# US 7,612,731 B2 · Methods and apparatus for reducing radio frequency interference for collocated antennas

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- Number: US 7,612,731 B2
- Document ID: US7612731B2
- Status: Granted
- Kind: B2
- Application number: 11/693,971
- Filed: 2007-03-30
- Published: 2007-11-08
- Granted: 2009-11-03
- Earliest claimed: 2006-03-31
- Assignees: Raytheon Company
- Inventors: Lewis Peterson
- Web page: https://patentgrep.com/patent/US7612731B2

## CPC

- H01Q 1/52: Means for reducing coupling between antennas; Means for reducing coupling between an antenna and another structure (absorbing means H01Q17/00)
- H01Q 1/521: {reducing the coupling between adjacent antennas}
- H01Q 1/526: {Electromagnetic shields}
- H01Q 15/0026: {said selective devices having a stacked geometry or having multiple layers}
- H01Q: ANTENNAS, i.e. RADIO AERIALS (radiators or antennas for microwave heating H05B6/72)

## Abstract

Methods and apparatus for a plate to prevent energy from a first antenna from interfering with a collocated second antenna. In one embodiment, the plate includes first and second conductive layers to shadow the second antenna and thereby block energy from reaching the second antenna. A resonant quarter wavelength spacing of the plates forces energy broadside minimizing the spillover the edge caused by diffraction. Multiple conductive layers having increasing radii can block diffracted energy from spilling over and around the plate. The multiple plates of increasing radii affect a waterfall-like spill wherein energy is lost in each level.

## Claims

### Claim 1

An apparatus, comprising:
a first conductive layer;
a first dielectric layer proximate the first conductive layer;
a second conductive layer substantially parallel to the first conductive layer and proximate the first dielectric layer so that the first and second conductive layers sandwich the first dielectric layer to create a resonant cavity for reducing radio frequency interference between a collocated first antenna and a second antenna operating in a first frequency band;
a third conductive layer substantially parallel to the second conductive layer and proximate a second dielectric layer so that the second and third conductive layers sandwich the second dielectric layer to create a further resonant cavity,
wherein the second conductive layer is larger than the first conductive layer to redirect energy due to diffraction at an edge of the first conductive layer, and the third conductive layer is larger than the second conductive layer to redirect energy due to diffraction at an edge of the second conductive layer,
wherein the first and second conductive layers are spaced at a quarter wavelength for a first frequency in the first frequency band and the second and third conductive layers are spaced at a quarter wavelength for a second frequency in the first frequency band.

### Claim 2 (depends on 1)

The apparatus according to claim 1, wherein the first and second layers are parallel to within a variation of one-tenth of a wavelength within the frequency band.

### Claim 3 (depends on 1)

The apparatus according to claim 1, wherein the first conductive layer has a surface area that is sufficient to shadow the first antenna from the second antenna.

### Claim 4 (depends on 1)

The apparatus according to claim 1, wherein a thickness of the dielectric layer is selected to take into account attenuation of velocity of wave propagation to achieve the one-quarter wavelength.

### Claim 5 (depends on 1)

The apparatus according to claim 1 wherein the dielectric layer includes a foam material.

### Claim 6 (depends on 1)

The apparatus according to claim 1 wherein the first, second, and third conductive layers are concentric circular disks.

### Claim 7 (depends on 1)

The apparatus according to claim 1, wherein a radius of the first conductive layer is an even multiple of a wavelength of the first frequency and a radius of the second conductive layer is an even multiple of the second frequency.

### Claim 8 (depends on 1)

The apparatus according to claim 1, further including a fourth conductive layer substantially parallel to the third conductive layer and sandwiching a third dielectric layer, wherein the fourth conductive layer is smaller than the third conductive layer.

### Claim 9

A method, comprising:
providing a first conductive layer;
providing a first dielectric layer proximate the first conductive layer;
providing a second conductive layer substantially parallel to the first conductive layer and proximate the first dielectric layer so that the first and second conductive layers sandwich the dielectric layer to create a resonant cavity for reducing radio frequency interference between a collocated first antenna and a second antenna operating in a first frequency band; and
providing a third conductive layer substantially parallel to the second conductive layer and proximate a second dielectric layer so that the second and third conductive layers sandwich the second dielectric layer to create a further resonant cavity,
wherein the second conductive layer is larger than the first conductive layer to redirect energy due to diffraction at an edge of the first conductive layer, and the third conductive layer is larger than the second conductive layer to redirect energy due to diffraction at an edge of the second conductive layer,
wherein the first and second conductive layers are spaced at a quarter wavelength for a first frequency in the first frequency band and the second and third conductive layers are spaced at a quarter wavelength for a second frequency in the first frequency band.

### Claim 10 (depends on 9)

The method according to claim 9, wherein the dielectric layer includes a foam material.

### Claim 11 (depends on 9)

The method according to claim 9, wherein the first and second conductive layers are concentric circular disks.

### Claim 12 (depends on 9)

The method according to claim 9, wherein the plate optically shadows the second antenna.

### Claim 13 (depends on 9)

The method according to claim 9, wherein a radius of the first conductive layer is an even multiple of a wavelength of the first frequency and a radius of the second conductive layer is an even multiple of the second frequency.
