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Featured researches published by R. Hillebrand.


Journal of Applied Physics | 2003

Perfect two-dimensional porous alumina photonic crystals with duplex oxide layers

Jinsub Choi; Yun Luo; Ralf B. Wehrspohn; R. Hillebrand; J. Schilling; Ulrich Gösele

A perfect two-dimensional porous alumina photonic crystal with 500 nm interpore distance was fabricated on an area of 4 cm2 via imprint methods and subsequent electrochemical anodization. By comparing measured reflectivity with theory, the refractive indices in the oxide layers were determined. The results indicate that the porous alumina structure is composed of a duplex oxide layer: an inner oxide layer consisting of pure alumina oxide of 50 nm in thickness, and an outer oxide layer of a nonuniform refractive index. We suggest that the nonuniform refractive index of the outer oxide arises from an inhomogeneous distribution of anion species concentrated in the intermediate part of the outer oxide.


ACS Nano | 2008

Self-ordered anodic aluminum oxide formed by H2SO4 hard anodization.

Kathrin Schwirn; Woo Y. Lee; R. Hillebrand; Martin Steinhart; Kornelius Nielsch; Ulrich Gösele

The self-ordering of nanoporous anodic aluminum oxide (AAO) in the course of the hard anodization (HA) of aluminum in sulfuric acid (H2SO4) solutions at anodization voltages ranging from 27 to 80 V was investigated. Direct H2SO4-HA yielded AAOs with hexagonal pore arrays having interpore distances D(int) ranging from 72 to 145 nm. However, the AAOs were mechanically unstable and cracks formed along the cell boundaries. Therefore, we modified the anodization procedure previously employed for oxalic acid HA (H2C2O4-HA) to suppress the development of cracks and to fabricate mechanically robust AAO films with D(int) values ranging from 78 to 114 nm. Image analyses based on scanning electron micrographs revealed that at a given anodization voltage the self-ordering of nanopores as well as D(int) depend on the current density (i.e., the electric field strength at the bottoms of the pores). Moreover, periodic oscillations of the pore diameter formed at anodization voltages in the range from 27 to 32 V, which are reminiscent of structures originating from the spontaneous growth of periodic fluctuations, such as topologies resulting from Rayleigh instabilities.


Nature Communications | 2016

Superconductivity in Weyl semimetal candidate MoTe2

Yanpeng Qi; Pavel G. Naumov; Mazhar N. Ali; Catherine R. Rajamathi; Walter Schnelle; Oleg Barkalov; Michael Hanfland; Shu-Chun Wu; Chandra Shekhar; Yan Sun; Vicky Süß; Marcus Schmidt; Ulrich Schwarz; Eckhard Pippel; P. Werner; R. Hillebrand; Tobias Förster; Erik Kampert; Stuart S. P. Parkin; R. J. Cava; Claudia Felser; Binghai Yan; Sergey A. Medvedev

Transition metal dichalcogenides have attracted research interest over the last few decades due to their interesting structural chemistry, unusual electronic properties, rich intercalation chemistry and wide spectrum of potential applications. Despite the fact that the majority of related research focuses on semiconducting transition-metal dichalcogenides (for example, MoS2), recently discovered unexpected properties of WTe2 are provoking strong interest in semimetallic transition metal dichalcogenides featuring large magnetoresistance, pressure-driven superconductivity and Weyl semimetal states. We investigate the sister compound of WTe2, MoTe2, predicted to be a Weyl semimetal and a quantum spin Hall insulator in bulk and monolayer form, respectively. We find that bulk MoTe2 exhibits superconductivity with a transition temperature of 0.10 K. Application of external pressure dramatically enhances the transition temperature up to maximum value of 8.2 K at 11.7 GPa. The observed dome-shaped superconductivity phase diagram provides insights into the interplay between superconductivity and topological physics.


Applied Physics Letters | 2005

Three-Dimensional Macroporous Silicon Photonic Crystal with Large Photonic Band Gap

Joerg Schilling; Jeffrey O. White; Axel Scherer; Gary W. Stupian; R. Hillebrand; U. Gösele

Three-dimensional photonic crystals based on macroporous silicon are fabricated by photoelectrochemical etching and subsequent focused-ion-beam drilling. Reflection measurements show a high reflection in the range of the stopgap and indicate the spectral position of the complete photonic band gap. The onset of diffraction which might influence the measurement is discussed.


Journal of Optics | 2001

A model system for two-dimensional and three-dimensional photonic crystals: macroporous silicon

J. Schilling; Ralf B. Wehrspohn; Albert Birner; Frank Müller; R. Hillebrand; Ulrich Gösele; S. W. Leonard; J. P. Mondia; F. Genereux; H. M. van Driel; P. Kramper; Vahid Sandoghdar; Kurt Busch

A review of the optical properties of two-dimensional and three-dimensional photonic crystals based on macroporous silicon is given. As macroporous silicon provides structures with aspect ratios exceeding 100, it can be considered to be an ideal two-dimensional photonic crystal. Most of the features of the photonic dispersion relation have been experimentally determined and were compared to theoretical calculations. This includes transmission and reflection of finite and bulk photonic crystals and their variation with the pore radius to determine the gap map. All measurements have been carried out for both polarizations separately since they decouple in two-dimensional photonic crystals. Moreover, by inhibiting the growth of selected pores, point and line defects were realized and the corresponding high-Q microcavity resonances as well as waveguiding properties were studied via transmission. The tunability of the bandgap was demonstrated by changing the refractive index inside the pores caused by an infiltrated liquid crystal undergoing a temperature-induced phase transition. Finally different realizations of three-dimensional photonic crystals using macroporous silicon are discussed. In all cases an excellent agreement between experimental results and theory is observed.


ACS Nano | 2008

Quantitative analysis of the grain morphology in self-assembled hexagonal lattices.

R. Hillebrand; Frank A. Müller; Kathrin Schwirn; Woo Lee; Martin Steinhart

We present a methodology for the analysis of the grain morphology of self-ordered hexagonal lattices and for the quantitative comparison of the quality of their grain ordering based on the distances between nearest neighbors and their angular order. Two approaches to grain identification and evaluation are introduced: (i) color coding the relative angular orientation of hexagons containing a central entity and its six nearest neighbors, and (ii) incorporating triangles comprising three nearest neighbors into grains or repelling them from grains based on deviations of the side lengths and the internal angles of the triangles from those of an ideal equilateral triangle. A spreading algorithm with tolerance parameters allows single grains to be identified, which can thus be ranked according to their size. Hence, grain size distributions are accessible. For the practical evaluation of micrographs displaying self-ordered structures, we suggest using the size of the largest identified grain as a quality measure. Quantitative analyses of grain morphologies are key to the systematic and rational optimization of the fabrication of self-assembled materials.


Langmuir | 2008

Adsorption hysteresis in self-ordered nanoporous alumina.

L. Bruschi; Giovanni Fois; Giampaolo Mistura; Kornelia Sklarek; R. Hillebrand; Martin Steinhart; Ulrich Gösele

We performed systematic adsorption studies using self-ordered nanoporous anodic aluminum oxide (AAO) in an extended range of mean pore diameters and with different pore topologies. These matrices were characterized by straight cylindrical pores having a narrow pore size distribution and no interconnections. Pronounced hysteresis loops between adsorption and desorption cycles were observed even in the case of pores closed at one end. These results are in contrast with macroscopic theoretical models and detailed numerical simulations of the adsorption in a single pore. Extensive measurements involving adsorption isotherms, reversal curves, and subloops carried out in closed-bottom pores suggest that the pores do not desorb independently from one another.


Optical Materials | 2001

Optical characterisation of 2D macroporous silicon photonic crystals with bandgaps around 3.5 and 1.3 μm

J. Schilling; A. Birner; Frank Müller; Ralf B. Wehrspohn; R. Hillebrand; Ulrich Gösele; Kurt Busch; Sajeev John; S. W. Leonard; H. M. van Driel

Abstract Transmission measurements were performed on thin 2D silicon photonic crystals (PCs) with 1–4 crystal rows in order to investigate the effect of a finite structure and to obtain an estimate of the crystal thickness necessary to minimize crosstalk between adjacent waveguides. For wavelengths deep within the H-bandgap a strong exponential decay revealing an attenuation constant of 10 dB per crystal row was measured. For opto-electronic applications, the lattice constant of macroporous Si was successfully downscaled from a pitch of 1.5 to 0.5 μm. Reflection measurements performed at these structures show good agreement with corresponding bandstructure calculations exhibiting a complete bandgap around λ=1.3 μm .


Nanotechnology | 2006

High-temperature resistant, ordered gold nanoparticle arrays

Danilo Zschech; Dong Ha Kim; Alexey P. Milenin; Sigrid Hopfe; R. Scholz; Petra Göring; R. Hillebrand; Stephan Senz; Craig J. Hawker; Thomas P. Russell; Martin Steinhart; Ulrich Gösele

Ordered gold nanoparticle arrays with high lateral density of 6.87 × 10 10 nanoparticles cm −2 ,w hichare stable up to temperatures of 600 ◦ C, were fabricated. To this end, nanoparticles formed by thermal vacuum evaporation of Au were immobilized within the pores of nanoporous silicon wafers prepared by block copolymer lithography coupled with dry plasma etching. Even after high-temperature treatment the degree of order imposed by the block copolymer template was retained. Optionally, a nanoporous silicon nitride mask can cover the nanoporous silicon.


IEEE Journal of Quantum Electronics | 2002

Silicon-based photonic crystal slabs: two concepts

Cecile Jamois; Ralf B. Wehrspohn; J. Schilling; Frank Müller; R. Hillebrand; W. Hergert

We compare theoretically two different concepts of vertical light confinement in two-dimensional (2-D) silicon photonic crystals. Light guidance obtained by variation of the refractive index in an SiO/sub 2//Si/SiO/sub 2/ sandwich structure leads to a complete bandgap for all directions and polarizations with a gap-midgap ratio of about 8.5% and a bandgap for even modes only of about 27%. The complete bandgap is 50% smaller than for 2-D photonic crystals due to the lower confinement of light in the high-index material silicon and polarization mixing. Light guidance obtained by a vertical variation of the porosity, i.e., pore radius, leads under optimum conditions to a bandgap for even modes only, with a gap-midgap ratio of about 10%. The feasibility of such a structure is shown for macroporous silicon where the pore diameter can be varied with depth. In both cases, the optimum slab thickness can be approximated by classical waveguide optics, reducing the parameter space for optimization.

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Ralf B. Wehrspohn

Martin Luther University of Halle-Wittenberg

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