The present disclosure concerns a self-referenced magnetic random access memory (MRAM) element having a field line adapted to provide an improved magnetic field. The present disclosure further concerns a self-referenced MRAM device comprising the MRAM elements.
Self-referenced MRAM devices comprise a plurality of MRAM cells sharing common conducting lines. In particular, the plurality of MRAM cells can share a field line being arranged for passing a field current for generating a magnetic field destined to the writing of the MRAM cells and/or to the reading of the MRAM cells.
In the above configurations of self-referenced MRAM elements, a magnetic field generated by the field current passing in the field line 5 varies a magnetoresistance of the magnetic tunnel junction 2, such that the MRAM element 1 can be written or read. Writing and/or reading the MRAM element requires passing the field current with a magnitude being high enough for the generated magnetic field to be able to vary/switch a magnetization of the magnetic tunnel junction 2. Indeed, the magnetic field should have a magnitude being typically comprised between 0 and 200 Oe, and preferably between 50 and 100 Oe.
In low power application, such as in mobile devices, high field currents are detrimental. The same applies for applications requiring a MRAM device having a high surface density of MRAM elements where high magnetic fields must be generated by small field lines.
Obtaining a self-referenced MRAM element and device wherein the field line is capable of generating a larger magnetic field for a given field current would thus be advantageous.
The present disclosure concerns a self-reference-based MRAM element comprising a first magnetic tunnel junctions and a second magnetic tunnel junctions, each having a magnetoresistance that can be varied; and a field line for passing a field current destined to vary the magnetoresistance of the first and second magnetic tunnel junctions; the field line comprising a first branch and a second branch electrically connected in parallel with the first branch, the first branch being arranged for passing a first portion of the field current to selectively vary the magnetoresistance of the first magnetic tunnel junction, and the second branch being arranged for passing a second portion of the field current to selectively vary the magnetoresistance of the second magnetic tunnel junction.
In an embodiment, the first and second branches can be arranged so that a first portion of magnetic field generated by passing the first portion of field current in the first branch can only vary the magnetization of the first magnetic tunnel junction, and a second portion of magnetic field generated by passing the second portion of field current in the second branch can only vary the magnetization of the second magnetic tunnel junction.
In another embodiment, each of the first and second branches can comprise a cladding. Each of the first and second branches can have a rectangular cross section, and the cladding can be comprised on three sides of the rectangular cross section. The cladding can comprise a ferromagnetic material such as a NiFeCo alloy.
In yet another embodiment, the MRAM element can further comprise at least one current line electrically connected to one end each of the first and second magnetic tunnel junctions.
The present disclosure also concerns a MRAM device comprising a plurality of the MRAM elements. The plurality of the MRAM elements can be arranged in rows and columns, and the field line can extend along a row of MRAM elements with the first branch extending along the first magnetic tunnel junctions such as to selectively vary the magnetoresistance of the first magnetic tunnel junction of the MRAM elements in the row when the first portion of the field current is passed. The second branch can extend along the second magnetic tunnel junctions such as to selectively vary the magnetoresistance of the second magnetic tunnel junction of the MRAM elements in the row when the second portion of the field current is passed.
The disclosed self-referenced MRAM element and MRAM device can use a reduced field current in comparison to the one used in conventional self-referenced MRAM elements and devices. The magnetoresistance of the first and second magnetic tunnel junctions can also be varied with increased selectivity.
The disclosure will be better understood with the aid of the description of an embodiment given by way of example and illustrated by the figures, in which:
The field line 5 comprises a first branch 5′ and a second branch 5″ electrically connected in parallel with the first branch 5′. The first branch 5′ is arranged for passing a first portion 51′ of the field current and the second branch 5″ is arranged for passing a second portion 51″ of the field current. In this arrangement, the first portion 51′ of the field current generates a first portion 52′ of magnetic field that is capable of switching the first magnetization of the first ferromagnetic layer (or the second magnetization of the second ferromagnetic layer), such as to vary the magnetoresistance of the first magnetic tunnel junction 2. Similarly, the second portion 51″ of the field current generates a second portion 52″ of magnetic field that is capable of varying the magnetoresistance of the second magnetic tunnel junction 2′. Preferably, the first and second branches 5′, 5″ are arranged so that the first portion 52′ of magnetic field generated by passing the first portion 51′ of field current in the first branch 5′ can only vary the magnetization of the first magnetic tunnel junction 2, and the second portion 52″ of magnetic field generated by passing the second portion 51″ of field current in the second branch 5″ can only vary the magnetization of the second magnetic tunnel junction 2′.
In the configuration of
The MRAM element 1 can further comprise a current line 3 connected to the other end of the first and second magnetic tunnel junction 2, 2′. In
In a preferred embodiment, at least a portion of each of the first and second branches 5′, 5″ comprise a cladding 6. In the particular example of
For an uncladded field line, the magnetic field H is given by the equation H=I/2 w, where I is the current flowing through the branch 5′, 5″ and w is the width of the branch 5′, 5″. Here, the field loss caused by the finite thickness of the branch is ignored. For the branch 5′, 5″ being cladded on three sides as in the example of
In a variant of the embodiment, the cladding can comprise a soft ferromagnetic material. The soft ferromagnetic material can include ferromagnetic materials that have high magnetic permeability, such as NiFeCo alloys. With a high permeability, the cladding magnetization rotates in response to the generated magnetic field which enables the focusing and enhancement of the magnetic field 52′, 52″ in the portion of the branch 5′, 5″ comprising the cladding 6. Moreover, in the region of the first and second magnetic tunnel junctions 2, 2′, the magnetic field 52′, 52″ has a component being substantially parallel to the plan of the ferromagnetic layer magnetization being written (or read).
Number | Date | Country | Kind |
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12290360 | Oct 2012 | EP | regional |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2013/071357 | 10/11/2013 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2014/063938 | 5/1/2014 | WO | A |
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Number | Date | Country | |
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20150287764 A1 | Oct 2015 | US |