Abstract:We report a new method for the nucleation and growth of diamonds by employing an electron-temperature control technique in CH 4 /H 2 radio frequency glow discharge plasma under a low gas pressure of 100 mTorr. The electron temperature in the plasma is controlled under constant gas pressure in a range from 0.5 to 2.5 eV continuously by changing the open area of the slits situated around a grid that is kept at the floating potential. It is observed that the film quality is changed in accordance with the variatio… Show more
“…In the particle-levitation region they lose their kinetic energy through ionizations and collisions with molecules. In the particle-levitation region there is no rf electric field to accelerate electrons, therefore, we have a low electron-temperature plasma in this region [5,6]. This procedure to control the electron temperature was investigated in detail by Shimizu and coworkers [5,6].…”
Section: Methodsmentioning
confidence: 99%
“…For controlling the electron temperature, K. Kato et al developed a grid method [5]. Furthermore, it has been found that the electron temperature plays an important role for diamond deposition [6] and a-Si:H process [7].…”
Particle growth and the behavior of particle clouds in hydrogen-methane capacitively-coupled rf plasmas are investigated. At room temperature most for different wall temperatures and gas compositions of these particles are due to flakes of layers delaminated from the electrode surfaces. Heating of the electrodes up to 800 K and dilution by hydrogen (up to H 2 :CH 4 = 20:1) suppresses the production of the particles from the electrode surfaces. The electron temperature in the particle levitation region is controlled by introducing an additional electrode made from a grid (= gridded electrode) in between the levitation electrode and the driven electrode. If we introduce diamond seed particles (~2.8 µm in diameter) into the plasma with the gridded electrode in place, we observe nucleation of new grains (~100 nm) on the surfaces of the diamond particles. On the other hand, without the gridded electrode we don't observe nucleation but growth of amorphous carbon films on them.
“…In the particle-levitation region they lose their kinetic energy through ionizations and collisions with molecules. In the particle-levitation region there is no rf electric field to accelerate electrons, therefore, we have a low electron-temperature plasma in this region [5,6]. This procedure to control the electron temperature was investigated in detail by Shimizu and coworkers [5,6].…”
Section: Methodsmentioning
confidence: 99%
“…For controlling the electron temperature, K. Kato et al developed a grid method [5]. Furthermore, it has been found that the electron temperature plays an important role for diamond deposition [6] and a-Si:H process [7].…”
Particle growth and the behavior of particle clouds in hydrogen-methane capacitively-coupled rf plasmas are investigated. At room temperature most for different wall temperatures and gas compositions of these particles are due to flakes of layers delaminated from the electrode surfaces. Heating of the electrodes up to 800 K and dilution by hydrogen (up to H 2 :CH 4 = 20:1) suppresses the production of the particles from the electrode surfaces. The electron temperature in the particle levitation region is controlled by introducing an additional electrode made from a grid (= gridded electrode) in between the levitation electrode and the driven electrode. If we introduce diamond seed particles (~2.8 µm in diameter) into the plasma with the gridded electrode in place, we observe nucleation of new grains (~100 nm) on the surfaces of the diamond particles. On the other hand, without the gridded electrode we don't observe nucleation but growth of amorphous carbon films on them.
“…However, we have already demonstrated that the grid bias method can still control e over a wide range [9]. In fact, high-quality diamond was produced in RF discharge CH 4 /H 2 plasmas [14], where e was decreased by varying mechaniclly the length of slits in plasmas [8]. In the case of Argon plasma, e was widely controlled by almost one order of magnitude by changing the mesh size of the grid electrode.…”
ABSTRACT:Volume production of negative hydrogen ions is established efficiently in a pure hydrogen RF discharge plasma by using a self-biased grid electrode for production of low electron-temperature and high density plasma. Using this electrode both high and low electron temperature plasmas are produced in the regions separated by the grid electrode in the chamber, in which the electron temperature in the downstream region is controlled by the mesh size and plasma production parameters. The production rate of negative ions depends strongly on the electron temperature varied by the RF input power and hydrogen pressure. In the case of the grid electrode with the 5 mesh/in., the negative hydrogen ions are produced effectively in the downstream region in the hydrogen pressure range of 0.9 − 2.7 Pa. In addition, the production rate of the negative ion H − raises from 62 % to 87 % at 0.9 Pa by changing the RF power from 20 W to 80 W.
“…On the other hand, the growth of diamond on Mo was relatively easy because of a formation of Mo 2 C layer, which could provide a favorable intermediate layer for diamond nucleation. The growth of diamond on Ni substrate was also studied [2,7] Here, high quality diamond could be produced in a low electron temperature plasma, where a novel method for the control of electron energy distribution function has been developed in order to reduce higher order dissociation of CH 4 [8]. This technique was applied to CH 4 / H 2 plasma for diamond deposition.…”
Formation of diamond particles was investigated in an energy-controlled CH 4 /H 2 radio-frequency (RF) discharge plasma. Here, in particular, it was examined how diamond particles grew on a nickel substrate under an influence of Cu vapor that was supplied from a heated Cu wire. Here, the plasma was generated by a hollow-magnetron-type (HMT) RF plasma source at the frequency of 13.56 MHz. Total pressure was kept at 100 mTorr. Diamond particles grew besides Ni and Cu particles. From Raman spectrum the substrate surface was covered with thin graphite film deposited as a background layer. It was shown that diamond could grow in a self-organized manner even when the other atomic gas species such as Ni and Cu were contained in the gas at the same time during the growth process.
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