Composite dipole array

• US 7,486,250 B2
• Filed: 02/15/2005
• Issued: 02/03/2009
• Est. Priority Date: 02/16/2004
• Status: Active Grant

• Current Assignee: The Boeing Co.
• Original Assignee: The Boeing Co.
• Inventors: Vetrovec, Jan, Holly, Sandor
• Primary Examiner(s): PHAN, THO GIA
• Application Number:
  US11/057,937
• Publication Number:
  US 20050200550A1
• Time in Patent Office: 1,449 Days
• Field of Search: 343/793, 343/795, 343/802, 343/814, 343/816, 343/820, 343/822, 343/824
• US Class Current: 343/820
• CPC Class Codes: F41H 11/136 Magnetic, electromagnetic, acoustic or radiation systems, e.g. ground penetrating radars or metal-detectors
• CPC Class Codes: G01N 21/3581 using far infrared light; using Terahertz radiation
• CPC Class Codes: H01Q 21/00 Antenna arrays or systems arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system H01Q3/00
• CPC Class Codes: H01Q 21/062 using dipole aerials; H01Q21/067, H01Q21/068 take precedence
• CPC Class Codes: H01Q 23/00 Antennas with active circuits or circuit elements integrated within them or attached to them

Abstract

Methods and systems for generating and imaging THz electromagnetic radiation using a composite dipole array made up of novel structures of non-linear dipole strings with dual frequency resonances for frequency up conversion and frequency down conversion are disclosed. THz electromagnetic radiation resulting from the frequency down conversion process can be used as an illumination source for imaging, as a carrier for communications, or as an energy source for spectroscopy, for example. Optical electromagnetic radiation resulting from the frequency up conversion process can be used to form images from THz electromagnetic radiation for contraband detection, guidance systems, and medical applications, for example.

Claims

1. A linear dipole array comprising:

a plurality of dipoles arranged end-to-end and defining a generally one-dimensional linear array, wherein all of the dipoles are substantially identical; and

a non-linear resonant circuit electrically interconnecting ends of corresponding adjacent dipoles throughout the linear dipole array such that a serial path is formed through all of the dipoles and the non-linear resonant circuits within the linear dipole array, wherein the linear dipole array forms a macro-dipole antenna, and wherein the dipoles are resonant at a higher frequency than a resonant frequency of the macro-dipole antenna.

2. The linear dipole array of claim 1, wherein the linear dipole array is one of a plurality of linear dipole arrays which form a composite dipole array, with the non-linear resonant circuits adapted to allow current flow serially through all of the dipoles and the non-linear resonant circuits within each of the linear dipole arrays, and wherein the linear dipole arrays are configured to be resonant at a terahertz frequency.

3. The linear dipole array of claim 1 wherein the non-linear resonant circuits couple the plurality of dipoles to facilitate current flow between the dipoles to radiate electromagnetic radiation at the resonant frequency of the macro-dipole antenna.

4. A composite dipole array comprising:

a plurality of linear dipole arrays defining a generally planar array, each of the linear dipole arrays comprising;

a plurality of dipoles defining a generally linear array, wherein all of the dipoles are substantially identical; and

a non-linear resonant circuit electrically interconnecting corresponding adjacent dipoles within the linear dipole array such that a serial path is formed through all of the dipoles and the non-linear resonant circuits within the linear dipole array, wherein each of the linear dipole arrays forms a macro-dipole antenna, and wherein the dipoles are resonant at a higher frequency than a resonant frequency of the macro-dipole antenna.

5. The composite dipole array of claim 4, wherein the individual dipoles are configured to be resonant at a frequency and the linear dipole arrays are configured to be resonant at another frequency.

6. The composite dipole array of claim 4, wherein the individual dipoles are configured to be resonant at an infrared frequency and the linear dipole arrays are configured to be resonant at a THz frequency.

7. The composite dipole array of claim 4, wherein the non-linear resonant circuits are configured to inhibit current flow between adjacent dipoles at one frequency more than they inhibit current flow between adjacent dipoles at another frequency.

8. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a diode.

9. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a diode and at least one of a capacitor and an inductor.

10. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a field effect diode.

11. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a triode.

12. The composite dipole array of claim 4, wherein:

the non-linear resonant circuit comprises a triode; and

a grid of the triode is in electrical communication with an antenna.

13. The composite dipole array of claim 4, further comprising a substrate upon which the dipoles and the nonlinear resonant circuits are formed.

14. The composite dipole array of claim 4, wherein the nonlinear resonant circuits comprise:

a diode having a gap between a cathode and an anode thereof; and

a substrate upon which the diodes are formed, the substrate having a trench formed therein proximate the gap so as to mitigate perturbation of an electrical field within the gap.

15. The composite dipole array of claim 4, further comprising:

a substrate upon which the linear dipole arrays are formed; and

an insulating layer formed intermediate the linear dipole arrays and the substrate.

16. The composite dipole array of claim 4, further comprising:

a substrate upon which the linear dipole arrays are formed; and

an insulating layer formed intermediate the linear dipole arrays, and the substrate, the insulating layer being formed of a plurality of dielectric layers.

17. The composite dipole array of claim 4, further comprising:

a substrate upon which the linear dipole arrays are formed; and

an insulating layer formed intermediate the linear dipole arrays and the substrate, the insulating layer being formed of a plurality of dielectric layers having thicknesses that enhances reflection at a predetermined frequency.

18. The composite dipole array of claim 4, further comprising:

a substrate upon which the linear dipole arrays are formed; and

an insulating layer formed intermediate the linear dipole arrays and the substrate, the insulating layer being formed of a plurality of dielectric layers having thicknesses that enhance transmission at a predetermined frequency.

19. The composite dipole array of claim 4, further comprising;

a substrate upon which the linear dipole arrays are formed; and

a reflector formed upon the substrate and configured so as to reflect electromagnetic radiation emitted from the composite dipole array in one direction such that it constructively interferes with electromagnetic radiation emitted from the composite dipole array in another direction.

20. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a diode formed of ends of the dipoles.

21. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a diode formed of layers of a material different from that of the dipoles proximate ends of the dipoles.

22. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises a diode formed of layers of refractory material proximate ends of the dipoles.

23. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises an inductor defined by a generally arc-shaped conductive path between a cathode and an anode of a diode of the non-linear resonant circuit.

24. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises an inductor defined by two generally arc-shaped conductive paths between a cathode and an anode of a diode of the nonlinear resonant circuit.

25. The composite dipole array of claim 4, wherein the non-linear resonant circuit comprises an inductor defined by two generally arc-shaped conductive paths between a cathode and an anode of a diode of the non-linear resonant circuit, at least one of the generally arc-shaped conductive paths having a capacitor formed therein.

26. The composite dipole array of claim 4, wherein the plurality of dipoles defining a generally linear array is configured to receive electromagnetic radiation at a first frequency and a second frequency and to re-radiate electromagnetic radiation at a third frequency.

27. The composite dipole array of claim 26, wherein the individual dipoles are configured to be resonant at the first and the second frequency and the linear dipole arrays are configured to be resonant at the third frequency.

28. The composite dipole array of claim 26, wherein the individual dipoles are configured to be resonant at infrared frequencies and the linear dipole arrays are configured to be resonant at a THz frequency.

29. The composite dipole array of claim 26, wherein the non-linear resonant circuits are configured to inhibit current flow between adjacent dipoles at the first and the second frequency more than they inhibit current flow between adjacent dipoles at the third frequency.

30. The composite dipole array of claim 4, wherein the non-linear resonant circuits couple the plurality of dipoles within each of the linear dipole arrays to facilitate current flow between the dipoles to radiate electromagnetic radiation at the resonant, frequency of the macro-dipole antenna.

31. A method for forming a linear dipole array, the method comprising forming a plurality of non-linear resonant circuits intermediate a corresponding plurality of pairs of substantially identical adjacent dipoles such that a serial path is formed through all of the dipoles and the non-linear resonant circuits within the linear dipole array, wherein the linear dipole array forms a macro-dipole antenna, and wherein the dipoles are resonant at a higher frequency than a resonant frequency of the macro-dipole antenna.

32. The method as recited in claim 31, wherein forming a non-linear resonant circuit comprises forming a field emission device.

33. The method as recited in claim 31, wherein the linear dipole array is one of a plurality of linear dipole arrays formed to provide a composite dipole array.

34. The method as recited in claim 31, wherein the nonlinear resonant circuits couple the plurality of dipoles to facilitate current flow between the dipoles to radiate electromagnetic radiation at the resonant frequency of the macro-dipole antenna.