Distributed array for direction and frequency finding
An optical imaging system and method that reconstructs RF sources in k-space by utilizing interference amongst modulated optical beams. The system and method involves recording with photodetectors the interference pattern produced by RF-modulated optical beams conveyed by optical fibers having unequal lengths. The photodetectors record the interference, and computational analysis using known tomography reconstruction methods is performed to reconstruct the RF sources in k-space.
1. An optical imaging receiver comprising:
a phased-array antenna including a plurality of antenna elements arranged in a first pattern configured to receive RF signals from at least one RF source;
a plurality of electro-optic modulators corresponding to the plurality of antenna elements, each modulator configured to modulate an optical carrier with a received RF signal to generate a plurality of modulated optical signals;
a plurality of optical channels configured to carry the plurality of modulated optical signals and configured to cause interference amongst the optical signals, each of the plurality of optical channels having an output to emanate the corresponding modulated optical signal out of the corresponding optical channel, the outputs of the plurality of optical channels arranged in a second pattern which does not correspond to the first pattern;
a plurality of photodetectors for recording the optical signal interference; and
a module for computationally reconstructing RF sources in k-space from the recorded interference.
2. The optical imaging receiver of claim 1 , said plurality of optical channels comprising a plurality of optical fibers, the optical fibers having varying lengths.
3. The optical imaging receiver of claim 2 , wherein at least two optical fibers of said plurality of optical fibers are connected to the output of at least one of the plurality of modulators.
4. The optical imaging receiver of claim 1 , wherein the distribution of antennas in the phased-array antenna is non-coplanar.
5. The optical imaging receiver of claim 1 , wherein the module uses a computational tomography technique which include algebraic reconstruction technique (ART) or its multiplicative version (MART) in reconstructing the RF sources in k-space from the recorded interference.
6. The optical imaging receiver of claim 2 , wherein lengths of the optical fibers vary linearly in accordance with their position in relation to the antenna array.
7. A method utilized by an optical imaging receiver for RF signal processing, comprising:
receiving incoming RF signals at a phased-array antenna including a plurality of antenna elements arranged in a first pattern;
modulating the received RF signals from each of the plurality of antenna elements onto an optical carrier to generate a plurality of modulated optical signals;
directing the plurality of modulated optical signals to a plurality of optical channels, configured to cause interference amongst the optical signals, each of the plurality of optical channels having an output to emanate the corresponding modulated optical signal out of the corresponding optical channel, the outputs of the plurality of optical channels arranged in a second pattern which does not correspond to the first pattern;
providing a plurality of photodetectors for recording the optical signal interference; and
computationally reconstructing RF sources in k-space from the recorded interference.
8. The method of claim 7 , said plurality of optical channels comprising a plurality of optical fibers, the optical fibers having varying lengths.
9. The method of claim 8 , wherein at least two optical fibers having varying lengths of said plurality of optical fibers are connected to the output of at least one of said plurality of modulators.
10. The method of claim 7 , wherein the distribution of antennas in the phased-array antenna is non-coplanar.
11. The method of claim 7 , wherein computationally reconstructing involves using a technique which includes algebraic reconstruction technique (ART) or its multiplicative version (MART) for reconstructing the RF sources in k-space from the recorded interference.
12. The method of claim 8 , wherein the lengths of the optical fibers vary linearly in in accordance with their position in relation to the antenna array.