Abstract: Magnetic tunnel junction transistor devices and methods for operating and forming magnetic tunnel junction transistor devices. In one aspect, a magnetic tunnel junction transistor device includes a first source/drain electrode, a second source/drain electrode, a gate electrode, and a magnetic tunnel junction disposed between the gate electrode and the second source/drain electrode. The magnetic tunnel junction includes a magnetic free layer that extends along a length of the gate electrode toward the first source/drain electrode such that an end portion of the magnetic free layer is disposed between the gate electrode and the first source/drain electrode. The magnetic tunnel junction transistor device switches a magnetization orientation of the magnetic free layer by application of a gate voltage to the gate electrode, thereby changing a resistance between the first and second source/drain electrodes through the magnetic free layer.

Abstract: A magnetic circuit in one aspect comprises a plurality of tapered magnetic wires each having a relatively wide input end and a relatively narrow output end, with the output end of a first one of the tapered magnetic wires being coupled to the input end of a second one of the tapered magnetic wires. Each of the tapered magnetic wires is configured to propagate a magnetic domain wall along a length of the wire in a direction of decreasing width from its input end to its output end. In an illustrative embodiment, the magnetic circuit comprises a logic buffer that includes at least one heating element. The heating element may be controlled to facilitate transfer of a magnetic moment from the output end of the first tapered magnetic wire to the input end of the second tapered magnetic wire.

Abstract: Magnetoresistive structures, devices, memories, and methods for forming the same are presented. For example, a magnetoresistive structure includes a ferromagnetic layer, a ferrimagnetic layer coupled to the ferromagnetic layer, a pinned layer and a nonmagnetic spacer layer. A free side of the magnetoresistive structure comprises the ferromagnetic layer and the ferrimagnetic layer. The nonmagnetic spacer layer is at least partly between the free side and the pinned layer. A saturation magnetization of the ferromagnetic layer opposes a saturation magnetization of the ferrimagnetic layer. The nonmagnetic spacer layer may include a tunnel barrier layer, such as one composed of magnesium oxide (MgO), or a nonmagnetic metal layer.

Abstract: A magnetic tunnel junction stack that includes a pinned magnetic layer, a tunnel barrier layer formed of magnesium oxide (MgO), and a free magnetic layer formed adjacent to the tunnel barrier layer and of a material having a magnetization perpendicular to an MgO interface of the tunnel barrier layer and with a magnetic moment per unit area within a factor of 2 of approximately 2 nanometers (nm)×300 electromagnetic units per cubic centimeter (emu/cm3).

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: A magnetic circuit in one aspect comprises a plurality of tapered magnetic wires each having a relatively wide input end and a relatively narrow output end, with the output end of a first one of the tapered magnetic wires being coupled to the input end of a second one of the tapered magnetic wires. Each of the tapered magnetic wires is configured to propagate a magnetic domain wall along a length of the wire in a direction of decreasing width from its input end to its output end. In an illustrative embodiment, the magnetic circuit comprises a logic buffer that includes at least one heating element. The heating element may be controlled to facilitate transfer of a magnetic moment from the output end of the first tapered magnetic wire to the input end of the second tapered magnetic wire.

Abstract: Techniques for exchange coupling of magnetic layers in semiconductor devices are provided. In one aspect, a semiconductor device is provided. The device comprises at least two magnetic layers, and a spacer layer formed between the magnetic layers, the spacer layer being configured to provide ferromagnetic exchange coupling between the layers, the magnetic layers experiencing anti-ferromagnetic dipole coupling, such that a net coupling of the magnetic layers is anti-ferromagnetic in a zero applied magnetic field. The semiconductor device may comprise magnetic random access memory (MRAM). In another aspect, a method for coupling magnetic layers in a semiconductor device comprising at least two magnetic layers and a spacer layer therebetween, the method comprises the following step.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Magnetoresistive structures, devices, memories, and methods for forming the same are presented. For example, a magnetoresistive structure includes a ferromagnetic layer, a ferrimagnetic layer coupled to the ferromagnetic layer, a pinned layer and a nonmagnetic spacer layer. A free side of the magnetoresistive structure comprises the ferromagnetic layer and the ferrimagnetic layer. The nonmagnetic spacer layer is at least partly between the free side and the pinned layer. A saturation magnetization of the ferromagnetic layer opposes a saturation magnetization of the ferrimagnetic layer. The nonmagnetic spacer layer may include a tunnel barrier layer, such as one composed of magnesium oxide (MgO), or a nonmagnetic metal layer.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.

Abstract: Techniques for data storage are provided. In one aspect, a method for writing one or more magnetic memory cells comprises the following steps. Data is written to one or more of the magnetic memory cells. It is detected whether there are any errors in the data written to the one or more magnetic memory cells. The data is rewritten to each of the one or more previously written magnetic memory cells in which an error is detected.

Abstract: Apparatus and methods for optimizing a toggle window for a magnetic tunnel junction (MTJ) having a multicomponent free layer are provided. In accordance with an aspect of the invention, a MTJ comprises a free layer, a pinned layer, and a barrier layer formed between the free layer and the pinned layer. The free layer, in turn, includes a plurality of free magnetic sublayers while the pinned layer includes a plurality of pinned magnetic sublayers. Each of the pinned magnetic sublayers exerts a magnetic field on the free magnetic sublayers. To optimize the toggle window for the device, the dimensions of each of the pinned magnetic sublayers are selected to substantially equalize average magnetic fields acting on each of the free magnetic sublayers.

Abstract: The present invention provides techniques for data storage. In one aspect of the invention, a semiconductor device is provided. The semiconductor device comprises at least one free layer and at least one fixed layer, with at least one barrier layer therebetween. At least one pinned magnetic layer is separated from the at least one free layer by at least one non-magnetic layer, the at least one pinned magnetic layer and non-magnetic layer being configured to cancel out at least a portion of a Neel coupling between the at least one free layer and the at least one fixed layer.

Abstract: Techniques for improved semiconductor device performance are provided. In one aspect, a semiconductor device is provided. The device comprises at least one free magnetic layer, and a magnetic amplifier interacting with the free magnetic layer comprising two or more magnetic layers with at least one nonmagnetic layer therebetween. The nonmagnetic layer may be configured to provide parallel exchange coupling J of the magnetic layers in a range of 0 < J < 4 ? ? ? ? t 2 ? M S 2 ? n y b , the magnetic layers having a long axis and a short axis, wherein t is a thickness of each magnetic layer, Ms is magnetization, ny is a demagnetizing factor defined along the short axis of the magnetic layers and b is a diameter along a short axis of the magnetic layers. A method for switching a semiconductor device having at least one free magnetic layer is also provided.

Abstract: Probes are electrically connected to a surface of a tunnel junction film stack comprising a free layer, a tunnel barrier, and a pinned layer. Resistances are determined for a variety of probe spacings and for a number of magnetizations of one of the layers of the stack. The probe spacings are a distance from a length scale, which is related to the Resistance-Area (RA) product of the tunnel junction film stack. Spacings from as small as possible to about 40 times the length scale are used. Beneficially, the smallest spacing between probes used during a resistance measurement is under 100 microns. A measured in-plane MagnetoResistance (MR) curve is determined from the “high” and “low” resistances that occur at the two magnetizations of this layer. The RA product, resistances per square of the free and pinned layers, and perpendicular MR are determined through curve fitting.