A. van Houselt

Germanene: the germanium analogue of graphene

Recently, several research groups have reported the growth of germanene, a new member of the graphene family. Germanene is in many aspects very similar to graphene, but in contrast to the planar graphene lattice, the germanene honeycomb lattice is buckled and composed of two vertically displaced sub-lattices. Density functional theory calculations have revealed that free-standing germanene is a 2D Dirac fermion system, i.e. the electrons behave as massless relativistic particles that are described by the Dirac equation, which is the relativistic variant of the Schrödinger equation. Germanene is a very appealing 2D material. The spin-orbit gap in germanene (~24 meV) is much larger than in graphene (<0.05 meV), which makes germanene the ideal candidate to exhibit the quantum spin Hall effect at experimentally accessible temperatures. Additionally, the germanene lattice offers the possibility to open a band gap via for instance an externally applied electrical field, adsorption of foreign atoms or coupling with a substrate. This opening of the band gap paves the way to the realization of germanene based field-effect devices. In this topical review we will (1) address the various methods to synthesize germanene (2) provide a brief overview of the key results that have been obtained by density functional theory calculations and (3) discuss the potential of germanene for future applications as well for fundamentally oriented studies.

Droplet impact on superheated micro-structured surfaces

When a droplet impacts upon a surface heated above the liquids boiling point, the droplet either comes into contact with the surface and boils immediately (contact boiling), or is supported by a developing vapor layer and bounces back (film boiling, or Leidenfrost state). We study the transition between these characteristic behaviors and how it is affected by parameters such as impact velocity, surface temperature, and controlled roughness (i.e., micro-structures fabricated on silicon surfaces). In the film boiling regime, we show that the residence time of droplets impacting upon the surface strongly depends on the drop size. We also show that the maximum spreading factor Γ of droplets in this regime displays a universal scaling behavior Γ [similar] We3/10, which can be explained by taking into account the drag force of the vapor flow under the drop. This argument also leads to predictions for the scaling of film thickness and velocity of the vapor shooting out of the gap between the drop and the surface. In the contact boiling regime, we show that the structured surfaces induce the formation of vertical liquid jets during the spreading stage of impacting droplets

Two-dimensional Dirac signature of germanene

The structural and electronic properties of germanene coated Ge 2Pt clusters have been determined by scanning tunneling microscopy and spectroscopy at room temperature. The interior of the germanene sheet exhibits a buckled honeycomb structure with a lattice constant of 4.3 A and a buckling of 0.2 A. The zigzag edges of germanene are reconstructed and display a 4× periodicity. The differential conductivity of the interior of the germanene sheet has a V-shape, which is reminiscent of the density of states of a two-dimensional Dirac system. The minimum of the differential conductivity is located close to the Fermi level and has a non-zero value, which we ascribe to the metallic character of the underlying Ge 2Pt substrate. Near the reconstructed germanene zigzag edges the shape of the differential conductivity changes from a V-shape to a more parabolic-like shape, revealing that the reconstructed germanene zigzag edges do not exhibit a pronounced metallic edge state.

Absence of an evaporation-driven wetting transition on omniphobic surfaces

Surfaces that exhibit contact angles close to 180° for both polar and non-polar solvents are rare. Here we report the fabrication of such “omniphobic” surfaces by photolithography. We investigate their stability against a so-called wetting transition during evaporation of millimetric water droplets by systematically varying the shape and surface roughness of the micropillars on the surface. We show that a low edge curvature of the top of the micropillars strongly delays the transition, while it completely disappears when the surface roughness is increased. We compare these experimental findings with existing models that describe the Cassie–Baxter to Wenzel transition and conclude that new models are needed which include the hurdle of an energy barrier for the wetting transition. Our results reveal that by increasing the roughness of the micropillars we do not affect the apparent equilibrium contact angle of the droplets. The dynamic robustness of the surface is, however, dramatically enhanced by an increase of the surface roughness.

One-step sculpting of silicon microstructures from pilars to needles for water and oil repelling surfaces

Surfaces that repel both water and oil effectively (contact angles > 150°) are rare. Here we detail the microfabrication method of silicon surfaces with such properties. The method is based on careful tuning of the process conditions in a reactive etching protocol. We investigate the influence of SF6, O2 and CHF3 gases during the etching process using the same pitch of a photolithographic mask. Varying the loading conditions during etching, we optimized the conditions to fabricate homogeneous pedestal-like structures. The roughness of the microstructures could also effectively be controlled by tuning the dry plasma etching conditions. The wetting behavior of the resulting microstructures was evaluated in terms of the water and oil contact angles. Excitingly, the surfaces can be engineered from superhydrophobic to omniphobic by variation of the aforementioned predefined parameters

Spatial mapping of the inverse decay length using scanning tunneling microscopy

We present a scanning tunneling spectroscopy technique that allows one to make spatial maps of the characteristic length, i.e., the inverse decay length (), in electron tunneling. The method requires that the tunneling current i and its first and second derivative with distance di/dz and d2i/dz2, respectively, are simultaneously recorded. The derivatives di/dz and d2i/dz2 are recorded using a lock-in technique. A spatial map of provides valuable information on the electronic structure of surfaces, especially in case of semiconductors, nanostructured surfaces and molecules at surfaces. We have coined this spectroscopic technique microscopy.

Controlled damaging and repair of self-organized nanostructures by atom manipulation at room temperature

The possibility of controlled local demolition and repair of the recently discovered self-organized Pt nanowires on Ge(001) surfaces has been explored. These nanowires are composed of Pt dimers, which are found to be rather weakly bound to the underlying substrate. Using this property, we demonstrate the possibility of carrying the constituting dimers of the Pt nanowires from point to point with atomic precision at room temperature. Pt dimers can be picked-up in two configurations: (i) a horizontal configuration at the tip apex, resulting in double tip images and (ii) a configuration where the Pt dimer is attached to the side of the tip apex, resulting in well-defined atomically resolved images.

Physics in one dimension

With modern microelectronics moving towards smaller and smaller length scales on the (sub-) nm scale, quantum effects (apart from band structure and band gaps) have begun to play an increasingly important role. This especially concerns dimensional confinement to 2D (high electron mobility transistors and integer/fractional quantum Hall effect physics, graphene and topological insulators) and 1D (with electrical connections eventually reaching the quantum limit). Recent developments in the above-mentioned areas have revealed that the properties of electron systems become increasingly exotic as one progresses from the 3D case into lower dimensions. As compared to 2D electron systems, much less experimental progress has been achieved in the field of 1D electron systems. The main reason for the lack of experimental results in this field is related to the difficulty of realizing 1D electron systems. Atom chains created in quantum mechanical break junction set-ups are too short to exhibit the typically 1D signatures. As an alternative, atomic chains can be produced on crystal surfaces, either via assembling them one-by-one using a scanning tunnelling microscope or via self-assembly. The drawback of the latter systems is that the atomic chains are not truly 1D since they are coupled to the underlying crystal and sometimes even to the neighbouring chains. In retrospect, this coupling turns out to be an absolute necessity in the experiment since true 1D systems are disordered at any non-zero temperature [1]. The coupling to the crystal and/or neighbouring chains shifts the phase transition, for example, a Peierls instability, to a non-zero temperature and thus allows experiments to be performed in the ordered state. Here, we want to emphasize that the electronic properties of the 1D electron system are fundamentally different from its 2D and 3D counterparts. The Fermi liquid theory, which is applicable to 2D and 3D electron systems, breaks down spectacularly in the 1D case and should be replaced by the Luttinger liquid theory [2, 3]. In 1D electron systems electron–electron interactions play a very prominent role, and one of the most exciting predictions is that the electron loses its identity and separates into two collective excitations of the quantum mechanical many body system: a spinon that carries spin without charge, and a holon that carries the positive charge of a hole without its spin. In this special section, we have attempted to collect a series of papers that gives an impression of the current status of this rapidly evolving field. The first article is a comprehensive review by Kurt Schonhammer that provides the reader with an introduction into the exciting theory of the 1D electron system as well as its mathematical formalism. Acknowledgments We would like to thank the editorial staff of Journal of Physics: Condensed Matter for their help in producing this special section. We hope that it conveys some of the excitement and significance of this rapidly emerging field. References [1]Mermin N D and Wagner H 1966 Phys. Rev. Lett. 17 1133 [2]Haldane F D M 1981 J. Phys. C: Solid State Phys. 14 2585 [3]Voit J 1995 Rep. Prog. Phys. 58 977 Physics in one dimension contents Physics in one dimensionA van Houselt, J Schafer, H J W Zandvliet and R Claessen Physics in one dimension: theoretical concepts for quantum many-body systemsK Schonhammer Local density of states of the one-dimensional spinless fermion modelE Jeckelmann Local spectral properties of Luttinger liquids: scaling versus nonuniversal energy scalesD Schuricht, S Andergassen and V Meden Spin ladders and quantum simulators for Tomonaga–Luttinger liquidsS Ward, P Bouillot, H Ryll, K Kiefer, K W Kramer, Ch Ruegg, C Kollath and T Giamarchi Peierls to superfluid crossover in the one-dimensional, quarter-filled Holstein modelM Hohenadler and F F Assaad Pressure-dependent structural and electronic properties of quasi-one-dimensional (TMTTF)2PF6E Rose, C Loose, J Kortus, A Pashkin, C A Kuntscher, S G Ebbinghaus, M Hanfland, F Lissner, Th Schleid and M Dressel Photoemission spectroscopy and the unusually robust one-dimensional physics of lithium purple bronzeL Dudy, J D Denlinger, J W Allen, F Wang, J He, D Hitchcock, A Sekiyama and S Suga Luttinger liquid behaviour of Li0.9Mo6O17 studied by scanning tunnelling microscopyT Podlich, M Klinke, B Nansseu, M Waelsch, R Bienert, J He, R Jin, D Mandrus and R Matzdorf Mn-silicide nanostructures aligned on massively parallel silicon nano-ribbonsPaola De Padova, Carlo Ottaviani, Fabio Ronci, Stefano Colonna, Bruno Olivieri, Claudio Quaresima, Antonio Cricenti, Maria E Davila, Franz Hennies, Annette Pietzsch, Nina Shariati and Guy Le Lay Iridium silicide nanowires on Si(001) surfacesNuri Oncel and Dylan Nicholls Structure and growth of quasi-one-dimensional YSi2 nanophases on Si(100)V Iancu, P R C Kent, S Hus, H Hu, C G Zeng and H H Weitering Metallic rare-earth silicide nanowires on silicon surfacesMario Dahne and Martina Wanke One-dimensional collective excitations in Ag atomic wires grown on Si(557)U Krieg, C Brand, C Tegenkamp and H Pfnur Interfering Bloch waves in a 1D electron systemR Heimbuch, A van Houselt, M Farmanbar, G Brocks and H J W Zandvliet Au-induced quantum chains on Ge(001)—symmetries, long-range order and the conduction pathC Blumenstein, S Meyer, S Mietke, J Schafer, A Bostwick, E Rotenberg, R Matzdorf and R Claessen