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. 2015 Oct 12:6:8628.
doi: 10.1038/ncomms9628.

Single Abrikosov vortices as quantized information bits

Affiliations

Single Abrikosov vortices as quantized information bits

T Golod et al. Nat Commun. .

Abstract

Superconducting digital devices can be advantageously used in future supercomputers because they can greatly reduce the dissipation power and increase the speed of operation. Non-volatile quantized states are ideal for the realization of classical Boolean logics. A quantized Abrikosov vortex represents the most compact magnetic object in superconductors, which can be utilized for creation of high-density digital cryoelectronics. In this work we provide a proof of concept for Abrikosov-vortex-based random access memory cell, in which a single vortex is used as an information bit. We demonstrate high-endurance write operation and two different ways of read-out using a spin valve or a Josephson junction. These memory cells are characterized by an infinite magnetoresistance between 0 and 1 states, a short access time, a scalability to nm sizes and an extremely low write energy. Non-volatility and perfect reproducibility are inherent for such a device due to the quantized nature of the vortex.

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Figures

Figure 1
Figure 1. Operation of a memory cell with a Josephson spin-valve read-out.
(a) Sketch of a Josephson spin-valve device. (b) Magnetic field dependence of Josephson critical current through the JSV#1 at T=2.4 K. A jump, marked by a circle, is due to antivortex exit. (c) Magnetic field dependence of a.c. resistance for JSV#1 at Ia.c.=50 (bottom plot) and 100 (top plot) μA. It is seen that the vortex exit field depends on the current. (d) High-bias spin-valve MR for a JSV#2 at T=1.8 K. Multiple branches at high fields are caused by entrance of vortices. The number of vortices (0–3) is marked at each branch. (e) Scanning electron microscopy image of JSV#3 AVRAM cell with a vortex trap. Scale bar, 500 nm. (f) Demonstration of write and erase operations for the same cell at T=1.8 K and H=2.4 kOe. Top plot shows applied current pulses, bottom plot the a.c. resistance.
Figure 2
Figure 2. Operation of a memory cell with planar Josephson junctions.
(a) Scanning electron microscopy (SEM) image and sketch of a planar AVRAM cell with a vortex trap and two read-out planar Josephson junctions. The scale bar in SEM image is 1 μm. (b) Magnetic field modulation of the critical current for the first read-out junction without (black) and with a vortex (red). (c) Magnetic field dependence of a.c. resistance without a vortex (black), with a vortex (red) and with an antivortex (blue line). (d) Demonstration of write and erase operations by current pulses of different amplitudes. (e) Demonstration of controllable 0–1 switching in a broad field range. (f) Evolution of the device state on applying a pulse train with growing amplitude. Note excellent half-selection stability. (g) Dependence of the final state on the pulse amplitude. (h) Demonstration of high-endurance 0–1 switching at zero applied field.

References

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