Optical RF filtering system

Claim 2

In an optical method for RF receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator: passing a beam of substantially coherent radiation through said acousto-optical modulator to modulate said beam with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and impinging it on sensing means such that the spectral frequency location in said beam of narrow-band interfering signals whose amplitude exceeds a predetermined background level is detected; programming a spatial filter located at said Fourier plane with the spectral location of said detected narrow-band interfering signals; passing said transformed modulated beam through said programmed spatial filter such that said detected interfering signals at said spectral locations are deleted; optically inversely transforming said filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; passing the photodetector output to said RF receiver for post processing.

Claim 3

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acousto-optical modulator to modulate with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and impinging it on a linear array of photodetectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; programming a spatial filter positioned at said Fourier plane with the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of segments corresponding substantially with said photodetectors in said linear array, such that photodetectors in said array receiving radiation of an amplitude representing a narrow-band interfering signal produce an output which renders its associated filter segment in said linear arrangement opaque to block radiation at the spectral location to notch said narrow-band interfering signal out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodetector output to said RF receiver for post processing.

Claim 4

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acousto-optical modulator to modulate with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and impinging it on a linear array of photodetectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; programming a spatial filter positioned at said Fourier plane with the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of segments corresponding substantially with said photodetectors in said linear array, such that photodetectors in said array receiving radiation of an amplitude representing a narrow-band interfering signal produce an output which renders its associated filter segment in said linear arrangement opaque to block radiation at the spectral location to notch said narrow-band interfering signal out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodetector output to said RF receiver for post processing.

Claim 5

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acoustr-optical modulator to modulate said beam with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and impinging it on a linear array of photodetectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; intergrating the optical spectrum detected by said linear array of photodetectors to derive the voltage analogue of said spectrum; passing said voltage analogue through a threshold detector which is set to pass voltage signals corresponding to the amplitude of said interfering signals; providing address means to designate an address which codes the precise position of each of said interfering signals corresponding to their location in the RF radiation spectrum; programming a spatial filter positioned at said Fourier plane using said address code to designate the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of segments having a substantially one to one correspondence with said photodetectors in said linear array such that the filter segments at the addresses designating narrow-band interfering signals are rendered opaque to block radiation at the spectral location to notch said narrow-band interfering signals out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodector output to said RF receiver for post processing.

Claim 6

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acoustr-optical modulator to modulate said beam with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and impinging it on a linear array of photodetectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; intergrating the optical spectrum detected by said linear array of photodetectors to derive the voltage analogue of said spectrum; passing said voltage analogue through a threshold detector which is set to pass voltage signals corresponding to the amplitude of said interfering signals; providing address means to designate an address which codes the precise position of each of said interfering signals corresponding to their location in the RF radiation spectrum; programming a spatial filter positioned at said Fourier plane using said address code to designate the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of segments having a substantially one to one correspondence with said photodetectors in said linear array such that the filter segments at the addresses designating narrow-band interfering signals are rendered opaque to block radiation at the spectral location to notch said narrow-band interfering signals out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodector output to said RF receiver for post processing.

Claim 7

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acousto-optical modulator to modulate said beam with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and implinging it on a linear array of photodectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; integrating the optical spectrum detected by said linear array of photodetectors to derive the voltage analogue of said spectrum; passing said voltage analogue through a threshold detector which is set to pass voltage signals corresponding to the amplitude of said interfering signals; providing address means to designate an address which codes the precise position of each of said interfering signals corresponding to their location in the RF radiation spectrum; programming a spatial filter positioned at said Fourier plane using said address code to designate the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of liquid crystal segments having a substantially one-to-one correspondence with said photodetectors in said linear array, the crystalline structure of said segments changing its alignment under the influence of an electric field to vary the light-transmitting properties thereof, each of said liquid crystal segments being in circuit electrically through said address means with a specific associated photodector in said linear photodetector array, an electric field being applied to said liquid crystal segments under the designation of said address means in correspondence with the linear location of interfering signals detected by said linear array such that the filter segments at the addresses designating narrow-band interfering signals are rendered opaque to block radiation at that spectral location to notch said narrow-band interfering signals out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodetector output to said RF receiver for post processing.

Claim 8

In an optical method for RF spread spectrum receivers for the multifrequency filtering of RF narrow-band interfering signals, the steps comprising: inputting RF input signals from said receiver into an acousto-optical modulator; passing a beam of substantially coherent radiation through said acousto-optical modulator to modulate said beam with said RF signal input; transforming said modulated beam by passing it through optical Fourier transform means to produce a transformed beam having a spatial frequency distribution at the back focal plane of said transform means corresponding with said RF signal input spread spectrum frequency distribution, said back focal plane being the Fourier plane; diverting energy from said transformed modulated beam and implinging it on a linear array of photodectors, said photodetectors in said linear array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level; integrating the optical spectrum detected by said linear array of photodetectors to derive the voltage analogue of said spectrum; passing said voltage analogue through a threshold detector which is set to pass voltage signals corresponding to the amplitude of said interfering signals; providing address means to designate an address which codes the precise position of each of said interfering signals corresponding to their location in the RF radiation spectrum; programming a spatial filter positioned at said Fourier plane using said address code to designate the spectral location of said detected narrow-band interfering signals, said spatial filter having a comb-like linear arrangement of liquid crystal segments having a substantially one-to-one correspondence with said photodetectors in said linear array, the crystalline structure of said segments changing its alignment under the influence of an electric field to vary the light-transmitting properties thereof, each of said liquid crystal segments being in circuit electrically through said address means with a specific associated photodector in said linear photodetector array, an electric field being applied to said liquid crystal segments under the designation of said address means in correspondence with the linear location of interfering signals detected by said linear array such that the filter segments at the addresses designating narrow-band interfering signals are rendered opaque to block radiation at that spectral location to notch said narrow-band interfering signals out of the radiation passing through said spatial filter; optically inversely transforming the filtered beam from said spatial filter by passing it through an optical inverse Fourier transform means having its front focal plane at said Fourier plane to transform said filtered RF spectra into the time domain; optically combining said inversely transformed beam with an optical local oscillator reference beam to eliminate positional dependence and to generate a difference frequency by a heterodyning action; impinging said combined beams on a square-law photodetector at the inverse transform plane of the inverse transform means; electrically filtering the photodetector output to remove outband noise; passing the filtered photodetector output to said RF receiver for post processing.

Claim 9

An optical spatial filtering system for RF spread spectrum signals comprising: an RF signal source, a radiation source for producing a beam of substantially coherent collimated optical radiation, an acousto-optical modulator driven by Rf signals from said RF source, means for producing an optical Fourier transform of said optical radiation beam modulated by said RF signals, a programmable optical notching filter at the back focal plane of said optical Fourier transform means, said back focal plane being the Fourier plane, means for diverting energy from said modulated radiation beam, linear array means for sensing the location in the frequency domain of narrow-band interfering signals in said diverted modulated radiation beam, means using the output of said linear array of sensing means for programming said programmable notching filter to reject signals having an amplitude above a predetermined threshold, optical means having its front focal plane at said Fourier plane for producing an inverse optical transform, an optical local oscillator, an optical beam combiner, detecting means at the inverse transform plane of said inverse optical transform means for converting optical input signals into an electrical output, and an electrical bandpass filter, whereby RF signals from said RF source are used to drive said acousto-optical modulator to impress a spread RF spectrum on said beam of optical radiation and an optical Fourier transform is taken of said modulated beam of radiation, which transformed beam is filtered by said programmable filter to notch out signals in said spread spectrum whose amplitude has identified them as comprising noise and said filtered optical radiation is inversely optically Fourier transformed and combined by said beam combiner with radiation from said local oscillator such that positional dependence is eliminated to produce a summed output which is detected by said detecting means, the electrical output of which is filtered by said band-pass filter to thereby deliver down-converted EMI-free RF spectra for post processing in said RF receiver.

Claim 10

An optical spatial filtering system for RF spread spectrum signals comprising: an RF signal source, a radiation source for producing a beam of substantially coherent collimated optical radiation, an acousto-optical modulator driven by Rf signals from said RF source, means for producing an optical Fourier transform of said optical radiation beam modulated by said RF signals, a programmable optical notching filter at the back focal plane of said optical Fourier transform means, said back focal plane being the Fourier plane, means for diverting energy from said modulated radiation beam, linear array means for sensing the location in the frequency domain of narrow-band interfering signals in said diverted modulated radiation beam, means using the output of said linear array of sensing means for programming said programmable notching filter to reject signals having an amplitude above a predetermined threshold, optical means having its front focal plane at said Fourier plane for producing an inverse optical transform, an optical local oscillator, an optical beam combiner, detecting means at the inverse transform plane of said inverse optical transform means for converting optical input signals into an electrical output, and an electrical bandpass filter, whereby RF signals from said RF source are used to drive said acousto-optical modulator to impress a spread RF spectrum on said beam of optical radiation and an optical Fourier transform is taken of said modulated beam of radiation, which transformed beam is filtered by said programmable filter to notch out signals in said spread spectrum whose amplitude has identified them as comprising noise and said filtered optical radiation is inversely optically Fourier transformed and combined by said beam combiner with radiation from said local oscillator such that positional dependence is eliminated to produce a summed output which is detected by said detecting means, the electrical output of which is filtered by said band-pass filter to thereby deliver down-converted EMI-free RF spectra for post processing in said RF receiver.

Claim 11

The optical filtering system set forth in claim 5 wherein the linear array means for sensing is a linear array of photodetectors, said photodetectors in said array detecting the linear location in the incident spread spectrum radiation of narrow-band interfering signals whose amplitude exceeds a predetermined background level.

Claim 12

The optical filtering system set forth in claim 6 wherein the optical spectrum detected by said linear array is integrated to derive the voltage analogue of said spectrum, said voltage analogue being processed in a threshold detector which outputs voltage signals exceeding a predetermined amplitude.

Claim 13

The optical filtering system set forth in claim 5 wherein the programmable filter has a comb-like linear arrangement of segments having a substantially one-to-one correspondence with said photodetectors in said linear array such that said filter segments can be programmed to become opaque at locations designated by the linear array of sensing means to block radiation at that spectral location to notch narrow-band interfering signals.

Claim 14

The optical filtering system set forth in claim 8 wherein the linear arrangement of segments of the programmable filter are liquid crystals, the crystalline structure of which changes its alignment under the influence of an electric field to vary the light-transmitting properties thereof, each of said segments being in circuit electrically with a specific associated photodetector in the linear photodetector array, an electric field being applied to said segments by said linear photodetector array to render said segments opaque at the locations identifying narrow-band interfering signals such that those signals are notched by said filter.

Claim 15

The optical filtering system set forth in claim 7 wherein the threshold detector output is passed to address means to designate notching means in the programmable notching filter at the locations in the RF radiation spectrum of narrow-band interfering signals such that said notching means can be programmed to notch said interfering signals.