time | lecturer, title and abstract |
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HEA workshop, dedicated to the 65th anniversary of Prof. Janez Dolinšek | |
13:00 | Ante Bilušić, Julian Ledieu, Magdalena Wencka: opening |
13:15 |
Sheng GuoEutectic High-Entropy Alloys & Refractory High-Entropy Alloys: Opportunities and ChallengesThe alloying concept of high entropy alloys (HEAs) opens a vast unexplored compositional space potentially leading to numerous new materials and new applications, but also brings new challenges on how to design these alloys properly. In this lecture, I will show opportunities and challenges that are brought by two particular examples of HEAs, refractory HEAs and eutectic HEAs. Refractory HEAs are promising candidates for ultra-high temperature applications, but how to satisfy demanding material requirements to simultaneously obtain decent room-temperature ductility, high-temperature strength and oxidation resistance pose a formidable scientific challenge. Eutectic HEAs, recently becoming prototype dual-phase materials, show a wide spectrum of mechanical properties when they are subject to thermomechanical treatments, while their good castability and decent mechanical properties and corrosion resistance render great application potential where directly cast materials are in need. |
Session 1: Structure and surfaces Chair person: Sheng Guo |
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14:00 |
Anton MedenPhase Identification and Quantification in High Entropy Alloys Using X-Ray Powder DiffractionIdeally, high entropy alloys (HEA) are single phase with randomly mixed atoms of the constituent elements at crystallographic sites of a (simple) crystal structure. In such cases, X-ray powder diffraction (XRPD) is an efficient tool to: 1. prove the phase purity, 2. determine the structure type, 3. determine the exact parameters of the unit cell, 4. estimate the size and strain of the coherently scattering domains.Often HEAs are (complex) multiphase mixtures, and in such cases the XRPD is an essential tool for phase identification and quantification. For the identified phases, points 2 and 3 above also apply, point 4 is only possible for predominant phases. The reliability of the results is greatly increased when XRPD methods are used together with scanning electron microscopy techniques (SEM) (BSE imaging and EDS grain analysis). The above is illustrated with examples (as in Fig. 1). |
14:30 |
Marc ArmbrűsterHEAs in Catalysis - An OverviewHigh-entropy alloys are an interesting new class of materials and their physical and chemical properties are momentarily explored. For heterogeneous catalysis the randomly occupied crystallographic sites are principally offering a nearly endless variety of potentially active sites. This opens the possibility that there are active sites available for every heterogeneously catalysed reaction resulting in “general“ catalysts.This resulted in tests of HEAs in a number of catalytic reactions. Publications in the field will be presented and critically analysed concerning the phases present and evaluation of the catalytic properties. In addition, a brief outlook on the potential of HEAs in heterogeneous catalysis will be presented. |
15:00 |
Andreja JelenMulti-phase structure of AlCoFeNiCux (x = 0.6 - 3.0) HEAsTailoring of new materials is a playground for many scientists. Searching for a material that possesses a combination of excellent magnetic softness and vanishing magnetostriction has led us to investigate the ferromagnetic high-entropy alloy (HEA) system AlCoFeNiCux (x = 0.6 – 3.0). The alloys develop multi-phase (up to three phases) composite microstructure that is further nanostructured on the 10-nm scale. One of them (x = 3) is presented at the micro-level in Fig.1 by SEM EDS elemental maps. |
15:20 | Coffee break (birthday cake & more…) |
Session 2: Physical properties Chair person: Peter Gille |
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16:20 |
Jože LuzarAlCoFeNiCux (x = 0.6 – 3.0) zero-magnetostriction magnetically soft high-entropy alloysThis contribution [1] will present our efforts in further advancing soft ferromagnetic high-entropy alloys towards practical magnetic applications via a study of the AlCoFeNiCux (x = 0.6 – 3.0) system. AlCoFeNiCu2.0 proved to have superior magnetostriction and magnetic softness properties. It shows precisely zero magnetostriction, λs = 0, reasonably low coercivity Hc ≈ 650 Am–1 and substantial saturation magnetic polarization of Js ≈ 0.55 T. Near zero magnetostriction was also observed for x = 2.5 and 3.0, so that AlCoFeNiCux HEAs for x = 2.0 – 3.0 are all relevant for applications as supersilent (inaudible to a human ear) materials. In the alloys, three phases develop on the microscale and are further nanostructured on the 10-nm scale. It is considered that the ideal zero magnetostriction in the AlCoFeNiCu2.0 alloy is a consequence of the three-phase microstructure, in which the magnetostrictions of different signs in the three phases exactly compensate each other. The magnetic softness of the HEAs is attributed to the mechanism of exchange-averaging of magnetic anisotropy.Reference: [1] J. Luzar, P. Priputen, S. Vrtnik, et al., Adv. Mater. Interfaces. Available online prior to inclusion in an issue: https://doi.org/10.1002/admi.202201535 |
16:40 |
Primož Koželj
High-entropy alloys can be viewed as materials that are half way between ordered crystals and amorphous substances – they exhibit a topologically ordered lattice but on the other hand also an immense amorphous-type chemical disorder. This contribution will present our efforts [1] at determining the importance of the crystal lattice vs the importance of the disorder on the electronic transport in HEAs through a comparative study of a 6 component Al0.5TiZrPdCuNi synthesized in either high-entropy alloy (HEA) or metallic glass (MG) form.
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Round table discussion and closing Chair person: Magdalena Wencka |
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17:00 | Trends in development of high-entropy alloys |
17:20 | Janez Dolinšek, Julian Ledieu: closing |
time | lecturer, title and abstract |
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8:50 | opening |
Chair person: Ana Smontara, Zagreb | |
9:00 |
Emil Babić, Zagreb
Despite a huge expansion of research on compositionally complex alloys, CCA (such as the entropy alloys, HEA and the corresponding glassy alloys) their comprehension is still limited, which is detrimental both for the design of CCAs and for their application. The broad compositional range in CCAs enables simple tuning of their properties by varying the contents of their constituent elements. Accordingly, the study of transition from CCA to conventional alloy, CA composed from the same constituents is important, both for understanding the formation of solid solutions in CCAs and for proper evaluation of their potential with respect to that of CAs. However, this transition has so far been studied systematically in only two types of alloys: isopleths of the Cantor alloy and glassy TiZrNbCuNi/Co alloys with variable Co, Ni or Cu content (Materials 14 (2021) 5824 and ref. therein). In both alloy systems the variation of a given property with composition depends sharply on the selected principal component and can be either monotonic (like that in the ideal solid solution) or non-monotonic. When the variation is non-monotonic, the maximum value of the selected property is usually outside of HEA composition range.
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9:30 |
Farid Labib, Tokyo
This study reports the first observation of ferromagnetic (FM) order in the non-Au-based approximant crystals (ACs) using a novel approach whereby a total electron-per-atom (e/a) ratio of the spin-glass Ga |
9:50 |
Mario Novak, Zagreb
We shall present a unique approach to test the signature of the nodal-line physics by thermodynamic methods. By measuring magnetic susceptibility in ZrSiS we found an intriguing temperature-driven crossover from dia- to paramagnetic behavior. We show that the anomalous behavior represents a real thermodynamic signature of the underlying nodal-line physics through the means o chemical pressure (isovalent substitution of Zr for Hf), quantum oscillations, and theoretical model ng. The anomalous part of the susceptibility is orbital by nature, and it arises due to the vicinity of the Fermi level to a degeneracy point created by the crossing of two nodal lines.
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10:10 |
Neveen Singh Dhami, Zagreb
Intermetallic EuTX3 (T: transition metal, X= Si/Ge) forms a non-centrosymmetric BaNiSn3-type structure and has been attracting considerable attention due to complex magnetic structures and unique pressure phase diagram that potentially accommodates superconductivity under pressure [1, 2]. At ambient pressure, EuTGe3 series host divalent Eu ions (4f7, J=7/2) and exhibit antiferromagnetic ordering at low temperature (< 15 K), while the ordering direction depends on the selection of T [1]. We studied the pressure evolution of the electronic and crystal structures of EuTGe3 (T= Co, Rh, Ir) by high-resolution x-ray absorption spectroscopy and powder x-ray diffraction. Our study unveiled that the pressure gradient of the Eu valence change varies depending on T. By applying pressure, a continuous contraction of the lattice volume was observed in both EuCoGe3 and EuRhGe3. EuIrGe3 implied possible structural transition above 34 GPa.
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10:30 | Coffee break |
Chair person: Janez Dolinšek, Ljubljana | |
11:00 |
Holger Schwarz, Chemnitz
Multicomponent alloys of at least four elements with near equimolar percentage were first reported and investigated by Cantor et al.[1] and Yeh et al.[2] in 2004 and are nowadays often referred to as High-Entropy Alloys (HEAs). This composition is expected to support the formation of single-phase solid solutions, which lead to extensive research on the mechanical properties of HEAs in the past decades, but surface physics are barely investigated so far. We demonstrate the formation of crystalline thin films of CoCrFeNi via magnetron sputtering from homemade targets on MgO (100) and Al2O3 (0001) single crystal substrates. Following a proper UHV surface treatment, the structural and electronic behaviour is accessible by means of low energy electron diffraction and angle resolved photoelectron spectroscopy.
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11:20 |
Priyanka Reddy, Zagreb
Despite exceptional scientific efforts over several decades, there is almost no universal agreement about the superconducting state of cuprate compounds. A constructive way to improve understanding would be to synthesize and investigate a new system, which displays superior crystal chemical flexibility and tunability of the valence of the transition metal ions. One could then manipulate its various electronic, metallic, and mechanical properties. Here we study Murunskite, which interpolates between cuprates and pnictides[1]. In this presentation, I will present the successful growth and characterization of the first-ever high-quality Murunskite single crystals. These crystals show semiconducting behaviour in resistivity and optical transmittance, and antiferromagnetic ordering around 100 K. Spectroscopy (XPS) and Density Functional Theory (DFT) calculations concur that the sulfur 3p orbitals are partially open, making them accessible for charge manipulation, which is a prerequisite for superconductivity in analogous layered structures. Furthermore, DFT indicates that the valence band is more cuprate-like, while the conduction band is more pnictide-like. We also managed to electron-dope the parent compound, whose transport and optical conductivity measurements will be discussed in the presentation.
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11:40 |
Josipa Šćurla, Split
The organo-metallic photovoltaic (PV) perovskite (CH3NH3PbI3) has reached more than 25% conversion efficiency (in single junction configuration [1]), which suggests its imminent commercialization. Before public usage its health hazard needs to be adressed because of the lead in the formula. We have examined in-vivo toxicity of two types of PV perovskites; CH3NH3PbI3 and its possibly less toxic sister compound CH |
12:00 |
Željana Bonačić Lošić, Split
We study the coupling between plasmon modes due to the long-range Coulomb electron–electron interaction for a composite system consisting of a two-dimensional system of Dirac electrons placed in three-dimensional Dirac semimetal [1]. The mixing of the collective plasmon modes is obtained as the two-dimensional acoustic plasmon mode dispersion crosses the bulk plasmon mode. We show that the coupled plasmon modes become more separated with decreasing spacing between the two subsystems as the coupling increases due to the enhanced Coulomb interaction between electrons from different subsystems. We also investigate the effects of the Dirac cone tilts and anisotropies on coupled plasmon modes in both subsystems and find that they increase the coupled plasmon mode energies and renormalize their spectral weights [2]. The anisotropic effects of tilts are more significant for the larger separations of the subsystems when the Coulomb coupling is weaker.
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12:20 |
Marc de Boissieu, Grenoble
The lattice thermal conductivity of many aperiodic crystals displays a ‘glass like behavior’ [1], with a relatively small value of the lattice thermal conductivity at ambient temperature and an almost independent temperature dependence in the range 20 to 300 K. The Umklapp peak observed in simple structure is largely suppressed. This is true for instance for the icosahedral quasicrystal i-AlPdMn [2], but also for the Rb2ZnCl4 phase that displays an incommensurately modulated phase between 190 and 300 K [3]. The detailed understanding of this behavior is still a matter of debate.
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12:40 | Lunch |
Chair person: Janusz Tobola, Kraków | |
14:30 |
Silke Bühler Paschen, Vienna
Complexity has many faces, one of them being strongly correlated ternary intermetallic compounds that are further enriched by nontrivial electronic topology. I will provide an overview of the recent activities of the Quantum Materials group at TU Wien in this emerging field. They range from investigations of the first Weyl-Kondo semimetal Ce3Bi4Pd3 [1] and its relatives, to the exploration of topological phases and topological phase transitions by tuning [2], and the search for new topological phases by exploiting crystal symmetries [3] and quantum fluctuations [4].
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15:00 |
Gaku Eguchi, Vienna
The past decade has seen a wealth of investigations on materials that are considered as topological semimetals and insulators. In the by far best studied regime of noninteracting or weakly interacting topological materials, key characterization tools are ARPES and quantum oscillation experiments together with density functional theory. In the recently evidenced strong correlation regime, by contrast, these tools fail and new ones have been put forward, with specific heat measurements being one of them [1-4].
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15:20 |
Shovan Dan, Wrocław
In recent years, rare-earth-based half-Heusler (HH) pnictides have gained tremendous attention due to a range of non-trivial physical properties that have opened the door to various applications, such as in spintronics, green energy harvesting or quantum computing. Although many HH phases have been investigated in depth, some are still poorly characterized.
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15:40 |
Karan Singh, Wrocław
Manipulation of charge transport by spin degrees of freedom has attracted a great interest in topological materials because of their exotic fundamental physics and potential applications. In this context, the compounds EuCd2As2 and EuZn2As2 gained special attention [1,2].
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16:00 | Coffee break |
Chair person: Silke Bühler Paschen, Vienna | |
16:30 |
Petar Popčević, Zagreb
2H-NbS2 is superconducting, quasi 2D system, which can host different ions and molecules in van der Waals gaps between metallic layers. When intercalated with transition metal (TM) ions system becomes magnetic. The coexistence of metallic and magnetic degrees of freedom coupled with reduced dimensionality and anticipated frustration renders these compounds battlefield of different interactions resulting in different magnetically ordered ground states.
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16:50 |
Eteri Svanidze, Dresden
Mercury, in both elemental form and as part of compounds and amalgams has played an important role in solid-state chemistry and condensed matter physics [1-3]. However, much care must be taken both during synthesis as well as during characterization of this peculiar element and its compounds – from toxicity concerns to high chemical reactivity – these systems pose several experimental challenges. In this talk, I will showcase that, nonetheless, mercury-based materials offer unique crystallographic motifs and, as a result, peculiar physical properties [4-6]. In particular, I will concentrate on the binary compounds of mercury and lanthanide as well as actinide elements, which have so far been under investigated. Using a unique laboratory environment, we are able to synthesize single crystals of several binary phases (Figure 1) and study their chemical and physical properties in detail. By looking at the evolution of crystallographic complexity across several series of compounds, I will discuss how intrinsic crystal chemistry affects the resultant ground states
References: |
17:10 |
Mitja Krnel, Dresden
Although typically, the lack of translational symmetry prohibits the appearance of superconductivity, the coexistence of the latter with structural disorder has been observed in some materials [1-3]. However the influence of structural disorder on superconductivity is not yet fully understood. Hg-based materials often have complex crystallographic arrangements making them candidates for interesting physical properties. A detailed examination of crystallographic and physical properties of LaHg6.4 [4] reveals that this material has a transition to a superconducting state at Tc = 2.4 K while showing crystallographic disorder in one dimension. We were able to determine in detail the structure type of Lanthanum mercuride (space group Cmcm, a = 9.779(2) Å, b = 28.891(4) Å, c = 5.0012(8) Å, Z = 8), which has remained out of reach for nearly 50 years. In this crystal structure, strong disorder is present in the channels that propagate along the [001] direction. By using a combination of specific synthesis and characterization techniques, we were able to avoid the problems associated with the low formation temperature and chemical reactivity of this substance, thus making it possible to study the physical properties of LaHg6.4.
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17:30 |
Diana Kirschbaum, Vienna
The interplay of nontrivial electronic topology and strong correlations can lead to the realization of entirely new quantum phases, and thus is of great current interest. A prime example is the newly discovered Weyl-Kondo semimetal phase realized in Ce3Bi4Pd3 [1-3]. There, a cubic-in-temperature contribution to the electronic specific heat [1] and a giant spontaneous Hall response [3] are attributed to the presence of Weyl nodes in the immediate vicinity of the Fermi energy. Another candidate material theoretically predicted to host Weyl points near EF is the tetragonal, noncentrosymmetric Kondo semimetal CeRu4Sn6 [4]. The recent discovery that CeRu4Sn6 is quantum critical without tuning [5], makes it a unique platform to study the possible role of quantum criticality in the formation mechanism of Weyl-Kondo semimetals. Here we probe the phase diagram of CeRu4Sn6 by means of electrical transport and specific heat measurements under hydrostatic pressure and discuss evidence for Weyl-Kondo physics emerging at finite pressure.
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17:50 | Poster session |
19:30 | EB meeting |
time | lecturer, title and abstract |
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Chair person: Peter Gille, München | |
9:00 |
Yuri Grin, Dresden
A common strategy to describe CMA from a geometric point of view is the grouping of atoms into local atomic arrange-ments (crystallographic clusters), which makes the crystal structure easier to visualize, to perceive and understand the geometric organisation; it reduces the degree of complexity and allows to relate the CMA to simpler crystal structures. This is the nested-polyhedra units approach, which was introduced first for the description of the γ–brass-derived structures. The choice of a crystallographic cluster is considered as reasonable, if its shells are as spherical as possible and are quite separate with respect to the distances between the shells and with respect to the centre of the nested polyhedrons. On the other hand, the so defined crystallographic clusters are not in agreement with the chemical definition of such an entity, as the chemical definition entails atomic interactions within the chemical clusters that are stronger than the interaction of the clusters with neighbouring aggregates, would be preferable, thus raising the question about the stabilization mechanisms for these structural. Quantum chemical investigations of chemical bonding in CMA are naturally hindered by the huge size of the unit cells and inherent disorder. In particular, the role of the charge transfer in the stabilization was studied on example of the CMA Mg29-xPt4+y [1] in comparison with Be21Pt5 [2], and their chemically analogous but non-complex Be5Pt [3].
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9:30 |
Marc Armbrüster, Chemnitz
Changing our energy supply towards a renewable and sustainable energy scenario requires storage and transport of large amounts of renewable energy. Due to their high chemical storage capacity for hydrogen, small molecules like CH4, NH3 or methanol are promising candidates. Methanol is liquid at normal conditions and possesses a high volumetric and gravimetric energy density.[1] To release the hydrogen on demand, methanol steam reforming can be applied (CH3OH + H2O › 3 H2 + CO2). Since the identification of ZnPd/ZnO as highly selective catalyst[2], it could be shown that high selectivity is achieved only if ZnPd and ZnO are present[3]. While the necessity could be shown, it is still unclear how the phases contribute to the catalytic cycle.
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9:50 |
Oytun Tiryaki, Chemnitz
ZnPd-based catalysts for methanol steam reforming (MSR) have superior stability without being pyrophoric and possess comparable CO2 selectivity (about 99%) to commercial Cu-based catalysts[1-3]. As of now, supported ZnPd/ZnO systems have addressed the impact of ZnPd-particle size on the catalytic characteristics in MSR. However, no conclusive evidence was obtained regarding how the particle size affects the catalytic properties of ZnPd/ZnO in MSR[2,4,5]. To simplify the materials, unsupported ZnPd with different crystallite sizes have been successfully synthesized via electroless plating without the use of surfactants. These materials enable to address the size influence on the catalytic properties in methanol steam reforming without the influence of the supporting ZnO. Characterization after catalysis revealed that the smaller starting particles showed more severe sintering which turned the sample into the larger sized particles, which might be the reason for the inconclusive results described in literature.
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10:10 |
Fatma Aras, Dresden
Oxygen evolution reaction (OER) is the slowest step of water electrolysis, demanding an active electrocatalyst, that should be also stable under strong oxidative conditions of OER. With the help of (partially) ordered crystal structures and well-defined electronic states of the elements in these compounds, intermetallic compounds possess an interesting class of materials for electrocatalysis. [1] The binary compounds in Mo-Ni and Mo-B systems were extensively studied as electrocatalysts for the hydrogen evolution reaction (HER). [2-4] In present study, intermetallic compounds Mo2TMB2 (TM: Fe, Co, Ni) were extensively investigated under conditions of OER in alkaline media.
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10:30 | Coffee break |
Chair person: Émilie Gaudry, Nancy | |
11:00 |
Hem Raj Sharma, Liverpool
We present the recent studies of surface structures and chemical properties of Ga3Ni2 and In3Ni2 intermetallic catalysts by various surface science techniques, namely, x-ray photoelectron spectroscopy (XPS), low energy electron diffraction (LEED), and scanning tunneling microscopy (STM).
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11:20 |
Alexis Front, Nancy
At the nanoscale, materials exhibit unique properties that differ greatly from those of the bulk state. In this context, atomic arrangments of nanoalloys must be perfectly characterized in order to master and tune physical-chemistry properties. Transition metal based nanoalloys have been extensively investigated both experimentally and theoretically [1]. However the search of sustainable materials imposes to go beyond. Intermetallic nanoalloys may be a key. In-Pd nanoalloys have been synthesized mainly for their unique catalytic properties [2-3]. The main bottleneck in the development of intermetallic nanoalloys is the lack of structural characterization.
We have adopted a multiscale approach using DFT calculations and atomistic modelling to investigate structural stability as a function of sizes and compositions of In-Pd nanoalloys. Equilibrum crystalline shapes have been determined with the Wulff theorem and compare to other structures. The most stable nanoparticles are those chemically ordered showing a Wulff shape (Fig. 1). Disordered nanoparticles are less stable and become amorphous when the concentration of In increases.
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11:40 |
Thiago Trevizam Dorini, Nancy
The formation of complex oxide structures is possible when two-dimensional (2D) oxide materials are grown on intermetallic single crystal substrates [1]. Modelling such phases using Density Functional Theory (DFT) computations is a challenging task. It has been shown for recently discovered ultrathin quasicrystal structures that methods of tiling, using particular atomic decorations for the tiles, can be used to develop such models [2]. Crystal structures of two-dimensional materials may also be predicted with great accuracy by evolutionary algorithms [3].
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12:00 |
Oscar Shedwick, Livrepool
Ga3Ni2 has been reported as a potential heterogeneous catalyst in the hydrogenation of CO into methanol at atmospheric pressure [1]. Understanding the surface of a catalyst is paramount to get insight to the chemical processes [2].
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12:40 | Lunch |
Chair person: Ronan McGrath, Liverpool | |
14:30 |
Marek Mihalkovič, Bratislava
Diamond and clathrate structures can form coherent, sp3-bonded interface stable against annealing at temperatures approaching melting point of the constituents, and bearing over 15% tensile deformation in ab-initio model simulations. Bonding between the two structures occurs via common transitional layer known as 3×3 dimer-stacking fault (DS) reconstruction on the diamond side, matching a layer with identical geometry found in clathrate type II or III. The uniform-chemistry interface ∼10% mismatch can be eliminated by tuning composition of one or both constituent structures. Appropriate diamond-structure support can be used to grow new metastable clathrate compositions.
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15:00 |
Émilie Gaudry, Nancy
Interfaces are known to play an important role in a broad range of scientific and technological fields. Their design is crucial to improve the performances of heterostructures. In metallurgy, aluminized steel combines the low weight of aluminium with the high strength of steel. But the distinct thermal and physical properties of Al and Fe metals make it challenging to join. Buffer layers made of Al-Fe intermetallic compounds generally forms at the interface. Their nature depends on the chemical potentials, the nucleation conditions and the mobilities of the elements.
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15:20 |
Wilfried Bajoun Mbajoun, Nancy
RE-Au-Si (RE=Gd,Tb,Ho) Tsai-type 1/1 approximants structures are built from a specific cluster type where the central disordered tetrahedron can be partially or totally replaced by a RE atom leading to alteration of magnetic and thermoelectric properties[1].
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15:40 |
Vincent Fournée, Nancy
Ferromagnetic shape memory (FSM) Heusler compounds are a class of “smart materials”, i.e. materials with multifunctional properties that can be activated through an external stimulus [1]. The prototype of FSM Heuslers is the Ni2MnGa intermetallic, because it shows the largest magnetic shape memory effect obtained so far. The key point at the heart of these externally driven physical changes and multifunctionality is a reversible martensitic transformation combined with a strong magnetostructural coupling. Here we report first results on the surface of an epitaxial Ni-Mn-Ga thin film grown on MgO(001) by RF sputtering technique at elevated temperature (623K) [2]. We use scanning tunneling microscopy (STM) imaging and low-energy electron diffraction (LEED) to study the structural and microstructural changes occuring across the phase transition between the high temperature austenite with L21 structure and the low temperature martensite with seven-fold modulated monoclinic structure (Fig.1).
References: |
16:00 | Coffee break |
Chair person: Eteri Svanidze, Dresden | |
16:30 |
Janusz Tobola, Kraków
The efficiency of materials converting various forms of energy due to thermoelectric or electrochemical effects is partly related to peculiar electronic properties driving transport and electrochemical behaviors. The KKR-CPA method is implemented for electronic structure calculations to account for disorder in thermoelectric and ion-battery systems. The ab initio results combined with modeling of electron transport and electrochemical properties in selected thermoelectrics [1,2] and Li-/Na-ion batteries [3] are presented. Noteworthy, unusual electronic structure features appearing in these materials, namely band convergence, entropy induced band engineering (thermoelectrics) and specific character of charge/discharge curves correlated with electromotive force (batteries), directly determining their performance. Finally, recent studies of high-entropy oxides for the Na-ion cathode is discussed [4].
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16:50 |
Monika Lužnik, Vienna
Sustainable solutions to our energy crisis are needed more urgently than ever. While not being the answer to all of our problems, thermoelectric materials play an important role in regaining some of the otherwise lost waste heat. Their conversion efficiency is defined by the dimensionless figure of merit ZT = σS2T/κ, with the electrical conductivity σ, the thermopower S, the temperature T and the thermal conductivity κ. Therefore, a good thermoelecttric material should have a high σ and S, but also a low κ. Here we present a size study on type-I clathrates, in which the phonon Kondo effect is held responsible for a flattening of the acoustic phonon modes in a sizable range of momentum space, thereby lowering the phonon thermal conductivity [1]. To scrutinize this picture, we use well-studied single crystals [2, 3] and shape them into nanowires with different diameters using a focused ion beam (FIB) technique. Because in the above picture only long-wavelength phonons carry heat in these materials, the dependence of κ on the diameter should be noticeable. Additionally, we compare the electrical resistivities of the nanowires to get a full picture of how size affects the transport properties of type-I clathrate nanowires.
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17:10 |
Laura Agnarelli, Dresden
During the study of the Be-Ru binary system, the crystal structure of Be2Ru was reinvestigated. Differently from what is reported in literature, Be2Ru crystallizes with hexagonal Fe2P-type structure. The crystal structure can be described as constituted by a substructure of ruthenium atoms arranged within planar layers in the form of condensed six-membered rings in the ab plane. The latter are separated by a layer formed by Be atoms found at half of the c axis’ length of the unit cell, in a ABAB sequence. Analysis of the collected single-crystal data revealed a crystal structure more complicated than expected. In fact, an additional position very close in distance to the Ru1 atom can be recognised. The possibility of a stacking fault in the ab plane was advanced and a TEM investigation was carried out, which confirmed such hypothesis. The calculated electronic density of states (DOS), revealed that, contrary to typical intermetallic compounds, Be2Ru shows a pseudo gap in the vicinity of the Fermi level. The temperature dependence of the electrical resistivity of Be2Ru, shows metallic behaviour in agreement with the non-zero DOS at the Fermi level.
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17:30 | Concluding remarks |
19:30 | Conference dinner |
time | event |
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8:15 | Science Board Meeting |
10:15 | Break |
10:30 - 12:00 | Governing Board Meeting and General Assembly |
13:00 - 17:00 |
Katarzyna Gliszczyńska
During our workshop we will use a design-driven innovation approach to touch issues to learn, experience, practice, ask, answer and discuss what follows:
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