Tunable superconductivity coexisting with the anomalous Hall effect in a transition metal dichalcogenide.

Transition metal dichalcogenides display a high technological potential due to their wide range of electronic ground states. Here, we unveil that by tuning hydrostatic pressure P, a cascade of electronic phase transitions can be induced in the few-layer transition metal dichalcogenide 1T'-WS. As P increases, we observe the suppression of superconductivity with the concomitant emergence of an anomalous Hall effect (AHE) at GPa.

Comparison of the long-term outcome of home vs. inpatient treatment: 18-24 months follow-up of a non-randomized controlled trial.

Home Treatment (HT) in child and adolescent psychiatry is an increasingly important topic in the current context of global crises and strained mental health systems. We implemented a HT program provided by a multiprofessional treatment team and compared long-term outcomes of 27 patients (48% female, Ø15.15 ± 2.

Discovery of a New Phase in Thin Flakes of KVSb under Pressure.

Results of magnetotransport measurements are reported on KVSb thin flakes under pressure. The zero-field electrical resistance reveals an additional anomaly emerging under pressure (p), marking a previously unidentified phase boundary T*(p). Together with the established T(p) and T(p), denoting the charge-density-wave transition and a superconducting transition, respectively, the temperature-pressure phase diagram of KVSb features a rich interplay among multiple phases.

The dHvA effect in Sn-doped PbTe topological crystalline insulator.

We report the synthesis, electrical transport, magnetotransport, and high-field torque magnetometry studies of the topological crystalline insulator SnPb1-xTe (= 0, 0.2, and 0.4).

Electronic commensuration of a spin moiré superlattice in a layered magnetic semimetal.

Spin moiré superlattices (SMSs) have been proposed as a magnetic analog of crystallographic moiré systems and a source of electron minibands offering vector-field moiré tunability and Berry curvature effects. However, it has proven challenging to realize an SMS in which a large exchange coupling is transmitted between conduction electrons and localized spins. Furthermore, most systems have carrier mean free paths shorter than their spin moiré lattice constant , inhibiting miniband formation.