Magnetic field sensor arrangement with flux concentrators and an air gap measures signal components in distinct directions.
A magnetic sensor uses a bias field generation unit to stabilize magnetization within the magnetoresistive element.
Segmented pixel cells with orthogonal sensors suppress stray fields to improve angle detection precision.
Dual-frequency microwave modulation drives distinct spin transitions in a diamond nitrogen-vacancy center sensor for precise magnetic field detection.
A nulling magnet reduces transducer magnetic field strength at the sensor, enabling accurate Earth's magnetic field detection despite device proximity.
Magneto-resistive sensors detect sector origin by analyzing phase shifts from AC perturbation fields, resolving directional ambiguity.
A test magnetic field generator compensates for sensitivity variations caused by temperature and external fields.
A magnetoresistive data reader uses a biasing structure to set front shield magnetization and maintain consistent magnetic coupling.
Signal space separation isolates internal biomagnetic data from external interference, improving measurement accuracy by removing common variation components.
A planar electron gun emits electrons through a vacuum chamber to detect magnetic fields via the Lorentz force.
Integrated solenoids guide flux through closed circuits, reducing susceptibility to environmental noise and enabling recalibration.
Phase blended arrayed multiloop inductive coils with layout compensated geometry increase signal strength and improve signal-to-noise ratio.
Initializing magnetization through a conductive layer stabilizes detection against unintended surrounding magnetic fields.
Quadrupole magnets and segmented pixel cells suppress magnetic stray fields to improve rotation angle measurement accuracy.
Auxiliary structure on chip carrier induces predefined magnetic field for sensor calibration, eliminating external equipment needs.
A chirality detector applies voltage to generate spin-polarized electrons for material discrimination.
Annular magnetic structures with excitation coils modulate detection signals via AC currents, reducing 1/f noise for high sensitivity low frequency measurement.
Switching circuit reconfigures magnetic field sensing elements for diagnostic mode self-testing.
Differential subtraction of offset voltage from a spinning-mode sensor reduces power consumption while maintaining high measurement precision.
Iterative method estimates sensor bias using rotational frame operators to correct measurements without user intervention.
Integrated coils generate directional magnetic fields to compensate for external interference, achieving 1% trimming accuracy without complex test equipment.
A serpentine conductive track design integrates input and output portions to generate corrective magnetic fields within a SQUID detection device.
A magnetometer calculates a constant calibration value from multiple intensity readings to determine object orientation accurately.
Five-connection Hall sensors combine differential signals measured at different common-mode potentials to reduce residual offset errors.
Beam splitters distribute light to vapor cells in an optically pumped magnetometer array, replacing bulky SQUIDs for portable MEG.
Segmented magnetoresistive elements in a bridge circuit cancel stress-induced resistance variations to maintain measurement accuracy.
Segmented resistive strip with varying widths and angles in an AMR sensor corrects non-linear magnetic field responses.
Switching circuits couple sensing elements to generate reference signals, enabling gain adjustment and circuit verification without external equipment.
Replacing bulky cryogenic sensors, the ADFMR array uses surface acoustic waves for precise magnetic detection while reducing power consumption.
A magnetic sensor uses a magnetism collecting member with 0.1 μm waviness to minimize gaps against the sensor chip element formation surface.
Active background field compensation enables wearable magnetoencephalography outside shielded rooms.
A magnetic field sensor calibration method uses a transformation matrix to map sensitivity vectors from an oblique coordinate system into orthogonal axes.
A sensor unit with multiple magnetic sensors detects field components in different directions to determine sensitivities and positional tolerances.
A magnet arrangement uses coaxial Maxwell and quadrupole systems to generate selection magnetic fields with gradients and field-free regions.
Digital feedback loop compensates for sensitivity mismatches and temperature drift in angle sensors by adjusting analog frontend gain and offset.
A nulling magnet counteracts the transducer's magnetic field, allowing the magnetometer to detect Earth's field accurately despite device size constraints.
Microwave resonator readout encodes quantum states in radiation phase, replacing fluorescence methods that cause information loss and prolong measurement time.
A three-dimensional magnetic sensor array detects cardiac fields using magnetoresistive elements and flux concentrators.
A magnetic sensor integrated circuit generates reference voltage based on input common-mode voltage to simplify the power module.
Exchange coupling bias films set independent magnetization axes in full-bridge sensors, resolving mutual interference while maintaining strong field resistance.
A dual integrator system with a switching network alternates between signal integration and reference voltage sampling to process differential Hall sensor outputs.
A wafer probe test system uses a rotary magnet and sensor to measure magnetic flux density across multiple sites.
A Wheatstone bridge sensor uses a ferromagnetic flux concentration element to detect perpendicular magnetic field components.
A removable ferromagnetic cap collects magnetic impurities from eddy current sensors to maintain detection accuracy.
A magnetic field detector adjusts its threshold offset based on rotation speed and signal level to ensure reliable switching across varying airgap conditions.
A magnetic sensor reading circuit uses a full-scale control stage to automatically select an optimized gain value for the signal conditioning path.
Segmented magnetic shields and balance coils reduce residual magnetization, maintaining detection accuracy under strong currents.