Nonlinear conductivity in CaRuO3 thin films measured by short current pulses

Metals near quantum critical points have been predicted to display universal out-of equilibrium behavior in the steady current-carrying state. We have studied the non-linear conductivity of high-quality CaRuO$_3$ thin films with residual resistivity ratio up to 57 using micro-second short, high-field current pulses at low temperatures. Even for the shortest pulses of $5\mu$s, Joule heating persists, making it impossible to observe a possible universal non-linearity. Much shorter pulses are needed for the investigation of universal non-linear conductivity.Comment: 9 pages, 7 figure

How the new running shoe technologies influence biomechanics and injury outcomes in recreational runners

The biomechanical study of 38 male and female recreational runners demonstrates the relationship between the four most frequently used footwear technologies and the biomechanical loading of the lower extremities in running. Running in the four midsole technologies (1. NEUTRAL (N_RS): neutral, cushioning running shoes, 2. SUPPORT (S_RS): support, motion control running shoes, 3. MAX (M_RS): maximalist, carbon-fiber plate running shoes, and 4. UTEC (U_RS): running shoes with a U-shaped midsole construction and highly cushioning foam) indicate a strong impact of midsole technology on the kinetics of the lower extremities. Midsole construction and material of the four running shoe categories systematically modulate the joint moments at the foot, the ankle joint, and the knee joint and thus the mechanical loading of the biological structures of the lower extremities in every step when running. The data demonstrates no significant differences in running kinetics between NEUTRAL running shoes and SUPPORT running shoes while MAX running shoes increase and UTEC running shoes decrease ankle joint and knee joint loading during the stance phase. A 12-month standardized and randomized intervention trial surveyed 1697 recreational runners who used one of the four dedicated running shoe categories in more than 75% of their runs. The results demonstrate a strong relation between the development of running-associated injuries in general and knee and Achilles tendon problems in particular and the footwear categories. While neutral and support running shoes show no significant differences in the development of running-related injuries, M_RS increase and U_RS decrease this risk, especially the occurrence of knee pain. Other risk factors, like age, gender, BMI, running distance, average speed, surface as well as foot morphology and leg axis, only have a minor effect on the development of running-related injuries in the 12-months survey. Running shoe midsole technologies provide access to a sophisticated causal explanation of overload injuries of biological structures of the lower extremity during running and the resulting running-related injuries

Angular dependence of Hall effect and magnetoresistance in SrRuO3−SrIrO3 heterostructures

Perovskite SrRuO$_3$ is a prototypical itinerant ferromagnet which allows interface engineering of its electronic and magnetic properties. We report synthesis and investigation of atomically flat artificial multilayers of SrRuO$_3$ with the spin-orbit semimetal SrIrO$_3$ in combination with band-structure calculations with a Hubbard $U$ term and topological analysis. They reveal an electronic reconstruction and emergence of flat Ru-4d$_{xz}$ bands near the interface, ferromagnetic interlayer coupling and negative Berry-curvature contribution to the anomalous Hall effect. We analyze the Hall effect and magnetoresistance measurements as a function of the field angle from out of plane towards in-plane orientation (either parallel or perpendicular to the current direction) by a two-channel model. The magnetic easy direction is tilted by about $20^\circ$ from the sample normal for low magnetic fields, rotating towards the out-of-plane direction by increasing fields. Fully strained epitaxial growth enables a strong anisotropy of magnetoresistance. An additional Hall effect contribution, not accounted for by the two-channel model is compatible with stable skyrmions only up to a critical angle of roughly $45^\circ$ from the sample normal. Within about $20^\circ$ from the thin film plane an additional peak-like contribution to the Hall effect suggests the formation of a non-trivial spin structure.Comment: to be published in Phys. Rev.

Strong terahertz third-harmonic generation by kinetic heavy quasiparticles in CaRuO3

We report on time-resolved nonlinear terahertz spectroscopy of a strongly correlated ruthenate, CaRuO3, as a function of temperature, frequency, and terahertz field strength. Third-harmonic radiation for frequencies up to 2.1 THz is observed evidently at low temperatures below 80 K, where the low-frequency linear dynamical response deviates from the Drude model and a coherent heavy quasiparticle band emerges by strong correlations associated with the Hund’s coupling. Phenomenologically, by taking an experimentally observed frequency-dependent scattering rate, the deviation of the field driven kinetics from the Drude behavior is reconciled in a time-dependent Boltzmann description, which allows an attribution of the observed third-harmonic generation to the terahertz field driven nonlinear kinetics of the heavy quasiparticles

Strong terahertz third-harmonic generation by kinetic heavy quasiparticles in CaRuO3_3

We report on time-resolved nonlinear terahertz spectroscopy of a strongly correlated ruthenate, CaRuO$_3$, as a function of temperature, frequency and terahertz field strength. Third-harmonic radiation for frequencies up to 2.1 THz is observed evidently at low temperatures below 80 K, where the low-frequency linear dynamical response deviates from the Drude model and a coherent heavy quasiparticle band emerges by strong correlations associated with the Hund's coupling.Phenomenologically, by taking an experimentally observed frequency-dependent scattering rate, the deviation of the field driven kinetics from the Drude behavior is reconciled in a time-dependent Boltzmann description, which allows an attribution of the observed third-harmonic generation to the terahertz field driven nonlinear kinetics of the heavy quasiparticles.Comment: 5 pages, 3 figure

Electronic reconstruction and charge transfer in strained Sr2CoIrO6 double perovskite

The electronic, magnetic and optical properties of the double perovskite Sr$_2$CoIrO$_6$ (SCIO) under biaxial strain are explored in the framework of density functional theory (DFT) including a Hubbard $U$ term and spin-orbit coupling (SOC) in combination with absorption spectroscopy measurements on epitaxial thin films. While the end member SrIrO$_3$ is a semimetal with a quenched spin and orbital moment and bulk SrCoO$_3$ is a ferromagnetic (FM) metal with spin and orbital moment of 2.50 and 0.13 $\mu_{B}$, respectively, the double perovskite SCIO emerges as an antiferromagnetic Mott insulator with antiparallel alignment of Co, Ir planes along the [110]-direction. Co exhibits a spin and enhanced orbital moment of $\sim 2.35-2.45$ and $0.31-$0.45 $\mu_{B}$, respectively. Most remarkably, Ir acquires a significant spin and orbital moment of 1.21-1.25 and 0.13 $\mu_{B}$, respectively. Analysis of the orbital occupation indicates an electronic reconstruction due to a substantial charge transfer from minority to majority spin states in Ir and from Ir to Co, signaling an Ir$^{4+\delta}$, Co$^{4-\delta}$ configuration. Biaxial strain, varied from -1.02% ($a_{\rm NdGaO_3}$) through 0% ($a_{\rm SrTiO_3}$) to 1.53% ($a_{\rm GdScO_3}$), influences in partcular the orbital polarization of the $t_{2g}$ states and leads to a nonmonotonic change of the band gap between 163 and 235 meV. The absorption coefficient reveals a two plateau fearure due to transitions from the valence to the lower lying narrow $t_{2g}$ and the higher lying broader $e_{g}$ bands. Inclusion of many body effects, in particular, excitonic effects by solving the Bethe-Salpeter equation (BSE), increases the band gap by $\sim0.2$ and improves the agreement with the measured spectrum concerning the position of the second peak at $\sim 2.6$ eV.Comment: 11 pages, 10 figure