Pulsed terahertz frequency domain spectrometer with single mode-locked laser and dispersive phase modulator

• US 20080179528A1
• Filed: 04/26/2007
• Published: 07/31/2008
• Est. Priority Date: 01/31/2007
• Status: Active Grant

• Current Assignee: Joseph R. Demers
• Original Assignee: Emcore Corporation
• Inventors: Demers, Joseph R.
• Granted Patent: US 7,439,511 B2
• Time in Patent Office: Days
• US Class Current: 250/341.1
• CPC Class Codes: G01J 3/42 Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry beam switching arrangements G01J3/08
• CPC Class Codes: G01N 21/3581 using far infrared light; using Terahertz radiation
• CPC Class Codes: G01N 2201/0221 Portable; cableless; compact; hand-held

Abstract

An apparatus for analyzing, identifying or imaging an target including a source of pulsed signals in the range of frequencies from 100 GHz to over 2 THz focused on or transmitted through the target; and a detector for acquiring spectral information from signals reflected from the target and using a multi-spectral heterodyning process to generate an electrical signal representative of some characteristics of the target. The source of pulse signals and the detector are photoconductive switches activated by a pulsed laser beam from a single mode-locked laser.

Claims

1. An apparatus for analyzing, identifying or imaging a target, comprising:

a source of pulse signals in the range of frequencies from 100 GHz to over 2 THz including a first photoconductive switch activated by a pulsed optical beam from a laser resulting in a frequency spectrum f, 2f, 3f, . . . etc. where f is the order of 100 MHz;

a radiator for causing said signals to be substantially simultaneously focused on or through said target; and

a detector for acquiring spectral information reflected from said target and coupled to a second pulsed optical beam derived from said laser for generating an electrical signal representative of some characteristic of the target.

2. An apparatus as in claim 1, wherein said detector includes a second photoconductive switch activated by a pulsed laser beam derived from said laser and having the frequency spectrum f+Δ

f, 2(f+Δ

f), 3(f+Δ

f), . . . etc., where Δ

f is of the order of 2.5 KHz.

3. An apparatus as defined in claim 1, further comprising a processor coupled to said detector for analyzing said electrical signal and determining a characteristic of said target based upon the absorption characteristics of said target in the 100 GHz to over 2 THz frequency band.

4. An apparatus as defined in claim 1 wherein said laser is a mode-locked laser for generating the respective pulsed laser beams directed to the first photoconductive switch.

5. An apparatus as defined in claim 4, wherein the output of the laser is split into two paths, the first path coupled to the first photoconductive switch, and the second path coupled to a beam modifying component.

6. An apparatus as defined in claim 5, wherein the output of said beam modifying component is coupled to said detector.

7. An apparatus as defined in claim 5, wherein said beam modifying component is a dispersive phase modulator.

8. An apparatus as defined in claim 7, wherein said dispersive phase modulator produces an output signal with a sequence of frequency shifted components with respect to the pulsed laser beam with each frequency shift in said sequence increasing with increasing optical frequency.

9. An apparatus as defined in claim 7, wherein said dispersive phase modulator is a lithium niobate modulator with the pulse intensity of the input pulse adjusted so as to adjust the dispersion in the non-linear lithium niobate medium

24. An apparatus as in claim 1 wherein the source of pulsed signals in the range of frequencies further comprises hundreds of locked modes spanning more than 1000 GHz.

10. An apparatus for analyzing, identifying or imaging a target, comprising:

a source of pulse signals in the range of frequencies of from 100 GHz to 3 THz;

a radiator for causing said signals to be substantially simultaneously focused or through said target;

a detector including a photoconductive switch activated by a pulsed laser beam with the frequency spectrum f+Δ

f, 2(f+Δ

f), 3(f+Δ

f), . . . etc. where f is the order of 100 MHz and Δ

f is of the order of 2.5 KHz, for acquiring spectral information reflected from or transmitted through said target for generating an electrical signal representative of some characteristics of the target; and

means coupled to said detector for processing said electrical signal.

11. An apparatus as defined in claim 10, further comprising a processor coupled to said detector for analyzing said electrical signal and determining a characteristic of said target based upon the absorption characteristics of said target in the 100 GHz to over 2 TH frequency band.

12. An apparatus as defined in claim 10, further comprising:

a mode-locked laser for generating a pulsed laser beam wherein the output of the laser is split into two paths, the first path coupled to the source of pulse signals in the range 100 GHz to over 2 THz, and the second path coupled to a beam modifying component having an output coupled to the detector.

25. An apparatus as in claim 10 wherein the pulsed beam further comprises hundreds of locked modes spanning more than 1000 GHz.

13. A portable apparatus for analyzing, identifying or imaging a target, comprising:

a housing capable of being supported by a user;

a source of pulse signals in said housing including a single mode-locked laser, said signals having simultaneous respective frequencies of f, 2f, 3f, . . . etc. where f is the order of 100 MHz and said signals being in the range of frequencies from 100 GHz to over 2 THz;

a radiator coupled to said source of pulsed signals for causing said signals to be focused on said target;

a detector in said housing for acquiring spectral information reflected from or transmitted through said target and generating an electrical signal representative of some characteristics of the target; and

a processor in said housing coupled to said detector for processing said electrical signal.

26. An apparatus as in claim 13 wherein the source of pulsed signals further comprises hundreds of locked modes spanning more than 1000 GHz.

14. A transceiver comprising:

a mode-locked laser for generating a pulsed laser beam;

a beam splitter for splitting said beam into first and second optical beams;

a photoconductive switch activated by said first optical beam resulting in a frequency spectrum f, 2f, 3f, . . . etc. where f is the order of 100 MHz; and

a detector including a photoconductive switch activated by said second optical beam with the frequency spectrum f+Δ

f, 2(f+Δ

f), 3(f+Δ

f), . . . etc. where Δ

f is of the order of 2.5 KHz, for acquiring spectral information reflected from or transmitted through said target and coupled to source for generating an electrical signal representative of some characteristics of the target.

27. An apparatus as in claim 14 wherein the first optical beam further comprises hundreds of locked modes spanning more than 1000 GHz.

15. A method of identifying or imaging a target comprising:

providing a single mode-locked laser for generating a pulsed laser beam;

simultaneously transmitting a predetermined spectral pattern of pulse signals derived from said pulsed laser beam to a target, said signals having respective frequencies of f, 2f, 3f, . . . etc. where f is the order of 100 MHz and said signals being in the range of frequencies from 100 GHz to over 2 THz;

detecting the return signals in said frequency range after transmission through or reflection from said target by utilizing a detector tuned to said spectral pattern derived from said pulsed laser beam shifted by a sequence of non-identical small amounts from said spectral pattern; and

analyzing said spectral information to identify said target or a compositional characteristic thereof.

16. A method as defined in claim 15, further comprising driving said detector by a dispersive phase modulator.

17. A method as defined in claim 15, further comprising driving said dispersive phase modulator by a sawtooth generator and said pulsed laser beam.

18. A method as defined in claim 15, wherein said pulsed laser beam activates a photoconductive switch resulting in a frequency spectrum f, 2f, 3, . . . etc. where f is the order of 100 MHz.

19. A method as defined in claim 15, wherein said pulsed laser beam is applied to and acted upon by a dispersive phase modulator.

20. A method as defined in claim 15, wherein said pulsed laser beam is split into two parts, with one part activating a photoconductive switch, and a second part being applied to and acted upon by a dispersive phase modulator.

21. A method as defined in claim 20, wherein the output of the dispersive phase modulator is coupled to said detector.

22. A method as defined in claim 15, wherein said detector is activated by a pulsed optical beam with the frequency spectrum f+Δ

f, 2(f+Δ

f), 3(f+Δ

f), . . . etc. where Δ

f is of the order of 2.5 KHz.

23. A method as defined in claim 15, wherein said detecting step provides instantaneous multi-spectral heterodyne down conversion of said return signals.

28. An apparatus as in claim 15 wherein the predetermined spectral pattern of pulse signals further comprises hundreds of locked modes spanning more than 1000 GHz.