This application claims the priority benefit of Italian Application for Patent No. 102016000098500, filed on Sep. 30, 2016, the disclosure of which is hereby incorporated by reference in its entirety.
The present invention relates to an electronic component including a micro-transformer with magnetic field confinement and to a method for manufacturing said electronic component.
Integrated transformers, of micrometric dimensions, are widely used in a wide range of fields of application, such as galvanic insulation, transfer of signals, and transfer of energy. For instance, in the field of galvanic insulation, integrated transformers are fundamental components in many modern electronic products that require exchange of data between two insulated electrical domains, for example, medical devices, controllers of motors, and communication devices. Commercially available systems typically use a plurality of coupling methods, which include inductive coupling based upon planar transformers, with a diameter of the windings of less than 1 mm. The reasons for these choices are multiple and include, for example, protection from voltages and currents.
A further field of application regards power conversion. Power converters are important components of battery-supplied portable electronic devices, and microtransformers are fundamental components thereof.
The miniaturization and integration of microtransformers is frequently in contrast with the high performance required by the aforementioned applications, and the development of high-performance, highly miniaturized, and integrated microtransformers today represents a challenge. The integration of high-quality magnetic cores using an effective manufacturing process represents a gap in the prior art. In fact, on account of the complexity of processing and definition of the materials that could be used, the choice of the magnetic materials employed in practice for the formation of the magnetic core is limited by the deposition processes available, such as sputtering or electroplating. However, these deposition processes may be used for depositing materials with limited thicknesses and homogeneity. Materials typically deposited with these methods include Ni—Fe. Other possibilities of fabrication regard the casting of ferrite or the assembly of magnetic ribbons (the latter being a non-integrated solution).
The inventors have detected the presence of a further problem of microtransformers according to the known art as regards their operation at frequencies of the order of megahertz or higher, i.e., at frequencies such that the magnetic losses become dominant on account of the parasitic currents (also known as “eddy currents” or “Foucault currents”). It has been found that, for high-frequency applications, it is likewise important to minimize the parasitic currents, for example, by making the magnetic core of a high-resistivity material and exploiting at the same time high-resistance substrates. There coexist the opposed needs of minimizing the effects of saturation by providing a sufficiently thick core, but at the same time of minimizing the thickness of the core to reduce costs.
Furthermore, to reduce the effects of parasitic currents in the substrate, the inventors have found, as has been said, that it is convenient to use substrates of highly resistive silicon. However, this type of substrate is not the substrate typically used in BCD (Bipolar-CMOS-DMOS) technology, which is a technology that integrates three different technologies: bipolar technology for precise analog functions; CMOS (Complementary Metal Oxide Semiconductor) technology for digital circuits; and DMOS (Double-Diffused Metal Oxide Semiconductor) technology for power and high-voltage components.
In an embodiment, a micro-integrated transformer is provided that will overcome the drawbacks mentioned above, and in particular that will enable reduction of the losses caused by the parasitic currents in the silicon substrate and, in general, increase of the efficiency of transfer by improving the magnetic coupling between the windings of the microtransformer. A method for manufacturing the micro-integrated transformer is also provided.
The present disclosure finds use in micro-integrated transformers in semiconductor structures or components which in particular include a substrate (e.g., a silicon substrate) over which one or more dielectric layers extend. The dielectric layers may house, in a per se known manner, metal layers (e.g., for routing of signals) and the mutually facing windings of the micro-transformer. According to one aspect of the present disclosure, a first layer of magnetic material is integrated between the silicon substrate and a bottom winding of the microtransformer, for providing a protective barrier or shield for the substrate from the magnetic field generated in use by the windings of the microtransformer. In other words, said shielding layer operates as element for confinement of the magnetic field generated in use by the bottom winding. A second layer of magnetic material extends over the microtransformer, above the top winding of the latter. Thus, the microtransformer (more precisely, the windings of the microtransformer) extends between the first and second layers of magnetic material.
According to further embodiments of the present disclosure, just one of the first and second layers of magnetic material may be present. The presence of the first or second layer of magnetic material, or of both of them, forms a low-reluctance path for the magnetic field generated by the respective windings and enables increase of the efficiency of transfer between the primary winding and the secondary winding, improving the magnetic coupling between them.
More in particular, the first layer of magnetic material concentrates the magnetic field generated by the windings of the microtransformer and limits the parasitic currents in the overlying silicon substrate, thus increasing the efficiency of the microtransformer. Both for the first layer and for the second layer of magnetic material, the increase in efficiency of the microtransformer is represented by the use and presence, in the path of the magnetic field lines, of a magnetic material with low reluctance if compared to air or silicon oxide, or to other non-magnetic materials.
However, since the loss due to parasitic currents also afflicts the first and second layers of magnetic material, according to a further aspect of the present disclosure, the layers of magnetic material include a plurality of magnetic sub-layers and insulating sub-layers alternating with one another in a laminated structure. The thickness of each of the magnetic layers of the laminated structure is chosen to be substantially equal to the skin depth δ of each of them. This embodiment enables interruption of the path of the currents in the respective layer of magnetic material.
According to a different embodiment, the first layer and/or second layer of magnetic material, having a thickness greater than the skin depth δ, may be sectioned in the direction of the thickness to form slices, which have a dimension (in this case, the width) equal to or less than the skin depth δ, separated from one another by dielectric layers. Also this embodiment enables interruption of the path of the currents in the respective layer of magnetic material.
For a better understanding of the invention, some embodiments thereof will now be described, purely by way of non-limiting example and with reference to the attached drawings, wherein:
The system of
In use, the transmitter TX receives an input signal (to be transmitted) from a control circuitry, and supplies the input signal to a primary winding 2b. The receiver RX is coupled for receiving from the secondary winding 2a a signal corresponding to the input signal supplied to the primary winding 2b, and generates an output signal comprising a reconstituted input signal.
With reference to
The transformer 2 includes a bottom winding 2a (in this example, the secondary winding) and a top winding 2b (in this example, the primary winding), here represented purely by way of example as each having four turns designated by the references 21 and 23, respectively.
It is, however, evident that the number of turns may be other than four, and chosen as required, for example, in a number comprised between two and thirty. The bottom winding 2a and top winding 2b extend at a distance from one another along the axis Z, separated by one or more layers of dielectric material (e.g., silicon oxide) that forms a galvanic-insulation region 13.
An electrical-contact region 3, of metal material (e.g., copper), extends at the same metal level as the top winding 2b, inside the turns 23 thereof and is electrically coupled to the turns of the top winding 2b. The electrical-contact region 3 is likewise electrically coupled to a bonding wire 9 by a bonding region 10.
The microtransformer 2 functions as galvanic-insulation module and as interface for transfer of power between the transmitter TX, which is external to the device 1, and the receiver RX, which is integrated in a semiconductor body (substrate) 6 of the device 1, or vice versa.
The receiver RX includes, in a per se known manner and on the basis of the signal that it has to receive, electronic components/circuits designated as a whole by the references 4 and 5, which function, for example, at voltages in the range between 1 V and 40 V. The receiver RX is operatively coupled to the bottom winding 2a, to acquire from the bottom winding 2a the signal transmitted by the transmitter TX. The electrical components and/or circuits 4 may be located in the region overlying the microtransformer 2, as illustrated in
The semiconductor body 6 (for example, including silicon) is, in particular, obtained in BCD (Bipolar-CMOS-DMOS) technology, which is a technology that integrates three different technologies: bipolar technology for precise analog functions; CMOS (Complementary Metal Oxide Semiconductor) technology for digital circuits; and DMOS (Double-Diffused Metal Oxide Semiconductor) technology for power and high-voltage components.
Extending over the semiconductor body 6 are one or more metal levels. In the embodiment of
According to an aspect of the present disclosure, in the dielectric region that extends between the bottom winding 2a and the substrate 6 electronic circuits and components may be formed, at least in part. In this case, said region comprised between the bottom winding 2a and the substrate 6 is an active-area region of the device 1.
According to a different embodiment, the dielectric region that extends between the bottom winding 2a and the substrate 6 does not comprise electronic components or circuits. In this case, the microtransformer 2 is formed alongside the active-area region of the device 1.
Extending between the third metal level M3 and the fourth metal level M4 is the galvanic-insulation layer 13, in the form of thick dielectric layer, having a thickness, along the Z axis, comprised between 1 μm and 30 μm, for example, 10 μm. The galvanic-insulation layer 13 is the layer that separates the bottom winding 2a from the top winding 2b of the transformer 2, and its thickness is chosen according to the voltage class required for galvanic insulation and such as to guarantee that class.
The metal region 14d of the fourth metal level M4 is exposed at a front side 1a of the device 1 (to form an external electrical contact pad). For this purpose, the metal region 14d is electrically coupled to a bonding wire 16 by a bonding region 19. The bonding wire 16 and the bonding region 19 are of conductive metal material, for example, gold.
Each metal level M2-M4 is electrically coupled to the bottom metal level M1-M3 by via levels L2-L4. A further via level L1 extends underneath the first metal level M1 to form an electrical contact towards the semiconductor body 6. The via levels L1-L4 include conductive through vias 17a-17d. The conductive vias 17a-17d are, for example, of metal material, such as tungsten or copper. Dielectric layers 20a-20c, made for example, of silicon oxide, extend between one metal level M1-M3 and the next, and between the first metal level M1 and the semiconductor body 6, as well as alongside each metal region belonging to a same metal level M1-M4.
The semiconductor body 6 may integrate a wide range of electrical and electronic components/circuits 5, which have specific functions that are not described in detail herein in so far as they do not form a subject of the present disclosure. Irrespective of the functions of said electronic circuits 5, conduction terminals thereof are electrically coupled with the outside of the device 1 via the metal regions 14a-14d and the conductive vias 17a-17c, for transmission/reception of electrical control signals thereof.
One or more insulation and passivation layers 24, 26 extend on the front side of the device 1. Furthermore, a resin layer 30 (for example, a layer of epoxy resin) covers the device 1 and forms part of the package (not illustrated in its entirety) of the device 1.
According to one aspect of the present disclosure, the device 1 further includes a first layer of magnetic material and a second layer of magnetic material (which are defined hereinafter also as “confinement layers”) 27, 28, designed to confine the magnetic field generated in use by the bottom winding 2a and the top winding 2b of the transformer 2.
The first and second confinement layers 27, 28 include, as has been said, magnetic material, in particular of an electrically conductive type, for example, an alloy including cobalt.
The first confinement layer 27 extends underneath the bottom winding 2a and is substantially arranged, in the view along the Z axis, underlying the bottom winding 2a. More in particular, the first confinement layer 27 extends within the via level L3, embedded in a layer of dielectric material. In one embodiment, the distance d1, along the Z axis, between the first confinement layer 27 and the bottom winding 2a is comprised between 600 nm and 800 nm. The thickness t1 of the first confinement layer 27, measured along the Z axis, is chosen so that, as a function the power of the signal to be transferred, there do not occur phenomena of saturation of the first confinement layer 27, thus enabling the transformer to work in linear regime. For instance, the thickness t1 of the first confinement layer 27 is comprised between 200 nm and 1000 nm.
The second confinement layer 28 extends over the top winding 2b, and substantially arranged, in the view along the Z axis, overlying the top winding 2b. More in particular, the second confinement layer 28 extends over the fourth metal level M4 and is separated from the latter by a dielectric layer. Dielectric material likewise forms the layer 24 that covers the second confinement layer 28. In one embodiment, the distance d2, along the Z axis, between the second confinement layer 28 and the top winding 2b is comprised between 600 nm and 800 nm. In general, this distance is chosen so that the excitation current, which flows in the winding 2b, will not generate a field such as to saturate the magnetic material having a thickness t2. The thickness t2 of the second confinement layer 28, measured along the Z axis, is chosen taking into consideration both the value of the excitation current of the winding 2b and the distance d2, so that the resulting magnetic field may concatenate therewith, without saturating it, and thus keep the transformer operating in linear regime.
In top plan view, i.e., viewing the plane XY in the direction of the Z axis, the second confinement layer 28, the top winding 2b, the bottom winding 2a, and the first confinement layer 27 are arranged on top of one another, i.e., substantially aligned with each other along the Z axis.
The extension along the X axis of the first and second confinement layers 27, 28 is equal to or greater than the extension, along the X axis, of the top and bottom windings 2b, 2a. In particular, in top plan view, the first and second confinement layers 27, 28 have a circular shape with a diameter greater than the respective diameter of the top and bottom windings 2b, 2a (the latter, for example, being of a circular, quadrangular, or generically polygonal shape).
In one embodiment, at least the second confinement layer 28 has a central opening that bestows a doughnut shape thereon. Said central hole enables access to the electrical-contact region 3 by the bonding wire 9. It is evident that the conductive connection between the electrical-contact region 3 and the bonding region 10 may be obtained in some other way, so that the central opening of the second confinement layer 28 is not necessary. Furthermore, the inventors have found that the central region of the first and second confinement layers 27, 28 does not make a significant contribution in terms of improvement of the transfer efficiency of the integrated transformer (in fact, in this region the field lines are coming out). For this reason, removal of the magnetic material for formation of the central opening has no impact on the aforementioned advantages. Instead, since in some particular situations said central region could be biased in an undesired way, its removal is, in specific operating conditions, advantageous.
As mentioned previously, since the presence of parasitic currents (eddy currents or Foucault currents) also afflicts the first and second confinement layers 27, 28, according to a further aspect of the present disclosure both the first confinement layer 27 and the second confinement layer 28 have a stacked structure, or laminated structure, (e.g., the stack 29 of
With reference to
The skin-depth parameter 6 is given by the following formula:
where ρ is the electrical resistivity of each of the magnetic layers of the stack, w is the angular frequency (2πf) of the field (e.g., RF field) generated in use by the windings traversed by alternating current, and μ is the magnetic permeability of the magnetic material of each of the magnetic layers of the stack. For instance, in the range of frequencies f of interest (3 MHz-500 MHz), the skin depth δ is comprised between 1000 nm and 80 nm considering a magnetic material having values of ρ=140 Ωcm and μ=μ0μr, where μ0 is the magnetic permeability of vacuum and μr is the relative permeability of the magnetic material, for example, of the order of 105.
Illustrated in greater detail in lateral sectional view in
As an alternative to what is illustrated in
In general, the cuts 31″ delimit wafers of magnetic material which have a width equal to or less than δ and generate an electrical discontinuity that acts against the circulation of the parasitic currents in the layers of magnetic material.
The laminated structure 29 of
The embodiments of
Illustrated in
With reference to
The first confinement layer 27 is then coated with a layer of dielectric material, for example, silicon oxide.
Then (
Next (
There is then deposited a layer of dielectric material on top of the metal region 14c and of the bottom winding 2a, as well as between the turns 21 of the bottom winding 2a, thus completing formation of the third metal level M3. More in particular, as illustrated in
Then (
Then (
Then (
Next (
Finally, a step of pouring of a resin, for example, epoxy resin, enables formation of the resin layer 30, to obtain the device 1 of
Finally, it is evident that modifications and variations may be made to the present disclosure, without departing from the scope of the invention, as defined in the annexed claims.
In the embodiments of
Number | Date | Country | Kind |
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102016000098500 | Sep 2016 | IT | national |