Scientific Highlights

Polarisierte Neutronen beider Spinausrichtungen up (blau) und down (rot) gelangen unter sehr kleinen Einfallswinkeln in eine Probe. Dort werden sie an den im Magnetfeld H ausgerichteten Momenten gestreut, hier dargestellt für eine Grenzfläche. Aus den gemessenen Unterschieden der Winkelabhängigkeit für beide Spinrichtungen lässt sich ein magnetisches Tiefenprofil ableiten.

Magnetismus im Stress: Gleichzeitiger Anti- und Ferromagnetismus

Die gleichzeitige Existenz von Magnetismus und Ferroelektrizät in einem Material ist selten. Setzt sich dieser Magnetismus aus mehreren unabhängigen, magnetischen Grundzuständen zusammen, ist das ungewöhnlich. Einer schweizerisch-französischen Zusammenarbeit unter Leitung des Paul Scherrer Instituts ist es gelungen, mehrere magnetische Grundzustände in einem Material zu realisieren und detailliert zu untersuchen.

Photograph (a) and schematic cross section (b) of a typical Au–LaAlO3–SrTiO3 tunnel device. The broad gold ring (inner diameter, 160 μm) lies on top of the LaAlO3 layer, which serves as a tunnel barrier between the 2DEL and the Au. The outer ring and the centre contact of the device are Au-covered Ti contacts to the 2DEL. c, Cross-sectional high-angle annular dark-field STEM image of a Au–LaAlO3–SrTiO3 tunnel junction. The image is taken along the zone axis of the perovskite unit cells. a.u., arbitrary uni…

Interface superconductor with gap behaviour like a high-temperature superconductor

The physics of the superconducting state in two-dimensional (2D) electron systems is relevant to understanding the high-transition-temperature copper oxide superconductors and for the development of future superconductors based on interface electron systems. But it is not yet understood how fundamental superconducting parameters, such as the spectral density of states, change when these superconducting electron systems are depleted of charge carriers.

Diagram of the processes in the LuMnO3 layers studied. The layer is highly strained close to the substrate, which leads to a ferromagnetic (FM) order there. As the distance grows, the strain decreases so that two antiferromagnetic (AFM) orders appear: the spin spirals and the E-type, where two spins point in one direction and the next two in the other.

Strain-Induced Ferromagnetism in Antiferromagnetic LuMnO3 Thin Films

Single phase and strained LuMnO3 thin films are discovered to display coexisting ferromagnetic and antiferromagnetic orders. A large moment ferromagnetism (≈1μB), which is absent in bulk samples, is shown to display a magnetic moment distribution that is peaked at the highly strained substrate-film interface. We further show that the strain-induced ferromagnetism and the antiferromagnetic order are coupled via an exchange field, therefore demonstrating strained rare-earth manganite thin films as promising candidate systems for new multifunctional devices.

HAADF STEM micrographs of YSZ thin films deposited by different methods. a) 8YSZ SP (Tdep = 370 °C; Tpa = 600 °C, 20 h), b) 8YSZ AA-CVD (Tdep = 450 °C, Tpa = 600 °C, 20 h), c) 8YSZ AA-CVD (Tdep = 600 °C, Tpa = 600 °C for 20 h), d) 3YSZ PLD (Tdep = 450 °C, pO2 = 7 Pa, Tpa = 600 °C, 1 h) with top and bottom electrode, e) 3YSZ PLD (Tdep = 450 °C, pO2 = 1 Pa, Tpa = 600 °C, 1 h), and f) 8YSZ PLD (Tdep = 700 °C, pO2 = 2.7 Pa, Tpa = 600 °C, 20 h) with top and bottom electrodes.

On Proton Conductivity in Porous and Dense Yttria Stabilized Zirconia at Low Temperature

The electrical conductivity of dense and nanoporous zirconia-based thin films is compared to results obtained on bulk yttria stabilized zirconia (YSZ) ceramics. Different thin film preparation methods are used in order to vary grain size, grain shape, and porosity of the thin films. In porous films, a rather high conductivity is found at room temperature which decreases with increasing temperature to 120 °C. This conductivity is attributed to proton conduction along physisorbed water (Grotthuss mechanism) at the inner surfaces.

Applications of laser printing for organic electronics

The development of organic electronic requires a non contact digital printing process. The European funded e-LIFT project investigated the possibility of using the Laser Induced Forward Transfer (LIFT) technique to address this field of applications. This process has been optimized for the deposition of functional organic and inorganic materials in liquid and solid phase, and a set of polymer dynamic release layer (DRL) has been developed to allow a safe transfer of a large range of thin films.

(a), (b) IR spectra showing the T dependence of the R mode in a SrTi18O3 single crystal with a ferroelectric transition at TCurie=23  K. (c), (d) Corresponding spectra of quantum paraelectric SrTi16O3.

Electric-Field-Induced Polar Order and Localization of the Confined Electrons in LaAlO3/SrTiO3 Heterostructures

With ellipsometry, x-ray diffraction, and resistance measurements we investigated the electric-field effect on the confined electrons at the LaAlO3/SrTiO3 interface. We obtained evidence that the localization of the electrons at negative gate voltage is induced, or at least enhanced, by a polar phase transition in SrTiO3 which strongly reduces the lattice polarizability and the subsequent screening. In particular, we show that the charge localization and the polar order of SrTiO3 both develop below ∼50  K and exhibit similar, unipolar hysteresis loops as a function of the gate voltage.

A scheme showing the LIFT process. The laser beam punching out an Alq3 pixel for transfer from the donor to the receiver substrate is shown in (a), and pair of electroluminescent pixels are shown with a bias applied in(b).

The fabrication of small molecule organic light-emitting diode pixels by laser-induced forward transfer

Laser-induced forward transfer (LIFT) is a versatile organic light-emitting diode (OLED) pixel deposition process, but has hitherto been applied exclusively to polymeric materials. Here, a modified LIFT process has been used to fabricate small molecule Alq3 organic light-emitting diodes (SMOLEDs). Small molecule thin films are considerably more mechanically brittle than polymeric thin films, which posed significant challenges for LIFT of these materials.