“A Fourier transform laser microprobe mass spectrometer with external ion source for organic and inorganic surface and micro-analysis”. van Roy W, Struyf H, van Vaeck L, Gijbels R, Caravatti P Wiley, Chichester, page 463 (1994).
Keywords: H3 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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Tan H (2012) From EELS to oxidation state mapping : an investigation into oxidation state mapping of transition metals with electron energy-loss spectroscopy. Antwerpen
Keywords: Doctoral thesis; Electron microscopy for materials research (EMAT)
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Shi H (2014) From functional properties to micro/nano-structures : a TEM study of NiTiNb shape memory alloys. Antwerpen
Keywords: Doctoral thesis; Electron microscopy for materials research (EMAT)
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Ke X (2010) From top-down to bottom-up : from carbon nanotubes to nanodevices. Antwerpen
Keywords: Doctoral thesis; Electron microscopy for materials research (EMAT)
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“Functional imaging to predict treatment success of mandibular advancement devices in sleep-disordered breathing”. de Backer J, Vanderveken O, Vos W, Devolder A, Verhulst S, Verbraecken J Antwerpen, page 141 (2008).
Keywords: H3 Book chapter; Condensed Matter Theory (CMT); Laboratory Experimental Medicine and Pediatrics (LEMP); Translational Neurosciences (TNW)
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Khaletskaya K (2014) Functional metal-organic frameworks : from bulk to surface engineered properties. Antwerpen
Keywords: Doctoral thesis; Electron microscopy for materials research (EMAT)
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“Functioning of thiocyanate ions during sulphur and sulphur-plus-gold Sensitization”. Charlier E, Gijbels R, Van Doorselaer M, De Keyzer R, , 172 (2000)
Abstract: Not much about the effect of thiocyanate addition on the sulphur ripening is known, although it is used for many applications in photographic practice. Via a combination of tracer analysis and diffuse reflectance spectroscopy the effect of thiocyanate addition on the sulphur and sulphur-plus-gold ripening could be unveiled. When thiocyanate is added prior to the sulphur addition, it appears to rearrange the silver halide surface in such way that the sulphur deposition rate is enhanced, but the supply of interstitials is limited. Addition of thiocyanate after the sulphur reaction results in the formation of thiocyanate complexes with silver, from which a silver ion is more easily deposited in a surface cell of the silver sulphide clusters thus enhancing the sensitization rate. For sulphur-plus-gold sensitized emulsions it was observed that part of the gold ions could be removed out of the Ag2-xAuxS clusters by addition of thiocyanate ions and subsequent washing. Hence, it was concluded that two different types of gold ions are present in the silver sulphide clusters; 1. gold ions which are substitutional for silver (bound between sulphur and bromide ions) 2. gold ions which bridge two or three sulphur atoms. Incorporation of gold ions into silver sulphide clusters suppresses their optical absorption in diffuse reflectance spectroscopy. Since the optical absorption at 505 nm can completely be restored by addition of thiocyanate, it is assumed that the entity absorbing at this wavelength is a monomer of silver sulphide.
Keywords: P1 Proceeding; Engineering sciences. Technology; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Fundamental aspects of an analytical glow discharge”. van Straaten M, Gijbels R Royal Society of Chemistry, Cambridge, page 130 (1993).
Keywords: H3 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Geometry induced defects in a confined Wigner lattice”. Peeters FM, Kong M, Partoens B, , 192 (2002)
Keywords: P1 Proceeding; Condensed Matter Theory (CMT)
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“Geothermal water analysis by X-ray fluorescence and neutron activation”. van Grieken R, Gijbels R, Blommaert W, Vandelannoote R, Van 't dack L US Energy Research and Development Administration, S.l., page 368 (1978).
Keywords: H3 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT); AXES (Antwerp X-ray Analysis, Electrochemistry and Speciation)
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“Glow discharge mass spectrometry, methods”. Bogaerts A Academic Press, San Diego, Calif., page 669 (2000).
Keywords: H3 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Glow discharge optical spectroscopy and mass spectrometry”. Steiner RE, Barshick CM, Bogaerts A Wiley, Chichester, page 1 (2009).
Abstract: Optical (atomic absorption spectroscopy, AAS; atomic emission spectroscopy, AES; atomic fluorescence spectroscopy, AFS; and optogalvanic spectroscopy) and mass spectrometric (magnetic sector, quadrupolemass analyzer, QMA; quadrupole ion trap, QIT; Fourier transform ion cyclotron resonance, FTICR; and time-of-flight, TOF) instrumentation are well suited for coupling to the glow discharge (GD). The GD is a relatively simple device. A potential gradient (5001500 V) is applied between an anode and a cathode. In most cases, the sample is also the cathode. A noble gas (e.g. Ar, Ne, and Xe) is introduced into the discharge region before power initiation. When a potential is applied, electrons are accelerated toward the anode. As these electrons accelerate, they collide with gas atoms. A fraction of these collisions are of sufficient energy to remove an electron from a support gas atom, forming an ion. These ions are, in turn, accelerated toward the cathode. These ions impinge on the surface of the cathode, sputtering sample atoms from the surface. Sputtered atoms that do not redeposit on the surface diffuse into the excitation/ionization regions of the plasma where they can undergo excitation and/or ionization via a number of collisional processes. GD sources offer a number of distinct advantages that make them well suited for specific types of analyses. These sources afford direct analysis of solid samples, thus minimizing the sample preparation required for analysis. The nature of the plasma also provides mutually exclusive atomization and excitation processes that help to minimize the matrix effects that plague so many other elemental techniques. Unfortunately, the GD source functions optimally in a dry environment, making analysis of solutions more difficult. These sources also suffer from difficulties associated with analyzing nonconductingsamples. In this article, first, the principles of operation of the GD plasma are reviewed, with an emphasis on how those principles relate to optical spectroscopy and mass spectrometry. Basic applications of the GD techniques are considered next. These include bulk analysis, surface analysis, and the analysis of solution samples. The requirements necessary to obtain optical information are addressed following the analytical applications. This section focuses on the instrumentation needed to make optical measurements using the GD as an atomization/excitation source. Finally, mass spectrometric instrumentation and interfaces are addressed as they pertain to the use of a GD plasma as an ion source. GDsources provide analytically useful gas-phase species from solid samples. These sources can be interfaced with avariety of spectroscopic and spectrometric instruments for both quantitative and qualitative analysis.
Keywords: H1 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Glow discharges in emission and mass spectrometry”. Jakubowski N, Bogaerts A, Hoffmann V Blackwell, Sheffield (2003).
Keywords: H3 Book chapter; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Gold mobility in waters from temperate regions”. Cidu R, Fanfani L, Shand P, Edmunds WM, Van 't dack L, Gijbels R, (1995)
Keywords: P3 Proceeding; Plasma Lab for Applications in Sustainability and Medicine – Antwerp (PLASMANT)
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“Gold particles supported on TiO2”. Giorgio S, Henry CR, Pauwels B, Van Tendeloo G, , 369 (2000)
Keywords: P3 Proceeding; Electron microscopy for materials research (EMAT)
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“Granular films assembled of CoN, CrM and mixtures of CoN and CrM clusters: structure and electron transport properties”. Kuhn LT, Vanhoutte F, Cannaerts M, Neukermans S, Verschoren G, Bouwen W, van Haesendonck C, Lievens P, Silverans RE, Pauwels B, Van Tendeloo G, (2000)
Keywords: P3 Proceeding; Electron microscopy for materials research (EMAT)
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Amelinckx S, van Dyck D, van Landuyt J, Van Tendeloo G (1997) Handbook of microscopy: applications in materials science, solid-state physics and chemistry. Vch, Weinheim
Keywords: ME1 Book as editor or co-editor; Electron microscopy for materials research (EMAT); Vision lab
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“High energy transitions and phonon-assisted harmonics of a shallow magneto-donor in GaAs/AlGaAs multiple quantum wells”. Bruno-Alfonso A, Hai G-Q, Peeters FM, Yeo T, Ryu SR, McCombe BD, , 1413 (2001)
Keywords: P1 Proceeding; Condensed Matter Theory (CMT)
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“High field magnetotransport in a Ga0.8In0.2As quantum well with a parallel δ-layer”. van der Burgt M, Karavolas VC, Peeters FM, Singleton J, Nicholas RJ, Herlach F, Harris JJ, van Hove M, Borghs G, , 588 (1995)
Keywords: P3 Proceeding; Condensed Matter Theory (CMT)
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“High resolution electron microscopy for materials”. van Landuyt J Eurem 92, Granada, page 23 (1992).
Keywords: H3 Book chapter; Electron microscopy for materials research (EMAT)
Times cited: 7
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“High-resolution electron microscopy for semiconducting materials science”. van Landuyt J, Vanhellemont J Elsevier, Amsterdam, page 1109 (1994).
Keywords: H3 Book chapter; Electron microscopy for materials research (EMAT)
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“High-resolution visualization techniques : structural aspects”. Schryvers D, Van Aert S Springer, Berlin, page 135 (2012).
Keywords: H1 Book chapter; Electron microscopy for materials research (EMAT)
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“Hole band engineering in self-assembled quantum dots and molecules”. Peeters FM, Tadić M, Janssens KL, Partoens B s.l., page 191 (2004).
Keywords: H1 Book chapter; Condensed Matter Theory (CMT)
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“How to interpret short-range order HREM images”. De Meulenaere P, Van Tendeloo G, van Landuyt J, (1996)
Keywords: P3 Proceeding; Engineering sciences. Technology; Electron microscopy for materials research (EMAT)
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“HREM for characterisation of nanoscale microstructures”. van Landuyt J, Van Tendeloo G, , 15 (1998)
Keywords: P3 Proceeding; Electron microscopy for materials research (EMAT)
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“HREM imaging analysis in the study of pretransition and nucleation phenomena in alloys (Invited)”. Schryvers D, Van Tendeloo G, van Landuyt J, Le Tanner, , 659 (1994)
Keywords: P1 Proceeding; Electron microscopy for materials research (EMAT)
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“HREM investigation of La(1-x)Ca(x)MnO3-delta thin films”. Lebedev O, Van Tendeloo G, Amelinckx S, Leibold B, Habermeier HU, , 517 (1998)
Keywords: P1 Proceeding; Electron microscopy for materials research (EMAT)
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“HREM of defects in cubic boron nitride single crystals”. Nistor LC, van Landuyt J, Dincã, G, , 695 (1998)
Keywords: P1 Proceeding; Electron microscopy for materials research (EMAT)
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“HREM study of short-range order in Cu-Pd alloys”. Rodewald M, Rodewald K, De Meulenaere P, Van Tendeloo G, (1996)
Keywords: P3 Proceeding; Electron microscopy for materials research (EMAT)
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“Hybrid magnetic-semiconductor nanostructures”. Peeters FM, de Boeck J Academic Press, New York, page 345 (1999).
Keywords: H3 Book chapter; Condensed Matter Theory (CMT)
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