Systems and methods for acoustically actuated ferromagnetic resonance sensor devices

Abstract

A new and useful high sensitivity and low noise sensor readout system and method for acoustically driven ferromagnetic resonance is provided. A system and method for an acoustically driven ferromagnetic resonance (ADFMR) based sensor includes a power source that provides an electrical signal to power the system, and an ADFMR circuit that is sensitive to electromagnetic fields. The ADFMR circuit includes an ADFMR device. The system functions to detect and measure external electromagnetic (EM) fields by measuring perturbations in the electrical signal passing through the ADFMR circuit due to the external EM field.

Description

[Technical Field]

[0001] (CROSS-REFERENCE TO RELATED APPLICATIONS)

[0001] This application claims the benefit of U.S. Provisional Application No. 62 / 948,146, filed December 13, 2019, which is incorporated herein by reference in its entirety.

[0002] The present invention relates generally to the field of ferromagnetic resonance based sensors, and more particularly to a novel and useful high sensitivity and low noise sensor readout system and method for acoustically driven ferromagnetic resonance. [Background technology]

[0003] Ferromagnetic resonance (FMR) can be used to measure the magnetic properties of materials by detecting the precession of magnetization in ferromagnetic samples. Various types of FMR include externally driven FMR and current-driven FMR. FMR can be excited using a wide variety of techniques, such as cavity excitation, stripline excitation, spin transfer excitation, and spin-orbit torque, among others. These applications are typically incompatible with device applications. They require large cavities and high-power drives to be effective and use large sample volumes. For this reason, the use of FMR is primarily limited to large experimental setups and research projects. Production-ready systems are not currently available. Furthermore, systems for circuit integration are not available in current implementations. Summary of the Invention

[0004]

[0004] Other types of magnetic sensors exist but have various limitations. For example, SERF and SQUID magnetic sensing techniques have high sensitivity, but can be large, complex, and difficult to integrate into systems. Hall effect and magnetoresistive sensors are more compact, but can sacrifice sensitivity. Thus, there is a need in the field of magnetic field sensors for acoustically actuated ferromagnetic resonance sensor devices. The present invention provides such a novel and useful system and method. [Brief explanation of the drawings]

[0005] [Figure 1]

[0005] FIG. 1 is a simplified schematic diagram of a system of a preferred embodiment. [Figure 2]

[0006] FIG. 1 is a schematic diagram of an interferometer system. [Figure 3]

[0007] FIG. 1 is a schematic diagram of a one-dimensional gradiometer system. [Figure 4]

[0008] FIG. 1 is a schematic diagram of a low energy interferometer system. [Figure 5]

[0009] FIG. 1 is a schematic diagram of an interferometer system implementing noise reduction. [Figure 6]

[0010] FIG. 1 is a schematic diagram of a large disparity EM field interferometer. [Figure 7]

[0011] FIG. 1 is a schematic diagram of the overall circuit of an interferometer system. [Figure 8]

[0012] FIG. 1 is a schematic diagram of the overall circuit of the system. [Figure 9]

[0013] 2 is a schematic diagram of the test circuit, a two-dimensional interferometer. [Figure 10]

[0014] 2 is a second schematic diagram of the test circuit, a two-dimensional interferometer. [Figure 11]

[0015] 1 is a schematic diagram of the test circuit, a two-dimensional interferometer. [Figure 12]

[0016] FIG. 1 is a sample diagram of an interdigitated transducer (IDT). [Figure 13]

[0016] FIG. 1 is a schematic diagram of a surface acoustic wave (SAW) device. [Figure 14]

[0017] 1 is a schematic diagram of an alternative variation of a SAW device. [Figure 15] 1 is a schematic diagram of an alternative variation of a SAW device. [Figure 16] 1 is a schematic diagram of an alternative variation of a SAW device. [Figure 17] 1 is a schematic diagram of an alternative variation of a SAW device. [Figure 18] 1 is a schematic diagram of an alternative variation of a SAW device. [Figure 19]

[0018] 1 is an example plot showing the absorption spectrum of a ferromagnetic material as a function of applied field strength. [Figure 20]

[0019] FIG. 1 is a diagram of a circuit representation of a gradiometer. [Figure 21]

[0020] FIG. 1 is a schematic diagram of a vector modulator circuit. [Figure 22]

[0021] FIG. 1 is a schematic diagram of an IQ mixer circuit. [Figure 23]

[0022] FIG. 2 is a schematic diagram of a linearization circuit. [Figure 24]

[0023] FIG. 1 is a schematic diagram of an amplifier circuit. [Figure 25]

[0024] FIG. 2 is a schematic diagram of a detection circuit. [Figure 26]

[0025] FIG. 1 is a schematic diagram of a circuit representation of an interferometer system incorporating analog subtraction. [Figure 27]

[0026] FIG. 1 is a schematic diagram of a circuit representation of an interferometer system incorporating a linearization circuit. [Figure 28]

[0027] FIG. 1 is a simplified schematic diagram of an interferometer. [Figure 29]

[0028] FIG. 1 is a schematic diagram of a circuit representation of an interferometer. [Figure 30]

[0029] 1 is a schematic diagram of an exemplary interferometer including subcomponents. [Figure 31]

[0030] FIG. 1 is a schematic diagram of a circuit representation of a gradiometer. [Figure 32]

[0031] FIG. 1 is a schematic diagram of a circuit representation of an interferometer having a vector modulator circuit. [Figure 33]

[0032] FIG. 1 is a schematic diagram of a circuit representation of an interferometer having an IQ mixer circuit. [Figure 34]

[0033] FIG. 1 is a schematic diagram of a circuit representation of an interferometer having a linearization circuit. [Figure 35]

[0034] 1 is a flowchart of the method of the preferred embodiment. [Figure 36]

[0035] 1 is an exemplary system architecture that may be used in implementing the systems and / or methods. [Figure 37]

[0036] 1 is a glossary of exemplary circuit subcomponents. DETAILED DESCRIPTION OF THE INVENTION

[0006]

[0037] The following description of embodiments of the invention is intended to enable those skilled in the art to make and use the invention, but not to limit the invention to these embodiments.

[0007] 1. Overview

[0038] A system and method for an acoustically driven ferromagnetic resonance (ADFMR) sensor device serves to facilitate the design and operation of chip-scale ADFMR devices that can be used to measure electromagnetic (EM) fields. The system and method preferably uses magnetic resonance to measure the EM field and can then use this information to determine the magnitude and / or gradient of the EM field. The system and method preferably includes a voltage oscillator operating on the order of MHz to GHz to generate an oscillation signal, a power splitter that divides the oscillation signal into a test signal and a reference signal, an ADFMR circuit comprising an ADFMR device that alters the test signal with respect to a magnetic field, and a detector that determines the magnitude and / or gradient of the magnetic field using the altered test signal and reference signal. The ADFMR device may include a base piezoelectric substrate, at least two acoustic transducers on the piezoelectric substrate, and a ferromagnetic material between the at least two acoustic transducers on the piezoelectric substrate. An acoustic wave is generated from a test signal in a first of at least two acoustic transducers, and the acoustic wave propagates along the ferromagnetic material, exciting the ferromagnetic material into resonance or near resonance. The ferromagnetic material modifies the acoustic wave through absorption, and the modified acoustic wave is converted into a modified signal in a second of the at least two acoustic transducers. In many variations, the ADFMR device is a surface acoustic wave (SAW) device. SAW is the acoustic wave used to drive the sensor, although any common type of acoustic wave can be implemented with the system and method.

[0008]

[0039] The systems and methods may provide many potential advantages. The systems and methods are not limited to always providing such advantages, and are presented only to provide exemplary illustrations of how the systems and methods may be put into practice. The list of advantages is not intended to be exhaustive, and other advantages may exist in addition or alternatively.

[0009]

[0040] One potential advantage of the system and method is that it can provide a compact magnetic field sensor device relative to comparable solutions. Where a typical implementation is a large benchtop laboratory setup, the magnetic field sensor device can utilize magnetic resonance to measure magnetic fields without the typical space requirements. More specifically, the system and method can utilize ferromagnetic resonance. This advantage allows the system and method to implement this capability in many situations where it was not previously possible. The system and method preferably provides a chip-scale solution that can be integrated into a circuit design printed circuit board (PCB). The resulting sensor device allows for CMOS-compatible processing, making the sensor device inexpensive and more scalable to produce. The system and method can use ADFMR devices to create magnetic sensors that are easier to integrate.

[0010]

[0041] Another potential advantage of the systems and methods is that ADFMR sensors can have high sensitivity compared to other magnetic sensor technologies. The systems and methods can be sensitive to magnetic fields over a wide frequency spectrum (0-10 GHz). This provides the advantage that the systems and methods can be implemented in a wide variety of sensor devices.

[0011]

[0042] With the potential advantage of a compact form factor, the systems and methods may provide magnetic sensing devices with the high sensitivity required for certain applications, while significantly facilitating integration in terms of size and device package design. In an exemplary field of use, such as a magnetoencephalography system used to measure brain activity, the systems and methods may be chip-based solutions yet meet the sensitivity requirements necessary for monitoring neuronal fields.

[0012]

[0043] Another potential advantage of the system is that the system and method may require low power to function. The system and method may be implemented using significantly less power than other FMR devices. The low power requirement provides the additional benefit of low heat generation. Low heat generation allows the system and method to be implemented in temperature-sensitive environments.

[0013]

[0044] The system and method can be applied to almost any field requiring electromagnetic field measurements. The small size, low power consumption, and high dynamic range functionality allow the system and method to be integrated almost anywhere. The system and method can be particularly useful in mechanical sensor devices and magnetic imaging, as a replacement for SQUID devices, and in conjunction with any device requiring electromagnetic field measurements.

[0014]

[0045] The systems and methods may provide many potential advantages. The systems and methods are not limited to always providing such advantages, and are presented only to provide exemplary illustrations of how the systems and methods may be put into practice. The list of advantages is not intended to be exhaustive, and other advantages may exist in addition or alternatively.

[0015] 2. System

[0046] As shown in FIG. 1 , a system for an acoustically driven ferromagnetic resonance (ADFMR)-based sensor includes a power source 110 that provides an electrical signal to power the system, an ADFMR circuit 120 including an ADFMR device 122, i.e., a first “test” circuit sensitive to electromagnetic fields, and a detector circuit including an analog-to-digital converter. The system functions to detect and measure external electromagnetic (EM) fields by measuring perturbations that occur in the electrical signal passing through the ADFMR circuit due to the external EM field. In some preferred embodiments, the system may include at least one additional circuit (e.g., an additional test or reference circuit). The system further includes at least one power splitter 130 that splits the electrical signal for at least one circuit and at least one power combiner 132 that combines a potentially perturbed electrical signal output from the ADFMR circuit 120 with other electrical signals.

[0016]

[0047] In some variations that include at least one additional circuit, the at least one additional circuit includes a first signal processing circuit, as shown in FIG. 2. The first signal processing circuit is placed in parallel with the ADFMR circuit 120 and serves as a "reference" for the ADFMR circuit. This system variation, or interferometer variation, functions to detect and measure external electromagnetic (EM) fields by comparing perturbations in the electrical signal passing through the ADFMR circuit 120 to the unperturbed electrical signal passing through the first signal processing circuit, or first reference circuit. That is, in the interferometer variation of the system, the power signal passing through the ADFMR circuit 120 is perturbed by the external field and then interferes with the unperturbed reference signal from the reference circuit. The interference (e.g., destructive interference) profile between the test signal and the reference signal can then be used by a detector circuit to determine the strength of the external field.

[0017]

[0048] In another variation, as shown in FIG. 3, the system can function to measure changes (i.e., gradients) in an external EM field, i.e., function as a gradiometer. In gradiometer variations, at least one circuit can include an additional ADFMR circuit 120, i.e., a second test circuit sensitive to the EM field. In these variations, the difference in measurements between the first and second test circuits can be used to determine the gradient of the EM field. That is, in gradiometer variations of the system, the power signals passing through both ADFMR circuits 120 are perturbed by the external field. By taking into account the position dependence of the two circuits, the gradient of the external field can be measured by measuring the interference (e.g., destructive interference) between the two signals.

[0018]

[0049] In many variations, the system may additionally or alternatively include subcomponents to enhance and / or modify system functionality. Examples include additional ADFMR devices 122 (e.g., to enable multidimensional field measurements), amplifiers (e.g., to amplify power / electrical signals), filters (e.g., to reduce internal and background noise), matching networks (e.g., to match signal power between parallel circuits), attenuators, phase shifters (e.g., to alter the interference pattern between the test signal and the reference signal), mixers (e.g., to mix signal frequencies), magnetic field coils (e.g., to shift the signal band), and any other desired components. Examples of possible system subcomponents include signal amplifiers (A), bandpass filters (F), attenuators (l), inductors (L), phase shifters (γ), couplers (c), mixers (X), matching networks (M), analog-to-digital converters (ADCs), digital-to-analog converters (DACs), comparators (≧), logic circuits, and magnetic field coils. The system may also include any other desired components, if applicable. Some examples of these components are discussed further below. Figure 37 includes a glossary and designations for subcomponents implemented in some variations of the system.

[0019]

[0050] These subcomponents allow for many additional variations. For example, the system may include variations optimized for low energy consumption as shown in the example of Figure 4, variations to reduce noise as shown in the example of Figure 5, and variations to optimize the sensitivity and / or operating range of the system as shown in the example of Figure 6. The system may additionally or alternatively include any combination or additional variations as desired.

[0020]

[0051] A system may include parallel or series circuits and circuit segments as part of the system. These circuits may include any circuit subcomponents (e.g., those subcomponents described above) as required for functionality. As used herein, the term "circuit" is used generally to refer to either an entire circuit or a circuit segment. That is, a circuit does not necessarily form a closed loop by itself, but rather may function as part of a closed loop in combination with additional circuitry, which may or may not be explicitly presented herein.

[0021]

[0052] As shown in Figures 7 and 8, the circuit numbering indicates the number of the test circuit (indicated by a subscript number with a prime), the circuit containing the ADFMR device subcomponents, and the signal processing circuit (indicated by a subscript number). The test circuit may also be referred to as the ADFMR circuit or the sensor circuit. Furthermore, the first test circuit may also be referred to without a number, for example, as the test circuit or the ADFMR circuit. Although the circuits are simply shown numbered in parallel in these figures, variations of the system may include test circuits and / or signal processing circuits in other non-parallel configurations within the circuit (e.g., as shown in Figure 6).

[0022]

[0053] In a typical circuit layout for a system, as shown in Figure 8, the system may include "n" test circuits and "N" signal processing circuits, where n and N are any integers determined by the particular implementation. Circuit subcomponents, i.e., components on a particular circuit, may be referred to using subscripts representing the circuit number. Test circuit subcomponents are referred to using subscripts with a prime (e.g., L 2’ refers to an inductor on the second test circuit), and signal processing circuit subcomponents are designated with subscripts without a prime (e.g., L2 refers to an inductor on the second signal processing circuit). In some variations, certain subcomponents may appear in areas where it is not clear to which circuit they belong. These subcomponents may be included without a subscript, or may include a subscript that associates them with the desired circuit (e.g., if the subcomponent has a complementary function to the desired circuit).

[0023]

[0054] As part of the circuit name, circuit subcomponents may be described as being upstream or downstream relative to one another. "Upstream" and "downstream" are used herein to indicate the direction of power traveling through the circuit. That is, subcomponent "A" downstream of subcomponent "B" indicates the positionality where power travels from subcomponent "B" to subcomponent "A," regardless of whether there are other components between them. Subcomponent "A" upstream of subcomponent "B" indicates the positionality where power travels from subcomponent "A" to subcomponent "B," regardless of whether there are other components between them.

[0024]

[0055] The system may include a power source 110. The power source functions as an energy source and provides an electrical signal to the system. In some variations, the power source 110 is an electronic oscillator. The electronic oscillator functions to provide an oscillating voltage, or alternating current (AC), power signal to the system. Power from the oscillator is used to activate the sensor circuitry. Alternatively, other types of electrical current, such as direct current (DC), may be used.

[0025]

[0056] In some variations, the electronic oscillator is a voltage-controlled oscillator (VCO). Preferably, the oscillator frequency is on the order of gigahertz, more preferably ∼2 GHz. The oscillator's high frequency pulsing can enable fast turn-on and turn-off times for the sensor. Fast turn-on / turn-off times can be on the order of microseconds or faster. Because the ADFMR device 122 can function with MHz oscillations, the oscillator can alternatively be in any range that enables ADFMR functionality, i.e., on the order of MHz to GHz.

[0026]

[0057] The system may include at least one ADFMR circuit 120. The ADFMR circuit 120 functions as a “test” circuit including an ADFMR device that enables sensor operation for the system. The ADFMR circuit 120 may also be referred to as a sensor circuit or a test circuit. Depending on the variation, the system may include one or more ADFMR circuits 120. Each ADFMR circuit may share multiple ADFMR devices 122, have a single ADFMR device, or have multiple ADFMR devices. In some variations, the system may include a set of ADFMR circuits. Multiple ADFMR circuits 120 may be used for gradient field measurements, multi-dimensional field measurements, and / or improved field measurement accuracy (e.g., through redundant measurements). Positioning the ADFMR circuit 120 downstream of the power source 110 allows the electrical signal provided by the power source to be implemented as a test signal along the ADFMR circuit.

[0027]

[0058] In some variations, the system may include multiple ADFMR devices 122 distributed across the ADFMR circuit 120. In one variation, multiple ADFMR circuits 120 measuring one or multiple dimensions may be implemented on a single chip, very similar to a layout such as that shown in Figure 9 or Figure 10. Depending on the desired implementation, the functionality of each dimension may be activated or deactivated.

[0028]

[0059] In one variation, a single ADMR circuit 120 can be implemented on a single chip to measure one, several, or all desired dimensions, very similar to a layout such as that shown in Figure 11. The functionality of each dimension can be activated or deactivated depending on the desired implementation.

[0029]

[0060] The ADFMR device 122 is preferably a component of the system, and even a subcomponent of the ADFMR circuit 120. The ADFMR device 122 functions as a device that "measures" an EM field by enabling the modification of a radio frequency (RF) carrier signal (i.e., a test signal) using acoustically driven magnetic resonance. In many variations, the magnetic resonance is implemented by a ferromagnetic material (i.e., ferromagnetic resonance), but can be implemented using any magnetic material. Examples of other types of magnetic materials include antiferromagnets, ferrimagnetic materials, etc. That is, although the device is referred to as the ADFMR device 122, the ADFMR device may actually be, for example, a ferrimagnetic resonance device. The ADFMR device 122 may include at least one acoustic transducer that generates and / or absorbs acoustic waves, an acoustic resonator that provides a medium for acoustic wave propagation, and a magnetic material that perturbs the acoustic waves with an EM field using magnetic resonance.

[0030]

[0061] The ADFMR device 122 preferably includes an acoustic transducer that functions to convert a test signal into an acoustic wave and / or convert an acoustic wave into an RF signal (e.g., an altered test signal) and that generates and / or absorbs, from the electrical signal, an acoustic wave (or pressure wave) that propagates along an acoustic resonator (e.g., a piezoelectric substrate).

[0031]

[0062] Preferably, the acoustic transducers are implemented in pairs, with acoustic waves generated by one transducer propagating to the other acoustic resonator and then absorbed by the second transducer. That is, a first acoustic transducer converts a test signal traveling through the ADFMR circuit 120 into an acoustic wave, which propagates within or along the ADFMR device 122 to a second acoustic transducer, which then converts the acoustic wave into an electrical signal. Alternatively, a single acoustic transducer can both convert an RF test signal into an acoustic wave and reconvert the acoustic wave back into an RF signal. For example, an electrical signal can be converted into an acoustic wave by an acoustic transducer, which propagates and reflects back to the acoustic transducer, which then reconverts the acoustic wave into an electrical signal. In other examples, multiple acoustic transducers can be implemented to both generate and absorb acoustic waves. That is, multiple acoustic transducers may be implemented per ADFMR device 122 to convert single or multiple RF signals into acoustic waves and / or convert acoustic waves into RF signals one or more times.

[0032]

[0063] The acoustic transducer preferably generates acoustic waves appropriate for the type of ADFMR device 122. Examples of generated acoustic waves may include surface acoustic waves (SAW), bulk acoustic waves (BAW), and Lamb waves. The particular acoustic transducer may be implementation-specific. The type of acoustic transducer may depend on the electrical signal (e.g., signal frequency, signal power) and / or the type of acoustic wave (e.g., surface acoustic wave, bulk acoustic wave) generated. For example, in variations in which the system uses Lamb waves, the acoustic transducer may comprise an electromagnet-acoustic transducer (EMAT). In variations in which the system uses SAW, the acoustic transducer may include an interdigital transducer (IDT). Alternatively, other types of transducers (e.g., film bulk acoustic resonators, high-harmonic bulk acoustic resonators) that generate either SAW or other types of acoustic waves may be implemented. The acoustic waves are preferably generated at or near the resonant frequency of the ferromagnetic material. The acoustic waves preferably propagate through the ferromagnetic material within or alongside the acoustic resonator, thereby causing the ferromagnetic material to function at or near resonance.

[0033]

[0064] In some variations in which the system uses SAWs, the acoustic transducer may include an IDT. The IDT may function to generate a SAW from an electrical signal (or generate an electrical signal from a SAW) using the piezoelectric effect. The IDT is a device positioned on a piezoelectric substrate (e.g., quartz, lithium niobate) and configured with an interdigitated array of metal electrodes to form a periodic structure. The IDT may have any desired configuration / shape. An example IDT configuration is shown in FIG. 12. In a pair of IDTs, preferably, one functions as an input IDT and one functions as an output IDT. The input IDT can convert a radio frequency (RF) electrical signal into a surface acoustic wave (SAW) using the piezoelectric effect. The output IDT functions by absorbing the SAW and reconverting it into an electrical signal.

[0034]

[0065] The ADFMR device 122 may include an acoustic resonator. The acoustic resonator acts as a medium that allows for the propagation of acoustic waves. The acoustic resonator may allow for wave propagation through a volume (e.g., BAW), wave propagation along the surface of a medium (e.g., SAW), or wave propagation through a cavity in a medium (e.g., sound wave propagation through an air cavity in the acoustic resonator). The acoustic resonator may be composed of any material that allows for the desired type of acoustic wave propagation. In some variations, the acoustic resonator is composed of a piezoelectric substrate (e.g., quartz). In some variations, the acoustic resonator comprises the main “body” of the ADFMR device 122, with all other components disposed on or around the acoustic resonator.

[0035]

[0066] In some variations, the acoustic resonator is a piezoelectric substrate. The piezoelectric substrate allows for the generation and propagation of acoustic waves through the piezoelectric effect. The piezoelectric substrate can be made of any desired piezoelectric compound (e.g., most crystalline or ceramic compounds). In one preferred variation, a Y-cut lithium niobate substrate is used as the piezoelectric substrate. In some variations including two acoustic transducers, the length of the space between the two acoustic transducers (i.e., the delay line) is 1 to 3 mm. In one example, the piezoelectric substrate (e.g., zinc oxide) is positioned below or above the two IDTs on the ADFMR base (e.g., diamond-based material).

[0036]

[0067] ADFMR devices may include a magnetic material, preferably a magnetostrictive material. Magnetostrictive properties allow magnetic materials to convert strain into changes in magnetization or vice versa. The only constraint on the magnetic material is that it must be capable of achieving macroscopic resonance (i.e., resonance beyond the excitation of individual molecules and / or atoms). Examples of magnetic materials include ferromagnetic materials, ferrimagnetic materials, antiferromagnetic materials, paramagnetic materials, diamagnetic materials, etc. In some variations, the magnetic material may include ferromagnetic materials and / or ferromagnetic mixtures. The magnetic material functions to absorb acoustic waves, and this absorption is highly sensitive to magnetic fields at resonance. Preferably, the magnetic material is positioned within the path of the acoustic wave (along a delay line) so that the local magnetic field sets the resonant frequency of the magnetic material at or near the acoustic wave frequency. This allows the magnetic material to effectively absorb the acoustic wave and alter the propagating acoustic wave relative to the magnitude of the magnetic field. In a preferred variation, a ferromagnetic material (e.g., as a magnetic film) is disposed between the two acoustic resonators; the thickness and length of the magnetic material play a large role in absorption, and the magnetic material may have variable thickness and different lengths depending on the embodiment. In the ferromagnetic variation, examples of the types of ferromagnetic material implemented include iron, nickel, and cobalt, but any suitable type of ferromagnetic material may be used. In some variations, the system may be implemented using other magnetic materials. For example, paramagnetic, diamagnetic, ferrimagnetic, antiferromagnetic, or any combination of these materials may be used. As with the ferromagnetic variation, the magnetic material may be implemented at or near resonance to absorb the magnetic field.

[0037]

[0068] In some variations, the ferromagnetic material has a spatial orientation. That is, the ferromagnetic material can be constructed and oriented so that EM fields in one spatial orientation (e.g., the x-direction) affect the interaction of the magnet with the acoustic wave, while fields in other orientations leave the ferromagnetic material unaffected. Thus, depending on the ferromagnetic material implemented, the ferromagnetic material (and therefore the ADFMR device 122) can be sensitive to one, two, or three spatial dimensions.

[0038]

[0069] In some variations, the ADFMR device 122 may include a signal detector. The signal detector functions to measure the output power signal from the ADFMR device 122. Because the output power signal may be perturbed by the applied field, the output power signal can be used to determine the strength of the electromagnetic field. The signal detector may also include noise reduction functionality. In one variation, the signal detector may perform a Fourier transform to separate the desired output signal from other unrelated electromagnetic (EM) waves. For example, the input acoustic transducer may also generate unrelated EM waves. The signal detector may perform a fast Fourier transform to separate and remove these unrelated EM waves from the desired signal. Because acoustic wave propagation has a time delay compared to EM wave propagation, other time-dependent methods may also be used to separate the acoustic wave from the EM wave. For example, in one embodiment, an electronic oscillator is repeatedly turned on and off for a fixed time period, and measurements of the propagating acoustic wave are taken during the electronic oscillator's off cycle, allowing for the removal of the undesired signal.

[0039]

[0070] In some variations, the ADFMR device 122 can be a SAW device, as shown in the example of FIG. 13 . That is, in one example of a SAW device, the ADFMR device 122 can include two IDTs, an input IDT and an output IDT, positioned along a piezoelectric substrate. A magnetic film is positioned along the piezoelectric substrate between the two IDTs. The specific configuration and shape of the SAW device can vary depending on the implementation. Examples of these variations include having a single SAW device per ADFMR circuit 120 (e.g., the SAW device of FIG. 13 ), having spatially oriented ferromagnetic material(s) on the SAW device for a multidimensional field sensor, as shown in FIGS. 14 and 15 , using a single SAW device with a single ferromagnetic material between multiple ADFMR circuits 120, as shown in FIG. 16 , using a single SAW device with multiple ferromagnetic materials as either an interferometer or gradiometer implementation, as shown in FIG. 17 , and having multiple individually oriented series ferromagnetic materials (e.g., as part of a series multidimensional sensor), as shown in FIG. 18 . Particular variations may include fewer components or additional components, as desired or needed.

[0040]

[0071] In some variations, the ADFMR device includes a field coil (FC). The field coil may be a direct current (DC) coil and / or any suitable coil or system for generating a magnetic field. Any other suitable component capable of generating a magnetic field to offset the power output may also be used. The field coil functions to generate a magnetic field bias to offset the output of the ADFMR device 122 positively or negatively. In one variation, the field coil reduces the power output by inducing a small external field to which the ADFMR device 122 is exposed. The field coil is implemented to offset the power output to a small output regime where the circuit components function linearly, thereby reducing systematic errors due to nonlinearities. For example, the amplifier may have a much smaller linear amplification range than the output of the ADFMR device 122. Thus, reducing the range of the sensor output allows for linear functionality of the amplifier. The field coil may apply a magnetic field at any frequency (or combination of frequencies) as desired. For example, if the system is exposed to a large undesired signal (e.g., 60 Hz) from a power line in addition to the Earth's magnetic field, the undesired field altered by the power line and the Earth's magnetic field can be counteracted. Any suitable type of counteracting magnetic field can be applied using a magnetic field coil.

[0041]

[0072] The magnetic field coils can offset the power output to any desired range. In some variations, the magnetic field coils can offset the external field to near zero. In other variations, the magnetic field coils can alternatively or additionally offset the magnetic field to a range where the ADFMR sensor functions optimally. For example, in embodiments where the system is used as a gradiometer, the magnetic field coils can offset the magnetic field to a regime where changes in the external field cause the greatest change in the power output (e.g., an inflection point in the output power spectrum). Figure 19 shows a sample absorption spectrum as a function of the external field. Thus, at a given frequency, the magnetic field coils can vary the external field so that the center of operation is the inflection point of the curve.

[0042]

[0073] The system may include a detector circuit. The detector circuit functions to obtain the output of the ADFMR circuit 120 (i.e., the potentially perturbed electrical signal) and the output of any other components and determine the strength of the EM field. In many variations, the detector circuit includes an analog-to-digital converter (ADC). The ADC functions to convert the analog signal to a digital signal. In some variations, the ADC can be used to convert the output signal to a digital signal for analysis. In some variations, an ADC can be implemented for each circuit (including the ADFMR circuit 120). In these variations, the ADC converts the circuit's signal output to a digital output before combining the circuit signals. All circuit digital outputs can then be combined into a digital output signal.

[0043]

[0074] In variations including parallel circuits, the system may further include a power splitter 132 and / or a power combiner 134. The power splitter 132 functions to split the power signal into multiple portions to allow for the connection of additional parallel circuit components. The power combiner 134 functions to combine multiple circuits. In many variations, the power splitter 132 can split the initial power signal into a test signal and a reference signal. Additionally or alternatively, the power splitter can split the power signal into multiple test signals and / or multiple reference signals. In addition to other properties, the power splitter / combiner set enables interferometric functionality for field measurements. That is, the power signal can be split into two portions (e.g., a test signal and a reference signal) and one (or both) of these signals can be altered (e.g., by field power absorption via an ADFMR device). The field can then be measured by examining the interference pattern produced when these two signals are combined. The system may include a pair of power splitter / combiners in each of the parallel circuits included in the system. Alternatively, the system may include more or fewer power splitter / combiner pairs in each of the parallel circuits included within the system. In some variations, the system may include a different number of power splitters 132 and power combiners 134 (e.g., one split power signal may be connected to ground, eliminating the need for a power combiner).

[0044]

[0075] In some multidimensional field detection embodiments, the system can include additional power splitters / combiners to accommodate additional ADFMR circuits 120. For example, as shown in FIG. 9, in an embodiment that allows for multiple field measurements in a plane, the system can include a power splitter 132 that splits the circuit into a first test circuit and a second test circuit, and a power combiner 134 that combines the first ADFMR circuit 120 measuring the field in the “x-direction” and the second ADFMR circuit measuring the field in the “y-direction.” The system can also include a second pair of power splitters / combiners (instead of the couplers shown) to initially split the power signal into a reference signal and a test signal. Alternatively, as shown in FIG. 11, a single test circuit can include multiple series ADFMR devices 122 (e.g., with different orientations) that allow for multidimensional field measurements depending on their orientation. In some variations, these series ADFMR sensors can function simultaneously, while in other variations, they can operate alternately.

[0045]

[0076] As previously discussed, the system may further include a combination of various subcomponents. Examples of subcomponents include signal amplifiers, bandpass filters, attenuators, inductors, phase shifters, couplers, mixers, matching networks, field coils, and comparators. The subcomponents may be incorporated into test circuitry, signal processing circuitry, or any other part of the system, as desired.

[0046]

[0077] In some variations, the system includes at least one amplifier (A). The amplifier functions to increase the signal strength. The amplifier can help counteract the effects of power loss and power reduction due to dividing the original power. The amplifier can be an active or passive amplifier.

[0047]

[0078] In some variations, the system may include an attenuator (1). The attenuator functions to reduce the power of the signal without affecting the signal waveform. In some variations, the attenuator is implemented to reduce noise. The attenuator can also match the power signal amplitude between parallel circuits (e.g., between a test circuit and a reference circuit). The attenuator can be digital or analog. In some variations, a digital attenuator is used to maximize the rejection of 1 / f "pink" noise, i.e., noise proportional to power. Analog attenuators also reduce 1 / f noise, but depend on the noise signal of their control voltage. In some variations, the ADFMR circuit 120 may include an attenuator.

[0048]

[0079] In some variations, the system includes at least one bandpass filter (F). A bandpass filter functions to narrow the electrical signal band, thereby allowing for a narrow waveband for use and / or analysis. Furthermore, this may be true even if the signal is amplified, necessarily broadening the signal spectrum.

[0049]

[0080] In some variations, the system includes at least one inductor (L). The inductor functions to store energy in a magnetic field. The matching inductor can match the impedance of the transducer to any circuit components adjacent to the transducer. In some variations, the system can include a matching inductor that matches the acoustic transducer to the mixer input.

[0050]

[0081] In some variations, the system includes at least one phase shifter (γ). A phase shifter functions by "shifting" the phase of an electrical signal. Phase shifters can be implemented to provide constructive or destructive interference between parallel circuits that are subsequently coupled. This is particularly important in implementing interferometers.

[0051]

[0082] In some variations, the system may include at least one mixer (e.g., a frequency mixer (X)). The mixer functions to combine two electrical signals into one. The mixer can multiply signals to enable frequency mixing. In some variations, the mixer can reduce the ∼1 GHz frequency from the ADFMR device 122 to zero frequency DC. Additionally, the mixer can mix the original power source 110 signal with the output of the ADFMR device 122 to remove electronic oscillator noise.

[0052]

[0083] In some variations, the system includes at least one coupler. The coupler functions to couple power traveling through one circuit to another circuit, allowing the same signal to be used in the other circuit. In some variations, a coupler can be used instead of a power splitter to maintain the same power level in both paths. In some variations, the system can also include a hybrid coupler. The hybrid coupler allows two input sources to be combined into two output sources. In some preferred variations, the hybrid coupler is implemented to split a single input source and shift the phase of the output source.

[0053]

[0084] In some variations, the system includes at least one matching network. The matching network may include a combination of inductors and capacitors. The matching network may function to provide impedance matching between the acoustic transducer and adjacent circuit components (e.g., mixer inputs) and to increase the apparent impedance of the transducer so that the transducer can be attached to a high-efficiency (low-power) oscillator. In some variations, the matching network may match the impedance of the transducer to any circuit components adjacent to the transducer. In some variations, the system may include a matching network that matches the acoustic transducer to the mixer input.

[0054]

[0085] In some variations, the system includes at least one comparator (≧). The comparator functions to detect the sign of the output signal, i.e., positive, negative, or zero. The comparator is used in conjunction with logic circuitry to allow for gradual changes to the output signal.

[0055]

[0086] As described above, the system includes at least one ADFMR circuit 120 (i.e., a first ADFMR circuit) including at least one ADFMR device 122. Each ADFMR circuit includes an ADFMR device subcomponent and / or shares an ADFMR device subcomponent with other ADFMR circuits (e.g., as shown in FIG. 10 ). The ADFMR circuit 120 functions to measure an external magnetic field. Depending on the variation, each ADFMR circuit 120 can be identical or different. The ADFMR circuit 120 can have additional subcomponents depending on the embodiment. For example, in one embodiment, the ADFMR circuit 120 can include a matching network. In other variations, the ADFMR circuit 120 can include an inductor and / or an attenuator. The ADFMR circuit 120 can additionally or alternatively include other components, such as an amplifier or a phase shifter.

[0056]

[0087] In a "low power" variation, the ADFMR circuit 120 includes a matching network. In this variation, the matching network may function to match the impedance of the ADFMR circuit with another circuit. In this variation, the system may include a high-impedance power source (e.g., an oscillator), and the acoustic transducer of the ADFMR device may be low-impedance.

[0057]

[0088] In another variation, the ADFMR circuit 120 includes a digital attenuator upstream of the ADFMR device 122 and two matching inductors. One of the two matching inductors is upstream of the ADFMR device and the other is downstream. Compared to an analog attenuator, the digital attenuator can reduce power and help reduce 1 / f noise. The matching inductor can match impedance between the IDT and other components (e.g., a mixer) in the ADFMR device 122.

[0058]

[0089] In some variations, the system may include multiple ADFMR circuits (e.g., a first ADFMR circuit, a second ADFMR circuit, etc.). The multiple ADFMR circuits 120 may function to enable additional and / or improved sensing capabilities for the system. In some system embodiments, multiple ADFMR circuits 120 (e.g., a first test circuit and a second test circuit) may be arranged in parallel at separate spatial locations so that the system can function as a gradiometer. Thus, reference to a gradiometer refers to at least two parallel ADFMR circuits 120 and a set of power splitters / combiners that split and combine the original power signal into two test signals, as seen in the exemplary schematic diagram of FIG. 20. Generally, additional circuitry (e.g., additional test circuits and / or signal processing circuits) and additional subcomponents may be added depending on the desired implementation. The additional subcomponents may be both serial and parallel depending on the implementation requirements.

[0059]

[0090] The system may include at least one signal processing circuit, such as a first signal processing circuit. The signal processing circuit may be in parallel with the ADFMR circuit 120. Alternatively, the signal processing circuit may be in series with the ADFMR circuit 120. Depending on the embodiment, the signal processing circuits may be the same or different and may serve multiple functional roles as part of the system. In some variations, the first signal processing circuit is a reference circuit in parallel with the ADFMR circuit 120.

[0060]

[0091] Depending on the embodiment, a first signal processing circuit, or reference circuit, functions in conjunction with the ADFMR circuit 120 such that the two together can function as an interferometer. In these embodiments, the reference circuit can include a phase shifter and an attenuator. Thus, the interferometer refers to the ADFMR circuit 120, the reference circuit, and a set of power splitters / combiners that split and combine the original power signal into a test signal and a reference signal, as seen in the exemplary schematic diagram of FIG. 4 . Generally, additional circuitry (e.g., additional test circuits and / or signal processing circuits) and additional subcomponents can be added depending on the desired embodiment. The additional subcomponents can be in both series or parallel, depending on the requirements of the embodiment. A phase shifter in the reference circuit can function to change the phase of the reference signal so that the reference circuit can destructively interfere with the ADFMR circuit 120.

[0061]

[0092] In some variations, the system includes a signal processing circuit that is a vector modulator circuit, as shown in the exemplary schematic diagram of FIG. 21. The vector modulator circuit is preferably in parallel with the ADFMR circuit 120, but may also be in series with the ADFMR circuit. The vector modulator circuit functions as a reference circuit and, together with the test circuit, forms an interferometer. The vector modulator circuit may also function to reduce noise (e.g., as an analog subtraction circuit), but may have other or additional functions. The vector modulator circuit preferably includes at least one attenuator. In one preferred example, the vector modulator circuit includes an upstream attenuator, and a hybrid coupler provides outputs from this one upstream attenuator to two downstream attenuators, which are then recombined. The two downstream attenuators may implement a desired phase shift in the power signal. The vector modulator circuit implements the desired phase solely using the attenuators, thereby minimizing noise due to the phase shift. In some variations, as shown in FIG. 32, the vector modulator circuit may function solely as a reference circuit and, when used in conjunction with the test circuit, function as an interferometer circuit. The vector modulator circuit may additionally or alternatively work in conjunction with a separate interferometer or gradiometer circuit to reduce signal amplitudes that do not originate from the signal of interest.

[0062]

[0093] In some variations, the system includes a signal processing circuit that is an IQ mixer circuit, as shown in the exemplary schematic diagram of FIG. 22. The IQ mixer circuit can be in parallel with the ADFMR circuit 120 or in series with the ADFMR circuit 120. The IQ mixer can include a power splitter 134 that splits the power in half, a mixer connected to a hybrid coupler downstream of the power splitter that shifts one half of the power signal out of phase, and a mixer connected to the unshifted output of the hybrid coupler downstream of the power splitter that mixes the other half of the power signal without shifting the signal. The IQ mixer can function to generate a linear combination of an “in-phase” power signal and a 90-degree “out-of-phase” power signal to better measure the amplitude and phase of the power signal. Additionally, the IQ mixer circuit can function to center and normalize the test signal, but can also include other or additional functions. The IQ mixer circuit can be implemented in conjunction with either an interferometer circuit or a gradiometer circuit.

[0063]

[0094] In some variations, the system includes a signal processing circuit that is a linearization circuit, as shown in the exemplary schematic diagram of FIG. 23. In some variations, the linearization circuit can be in series with the ADFMR circuit 120 or in parallel to the ADFMR circuit. In one embodiment of the linearization circuit, the linearization circuit can include at least one comparator and logic circuit. The linearization circuit functions to minimize nonlinear outputs of system subcomponents by narrowing the system's output voltage into a smaller, more linear regime. The linearization circuit can be used in conjunction with a magnetic field coil to function as a feedback loop directed by the logic circuit. The logic circuit uses input information from the comparator to direct the magnetic field coil current. The linearization circuit can be implemented with any desired ADFMR circuit 120.

[0064]

[0095] The linearization circuit can be configured to function in a “setup” mode prior to final field measurement. The setup mode functions to optimize the voltage output of the ADFMR circuit 120 and / or the external field applied to the ADFMR circuit to the desired measurement / output regime (i.e., the desired operating regime). During the setup mode, the linearization circuit can gradually change the magnetic field via the field coil voltage. Through cycles, the field coil voltage can be increased or decreased until the desired operating regime of the field is reached. Once the desired regime is reached, the setup mode can be stopped and an effective field measurement can be performed. The actual field strength can be determined by considering the current or voltage supplied to the field coil. Alternatively, the linearization circuit may include a simpler field detector to determine an approximate desired voltage and allow the field coil to reach the desired operating regime in one or a very small number of incremental cycles (e.g., in a field programmable gateway array implementation).

[0065]

[0096] In one example using a linearization circuit, the desired operating regime of the external field is zero (or near zero), and the magnetic field coil is a DC coil. In this example, during setup mode, the voltage on the DC coil can be increased or decreased until the effective field on the sensor is near zero. Once the effective field is near zero, the ADFMR circuit can perform a "final" measurement of the effective field. The system can then use the voltage across the DC coil to calculate the actual field strength.

[0066]

[0097] In some variations, the system may include a signal processing circuit that is an amplifier circuit, as shown in the exemplary schematic diagram of FIG. 24. The amplifier circuit may be in series with the ADFMR circuit 120 and function to amplify the power signal (e.g., the test signal). The amplifier circuit preferably includes at least one amplifier. In some variations, the amplifier circuit includes bandpass filters upstream and downstream of the amplifier to maintain a narrow power spectrum. The amplifier circuit may be implemented to compensate for power loss and / or power reduction due to circuit division.

[0067]

[0098] In some variations, the system may include a detection circuit, as shown in the exemplary schematic diagram of FIG. 25. The detection circuit functions to "read" the system's output voltage as the applied field. Generally speaking, this requires normalizing the output signal and converting it to a quantity that can be analyzed by the detection circuit. The detection circuit preferably functions in conjunction with an IQ mixer circuit, but may be implemented independently of the detection circuit. Any conventional detection circuit capable of functioning within the desired range may be used for this function. In one preferred variation, the detection circuit includes an amplifier and an analog-to-digital converter (ADC). Additionally, the detection circuit may include an inductor.

[0068]

[0099] The circuit components described above can be used in any desired manner with basic interferometer / gradiometer components. Generally speaking, any embodiment can be used as an interferometer or gradiometer as discussed above. In a first example of general interferometer use, the basic system further includes a vector modulator circuit, an IQ mixer circuit, an amplifier circuit, and a detector circuit. Figure 26 shows this example implemented as an interferometer. In this example, the amplifier circuit amplifies the outputs of the "inner" and "outer" interferometers and the vector modulator circuit, which are then connected to the IQ mixer. All signals are finally combined and output to the detector circuit. This general use example functions to measure a field as desired. Additionally or alternatively, this example can be implemented for a gradiometer system.

[0069]

[0100] In large difference examples, which may include large differences in field strength, the conventional general use case may also include a linearization circuit, as shown in Figure 27. The large difference example functions to precisely measure fields that may have significant differences in magnitude. While the general use case may function over a wide range, the large difference example includes a feedback loop that may reduce nonlinear effects due to significant differences in field magnitude, thereby increasing the accuracy of the field measurement.

[0070]

[0101] In a third low-power example, the system may include only a mixer and detection circuitry. The low-power example functions to detect fields with extremely low power consumption (less than 25 μW). In a variation where the ADFMR device includes a SAW device, the system may further include matching networks before and after the interferometer. The matching networks provide high resistance and can match the IDT impedance to the impedance of the electronic oscillator and mixer, thereby matching their voltages.

[0071] 3. System implementation example

[0102] In this section, sample system variations are provided. The details of the variations described can be used in combination with or in place of other system variations described herein. The description of these examples is not intended to limit the system to these examples.

[0072]

[0103] In a first system variation, as shown in FIG. 1, a system for an acoustically driven ferromagnetic resonance (ADFMR)-based sensor includes a power source including an electronic oscillator that provides an electrical signal, at least one circuit including a first ADFMR circuit that includes an ADFMR device and allows perturbation of the electrical signal by an electromagnetic (EM) field, and a detector circuit that determines the EM field from the perturbation of the electrical signal. In many variations, the detector circuit includes an analog-to-digital converter. The system functions as a sensor capable of detecting EM fields.

[0073]

[0104] As shown in FIG. 28 , in a first interferometer example of the first system variation, the at least one circuit includes an interferometer circuit. In some variations, the at least one circuit includes the aforementioned first ADFMR circuit (also referred to as a first test circuit) and a first signal processing circuit, which is a first reference circuit. The first reference circuit is arranged in parallel with the first ADFMR circuit, such that the first ADFMR circuit and the first reference circuit combine to form the interferometer circuit. The interferometer circuit functions to measure the EM field by interfering a perturbed electrical signal passing through the first test circuit with an unperturbed signal passing through the first reference circuit. In some variations, the interferometer circuit can include multiple test circuits and / or reference circuits, where one or more test circuits and one or more reference circuits collectively enable the measurement of the EM field through interference.

[0074]

[0105] As shown in Figure 29, in a second interferometer example of the first system variation, the at least one circuit further includes a first signal processing circuit that is a first reference circuit arranged in parallel with the first ADFMR circuit. The system further includes a power splitter arranged upstream of the first ADFMR circuit and the first reference circuit, the power splitter configured to split the electrical signal into a test signal that travels through the first ADFMR circuit and a reference signal that travels through the first reference circuit. The system also includes a power combiner arranged downstream of the first ADFMR circuit and the first reference circuit, the power combiner configured to combine the test signal output from the first ADFMR circuit and the reference signal output from the first reference circuit. The first ADFMR circuit and the first reference circuit can collectively function as an interferometer circuit to measure an EM field.

[0075]

[0106] The first ADFMR circuit of the interferometer variant may also have a low-energy / minimum embodiment. As shown in FIG. 4, in a "low-power" embodiment, the ADFMR circuit may include an upstream matching network upstream of the ADFMR device and a downstream matching network downstream of the ADFMR device.

[0076]

[0107] As shown in the example of FIG. 30 , in a second embodiment of the interferometer circuit of the first system, the ADFMR circuit includes the aforementioned ADFMR device and an attenuator. In some variations, the attenuator can be located upstream of the ADFMR device. Alternatively, the attenuator can be located downstream of the ADFMR device. The ADFMR device can optionally have an upstream inductor located upstream of the ADFMR device and a downstream inductor located downstream of the ADFMR device. The reference circuit can have many different variations. In one variation, the reference circuit includes a phase shifter and an attenuator. The phase shifter functions to shift the unaltered reference signal 180 degrees out of phase so that when combined with the unaltered test signal, the test signal and the reference signal completely destructively interfere with each other.

[0077]

[0108] The system may also be used as a gradiometer. The gradiometer functionality may be an additional or alternative function of the system depending on the embodiment. As shown in FIG. 31 , in a first gradiometer variation of the first system, the system includes a power source, at least one circuit, and a detector circuit including an analog-to-digital converter. The at least one circuit preferably includes an ADFMR circuit set including at least a first ADFMR circuit and a second ADFMR circuit. The second ADFMR circuit is disposed in parallel with the first ADFMR circuit. Furthermore, the first ADFMR circuit and the second ADFMR circuit may be spatially positioned such that the vector displacement between the two ADFMR circuits is known. The system further includes a power splitter disposed upstream of the first test circuit and the second test circuit, the power splitter configured to split the electrical signal into two test signals: a first test signal traveling through the first ADFMR circuit and a second test signal traveling through the second ADFMR circuit. The system also includes a power combiner disposed downstream of the first ADFMR circuit and the second ADFMR circuit, the power combiner configured to combine a first test signal output from the first ADFMR circuit and a second test signal output from the second ADFMR circuit. A gradiometer variant of the system may function to measure the gradient of the EM field by measuring the difference in perturbations of the altered first test signal traveling through the first ADFMR circuit and the altered second test signal traveling through the second ADFMR circuit. Depending on the embodiment, additional test signals may be added to the system, enabling, for example, a full three-dimensional field gradient measurement.

[0078]

[0109] In one example of a gradiometer variation of the first system, the first ADFMR circuit includes a first ADFMR device and a first attenuator. In some variations, the first attenuator may be disposed upstream of the first ADFMR circuit. Alternatively, the first attenuator may be disposed downstream of the first ADFMR circuit. Furthermore, the second ADFMR circuit may include a second ADFMR device and a second attenuator. In some variations, the second attenuator may be disposed upstream of the second ADFMR circuit. Alternatively, the second attenuator may be disposed downstream of the second ADFMR circuit. The first ADFMR device may optionally have a first upstream inductor disposed upstream of the first ADFMR device and a first downstream inductor disposed downstream of the first ADFMR device. The second ADFMR device may optionally have a second upstream inductor disposed upstream of the second ADFMR device and a second downstream inductor disposed downstream of the second ADFMR device.

[0079]

[0110] All variations of the ADFMR device may have different configurations. In some variations, the ADFMR device includes a surface acoustic wave (SAW) device. In particular, in both the interferometer and gradiometer variations, the ADFMR device may include a SAW device. The SAW device functions to generate and use SAW waves to achieve ferromagnetic resonance, thereby measuring the EM field (and EM field gradients) via the SAW waves. Depending on the embodiment, other types of ADFMR devices may be used. Other examples include F-bar and BAW devices.

[0080]

[0111] Because SAWs are altered due to the magnetostrictive properties of ferromagnetic materials embedded in the SAW device, in many variations, a single SAW device is typically sensitive to EM fields in a single orientation (e.g., capable of measuring fields in the "x" direction). Depending on the desired implementation, more complex SAW devices (e.g., those of FIGS. 14-18) or multiple SAW devices can be implemented for multidimensional field and field gradient measurements. In one three-dimensional interferometer embodiment, the system includes three ADFMR test circuits, each including an ADFMR device arranged in an orthogonal direction. In one three-dimensional gradiometer embodiment, the system includes twelve ADFMR test circuits, each set of four having an ADFMR device with the same orientation, each set of four defining a three-dimensional space spanning the position (e.g., measuring the x-direction gradient of an EM field in the x, y, and z directions).

[0081]

[0112] In some variations, the system can be implemented for multidimensional functionality. Multidimensional functionality can be implemented using any of the variations of the system, including interferometer and gradiometer embodiments. In one multidimensional embodiment, as shown in FIG. 9 , the ADFMR device of the first ADFMR circuit includes a first ADFMR device, and at least one circuit includes a second ADFMR circuit including a second ADFMR device, where the second ADFMR device has a different sensing orientation than the first ADFMR device. In this two-dimensional embodiment, the system can have two-dimensional functionality for measuring in-plane EM fields.

[0082]

[0113] In another multidimensional embodiment, multidimensional sensing can be set up in series, where a first ADFMR circuit includes two ADFMR devices, each of which can have a separate sensing orientation, as shown in FIG.

[0083]

[0114] In some variations, the system may be implemented with noise reduction and / or noise cancellation functionality. Noise reduction functionality may be implemented with any variation of the system, including interferometer and gradiometer embodiments. In one noise reduction interferometer variation, as shown in FIG. 32, the interferometer system may further include a vector modulator circuit acting as an "external" interferometer, arranged in parallel with the first ADFMR circuit. Depending on the embodiment, the vector modulator circuit may function as an analog subtraction circuit to reduce ambient noise and / or 1 / f noise.

[0084]

[0115] In some variations, the system may be implemented using an IQ mixer circuit. The IQ mixer circuit may improve signal measurement by separating the perturbed electrical signal into a linear combination of orthogonal waves. The IQ mixer may be implemented in any system variation, including interferometer and gradiometer embodiments. In one IQ mixer interferometer variation, as shown in FIG. 33, the interferometer system further includes an IQ mixer circuit positioned upstream of the detector circuit to receive the electrical signal output from the interferometer circuit and another electrical signal input. In some embodiments, this other signal input includes an input from the original electrical signal. Depending on the desired embodiment, the original electrical signal to the IQ mixer may be unchanged or modified (e.g., by including an amplifier circuit between the power source and the IQ mixer).

[0085]

[0116] The system can be modified to measure the applied external EM field within a desired field magnitude bandwidth so that the ADFMR device performs optimally or near-optimally. In these variations, the system can be implemented with a linearization circuit. The linearization circuit allows for normalization of the external EM field to the desired field magnitude bandwidth. Linearization can be implemented in any system variation, including interferometer and gradiometer embodiments. In one interferometer system embodiment of the linearization circuit, as shown in FIG. 34, the system further includes a linearization circuit. The linearization circuit includes an EM field source targeting the first ADFMR circuit, a comparator, and logic circuitry. The linearization circuit can be configured to operate in a setup mode in which the EM field source modifies the applied EM field so that the EM field applied to the first ADFMR circuit is within an improved measurement regime. The setup mode can thus gradually improve the measurement regime, thereby gradually bringing the system into an optimal or near-optimal measurement regime.

[0086] 3. Method

[0117] As shown in FIG. 35, a method for measuring an EM field using an acoustically driven ferromagnetic (ADFMR) sensor includes generating an electrical signal in an oscillator (S110), converting the electrical signal to an acoustic wave in the ADFMR sensor (S120), propagating the acoustic wave to a magnetic material in the ADFMR sensor (S130), thereby modifying the acoustic wave proportionally to the EM field affecting the magnetic material, converting the modified acoustic wave to a modified electrical signal in the ADFMR sensor (S140), and measuring the EM field using the modified acoustic wave (S150).

[0087]

[0118] The method functions to measure an EM field by utilizing the sensitivity of a ferromagnetic material at or near resonance to the EM field. In preferred variations, the method may include additional steps to optimize the field measurement. These additional steps may include reducing signal bandwidth, reducing signal noise, and optimizing field absorption. The method may additionally and / or alternatively include other steps to improve the field measurement. While the method is preferably used with the systems described above, it may be practiced with any desired applicable system. The method may be particularly useful when the ADFMR sensor is implemented as an interferometer to measure the EM field by recombining an altered electrical signal with an unaltered reference signal. The method may also be particularly useful when the ADFMR sensor is implemented as a gradiometer to determine changes in the EM field using multiple field measurements in space.

[0088]

[0119] In some variations, the method may be implemented to enable interferometer functionality, and may further include splitting the electrical signal into a test electrical signal and a reference electrical signal before the ADFMR sensor, combining the altered electrical signal with the reference electrical signal after the ADFMR sensor, and determining the EM field strength using the reference signal.

[0089]

[0120] In some variations, the method may be implemented to enable gradiometer functionality. In these variations, the method may further include splitting the electrical signal into multiple test signals prior to the ADFMR sensor.

[0090]

[0121] Block S110, which includes generating an electrical signal, functions to provide power for the ADFMR functionality. The generating of the electrical signal (S110) can generate either a direct current (DC) or an alternating current (AC). In some variations, the electrical signal is AC, and the generating of the electrical signal (S110) is performed with a voltage generator. In some variations, the AC may be on the order of MHz to GHz. Alternatively, the AC frequency may be higher or lower. In preferred variations, the AC frequency is on the order such that the electrical signal complements an acoustic transducer, and all or a portion of the electrical signal can be converted into acoustic waves.

[0091]

[0122] In many variations, the method can include splitting an electrical signal. Splitting an electrical signal functions to take a single current (e.g., AC or DC) and split it into two currents. In interferometer variations, these currents can include a test signal and a reference signal for the ADFMR sensor. Splitting the current can enable comparative measurements of the test signal and the reference signal as part of the interferometer variations. In gradiometer embodiments, splitting the signal can split the electrical signal into two test signals (e.g., a first test signal and a second test signal) that are sent to separate ADFMR sensors. Depending on the embodiment, all method steps that refer to or apply to a test signal or ADFMR sensor refer to or apply equally to all ADFMR sensors and / or all test signals.

[0092]

[0123] In addition to interferometer and gradiometer variations, electrical signal splitting can be implemented to enhance or improve the functionality of EM field measurements in many variations. Electrical signal splitting can be performed zero, one, or multiple times, depending on the embodiment. For example, electrical signal splitting can be implemented in combination with specific circuits and components to amplify desired signals, perform multi-dimensional field measurements, filter noise (e.g., reduce 1 / f noise), optimize field detection (e.g., by field normalization), and / or improve field measurements. In variations involving electrical signal splitting, the method can further include the additional step of combining the electrical signals into a single signal.

[0093]

[0124] Block S120, which includes converting the electrical signal into acoustic waves (S120), functions to convert part or all of the electrical signal into acoustic waves. The conversion of the electrical signal is preferably performed in the ADFMR sensor. More precisely, block S120 is performed in an acoustic transducer in or on the ADFMR sensor, where the electrical signal is absorbed to generate acoustic waves of a desired type, frequency, and amplitude.

[0094]

[0125] The acoustic waves generated can be of any desired type, provided that they function with the ADFMR sensor. Examples of acoustic waves that can be generated include surface acoustic waves (SAW), bulk acoustic waves (BAW), Fbar, Lamb waves, and any other type of acoustic wave. In a preferred variation, the frequency and amplitude of the acoustic wave are proportional to the converted electrical signal. That is, a relatively large electrical signal can generate a relatively large acoustic wave, and / or a relatively high frequency electrical signal can generate a relatively high frequency acoustic wave.

[0095]

[0126] In some variations, converting the electrical signal to an acoustic wave (S120) includes generating a SAW from the electrical signal. In these variations, the ADFMR sensor may include a SAW device. In these variations, generating the SAW may include generating the SAW from the electrical signal using a piezoelectric material. In a preferred variation, the electrical signal is converted into a radio frequency (RF) field, which is then converted into a SAW by an input interdigital transducer (IDT), although other methods may be implemented. In this variation, the input IDT is preferably a component of the SAW device, and the SAW device further includes a piezoelectric substrate base, an output IDT, and a ferromagnetic material along the piezoelectric substrate between the input and output IDTs. Generating the SAW preferably generates a SAW at or near the resonant frequency of the ferromagnetic material.

[0096]

[0127] Block S130, which includes propagating an acoustic wave to a magnetic material on the ADFMR sensor, allows for perturbation of the acoustic wave proportional to the effect of the EM field on the magnetic material. The external EM field biases the magnetic material, thereby altering the acoustic wave proportional to the magnitude of the EM field. In SAW device variations, as the SAW travels along a ferromagnetic material, the ferromagnetic material may be excited into resonance, causing the ferromagnetic material to absorb a portion of the incident acoustic wave. Near resonance, the amount of absorbed acoustic power varies significantly with the external magnetic field. In some variations, the ferromagnetic material is magnetostrictive, and the propagating acoustic wave may generate an effective RF magnetic field (at the frequency of the acoustic wave or an integer multiple thereof) within the ferromagnetic material. In other variations, the ferromagnetic material may have other properties that allow for perturbation of the propagating acoustic wave. The perturbation of the acoustic wave can be of any desired type, with the limiting factor being that the perturbation is proportional to the magnitude and direction of the EM field. Thus, Block S130 may include sensing the external EM field using the altered acoustic wave.

[0097]

[0128] Block S140, converting the altered acoustic wave to an altered electrical signal, allows the altered electrical signal to be used to measure the field. The conversion of the altered acoustic wave to an altered electrical signal can be performed in the ADFMR sensor, preferably in an acoustic transducer. In variations in which the ADFMR sensor includes a SAW device, the acoustic transducer can include an output IDT. Thus, the conversion of the altered acoustic wave to an altered electrical signal (S140) can be performed in an output IDT on the piezoelectric substrate of the SAW device. Thus, like the altered acoustic wave, the altered electrical signal contains information about the external EM field.

[0098]

[0129] Block S150, which includes measuring the field, functions to determine the strength of the EM field at the detector. This is preferably accomplished by combining the altered electrical signal with a reference signal and using interference (e.g., destructive interference) to determine the field strength. In some variations using destructive interference, measuring the field (S150) may include shifting the phase of the reference field by one half period so that the reference signal and the original electrical signal cancel each other. In an alternative preferred variation for measuring the field gradient, measuring the field (S150) may include determining the difference in field strength between the altered electrical signals (e.g., determining the difference between first and second altered test signals).

[0099]

[0130] Measuring the field (S150) may include converting the signal to a digital signal. Converting the signal to a digital signal may have two variations: the test signal and the reference signal may be first combined and then digitized, or they may be digitized separately and then combined. Measuring the field (S150) may include combining the altered electrical signal and the reference signal and then converting the combined signal to a digital output signal, or may include converting the altered electrical signal to an altered digital electrical signal and converting the reference signal to a digital reference signal and then combining the digital test signal and the digital reference signal.

[0100]

[0131] Extremely sensitive measurements, noise, and other environmental issues can impair the accuracy of electromagnetic field measurements made using this method. The method can include additional steps to improve the electromagnetic field measurements. In addition to other possible improvement steps, the method can include reducing the signal bandwidth, reducing signal noise, and optimizing field absorption.

[0101]

[0132] Signal bandwidth reduction serves to produce a narrow, coherent signal band rather than a large signal spectrum. Signal bandwidth reduction is preferably performed with a bandpass filter, although other filters may additionally or alternatively be used. Signal bandwidth reduction can reduce signal noise. Furthermore, signal bandwidth reduction can improve the size and spacing of acoustic wave packets to minimize interference between separate acoustic wave packets.

[0102]

[0133] Signal noise reduction serves to reduce system noise that can affect electromagnetic field measurements. In particular, 1 / f (i.e., pink noise) can be a major factor impeding accurate electromagnetic field measurements. Signal noise reduction can include reducing the power of the signal and filtering the signal to reduce noise. Signal noise reduction can include passing the electrical signal through an attenuator. Digital attenuators can be implemented to remove all activity below a certain threshold, and analog attenuators can be implemented to reduce power and minimize noise. 1 / f noise can also be minimized by using interferometers or bias coils to minimize the signal power input to any amplifiers or other active components.

[0103]

[0134] In some variations, the method may include optimizing field absorption. Optimizing field absorption functions to improve field absorption by the ferromagnetic material. The ferromagnetic material may have an optimal field strength where the magnitude of absorption is most sensitive to the external field. Optimizing field absorption may include modifying the applied field strength to improve the electromagnetic field measurement. In one example, optimizing field absorption may include determining an optimal field absorption strength range and applying a field to the ADFMR sensor such that the total applied field is at or approximately this optimal field absorption strength range.

[0104] 4. System Architecture

[0135] Systems and methods of embodiments can be embodied and / or performed, at least in part, in association with a computing system including at least one machine configured to receive a computer-readable medium having computer-readable instructions stored thereon. The ADFMR device-enabled systems and methods described above can be integrated within a computing system to enable programmatic control of such devices. The computing system can utilize sensor inputs providing EM field sensor data. The computing system can include one or more ADFMR-enabled systems. The instructions can be executed by computer-executable components integrated with an application, applet, host, server, network, website, communication service, communication interface, hardware / firmware / software elements of a user computer or mobile device, wristband, smartphone, or any suitable combination thereof. Other systems and methods of embodiments can be embodied and / or performed, at least in part, as a machine configured to receive a computer-readable medium having computer-readable instructions stored thereon. The instructions can be executed by computer-executable components integrated with devices and networks of the types described above. The computer-readable medium may be stored on any suitable computer-readable medium, such as RAM, ROM, flash memory, EEPROM, an optical device (CD or DVD), a hard drive, a floppy drive, or any suitable device. The computer-executable component may be a processor, although any suitable dedicated hardware device may (alternatively or additionally) execute the instructions.

[0105]

[0136] In one variation, the system comprises one or more computer-readable media storing instructions that, when executed by one or more computer processors, cause the computing platform to perform operations including those of the systems or methods described herein, such as generating electrical signals, converting electrical signals into acoustic waves, propagating acoustic waves through magnetic materials, converting the altered acoustic waves into altered electrical signals, and measuring electromagnetic fields.

[0106]

[0137] In one variation, the non-transitory computer-readable medium stores instructions that, when executed by one or more computer processors of a computing platform, cause the computing platform to perform operations including those of the systems or methods described herein, such as generating electrical signals, converting the electrical signals into acoustic waves, propagating the acoustic waves through a magnetic material, converting the altered acoustic waves into altered electrical signals, and measuring electromagnetic fields.

[0107]

[0138] 36 is an exemplary computer architecture diagram of one embodiment of the system. In some embodiments, the system is implemented on multiple devices in communication with a communication channel and / or network. In some embodiments, elements of the system are implemented on separate computing devices. In some embodiments, two or more of the system elements are implemented on the same device. The system and portions of the system may be integrated into a computing device or system that can function as or within the system.

[0108]

[0139] The communication channel 1001 interfaces with the processors 1002A-1002N, memory (e.g., random access memory (RAM)) 1003, read-only memory (ROM) 1004, processor-readable storage medium 1005, display device 1006, user input device 1007, and network device 1008. As shown, a computer infrastructure can be used to connect the power source 1101, ADFMR circuitry 1102, detector circuitry 1103, and / or other suitable computing devices. Alternatively, the systems described above can be implemented as self-contained systems connected to a computer infrastructure.

[0109]

[0140] The processors 1002A-1002N can take many forms, such as a CPU (Central Processing Unit), a GPU (Graphics Processing Unit), a microprocessor, an ML / DL (Machine Learning / Deep Learning) processing unit such as a tensor processing unit, an FPGA (Field Programmable Gate Array), a custom processor, and / or any suitable type of processor.

[0110]

[0141] The processors 1002A-1002N and main memory 1003 (or any subcombination) may form a processing unit 1010. In some embodiments, the processing unit includes one or more processors communicatively coupled to one or more of RAM, ROM, and a machine-readable storage medium. The one or more processors of the processing unit receive instructions stored by one or more of RAM, ROM, and a machine-readable storage medium via a bus and execute the received instructions. In some embodiments, the processing unit is an ASIC (application-specific integrated circuit). In some embodiments, the processing unit is a SoC (system-on-chip). In some embodiments, the processing unit includes one or more of the elements of a system.

[0111]

[0142] The network device 1008 may provide one or more wired or wireless interfaces for exchanging data and commands between the system and / or other devices, such as devices in external systems, including, for example, a Universal Serial Bus (USB) interface, a Bluetooth interface, a Wi-Fi interface, an Ethernet interface, a near field communication (NFC) interface, etc.

[0112]

[0143] Computer and / or machine-readable executable instructions comprising configurations for software programs (such as operating systems, application programs, and device drivers) can be stored in memory 1003 from processor-readable storage medium 1005, ROM 1004, or any other data storage system.

[0113]

[0144] Each machine-executable instruction, when executed by one or more computer processors, may be accessed by at least one of processors 1002A-1002N (of processing unit 1010) via communication channel 1001 and then executed by at least one of processors 1001A-1001N. Data, databases, data records, or other forms of storage of data generated or used by the software programs may also be stored in memory 1003. Such data is accessed by at least one of processors 1002A-1002N during execution of the machine-executable instructions of the software programs.

[0114]

[0145] The processor-readable storage medium 1005 may be one (or a combination of two or more) of a hard drive, a flash drive, a DVD, a CD, an optical disk, a floppy disk, flash storage, a solid-state drive, a ROM, an EEPROM, an electronic circuit, a semiconductor memory device, etc. The processor-readable storage medium 1005 may include an operating system, software programs, device drivers, and / or other suitable subsystems or software.

[0115]

[0146] As used herein, first, second, third, etc. are used to characterize and distinguish various elements, components, regions, layers, and / or sections. These elements, components, regions, layers, and / or sections are not limited by these terms. The use of numerical terms may be used to distinguish one element, component, region, layer, and / or section from another element, component, region, layer, and / or section. The use of such numerical terms does not imply a sequence or order unless the context clearly dictates otherwise. Such numerical reference symbols may be used interchangeably without departing from the teachings of the embodiments and variations herein.

[0116]

[0147] Those skilled in the art will appreciate from the foregoing detailed description, and from the drawings and claims, that changes and variations can be made to the embodiments of the invention without departing from the scope of the invention, which is defined in the claims that follow.

Claims

1. 1. A system for an acoustically driven ferromagnetic resonance (ADFMR) based sensor, comprising: a power source including an electronic oscillator providing an electrical signal; an ADFMR circuit set including a first ADFMR circuit including an ADFMR device and a second ADFMR circuit, the first ADFMR circuit enabling perturbation of the electrical signal by an electromagnetic (EM) field, the second ADFMR circuit connected in parallel to the first ADFMR circuit; a current splitter arranged upstream of the first ADFMR circuit and the second ADFMR circuit, for splitting the electrical signal into two test signals, a first test signal passing through the first ADFMR circuit and a second test signal passing through the second ADFMR circuit; a power combiner disposed downstream of the first ADFMR circuit and the second ADFMR circuit, for combining the first test signal output from the first ADFMR circuit and the second test signal output from the second ADFMR circuit; a detector circuit for determining the EM field from perturbations in the electrical signal; A system including:

2. The system of claim 1 , wherein the ADFMR circuit set includes an interferometer circuit.

3. 3. The system of claim 2, wherein the ADFMR circuit set further includes a first signal processing circuit that is a first reference circuit, the first reference circuit being arranged in parallel with the first ADFMR circuit such that the first ADFMR circuit and the first reference circuit combine to form an interferometer circuit.

4. The first ADFMR circuit comprises: an upstream matching network upstream of the ADFMR device; a downstream matching network downstream of the ADFMR device; The system of claim 1 further comprising:

5. The system of claim 1 , wherein the first ADFMR circuit further comprises an attenuator.

6. The system of claim 5 , wherein the first ADFMR circuit further comprises a phase shifter.

7. The system of claim 6 , wherein the ADFMR device comprises a surface acoustic wave device.

8. The system of claim 1 , wherein the ADFMR device includes a first ADFMR device, and the first ADFMR circuit includes the first ADFMR device and a first attenuator.

9. The system of claim 8 , wherein the second ADFMR circuit includes a second ADFMR device and a second attenuator.

10. The system of claim 9 , wherein the first ADFMR device comprises a first surface acoustic wave device and the second ADFMR device comprises a second surface acoustic wave device.

11. the ADFMR device of the first ADFMR circuit includes a first ADFMR device; the second ADFMR circuit includes a second ADFMR device; The system of claim 1 , wherein the second ADFMR device has a different sensing orientation than the first ADFMR device.

12. The system of claim 1 , wherein the first ADFMR circuit includes a first ADFMR device and a second ADFMR device, each ADFMR device having a different sensing orientation.

13. The system of claim 3 , wherein the set of ADFMR circuits further includes a vector modulator circuit arranged in parallel with the first ADFMR circuit.

14. the ADFMR circuit set further includes an IQ mixer circuit; the IQ mixer circuit is positioned upstream of the detector circuit to receive the electrical signal output from the interferometer circuit and another electrical signal input; The system of claim 3.

15. 15. The system of claim 14, wherein the other electrical signal input comprises an input from the electrical signal provided by the electronic oscillator.

16. 4. The system of claim 3, wherein the ADFMR circuit set further includes a linearization circuit, the linearization circuit including an EM field source targeted at the first ADFMR circuit, a comparator, and a logic circuit.

17. 17. The system of claim 16, wherein the linearization circuit is configured to operate in a setup mode in which the EM field source varies the applied EM field so that the EM field applied to the first ADFMR circuit is within a desired measurement regime.

18. 1. A method for EM field measurement using a system for acoustically driven ferromagnetic (ADFMR) sensors, comprising: generating an electrical signal in an oscillator; - converting said electrical signal into an acoustic wave in an ADFMR sensor; propagating the acoustic wave in a magnetic material in the ADFMR sensor, thereby modifying the acoustic wave in proportion to the magnitude of the EM field; converting the altered acoustic waves into altered electrical signals in the ADFMR sensor; Including, The system comprises: a power source including said oscillator; an ADFMR circuit set including a first ADFMR circuit and a second ADFMR circuit, the first ADFMR circuit enabling perturbation of the electrical signal by the EM field, and the second ADFMR circuit connected in parallel to the first ADFMR circuit; a current splitter preceding the ADFMR sensor, which splits the electrical signal into two test signals, a first test signal which passes through the first ADFMR circuit and a second test signal which passes through the second ADFMR circuit; a power combiner downstream of the ADFMR sensor, which combines the first test signal output from the first ADFMR circuit and the second test signal output from the second ADFMR circuit; A method comprising:

Images