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Physics of High-Density Radio Frequency Capacitively Coupled Plasma with Various Electrodes and Its Applications

Written By

Yasunori Ohtsu

Submitted: 30 November 2017 Reviewed: 08 May 2018 Published: 05 November 2018

DOI: 10.5772/intechopen.78387

From the Edited Volume

Plasma Science and Technology - Basic Fundamentals and Modern Applications

Edited by Haikel Jelassi and Djamel Benredjem

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The radio frequency discharge plasma sources are widely utilized to prepare functional thin films and to etch insulated layers in semiconductor devices in microelectronic industry. Especially, a capacitively coupled plasma (CCP) is the most popular discharge because the equipment is very simple and almost maintenance free. However, there is a problem such as low-density plasma under low-gas pressure less than 10 Pa, that is, low processing rate. In this chapter, the production principle of conventional CCP and the special CCP with various electrodes and magnets is reviewed. The applications prepared by the special CCP system are also presented. Finally, the future plan including problems is described.


  • RF plasma
  • capacitively coupled plasma
  • plasma processing
  • hollow cathode discharge
  • ring-shaped hollow plasma
  • magnetized plasma

1. Introduction

A large-scale integrated circuit (LSI), various sensors, and other semiconductor devices are essential for various electrical and electronic devices and automobile [1, 2]. In general, these devices are fabricated by plasma-processing techniques such as dry etching and plasma deposition using low-pressure plasma. The plasma processing is the most usually utilized chemical and physical processes in microelectronics fabrication for functional thin film preparation and dry etching of silicon-based films.

In the dry-etching processing, the silicon wafer patterned by the photoresist mask for LSI is exposed in plasma containing halogen molecules (e.g., CF4, CHF3, SF6) [3, 4, 5, 6, 7]. In the case of these gases, the fluorine atoms dissociated by an electron impact collision with the molecules react with the silicon surface to generate a volatile etch product like SiF4 so that the silicon wafer is etched with assistance of energetic ions produced in the plasma. For example, a high-density plasma sources have been developed to challenge patterning features less than 0.25 μm with high aspect ratios [8].

The plasma deposition has a sputtering deposition and a plasma-enhanced chemical vapor deposition (PECVD) method. The sputtering deposition is to impinge ions to the material target biased by a negative potential so as to sputter atoms from the target. The functional thin films such as transparent conductive oxide used in tableted computer and smartphone are deposited by sputtering method [9]. The sputtering depositions are prepared by DC magnetron and radio frequency (RF) magnetron plasma sources [10]. Various typed sputtering sources have been developed for the synthesis of high-quality thin films [10]. Especially, RF magnetron plasma source has an advantage that the insulated films can be deposited on the various substrates compared with DC magnetron plasma source. The PECVD is to dissociate molecule by electron impact so as to deposit radicals [8].

In these plasma-processing techniques, capacitively coupled plasma (CCP) with parallel plates was widely utilized. The physics of CCP has been studied by many researchers [11, 12, 13, 14, 15, 16]. The sustaining mechanism of CCP is the electron heating process that the oscillating radio frequency sheath near the powered electrode plays an important role in electron acceleration as well as the collisional heating in the presence of electric fields and the emission process of secondary electrons from the electrode [11, 12, 13, 14, 15, 16]. However, the electron heating process cannot produce high-density plasma.

The requirement of these semiconductor devices with high-speed operation and high performance is increasing annually. In order to perform the demand, high-speed plasma processing, that is, a high-density plasma production, is important. However, CCP does not attain high-density plasma. Thus, the high-density CCP is required. In this chapter, the production principle of conventional CCP and the special CCP with various electrodes and magnets is reviewed.


2. Production principle of conventional capacitively coupled plasma

In order to perform the high-speed processing of the LSI semiconductor, high-density plasma is needed for CCP. The power balance of CCP in the form of a global model [17] is expressed as the following equation:


Here, Pab, e, uB, and S are the total absorbed power, the electronic charge, the Bohm velocity, and the surface area, respectively. εe and εi are the averaged energy loss per electron and ion lost to the electrodes. εc denotes the collisional energy loss per electron-ion pair created. The plasma density, ne, can be determined from Eq. (1)


When only thermal electrons are lost to the boundary surfaces [18], εe will be negligible. In general, the electron temperature decreases with increasing gas pressure [17]. Then, εc increases, while εi regularly decreases with increasing gas pressure, because the sheath is more collisional. For a fixed absorbed power, the increase in the plasma density is resulted with increasing gas pressure. Even for a relatively high-gas pressure of 50 Pa used in RF PECVD, however, the plasma density at a conventional driving frequency of 13.56 MHz is less than 1010 cm−3.

In order to increase the plasma density at the typical frequency of 13.56 MHz, ingenious device is required. In the next section, the various ingenuities will be introduced.


3. Effect of high secondary electron emission oxide on high-density capacitively coupled plasma production

In general, plasma is generated by electrons with an energy higher than an ionization potential of target neutral gas [19]. According to the ionization cross section [20] for noble gases of He, Ne, Ar, and Xe, their ionization energy ranges from 10 to 30 eV, while the energy is a few 100 electron volts when the ionization cross section becomes maximum. These electrons are effectively possible to ionize neutral gases through inelastic collisions. Then, it is expected to produce high-density plasma. In CCP discharge, it is also easy to generate a high voltage of a few hundred volts between the powered and grounded electrodes, that is, CCP can generate secondary electron emission (SEE) from the powered electrode. It was reported that magnesium oxide (MgO) electrodes have a high SEE coefficient which are a few 10 times higher than that of conventional metal electrodes such as aluminum [21].

In this section, the effect of SEE as the acceleration mechanism of electrons is proposed to solve the serious problem of CCP density. The RF breakdown voltage and plasma density are studied experimentally. As show in Figure 1(a), an RF power of 13.56 MHz was supplied to generate CCP between two electrodes of 20-mm diameter with a gap dgap of 10 mm, which were mounted into the center of a cylindrical vessel of 160-mm diameter and 200-mm length. The back of the RF electrode is covered by a grounded metal enclosure to avoid additional discharge between the RF electrode and the grounded vessel. An MgO disk of 20-mm diameter and 2-mm thickness was connected to the Al metal electrode, as shown in Figure 1(b). As a working gas, Ne or Ar gas was introduced in the vessel at 133 Pa.

Figure 1.

(a) Experimental apparatus and (b) electrode construction.

Figure 2 shows RF breakdown voltage VBrf characteristics. VBrf is expressed as a peak-to-peak value measured by a high voltage probe and a digital oscilloscope. VBrf characteristics exhibit a roughly U-shaped distribution like Paschen’s curve of Townsend discharge [22] for both Ne and Ar gases. It is found that VBrf for MgO electrode is higher than that for Al electrode for both Ne and Ar gases, whereas it is reported [21] that the coefficient of SEE for MgO is higher than that for Al. This is ascribed by the effect of voltage drop across MgO. It is also observed that VBrf for Ar gas is lower than that for Ne gas because the ionization potential of Ar gas is lower than that of Ne gas [20].

Figure 2.

Breakdown voltage VRF as a function of pdgap. Here, p and dgap denote gas pressure and gap distance, respectively.

Figure 3 shows plasma density jis as a function of RF voltage VRF applied between the RF electrode and the grounded vessel. The plasma density was estimated from an ion saturation current density jis [23] measured by a tiny Langmuir probe to avoid the disturbance of the plasma by the probe. This is because the electron temperature was almost constant as a function of the RF voltage. The solid line shown in Figure 3 corresponds to jis when it is proportional to VRF. The value of jis = 8 × 10−3 A/cm2 is almost an electron density of approximately 1010 cm−3. As mentioned in Figure 3, the breakdown voltage VBrf for Ne gas at both MgO and Al electrodes ranged from 500 to 1750 Vpp. For Al electrode, it is found that plasma density increases roughly proportionally to VRF. The plasma density is only of the order of 109 cm−3 at even VRF = 1 kVpp.

Figure 3.

Plasma density jis as a function of VRF for Al and MgO electrodes. The solid line is the line of neω.

According to the scaling law under the assumption that the stochastic heating without the SEE effect in the main discharge mechanism in CCP [17], the plasma density can be expressed as


where ω, VRF, and ε are the angular driving frequency, the RF voltage, and the energy needed to generate electrons and ions, respectively. Eq. (3) expresses that ne is proportional to VRF under the experiment that ω and ε are fixed. In the case of Al electrode, the experimental data almost correspond to the line of neω. That is, the plasma production without SEE effect is predominant by stochastic heating where electrons accelerated by the oscillating RF sheath ionize neutral particles.

For MgO electrode, the plasma density is one order of magnitude higher than that for Al electrode. It is found that plasma density increases obviously with increasing VRF for VRF > 400 Vpp, and then attained over 1010 cm−3 for VRF > 800 Vpp and then saturates. The SEE energy emitted from the MgO electrode corresponds to approximately 200 eV at VRF = 400 Vpp. For electron-Ne gas inelastic collision, this SEE energy of ESEE = 200 eV has the maximum ionization cross section [20]. Thus, for VRF > 400 Vpp, the ionization of Ne gas is effectively enhanced by the high SEE coefficient of MgO [21], which leads to the marked increase of plasma density. In fact, the RF power input to the plasma for MgO was higher than that for Al at a fixed applied voltage. Unfortunately, the power efficiency of the reactor could not be estimated because it was not easy to directly monitor current and phase difference between voltage and current.

The reason why the plasma density for MgO becomes constant for VRF > 800 Vpp is considered as follows. The ionization cross section starts to decrease with increasing ESEE for ESEE > 400 eV [20]. Thus, the plasma density decreases with increasing VRF for VRF > 800 Vpp.

Figure 4 shows optical emission intensity of the Ne I line (588.1 nm) as a function of VRF. Here, the optical emission intensity was measured with a spectrometer and a digital oscilloscope. The intensity increases markedly with increasing VRF, in the same manner as plasma density. Therefore, the high-density plasma production is realized by using MgO with a high SEE coefficient in CCP. The effect of high secondary electron emission is one candidate to produce high-density plasma.

Figure 4.

Optical emission intensity of He I line (588.1 nm) as a function of VRF.


4. Effect of structured electrodes on high-density capacitively coupled plasma production

In this section, it is described that structured electrodes can produce the high-density capacitively coupled plasma. One of the structured electrodes is a hollow cathode. The hollow cathode discharge [24] is applied into a production mechanism of CCP to attain high-density plasma.

4.1. Multi-hollow electrode

The effects of a multi-hollow cathode discharge and a high SEE are applied to capacitively coupled plasma to produce high-density plasma [25, 26]. Figure 5(a) and (b) shows the experimental apparatus and construction of the multi-hollow electrode, respectively. As shown in Figure 5(b), one plate has 35 holes with 5-mm diameter and 15-mm length, and these holes lay on a concentric circle. In order to emit secondary electron emission from the electrode facing the multi-hollow electrode, the other electrode is biased by the voltage of low frequency of 1 MHz. The plate is called as the substrate electrode.

Figure 5.

(a) Experimental apparatus and (b) construction of multi-hollow electrode.

Figure 6 shows plasma density and electron-neutral mean free path as a function of Ar gas pressure. Here, plasma density was estimated by ion saturation current density of a negatively biased probe because plasma density is proportional to ion saturation current [27]. The electron-neutral mean free path λen was also calculated by the following equation:


Figure 6.

Plasma density and electron-neutral mean free path as a function of Ar gas pressure.

where σ and n are electro-neutral cross section and Ar gas density, respectively. In Figure 6, as a reference value, an absolute value of the plasma density for Ar gas pressure 37.5 mTorr was estimated from electron saturation current density of probe and is approximately 8 × 1010 cm−3. The plasma density drastically increases with an increasing gas pressure from 7.5 to 22.6 mTorr Pa and then varies by order, although the electron-neutral mean free path is inversely proportional to the gas pressure and reaches the hole size of 5 mm at the gas pressure of 113 mTorr. It is confirmed that the hollow cathode effect is achieved at the pressure range of 22.6–112.5 mTorr where the mean free path is comparable to the hole size of 5 mm.

The effect of SEE to attain high-density plasma production was examined by biasing the substrate electrode. Figure 7 shows plasma density as a function of substrate biasing voltage Vb for axial position z = 5 mm and radial position r = 0 where the origins of z and r are the surface and the center of the powered electrode, respectively. The dashed line denotes the absolute value of plasma density for Vb = 0, which was estimated to be approximately 1010 cm−3 from probe characteristics. It is seen that plasma density increases with the substrate-biased voltage Vb and approached approximately 1011 cm−3 at Vb = −800 V. This suggests that the increase in Vb performs to ionize neutral atoms by inelastic collisions of secondary high-energy electrons. The film preparation is tried by using methane gas. Figure 8 shows the deposition rate as a function of substrate biased voltage Vb. It is found that the deposition rate exponentially increases with increasing Vb in the range of 100 < Vb < 500 V and then saturates. This is because the hybrid discharge combines the hollow cathode discharge and the secondary electron emission. Therefore, the drastic increase in the deposition rate is ascribed by realizing this hybrid discharge. For Vb > 300 V, the deposition rate exceeds the previous reported maximum value which is approximately 30 nm/min [28]. The deposition rate of 200 nm/min is attained at Vb > 500 V.

Figure 7.

Plasma density as a function of RF-biased voltage.

Figure 8.

Deposition rate of thin films and plasma density as a function of RF-biased voltage.

4.2. Ring-shaped hollow electrode

In the previous subsection, the effect of multi-hollow electrode on high-density capacitively coupled plasma was described [29]. In this subsection, the ring-shaped hollow electrode was tried to produce high-density capacitively coupled plasma. The high-density plasma in the trench diffuses toward the downstream region, and then the radial profile of plasma density becomes uniform at a certain axial position. The influence of trench width and gas pressure on plasma density and its profile is examined, comparing the case of a conventional flat electrode.

It is very important to accelerate electrons in the trench by moving RF cathode sheath for producing the high-density plasma with a hollow cathode effect. To satisfy the hollow cathode effect, it is required that the hollow trench width W be twice as long as the sheath thickness ds as shown in Figure 9(a). The depth of the hollow trench must be larger than the sheath thickness. In order to determine the trench width W, the sheath thickness ds can be estimated by the following equation:


where λD, Te, and Vsh denote the Debye length, the electron temperature, and the time-averaged sheath voltage of the RF electrode which was used as the typical self-biased voltage, respectively. Eq. (1) is derived from the Child-Langmuir Law [1, 11]. The sheath thickness ds can be estimated to be approximately 2 mm by Eq. (4) using Te = 4 eV, ne = 1010 cm−3 and Vsh = 200 V. In this experiment, D is set at 5 and 10 mm. Figure 9(b) shows the cross section of the ring-shaped hollow electrode with 100-mm diameter and 20-mm thickness.

Figure 9.

(a) Cross section near the ring-shaped trench and (b) structure of the RF hollow powered electrode.

Figure 10(a) and (b) show typical images of plasma emission near the RF electrode for the ring-shaped hollow electrode and the flat electrode, respectively. As shown in Figure 10(a), a high intensity of plasma emission is observed near the ring-shaped hollow trench for the ring-shaped hollow electrode. The hollow cathode effect is attained in the trench. On the other hand, the conventional flat electrode shows a uniform glow plasma on the whole electrode.

Figure 10.

Typical images of plasma structure for (a) the hollow and (b) the flat electrodes.

Figure 11 shows plasma density ne as a function of Ar gas pressure p for the hollow and the flat electrodes. The position is fixed at z = 8 mm and r = 38 mm. For the hollow electrode, the plasma density raises rapidly with raising Ar gas pressure p and has a peak at p = 180 mTorr and then remains almost constant. At p = 350 mTorr, the plasma density decreases discontinuously, and then at p > 350 mTorr, the plasma density is independent of the gas pressure. The electron-neutral mean free path λen decreases with increasing gas pressure. λen at p = 350 mTorr is approximately 1 mm which is of the order of the magnitude of the hollow trench size. The maximum plasma density is approximately 2 × 1011 cm−3. It is seen that the high-density plasma with the order of magnitude of 1011 cm−3 is achieved in a wide range of gas pressure from 100 to 300 mTorr. In the flat electrode, the plasma density shows a similar tendency with the hollow electrode. The maximum value of the plasma density is one order of magnitude lower than that of the hollow electrode.

Figure 11.

Plasma densities as a function of Ar gas pressure for the hollow (solid circles) and the flat electrodes (squares). Here, the ring-shaped trench width is W = 5 mm.

Figure 12 shows plasma density as a function of Ar gas pressure for W = 5 and 10 mm. Here, the measured position is at z = 12 mm and r = 38 mm. It is seen that the critical pressure when the plasma density attained 1011 cm−3 decreases with increasing the trench width. In fact, the critical values are 140 and 100 mTorr at W = 5 and 10 mm, respectively. The sheath thickness ds was calculated to be approximately 1.7 mm at ne = 1011 cm−3 at the critical gas pressures. The condition of W > 2ds is satisfied at the critical gas pressure.

Figure 12.

Plasma density as a function of Ar gas pressure at the hollow electrode for W = 5 and 10 mm under lower pressure conditions.

4.3. Magnetized ring-shaped hollow cathode discharge

In a low pressure of 1 Pa, it is difficult to produce plasma using only hollow cathode discharge [30]. In this subsection, in order to attain high-density plasma in the low-gas pressure, the combination of hollow cathode discharge and magnetic confinement with magnets is proposed. The addition of a magnetic field is one candidate for performing discharge in the low-gas pressure. It is easy to magnetize electrons under the low-gas pressure.

Figure 13 shows the construction of a ring-shaped hollow cathode for (a) the NS-NS arrangement, (b) the NS-SN arrangement, and (c) the NS arrangement of permanent magnets. The neodymium magnets were used. Three arrangements of permanent magnets were investigated. The NS-Ns arrangement is that two NS magnets with 7 × 10 mm2 in cross section and 10 mm in length are positioned at both walls of a hollow trench and six couples of the NS-NS magnets are used as shown in Figure 13(a). In the NS-SN arrangement, NS and SM magnets are mounted as shown in Figure 13(b). As shown in Figure 13(c), six NS magnets with 10 × 15 mm2 in cross section and 6 mm in length are set at the bottom of a hollow trench for the NS arrangement. The outside of magnets is covered by iron yokes with 1 mm in thickness as shown in Figure 13.

Figure 13.

Constructions of a ring-shaped hollow cathode for (a) the NS-NS arrangement, (b) the NS-SN arrangement, and (c) the NS arrangement of permanent magnets. The neodymium magnets were used.

Figure 14 shows two-dimensional distributions of magnetic field lines at (a) NS-NS, (b) NS-SN, and (c) NS arrangements of permanent magnets, respectively. Here, the area enclosed by dashed lines is the hollow trench. As shown in Figure 14(b), for the NS-SN arrangement, it is clear that the profile of the magnetic field lines is quite different from the other arrangement. The magnetic field lines show a cusp profile in the trench. The NS-SN arrangement is the best profile for magnetic confinement of electrons.

Figure 14.

Two-dimensional distributions of magnetic field lines near the hollow cathode for (a) the NS-NS arrangement, (b) the NS-SN arrangement, and (c) the NS arrangement of the permanent magnets.

Figure 15 shows plasma density as a function of gas pressure at r = 29 mm and z = 23 mm at various arrangements. For the case without magnet, it is found that plasma density decreases from approximately 1011 cm−3 to 8 × 109 cm−3 with a decreasing gas pressure less than 80 mTorr and saturates for a gas pressure region of 80–200 mTorr. It is difficult to sustain high-density plasma without magnet at a low-gas pressure. It is noticeable that the addition of magnets with hollow cathode discharge is effective for producing high-density plasma under the low-gas pressure. For the case of NS-SN arrangement, high-density plasma over 1011 cm−3 is achieved at all gas pressures.

Figure 15.

Plasma density as a function of Ar gas pressure at r = 29 mm and z = 23 mm at various magnet arrangements. Here, the data without magnetic field are also included for the comparison.

In these chapters, in order to improve the plasma density in CCP, various typed CCP discharges have been presented. In Section 3, it is indicated that RF electrode with a high secondary electron emission oxide of MgO is effective to produce high-density capacitively coupled plasma. The plasma density for MgO electrode increases drastically with increasing RF voltage compared with the metal electrode of Al. In Section 4, it is described that the structured electrode plays an important role to improve the plasma density. This mechanism is ascribed by the hollow cathode effect.


5. Conclusions

The radio frequency capacitively coupled plasma source is widely utilized in the semiconductor fabrications. However, the source has a serious problem, although it has some merits such as simple structure and maintenance free. In this chapter, some solutions are introduced by adding simple methods. The first method is the high secondary electron emission electrode. The second method is multi-hollow and ring-shaped electrodes. The third method is magnetized ring-shaped electrode. All methods attained high-density plasma production. Especially, the ring-shaped electrode with magnets performed high-density plasma with 1011 cm−3 under a low-gas pressure. These methods will be useful to advance capacitively coupled plasma for microelectronic technology.


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Written By

Yasunori Ohtsu

Submitted: 30 November 2017 Reviewed: 08 May 2018 Published: 05 November 2018