importance, considerable research was carried out over the years to understand their working mechanisms, and the physical properties of the CCP discharges were measured by many research groups, while simulations of their characteristics were often performed using both fluid and kinematic models. However, most of the simulation and characterization work found in the literature is focused on the discharge steady-state characteristics, since most of the applications rely on its properties, while less information is available on the early stages. In fact, the initial stages of CCP plasma discharges are of great importance to improve the understanding of their ignition process as well as to figure out the working mechanism of pulsed discharges, the use of which has increased in importance in recent years. In this work, a review of the results published in recent years concerning the physical mechanisms involved in the very first stages of low-pressure CCP discharges is presented, focusing on the first few microseconds of discharge time.
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