The Josephson effect describes the generic appearance of a supercurrent in a weak link between two superconductors. Its exact physical nature deeply influences the properties of the supercurrent. In recent years, considerable efforts have focused on the coupling of superconductors to the surface states of a three-dimensional topological insulator. In such a material, an unconventional induced p-wave superconductivity should occur, with a doublet of topologically protected gapless Andreev bound states, whose energies vary 4π-periodically with the superconducting phase difference across the junction. In this article, we report the observation of an anomalous response to rf irradiation in a Josephson junction made of a HgTe weak link. The response is understood as due to a 4π-periodic contribution to the supercurrent, and its amplitude is compatible with the expected contribution of a gapless Andreev doublet. Our work opens the way to more elaborate experiments to investigate the induced superconductivity in a three-dimensional insulator.
Transport measurements are presented on a class of electrostatically defined lateral dots within a high mobility two dimensional electron gas (2DEG). The new design allows Coulomb Blockade(CB) measurements to be performed on a single lateral dot containing 0, 1 to over 50 electrons. The CB measurements are enhanced by the spin polarized injection from and into 2DEG magnetic edge states. This combines the measurement of charge with the measurement of spin through spin blockade spectroscopy. The results of Coulomb and spin blockade spectroscopy for first 45 electrons enable us to construct the addition spectrum of a lateral device. We also demonstrate that a lateral dot containing a single electron is an effective local probe of a 2DEG edge.
We introduce a new class of spintronics devices in which a spin-valve like effect results from strong spin-orbit coupling in a single ferromagnetic layer rather than from injection and detection of a spin-polarized current by two coupled ferromagnets. The effect is observed in a normalmetal/insulator/ferromagnetic-semiconductor tunneling device. This behavior is caused by the interplay of the anisotropic density of states in (Ga,Mn)As with respect to the magnetization direction, and the two-step magnetization reversal process in this material.PACS numbers: 75.50. Pp, 85.75.Mm Devices relying on spin manipulation are hoped to provide low-dissipative alternatives for microelectronics. Furthermore, spintronics is expected to lead to full integration of information processing and storage functionalities opening attractive prospects for the realization of instant on-and-off computers. A primary goal of current spintronics research is to realize a device with metal spin-valve like behavior [1] in an all semiconductor-based structure enhancing integration of spintronics with existing microelectronics technologies. An oft proposed scheme for such a device consists of a tunnel barrier between two ferromagnetic semiconductors. As such, (Ga,Mn)As/(Al,Ga)As/(Ga,Mn)As structures have previously been studied [2,3] with some promising results. However, realizing the full potential of these systems will require a complete understanding of the physics of tunneling into (Ga,Mn)As, which we have found to be rather different than previously thought.In this spirit, we investigate transport in a structure consisting of a single ferromagnetic (Ga,Mn)As layer fitted with a tunnel barrier and a non-magnetic metal contact. We report some of the rich experimental properties of such a tunneling structure and provide an interpretation of the measured spin-valve like effect as a tunneling anisotropic magnetoresistance (TAMR) due to a two-step magnetization reversal and a magnetization dependent density of states (DOS) in the (Ga,Mn)As layer.The magnetic layer in our sample is a 70 nm thick epitaxial (Ga,Mn)As film grown by low temperature (270• C) molecular beam epitaxy onto a GaAs (001) substrate [4]. High-resolution x-ray diffraction showed that the sample had high crystalline quality comparable to that of the substrate. From the measured lattice constant and the calibration curves of Ref.[5], the Mn concentration in the ferromagnetic layer is roughly 6%. Etch capacitance-voltage control measurements yielded a hole density estimate of ∼ 10 21 cm −3 and the Curie temperature of 70 K was determined from SQUID measurements.After growth, the sample surface was Ar sputtered to remove any potential oxides, and a 1.4 nm Al layer was deposited at a rate of 0.
We have fabricated all II-VI semiconductor resonant tunneling diodes based on the (Zn,Mn,Be)Se material system, containing dilute magnetic material in the quantum well, and studied their current-voltage characteristics. When subjected to an external magnetic field the resulting spin splitting of the levels in the quantum well leads to a splitting of the transmission resonance into two separate peaks. This is interpreted as evidence of tunneling transport through spin polarized levels, and could be the first step towards a voltage controlled spin filter.
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