This application claims the priority benefit of Italian patent application number TO2008A000897, filed on Dec. 3, 2008, entitled “BROAD-RANGE MAGNETIC SENSOR AND MANUFACTURING PROCESS THEREOF,” which is hereby incorporated by reference to the maximum extent allowable by law.
1. Field of the Invention
The present invention relates to a broad-range magnetic sensor and a corresponding manufacturing process.
2. Discussion of the Related Art
Among high-sensitivity magnetic-field sensors capable of detecting low-intensity magnetic fields, the magnetic sensor known as a fluxgate sensor offers the best compromise between cost and performance (see, for example, the planar fluxgate sensor described in U.S. Pat. No. 6,404,192). In practice, a planar fluxgate sensor comprises a magnetic core, of a generally elongated shape, overlying an energizing coil. By supplying the energizing coil with an appropriate a.c. excitation current, it is possible to bring the magnetic core into a series of cycles of magnetic saturation. Sensing of external fields is obtained via a pair of sensing coils, generally set underneath the ends of the magnetic core.
For a better understanding, reference is made to
Considering initially only the first arm 4a and the sensing coils 3a, 3b, if the energizing coil is supplied with an appropriate excitation current, able to cause saturation of the magnetic material at an appropriate frequency, the two halves of the first arm 4a are magnetized in opposite directions, as is shown by the arrows 7 in
Instead, if an external magnetic field is applied (arrow H in
The presence of the second arm 4b of the magnetic core enables detection of magnetic fields having a direction perpendicular to the external field M and bestows upon the magnetic sensor 1 two sensitivity axes.
With the fluxgate technology it is possible to provide sensors able to measure d.c. or slowly variable magnetic fields, of an intensity comprised between a few μG and a few G, with a high resolution, of the order of nG. In terms of dynamic range and resolution, the fluxgate devices fall between Hall-effect magnetic-field sensors (which are typically able to detect fields comprised between 10 G and 106 G) and SQUIDs (Superconducting Quantum Interference Devices, which are typically able to detect fields comprised between 10−10 and 10−5 G).
For low values of the magnetic field, fluxgate sensors are preferable to Hall-effect sensors on account of their better performance, and find a wider application as compared to SQUID sensors, thanks to their lower cost and encumbrance. Thus, fluxgate sensors could find application in either portable or non-portable systems where Hall sensors do not have a sufficient sensitivity.
However, in order to continue to exploit the widespread knowledge of the technologies for the production of Hall sensors, there exist solutions in which an attempt has been made to extend the sensitivity of Hall sensors to the range of fluxgate sensors, exploiting the addition, to a Hall sensor, of magnetic material (or concentrator, see, for example, U.S. Pat. No. 6,545,462; U.S. Pat. No. 6,184,679 and U.S. Pat. No. 7,235,968).
These solutions, however, still do not enable the same performance that can be obtained via the fluxgate sensors.
One aim of the present invention is thus to provide a magnetic sensor that overcomes the limitations of known sensors.
According to at least one embodiment of the invention there is provided a magnetic sensor, the corresponding manufacturing process, a magnetometer, and an electronic apparatus.
According to another embodiment of the invention, there is provided a magnetic sensor, comprising a fluxgate sensor and a Hall sensor integrated in the same integrated device.
According to another embodiment of the invention, there is provided a process for manufacturing a magnetic sensor, comprising the step of forming a fluxgate sensor and a Hall sensor in the same integrated device.
In one embodiment the present sensor is formed by the superposition of a fluxgate sensor and of a Hall sensor provided with a concentrator, and the magnetic core of the fluxgate sensor also forms a concentrator for the Hall-effect sensor.
For a better understanding of the present invention, an embodiment thereof is now described, purely by way of non-limiting example, with reference to the attached drawings, wherein:
The fluxgate sensor 11 is, for example, obtained as the fluxgate sensor of
In detail, in the embodiment of
An insulating material layer 20 extends on the body 14 and is formed by a plurality of layers arranged on top of one another and embedding the fluxgate sensor 11. In particular, the fluxgate sensor 11 is formed in three metallization levels and by the magnetic region 13. In detail, a first metallization level forms connection lines 21, a second metallization level forms sensing coils (here only two are visible, designated by 22a and 22b), and a third metallization level forms an energizing coil 23.
The connection lines 21 are connected, through plugs (not illustrated), to the sensing coils 22a, 22b and enable electrical connection thereof to a supply/control circuitry (not shown), for example, integrated in the epitaxial layer 16. Similar connection lines (not shown) may enable connection of the energizing coil 2 to the respective supply/control circuitry.
The magnetic region 13 is made of a ferromagnetic material having the following characteristics:
In particular, if the magnetic region 13 is made of NiFe (permalloy), it has a saturation magnetization Bsat of 1 T and a relative permeability of approximately 3,500 at 500 MHz. Alternatively, NiFeMo or other appropriately developed dedicated magnetic alloys can be used.
A passivation layer 25 extends on the magnetic region 13.
In practice, the presence of the Hall sensor 12 underneath the fluxgate sensor 11 enables exploitation of the magnetic region 13 for measuring magnetic fields having an intensity greater than the upper limit of the range of sensitivity of the fluxgate sensor 11, extending the sensitivity of the resulting magnetometer.
In fact, as is known, operation of the Hall-effect cells 12 is based upon detection of the Hall voltage between pairs of conductive regions extending in a direction transverse to the conductive regions 19, as a result of the interaction between a current flowing between the conductive regions 19 themselves and an external magnetic field, orthogonal to the current and, in the case considered, to the surface of the body 14. The magnetic region 13 acts here as concentrator and has the purpose of modifying the lines of magnetic flux of an external magnetic field parallel or co-planar to the surface of the body 14 so that the lines of flux traverse vertically the Hall-effect cells 12 arranged underneath the ends of the magnetic region 13, in addition to providing amplification. In this way, a magnetic field parallel or co-planar to the surface of the body 14 becomes detectable by the Hall-effect cells 12, as is, for example, described in Christian Shott et al., “A CMOS Single-Chip Electronic Compass with Microcontroller”, 2007 IEEE International Solid-State Circuit Conference, ISSCC 2007/SESSION 21/SENSORS AND MEMS/21.2.
The magnetic sensor 10 of
Initially (
Then (
Next (
Then (
Next (
The magnetic material is deposited via sputtering so as to obtain a typical thickness around 1-5 μm. The sputtering technique (see, for example, Andrea Baschirotto et al., “An integrated microFluxgate sensor with sputtered ferromagnetic core”, IMTC 06), enables provision of amorphous thin films with the indicated thickness so as to require a lower power consumption in order to saturate as compared to thicker layers deposited with other techniques (for example, by electroplating).
Finally, the deposited ferromagnetic layer is defined so as to have the cross shape, and the passivation layer 25 is deposited so as to cover the magnetic region 13, in order to obtain the structure of
The sensor described herein has numerous advantages. In fact, it represents a device capable of operating on the set of ranges of sensitivity of a fluxgate sensor and of a Hall sensor with magnetic concentrator, greatly extending the possible applications of the resulting magnetometer.
The magnetic sensor 10 can be integrated alone or be integrated in the same chip with the respective supply/control circuitries.
The magnetometer 40 has a multiplicity of possible applications. For example, it can be used as current meter, as is shown in
The magnetometer 40 can also be used as electronic compass, for example, in a cellphone or other electronic apparatus having navigation functions. In this case, as is shown in
Further possible applications comprise, among other things, apparatuses for detecting physiological parameters (heartbeat, cerebral waves, blood pressure, etc.), position detectors (whether linear or rotary, for example, for knobs, cursors, joysticks and the like, or mobile members, such as pistons, etc.), level indicators, and so on.
Finally, it is clear that modifications and variations can be made to the magnetic sensor and to the corresponding manufacturing process, described and illustrated herein, without thereby departing from the scope of the present invention, as defined in the annexed claims. For example, even though
Having thus described at least one illustrative embodiment of the invention, various alterations, modifications, and improvements will readily occur to those skilled in the art. Such alterations, modifications, and improvements are intended to be within the spirit and scope of the invention. Accordingly, the foregoing description is by way of example only and is not intended as limiting. The invention is limited only as defined in the following claims and the equivalents thereto.
Number | Date | Country | Kind |
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TO2008A000897 | Dec 2008 | IT | national |