BROADBAND JUNCTION FERRITE CIRCULATOR

Abstract

A rectangular waveguide circulator consists of multiple sections that meet at a common junction where a tapered ferrite portion is disposed. A ferrite portion is disposed within a hollow space adjacent the common junction. The ferrite portion has a shape that includes an upper portion, a middle portion, and a lower portion, such that a cross sectional area of the upper portion is greater than a cross-sectional area of the middle portion, and such that a cross sectional area of the lower portion is greater than the cross-sectional area of the middle portion.

Claims

1. A circulator device comprising: three sections of rectangular conductively bounded hollow waveguide, the three sections connected to meet in a common junction; and a ferrite portion, disposed within a hollow space adjacent the common junction, the ferrite portion having a shape that includes an upper portion, a middle portion, and a lower portion, such that a cross sectional area of the upper portion is greater than a cross-sectional area of the middle portion, and such that a cross sectional area of the lower portion is greater than the cross-sectional area of the middle portion.

2. The device of claim 1 wherein the ferrite portion further comprises three ordered cross-sections A, B, and C such that: a. cross-section A is located closer to a top wall of the common junction than a plane at cross-section B or C; b. cross-section C is located closer to another wall of the common junction than a plane at either A or B; and/or c. an area of cross-section B is less than either the areas of cross-section A or cross-section C.

3. The device of claim 1 further wherein the shape of the ferrite portion is such that an operation band falls within a desired range with a broadened frequency response.

4. The device of claim 1 wherein the upper portion has a different cross sectional shape than a cross sectional shape of the lower portion.

5. The device of claim 1 wherein the shape of the ferrite portion has a continuous taper from the upper portion through the middle portion to the lower portion.

6. The device of claim 1 wherein the ferrite portion further comprises a plurality of stacked ferrite material sections, each material section being generally planar.

7. The device of claim 1 wherein at least one of the upper portion, middle portion or lower portion has a circular cross-sectional shape.

8. The device of claim 1 wherein at least one of the upper portion, middle portion or lower portion has a triangular cross-sectional shape.

9. The device of claim 1 wherein the ferrite portion is interposed with at least one dielectric layer.

10. The device of claim 1 wherein the ferrite portion is interposed with at least one electrically conductive layer.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0019] FIG. 1 illustrates an example circulator device implemented in rectangular waveguide sections arranged in a Y-junction.

[0020] FIG. 2 shows an example ferrite post in more detail.

[0021] FIGS. 3A, 3B, 3C and 3D each depict still other configurations of ferrite posts.

[0022] FIG. 4 is another example of a ferrite post.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

[0023] Referring to FIG. 1, a rectangular waveguide circulator device has three or more ports 94, 95, and 96 connected through respective waveguides 93 to a common junction 92. The waveguides may be rectangular, conductively bounded hollow waveguides. A ferrite portion, typically a post, 91 of center-narrowed cross-section is disposed in a hollow space formed at the waveguide junction 92. An external magnetic field 97 is applied to the device. Typically, the strength of the magnetic field may be 1000 to 5000 Gauss. The magnetic field is strong enough to bias the ferrite material near saturation. The direction of the magnetic field determines the rotation of the circulator. Methods for providing a magnetic bias field include permanent magnets and electromagnets deposed around the junction (not shown here).

[0024] Use of a tapered ferrite has been found to broaden the frequency response of the circulator. A key feature of this device is the taper of the ferrite post 91 toward the center of the waveguide along the direction of the bias field and normal to the direction of signal propagation. This taper of the post 91 thus acts to broaden the frequency response of the circulator which is desirable for many applications.

[0025] The profile of the taper of the ferrite can be along a continuous curve (as depicted in FIG. 1) or can have one or more step discontinuities 98 as shown in FIG. 2. The ferrite post 91 can be of any shape provided the cross-section area is smaller in the middle of the ferrite than at the ends.

[0026] Referring to FIGS. 3A through 3D, ferrite posts 91 can be described as having three ordered horizontal cross-sections 105, 106 and 107 where the upper cross-section at 105 is closer to a top wall of the waveguide 101 than the cross-sections at 106 and 107. The lower cross-section at 107 is closer to the bottom wall 102 than cross-sections at 105 and 106. The middle cross-sectional area at point 106 is less than cross-sectional area at 105 and less than the cross-sectional area at 107.

[0027] The ferrite post 91 may be interposed or stacked with non-ferrite layers at any number of distances along its length. These layers can be generally planar dielectric layers or generally planar electrically conductive layers. These features are used, for example, to change the waveguide impedance at the junction, or to provide thermal heat transfer, or to alter the boundary conditions at the ferrite interfaces. Examples are shown in FIGS. 3A, 3C, and 3D where these non-ferrite layers or plates 110 are disposed along the length of the ferrite post 91 at various locations including one or both ends of the ferrite post 91 and/or in the middle. The general case of a dielectric is intended to include air and vacuum.

[0028] The device need not be rotationally symmetric along the magnetic field axis. For example, FIG. 4 shows a bi-pyramidal ferrite post 120.

[0029] Although ferrite materials are used almost universally at the present time, it is anticipated that any non-reciprocal material performing the same function can equivalently be used in place of a ferrite.

[0030] In one possible embodiment, the ferrite is a general cylinder shape with a tapered middle section forming a narrow waist or neck in the ferrite. In one embodiment the ferrite tapered section has a quadratic profile. In another embodiment, the ferrite tapered section has a linear profile (straight lines). In another embodiment, the ferrite taper has a circular profile. In another embodiment, the profile of the taper is a series of steps rather than a continuous curve. In another embodiment the waveguide wall has a step in the height of the waveguide over a portion that includes the tapered ferrite. In another embodiment the waveguide wall has a step in the width of the waveguide over a portion that includes the tapered ferrite.

[0031] It should be understood that while a particular feature may have been disclosed above with respect to only one of several embodiments, that particular feature may be combined with one or more other features of the other embodiments as may be desired and advantageous for any given or particular application. It is, of course, not possible to describe every conceivable combination of components or methodologies for purposes of describing the innovations herein, and one skill in the art may now, in light of the above description, recognize that many further combinations and permutations are possible. Accordingly, the claimed subject matter is intended to embrace all such alterations, modifications, and variations that fall within the spirit and scope of the appended claims.