Search

By coupling two quantum dots via a superconductor-semiconductor hybrid region in a 2D electron gas, the authors achieve efficient splitting of Cooper pairs. Further, by applying a magnetic field perpendicular to the spin-orbit field, they can induce and measure large triplet correlations in the Cooper pair splitting process.

The second sound is an entropy oscillation propagating with constant pressure. Here the authors demonstrate the variation of the second sound wave in the crossover from the Bose-Einstein condensate to the Bardeen-Cooper-Schrieffer superfluid using 6Li.

DC-powered microwave amplifiers approach the quantum noise limit by using the interaction between microwave radiation and inelastic Cooper-pair tunnelling across a voltage-biased Josephson junction.

Disorder leads to localization of electrons at low temperatures, changing metals to insulators. In a superconductor the electrons are paired up, and scanning tunnelling microscopy shows that the pairs localize together rather than breaking up and forming localized single electrons in the insulating state.

Controllable detection of singlet and triplet Cooper pair splitting via crossed Andreev reflection is demonstrated in spin-polarized quantum dots on a superconducting nanowire platform with strong spin–orbit coupling.

Quantum phase transitions are most commonly found to occur at zero temperature. Cuevaset al.present numerical evidence confirming that a quantum phase transition can also occur at finite temperature, provided strong disorder is present.

Thermoelectricity due to the interplay of the nonlocal Cooper pair splitting and the elastic co-tunneling in normal metal-superconductor-normal metal structure is predicted. Here, the authors observe the non-local Seebeck effect in a graphene-based Cooper pair splitting device.

The pseudogap state in the cuprate superconductors shows signs of electronic pair formation above the superconducting temperature. Is it just a ‘precursor’ state or a separate (and competing) state? In fact, both interpretations seem to be correct.

One of the most counterintuitive fundamental properties of quantum mechanics is non-locality, which manifests itself as correlations between spatially separated parts of a quantum system. Although experimental tests of non-locality (Bell inequalities) have been successfully conducted with pairwise entangled photons, similar demonstrations using electrons have so far not been possible. The realization of a Y-shaped tunable Cooper pair splitter, to split entangled electrons on demand, brings this one step closer.

By pushing scanning tunnelling spectroscopy down to millikelvin temperatures, it is now possible to image a heavy fermion superconductor and measure the superconducting gap symmetry, with gap nodes in unexpected momentum-space locations.

Owing to electron localization, two-dimensional materials are not expected to be metallic at low temperatures, but a field-induced quantum metal phase emerges in NbSe₂, whose behaviour is consistent with the Bose-metal model.

Although quantum phase transitions are attracting increasing attention as the conceptual link between conventional and exotic states of quantum matter—having been implicated, for example, in the properties of high-temperature superconductors—there are few model systems in which they can be studied and understood. Now it is revealed that placing simple elemental chromium under pressure suppresses its normal magnetic state and gives direct experimental access to the underlying quantum phase transition responsible for these changes.

Scanned Josephson tunnelling microscopy is used to image Cooper pair tunnelling from a superconducting microscope tip to the quantum condensate of Bi₂Sr₂CaCu₂O_8+x, thus revealing the spatially modulated density of Cooper pairs predicted from several theories of the cuprate pseudogap phase.

Electronic devices operating at the nanoscale can exhibit unique electrical and thermal phenomena that can affect overall performance and so it is necessary to understand and control these types of fluctuations. Here, the authors theoretically and experimentally investigate quantum phase slips which can proliferate at low-temperatures in miniaturised superconducting devices and determine how this impacts on the resultant transport properties.

The realization of cold and dense electron–hole systems by optical excitation is hindered by the heating caused by particle recombination. Now, cold and dense electron–hole systems have been observed in heterostructures with separated electron and hole layers.

Due to their small size, atomic-scale Josephson junctions are vulnerable to thermal fluctuations. Escribano et al. show that introducing a delayed feedback element, a common method to mitigate thermal noise, induces spontaneous oscillations that enhance capabilities of Josephson microscopy.

The authors present experimental evidence of three-dimensional superinsulation in a nanopatterned slab of NbTiN. In the electric Meissner state, they find polar nematic order arising from ferroelectric alignment of short electric strings excited by external electromagnetic fields.

The BCS-BEC crossover is typically observed using ultracold atomic systems but recent experiments suggest investigations may also be possible using strongly correlated systems. Here, the authors use FeSe_1−xS_x to investigate the evolution of the superconducting state in the BCS-BEC crossover regime observing multiband nature of the BCS-BEC crossover with a suppression of the nematic order upon S-substitution.

Superconducting spintronics has the potential to enhance device functionality by realising spin polarised supercurrents with greater coherence and reduced dissipation. Here, using ferromagnetic resonance, the authors investigate the temperature dependence of the Gilbert damping for the Fe layer of Nb/Fe/Nb and Nb/Cr/Fe/Cr/Nb stacks and the impact superconducting spin triplets have on the spin pumping behaviour.

Magnetic molecules deposited on a metallic substrate constitute a method to engineer the spin properties of the molecule and has potential application in low-power information storage devices. Here, the authors investigate a superconductor/molecule/normal metal heterostructure and demonstrate spin-ordering and proximity induced superconducting properties at the metallo-molecular interface.

The authors introduce a new spectroscopic technique for studying Higgs modes in superconductors and apply it to a cuprate superconductor. The method involves a soft quench of the Mexican-Hat potential, populating Higgs modes of different symmetries, which are then probed by non equilibrium anti-Stokes Raman scattering.

Quarks in the interior of hadrons make up most of ordinary matter, yet their observation is not possible, and their properties can only be probed indirectly. Adopting an analogy between physics of superinsulators and high energy physics, the authors present direct observations of the interior of electric mesons made of Cooper pairs by standard transport measurements.

Finite momentum superconducting pairing refers to a class of unconventional superconducting states where Cooper pairs acquire a non-zero momentum. Here the authors report a new superconducting state in bulk 4Hb-TaS₂, where magnetic fields induce finite momentum pairing via magnetoelectric coupling.

By tuning and mapping Josephson currents at the atomic scale, researchers uncover how competing superconducting phases in FeSe interfere, revealing the fingerprints of s^±-wave pairing and frustrated Josephson coupling.

Pearl inductance in thin films of YBCO enables terahertz superinductance and achieves impedance surpassing the quantum resistance limit, promising advancements in quantum and photonic technologies.

African ancestry is a known risk factor for prostate cancer development, but the genetic determinants of this are incompletely understood. Here, the authors identify 172 potentially pathogenic variants which are enriched in an African population.

Resistance mutations in BCL-2 reduce the clinical efficacy of venetoclax. DeAngelo et al. show stapled BAD BH3 peptides can retain and even enhance binding to these mutants, offering a structurally informed strategy to overcome this mechanism of cancer drug resistance.

In condensed matter physics, p-wave chiral superfluidity is an unconventional topological many-body quantum state. Here, Liu et al. report a new mechanism to achieve a centre-of-mass p-wave chiral superfluid state in a spin imbalanced atomic Fermi gas with s-wave interaction.

The mechanism of high-temperature superconductivity remains a subject of debate. Krasnov et al.describe a technique for measuring the spectra of bosons generated during the formation of Cooper pairs in a cuprate, the results of which suggest that the process is governed by electron–electron interactions.

Spin correlation experiments are demonstrated in an electron entangler device based on the ‘splitting’ of Cooper pairs from a superconductor, which can potentially be used to investigate many fundamental phases and processes related to the electron spin.

Using torque magnetometry, the thermodynamic signatures of bosonic Landau level transitions are observed in a layered superconductor, owing to the formation of Cooper pairs with finite momentum.

Chiral superconductors are very rare topological materials. Here, the authors report spontaneous magnetic fields inside the superconducting state and low temperature linear behavior in the superfluid density in LaPt₃P, suggesting a chiral d-wave singlet superconducting state.

In disordered superconductors, the localization of Cooper pairs enhances the local critical temperature (Tc) but suppresses the supercurrent. The authors propose an approach which resolves this inherent trade-off by showing that when such a system is coupled to a clean conductor, a synergetic effect emerges: the hybrid structure simultaneously mainteins elevated Tc and robust supercurrent transport.

When a Josephson junction is embedded into a highly-resistive environment, it loses its superconducting properties and starts to behave as an insulator. This results in voltage oscillations across the current-biased junction - the Bloch oscillations. Here the authors develop a fully quantum theory of this effect.

Pairing interaction appears at room temperature in traditional superconductors with a Cooper instability in the Fermi sea. Here, Maier et al.report that in the pseudogap phase of cuprate, where this instability is absent, superconductivity arises from an increase in the strength of the spin fluctuation pairing interaction as the temperature decreases.

Superconductivity has not been observed in any antiperovskite oxide up to now. Here Oudahet al. report superconducting transition around 5 K in antiperovskite oxide Sr_3−xSnO, making it a new class of oxide superconductors.