Superconducting properties of BaBi3 at ambient and high pressures.

Herein, we report the preparation and characterization of BaBi3 clarified by DC magnetic susceptibility, powder X-ray diffraction (XRD), and electrical transport. The superconducting properties of BaBi3 were elucidated through the magnetic and electrical transport properties in a wide pressure range. The superconducting transition temperature, Tc, showed a slight decrease (or almost constant Tc) against pressure up to 17.2 GPa. The values of the upper critical field, Hc2, at 0 K, were determined to be 1.27 T at 0 GPa and 3.11 T at 2.30 GPa, using the formula, because p-wave pairing appeared to occur for this material at both pressures, indicating the unconventionality of superconductivity. This result appears to be consistent with the topological non-trivial nature of superconductivity predicted theoretically. The pressure-dependent XRD patterns measured at 0-20.1 GPa indicated no structural phase transitions up to 20.1 GPa, i.e., the structural phase transitions from the α phase to the ß or γ phase which are induced by an application of pressure were not observed, contrary to the previous report, demonstrating that the α phase is maintained over the entire pressure range. Admittedly, the lattice constants and the volume of the unit cell, V, steadily decrease with increasing pressure up to 20.1 GPa. In this study, the plots of Tcversus p and V versus p of BaBi3 are depicted over a wide pressure range for the first time.

Emergence of a Pressure-Driven Superconducting Phase in Ba0.77Na0.23Ti2Sb2O.

We investigated the pressure dependence of electric transport in a superconducting sample, Ba0.77Na0.23Ti2Sb2O, to complete the phase diagram of superconducting transition temperature (Tc) against pressure (p). This superconducting sample exhibits a Tc value of 5.8 K at ambient pressure. Here, the superconductivity of the recently reported sample was investigated over a wide pressure range. The Tc value monotonously decreased with pressure below 8 GPa. Interestingly, the Tc value rapidly increased above 8 GPa and slowly declined with pressure above 11 GPa. Thus, a new superconducting phase was discovered above ∼9 GPa. The crystal structure of Ba0.77Na0.23Ti2Sb2O was also elucidated at 0-22.0 GPa with synchrotron X-ray powder diffraction. Consequently, an evident relation between the crystal structure and the superconductivity was revealed, namely, a clear structural phase transition was observed at 8-11 GPa, where the Tc value rapidly increased against pressure. This study provides detailed information on the superconductivity of Ba0.77Na0.23Ti2Sb2O under pressure, which will lead to a comprehensive understanding of pressure-driven superconductivity.

Superconducting behavior of BaTi2Bi2O and its pressure dependence.

A new superconducting sample, BaTi2Bi2O, was synthesized and characterized over a wide pressure range. The superconducting transition temperature, Tc, of BaTi2Bi2O was 4.33 K at ambient pressure. The crystal structure was tetragonal (space group of P4/mmm (No. 123)), according to the X-ray diffraction (XRD) pattern at ambient pressure. The XRD pattern was analyzed using the Le Bail method. The magnetic-field dependence of the magnetization at different temperatures was precisely investigated to elucidate the characteristics of the superconductivity. The pressure-dependent XRD patterns showed absence of structural phase transitions up to 19.8 GPa. The superconducting properties of BaTi2Bi2O were investigated under pressure. Tc monotonously increased with the pressure (p) up to 4.0 GPa and saturated above 4.0 GPa. The variations in the Tc-p plot were thoroughly analyzed. The Cooper pair symmetry (or superconducting pairing mechanism) was analyzed based on the magnetic field dependence of the superconductivity at ambient and high pressures, which indicated a sign of p-wave pairing for the superconductivity of BaTi2Bi2O, i.e., topologically nontrivial sign was suggested for BaTi2Bi2O.

Superconductivity in Bi2-x Sb x Te3-y Se y (x = 1.0 and y = 2.0) under pressure.

The crystal structure of BiSbTeSe2 (Bi2-x Sb x Te3-y Se y (x = 1.0 and y = 2.0)) at 0-29 GPa is investigated through synchrotron x-ray diffraction (XRD) and two structural phase transitions are discovered. The stoichiometry of BiSbTeSe2 employed in this study is Bi1.19(4)Sb0.81(4)Te0.83(4)Se2.17(4), as determined from energy-dispersive x-ray spectroscopy. The sample demonstrated structural transitions, from a rhombohedral structure (space group no 166, R [Formula: see text] m) (phase I) to a monoclinic structure (space group no 12, C2/m) (phase II), and from phase II to a 9/10-fold monoclinic structure (space group no 12, C2/m) (phase III). The temperature dependence of resistance (R-T plot) exhibited a semiconducting behavior in a low pressure range and changed from semiconducting to metallic behavior with increasing pressure. Pressure-driven superconductivity is observed above 9.1 GPa in Bi1.19(4)Sb0.81(4)Te0.83(4)Se2.17(4). The pressure phase corresponds to phase II. The superconducting transition temperature, T c, increased with pressure. The maximum T c value is 8.3 K at 19.1 GPa. The magnetic field dependence of T c in phase II of Bi1.19(4)Sb0.81(4)Te0.83(4)Se2.17(4) is proceeded by a p-wave polar model, indicating topologically nontrivial superconductivity. In addition, the emergence of superconductivity and the change in superconducting behavior are closely associated with the structural transitions.

Preparation and characterization of a new graphite superconductor: Ca0.5Sr0.5C6.

We have produced a superconducting binary-elements intercalated graphite, CaxSr1-xCy, with the intercalation of Sr and Ca in highly-oriented pyrolytic graphite; the superconducting transition temperature, T c, was ~3 K. The superconducting CaxSr1-xCy sample was fabricated with the nominal x value of 0.8, i.e., Ca0.8Sr0.2Cy. Energy dispersive X-ray (EDX) spectroscopy provided the stoichiometry of Ca0.5(2)Sr0.5(2)Cy for this sample, and the X-ray powder diffraction (XRD) pattern showed that Ca0.5(2)Sr0.5(2)Cy took the SrC6-type hexagonal-structure rather than CaC6-type rhombohedral-structure. Consequently, the chemical formula of CaxSr1-xCy sample could be expressed as 'Ca0.5(2)Sr0.5(2)C6'. The XRD pattern of Ca0.5(2)Sr0.5(2)C6 was measured at 0-31 GPa, showing that the lattice shrank monotonically with increasing pressure up to 8.6 GPa, with the structural phase transition occurring above 8.6 GPa. The pressure dependence of T c was determined from the DC magnetic susceptibility and resistance up to 15 GPa, which exhibited a positive pressure dependence of T c up to 8.3 GPa, as in YbC6, SrC6, KC8, CaC6 and Ca0.6K0.4C8. The further application of pressure caused the rapid decrease of T c. In this study, the fabrication and superconducting properties of new binary-elements intercalated graphite, CaxSr1-xCy, are fully investigated, and suitable combinations of elements are suggested for binary-elements intercalated graphite.

Effluent syntaxin3 from dying cells affords protection against apoptosis in epidermal keratinocytes.

Ultra-violet B (UVB)-induced oxidative stress crucially perturbs the epidermal homeostasis, and the skin is endowed with protective mechanisms to take action against such damage. Here, we show the possible involvement of t-SNARE protein syntaxin3, a membrane fusion mediator of cytoplasmic vesicles, and which is released from dying keratinocytes, to play a role in this response. UVB irradiation, which generates reactive oxidative stress in cells, was shown to lead to the keratinocyte cell death accompanied by a release of cytoplasmic syntaxin3. We found that such extracellularly sourced syntaxin3 completely blocked the processing of a crucial effector for apoptotic cell death, caspase-3, and thus facilitated the survival of keratinocytes damaged by oxidative stress. These results demonstrate the latent prosurvival function of syntaxin3 and underline the importance of intracellular molecular elements for the maintenance of homeostasis in epidermal keratinocytes.

Extracellular syntaxin4 triggers the differentiation program in teratocarcinoma F9 cells that impacts cell adhesion properties.

The proteins in the syntaxin family are known to mediate fusion of cytoplasmic vesicles to the target membrane, yet subpopulations of certain syntaxins, including syntaxin4, translocate across the cell membrane in response to external stimuli. Here, we show that extracellularly presented syntaxin4 impacts cell behavior and differentiation in teratocarcinoma F9 cells. While undifferentiated F9 cells extruded a small subpopulation of extracellular syntaxin4 at the lateral cell membrane, the induction of differentiation with all-trans retinoic acid (RA) abolished this localized expression pattern. We found that the cells that were stimulated in a non-directional fashion by extracellular syntaxin4 displayed a flattened shape and retained a substrate-bound morphology even under a long-term, serum-starved cultivation. Such a cellular response was also elicited by a circular peptide composed of the potential functional core of syntaxin4 (AIEPQK; amino acid residues 103~108) (ST4n1). While the proliferation and metabolism were not affected in these cells, cell-cell interaction became weakened and the expression of vinculin, a regulator of both intercellular and cell-substrate adhesion molecules, was altered. We also found that the expressions of several differentiation markers were up-regulated in cells stimulated with extracellular syntaxin4 and that syntaxin3, another family member, was most prominent. Intriguingly, forced expression of syntaxin3 induced the spread morphology in F9 cells, indicating that syntaxin3 partly mediates the function of extracellular syntaxin4. These results demonstrate the involvement of a non-directional stimulation of extracellular syntaxin4 in the functional and morphological differentiation of F9 cells.

The impact of extracellular syntaxin4 on HaCaT keratinocyte behavior.

Syntaxin4 belongs to t-SNARE protein family and functions as a vesicular fusion mediator in the plasma membrane in a wide variety of cell types. This protein resembles another family member, epimorphin, a subpopulation of which has been shown to be secreted extracellularly in order to exert signaling functions. Here, we demonstrate the secretion of syntaxin4 via a non-classical pathway and its extracellular functions by using the functionally normal keratinocyte HaCaT. Extracellularly presented syntaxin4 appeared to elicit many cell responses similar to epimorphin with an important exception: it clearly facilitated keratinocyte cornification. The circularized peptide ST4n1 was synthesized from the putative functional core of syntaxin4 (a.a. 103-108), which is equivalent to the previously generated antagonist of epimorphin, and neutralized this contradictory effect. Intriguingly, an epimorphin mutant (EP4M) in which the functional core was replaced by that of syntaxin4 behaved like epimorphin, which was again antagonized by ST4n1. Electrophoresis-based analyses demonstrated the distinct structure of syntaxin4 compared to epimorphin or EP4M. These results revealed, for the first time, the extracellular role of syntaxin4 and shed light on the division of the extracellular effects exerted by epimorphin and syntaxin4 on keratinocyte cornification.