This application is a U.S. national stage application of the PCT International Application No. PCT/JP2015/006064 filed on Dec. 7, 2015, which claims the benefit of foreign priority of Japanese patent application No. 2015-030475 filed on Feb. 19, 2015, the contents all of which are incorporated herein by reference.
The present invention relates to small and thin common mode noise filters employed in a range of electronic devices, such as digital equipment, audio-visual equipment, and information communication terminals.
The mobile industry processor interface (mipi) D-PHY standard has been adopted as a digital data transmission standard for connecting a main IC with display or camera in mobile equipment. The standard employs a system of transmitting differential signals via two transmission lines. Upon recent significant increase of camera resolutions, the mipi C-PHY standard is established and put in practical use as a transmission system with a higher speed, using three transmission lines. Different voltages are sent from a transmitter to transmission lines, and the receiver takes a difference among the lines for differential output.
For example, PTL1 discloses a conventional common mode noise filter similar to common mode noise filter 500.
PTL1: Japanese Patent Laid-Open Publication No. 2003-77727
A common mode noise filter includes non-magnetic layers stacked in a laminating direction, and first, second, and third coil conductors constituting independent first, second, and third coils, respectively, on the non-magnetic layers. The first and third coil conductors deviate from the second coil conductor in a direction perpendicular to the laminating direction.
This common mode noise filter can improve a balance among magnetic coupling between the first coil and the third coil, magnetic coupling between the first coil and the second coil, and magnetic coupling between the second coil and the third coil.
Before describing exemplary embodiments, a disadvantage of conventional common mode noise filter 500 shown in
In conventional common mode noise filter 500, coil 3 is disposed between coil 2 and coil 4. Therefore, coil 2 is far from coil 4, and thus magnetic coupling between coil 2 and coil 4 is hardly established.
If common mode noise filter 500 is applied to aforementioned three-wire differential signal line to transmit differential data signals, coil 2 and coil 4 that are not magnetically coupled to each other cannot cancel magnetic flux generated. Large residual inductance generated by a component not magnetically coupled produces a loss in the differential data signal. This greatly degrades the quality of differential signals.
However, in common mode noise filter 501, coil 3 is provided between coil 2 and coil 4, and a distance between coils 2 and 4 is long. Therefore, magnetic coupling is smaller than the other parts. This results in poor balance of magnetic coupling between the coils.
When a differential signal is input to common mode noise filter 501, the differential signal has less degradation in coil 3 since it has preferable magnetic coupling with adjacent coil 2 and coil 4. However, even in common mode noise filter 501, a distance between coil conductor 2b and coil conductor 4b and a distance between coil conductor 4a and coil conductor 2a are long and thus their magnetic coupling is weak. Accordingly, the differential signal flowing in coil 2 and coil 4 degrades, similarly to common mode noise filter 500.
Common mode noise filters in accordance with exemplary embodiments that can improve the balance among magnetic coupling between two coils far from each other, magnetic coupling between other two coils, and magnetic coupling between still other two coils will be described below with reference to drawings.
Exemplary Embodiment 1
As shown in
Non-magnetic layers 11a to 11g are stacked in laminating direction 1001a in this order from below. Non-magnetic layers 11a to 11g are made of sheets made of insulating non-magnetic material, such as Cu-Zn ferrite and glass ceramic, with thicknesses Ts identical to each other.
Coil conductors 12a, 12b, 13a, 13b, 14a, and 14b form three coils 12, 13, and 14 independent from each other. More specifically, coil 12 includes coil conductor 12a and coil conductor 12b, coil 13 includes coil conductor 13a and coil conductor 13b, and coil 14 includes coil conductor 14a and coil conductor 14b.
Each of these coil conductors is provided on the upper surface of the non-magnetic layer by plating or printing a conductive material, such as silver, in a spiral shape.
The shapes of the coil conductors will be described below. As shown in
In accordance with Embodiment 1, the width of the conductor, pitches of the conductors, and the thickness of the conductor in the main portion which is a spiral portion between the outer circumference and the inner circumference other than a portion of the conductor used for wiring are the same in coil conductors 12a, 12b, 13a, 13b, 14a, and 14b.
Coil conductor 12a is formed on upper surface 111a of non-magnetic layer 11a. Coil conductor 13a is formed on upper surface 111b of non-magnetic layer 11b. Coil conductor 14a is formed on upper surface 111c of non-magnetic layer 11c. Coil conductor 12b is formed on upper surface 111d of non-magnetic layer 11d. Coil conductor 13b is formed on upper surface 111e of non-magnetic layer 11e. Coil conductor 14b is formed on upper surface 111f of non-magnetic layer 11f. Non-magnetic layers 11a to 11e and coil conductors 12a, 12b, 13a, 13b, 14a, and 14b form laminate part 15 such that upper surface 111a of non-magnetic layer 11a is disposed on lower surface 211b of non-magnetic layer 11b, upper surface 111b of non-magnetic layer 11b is disposed on lower surface 211c of non-magnetic layer 11c, upper surface 111c of non-magnetic layer 11c is disposed on lower surface 211d of non-magnetic layer 11d, upper surface 111d of non-magnetic layer 11d is disposed on lower surface 211e of non-magnetic layer 11e, upper surface 111e of non-magnetic layer 11e is disposed on lower surface 211f of non-magnetic layer 11f, and upper surface 111f of non-magnetic layer 11f is disposed on lower surface 211g of non-magnetic layer 11g.
In other words, coil conductor 12a constituting coil 12, coil conductor 13a constituting coil 13, coil conductor 14a constituting coil 14, coil conductor 12b constituting coil 12, coil conductor 13b constituting coil 13, and coil conductor 14b constituting coil 14 are disposed in this order from below.
In laminate part 15, coil conductor 12a and coil conductor 12b constituting coil 12 are electrically connected with three via-electrodes 16a each provided in respective one of non-magnetic layers 11b to 11d. Coil conductor 13a and coil conductor 13b constituting coil 13 are electrically connected with three via-electrodes 16b each provided in respective one of non-magnetic layers 11c to 11e. Coil conductor 14a and coil conductor 14b constituting coil 14 are electrically connected with three via-electrodes 16c each provided in respective one of non-magnetic layers 11d to 11f.
Coil conductor 13a constituting coil 13 and coil conductor 14a constituting coil 14 are provided between coil conductor 12a and coil conductor 12b constituting coil 12. Coil conductor 14a constituting coil 14 and coil conductor 12b constituting coil 12 are provided between coil conductor 13a and coil conductor 13b constituting coil 13. Coil conductor 12b constituting coil 12 and coil conductor 13b constituting coil 13 are provided between coil conductor 14a and coil conductor 14b constituting coil 14.
In other words, between two coil conductors constituting one coil out of coils 12 to 14, total two coil conductors each of which is one of two coil conductors constituting respective one of the coils out of coils 12 to 14 other than the one coil are provided.
This structure provides three coils 12, 13, and 14 independent from each other. Coil 12 and coil 13 are magnetically coupled to each other, coil 13 and coil 14 are magnetically coupled to each other, and coil 14 and coil 12 are magnetically coupled to each other.
In common mode noise filter 1001 in accordance with Embodiment 1, coil conductors 12a, 14a, and 13b formed on non-magnetic layers 11a, 11c, and 11e at odd-numbered orders out of non-magnetic layers 11a to 11f sequentially stacked in laminating direction 1001a deviate from coil conductors 13a, 12b, and 14b provided on non-magnetic layers 11b, 11d, and 11f at even-numbered orders out of non-magnetic layers 11a to 11f in direction Ds perpendicular to laminating direction 1001a of laminate part 15. More specifically, coil conductors adjacent to each other deviate from each other in direction Ds perpendicular to laminating direction 1001a. In other words, winding axes of coil conductors adjacent to each other deviate from each other in direction Ds perpendicular to laminating direction 1001a in accordance with Embodiment 1.
In accordance with Embodiment 1, as shown in
Coil conductors 12a, 14a, and 13b are disposed such that main parts thereof having the spiral shapes overlap coil conductors 13a, 12b, and 14b viewing in laminating direction 1001a.
This configuration enables magnetic coupling to be adjusted by adjusting a distance between coil conductors adjacent to each other. Hence, magnetic coupling between coil 12 and coil 13 and magnetic coupling between coil 13 and coil 14 can be weakened to balance with magnetic coupling between coil 12 and coil 14. Direction Ds is not necessarily the above diagonal direction in the rectangular shape, and may be another direction perpendicular to laminating direction 1001a, providing the substantially same effects.
Coil conductor 14a and coil conductor 12b are arranged to overlap in a top view, i.e., viewing in laminating direction 1001a, thereby weakening magnetic coupling between coil 12 and coil 13 that include more pairs of coil conductors adjacent to each other and magnetic coupling of coil 13 and coil 14 that have more pair of coil conductors adjacent to each other to enhance magnetic coupling between coil 12 and coil 14 that include fewer pairs of coil conductors adjacent to each other. Accordingly, magnetic coupling can be balanced among three coils 12, 13, and 14. In this case, other coil conductors deviate in direction Ds perpendicular to laminating direction 1001a from a coil conductor adjacent to these coil conductors.
In common mode noise filter 1001 in accordance with Embodiment 1 in which each coil is composed of two coil conductors connected to each other, coil 12 and coil 13 are adjacent to each other at two parts while coil 13 and coil 14 are adjacent to each other at two parts. On the other hand, coil 12 and coil 14 are adjacent to each other only at one part. This configuration more weakens magnetic coupling between coil 12 and coil 13 that have more parts adjacent to each other and magnetic coupling between coil 13 and 14 that have more parts adjacent to each other. Accordingly, the magnetic couplings are balanced among coils 12, 13, and 14.
A coil composed of three or more coil conductors connected to each other can provide the same effects.
Even if a coil is composed of a single coil conductor, magnetic coupling between coil conductors adjacent to each other and magnetic coupling between other coil conductors adjacent to each other can be weakened to balance magnetic coupling with coil conductors away from each other.
The deviating of the coil conductors provided on non-magnetic layers at odd-numbered orders from the coil conductors provided on non-magnetic layers at even-numbered orders in direction Ds perpendicular to laminating direction 1001a of laminate part 15 means that a cross section of a portion of the coil conductor at the same order of turn of winding from the inner circumference to outer circumference of the coil conductor deviates in direction Ds perpendicular to laminating direction 1001a viewing from the cross section parallel to laminating direction 1001a.
The deviating of the cross section of each coil conductor is the deviating of a reference point set to each coil conductor. The reference point is a point in the same direction on the coil conductors. For example, in the case that the coil conductor has a rectangular cross section, the reference point on the coil conductor may be set to the center of the rectangle where diagonal lines of the rectangle cross or a corner of the rectangle. In the case that the coil conductor has an oblong or flat semicircular cross section, the reference point may be set to the center of the width and the thickness.
In accordance with Embodiment 1, deviating amount Ss that is a length by which coil conductors provided on non-magnetic layers at odd-numbered orders deviate from the coil conductors provided on non-magnetic layers at even-numbered order in direction Ds perpendicular to laminating direction 1001a of laminate part 15 and thickness Ts of the non-magnetic layers preferably satisfy 0<Ss≤2.0×Ts.
Deviating amount Ss even slightly more than 0 (zero) provides the aforementioned effect of weakening magnetic coupling to obtain the effect of balancing magnetic coupling among the coils.
As deviating amount Ss increases from 0 (zero), the balance of magnetic coupling among the coils further improve. However, if deviating amount Ss more than twice thickness Ts of the non-magnetic layers unpreferably weakens overall magnetic coupling between coil conductors.
Deviating amount Ss preferably satisfies 1.6×Ts≤Ss≤1.8×Ts.
This configuration can increase the number of turns of coils and thus, increases impedance of the coils when common mode noise enters thereto, thus improving the common mode noise elimination capability.
In the above structure, as shown in
The number of non-magnetic layer 11a to 11g and magnetic layer 17 is not limited to that indicated in
Laminate body 18 has the above structure. External electrodes are provided on both end surfaces of laminate body 18, and are connected to ends of coil conductors 12a, 12b, 13a, 13b, 14a, and 14b, respectively.
In accordance with the exemplary embodiment, the inner circumference and the outer circumference of each coil conductor has substantially a rectangular shape, and the coil conductors deviate in diagonal direction Ds of the rectangular shape. The common mode noise filter in accordance with Embodiment 1 may have coil conductors deviate in either a long side direction or a short side direction of the rectangular shape. This configuration can preferably balance magnetic coupling among the coil conductors.
The shape of the main portion of each coil conductor is not necessarily a rectangular shape. The shapes of the inner circumference and outer circumference of the main portion may be a circular, oblong, or oval shape. This configuration can also balance magnetic coupling among the coil conductors.
Furthermore, coil conductors 12a and 12b shown in
Exemplary Embodiment 2
Common mode noise filter 2001 in accordance with Embodiment 2 does not include non-magnetic layers 11g and 11f of common mode noise filters 1001 and 1002 in accordance with Embodiment 1. As shown in
Coil conductors 13a and 14a which constitute two coils 13 and 14 and which are positioned on the same plane (upper surface 111b) deviate from coil conductor 12a constituting other coil 12 in direction Ds perpendicular to laminating direction 1001a of laminate part 15. Coil conductors 13b and 14b which constitute two coils 13 and 14 and which are positioned on the same plane (upper surface 111d) deviate from coil conductor 12b constituting other coil 12 in direction Ds perpendicular to laminating direction 1001a of laminate part 15.
A coil conductor on the same plane as coil conductors 13a and 13b constituting coil 13 may be coil conductors 12a and 12b constituting coil 12.
This structure can reduce the thickness of entire laminate part 15.
The line connecting coil conductor 12a and coil conductor 13a, the line connecting coil conductor 13a and coil conductor 14a, and the line connecting coil conductor 12a and coil conductor 14a in a cross section of laminate part 15 in laminating direction 1001a in portions of the coil conductors at the same order of turn from the inner circumference forms an equilateral triangle, and thereby, locate the coil conductors away from each other by the same distance. This configuration can preferably balance magnetic coupling among the coil conductors. Still more, since a distance between coil conductor 13a and coil conductor 14a is adjusted to easily adjust distances among coil conductor 13a, coil conductor 14a and coil conductor 12a just by adjusting the thickness of non-magnetic layer 11b, so that mutual magnetic coupling among coils 12, 13, and 14 can be enhanced. Still more, since a distance between coil conductor 13b and coil conductor 14b is adjusted to easily adjust distances among coil conductor 13b, coil conductor 14b, and coil conductor 12b just by adjusting the thickness of non-magnetic layer 11d, so that mutual magnetic coupling of coils 12, 13, and 14 can be enhanced. Furthermore, since a distance between coil conductor 13b and coil conductor 14b is adjusted to easily adjust distances among coil conductor 13b, coil conductor 14b, and coil conductor 12b just by adjusting the thickness of non-magnetic layer 11d, so that mutual magnetic coupling of coils 12, 13, and 14 can be enhanced.
In addition to balanced magnetic coupling, it is also important to balance capacitances among the coils since characteristic impedance in a differential mode depends on capacitances in transmission of differential signals. To adjust this capacitances, non-magnetic layer 11e and non-magnetic layer 11d may have different dielectric constants.
Exemplary Embodiment 3
As shown in
As shown in
In
As shown in
In common mode noise filter 1001 in accordance with Embodiment 1, in the case that the portion of coil conductor 13b at the N-th turn from the inner circumference overlaps portions of coil conductors 12b and 14b at the (N−1)-th turn from the inner circumference viewing from above, i.e., viewing in laminating direction 1001a, undesired stray capacitance increases between the portion of coil conductor 13b at the N-th turn from the inner circumference and the portions of coil conductors 12b and 14b at the (N−1) turn. When a differential signal is input, the differential signal may degrade in a high-frequency range that tends to be affected by stray capacitance.
In common mode noise filter 3001 in accordance with Embodiment 3, the portion of coil conductor at the N-th turn does not overlap the portion of the coil conductor at the (N−1)-th turn viewing from above, i.e., viewing in laminating direction 1001a. Accordingly, undesired stray capacitance is reduced, thus reducing degradation of differential signals.
As shown in
In a three-wire differential signal line, undesired stray capacity between coil conductor 13b and portions of coil conductors 12b and 14b in the adjacent order of turn increases if distances Da and Db between a portion of coil conductors 12b and 14b at the N-th turn a portions of coil conductors 12b and 14b at the N-th turn are not longer than distances DLa, DLb, and DLc in the portion of coil conductor in the N-th turn and the portion of coil conductor in the (N−1) turn shown in
On the other hand, in common mode noise filter 3001 in accordance with Embodiment 3, distances Da and Db are longer than distances DLa, DLb, and DLc so that undesired stray capacitance between a portion of coil conductor 13b at a certain order of turn and each of portions of coil conductors 12b and 14b at an order of turn adjacent to the certain order of turn of coil conductor 13b can be further reduced.
Since two portions of coil conductor 13b have the same potential, no large undesired stray capacitance is generated between these portions. Still more, the above two portions of coil conductor 13b are positioned between portions of each of coil conductors 12b and 14b at the orders of turn adjacent to each other. This configuration provides a long distance between a portion of coil conductor 13b at a certain order of turn and each of portions of coil conductors 12b and 4b at an order of turn adjacent to the certain order of turn. This configuration reduces undesired stray capacitance between the above portion of coil conductor 13b and each of the portions of coil conductors 12b and 14b. Similarly, an undesired stray capacitance between each of two portions of coil conductor 12b and each of two portions of coil conductor 14b can be reduced by arranging a portion of the coil conductors at the (N−2)-th turn, as shown in
Still more, as shown in
Positions of coil conductors 12b, 13b, and 14b of coils 12, 13, and 14 are explained above. Other coil conductors 12a, 13a, and 14a or coils 12, 13, and 14 can be disposed similarly to coil conductors 12b, 13b, and 14b, respectively.
This configuration reduces undesired stray capacitance between a portion of coil conductor 13b at a certain order of turn and each of portions of coil conductors 12b and 14b at an order of turn adjacent to the certain order so as to prevent degradation of differential signals. At the same time, more number of windings increases impedance and improves noise elimination performance when a common mode noise is input.
Exemplary Embodiment 4
In common mode noise filter 4001 in accordance with Embodiment 4, as shown in
Distance T1 between coil conductor 12b and coil conductor 13b (thickness of non-magnetic layer 110 in laminating direction 1001a is longer than distance T2 between coil conductor 13b and coil conductor 14b (thickness of non-magnetic layer 11e) in laminating direction 1001a in order to form an equilateral triangle with line La connecting coil conductor 12b constituting coil 12 to coil conductor 13b constituting coil 13, line Lb connecting coil conductor 13b constituting coil 13 to coil conductor 14b constituting coil 14, and line Lc connecting coil conductor 12b constituting coil 12 to coil conductor 14b constituting coil 14. This structure balances magnetic coupling among coils.
If the thickness of the coil conductor is smaller than the line width thereof, capacitance between portions of coil conductor 12b and coil conductor 14b facing and overlapping each other viewing from above becomes larger than a capacitance between coil conductor 12b and coil conductor 13b or a capacitance between coil conductor 14b and coil conductor 13b with a small opposing area in common mode noise filter 3001 in accordance with Embodiment 3. In common mode noise filter 4001 in accordance with Embodiment 4, the capacitances among the coil conductors can be balanced since coil conductor 12b, coil conductor 14b, and coil conductor 13b do not overlap one another viewing from above, hence preventing degradation of differential signals.
In
Exemplary Embodiment 5
In common mode noise filter 5001 in accordance with Embodiment 5, as shown in
If the thickness of non-magnetic layer has a lower limit in view of production basis, a residual inductance is generated without completely cancelling magnetic flux generated in coil conductors 12b and 14b due to reduced electrostatic capacitance and slightly weakened magnetic coupling between coil conductors 12b and 14b facing each other. Accordingly, characteristic impedance in the differential mode increases when the differential signal flows between opposing coil conductors 12b and 14b. This may generate a reflection loss of differential signals and degrade differential signals. To reduce characteristic impedance in the differential mode, a capacitance between coil conductors 12b and 14b facing each other is adjusted to be slightly larger and line widths of coil conductors 12b and 14b be broader to increase the capacitance. This obtains consistency of characteristic impedance in the differential mode. Accordingly, signal degradation can be prevented.
Still more, as shown in
In
In the structure shown in
As described above, non-magnetic layers 11a to 11f and coils 12, 13, and 14 constitute laminate part 15a and laminate part 15b placed on laminate part 15a in laminating direction 1001a. Laminate part 15a includes coil conductors 12a to 14a and non-magnetic layers 11a to 11d out of non-magnetic layers 11a to 11f. Laminate part 15b includes coil conductors 12b to 14b and non-magnetic layers 11d to 11d in non-magnetic layers 11a to 11f. A distance between coil conductor 12a out of coil conductors 12a to 14a which is closest to laminate part 15b and coil conductor 12b out of coil conductors 12b to 14b which is closest to laminate part 15a is longer than a distance between coil conductors 12a and 13a, a distance between coil conductors 13a and 14a, a distance between coil conductors 12a and 14a, a distance between coil conductors 12b and 13b, a distance between coil conductors 13b and 14b, and a distance between coil conductors 12b and 14b.
Furthermore, coil conductors 12a to 14a and 12b to 14b are disposed in the order of coil conductor 14a, coil conductor 13a, coil conductor 12a, coil conductor 12b, coil conductor 13b, and coil conductor 14b in laminating direction 1001a.
In the embodiments, terms, such as “upper surface” and “lower surface”, indicating directions indicate relative positions determined only by relative positional relationship of components, such as non-magnetic layers and coil conductors, of the common mode noise filter, and do not indicate absolute directions, such as a vertical direction.
A common mode noise filter according to the present invention can be employed in three-wire differential lines. Balanced magnetic coupling can be achieved among three coils, quality of differential signals can be maintained, and common mode noise can be eliminated. In particular, it is effectively applicable to small and thin common mode noise filters used typically in digital equipment, AV equipment, and information communication terminals.
Number | Date | Country | Kind |
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2015-030475 | Feb 2015 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2015/006064 | 12/7/2015 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2016/132410 | 8/25/2016 | WO | A |
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