1. Field of the Invention
This invention relates generally to a three terminal magnetic-random-access memory (MRAM) cell, more particularly to methods of fabricating three terminal MRAM memory elements having ultra-small dimensions.
2. Description of the Related Art
In recent years, magnetic random access memories (hereinafter referred to as MRAMs) using the magnetoresistive effect of ferromagnetic tunnel junctions (also called MTJs) have been drawing increasing attention as the next-generation solid-state nonvolatile memories that can also cope with high-speed reading and writing. A ferromagnetic tunnel junction has a three-layer stack structure formed by stacking a recording layer having a changeable magnetization direction, an insulating tunnel barrier layer, and a fixed layer that is located on the opposite side from the recording layer and maintains a predetermined magnetization direction. Corresponding to the parallel and anti-parallel magnetic states between the recording layer magnetization and the reference layer magnetization, the magnetic memory element has low and high electrical resistance states, respectively. Accordingly, a detection of the resistance allows a magnetoresistive element to provide information stored in the magnetic memory device.
There has been a known technique for achieving a high MR ratio by forming a crystallization acceleration film that accelerates crystallization and is in contact with an interfacial magnetic film having an amorphous structure. As the crystallization acceleration film is formed, crystallization is accelerated from the tunnel barrier layer side, and the interfaces with the tunnel barrier layer and the interfacial magnetic film are matched to each other. By using this technique, a high MR ratio can be achieved.
Typically, MRAM devices are classified by different write methods. A traditional MRAM is a magnetic field-switched MRAM utilizing electric line currents to generate magnetic fields and switch the magnetization direction of the recording layer in a magnetoresistive element at their cross-point location during the programming write. A spin-transfer torque (or STT)-MRAM has a different write method utilizing electrons' spin momentum transfer. Specifically, the angular momentum of the spin-polarized electrons is transmitted to the electrons in the magnetic material serving as the magnetic recording layer. According to this method, the magnetization direction of a recording layer is reversed by applying a spin-polarized current to the magnetoresistive element. As the volume of the magnetic layer forming the recording layer is smaller, the injected spin-polarized current to write or switch can be also smaller.
Besides a write current, the stability of the magnetic orientation in a MRAM cell as another critical parameter has to be kept high enough for a good data retention, and is typically characterized by the so-called thermal factor which is proportional to the energy barrier as well as the volume of the recording layer cell size.
To record information or change resistance state, typically a recording current is provided by its CMOS transistor to flow in the stacked direction of the magnetoresistive element, which is hereinafter referred to as a “vertical spin-transfer method.” Generally, constant-voltage recording is performed when recording is performed in a memory device accompanied by a resistance change. In a STT-MRAM, the majority of the applied voltage is acting on a thin oxide layer (tunnel barrier layer) which is about 10 angstroms thick, and, if an excessive voltage is applied, the tunnel barrier breaks down. More, even when the tunnel barrier does not immediately break down, if recording operations are repeated, the element may still become nonfunctional such that the resistance value changes (decreases) and information readout errors increase, making the element un-recordable. Furthermore, recording is not performed unless a sufficient voltage or sufficient spin current is applied. Accordingly, problems with insufficient recording arise before possible tunnel barrier breaks down.
In the mean time, since the switching current requirements reduce with decreasing MTJ element dimensions, STT-MRAM has the potential to scale nicely at even the most advanced technology nodes. However, patterning of small MTJ element leads to increasing variability in MTJ resistance and sustaining relatively high switching current or recording voltage variation in a STT-MRAM.
Reading STT MRAM involves applying a voltage to the MTJ stack to discover whether the MTJ element states at high resistance or low. However, a relatively high voltage needs to be applied to the MTJ to correctly determine whether its resistance is high or low, and the current passed at this voltage leaves little difference between the read-voltage and the write-voltage. Any fluctuation in the electrical characteristics of individual MTJs at advanced technology nodes could cause what was intended as a read-current, to have the effect of a write-current, thus unintentionally reversing the direction of magnetization of the recording layer in MTJ.
Above issues or problems are all associated with the traditional two-terminal MRAM configuration. Thus, it is desirable to provide robust STT-MRAM structures and methods that realize highly-accurate reading, highly-reliable recording and low power consumption while suppressing destruction and reduction of life of MTJ memory device due to recording in a nonvolatile memory that performs recording resistance changes, and maintaining a high thermal factor for a good data retention.
The present invention comprises methods of making a low power spin-transfer-torque MRAM comprising a three terminal magnetoresistive memory cell, which has three terminals: an upper electrode connected to a bit line, a middle electrode connected to a select transistor and a digital line as a bottom electrode wherein an MTJ stack is sandwiched between an upper electrode and a middle electrode, a dielectric functional layer is sandwiched between a middle electrode and a digital line of each MRAM memory cell.
The memory cell further includes a circuitry coupled to the bit line positioned adjacent to selected ones of the plurality of magnetoresistive memory elements to supply a reading current or bi-directional spin polarized current to the MTJ stack, and coupled to the digital line configured to generate an electric field on the functional layer and accordingly to decrease the switching energy barrier of the recording layer. Thus magnetization of a recording layer can be readily switched or reversed to the direction in accordance with a direction of a current across the MTJ stack by applying a low spin transfer current.
The fabrication method of the MRAM cell includes formation of bottom electrode, formation of middle electric connecting layer, formation of magnetic memory cell and formation of top electrode and bit line, by repeated film deposition, photolithography patterning, etching, dielectric refilling and chemical mechanic lapping, in which metallic ion implantation is used to convert the isolated middle layers into electrically conducting layer to allow the current flow between middle magnetic recording layer and bottom electrode.
The exemplary embodiment will be described hereinafter with reference to the companying drawings. The drawings are schematic or conceptual, and the relationships between the thickness and width of portions, the proportional coefficients of sizes among portions, etc., are not necessarily the same as the actual values thereof.
a cross section view of the bottom connection layer formed in the open space;
In general, there is provided a magnetoresistive memory cell comprising:
A dielectric functional layer is made of a metal oxide (or nitride, chloride) layer having a naturally stable rocksalt crystal structure having the (100) plane parallel to the substrate plane and with lattice parameter along its {110} direction being larger than the bcc(body-centered cubic)-phase Co lattice parameter along {100} direction. As an amorphous ferromagnetic material, like CoFeB, in the recording layer is thermally annealed, a crystallization process occurs to form bcc CoFe grains having epitaxial growth with (100) plane parallel to surface of the rocksalt crystal functional layer.
In a rocksalt crystal structure of a functional layer, such as MgO, two fcc sublattices for metal atoms and O atoms, each displaced with respect to the other by half lattice parameter along the [100] direction. However, at a surface, O atoms protrude while metal atoms retreat slightly from the surface, forming a strong interface interaction with the bcc CoFe grains. Accordingly, a perpendicular anisotropy and a perpendicular magnetization are induced in the recording layer, as a result of the strong interface interaction between the recording layer and the functional layer.
Further, as an electric field is applied on the functional layer and perpendicular to the surface, the negative charged O atoms and positive charged metal atoms at surface are pulled toward opposite directions and modify the interface interaction between the bcc CoFe grains in the soft adjacent layer and the rocksalt crystal grains in the functional layer. When an electric field points down towards the top surface of a functional layer, O atoms protrude more from the surface and form a stronger interface interaction with the bcc CoFe grains, causing an enhanced perpendicular anisotropy, and vice versa. This mechanism is utilized hereafter to manipulate the perpendicular anisotropy strength and magnetization direction of the recording layer through applying an electric field on the dielectric functional layer.
An exemplary embodiment includes method of fabricating a spin-transfer-torque magnetoresistive memory including a circuitry coupled to the bit line positioned adjacent to selected ones of the plurality of magnetoresistive memory elements to supply a reading current or bi-directional spin-transfer recording current, and coupled to the digital line configured to generate an electric field on the functional layer and accordingly to manipulate the perpendicular anisotropy strength of the recording layer. Thus magnetization of a recording layer can be readily switched or reversed to the direction in accordance with a direction of a current across the MTJ stack by applying a low spin transfer current.
The following detailed descriptions are merely illustrative in nature and are not intended to limit the embodiments of the subject matter or the application and uses of such embodiments. Any implementation described herein as exemplary is not necessarily to be construed as preferred or advantageous over other implementations. Furthermore, there is no intention to be bound by any expressed or implied theory presented in the preceding technical field, background, brief summary, or the following detailed description.
A fabrication process to form such a three-terminal memory device is shown in the process flow chart in
By photolithography patterning, etch, dielectric refill of a SiO2 layer 240 and CMP, as shown in
Another photolithography patterning and etch are used to open a space down to the bottom electrode, as shown 370 in
Then the memory cell film stack 400 is deposited, as shown in
A single or dual photolithography patterning and etch is used to form a small Ta hard mask pillar 460 using a chemical gas (such as CF4) followed by oxygen ashing of the remaining photoresist and RIE redep. Then a chemical gas of CH3OH or CO/NH4 is used to etch the top Ru cap layer 450 and magnetic reference layer 440 and stops in the middle of MgO 430 using the just created Ta hard mask pillar. Immediately after etch, an insulating layer ILD 470 is deposited to conformally cover the exposed MgO junction edge and the entire flat surface, as shown in
Due to the presence of the ILD layer 410, the recording layer 420 is isolated from the top metal surface of the digital line. In order to connect the recording layer to the underneath bottom electrode, the ILD layer 410 outside the memory pillar must be conductive, which can be done by metal ion implantation to convert the isolated film stack (410-420,430) on the exposed surface outside the memory pillar into a thick conductive layer 480 (
To create an isolated middle conductive base, a photolithography patterning is used to cover the middle memory area before removing the outside conductive surface by etching. After etch, the surface is refilled with dielectric SiO2 layer 490 and CMP to flatten the surface, as shown in
Finally, the top bit line is formed by depositing 5 nm Ta layer 510/50 nm Ru layer 520/10 nm Ta layer 530, patterning, etch, dielectric SiO2 refill and CMP as shown in
While certain embodiments have been described above, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
This application claims the priority benefit of U.S. Provisional Application No. 61,771,857 filed on Mar. 3, 2013, which is incorporated herein by reference.
Number | Date | Country | |
---|---|---|---|
61771857 | Mar 2013 | US |