Abraham Rudolf Balkenende
Philips
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Featured researches published by Abraham Rudolf Balkenende.
Materials Science and Engineering B-advanced Functional Solid-state Materials | 2003
A. van Veen; R. Escobar Galindo; H. Schut; S.W.H. Eijt; C.V. Falub; Abraham Rudolf Balkenende; F.K. de Theije
Positron beam techniques have been employed to characterise low-k dielectric silica based films, which have two or three dimensional structures of nanometre size pores. Pore fractions vary from 5 to 50%. Positrons implanted in the layer slow down and eventually annihilate with the electrons from the layer. However, in pores of the dielectric films positronium (Ps) is formed before annihilation takes place. The two states of Ps (para-positronium (p-Ps) and ortho-positronium (o-Ps)) are formed with rather different life times of 125 ps and 142 ns, respectively. The behaviour of Ps in the porous material can be described as hot particles with 1 eV initial kinetic energy, which lose their energy by frequent collisions with the atoms of the pore walls. When the pores are interconnected or separated by thin walls allowing permeation of the Ps some of the Ps will effuse from the film into the vacuum. The 2D-ACAR technique enables one to monitor the velocity distribution of the annihilating p-Ps and shows an increasing fraction of surface emitted p-Ps when positrons are implanted closer to the film surface. Measurements of Doppler broadening of 2-gamma annihilation and detection of 3-gamma events (o-Ps) give insight into the frequency of other annihilation events. Combining the results, a complete picture can be obtained of the interactions and transport of the Ps particles in the material. By modelling the Ps behaviour information is obtained on structural parameters of the porous material. A transport model based on multi energy group diffusion of particles describes the results well.
Materials Science and Engineering B-advanced Functional Solid-state Materials | 2003
R. Escobar Galindo; A. van Veen; H. Schut; S.W.H. Eijt; C.V. Falub; Abraham Rudolf Balkenende; F.K. de Theije
Abstract Non-destructive Doppler Broadening (DB), Positronium fraction ( f-Ps ) and Two Dimensional Angular Correlation of Annihilation Radiation (2D-ACAR), Positron Beam Analysis (PBA) techniques have been used to study well-ordered mesoporous silica thin films with hydrophobic or hydrophilic character. The DB results, characterized by the S and W parameters, are related to both the open volume and the chemical environment at the positron annihilation site. The f-Ps and 2D-ACAR techniques are very sensitive probes to determine the type of porosity (open or closed in terms of positronium escape) in thin film materials. Samples with varying pore size (well-controlled at 2, 3 and 4.5 nm, or incorporating microporosity in the silica), pore fraction (from 4 to 57%) and extent of hydrophilicity have been studied. In the hydrophilic samples with small pore size the S -parameter increases with the porosity while the Ps -fraction remains almost unchanged. Increasing the pore size leads to smaller changes in S with increasing porosity. However, an abrupt change in the Ps -fraction is observed for samples with porosity higher than 45%, indicating a positronium percolation threshold for samples with 2D ordering structure. On the other hand, for hydrophobic samples with high porosity (57%) the highest S parameter and Ps -fraction were obtained for the three pore sizes studied. 2D-ACAR is used to determine the fraction and velocity of Ps escaping from some of the latter samples exhibiting positronium percolation. The relationship between these observations and porosity will be discussed in terms of branching of the positron annihilation channels inside the mesoporous films.
Radiation Physics and Chemistry | 2003
S.W.H. Eijt; A. van Veen; C.V. Falub; R. Escobar Galindo; H. Schut; P.E. Mijnarends; F.K. de Theije; Abraham Rudolf Balkenende
Abstract Depth-selective 2D-ACAR investigations on ordered mesoporous silica thin films provide direct evidence that para-positronium (p-Ps) created deep in the films can escape through a network of interconnected pores. The depth dependence of the escape fraction and of the average kinetic energy of non-thermally excited p-Ps is in quantitative agreement with Monte Carlo modeling, assuming classical collisions of p-Ps with the pore walls. The model provides insight in the shape of the angular correlation distributions and their sensitivity to, e.g., the effective wall mass Ms and pore dimensions.
Composites Science and Technology | 2003
R. Escobar Galindo; A. van Veen; H. Schut; C.V. Falub; Abraham Rudolf Balkenende; J.Th.M. De Hosson
Abstract The porosity in particle reinforced sol-gel coatings has been studied. Silica particles (Ludox-TM40) are introduced into methyl silicate coatings to increase the hardness, the elastic modulus and the fracture toughness. The methyl silicate has a relatively low density (about 1.2 g/cm2), while the silica particles are known to be porous. However, the porosity of the silica particles is not accurately known. For model calculations on mechanical properties like the E-modulus this porosity should be known. Positron Beam Analysis (PBA), using the Doppler Broadening (DB) and 2D-Angular Correlation of Annihilation Radiation (2D-ACAR) techniques, was therefore performed for analysis of the porosity. Samples with different weight fractions (0, 20 and 63 wt.%) of silica particles of typically 40 nm in diameter and treated at different curing temperatures (623 and 723 K) were measured. With increasing filler content we observed a decrease in the positron annihilation S-parameter and a broadening of the para-positronium (p-Ps) fraction. By neglecting positron diffusion we can separate porosity in the matrix from that in the particles. This assumption is valid as long as the expected positron diffusion length is short compared to the size of the filler particles, as in the present case. A more detailed description takes into account the local environment of the filler particles affecting their adhesion to the matrix. It is concluded that the density of the silica particles is about 1.4 g/cm2.
Archive | 2005
Robertus Theodorus Franciscus Van Schaijk; Prabhat Agarwal; Erik P. A. M. Bakkers; Martijn Henri Richard Lankhorst; Michiel Jos Van Duuren; Abraham Rudolf Balkenende; Louis Felix Feiner; P.H. Woerlee
Archive | 2008
Rifat Ata Mustafa Hikmet; Abraham Rudolf Balkenende
Archive | 2004
Erik P. A. M. Bakkers; Louis Felix Feiner; Abraham Rudolf Balkenende
Advanced Materials | 2003
Abraham Rudolf Balkenende; F.K. de Theije; Jan Cornelis Kriege
Archive | 2005
Abraham Rudolf Balkenende; Erik P. A. M. Bakkers; Louis Felix Feiner
Archive | 2004
Godefridus A. M. Hurkx; Prabhat Agarwal; Abraham Rudolf Balkenende; Petrus Hubertus Cornelis Magnee; Melanie Maria Hubertina Wagemans; Erik P. A. M. Bakkers; Erwin A. Hijzen