22nd International Symposium on Plasma Chemistry July 5-10, 2015; Antwerp, Belgium Numerical characterisation of strong magnetized inductively coupled plasmas at low pressure in argon S. Yang1, Y. Zhang2 and W. Jiang1 1 School of Physics, Huazhong University of Science and Technology, 430074 Wuhan, P.R. China Research group PLASMANT, Department of Chemistry University of Antwerp, 2610 Antwerpen-Wilrijk, Belgium 2 Abstract: A one-dimensional, implicit particle-in-cell Monte Carlo collision model is used to explore the effect of magnetic field on plasma characteristics for a single radio frequency magnetized inductively coupled plasma using a frequency source of 13.56MHz in argon (Ar) at low pressure of 10mTorr. Plasma densities and temperature under different magnetic field (0.1-0.4T) are shown. It is found that the increased magnetic field can prolong the lifetime of plasma. With the increase of magnetic field, species densities increase firstly and then decrease. The results indicate that the increased magnetic field can be used to prolong the lifetime of plasma, but at the cost of decreased plasma density. And the maximum value of species densities of Ar occurs at B=0.2T in our simulation. Keywords: magnetized inductively coupled plasma, numerical simulation, Ar discharges. 1. Introduction As widely used in the substrate etching, thin film growth, plasma propulsion, materials processing and semiconductor industry, inductively coupled plasma source (ICPs) excited by a single radio frequency is an important low temperature plasma source [1-3]. With the development of the technology of plasma processing, there is an increased demand for high density plasmas with good uniformity and other excellent properties. ICPs are expected to continue to play the key role in the next generation of plasma reactors. Many researches have been reported in the literature for the development of the ICPs [4, 5]; technological applications of ICP have been discussed in detail [6-8]; various ICP parameters have been measured [9-11] and theoretical models and simulation codes developed [12-15]. Although such experimental and theoretical studies have been devoted to the ICP, only a few researches have addressed the fundamental characteristics of magnetized inductively coupled plasma (MICP) discharge in the past. In an effort to explore MICP characteristics, Lieberman et al [16] developed a global model for homogeneous magnetized plasma and demonstrated the predicted relations of electron density with magnetic field, RF power and gas pressure. Lee et al [17] first established a model that applying a weak magnetic field to the planar coil RF-ICP plasma source. Their experimental results indicated that a proper application of magnetic field can effectively improve many discharge characteristics of the ICP, such as heating efficiency, uniformity, plasma potential and impedance matching. Its application to oxide etching revealed signs of less damage to the silicon surface with increased etch rate and selectivity [18]. Among these desirable properties of MICP, a further exploration on plasmas at a low pressure is especially P-II-5-20 valuable because of the future demand on the production of high density plasmas at very low pressure (≤ 1mTorr). Particle-in-cell Monte Carlo collision (PIC/MCC) model is a numerical simulation technique commonly used to simulate low temperature plasmas [19, 20]. It can provide valuable information for understanding plasma discharges. In this work, a one-dimensional, implicit PIC/MCC model has been used to research the effect of magnetic field on the species density and temperature of a single frequency inductively coupled plasma with a radiofrequency source interaction within them. 2. Model description We present a one-dimensional analysis of MICP properties between two parallel plate electrodes with a length of 20cm and the distance of two electrodes is 8cm. A radio-frequency source of 13.56MHz is used to drive the discharge. The Ar gas is used at a temperature of 300K and at a low pressure of 10mTorr. The application of external magnetic fields is varying from 0.1 to 0.4T. We use an implicit PIC/MC method [21] and the method has been described in detail and tested widely before [20, 23]. In this code scheme, the field equations are obtained from direct summation and extrapolation of the equations of particle motion. A standard MC procedure [22] is used, in which only electron-atom and ion-atom collisions are considered, such as electron-Ar and Ar+-Ar elastic collisions. Because the ionisation degree is under 1% and Coulomb collision are negligible [23]. Table1 shows the collision reactions of Ar in the simulation, including elastic, inelastic, ionisation and charge exchange processes. The cross sections for these reactions are adopted from this reference [24]. The simulation time-step is fixed at 2×10-11s, and the simulations are run for 104 time-steps. 1 Table 1. Collision reactions of Ar in the simulation. Number/description reaction Electron energy loss 1. Elastic e + Ar → e + Ar 2. Inelastic e + Ar → e + Ar* 11.5eV 3. Ionisation e + Ar → 2e + Ar+ 15.8eV 4. Elastic Ar+ + Ar → Ar+ + Ar 5. Charge exchange Ar+ + Ar → Ar + Ar+ Figure 1. Species densities of Ar with different magnetic field 3. Results and discussion Figure1 and 2 show the species densities and temperature of Ar plasma under different magnetic field correspondingly. It can be seen from the figures that with the increase of the external magnetic field, the time for plasma to reach the peak of density and temperature (i.e., complete ionization) is getting longer and the time interval between two different magnetic fields is longer. That is to say, the lifetime of plasma is longer. But we can observe the peak value of species densities increase firstly and then decrease with the increase of magnetic field and the maximum value occurs at B=0.2T. The results indicate that the increased magnetic field can be used to prolong the lifetime of plasma, but at the cost of decreased plasma density. Moreover, at the end of the plasma discharges, Ar+ density does not disappear immediately like electron density. It decreases rapidly by two orders of magnitude and then disappears after a short period of time. This is because the electrons are of high energy and are easy to get wall loss. And the electrons move much faster than the Ar+. Figure 2. Species temperature of Ar with different magnetic field 4. Conclusion The effect of external magnetic field on plasma characteristics for a single radio frequency strong magnetized inductively coupled plasma in Ar at a low pressure was investigated by a one-dimensional, implicit particle-in-cell Monte Carlo collision model. The simulation results show that the increased magnetic field can prolong the lifetime of plasma. Species densities increase firstly and then decrease with the increase of magnetic field. These indicate that the increased magnetic field can be used to prolong the lifetime of plasma, but at the cost of decreased plasma density. And the maximum value of species densities of Ar occurs at B=0.2T in our simulation. We think these discharge characteristics could have positive effects on the production. 5. 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