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.
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.
It is known that perpendicular magnet (PM) spin transfer torque magnetic random access memory pSTT-MRAM) is an ideal memory for future semiconducting device. Current STT-MRAM is a two-terminal device with magnetic memory layer and reference layer separated by a thin MgO dielectric layer to form a so-called magnetic tunneling junction (MTJ). The shortcomings of such two-terminal pSTT-MRAM are its large critical write current and narrow current separation between read and write process. It has been recently reported that by applying a bias voltage across the MTJ junction with a right polarization could reduce the Hc of the magnetic layer adjacent to the MgO layer. A so-called voltage-controlled pSTT-MRAM has been proposed [W.-G. Wang et al., Natural Materials, Vol. 11, 64, 2012].
The present invention comprises methods of making a low power spin-transfer-torque MRAM comprising 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.
The three-terminal spin transistor magnetic random access memory (
The fabrication process flow is shown in
By photolithography patterning, etch, dielectric refill (SiO2, 240) and CMP (
Then, a film stack (300) of ILD (310)/Ta(320)/metal(330)/Ta(340)/metal(350)/Ta(360) is deposited (
Then, a dielectric layer (SiO2, 410) is refilled in the etched area and flattened by CMP to cover the entire surface (
Then the memory cell film stack is deposited [
A dual photolithography patterning and etch (see our own U.S. patent application Ser. No. 14/170,645) is used to form a small Ta hard mask pillar (460) using C,H,F containing 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 (450) cap 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 [
Due to the presence of the ILD (410), the middle magnetic memory layer (420) is isolated from the top metal surface of VIA connecting to the bottom CMOS. In order to connect the middle memory layer to the underneath CMOS device, the ILD (410) outside the memory pillar must be conductive, which can be done by metal implantation to convert the isolated film stack (410-420,430) on the exposed surface outside the memory pillar into a thick conductive layer (480). Selection of metal for implantation can be Au, Ag, Cu, Ru, Li. After ion implantation, a high temperature anneal (>200 C) is needed to repair the film structure damage.
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 (
Finally, the top bit line is formed by deposition 50Ta (510)/500Ru(520)/100Ta(530), patterning, etch, dielectric (SiO2) refill and CMP, which has a magnetic memory cell sitting on a large VIA base in the middle and a digital line at the bottom with a metal pillar pointing towards the memory cell and a bit line on the top across each other (
This application claims the priority benefit of U.S. Provisional Application No. 61/834,562 filed on Jun. 13, 2013, which is incorporated herein by reference.