The present invention is related to the field of magnetic sensors and magnetic sensors based on magnetic tunnel junctions. More particularly, the present invention concerns a magnetic element having a linear and non-hysteretic behavior in a large measurement range.
A magnetization vortex is a coherent magnetic configuration in micro or nano magnetic structures with magnetization in the plane of the magnetic structure with magnetization rotations on a length scale comparable to the lateral dimension of the surface of the magnetic structure. The magnetization vortex results from an equilibrium between magnetostatic energy and exchange energy for cylindrical or near-cylindrical shaped micro or nano structures in magnetic layers, for which the radius and thickness are sufficiently large. Depending on the geometry of the magnetic structure, the vortex configuration is the stable spin configuration with the lowest energy at remanent state.
In a stable vortex configuration, the vortex can be deformed reversibly without being cancelled. More particularly, the vortex can deform reversibly under a moderate magnetic field. The part of the vortex magnetization parallel to the applied field tends to become larger and the part of the magnetization antiparallel to the applied field tends to become smaller. This causes displacement of the vortex core along the direction transverse to the direction of the applied field. When the magnetic field is reduced, the vortex core gradually returns to its equilibrium position in zero field. The equilibrium position of the vortex core in the case of a disk-shaped microstructure or nanostructure is at the center of the disk.
The vortex configuration provides a linear and non-hysteretic behavior in a large magnitude range of the external magnetic field 60, for practical size of the magnetoresistive sensor element 2 and thickness of the sense layer 21. The vortex configuration is thus advantageous for 1D magnetic sensor applications.
A ferromagnetic layer having a magnetization comprising a vortex configuration exhibits a hysteresis observed when a high bias field is applied, on one or the other direction (at zero field strength, the magnetization is offset from the origin by an amount called the remanence).
The intrinsic offset ΔMi is detrimental for sensors based on magnetic element comprising the ferromagnetic layer 21 since it decreases the measurement range allowed by such sensors.
WO2020217195 discloses a magnetic element comprising a first ferromagnetic layer having a first magnetization comprising a stable magnetization vortex configuration having a vortex core. The first ferromagnetic layer comprises an indentation configured such that the vortex core nucleates substantially at the indentation. Upon application 5 of an external magnetic field in a first field direction (−Hx), the vortex core moves along a first path and the first magnetization rotates around the vortex core in a counter-clockwise direction. Upon application of the external magnetic field in a second field direction (Hx) opposed to the first field direction, the vortex core moves along a 10 second path and the first magnetization rotates around the vortex core in a clockwise direction. Both the first and second field path are substantially identical and move the vortex core away from the indentation.
The present disclosure concerns a magnetic sensor device comprising a plurality of magnetic sensor elements; each magnetic sensor element comprising a magnetic tunnel junction including a reference layer having a reference magnetization, a sense layer having a sense magnetization and a tunnel barrier layer between the reference layer and the sense layer. The sense magnetization comprises a stable vortex configuration in the absence of an external magnetic field. The vortex has a core reversibly movable in a plane of the sense layer according to an external magnetic field. The sense layer comprises a peripheral shape in the plane, the peripheral shape comprising an asymmetric edge portion. The magnetic sensor elements are arranged such that the edge portion of a magnetic sensor element is opposite to the edge portion of the adjacent magnetic sensor element.
The magnetic sensor device disclosed herein allows for reducing the intrinsic offset ΔMi of each magnetic sensor element and the averaged offset ΔMa of the plurality of magnetic sensor elements. The magnetic sensor device has increased measurement range compared to conventional magnetic sensor devices. Measurement range can be above the vortex cancellation field, or expulsion field such that no hysteresis is observed when a high bias field is applied.
Exemplar embodiments of the invention are disclosed in the description and illustrated by the drawings in which:
The sense and reference layers 21, 23 can be made of a ferromagnetic material such as Fe based alloy, CoFe, NiFe or CoFeB. Optionally, the reference layer 23 can be pinned by an antiferromagnetic layer 24 by magnetic exchange bias coupling. The antiferromagnetic layer can comprise an alloy based on manganese Mn, such as alloys based on iridium Ir and Mn (e.g., IrMn); alloys based on Fe and Mn (e.g., FeMn); alloys based on platinum Pt and Mn (e.g., PtMn); and alloys based on Ni and Mn (e.g., NiMn). The reference layer 23 can comprise one or a plurality of ferromagnetic layers or a synthetic antiferromagnet (SAF). The tunnel barrier 22 can comprise an insulating material. Suitable insulating materials include oxides, such as aluminum oxide (e.g., Al2O3) and magnesium oxide (e.g., MgO). A thickness of the tunnel barrier layer 22 can be in the nm range, such as from about 1 nm to about 3 nm. The magnetic sensor element 10 can further comprises a capping layer 25, for example an electrode.
The edge portion 215 can comprise a substantially flat edge formed by partially cutting out the periphery of the sense layer 21 at one side of the peripheral shape 214.
In the example of
The peripheral shape 214 can have an elliptical shape aspect ratio (or eccentricity) between 1 and 2. Note that the peripheral shape 214 need not be circular or elliptical but can have other shapes such as square or rectangular.
In one aspect illustrated in
In a preferred embodiment, the edge portion 215 is provided at one side of the peripheral shape 214, substantially perpendicular to an easy axis of the sense layer 21. In the example of
The edge portion 215 can be oriented substantially parallel to the orientation of the external magnetic field 60. For example, the sense layer 21 can be arranged such that the external magnetic field 60 is oriented substantially parallel to the edge portion 215. In
In an embodiment, a magnetic sensor device comprises a plurality of the magnetic sensor elements 10.
The presence of the edge portion 215 in the sense layer 21 induces an off-centred vortex core 211 which induces a hysteresis, or an intrinsic offset ΔMi at zero field strength. The intrinsic offset ΔMi due to the presence of the edge portion 215 can reach about ±20 Oe, depending on the direction of the external magnetic field 60.
Preferably, the magnetic sensor elements 10 are arranged in a regular array, for example arranged in a plurality of rows and at least one column wherein in each row, the edge portion 215 of a magnetic sensor element 10 is opposite to the edge portion 215 of the adjacent magnetic sensor element 10.
In some aspects, a distance d between two adjacent magnetic sensor elements 10 is between 10 nm and 50 nm. The distance d allows to maximize the magnetostatic interaction between adjacent sensor element 10. The magnetostatic interaction between two adjacent magnetic sensor elements 10 increases with diminishing distance d.
In an embodiment shown in
The magnetic sensor device 100 disclosed herein allows for increasing the measurement range and avoiding 2-vortex configurations. A two-vortex configuration consists of two vortices in a magnetic sensor element. It is generally a stable configuration for circular of elliptical sensor elements with large radius (or small axis) and a thick sense layer. The measurement range can be above the expulsion field of the vortex such that no hysteresis is observed when a high bias field is applied. Only field limitation left will be associated to the SAF reference layer 23. In other words, the field limitation will be associated to possible modification of magnetization in the SAF for high fields (rotation of uniform magnetization is SAF for high magnetic fields). The arrangement of the magnetic sensor elements 10 in the array 200, or subarray 100) reduces the averaged offset ΔMa by recentering the vortex core 211 at zero field in each magnetic sensor element 10.
The edge portion 215 may further result in the first and second displacement directions 212, 213 of the vortex core 211 (see
Number | Date | Country | Kind |
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21315054.3 | Mar 2021 | EP | regional |
Filing Document | Filing Date | Country | Kind |
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PCT/IB2022/052046 | 3/8/2022 | WO |