Atsuro Eitoku
Katholieke Universiteit Leuven
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Publication
Featured researches published by Atsuro Eitoku.
Solid State Phenomena | 2009
Masayuki Wada; Kenichi Sano; James Snow; Rita Vos; L.H.A. Leunissens; Paul Mertens; Atsuro Eitoku
The introduction of metal gates and high-k dielectrics in FEOL and porous ULK dielectrics in BEOL presents severe issues [1] and leads to the requirement of new chemistries and processes. A major challenge in cleaning is the removal of photoresist (PR) in both FEOL and BEOL. In current semiconductor device fabrication flow, the photoresist strip process in FEOL is mostly achieved by applying a sequence of plasma ashing followed by a wet-clean step with sulfuric-peroxide mixture (SPM). But in general, ashing leads to strong oxidation or etching of silicon substrate. Hence, several approaches for ashless PR strip have been reported, such as hot SPM [2] and the combination of a pre-treatment using high velocity CO2 aerosol [3].
Solid State Phenomena | 2007
Guy Vereecke; J. Veltens; Kai Dong Xu; Atsuro Eitoku; Kenichi Sano; Sophia Arnauts; Karine Kenis; James Snow; Chris Vinckier; Paul Mertens
With the continuous shrinkage of critical sizes in semiconductor manufacturing, nano-particles smaller than 100-nm are becoming a potential threat to devices in chips. Storage of wafers contaminated during process steps often results in a decrease of particle removal efficiency in subsequent clean, a phenomenon referred to as aging. In this work, the influence of aging on the removal of silica and silicon nitride nano-particles from hydrophilic Si wafers was studied for different storage conditions. Trends observed for aging as a function of particle size and for different tools indicated that aging will become an issue for critical cleans where substrate etching must be kept very low and the physical component of the clean must be decreased to prevent damage to fine structures. Controlling the relative humidity during storage helped in lowering the effect of aging.
Meeting Abstracts | 2007
Cinzia De Marco; Kurt Wostyn; Twan Bearda; Kenichi Sano; Karine Kenis; Tom Janssens; Leonardus Leunissen; Atsuro Eitoku; P. Mertens
Physically-assisted-cleaning methods, e.g. megasonic cleaning, are evaluated by comparing particle removal efficiency (PRE) with added damage. [1] By identifying and classifying the added defects and linking them to the cleaning conditions, we expect to identify the weak spots in device structures and propose improved cleaning conditions. Weak spots could be related to material properties (e.g. line width roughness, poly-Si height variation, poly grain interfaces, etc). Aim of this work is to investigate if the defect distribution is supported by a random distribution of damage sites. Moreover we will study the impact of the megasonic cleaning settings on the damage size distribution.
Solid State Phenomena | 2005
Atsuro Eitoku; James Snow; Rita Vos; Karine Kenis; Paul Mertens
Introduction For the past few decades, RCA cleaning, that was developed by Kern, et.al. [1], has been the main method for cleaning wafers of semiconductor devices. SC1 (NH4OH/H2O2/H2O-mixture), which constitutes the first step of RCA cleaning, is one of the most widely used wet chemistries for particle and organic contaminants removal. SC2 (HCl/H2O2/H2O-mixture), which is the second component of the RCA cleaning procedure, removes metal contaminants.
Solid State Phenomena | 2007
Guy Vereecke; T. Veltens; Atsuro Eitoku; Kenichi Sano; Geert Doumen; Wim Fyen; Kurt Wostyn; James Snow; Paul Mertens
Cleaning of nano-particles is becoming a major challenge in semiconductor manufacturing as efficient particle removal must be achieved without substrate loss and without damage to fragile structures. In this work cleaning performance and structural damage by a mixed fluid-jet technique were evaluated and directly compared to the performance of several megasonic systems. The test vehicles were hydrophilic Si wafers contaminated with 78-nm SiO2 particles and 70-nm poly-gatestack line patterned wafers. The results showed a broader process window for particle removal without damaging for the mixed fluid-jet technique compared to the megasonic systems.
Solid State Phenomena | 2009
N. Kurumoto; Atsuro Eitoku; Katsuhiko Miya
As the critical dimension of LSI continues to decrease, the surface tension of water and its effect on the formation of watermarks is becoming a significant problem. It is known that watermarks are easily generated when a silicon hydrophobic surface is dried in a wet cleaning process. Many studies about watermarks have been reported [1, 2]. Additionally if the rinse and dry steps were performed under an inert (nitrogen) ambient and the rinse water had low oxygen concentration, watermarks could be effectively avoided [3, 4].
Solid State Phenomena | 2007
Kenichi Sano; Akira Izumi; Atsuro Eitoku; James Snow; L. Nyns; S. Kubicek; R. Singanamalla; Olivier Richard; Thierry Conard; Rita Vos; Paul Mertens
The surface preparation was done in a Dainippon Screen (DNS) single-wafer spin cleaning tool, SU-3000. 300-mm Si wafers (p-type, <100> and <110> ,Cz) were used for tests. The surface preparation recipe consisted of a HF etch step followed by DIO3 for pre-high-k interface layer formation. Due to a quick oxidation by O3, it was very difficult to obtain a uniform thin oxide surface. The original concentration of 10 ppm DIO3 had to be diluted to 1 ppm in the system. Consequently, this 1ppm slower oxidation rate and an optimized scanning pattern resulted in a uniform thin oxide. The HfO2 films were grown by Atomic Layer Deposition (ALD) in the ASM Polygon at 300°C with HfCl4 and H2O precursors. A five-cycle recipe was used for HfO2 monolayer growth in order to focus only on the HfO2 deposited interface between a Si sub-thin oxide and a HfO2 layer. TEM pictures were taken on a Tecnai F30 operating at 300 kV. Ellipsometer measurements were peformed on a KLA-Tencor Aset F5. Since ellipsometric thickness values of HfO2 layers are less accurate for thin high-k layers, more accurate Hf volume measurements were obtained via direct TXRF using an Atomika 8300 (W-Lb) TXRF instrument. XPS was measured by Thermo Theta300 with Al K-alpha X-ray (1486.6 eV) and used to characterize thin oxide ellipsometric thickness. C-V curves were measured by Agilent 4284A precision LCR meter at 100 kHz. Solid State Phenomena Online: 2007-11-20 ISSN: 1662-9779, Vol. 134, pp 53-56 doi:10.4028/www.scientific.net/SSP.134.53
Solid State Phenomena | 2009
Kenichi Sano; Masayuki Wada; Frederik Leys; Roger Loo; Andriy Hikavyy; Paul Mertens; James Snow; Akira Izumi; Katsuhiko Miya; Atsuro Eitoku
Strained silicon engineering was first used at the 90-nm node. Nowadays, a series of techniques has seen wide-spread use and many derivatives are available because of their ease of integration and cost-effective features [ , ]. As a main part of stressor technique, embedded SiGe-S/D technology is reported to improve the pMOSFET drive current [ , ].
Solid State Phenomena | 2009
Masayuki Wada; Sylvain Garaud; I. Ferain; Nadine Collaert; Kenichi Sano; James Snow; Rita Vos; L.H.A. Leunissens; Paul Mertens; Atsuro Eitoku
High-k gate dielectrics (HK), such as HfO2 or HfSiON, are being considered as the gate dielectric option for the 45nm node and beyond. In order to alleviate the Fermi-level pinning issue and to enhance the CET (Capacitive Effective Thickness) by generating the depletion layer in poly-Silicon gate, metal gate electrodes with proper work functions (WF) have to be used on the high-k dielectrics.
Solid State Phenomena | 2007
Kenichi Sano; Frederik Leys; G. Dilliway; Roger Loo; Paul Mertens; James Snow; Akira Izumi; Atsuro Eitoku
Epitaxial deposition of strained Si and SiGe to improve electron and hole mobility and Vt shift is becoming more and more part of the standard CMOS processing [1,2]. One of the most important restrictions imposed on advanced CMOS processing is that on thermal budget. For epitaxial growth processes this thermal budget is quite high. The main contribution comes however not from the growth itself, but from the in-situ H2 bake necessary to remove any oxide traces left prior to epi. Without any pre-epi etch, removal of the native oxide requires at least a bake for several minutes at 900 ̊C or higher. When combined with a wet clean which removes the native oxide and passivates the surface (usually H or Cl), this temperature can be reduced to the range of 850-750 ̊C, although this is always at the cost of a remaining C and O peak at the epi-substrate interface.