Abstract: A modular potentiometer includes a magnetic block slide unit including a slide and a magnetic block disposed on the slide; a magnetic field sensing unit parallel to the magnetic block slide unit and including at least one Hall device and a circuit board electrically connected to the at least one Hall device, wherein the circuit board is modularized so that portions thereof are connected in series; a signal processing unit electrically connected to the magnetic field sensing unit to receive a sensing signal from the magnetic field sensing unit and thereby calculate a distance traveled by the magnetic block. Hence, due to the aforesaid segmental design, the non-contact potentiometer is easy to manufacture, mount, demount, and carry, and its manufacturing cost is reduced by modularizaton.

Abstract: A sensor arrangement for measuring a rotor position of an electric motor, in particular of a motor vehicle control device, wherein the sensor arrangement is constructed as a sensor arrangement operating without contact, which includes at least one permanent magnet and at least one magnetic field sensor, wherein the permanent magnet has at least one depression in at least one top surface facing the magnetic field sensor. A magnetization device for magnetizing a permanent magnet of the sensor arrangement is also disclosed. The use of the sensor arrangement in a motor vehicle control device of a braking system of a motor vehicle is also disclosed.

Abstract: An elongated pressure sensitive potentiometer is disposed alongside and generally parallel to a reciprocating suspension component, such as a shock absorber, and between a steel track and a rolling or static magnet. The track and contained potentiometer extend from a mount at or near the top of a cylinder of the shock absorber to a point beyond the magnet when the shock absorber is in an uncompressed state. The mount couples the track to the shaft, parallel to and spaced apart from the shaft. Magnet attraction of the track compresses the potentiometer between the track and magnet.

Abstract: An angle detecting device includes a rotatably supported magnet, and a magnetic sensor disposed opposite to the magnet. An output of the magnetic sensor is changed based on a magnetic flux change due to a rotation of the magnet. The magnet is disposed such that a distance between the magnetic sensor and the magnet is changed by the rotation of the magnet.

Abstract: A gyrator for AC signals was developed. This gyrator comprises a Hall effect material, means for permeating this Hall effect material with a magnetic field that is perpendicular to the plane or surface of the material, at least one input port for coupling an alternating current (I1; I2) into the Hall effect material, and at least one output port for outcoupling an output voltage (U2; U1) which is a measure of the Hall voltage generated by the incoupled alternating current. Each of these ports has at least two terminals, which are connected to the outside. At least one terminal of each port is connected to a connecting electrode, which is electrically insulated from the Hall effect material and forms a capacitor together with the Hall effect material. The alternating current is thus capacitively coupled into the Hall effect material, and the output voltage is capacitively coupled out of the Hall effect material.

Abstract: A sensor includes a Hall-effect probe fastened only by way of its connection pins and includes a sensing element, a magnet having a cavity having a base, and in which cavity the sensing element is housed, and a cylindrical hole having an axis and which extends from the base toward the interior of the magnet, the Hall-effect probe being capable of moving inside the cavity.

Abstract: A Hall effect transducer in a semiconductor wafer comprises a first layer of semiconducting material, a second layer of semiconducting material, and a contact structure configured to provide a path for electrical current to pass through the second layer. The second layer has higher electron hole mobility than the first layer, and is epitaxially grown atop the first layer.

Abstract: A method of forming a magnetic tunnel junction device is disclosed that includes forming a trench in a substrate, the trench including a first sidewall, a second sidewall, a third sidewall, a fourth sidewall, and a bottom wall. The method includes depositing a first conductive material within the trench proximate to the first sidewall and depositing a second conductive material within the trench. The method further includes depositing a magnetic tunnel junction (MTJ) structure within the trench. The MTJ structure includes a fixed magnetic layer having a magnetic field with a fixed magnetic orientation, a tunnel junction layer, and a free magnetic layer having a magnetic field with a configurable magnetic orientation. The method further includes selectively removing a portion of the MTJ structure that is adjacent to the fourth sidewall to create an opening such that the MTJ structure is substantially u-shaped.

Abstract: A semiconductor device includes a Hall element, which is switched between a first and second mode. In the first mode, connection A between a first and second resistor and connection C between a third and fourth resistor are set to Vcc or GND. Connection D between the first and fourth resistor and connection B between the second and third resistor are set as output terminals. In the second mode, D and B are set to Vcc or GND and A and C are set as output terminals. When a first line placed along the second resistor and connected to A is set at Vcc in the first mode, a second line placed along the fourth resistor and connected to D is set at Vcc in the second mode. When the first line is set at GND in first mode, the second line is set at GND in the second mode.

Abstract: According to one embodiment, a magnetic memory element includes a stacked body and a conductive shield. The stacked body includes first and second stacked units. The first stacked unit includes first and second ferromagnetic layers and a first nonmagnetic layer. The first ferromagnetic layer has a fixed magnetization in a first direction. A magnetization direction of the second ferromagnetic layer is variable in a second direction. The first nonmagnetic layer is provided between the first and second ferromagnetic layers. The second stacked unit includes a third ferromagnetic layer stacked with the first stacked unit in a stacking direction of the first stacked unit. A magnetization direction of the third ferromagnetic layer is variable in a third direction. The conductive shield is opposed to at least a part of a side surface of the second stacked unit. An electric potential of the conductive shield is controllable.

Abstract: A tunneling magneto-resistor reference unit for sensing a magnetic field includes a first MTJ (magnetic tunneling junction) device and a second MTJ device connected in parallel. The first MTJ device has a first pinned layer having a first pinned magnetization at a pinned direction, and a first free layer having a first free magnetization parallel to the pinned direction in a zero magnetic field. The second MTJ device has a second pinned layer having a second pinned magnetization at the pinned direction, and a second free layer having a second free magnetization anti-parallel to the pinned direction in a zero magnetic field. Major axes of the first and second MTJ devices have an angle of 45 degrees to a direction of an external magnetic field when sensed.

Abstract: A Hall sensor has a P-type semiconductor substrate and a Hall sensing portion having a square shape and an N-type conductivity disposed on a surface of the semiconductor substrate. The Hall sensor includes Hall voltage output terminals having the same shape with each other, and control current input terminals having the same shape with each other. The Hall voltage output terminals are disposed at respective ones of four vertices of the Hall sensing portion. The control current input terminals include pairs of control current input terminals disposed at respective ones of the four vertices of the Hall sensing portion and arranged on both sides of respective ones of the Hall voltage output terminals in spaced apart relation from the Hall voltage output terminals so as to prevent electrical connection between the control current input terminals and the Hall voltage output terminals.

Abstract: Provided is a magnetic tunneling junction device including a first structure including a magnetic layer; a second structure including at least two extrinsic perpendicular magnetization structures, each including a magnetic layer and; a perpendicular magnetization inducing layer on the magnetic layer; and a tunnel barrier between the first and second structures.

Abstract: The present disclosure concerns a magnetic random access memory MRAM cell comprising a tunnel magnetic junction formed from a first ferromagnetic layer, a second ferromagnetic layer having a second magnetization that can be oriented relative to an anisotropy axis of the second ferromagnetic layer at a predetermined high temperature threshold, and a tunnel barrier; a first current line extending along a first direction and in communication with the magnetic tunnel junction; the first current line being configured to provide an magnetic field for orienting the second magnetization when carrying a field current; wherein the MRAM cell is configured with respect to the first current line such that when providing the magnetic field, at least a component of the magnetic field is substantially perpendicular to said anisotropy axis. The MRAM cell has an improved switching efficiency, lower power consumption and improved dispersion of the switching field compared to conventional MRAM cells.

Abstract: A method and system provide a magnetic junction usable in a magnetic device. The magnetic junction includes a pinned layer, a nonmagnetic spacer layer, and a free layer. The nonmagnetic spacer layer is between the pinned layer and the free layer. The magnetic junction is configured such that the free layer is switchable between a plurality of stable magnetic states when a write current is passed through the magnetic junction. At least one of the free layer and the pinned layer include at least one half-metal.

Abstract: A magnetic tunnel junction (MTJ) includes a magnetic free layer, having a variable magnetization direction; an insulating tunnel barrier located adjacent to the free layer; a magnetic fixed layer having an invariable magnetization direction, the fixed layer disposed adjacent the tunnel barrier such that the tunnel barrier is located between the free layer and the fixed layer, wherein the free layer and the fixed layer have perpendicular magnetic anisotropy; and one or more of: a composite fixed layer, the composite fixed layer comprising a dusting layer, a spacer layer, and a reference layer; a synthetic antiferromagnetic (SAF) fixed layer structure, the SAF fixed layer structure comprising a SAF spacer located between the fixed layer and a second fixed magnetic layer; and a dipole layer, wherein the free layer is located between the dipole layer and the tunnel barrier.

Abstract: An apparatus includes a substrate with a planar surface, a multilayer of semiconductor layers located on the planar surface, a plurality of electrodes located over the multilayer, and a dielectric layer located between the electrodes and the multilayer. The multilayer includes a 2D quantum well. A first set of the electrodes is located to substantially surround a lateral area of the 2D quantum well. A second set of the electrodes is controllable to vary a lateral width of a non-depleted channel between the substantially surrounded lateral area of the 2D quantum well and another area of the 2D quantum well. A third set of the electrodes is controllable to vary an area of a non-depleted portion of the lateral area.

Abstract: The invention relates to a spin current thermal conversion device and a thermoelectric conversion device, with which a spin current is thermally generated, and its concrete application is realized. A temperature gradient creating means which creates a temperature gradient in a thermal spin current generating member is provided in a thermal spin current generating member made of either a ferromagnetic member or a conductive member containing a ferromagnetic substance.

Abstract: An apparatus includes a substrate with a planar surface, a multilayer of semiconductor layers located on the planar surface, a plurality of electrodes located over the multilayer, and a dielectric layer located between the electrodes and the multilayer. The multilayer includes a 2D quantum well. A first set of the electrodes is located to substantially surround a lateral area of the 2D quantum well. A second set of the electrodes is controllable to vary a lateral width of a non-depleted channel between the substantially surrounded lateral area of the 2D quantum well and another area of the 2D quantum well. A third set of the electrodes is controllable to vary an area of a non-depleted portion of the lateral area.

Abstract: A magneto-resistance effect device (1) includes a semiconductor region (2) having a surface provided with a plurality of isolated metal micro-particles (3) of not more than 100 ?m disposed at intervals of not more than 1 ?m, a semiconductor or half-metal cap layer (4) for covering the semiconductor region and a plurality of electrodes (5) disposed on a surface of the cap layer and separated from each other. The device exhibits a high magneto-resistance effect at room temperature, is highly sensible to a magnetic field and can be produced through a simple manufacturing process. The device is formed of a magneto-resistant material easy to match a semiconductor fabrication process. A magnetic field sensor using the device (1) has various excellent characteristics.

Abstract: A multi-level lithography processes for the fabrication of suspended structures are presented. The process is based on the differential exposure and developing conditions of several a plurality of resist layers, without harsher processes, such as etching of sacrificial layers or the use of hardmasks. These manufacturing processes are readily suited for use with systems that are chemically and/or mechanically sensitive, such as graphene. Graphene p-n-p junctions with suspended top gates formed through these processes exhibit high mobility and control of local doping density and type. This fabrication technique may be further extended to fabricate other types of suspended structures, such as local current carrying wires for inducing local magnetic fields, a point contact for local injection of current, and moving parts in microelectromechanical devices.

Abstract: A Hall effect element includes a Hall plate with an outer perimeter. The outer perimeter includes four corner regions, each tangential to two sides of a square outer boundary associated with the Hall plate, and each extending along two sides of the square outer boundary by a corner extent. The outer perimeter also includes four indented regions. Each one of the four indented regions deviates inward toward a center of the Hall plate. The Hall plate further includes a square core region centered with and smaller than the square outer boundary. A portion of each one of the four indented regions is tangential to a respective side of the square core region. Each side of the square core region has a length greater than twice the corner extent and less than a length of each side of the square outer boundary.

Abstract: The present invention provides a magnetization control method controlling, utilizing no current-induced magnetic field or spin transfer torque a magnetization direction with low power consumption, an information storage method, an information storage element, and a magnetic function element. The magnetization control method involves controlling a magnetization direction of a magnetic layer, and includes: forming a structure including (i) the magnetic layer which is an ultrathin film ferromagnetic layer having a film thickness of one or more atomic layers and of 2 nm or less, and (ii) an insulating layer provided on the ultrathin film ferromagnetic layer and working as a potential barrier; and controlling a magnetization direction of the ultrathin film ferromagnetic layer by applying either (i) a voltage to opposing electrodes sandwiching the structure and a base layer or (ii) an electric field to the structure to change magnetic anisotropy of the ultrathin film ferromagnetic layer.

Abstract: The invention relates to a spin current thermal conversion device and a thermoelectric conversion device, with which a spin current is thermally generated, and its concrete application is realized. A temperature gradient creating means which creates a temperature gradient in a thermal spin current generating member is provided in a thermal spin current generating member made of either a ferromagnetic member or a conductive member containing a ferromagnetic substance.

Abstract: A method and system for providing a magnetic element that can be used in a magnetic memory is disclosed. The magnetic element includes pinned, nonmagnetic spacer, and free layers. The spacer layer resides between the pinned and free layers. The free layer can be switched using spin transfer when a write current is passed through the magnetic element. The free layer includes a first ferromagnetic layer and a second ferromagnetic layer. The second ferromagnetic layer has a very high perpendicular anisotropy and an out-of-plane demagnetization energy. The very high perpendicular anisotropy energy is greater than the out-of-plane demagnetization energy of the second layer.

Abstract: A semiconductor device including a Hall effect sensor and related method. The Hall effect device includes a substrate having a first conductivity type and an epitaxial layer having a second conductivity type defining a Hall effect portion. A conductive buried layer having the second conductivity type is situated between the epitaxial layer and the substrate. First and second output terminals and first and second voltage terminals are provided, with the second voltage terminal being coupled to the conductive buried layer.

Abstract: A Hall effect element includes a Hall plate with an outer perimeter. The outer perimeter includes four corner regions, each tangential to two sides of a square outer boundary associated with the Hall plate, and each extending along two sides of the square outer boundary by a corner extent. The outer perimeter also includes four indented regions. Each one of the four indented regions deviates inward toward a center of the Hall plate. The Hall plate further includes a square core region centered with and smaller than the square outer boundary. A portion of each one of the four indented regions is tangential to a respective side of the square core region. Each side of the square core region has a length greater than twice the corner extent and less than a length of each side of the square outer boundary.

Abstract: A Hall-effect magnetic sensor comprises a p-type Hall element and an n-type epitaxial Hall element. The p-type element can be implanted directly on top of the n-type element. The merged Hall elements can be biased in parallel to provide a nearly zero-bias depletion layer throughout for isolation. Electrical contacts to the n-type element can be diffused down through the p-type element and positioned to partially obstruct current flow in the p-type element. Electrical contacts can be diffused into the p-type element. Each bias contact of the p-type element can be connected to respective bias contacts of the n-type element in a parallel fashion. Then, an output signal can be taken at the sense contacts of the n-type element in order to provide improved magnetic responsivity. Further provided is a method for manufacturing the Hall-effect magnetic sensor.

Abstract: A Hall-effect magnetic sensor comprises a p-type Hall element and an n-type epitaxial Hall element. The p-type element can be implanted directly on top of the n-type element. The merged Hall elements can be biased in parallel to provide a nearly zero-bias depletion layer throughout for isolation. Electrical contacts to the n-type element can be diffused down through the p-type element and positioned to partially obstruct current flow in the p-type element. Electrical contacts can be diffused into the p-type element. Each bias contact of the p-type element can be connected to respective bias contacts of the n-type element in a parallel fashion. Then, an output signal can be taken at the sense contacts of the n-type element in order to provide improved magnetic responsivity. Further provided is a method for manufacturing the Hall-effect magnetic sensor.

Abstract: A driving circuit includes a power supply, an input capacitor, a Hall sensor, a first amplifier, a second amplifier, a full-bridge driver circuit, and a first operational amplifier. The input capacitor is coupled to the power supply. The input end of the first amplifier and the second amplifier is coupled to the output end of the Hall sensor. The control end of the full-bridge driver circuit is coupled to the output end of the first amplifier and the output end of the second amplifier. The first operational amplifier includes a first input end for receiving a first reference voltage and a second input end coupled to the first output end of the full-bridge driver circuit.

Abstract: A quantum computer can only function stably if it can execute gates with extreme accuracy. “Topological protection” is a road to such accuracies. Quasi-particle interferometry is a tool for constructing topologically protected gates. Assuming the corrections of the Moore-Read Model for ?=5/2's FQHE (Nucl. Phys. B 360, 362 (1991)) we show how to manipulate the collective state of two e/4-charge anti-dots in order to switch said collective state from one carrying trivial SU(2) charge, |1>, to one carrying a fermionic SU(2) charge |?>. This is a NOT gate on the {|1>, |?>} qubit and is effected by braiding of an electrically charged quasi particle ? which carries an additional SU(2)-charge. Read-out is accomplished by ?-particle interferometry.

Abstract: A quantum computer can only function stably if it can execute gates with extreme accuracy. “Topological protection” is a road to such accuracies. Quasi-particle interferometry is a tool for constructing topologically protected gates. Assuming the corrections of the Moore-Read Model for ?=5/2's FQHE (Nucl. Phys. B 360, 362 (1991)) we show how to manipulate the collective state of two e/4-charge anti-dots in order to switch said collective state from one carrying trivial SU(2) charge, |1>, to one carrying a fermionic SU(2) charge |?>. This is a NOT gate on the {|1>, |?>} qubit and is effected by braiding of an electrically charged quasi particle a which carries an additional SU(2)-charge. Read-out is accomplished by ?-particle interferometry.

Abstract: The invention relates to a semiconductor component (100) comprising a semiconductor chip (10) configured as a wafer level package, a magnetic field sensor (11) being integrated into said semiconductor chip.