Low Uniaxial Stress Research Articles

Designing the stripe-ordered cuprate phase diagram through uniaxial-stress.

The ability to efficiently control charge and spin in the cuprate high-temperature superconductors is crucial for fundamental research and underpins technological development. Here, we explore the tunability of magnetism, superconductivity, and crystal structure in the stripe phase of the cuprate La[Formula: see text]Ba[Formula: see text]CuO[Formula: see text], with [Formula: see text] = 0.115 and 0.135, by employing temperature-dependent (down to 400 mK) muon-spin rotation and AC susceptibility, as well as X-ray scattering experiments under compressive uniaxial stress in the CuO[Formula: see text] plane. A sixfold increase of the three-dimensional (3D) superconducting critical temperature [Formula: see text] and a full recovery of the 3D phase coherence is observed in both samples with the application of extremely low uniaxial stress of [Formula: see text]0.1 GPa. This finding demonstrates the removal of the well-known 1/8-anomaly of cuprates by uniaxial stress. On the other hand, the spin-stripe order temperature as well as the magnetic fraction at 400 mK show only a modest decrease under stress. Moreover, the onset temperatures of 3D superconductivity and spin-stripe order are very similar in the large stress regime. However, strain produces an inhomogeneous suppression of the spin-stripe order at elevated temperatures. Namely, a substantial decrease of the magnetic volume fraction and a full suppression of the low-temperature tetragonal structure is found under stress, which is a necessary condition for the development of the 3D superconducting phase with optimal [Formula: see text]. Our results evidence a remarkable cooperation between the long-range static spin-stripe order and the underlying crystalline order with the three-dimensional fully coherent superconductivity. Overall, these results suggest that the stripe- and the SC order may have a common physical mechanism.

Structural Evidence for a Reinforcing Response and Retention of Hydration During Confinement of Cartilage Lipids

Lipids have an important role in the complex lubrication of articulating joints, however changes in lipid phase behavior that occur owing to mechanical confinement are not well understood. Here, a surface force-type apparatus has been combined with neutron reflectometry to measure confinement-induced changes in the structure of lipids, the major surface-active component of the lubricant in articulating joints. The same incompressible state was accessed under low uniaxial stress (1 bar), irrespective of whether the lipids had started out unconfined above or below the Lα phase transition, and irrespective of whether they were fully or partially hydrated. In this incompressible state, the lipid component had thickened indicating extension and rearrangement of the lipid chains in response to the applied stress. The small amount of water remaining between each lipid bilayer was found to be similar for all chain lengths and starting phases. This represents the first structural evidence of the tightly bound water layer at the headgroups, which is required for hydration lubrication under load.

Using Uniaxial Stress to Probe the Relationship between Competing Superconducting States in a Cuprate with Spin-stripe Order.

We report muon spin rotation and magnetic susceptibility experiments on in-plane stress effects on the static spin-stripe order and superconductivity in the cuprate system La_{2-x}Ba_{x}CuO_{4} with x=0.115. Anextremely low uniaxial stress of ∼0.1 GPa induces a substantial decrease in the magnetic volume fraction and a dramatic rise in the onset of 3D superconductivity, from ∼10 to 32K; however, the onset of at-least-2D superconductivity is much less sensitive to stress. These results show not only that large-volume-fraction spin-stripe order is anticorrelated with 3D superconducting coherence but also that these states are energetically very finely balanced. Moreover, the onset temperatures of 3D superconductivity and spin-stripe order are very similar in the large stress regime. These results strongly suggest a similar pairing mechanism for spin-stripe order and the spatially modulated 2D and uniform 3D superconducting orders, imposing an important constraint on theoretical models.

3D surface condensation of large atomic shear strain in nanoscale metallic glasses under low uniaxial stress

Nanoscale metallic glasses (MGs) are frequently used in experimental and computational studies to probe the deformation mechanisms in amorphous metals. Potential consequences of the significant surface to volume ratio in these extremely small materials, nevertheless, are not well understood. Here, using molecular dynamics simulations and novel selective 3D visualization, we show that significant irreversible atomic shear strain condenses on the 3D surface of these materials under low uniaxial stress, while the interior atoms are bearing much lower, mostly reversible shear strain. This is observed for various sample geometries, dimensions, strain rates and temperatures, and attributable to the correlations of atomic shear strain with atomic potential energy and coordination number. The results reveal the profound influence of the surface on the strain partitioning in nanoscale MGs across the 3D volume, critical to the initiation and continuation of plasticity.

Mechanical properties of the human red blood cell membrane at −15 °C

The most common method for measuring the mechanical behavior of the human red blood cell (RBC) membrane is micropipette aspiration, because it can be used to apply both a low uniaxial stress at a small part of the membrane or high two-axial stresses to the whole membrane [E.A. Evans, R.E. Waugh, Mechano-chemical study of red cell membrane structure in situ, in: Kroc Foundation Series, vol. 13, Erythrocyte Mechanics and Blood Flow, Alan R. Liss. Inc., New York, 1980, pp. 31–56 (Chapter 3); H.J. Meiselman, Measures of blood rheology and erythrocyte mechanics, in: Kroc Foundation Series, vol. 13, Erythrocyte Mechanics and Blood Flow, Alan R. Liss. Inc., New York, 1980, pp. 75–117 (Chapter 5)]. The elastic shear moduli and area changes of the human RBC published to date were calculated by means of this technique. However, a main drawback of the method is its impracticability at subzero temperatures. Experiments at below 0 °C are of interest because it is at these temperatures that RBC lysis occurs during freezing and thawing after cryopreservation, via a mechanism that may be mechanical. A method for circumventing this limitation is deforming the cell membranes by applying an electric ac field to a supercooled suspension. In a previous study, we applied this technique to human RBCs down to −15 °C [M. Krueger, F. Thom, Deformability and stability of erythrocytes in high-frequency electric fields down to subzero temperatures, Biophys. J. 73 (1997) 2653–2666]. In this technique, the electrical dimensions must be translated into those of mechanics. We provided a formula for these calculations, which demonstrated excellent concordance with known mechanical measurements at room temperature [F. Thom, H. Gollek, Calculation of mechanical properties of human red cells based on electrically induced deformation experiments, J. Electrostat. 64 (2006) 53–61]. Using this formula, we have now calculated the shear moduli and stress–strain diagram for our deformation experiments at −15 °C and present the results below.

Low-stress pressure solution experiments on halite single-crystals

Pressure solution experiments on halite single-crystals in saturated solution were carried out at atmospheric pressure under uniaxial stress ranging from 0.1 to 2.0 MPa and at temperatures of 303 and 323 K. The experiments were performed in ceramic loading rigs with damp-proofed sample chambers. The low uniaxial stress is applied by loading the piston with steel weights ranging from 0.5 to 5.0 kg. The position of the piston is measured by an electronic displacement transducer, connected to a data acquisition system. Deviations caused by fluctuations of temperature and output voltage of the power supply are corrected after data acquisition. The halite cubes {100} with edge dimensions of 3–9 mm are prepared by cleaving and placed with a (100) cleavage face on the (001) face of a muscovite single-crystal (10×10×0.1 mm), a polished quartz (0001) plate, or another halite crystal oriented to form a 45° twist boundary. The four free (100) faces of the halite cube are in contact with the surrounding NaCl solution. The initial displacement rate of the piston after flooding of the system and loading is up to 50.0 μm/day, attributed to smoothing of the halite face and elimination of point contacts with high stress concentration. Within 2 to 3 days this stage grades into steady-state displacement with rates of 0.1–2.0 μm/day. In some experiments stages of higher displacement rates (2.0–5.0 μm/day) lasting for 3–5 days are observed episodically, with intervals of 10–15 days. These cycles appear not to be triggered by external events. Experiments with a dry mica–halite interface, carried out for comparison at the same temperature and at an uniaxial stress of 2 MPa, result in a displacement rate below the limits of detection. This rules out a significant contribution of crystal plastic deformation in the wet experiments. The experimental results show no simple correlation between displacement rate and magnitude of uniaxial stress, crystal size, type of the interface, and temperature. At the given conditions, convergence at a single interface due to pressure solution is apparently not a steady-state process. The alternating stages of lower and higher displacement rates observed in many experiments suggest that the mechanisms of transport or dissolution may change spontaneously during the experiment. It is possible that the process itself leads to an unstable configuration causing episodic changes.

Sinter-forged YBa2Cu3O7−x superconducting ceramics from the spray-roasted powders

The effect of applying a uniaxial stress, while varying the temperature and the time of sinter-forging, on the microstructure and critical current density of the sinter-forged YBa2Cu3O7−x ceramics has been investigated. Spray-roasted powders from a nitrate-based feed solution were prepared as the starting materials. By applying a relatively low uniaxial stress (2 MPa), the sintered density increased up to 95% of the maximum value. Critical current densities of between 360 and 420 A cm−2 were obtained for the sinter-forged samples which are significantly higher than values reported for pressureless-sintered samples prepared from solid-state reacted powders (typically 70 A cm−2). This increase in the density of the material and the critical current density can be explained by the alignment of the elongated YBa2Cu3O7−x grains under applied uniaxial stress during sintering. The elongated YBa2Cu3O7−x grains have been characterized by transmission electron microscopy.

Compressional wave velocities of a lunar regolith sample in a simulated lunar environment

Ultrasonic compressional wave velocities have been measured in the laboratory for an Apollo 15 soil sample (15301, 38) under very low uniaxial stress and high vacuum conditions. The velocities measured range from 125 to 522 m/s. The velocities of the soil are stress dependent and are strongly affected by compaction history. Hertzian contact theory does not appear to fit the data adequately for the pressure range of the experiment. Moderate increases in temperature do not have a significiant effect on the compressional wave velocities.

Stress effects on excitons bound to shallow acceptors in GaAs

We have performed stress-dependent photoluminescence measurements on excitons bound to neutral shallow acceptors (${A}^{0}X$) in GaAs. From their temperature and stress variation three lines (at zero stress) are proved to be due to the decay of (${A}^{0}X$) with the $J=\frac{5}{2}$ state lowest. When low uniaxial stress (0-2 ${\mathrm{kg}\mathrm{mm}}^{\ensuremath{-}2}$) is applied these three lines split into 7 or 8 components, although at high stress only one line remains with a stress shift equal to that for the conduction band to acceptor recombination. A theoretical interpretation based on a bonding two-hole state analogous to the ${\mathrm{H}}_{2}$ molecule is found to agree well with the data when the effects of a weak crystal field are included. Small deviations between this theory and experiment are presumed to indicate the importance of the antibonding two-hole functions in the (${A}^{0}X$) wave function.