ICMCTF2011 Session TS4-1: Characterization: Linking Synthesis, Microstructure, and Properties
Time Period MoM Sessions | Abstract Timeline | Topic TS4 Sessions | Time Periods | Topics | ICMCTF2011 Schedule
Start | Invited? | Item |
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10:00 AM | Invited |
TS4-1-1 Strain Mapping in Nanostructures and Thin Films by Dark-Field Electron Holography
Martin Hÿtch, N. Cherkashin, S. Reboh, E. Javon, F. Houdellier, E. Snoeck (CEMES-CNRS, Université de Toulouse, France) Dark-field electron holography (DFEH) is a new technique for measuring strain in crystalline materials [1]. The experimental setup is similar to conventional off-axis electron holography except that diffracted beams are used to create the interference. The diffracted beam emanating from a strained region of crystal is interfered with the diffracted beam coming from an unstrained part of the sample, typically the substrate. The holographic fringes encode the information about the relative deformation of the two crystalline lattices, and can be recovered using geometric phase analysis - a technique first developed for the analysis of high-resolution electron microscopy images (HRTEM) [2]. By combining the information from two diffracted beams, the full strain tensor can be determined in two dimensions. The advantage of the new technique is that strains can be measured to high precision, with nanometre spatial resolution and for micron fields of view. In addition, the samples are relatively thick, about 100-200 nm, and can be prepared by standard focussed-ion beam (FIB) or tripod polishing. Dark-field holography was first developed for mapping strains in strained-silicon MOSFET devices [1,3] but the technique is not limited to such cases. Strained layers grown epitaxially on a substrate also have the required geometry to apply the technique. Examples will be given of the measurement of strain in carbon-doped silicon and germanium layers grown on silicon substrates [4,5]. Results will be compared with modelling using the finite-element method (FEM). Indeed, we will show that local relaxation due to misfit dislocations can be studied and quantified in the course of the analysis. Finally, the limitations and experimental requirements will be discussed along with future developments. [1] M.J. Hÿtch, F. Houdellier, F. Hüe, and E. Snoeck, Nature 453 (2008) 1086-1089. [2] M.J. Hÿtch, E. Snoeck and R. Kilaas, Ultramicroscopy 74 (1998) 131–146. [3] F. Hüe, M.J. Hÿtch, F. Houdellier, H. Bender, and A. Claverie, Appl. Phys. Lett. 95, 073103 (2009). [4] N. Cherkashin, M. J. Hÿtch, F. Houdellier, F. Hüe, V. Paillard, A. Claverie, A. Gouyé, O. Kermarrec, D. Rouchon, M. Burdin, P. Holliger, Appl. Phys. Lett. 94 (2009) 141910. [5] J. M. Hartmann, L. Sanchez, W. Van Den Daele, A. Abbadie, L. Baud, R. Truche, E. Augendre, L. Clavelier, N. Cherkashin, M. Hytch, and S. Cristoloveanu, Semiconductor Science and Technology 45 (2010) 075010. |
10:40 AM |
TS4-1-3 Electronic Structure Investigation of Amorphous CrCx Films
Martin Magnuson (Linköping University, Sweden); Matilda Hanson (Uppsala University, Sweden); Jun Lu, Lars Hultman (Linköping University, Sweden); Ulf Jansson (Uppsala University, Sweden) Chromium-based carbides (CrCx) with different compositions constitute an interesting class of materials to investigate. This is mainly due to the large potential of making improved corrosion resistant coatings combined with other desired properties for potential applications as wear-resistant coatings, low-friction films, and electrical contacts. Moreover, CrCx carbides can be fabricated as amorphous materials that make them particularly interesting for electronic structure and mechanical property investigations. Detailed understanding of the chemical bonding is necessary to optimize their properties. In this work, the electronic structure of a series of amorphous-to-nanocrystalline CrCx (x = 0.2-0.8) films have been investigated by soft x-ray absorption (SXA) and emission (SXE) spectroscopy. The Cr 2p SXA spectra exhibit a crystal-field splitting of ~1.2 eV where the intensity of the unoccupied Cr states systematically increases as the C content increases. Correspondingly, the Cr L3/L2 branching ratio of the occupied states observed in SXE decreases simultaneously as the observed σ/π ratio in C K SXE decreases. This is a signature of an increased Cr ionicity as the C content increases. The results will be discussed together with XRD, XPS, TEM, and EELS results. The radial distribution functions obtained from EELS indicate a C-C bond distance of ~1.5 Å and a Cr-C distance of ~2.2 Å. The measured spectra are compared and interpreted with ab initio calculations including core-to-valence dipole matrix elements. The calculated results are found to yield consistent spectral functions to the experimental data. By varying the composition, a change of the electron population is achieved causing a change of covalent/ionic bonding between the Cr and C atoms, that enables control of the macroscopic properties of the materials. |
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11:00 AM |
TS4-1-4 Electrical and Structural Properties of Ultrathin Polycrystalline and Epitaxial TiN Films Grown by Reactive Magnetron Sputtering
Fridrik Magnus, Arni Ingason, Sveinn Olafsson (University of Iceland); Jon Gudmundsson (Shanghai Jiao Tong University, China) Ultrathin TiN films were grown by reactive magnetron sputtering using both dc and high power impulse magnetron sputtering (HiPIMS) on amorphous SiO2 substrates and single-crystalline MgO substrates at various growth temperatures. The resistance of the films was monitored in-situ during growth to determine the coalescence and continuity thicknesses. Structural characterization was carried out using X-ray diffraction and reflection methods. TiN films grown by dc magnetron sputtering on SiO2 are polycrystalline and for a growth temperature of 600oC the nominal coalescence and continuity thicknesses are 0.8 and 1.9 nm, respectively [1]. TiN films grow epitaxially on the MgO substrates from temperatures of 200oC and upwards as shown by XRD measurements [2]. As the growth temperature is increased from room temperature to 600oC the coalescence thickness drops from 1.09 nm to 0.08 nm and the minimum thickness for a continuous film drops from 5.5 nm to 0.7 nm [3]. A large drop in resistivity is seen with increasing growth temperature and the resistivity reaches 16.6 μΩcm for growth temperature of 600oC. X-ray reflection measurements indicate a significantly higher density and lower roughness of the epitaxial TiN films. [1] A. S. Ingason, F. Magnus, J. S. Agustsson, S. Olafsson, and J. T. Gudmundsson, In-situ electrical characterization of ultrathin TiN films grown by reactive dc magnetron sputtering on SiO2, Thin Solid Films, 517 (24) (2009) 6731-6736 [2] A. S. Ingason, F. Magnus, S. Olafsson and J. T. Gudmundsson, Morphology of TiN thin films grown on MgO [100] by reactive dc magnetron sputtering, Journal of Vacuum Science and Technology A, 28(4) (2010) 912 - 915 [3] F. Magnus, A. S. Ingason, S. Olafsson and J. T. Gudmundsson, Growth and in-situ electrical characterization of ultrathin epitaxial TiN films on MgO, Thin Solid Films, submitted June 2010 |
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11:20 AM |
TS4-1-5 On X-Ray Diffraction Study of Stresses and Preferred Grain Orientations in Thin Films - Specific Non-Routine Cases
Radomír Kužel (Charles University in Prague, Faculty of Mathematics and Physics, Czech Republic); Zdeněk Matěj, Lea Nichtová (Charles University in Prague, Faculty of Mathematics and Physics); Josef Buršík (Institute of Inorganic Chemistry of Academy of Sciences of the Czech Republic); Daniel Šimek (Technical University Bergakademie Freiberg, Germany); Jindřich Musil (University of West Bohemia, Czech Republic) Stresses and preferred grain orientations play an important role in thin films of many types and applications. X-ray diffraction (XRD) is one of the most important methods of their characterization. Selected examples of specific non-routine cases are presented we met recently during the study of thin films of a high technological interest (hard coatings, photocatalytic films, films with interesting electrical properties). In TiO2 thin films crystallized from amorphous state into anatase phase, tensile stresses are generated during the crystallization and inhibit further crystallization. This process results in strong dependence of both stresses and crystallization rate on the film thickness. The measured strains were highly anisotropic and recently calculated single crystal elastic constants of anatase were used for the stress evaluation by the conventional sin2ψ method and because of absence of texture simultaneously also by our newly developed software for total XRD powder pattern fitting. In the studied cubic KTAO3 thin films on Si substrate with Pt interlayer, rather unusual multicomponent textures were detected when each of the component had narrow orientation distribution. In this case, a set of the so-called ω-scans was collected for finding of all the components followed by the standard θ-2θ scans at specific pre-calculated sample inclinations. Then the so-called crystallite group method could be applied for the stress determination. The most difficult task was the analysis of compact highly textured hexagonal TiB2 hard coatings on steel. The (00l) texture was very sharp but of fiber type. None of the above methods could be applied since the range of possible inclinations ψ was very narrow and the ratio of lattice parameters c/a could not be determined independently. Therefore, full maps of reciprocal space had to be measured and calculated. Finally, the stress could be evaluated only from the deformation and/or inclination of the diffraction spot in the map by the reciprocal map fitting. In the last example, thin films of hexagonal ferrite SrFe12O19 on SrTiO3(111) substrate were analyzed. After routine scans (symmetric or asymmetric θ-2θ scan, ω-scan, φ-scan) it seemed that there is just a strong fiber texture. Only more complex study on asymmetric planes discovered well developed epitaxial growth as a main feature of the partially inhomogeneous film and shape of diffraction spots was analyzed. The examples showed that XRD studies of stresses in thin films at certain cases require also specific methods of measurement and evaluation and important (even dominant) features can easily be overlooked when routine methods are applied only. |
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11:40 AM |
TS4-1-6 Information Depth of Mono-Atomic and Poly-Atomic Primary Ions in Secondary Ion Mass Spectrometry (SIMS): Fundamentals and Applications
Felix Kollmer (ION-TOF GmbH, Germany); Daniel Breitenstein (Tascon GmbH, Germany); Nathan Havercroft (ION-TOF USA, Inc.); Philipp Bruener (ION-TOF GmbH, Germany); Michael Fartmann, Birgit Hagenhoff (Tascon GmbH, Germany); Ewald Niehuis (ION-TOF GmbH, Germany); Albert Schnieders (ION-TOF USA, Inc.) TOF-SIMS is a very sensitive surface analytical technique, covering a wide range of organic and inorganic applications. It provides detailed elemental and molecular information about surfaces, thin layers, interfaces, and full three-dimensional analysis of the sample. In recent years, the application of cluster primary ions has led to a major breakthrough in the analysis of molecular surfaces by TOF-SIMS. Compared to mono-atomic bombardment the accessible mass range has been considerably extended and the sensitivity has been increased by orders of magnitude. In particular the Bi LMIS cluster source combines the fundamental benefits of cluster ion bombardment with a high brightness source to give uncompromised lateral and mass resolution. Moreover, the Bi cluster source emits a large variety of singly and doubly charged clusters and is therefore well suited for fundamental studies.
The information depth is a key capability of every surface analytical technique. However, the influence of cluster bombardment on the information depth in SIMS has hardly been investigated. We determined the information depth for atomic Bi as well as for a large variety of Bi clusters (Bi2 to Bi7) at different primary ion energies. Additionally, we investigated the samples by LEIS (low energy ion scattering) which is known to be the most surface sensitive technique. The samples under investigation included different core shell nano-particles as well as special alloys which tend to form pure mono-layers of one metal component at the surface. |
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12:00 PM |
TS4-1-7 XPS on Ar Atoms to Determine Local Structures of Thin Films Prepared by Magnetron Sputtering and PECVD
Atena Rastgoo Lahrood, Teresa de los Arcos, Marina Prenzel, Jörg Winter (Ruhr-Universität Bochum, Germany) X-ray Photoelectron Spectroscopy (XPS) is commonly used technique for elemental near-surface analysis of the composition of materials and of their chemical binding. In this study we investigate the potential of XPS to gain structural information on thin films. It has been observed by XPS studies on Ar atoms (Ar 2p), naturally trapped in Al2O3 films deposited by RF magnetron sputtering, that the line shape has to be described as a superposition of at least two doublets. A doublet structure and the associated energy shift has been correlated in earlier work on pure metals with the existence of bubbles formed by coalescing noble gas atoms in the solid [1, 2]. In other works the shift of Ar 2p peaks has been used as a probe of residual stress in amorphous carbon ultrathin films [3]. In order to systematically study this effect we have implanted Ar atoms at various energies into different substrates: pure Al, Al2O3 deposited by RF magnetron sputtering, DLC (diamond-like carbon), Si single crystals and SiO2. In the case of Al2O3 the naturally trapped Ar from the deposition process were also measured. The doublets of 2p transitions of Ar have been analyzed by XPS. The line shape shows that in many cases more than one doublet structure is needed to describe the data. The relative intensities of these doublets change as a function of implantation energy and annealing temperature. There is evidence that a correlation of the local structure of the sample with the shape and shift of Ar 2p Peaks exists, making XPS on Ar a probe for the local structure of the dielectric thin films investigated in this study. The work is funded by DFG within SFB-TR 87. [1] C. Biswas, A. K. Shukla, S. Banik, S. R. Barman, Phys. Rev. Lett. 92 (2004) 115506. [2] P.H. Citrin, D.R. Hamann, Phys. Rev. B 10 (1974) 4948. [3] W. Lu, K. Komvopoulos, Appl. Phys. Lett. 76 (2000) 3206. |