Circular Polarizer Using Stepped Conductive and Dielectric Fins In An Annular Waveguide

NOTICE OF COPYRIGHTS AND TRADE DRESS

A portion of the disclosure of this patent document contains material which is subject to copyright protection. This patent document may show and/or describe matter which is or may become trade dress of the owner. The copyright and trade dress owner has no objection to the facsimile reproduction by anyone of the patent disclosure as it appears in the Patent and Trademark Office patent files or records, but otherwise reserves all copyright and trade dress rights whatsoever.

BACKGROUND

1. Field

This disclosure relates to linear polarization to circular polarization converters for use in coaxial waveguides.

2. Description of the Related Art

Satellite broadcasting and communications systems commonly use separate frequency bands for the uplink to and downlink from satellites. Additionally, one or both of the uplink and downlink typically transmit orthogonal right-hand and left-hand circularly polarized signals within the respective frequency band.

Typical antennas for transmitting and receiving signals from satellites consist of a parabolic dish reflector and a coaxial feed where the high frequency band signals travel through a central circular waveguide and the low frequency band signals travel through an annular waveguide coaxial with the high-band waveguide. An ortho-mode transducer (OMT) may be used to launch or extract orthogonal TE₁₁linear polarized modes into the high- and low-band coaxial waveguides. TE (transverse electric) modes have an electric field orthogonal to the longitudinal axis of the waveguide. Two orthogonal TE₁₁modes do not interact or cross-couple, and can therefore be used to communicate different information. A linear polarization to circular polarization converter is commonly disposed within each of the high- and low-band coaxial waveguides to convert the orthogonal TE₁₁modes into left- and right-hand circular polarized modes for communication with the satellite.

Converting linearly polarized TE₁₁modes into circularly polarized modes requires splitting each TE₁₁mode into two orthogonally polarized portions and then shifting the phase of one portion by 90 degrees with respect to the other portion. This may conventionally be done by inserting two or more dielectric vanes, oriented at 45 degrees to the polarization planes of the TE₁₁modes, into the waveguide as described in U.S. Pat. No. 6,417,742 B1. However, assembling the dielectric vanes at the precise angle within the waveguide can be problematic. Errors in assembling the dielectric vanes can result in imperfect polarization conversion and cross-talk between the two orthogonally polarized TE₁₁modes.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A is an end view of a coaxial waveguide including a linear polarization to circular polarization converter.

FIG. 1B is a side view of a coaxial waveguide including a linear polarization to circular polarization converter.

FIG. 2 is a longitudinal cross section of the coaxial waveguide of FIG. 1A.

FIG. 3A is a first axial cross section of the coaxial waveguide of FIG. 1B.

FIG. 3B is a second axial cross section of the coaxial waveguide of FIG. 1B.

FIG. 4A is a first axial cross section of another linear polarization to circular polarization converter.

FIG. 4B is a second axial cross section of the linear polarization to circular polarization converter of FIG. 4A.

FIG. 5 is a longitudinal cross section of a coaxial waveguide.

FIG. 6 is a perspective view of a stepped polarizer element.

FIG. 7 is a perspective view of a stepped polarizer element.

FIG. 8 is a perspective view of another stepped polarizer element.

FIG. 9 is a perspective view of another stepped polarizer element.

FIG. 10 is a graph showing the simulated performance of a linear polarization to circular polarization converter using the stepped polarizer element of FIG. 9.

Throughout this description, elements appearing in figures are assigned three-digit reference designators, where the most significant digit is the figure number where the element was first introduced and the two least significant digits are specific to the element. An element that is not described in conjunction with a figure may be presumed to have the same characteristics and function as a previously-described element having the same reference designator.

DETAILED DESCRIPTION

Description of Apparatus

FIG. 1A is an end view of a linear polarization to circular polarization converter 100, and FIG. 1B is a side view of the linear polarization to circular polarization converter 100. As shown in FIG. 1A, the linear polarization to circular polarization converter 100 may include an outer conductor 110 and an inner conductor 120. The inner conductor 120 may have an outer surface 122 that has a generally circular cross section except for two diametrically opposed fins 130 extending outward from the outer surface 122. The outer conductor 110 may have an inner surface 114 that is generally coaxial with the outer surface 122 of the inner conductor 120. In this description, the terms generally circular and generally coaxial mean circular and coaxial within the limits of reasonable manufacturing tolerances. The space between the inner surface 114 of the outer conductor 110 and the outer surface 122 of the inner conductor 120 may define an annular waveguide 140.

The inner conductor 120 may be generally in the form of a tube having an inner surface 124 with a generally circular cross section. The inner surface 124 may define a circular waveguide 150.

The outer conductor 110 may have an outer surface 112 that may be generally circular in cross section, as shown in FIG. 1A, or may be another shape. For example, the outer surface 112 may have a square cross section for ease of manufacturing and/or mounting.

FIG. 2 shows a cross section of the linear polarization to circular polarization converter 100 along a plane A-A as identified in FIG. 1A. The linear polarization to circular polarization converter 100 may include an outer conductor 110 having an outer surface 112 and an inner surface 114. The linear polarization to circular polarization converter 100 may also include an inner conductor 120 having an outer surface 122 and an inner surface 124. Two diametrically opposed fins 130 may extend from the outer surface 122 of the inner conductor 120.

The diametrically opposed fins 130 may include a conductive fin 132a/132b/132c and a dielectric fin 134. Each conductive fin 132a/132b/132c may be stepped in a longitudinal direction. Each conductive fin may include a central portion 132a flanked by symmetrical side portions 132b and 132c. The central portion 132a may extend a first distance d1 from the outer surface 122. The side portions 132b and 132c may extend a second distance d2 from the outer surface 122, where the second distance d2 is less than the first distance d1. Each dielectric fin 134 may extend at least a third distance d3 from the outer surface 122, where d3 is greater than d1. The distance that each dielectric fin 134 extends from the outer surface 122 may be stepped. Each dielectric fin may include a central portion that extends a fourth distance d4 from the outer surface 122, where d4 is greater than d3.

As shown in the detail at the lower left of FIG. 2, the conductive fin may include a step 133 between the side portion 132c and the central portion 132a. A similar step may exist between the central portion 132a and the side portion 132b. The dielectric fin may include a complementary step 135. The interface between the step 135 in the dielectric fin 134 and the step 133 in the conductive fin may act to position and constrain the dielectric fin 134 in the longitudinal direction.

FIG. 3A and FIG. 3B show cross sections of the linear polarization to circular polarization converter 100 along plane B-B and plane C-C, respectively, as identified in FIG. 1B and FIG. 2. Each dielectric fin 134 may be formed with a longitudinal (perpendicular to the plane of the drawings) notch that may engage the respective conductive fin portions 132a and 132b as shown in FIGS. 3A and 3B, respectively. The notch in each dielectric fin 134 may be conformal or nearly conformal to the conductive fin portions 132a and 132b such that the conductive fin portions 132a and 132b align and constrain the respective dielectric fin 134 in the transverse direction.

The conductive fin portions 132a, 132b, 132c (FIG. 2) may align and constrain the position of the respective dielectric fin 134 both longitudinally and transversely such that each dielectric fin 134 is interlocked with the corresponding conductive fin portions 132a, 132b, 132c. In this description, “interlocked” has the normal meaning of “connected in such a way that the motion of any part is constrained by another part”. Within the linear polarization to circular polarization converter 100, the position of each dielectric fin 134 may be aligned and constrained by the corresponding conductive fin portions 132a, 132b, 132c.

The inner conductor 120 may be fabricated from aluminum or copper or another highly conductive metal or metal alloy. The conductive fin portions 132a, 132b, 132c may be integral to the inner conductor. The conductive fin portions 132a, 132b, 132c may be fabricated by numerically controlled machining and thus may be precisely located on the outer surface 122 of the inner conductor 120. The dielectric fins 134 may be fabricated from a low-loss polystyrene plastic material such as REXOLITE® (available from C-LEC Plastics) or another dielectric material suitable for use at the frequency of operation of the linear polarization to circular polarization converter 100.

Referring to FIG. 3A, the conductive fin portions 132a, 132b (FIG. 3B) and the dielectric fins 134 may be symmetrical about a symmetry plane 136 passing through the axis of the inner conductor 120. In use, the symmetry plane 136 may be oriented at a 45 degree angle to the polarization planes 142 and 144 of two linearly polarized TE modes traveling in the annular waveguide 140.

FIG. 4A and FIG. 4B show cross sections of another linear polarization to circular polarization converter 400 along plane B′-B′ and plane C′-C′, respectively, which may be the same as planes B-B and C-C identified in FIG. 1B and FIG. 2.

The linear polarization to circular polarization converter 400 may include an inner conductor 420 having an outer surface 422. A pair of diametrically opposed conductive fins 462a/462b, shown in FIG. 4A and FIG. 4B respectively, may extend outward from the outer surface 422. A pair of dielectric fins 464a/464b, shown in FIG. 4A and FIG. 4B respectively, may be interlocked with the respective conductive fins. The dielectric fins 464a/464b may have a “T”-shaped cross-section. The legs of the “T”-shaped dielectric fins 464a/464b may fit within mating longitudinal slots in the corresponding conductive fins 462a/462b. The conductive fins 462a/462b may align and constrain dielectric fins 464a/464b as previously described.

The linear polarization to circular polarization converter 400 may include an inner conductor 420 having an outer surface 422. The outer surface 422 may have a cross-sectional shape of a hexagon, as shown, an octagon, or another regular polygon with an even number of sides. An outer surface having a circular cross section, such as the outer surface 112 in FIG. 1, may be fabricated by turning on a lathe. However, the presence of conductive fins 132a/132b/132c or 462a/462b precludes the use of a lathe, and the outer surface 122, 422 of the inner conductor 120, 420 may be fabricated by numerically controlled milling. The polygonal cross-section of the outer surface 422 may be less costly to machine than the circular cross-section of the outer surface 122.

The “T”-shaped dielectric fins 464a/464b and corresponding conductive fins 462a/462b of FIG. 4A and FIG. 4B, respectively, and the dielectric fins 134 (FIG. 2) and corresponding conductive fins 132a/132b of FIG. 3A and FIG. 3B, respectively, are examples of dielectric fins that are mechanically interlocked with conductive fins. The dielectric fins and the conductive fins may incorporate other combinations of tabs, slots, pins, holes, or any other mechanisms that allow the conductive fins to support and align the dielectric.

Other combinations of dielectric and conductive fins may be used with an inner conductor having an outer surface with either a circular cross-section or polygonal cross-section. For example, the “T”-shaped dielectric fins 464a/464b and corresponding conductive fins 462a/462b of FIG. 4A and FIG. 4B, respectively, may be used with an inner conductor having an outer surface with a circular cross section. Conversely, the dielectric fins 134 and corresponding conductive fins 132a/132b of FIG. 3A and FIG. 3B, respectively, may be combined with an inner conductor having an outer surface with a polygonal cross-section.

Structures, such as the previously-described dielectric and conductive fins, within an annular waveguide may cause undesired resonances within the operating bandwidth of a polarization converter within a feed network or other waveguide system. For example, resonances may occur due to excitation of higher order modes that then resonate within the annular waveguide. In this patent, the term “higher order” has the conventional meaning of any mode having an order higher than the desired propagating modes of the waveguide. For this application, the desired propagating modes in the annular waveguide are orthogonal TE₁₁or HE₁₁(if dielectric is present within the waveguide) modes. A resonating higher order mode may result in objectionable variations in the performance of the polarization converter as a function of frequency. To prevent the resonance of higher order modes, the conductive and/or dielectric fins may be configured to suppress propagation of one or more higher order modes in the annular waveguide.

FIG. 5 shows a cross section of waveguide device 500. The waveguide device 500 may include an outer conductor 510 having an outer surface 512 and an inner surface 514. The waveguide device 500 may also include an inner conductor 520 having an outer surface 522. An annular waveguide 570 may be defined by the outer surface 522 of the inner conductor 520 and the inner surface 514 of the outer conductor. The inner conductor 520 may be solid, or may have an inner surface 524 that defines a circular cylindrical waveguide 575 concentric with the annular waveguide 570.

The annular waveguide 570 may be divided into a plurality of regions along a direction of propagation. The plurality of regions may include normal waveguide regions 572a, 572b and an alternating sequence of high phase shift regions 574a, 574b, 574c and low phase shift regions 576a, 576b. In this context, a “phase shift region” is a portion of the annular waveguide in which the phase of a first mode is shifted with respect to the phase of a second mode orthogonal to the first mode. The terms “high” and “low” are relative. A “high phase shift region” provides more phase shift per unit propagation length than is provided by a “low phase shift region”. A low phase shift region may provide little or no phase shift. The high phase shift and low phase shift regions may be configured such that the cumulative phase shift introduced to the first mode after propagating the length of the annular waveguide 570 is 90 degrees, 180 degrees, or some other predetermined phase shift.

In the example of FIG. 5, the annular waveguide 570 includes three high phase shift regions 574a, 574b, 574c and two low phase shift regions 576a, 576b. An annular waveguide may have two or more high phase shift regions separated by low phase shift regions such that the number of low phase shift regions is one less than or one more than the number of high phase shift regions. The high phase shift regions are not necessarily identical in structure or length. When two or more low phase shift regions are present, the low phase shift regions are also not necessarily identical in structure or length.

The normal waveguide regions 572a, 572b may be configured to allow propagation of two orthogonal TE₁₁modes within a predetermined operating frequency band. In order to provide sufficient phase shift within a reasonable length device, it may be necessary to allow the high phase shift regions 574a, 574b, 574c to support propagation of one or more higher order modes within the operating frequency band. The supported higher order modes may include, for example, a TE₂₁mode and/or some other higher order mode. The low phase shift regions 576a, 576b may be configured to suppress propagation of the higher order modes supported by the high phase shift regions. The low phase shift regions 576a, 576b may be configured to allow propagation of only two orthogonal TE₁₁or HE₁₁modes within the operating frequency band. The high phase shift regions and the low phase shift regions may be collectively configured to prevent resonance of any higher order mode within the annular waveguide 570 over the operating frequency band.

The alternating sequence of high phase shift regions 574a, 574b, 574c and low phase shift regions 576a, 576b may be created by loading structures (not shown) within the annular waveguide 570. In this patent, a “loading structure” is any structure or material that changes the shape and/or impedance of the annular waveguide. The loading structures may be or include, for example, metal and/or dielectric fins extending from the outer surface 522 of the inner conductor 520, metal and/or dielectric fins extending from the inner surface 514 of the outer conductor 510, dielectric cards or blocks disposed within the annular waveguide 570, or any other structure adapted to shift the phase of the first mode with respect to the phase of the second mode.

The loading structures may be further configured to form transitions 578 between adjacent normal waveguide regions and high phase shift regions. Transitions 578 may also be formed between adjacent high phase shift and low phase shift regions. Transitions may provide, for example, impedance matching between adjacent regions of the annular waveguide. While FIG. 5 shows, for ease of illustration, abrupt boundaries between the transitions 578 and the adjacent regions of the annular waveguide 570, actual transitions may constitute a gradual change from one waveguide region to the next.

A waveguide device, such as waveguide device 500, may be designed by using a commercial software package such as CST Microwave Studio. An initial model of the device may be generated with estimated dimensions for the waveguide, conductive fins and dielectric fins. The structure may then be analyzed, and the reflection coefficients and the relative phase shift for two orthogonal linearly polarized modes may be determined. The dimensions of the model may then be iterated manually or automatically to minimize reflection coefficients and to set the relative phase shift at or near a desired value, such as 90 degrees, across the operating frequency band.

To ensure that an undesired higher order mode does not resonate within the waveguide device 500, the Transverse Resonance Method may be employed. To employ this method, a model of the waveguide device 500 is split at a plane orthogonal to the axis and passing through the center of one of the high phase shift region 574a, 574b, or 574c. The undesired higher order mode may be excited at this split. The reflection phase for the higher order mode propagating to the left of the split may be calculated. Similarly, the reflection phase for the higher order mode propagating to the right of the split may be calculated. If the sum of the reflection phase for the higher order mode propagating to the left and the reflection phase for the higher order mode propagating to the right of the split are about zero or 360 degrees, the higher order mode may resonate within the feed network. If the sum of the reflection phases for the higher order modes propagating to the left and to the right of the split do not add up to zero or 360 degrees (+/−about 10 degrees) for all wavelengths within the operating frequency band, the higher order mode will not resonate within the waveguide device 500.

FIG. 6 is a perspective view of an exemplary polarization converter 600 for use within an annular waveguide. The polarization converter 600 may include an inner conductor 620 having an outer surface 622. In use, the inner conductor 620 would typically be enclosed by an outer conductor (not shown) to form the annular waveguide. The outer surface 622 may have a cross-sectional shape of an octagon, as shown, a hexagon, or another regular polygon with an even number of sides. The outer surface 622 may have a circular cross section, similar to the outer surface 112 in FIG. 1. The cross section of the outer surface 622 may be a combination of circular segments and flat portions. The inner conductor 620 may be solid, as shown, or may be pierced by a cylindrical bore forming a circular waveguide coaxial with the annular waveguide. The presence or absence of the circular waveguide may not affect the operation of the polarization converter.

First and second diametrically-opposed fins 630 (only one of which is fully visible in FIG. 6) may extend from the inner conductor 620 into the annular waveguide. Each fin 630 may include a metal fin 632a-632e interlocked with a dielectric fin 634a-634e. The metal fins and dielectric fins may interlock using one or more of steps, tabs, slots, pins, notches, and holes as previously described. The metal fin may be divided into a plurality of sections 632a, 632b, 632c, 632d, 632e, each of which steps in height h and/or width w from adjacent metal fin sections. The dielectric fin may be divided into a plurality of sections 634a, 634b, 634c, 634d, 634e, each of which steps in at least width w from adjacent dielectric fin sections.

The fins 630 may function as loading structures to define a plurality of regions along a direction of propagation of electromagnetic waves within the annular waveguide. The fins 630 may define a first high phase shift region 674a and a second high phase shift region 674b separated by a low phase shift region 676. The fins 630 may define a first transition 678a and a second transition 678b adjacent to the high phase shift regions 674a, 674b, respectively. The transitions 678a, 678b may provide impedance matching between an annular waveguide without fins and the respective high phase shift regions 674a, 674b. The transitions 678a, 678b may introduce some phase shift and may be considered as additional low phase shift regions.

Specifically, the first transition 678a may correspond to the portion of the annular waveguide containing metal fin sections 632a, 632b and dielectric fin section 634a. The first high phase shift region 674a may correspond to dielectric fin section 634b in combination with metal fin section 632c. The low phase shift region 676 may correspond to dielectric fin section 634c in combination with metal fin section 632c. The second high phase shift region 674b may correspond to dielectric fin section 634d in combination with metal fin section 632c. In general, high phase shift regions may correspond to portions of the metal fins and/or dielectric fins having relatively larger height h and/or width w, and low phase shift regions may correspond to portions of the metal fins and/or dielectric fins having smaller height h and/or width w. The second transition 678b may correspond to the portion of the annular waveguide containing metal fin sections 632d, 632e and dielectric fin section 634e.

The fins 630 may be configured to provide, in combination, a desired phase shift, such as 90 degrees or 180 degrees, between two orthogonal electromagnetic waves propagating in the annular waveguide. The transition regions 678a, 678b, the high phase shift regions 674a, 674b, and the low phase shift region 676 may also be configured to act as a filter to suppress one or more undesired higher order modes from propagating or resonating in the annular waveguide. The low phase shift region 676 may be configured to allow propagation of orthogonal HE₁₁modes over a predetermined operating bandwidth while suppressing, or cutting off, one or more higher order modes, such as an HE₂₁mode, over the same operating bandwidth. For example, the fins 630 may be configured such that the HE₂₁mode or some other higher order mode can propagate in the high phase shift regions 674a, 674b but is cut off in the low phase shift region 676. The low phase shift region 676 may be configured to allow propagation of only orthogonal HE₁₁modes over the predetermined operating bandwidth.

FIG. 7 is a perspective view of another exemplary polarization converter 700 for use within an annular waveguide. The polarization converter 700 may include an inner conductor 720 having an outer surface 722. In use, the inner conductor 720 would typically be enclosed by an outer conductor (not shown) to form the annular waveguide. The outer surface 722 may have a cross-sectional shape of an octagon, as shown, a hexagon, or another regular polygon with an even number of sides. The outer surface 722 may have a circular cross section, similar to the outer surface 112 in FIG. 1. The cross section of the outer surface 722 may be a combination of circular and flat segments. The inner conductor 720 may be solid, as shown, or may be pierced by a cylindrical bore forming a circular waveguide coaxial with the annular waveguide. The presence or absence of the circular waveguide may not affect the operation of the polarization converter.

First and second diametrically opposed fins (only one of which is fully visible in FIG. 7) may extend from the outer surface 722. Each of the first and second fins may include a plurality of collinear finlets 730-1, 730-2, 730-3, 730-4. In this application, “finlet” is a coined term meaning a small fin that forms a portion of a greater fin. Each finlet may include a metal fin 732-1, 732-2, 732-3, 732-4 interlocked with a respective dielectric fin 734-1, 734-2, 734-3, 734-4. The metal fins and dielectric fins may interlock using one or more of steps, tabs, slots, pins, notches, and holes as previously described. In the example of FIG. 7, each of the first and second fins includes four finlets 730-1 to 730-4. A polarization converter may have more or fewer that four pairs of finlets.

Each metal fin 732-1 to 732-4 may be divided into a plurality of sections, each of which differs in height h and/or width w from adjacent metal fin sections. In the example of FIG. 4, each metal fin is divided into five sections. Each dielectric fin 734-1 to 734-4 may be divided into a plurality of sections, each of which differs in at least width w from adjacent dielectric fin sections. In the example of FIG. 7, each dielectric fin is divided into three sections. Fins may have more or fewer sections than shown in FIG. 7.

The finlets 730-1 to 730-4 may define a plurality of regions along a direction of propagation of electromagnetic waves within the annular waveguide. Each finlet 730-1 to 730-4 may define a high phase shift region sandwiched by two transitions. The transitions may provide impedance matching between the respective high phase shift regions and an annular waveguide without fins. The transitions may also contribute to the total phase shift provided by the polarization converter. The spaces between finlets 730-1 to 730-4 may define low phase shift regions. There may be no phase shift introduced over at least a portion of each low phase shift region.

The finlets 730-1 to 730-4 may be configured to provide, in combination, a desired phase shift, such as 90 degrees or 180 degrees, between two orthogonal electromagnetic waves propagating in the annular waveguide. The finlets 730-1 to 730-4 and the spaces between the finlets may also be configured to act as a filter to suppress one or more undesired higher order modes from propagating or resonating in the annular waveguide. The waveguide regions between the finlets may allow propagation of orthogonal TE₁₁modes over a predetermined operating bandwidth while suppressing, or cutting off, one or more higher order modes over the same operating bandwidth. The waveguide regions between the fins may be configured to allow propagation of only orthogonal TE₁₁modes over the predetermined operating bandwidth.

FIG. 8 is a perspective view of another exemplary polarization converter 800 for use within an annular waveguide. The polarization converter 800 may include an inner conductor 820 having an outer surface 822. In use, the inner conductor 820 would typically be enclosed by an outer conductor (not shown) to form the annular waveguide. The outer surface 822 may have a cross-sectional shape of an octagon, as shown, a hexagon, or another regular polygon with an even number of sides. The outer surface 822 may have a circular cross section, similar to the outer surface 112 in FIG. 1. The cross section of the outer surface 822 may be a combination of circular and flat segments. The inner conductor 820 may be solid, as shown, or may be pierced by a cylindrical bore forming a circular waveguide coaxial with the annular waveguide. The presence or absence of the circular waveguide may not affect the operation of the polarization converter.

First and second diametrically opposed fins (only one of which is visible in FIG. 8) may extend from the outer surface 822. Each of the first and second fins may include a plurality of collinear finlets 830-1, 830-2. Each finlet may include a metal fin 832a/832b/832c, 832d/832e/832f interlocked with a respective dielectric fin 834a/834b/834c, 834d/834e/834f. The metal fins and dielectric fins may interlock using one or more of steps, tabs, slots, pins, notches, and holes as previously described. In the example of FIG. 8, each of the first and second fins includes two finlets 830-1, 830-2. A polarization converter may have more or fewer that two pairs of finlets.

Each metal fin may be divided into a plurality of sections 832a-832f, each of which differs in width w from adjacent metal fin sections. The height h of the metal fin section 832a-832f may be equal. In the example of FIG. 8, each metal fin is divided into three sections. Each dielectric fin may be divided into a plurality of sections 834a-834f, each of which differs in at least width w from adjacent dielectric fin sections. The height h of the dielectric fin section 834a-834f may be equal. In the example of FIG. 8, each dielectric fin is divided into three sections. Fins may have more or fewer sections than shown in FIG. 8.

The finlets 830-1, 830-2 may define a plurality of regions along a direction of propagation of electromagnetic waves within the annular waveguide. Each finlet 830-1, 830-2 may define a high phase shift region sandwiched by two transitions. The transitions may provide impedance matching between the respective high phase shift regions and an annular waveguide without fins. The transitions may contribute to the total phase shift introduced by the finlets. The spaces between finlets 830-1, 830-2 may define a low phase shift region. There may be no phase shift introduced over at least a portion of the low phase shift region.

The finlets 830-1, 830-2 may be configured to provide, in combination, a desired phase shift, such as 90 degrees or 180 degrees, between two orthogonal electromagnetic waves propagating in the annular waveguide. The finlets 830-1, 830-2 and the space between the finlets may also be configured to act as a filter to suppress one or more undesired higher order modes from propagating or resonating in the annular waveguide. The low phase shift region between the finlets 830-1, 830-2 may allow propagation of orthogonal TE₁₁modes over a predetermined operating bandwidth while suppressing, or cutting off, one or more higher order modes over the same operating bandwidth. The low phase shift region between the finlets 830-1, 830-2 may be configured to allow propagation of only orthogonal TE₁₁modes over the predetermined operating bandwidth.

FIG. 9 is a perspective view of another exemplary polarization converter 900 for use within an annular waveguide. The polarization converter 900 may include an inner conductor 920 having an outer surface 922. In use, the inner conductor 920 would typically be enclosed by an outer conductor (not shown) to form the annular waveguide. The outer surface 922 may have a cross-sectional shape of an octagon, as shown, a hexagon, or another regular polygon with an even number of sides. The outer surface 922 may have a circular cross section, similar to the outer surface 112 in FIG. 1. The cross section of the outer surface 922 may be a combination of circular and flat segments. The inner conductor 920 may be solid, as shown, or may be pierced by a cylindrical bore forming a circular waveguide coaxial with the annular waveguide. The presence or absence of the circular waveguide may not affect the operation of the polarization converter.

First and second diametrically opposed fins (only one of which is fully visible in FIG. 9) may extend from the outer surface 922. Each of the first and second fins may include a plurality of collinear finlets 930-1, 930-2, 930-3. Each finlet may include a metal fin 932-1, 932-2, 932-3, interlocked with a respective dielectric fin 934-1, 934-2, 934-3. The metal fins and dielectric fins may interlock using one or more of steps, tabs, slots, pins, notches, and holes as previously described.

Each metal fin 932-1 to 932-3 may be divided into a plurality of sections, each of which differs in height and/or width from adjacent metal fin sections. In the example of FIG. 9, each metal fin is divided into three sections. Each dielectric fin 934-1 to 934-3 may be divided into a plurality of sections, each of which differs in at least width from adjacent dielectric fin sections. In the example of FIG. 9, each dielectric fin is divided into three sections.

The finlets 930-1 to 930-3 may be configured to provide, in combination, a phase shift of approximately 90 degrees between two orthogonal electromagnetic waves propagating in the annular waveguide. The finlets 930-1 to 930-3 and the spaces between the finlets may also be configured to act as a filter to suppress one or more undesired higher order modes from propagating or resonating in the annular waveguide.

FIG. 10 is a graph 1000 illustrating the simulated performance of a linear to circular polarization converter including a stepped polarizer element similar to the polarization converter 900 within an annular waveguide. The performance of the linear to circular polarization converter was simulated using finite integral time domain analysis. The time-domain simulation results were Fourier transformed into frequency-domain data as shown in FIG. 10. The solid line 1010 and the dashed line 1020 plot the return loss introduced by the linear to circular polarization converter in two orthogonal linearly polarized TE₁₁modes. The return loss is less than 19 dB over a frequency band from 19.4 GHz to 21.2 GHz. The stepped polarizer element provides a phase shift of approximately 90 degrees over the frequency band without any resonance of higher order modes.

Closing Comments

Throughout this description, the embodiments and examples shown should be considered as exemplars, rather than limitations on the apparatus and procedures disclosed or claimed. Although many of the examples presented herein involve specific combinations of apparatus elements, it should be understood that those acts and those elements may be combined in other ways to accomplish the same objectives. Elements and features discussed only in connection with one embodiment are not intended to be excluded from a similar role in other embodiments.

For means-plus-function limitations recited in the claims, the means are not intended to be limited to the means disclosed herein for performing the recited function, but are intended to cover in scope any means, known now or later developed, for performing the recited function.

As used herein, “plurality” means two or more.

As used herein, a “set” of items may include one or more of such items.

As used herein, whether in the written description or the claims, the terms “comprising”, “including”, “carrying”, “having”, “containing”, “involving”, and the like are to be understood to be open-ended, i.e., to mean including but not limited to. Only the transitional phrases “consisting of” and “consisting essentially of”, respectively, are closed or semi-closed transitional phrases with respect to claims.

Use of ordinal terms such as “first”, “second”, “third”, etc., in the claims to modify a claim element does not by itself connote any priority, precedence, or order of one claim element over another or the temporal order in which acts of a method are performed, but are used merely as labels to distinguish one claim element having a certain name from another element having a same name (but for use of the ordinal term) to distinguish the claim elements.

As used herein, “and/or” means that the listed items are alternatives, but the alternatives also include any combination of the listed items.

	Number	Date	Country
Parent	12058560	Mar 2008	US
Child	12685134		US

	Number	Date	Country
Parent	12685134	Jan 2010	US
Child	13220964		US

Circular Polarizer Using Stepped Conductive and Dielectric Fins In An Annular Waveguide

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