Patent Application
20130300408
N/A
As is well known, anisotropic magnetoresistance (AMR) causes a change in resistance of a thin strip of ferrous material when a magnetic field is applied perpendicular to a current flowing in the strip. Magnetic field sensors based on AMR characteristic of ferrous materials are also well known, as is the fact that these types of magnetometers need to apply an external magnetic field in order to set or reset the magnetic domain structure of the device after a large magnetic field disruption. The set/reset (S/R) field is usually generated by conductive coils either underneath or above the plane of the magnetic field sensing layer of the device. Based on Ampere's law, the field generated by the conductive coils is proportional to the current applied, thus, current strength is directly proportional to set or reset efficiency. Higher currents, however, come with a power consumption penalty that may outweigh any increase in sensor reliability or accuracy.
The modern electronic compass requires the magnetometer to be effectively used in a relatively high magnetic field environment, such as those found in smart phones or tablet computers. Increasing the effectiveness, however, usually requires a stronger set/reset field, which would be generated by a higher current and, therefore, would increase power consumption.
What is needed, therefore, is an accurate magnetic field sensor that is small in size, of low cost, that requires low power as is necessitated by mobile device applications, is easy to use and that is easily incorporated into a mobile device.
A magnetometer with a set/reset coil having portions that cross portions of sensing strips at an angle in order to create a magnetic field in the sensing strip that is at an angle with respect to the easy axis of magnetization of the sensing strip. Each sensing strip may have a portion having a magnetic field created therein that is different from a magnetic field created in another portion of the same sensing strip. As a result, a lower set/reset coil current is needed to initialize the magnetometer.
One embodiment of the present invention is a magnetometer with a plurality of sensing strips disposed in a planar substrate where each sensing strip has a long axis. A planar set/reset coil is disposed on the planar substrate parallel and adjacent to the plurality of sensing strips and a first coil portion of the set/reset coil is oriented with respect to a first portion of a first sensing strip at a first angle +α, where 0°<α<90°, with respect to a virtual line or axis perpendicular to the long axis of the first sensing strip.
Embodiments of the present invention may be better understood by referring to the following description in conjunction with the accompanying drawings in which:
It will be appreciated that for simplicity and clarity of illustration, elements shown in the drawings have not necessarily been drawn accurately or to scale. For example, the dimensions of some of the elements may be exaggerated relative to other elements for clarity or several physical components may be included in one functional block or element. Further, where considered appropriate, reference numerals may be repeated among the drawings to indicate corresponding or analogous elements. Moreover, some of the blocks depicted in the drawings may be combined into a single function.
This application claims priority of U.S. Provisional Patent Application Ser. No. 61/645,820 for “Magnetometer With Angled Set/Reset Coil,” filed May 11, 2012, the entire contents of which is incorporated by reference herein for all purposes.
In the following detailed description, numerous specific details are set forth in order to provide a thorough understanding of the embodiments of the present invention. It will be understood by those of ordinary skill in the art that these embodiments of the present invention may be practiced without some of these specific details. In other instances, well-known methods, procedures, components and structures may not have been described in detail so as not to obscure the embodiments of the present invention.
Prior to explaining at least one embodiment of the present invention in detail, it is to be understood that the invention is not limited in its application to the details of construction and the arrangement of the components set forth in the following description or illustrated in the drawings. The invention is capable of other embodiments or of being practiced or carried out in various ways. Also, it is to be understood that the phraseology and terminology employed herein are for the purpose of description only and should not be regarded as limiting.
It is appreciated that certain features of the invention, which are, for clarity, described in the context of separate embodiments, may also be provided in combination in a single embodiment. Conversely, various features of the invention, which are, for brevity, described in the context of a single embodiment, may also be provided separately or in any suitable sub-combination.
As is well known in the art, and with reference to
Each AMR resistor has the same resistance when no magnetic field is applied. An applied bridge voltage causes current to flow through the resistors and a cross-applied magnetic field will change the resistance in pairs of resistors in the bridge. An output of the bridge is, therefore, proportional to the applied magnetic field. In the presence of an external magnetic field, the resistance of the AMR resistors changes in accordance with the magnetic field magnitude and polarity so that a differential voltage signal appears on the two output nodes OUT+ and OUT−.
A magnetic field sensor based on AMR technology is known to include a thin film permalloy material deposited on a silicon wafer while a strong magnetic field is applied to create permalloy resistors, i.e., the AMR resistors in the bridge configuration. The magnetic domains of these permalloy resistors are aligned in the same direction as the applied field thereby establishing a magnetization vector. Subsequent lithographic and etching steps define the geometry of the AMR resistors.
Known AMR magnetometers in the market use set/reset coils having portions that are perpendicular to a sensor long axis so the generated magnetic field is parallel to the long axis. Thus, referring to
A set/reset (S/R) coil 112 is provided adjacent to the pluralities of left-side strips 108.n and right-side strips 104.n in a separate plane that is effectively parallel to the plane of the permalloy strips. The S/R coil 112 plane is shown herein as being “below” the plane of the strips in
Referring to
The generated magnetization vectors MR and ML are essentially parallel to the long axis of the strips 108.n and 104.n, respectively, because the coil portions of the S/R coil 112 are at right angles to the long axes of these strips. Thus, the current through the S/R coil 112 is used to initialize the magnetization vectors of the strips and initialize the Wheatstone bridge for measurements.
Thus, the known S/R coil 112 flips the magnetic domains of the strips in opposite directions. As a result of this flipping, the measurement signal changes polarity as well. The sensor offsets due to resistor manufacturing tolerances remain the same value, however, but by subtracting the two readings, the offset error can be eliminated from the output signal.
It is known, however, that the operation of the S/R coil 112 requires a significant amount of current in order to affect the magnetization of the strips. This requirement is a disadvantage in, for example, mobile, handheld and other similar applications where low power consumption is important in order to maximize battery life and, therefore, operating time.
Modern electronic compasses need a magnetometer with a higher linear range for use in a relatively high magnetic field environment, such as in smart phones. Even though the earth's magnetic field is less than one gauss, the electronics in smart phones could generate a magnetic field in a range from a few to ten gauss. One way to increase an AMR magnetometer's dynamic range is to increase its shape anisotropy. Unfortunately, the linear range increase may require a higher set/reset field, which needs to be generated by a higher current with its power consumption drawbacks. So, a mechanism other than simply adding more power to the coils is needed for practical applications.
Based on Stoner-Wohlfarth theory, a uniform magnetic particle can be switched much more easily when the magnetic field is applied to it at an angle between zero and 90 degrees. A magnetic film strip, for example, permalloy, however, is different from the case of uniform particles as the magnetic domain switching occurs through domain wall nucleation and propagation. The domain nucleation process also depends on the angle between an applied magnetic field and a sensor easy axis (long axis).
As represented in Equation 1, the magnetic field hS changes as a function of an angle α with respect to a line normal to the long axis of the magnetic strip.
As shown in
One consideration is, when the field is applied at an angle other than at zero degrees, i.e., perpendicular to the long axis, whether or not the magnetic domain in the strip will remain tilted after the field is removed by stopping the current. First of all, the sensor strip has a high aspect ratio, i.e., it is very long and very narrow or thin, and the magnetic domains are strongly coupled to each other because there is no decoupling boundary applied. After the field is removed, a majority of the domains will follow the easy axis, shape anisotropy, direction. In some instances, the domain will remain tilted because of local pinning or locally high anisotropy as even a field applied at zero degrees instead of a tilted field will stay tilted after the field is applied. It has been determined that as long as the angle is relatively small, the approach described herein provides advantages over the known approaches.
Referring now to
Thus, as a convention in this specification, referring to
Returning to
The SR legs 208 and 224 cross first and second end portions of each of the left-side strips 108.n, respectively, at opposite angles −α and +α but alternate with respect to adjacent strips. The SR leg 216 crosses a middle portion of each left-side strip 108.n at a right angle, i.e., α=0°. The SR leg 216 is much wider than the SR legs 208, 224 and covers a much wider section of the left-side strips 108.n. The width of the middle portion is anywhere from 3-6 times wider than each side portion and, therefore, covers most of the permalloy strip.
As a result, for example, in the left-side strips 108.n, a current +IU introduced at the IF+ lead of the SR coil 204 will induce a magnetization vector MRU in a left end portion of the left-side strip 108.4, a magnetization vector MR in a middle portion of the strip 108.4 and a magnetization vector MRD in a right end portion of the strip 108.4. These magnetization vectors will alternate in the left-side strips 108.n as shown.
In the right-side strips 104.n, a current +IU introduced at the IF+ lead of the SR coil 204 will induce a magnetization vector MLD in a left end portion of the right-side strip 104.4, a magnetization vector ML in a middle portion of the strip 104.4 and a magnetization vector MLU in a right end portion of the strip 104.4. These magnetization vectors will alternate in the right-side strips 104.n as shown.
As above, the strips are set up as a Wheatstone Bridge circuit where, for example, left-side strips 108.1 and 108.4 are in series with one another to form a first leg, and left-side strips 108.2 and 108.3 are in series with one another to form a second leg, right-side strips 104.1 and 104.4 are in series with one another to form a third leg and right-side strips 104.2 and 104.3 are in series with one another to form a fourth leg.
Of course, if the current were reversed, i.e., −IU, then the magnetization vectors would also be reversed.
With the SR coil 204, the left and right portions of each permalloy strip 108.n and 104.n are magnetized at different angles, respectively. The middle portion of each strip 108.n and 104.n is magnetized along the respective easy-axis.
In another embodiment of the present invention, as shown in
Referring now to
The S/R coil 404 includes six SR legs 408, 412, 416, 420, 424 and 428 that cross portions of the left-side strips 108.n and the right-side strips 104.n. The SR legs 408, 416 and 424 cross portions of the left-side strips 108.n and the SR legs 412, 420 and 428 cross portions of the right-side strips 104.n. The SR portions 416 and 420 cross the middle portions of the left-side strips 108.n and the right-side strips 104.n
The SR legs 408 and 424 cross first and second end portions of each of the left-side strips 108.n, respectively, at the same angle, either −α or +α, but alternate with respect to adjacent strips. The SR leg 416 crosses a middle portion of each left-side strip 108.n at a right angle, i.e., α=0°. The SR leg 416 is much wider than the SR legs 408, 424 and covers a much wider section of the left-side strips 108.n.
As a result, for example, in the left-side strips 108.n, a current +IU introduced at the IF+ lead of the SR coil 404 will induce a magnetization vector MRU in a left end portion of the left-side strip 108.4, a magnetization vector MR in a middle portion of the strip 108.4 and a magnetization vector MRU in a right end portion of the strip 108.4. These magnetization vectors will alternate in adjacent strips in the left-side strips 108.n as shown.
In the right-side strips 104.n, a current +IU introduced at the IF+ lead of the SR coil 404 will induce a magnetization vector MLU in a left end portion of the right-side strip 104.4, a magnetization vector ML in a middle portion of the strip 104.4 and a magnetization vector MLU in a right end portion of the strip 104.4. These magnetization vectors will alternate in adjacent strips in the right-side strips 104.n as shown. The left-side and right-side strips are similarly connected as described above to create the Wheatstone Bridge circuit.
As described above, the tilted coils 204, 404 can be used to start the domain wall at the end portions of the permalloy strips 108.n, 104.n. The perpendicular portions drive the domain wall propagation for the middle portions of the strips, which is also the sensing portion. As a result, the sensing elements will have the same magnetic domain configuration as in the non-tilted coil case.
In another embodiment of the present invention, as shown in
Referring now to
The S/R coil 504 includes six SR legs 508, 512, 516, 520, 524 and 528 that cross portions of the left-side strips 108.n and the right-side strips 104.n. The SR legs 508, 516 and 524 cross portions of the left-side strips 108.n and the SR legs 512, 520 and 528 cross portions of the right-side strips 104.n. The SR portions 516 and 520 cross the middle portions of the left-side strips 108.n and the right-side strips 104.n
The SR legs 508, 516 and 524 cross first and second end portions of each of the left-side strips 108.n, respectively, at the same angle, either −α or +α. The SR leg 516 is much wider than the SR legs 508, 524 and covers a much wider section of the left-side strips 108.n.
As a result, for example, in the left-side strips 108.n, a current +IU introduced at the IF+ lead of the SR coil 504 will induce a magnetization vector MRU in a left end portion of the left-side strip 108.4, a magnetization vector MRU in a middle portion of the strip 108.4 and a magnetization vector MRU in a right end portion of the strip 108.4. These magnetization vectors will alternate from adjacent strips in the left-side strips 108.n as shown.
In the right-side strips 104.n, a current +IU introduced at the IF+ lead of the SR coil 504 will induce a magnetization vector MLU in a left end portion of the right-side strip 104.4, a magnetization vector MLU in a middle portion of the strip 104.4 and a magnetization vector MLU in a right end portion of the strip 104.4. These magnetization vectors will alternate from adjacent strips in the right-side strips 104.n as shown. The left-side and right-side strips are similarly connected as described above to create the Wheatstone Bridge circuit.
Advantageously, when the magnetic fields in a strip are parallel to each other, the additional benefit of reduced switching current should be attainable.
It is also considered that other configurations are available. For example, the structures described above may be augmented with strips that are magnetized along the easy axis in all portions of the strip by providing multiple groups of left-side and right-side strips.
Of course, one of ordinary skill in the art will understand that the set/reset coil configurations shown herein are for explanatory purposes only. The geometry of an S/R coil could be different from that shown but still cross the permalloy strips at the appropriate angle. For example, depending on how the strips are coupled to one another, or arranged, a portion of the S/R coil may cross two permalloy strips at the appropriate angle thereby possibly saving space on the die or providing some other layout advantage.
Embodiments of the present invention, as described herein provide for improved set/reset operation efficiency by building set/reset coils that are at a pre-specified angle with respect to a sensor strip long axis. These configurations can be applied to AMR, GMR, or TGMR (MTJ) based sensor systems.
Having thus described several features of at least one embodiment of the present invention, it is to be appreciated that various alterations, modifications, and improvements will readily occur to those skilled in the art. Such alterations, modifications, and improvements are intended to be part of this disclosure and are intended to be within the scope of the invention. Accordingly, the foregoing description and drawings are by way of example only, and the scope of the invention should be determined from proper construction of the appended claims, and their equivalents.
This application claims priority of U.S. Provisional Patent Application Ser. No. 61/645,820 for “Magnetometer With Angled Set/Reset Coil,” filed May 11, 2012.
| Number | Date | Country | |
|---|---|---|---|
| 61645820 | May 2012 | US |
