Composite SOT-MTJ Memory for Ultra-Fast Low-Power Switching
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Solution Overview
Problem
Current spin-transfer torque (STT)-MRAM devices face issues with high voltage requirements for reading and writing, potential tunnel barrier breakdown, and increased readout errors due to fluctuations in electrical characteristics, especially at advanced technology nodes, which affect switching speed and reliability.
Innovation Solution
A composite SOT magnetic tunneling junction (CSOT-MTJ) element is introduced, comprising a magnetic flux guiding layer with high permeability, a spin Hall channel with a large positive spin Hall angle, an in-plane magnetic memory layer, a tunnel barrier layer, and a magnetic pinning stack, utilizing enhanced spin-orbit torque and Lorentz force to achieve ultra-fast magnetic writing, while reducing power consumption and eliminating the need for external magnetic fields through canted annealing or oval shaping.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If spin-transfer torque (STT) method is used to write magnetic memory, then magnetization switching can be achieved, but high voltage is required which may cause tunnel barrier breakdown
Solution Approach 1:
The patent introduces a spin Hall channel layer as an intermediary component between the current path and the magnetic tunnel junction. The charge current flows through the spin Hall channel which converts it to a transverse spin current via the spin Hall effect, which then acts on the recording layer. This intermediary mechanism allows writing without applying high voltage directly across the tunnel barrier, thus preventing breakdown while achieving magnetization switching.
Solution Approach 2:
The patent replaces the direct spin-transfer torque mechanism (which requires high voltage across the MTJ) with a spin-orbit torque mechanism utilizing the spin Hall effect. Instead of injecting spin-polarized current vertically through the tunnel barrier, a charge current is applied laterally through the spin Hall channel, generating spin current transverse to the current direction through the spin Hall effect. This substitution eliminates the high voltage requirement across the tunnel barrier.
2Measurement precision
If high voltage is applied to read MTJ resistance state, then accurate readout can be achieved, but the read current may inadvertently switch magnetization direction
Solution Approach 1:
The patent segments the read and write current paths. The write operation uses lateral current through the spin Hall channel, while the read operation uses vertical current through the MTJ stack. This segmentation allows independent optimization of read and write operations, enabling accurate readout without risking unintended magnetization switching that would occur with high voltage applied directly across the MTJ.
Solution Approach 2:
The spin Hall channel acts as an intermediary for write operations only, while read operations directly measure the MTJ resistance. This separation ensures that read currents, which are relatively low, do not trigger switching, while write currents are channeled through the spin Hall effect mechanism that is insensitive to the same stability constraints.
3Ease of operation
If conventional SOT-MRAM structure is used, then spin Hall effect can generate spin current, but external magnetic field is required for initial switching
Solution Approach 1:
The patent introduces a magnetic flux guiding layer with high magnetic permeability underneath the spin Hall channel, creating an asymmetric magnetic structure. This asymmetric configuration, combined with canted annealing or oval-shaped patterning of the recording layer, generates a uniaxial magnetic anisotropy that provides the necessary symmetry breaking for deterministic switching without external magnetic fields. The asymmetric structure guides magnetic flux preferentially in one direction, enabling field-free switching.
Solution Approach 2:
The patent changes the magnetic anisotropy parameters through canted annealing processes or geometric shaping (oval patterns) of the recording layer. By controlling the annealing temperature, magnetic field angle, or aspect ratio of the pattern, the magnetic energy landscape is modified to create a uniaxial anisotropy with an easy axis at a specific angle. This parameter change eliminates the need for external magnetic fields during operation, as the anisotropy itself provides the switching direction.
4Use of energy by moving object
If recording layer volume is reduced to lower writing current, then power consumption decreases, but thermal stability deteriorates
Solution Approach 1:
The patent applies local quality enhancement by introducing a magnetic flux guiding layer with high permeability in specific regions underneath the spin Hall channel. This localized structure concentrates and guides magnetic flux precisely where needed, enhancing the spin-orbit torque efficiency at the recording layer interface. The improved local magnetic field concentration allows for more effective magnetization switching with lower currents, enabling smaller recording layer volumes without sacrificing thermal stability.
Solution Approach 2:
The patent employs composite material structures including the spin Hall channel made of high-Z materials (Pt, β-Ta, β-W, doped Cu) with large spin Hall angles, combined with the recording layer and magnetic flux guiding layer. This composite structure leverages the high spin Hall angle material to generate stronger spin currents from the same charge current, improving switching efficiency and allowing reduced recording layer volume while maintaining thermal stability through the enhanced spin-orbit coupling.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
The CSOT-MTJ element enables ultra-fast switching with reduced power consumption and improved thermal stability, minimizing magnetic stray fields and allowing for high-speed, low-power operation suitable for cache applications in CPUs, GPUs, and TPUs without the need for external magnetic fields.
Implementation Method 1
It has been known that a spin current can, alternatively, be generated in non-magnetic transition metal material by a so-called Spin Hall Effect (SHE), in which spin-orbit coupling causes electrons with different spins to deflect in different directions yielding a pure spin current transverse to an applied charge current.
Implementation Method 2
A magnetic flux guide underneath a spin Hall channel is disclosed. The magnetic flux guide enhances the spin-orbit torque effect for easier switch
Implementation Method 3
An ultra-fast magnetic writing (recording) is achieved by a combined effort of enhanced spin orbit torque (SOT) in the SHC, Lorentz force generated by current-flowing wire (CFW) of the SHC
Implementation Method 4
Two methods of symmetry-breaking can be used to avoid using an external magnetic field for initial switch: In the first method, as-deposited CSOT-MTJ film stack is annealed with a magnetic field aligning at a canted angle in X-Y plane, while in the second method, the CSOT-MTJ recording cell is patterned into an oval shape with its long axis aligning at a canted angle in X-Y plane.
Data Source
AI summary
An ultra-fast magnetic random access memory (MRAM) comprises a three terminal composite SOT magnetic tunneling junction (CSOT-MTJ) element including a magnetic flux guide (MFG) having a very high magnetic permeability, a spin Hall channel (SHC) having a large positive spin Hall angle, an in-plane magnetic memory (MM) layer, a tunnel barrier (TB) layer, and a magnetic pinning stack (MPS) having a synthetic antiparallel coupling pinned by an antiferromagnetic material. The magnetic writing is significantly boosted by a combined effort of enhanced spin orbit torque (SOT) and Lorentz force generated by current-flowing wire (CFW) in the SHC layer and spin transfer torque (STT) by a current flowing through the MTJ stack, and further enhanced by a magnetic close loop formed at the cross section of MFG/SHC/MM tri-layer.


