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Dive into the research topics where H. Sugai is active.

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Featured researches published by H. Sugai.


Applied Physics Letters | 1989

Mass spectroscopic investigation of the CH3 radicals in a methane rf discharge

Hirotaka Toyoda; Hiroki Kojima; H. Sugai

Neutral CH3 radicals in a capacitively coupled rf discharge in methane have been detected with a quadrupole mass spectrometer utilizing a threshold ionization technique. The absolute density of CH3 radicals was measured at pressures from 0.5 to 20 mTorr, together with the ionic composition of the methane plasma. The principal ionic species were CH+5 and C2H+5 , except in the low‐pressure region, suggesting the importance of ion‐molecule reactions in the plasma. The lifetime of CH3 radicals in the afterglow of pulsed rf discharges was measured and explained in terms of the recombination reaction CH3 +CH3 →C2 H6.


Applied Physics Letters | 2007

Multibubble plasma production and solvent decomposition in water by slot-excited microwave discharge

Tatsuo Ishijima; H. Hotta; H. Sugai; Masanori Sato

Intense microwaves are injected from a slot antenna into water partly filling a metal vessel. When the vessel is evacuated to saturated vapor pressure (∼5×103Pa) of water, microwave breakdown gives rise to plasmas in many bubbles in the boiling water. Gas bubbling technique enables production of multibubble plasmas in water even at atmospheric pressure. Optical emissions from the exited species are investigated to identify radical species in water. In order to demonstrate application to purification of polluted water, methylene blue and trichlorethylene solution in 8l water were observed to rapidly decrease with multibubble plasma treatment.


Applied Physics Letters | 1990

Spatial distribution of CH3 and CH2 radicals in a methane rf discharge

H. Sugai; Hiroki Kojima; A. Ishida; Hirotaka Toyoda

Spatial distributions of neutral radicals CH3 and CH2 in a capacitively coupled rf glow discharge of methane were measured by threshold ionization mass spectrometry. A strong asymmetry of the density profile was found for the CH2 radical in the high‐pressure (∼100 mTorr) discharge. In addition, comprehensive measurements of electron energy distribution, ionic composition, and radical sticking coefficient were made to use as inputs to theoretical modeling of radicals in the methane plasma. The model predictions agree substantially with the measured radical distributions.


Applied Physics Letters | 2003

Electron heating mode transition observed in a very high frequency capacitive discharge

E. Abdel-Fattah; H. Sugai

The effect of excitation frequency in the 13.56–60 MHz range on the electron energy distribution function (EDF) of capacitively coupled plasma is investigated. Under a fixed rf voltage (50–130 V peak-to-peak) and argon pressure (100 mTorr), a remarkable change in the EDF is observed: a Druyvesteyn type at low frequencies (≃13.56 MHz) evolves into a bi-Maxwellian type in a very high frequency (VHF) above 30 MHz. The transition frequency decreases with increasing the rf voltage. The observed frequency effect on the EDF is tentatively explained in terms of the transition of electron heating mode from the collisional ohmic heating at low frequencies into the plasma surface heating in the VHF range.


Journal of Nuclear Materials | 2001

Rapid diffusion of lithium into bulk graphite in lithium conditioning

N. Itou; Hirotaka Toyoda; K. Morita; H. Sugai

One of the known lithium conditioning effects is the reduction of carbon impurities released from the graphite walls of a tokamak. However, little is known about the role of lithium in graphite-plasma interactions. Graphite intercalates lithium atoms between the hexagonal layer planes. The Li diffusion constant in the direction perpendicular to the basal planes of highly oriented pyrolytic graphite (HOPG) is measured for the first time using Rutherford backscattering spectrometry and is found to be D = 2.1 x 10 10 cm 2 /s with an activation energy of 0.26 eV, in the case of low temperatures (300 K) and low Li concentration (Li/C atomic ratio <3%). This value increases by a factor of two when HOPG is exposed to hydrogen plasma before lithium deposition. The implications resulting from the Li-graphite intercalation in lithium wall conditioning are discussed, focusing on Li-induced suppression of graphite sputtering.


Journal of Vacuum Science and Technology | 1998

Observation of surface dissociation of low-energy polyatomic ions relevant to plasma processing

H. Sugai; Yoshihito Mitsuoka; Hirotaka Toyoda

To gain insight into surface processes in plasma processing, basic ion beam experiments are performed on two representative polyatomic-ion species: hydrocarbon ions CHx+ for deposition processes and fluorocarbon ions CFx+ for etching processes (x=1,2,…). A single ion species is extracted from an inductive plasma via a mass filter and directed onto aluminum surfaces at energies 100 eV) i...


Applied Physics Letters | 2007

Role of atomic nitrogen during GaN growth by plasma-assisted molecular beam epitaxy revealed by appearance mass spectrometry

J. Osaka; M. Senthil Kumar; Hirotaka Toyoda; Tatsuo Ishijima; H. Sugai; Takashi Mizutani

To identify the species which contribute to GaN growth, the authors investigated the discharge parameter (0.3–4.8SCCM (SCCM denotes cubic centimeter per minute at STP), 150–400W) dependences of the atomic N flux by appearance mass spectrometry and of the incorporated nitrogen atoms into GaN layers grown by plasma-assisted molecular beam epitaxy (PAMBE) using the rf-plasma source. Ion fluxes were also evaluated by ion current measurements. A good correlation between the supplied atomic N flux and the incorporated nitrogen flux was obtained under a wide range of plasma conditions. It was clarified that the atomic N plays a dominant role in the growth of GaN by PAMBE.


Applied Physics Letters | 1989

Hydrogen retention and release dynamics of amorphous carbon films exposed to a hydrogen plasma

H. Sugai; S. Yoshida; Hirotaka Toyoda

H2 and DH release was investigated in a pulsed deuterium discharge over a carbon thin‐film deposited wall. A large quantity of hydrogen was desorbed by 300 eV D+2 irradiation from hydrogenated amorphous carbon (a‐C:H) deposited by a hydrogen‐admixed methane discharge. On the other hand, a strong pumping effect was observed in the case of films deposited by a helium‐admixed discharge. The wall pumping effect was attributed to the presence of interstitial vacancies rather than dangling bonds in the films. A linear dependence of the hydrogen release rate on the ion bombarding current suggests that molecular formation is by direct hydrogen abstraction instead of recombination of two free hydrogen atoms. A dynamic model of hydrogen release and retention for a‐C:H layers during hydrogen implantation is proposed. Corresponding calculations yield satisfactory agreement with observations when using appropriate rate constants for trapping and detrapping.


Applied Physics Letters | 1987

Control of hydrogen content of boron thin films produced in a dc toroidal discharge

Hirotaka Toyoda; H. Sugai; T. Isozumi; Takayoshi Okuda

Hydrogenated amorphous boron films have been produced by a toroidal glow discharge of B2H6/He mixtures at low pressures (10−2 Torr). Chemically stable pure films with a low hydrogen content can be formed at a moderate substrate temperature (∼200 °C) when the diborane flow rate is raised above 10 sccm with the discharge power lowered below 100 W. The controllability of H content is potentially interesting for applications in the coating of nuclear fusion devices, as well as for use in electronic devices.


Applied Physics Letters | 2005

Complex ion-focusing effect by the sheath above the wafer in plasma immersion ion implantation

Eugen Stamate; N. Holtzer; H. Sugai

The ion flux on the wafer surface during plasma immersion ion implantation is investigated by three-dimensional simulations and experiments. Due to the finite size of the wafer and its stage, the evolving sheath acts as a lens that focuses the positive ions to distinct regions on the wafer surface. Depending on the sheath profile, two focusing effects are identified. Discrete focusing involves ions entering the sheath from its frontal side and leads to the formation of a passive surface near the wafer edge, while the modal focusing affects ions entering the sheath from the lateral side of the stage and are eventually directed to the wafer center.

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