H03K19/18

Securing computing resources through multi-dimensional enchainment of mediated entity relationships
11710052 · 2023-07-25 ·

Synthesizing a control object for a computing event, the control object for securing a computing resource based on a set of access and privilege information provided through a set of mediated associations that are represented by an enchained set of certificates, portions of which are encrypted including entity-specific paths to entity-specific predecessor certificates and partial decryption keys therefor, wherein the control object is applied to secure the computing resource for performing a computing action indicated by a process-type entity identified in the certificate for the control object.

DIFFUSE IDENTITY MANAGEMENT IN TRANSPOSABLE IDENTITY ENCHAINMENT SECURITY

A transposable identity enchainment system for diffuse identity management processing entities for each of users, data, and processes equivalently and having a recombinant access mediation system that mediates association among entities, an associational process management system that creates entity-defining indices, and a multi-dimensional enchainment system that enchains aspects of entity identities via mediated association certificates including at least one root certificate for at least one of the entities.

Cyber security through generational diffusion of identities
11710050 · 2023-07-25 ·

Diffusing a root identity of an entity among association and event covenants in a multi-dimensional computing security system involves generating a first generation of diffusion of identities of entities participating in mediated association and generating a second generation of diffusion of identities of the entities through recombinant mediated association of the entities and at least one other entity. The second generation of diffusion of identities facilitates securely constraining a computing system action associated with one of the entities.

Reversible computing system and method based on conservative magnetic skyrmion logic

A skyrmion logic gate is provided. The logic gate comprises a first track configured for propagation of magnetic skyrmions and a second track configured for propagation of magnetic skyrmions. A junction links the first and second tracks. A continuous current flows through the logic gate, wherein skyrmions propagate due to the current.

MAGNETIC DEVICE AND ARITHMETIC DEVICE
20220399048 · 2022-12-15 · ·

According to one embodiment, a magnetic device includes first and second conductive portions, first and second stacked bodies, and a controller. The first conductive portion includes first to third region. The third region is between the first and second regions. The first stacked body includes first and second magnetic layers. The second magnetic layer is between the third region and the first magnetic layer. The second conductive portion includes fourth to sixth regions. The sixth region is between the fourth and fifth regions. The second stacked body includes third and fourth magnetic layers. The fourth magnetic layer is between the sixth region and the third magnetic layer. The first stacked body is configured to be in a first low or high electrical resistance state. The second stacked body is configured to be in a second low high electrical resistance state.

LOGIC GATES BASED ON PHASE SHIFTERS
20220392683 · 2022-12-08 ·

The disclosed technology relates to a logic device based on spin waves. In one aspect, the logic device includes a spin wave generator, a waveguide, at least two phase shifters, and an output port. The spin wave generator is connected with the waveguide and is configured to emit a spin wave in the waveguide. The at least two phase shifters are connected with the waveguide at separate positions such that, when a spin wave is emitted by the spin wave generator, it passes via the phase shifters. The at least two phase shifters are configured to change a phase of the passing spin wave. The output port is connected with the wave guide such that the at least two phase shifters are present between the spin wave generator and the output port.

MAGNETIC LOGIC DEVICE, CIRCUIT HAVING MAGNETIC LOGIC DEVICES, AND METHODS FOR CONTROLLING THE MAGNETIC LOGIC DEVICE AND THE CIRCUIT

A magnetic logic device having two magnetic elements and a conductive element coupled to the two magnetic elements and arranged at least substantially perpendicular to the magnetic elements, wherein the device is configured, for each magnetic element, to have a magnetisation state with a perpendicular easy axis, and to switch the magnetisation state in response to a spin current generated in the magnetic element in response to a write current applied to the magnetic element, and configured to generate, as an output, a Hall voltage across the conductive element in response to a respective read current applied to each magnetic element, wherein a magnitude of the Hall voltage is variable, depending on a direction of the magnetisation state of each magnetic element and a direction of the respective read current applied to each magnetic element, for the device to provide outputs corresponding to one of a plurality of logical operations.

MAGNETIC LOGIC DEVICE, CIRCUIT HAVING MAGNETIC LOGIC DEVICES, AND METHODS FOR CONTROLLING THE MAGNETIC LOGIC DEVICE AND THE CIRCUIT

A magnetic logic device having two magnetic elements and a conductive element coupled to the two magnetic elements and arranged at least substantially perpendicular to the magnetic elements, wherein the device is configured, for each magnetic element, to have a magnetisation state with a perpendicular easy axis, and to switch the magnetisation state in response to a spin current generated in the magnetic element in response to a write current applied to the magnetic element, and configured to generate, as an output, a Hall voltage across the conductive element in response to a respective read current applied to each magnetic element, wherein a magnitude of the Hall voltage is variable, depending on a direction of the magnetisation state of each magnetic element and a direction of the respective read current applied to each magnetic element, for the device to provide outputs corresponding to one of a plurality of logical operations.

Switching of perpendicularly magnetized nanomagnets with spin-orbit torques in the absence of external magnetic fields

A base element for switching a magnetization state of a nanomagnet includes a heavy-metal nanostrip having a surface. The heavy-metal nanostrip includes at least a first layer including a heavy metal and a second layer which includes a different heavy-metal. A ferromagnetic nanomagnet is disposed adjacent to the surface. The ferromagnetic nanomagnet includes a shape having a long axis and a short axis, the ferromagnetic nanomagnet having both a perpendicular-to-the-plane anisotropy H.sub.kz and an in-plane anisotropy H.sub.kx and the ferromagnetic nanomagnet having a first magnetization equilibrium state and a second magnetization equilibrium state. The first magnetization equilibrium state or the second magnetization equilibrium state is settable by a flow of electrical charge through the heavy-metal nanostrip. A direction of the flow of electrical charge through the heavy-metal nanostrip includes an angle ξ with respect to the short axis of the nanomagnet.

Switching of perpendicularly magnetized nanomagnets with spin-orbit torques in the absence of external magnetic fields

A base element for switching a magnetization state of a nanomagnet includes a heavy-metal nanostrip having a surface. The heavy-metal nanostrip includes at least a first layer including a heavy metal and a second layer which includes a different heavy-metal. A ferromagnetic nanomagnet is disposed adjacent to the surface. The ferromagnetic nanomagnet includes a shape having a long axis and a short axis, the ferromagnetic nanomagnet having both a perpendicular-to-the-plane anisotropy H.sub.kz and an in-plane anisotropy H.sub.kx and the ferromagnetic nanomagnet having a first magnetization equilibrium state and a second magnetization equilibrium state. The first magnetization equilibrium state or the second magnetization equilibrium state is settable by a flow of electrical charge through the heavy-metal nanostrip. A direction of the flow of electrical charge through the heavy-metal nanostrip includes an angle ξ with respect to the short axis of the nanomagnet.