This invention relates to the field of inductors which are used in integrated circuits. In particular, this invention relates to symmetric inductors particularly adequate for use in circuits using differential signals. The inductors winding preferably have either a spiral or a spiral-like planar configuration.
Patents relating to inductors abound in the prior art. However, most such patents refer to standard, asymmetric spiral inductors, and disclose various methods of improving characteristics of these spiral inductors, such as increasing Q=Ws/Wd (where Ws is the energy stored and Wd is the energy dissipated in the inductor per cycle) or reducing the size of the inductors. Examples of inductor patents are U.S. Pat. No. 3,765,082 relating to a method of making an inductor chip, U.S. Pat. No. 5,656,849 relating to a two-level spiral inductor structure having a high inductance to area ratio, U.S. Pat. No. 5,805,043 relating to a high Q compact inductors for monolithic integrated circuit applications, U.S. Pat. No. 5,793,272 relating to an integrated circuit toroidal inductor, U.S. Pat. No. 5,884,990 relating to an integrated circuit inductor, U.S. Pat. No. 6,008,713 relating to a monolithic inductor, U.S. Pat. No. 6,054,329 relating to a method of forming an integrated circuit spiral inductor with ferromagnetic liner, and U.S. Pat. No. 6,013,939 relating to a monolithic inductor with magnetic flux lines guided away from substrate.
Planar spiral inductors have been used for integrated circuits since the early 1970's. Such spiral inductors have been designed with an intrinsic asymmetry since one terminal of the inductor is at the outside of the spiral, while the other terminal is on the inside. This asymmetry usually does not have any substantial effects on circuits using single-ended signals, i.e., where the signal voltage is relative to ground or a fixed potential. However, many new circuits and systems use differential signals where the signal voltage is the difference between two terminals. Any asymmetry in circuits using differential signals (differential circuits) has the effect of degrading the signal quality, and is thus very undesirable.
The present invention addresses the above-noted problems encountered in the prior art. In particular, the present invention addresses signal degradation due to inductor asymmetry and conductor cross-over capacitive effects, by providing a symmetric spiral inductor and a method of making such spiral inductor.
In one aspect, the present invention relates to a inductor which is substantially symmetric and thus does not exhibit signal degradations due to asymmetry of the inductor. The symmetric inductor comprises concentric windings of different sizes or effective diameters, and winding crossovers which are disposed in such a way that the symmetry of the inductor is preserved. In this way, capacitive effects caused by conductor crossovers, are substantially minimized. The indictor is preferably of a spiral or spiral-like configuration and is preferably disposed on a planar substrate.
In another aspect, the present invention relates to a method of winding an inductor as concentric circles, rectangles, squares or other generally symmetric shapes, rather than a true spiral. The magnetic field coupling and inductive coupling needed for enhanced inductance is maintained, while providing a substantially symmetric structure. Furthermore, conductor crossovers can be symmetrically placed, preserving the symmetry of the structure and minimizing undesirable capacitive coupling.
Referring to
The path taken by the electrical current within the inductor winding 25 illustrates the fashion in which the windings 22 and 23 are formed and how the inductor may be fabricated. Starting at terminal 1 and traveling clockwise, the electrical current may travel through the left half 22L of the outer winding 22 and reaches conductor crossover 24 again. The conductor crossover 24 conductively connects the left half 22L of the outer winding 22 to right half 23R the inner winding 23. After crossing over, the current continues to travel clockwise through the right half 23R of inner winding 23, and then the left half 23L of the inner winding 23 to reach crossover 24. After crossing under, the current continues to travel clockwise through the right half 22R of outer winding 22, to finally reach terminal 2. Obviously, the electrical current may also travel counter clockwise within the inductor winding 25, by entering the inductor at terminal 2 and exiting at terminal 1. The foregoing description of the path taken by the electrical current is for the purpose of illustrating how the windings of the inductor are disposed, in accordance with one embodiment of the present invention.
To facilitate understanding of the configuration of the inductor winding 25, only two windings 22 and 23 are shown in
In the example of
The use of concentric circular windings affords the inductor a symmetrical configuration, eliminating signal degradation due to inductor asymmetry. In order for the center of one winding to substantially coincide with the center of other windings, the location of the centers of each winding are preferably controlled to +/−0.05 μm or better. Further, conductor crossovers are preferably disposed to best preserve the symmetry of the inductor. As shown in
Turning to
Again, the path taken by the electrical current within the inductor winding 31 illustrates the fashion in which windings 32, 33, 34, 35, and 36 are formed and how the inductor may be fabricated. Starting at terminal 1 and traveling clockwise, the electrical current may travel through the left half of winding 32, to then cross over at conductor crossover 38, to the right half of winding 33. After crossing over at cross over 39 to the left half of winding 34, the current continues on to cross over 40. After crossing over, the current travels through the right half of winding 35 to cross over 41 where is crosses over to the innermost winding 36. The current then travels through winding 36 back to crossover 41 where it crosses under to the left half of winding 35. It then crosses under at crossover 40 to travel through the right half of winding 34, to then cross under at crossover 39 to the left side of winding 33. After crossing under at crossover 38, the current travels through the right side of winding 32 to finally reach terminal 2.
The use of square windings which share a common center, affords the inductor a symmetrical configuration, eliminating signal degradation due to inductor asymmetry. In order for the center of one winding to substantially coincide with the center of other windings, the location of the centers of each winding are preferably controlled to +/−0.05 μm or better. Further, conductor crossovers are preferably disposed to best preserve the symmetry of the inductor. As shown in
When a conductor crosses over another conductor at the crossovers, the two conductors are insulated from each other. In the foregoing description one conductor is described as passing “over” the other conductor which is described as passing “under.” However, so long as the two conductors are insulated from one another, either one can pass “over” or “under” the other conductor at the crossovers.
Although described in the case of circular and square windings, any concentric arrangement of arbitrarily symmetric shapes may be used. Such other shapes may include, but are not limited to, hexagons, rectangles, ellipses, etc. In order to for the center of one winding to substantially coincide with the center of other windings, the location of the centers of each winding are preferably controlled to +/0.05 μm or better.
A typical number of windings included in the inductor of the present invention may be between 2 and 5 and the corresponding inductance may range between about 1 and 8 nH. However, as would be apparent to the skilled person, any number of concentric windings may be used to obtain the desired value of inductance.
The spacing between two adjacent windings preferably ranges from about 5 μm to about 15 μm. However, other spacings may also be adequate as would be apparent to the skilled person. The spacing between confronting edges of adjacent windings, excluding the crossover points, are preferably constant and should not vary by more than +/0.4 μm, thereby causing the windings to be generally symmetric one to another.
Inductors in accordance with the present invention, are particularly adequate for use in circuits using differential signals, such as oscillators, mixers and amplifiers. However, they can be used in any circuit where inductors are needed. Inductors in accordance with the present invention may be manufactured as part of an integrated circuit. One skilled in the art will appreciate that there are many techniques used to manufacture inductors as a part of integrated circuits. The inductors shown in
Any material with suitably low RF loss can be used as the substrate. InP and GaAs are preferable when the inductor is integrated with circuitry. When the inductor is not integrated with circuitry, then alumina or any number of ceramic or glass substrates can be used without loss of performance.
One skilled in the art will appreciate that the inductors of the present invention may be manufactured by any semiconductor process which allows the patterning of two layers of metal. Therefore, the present invention is independent of the semiconductor process used.
A typical equivalent circuit 50 for a planar spiral inductor is shown in
In the electromagnetic simulation, the material used for the windings of the inductor was Au, but any other conductive materials may be used as well. The insulating material was a polyimide with a thickness of approximately 2 μm. However, silicon dioxide, silicon nitride, or any other insulating film would be acceptable proved that it can be realized with similar dimension of thickness. The thickness of the insulator was chosen to minimize the crossover capacitance and make the inductor more idea. Making the thickness of the dielectric thicker up to a point where it is as think as the width of the windings is advantageous. However, practical considerations typically limit the thickness to approximately four micrometers.
Having described the invention in connection with certain embodiments thereof, modifications will certainly suggest themselves to those skilled in the art. As such, the invention is not to be limited to the disclosed embodiments except as required by the appended claims.
This application claims the benefit of U.S. Patent Provisional Patent Application Ser. No. 60/412,283 filed Sep. 20, 2002, the disclosure of which is hereby incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| 60412283 | Sep 2002 | US |