Method and apparatus for analyzing, identifying or imaging a target

• US 8,957,377 B2
• Filed: 10/15/2013
• Issued: 02/17/2015
• Est. Priority Date: 05/19/2008
• Status: Active Grant

• Current Assignee: Joseph R. Demers
• Original Assignee: Emcore Corporation
• Inventors: Logan, Ronald T., Demers, Joseph R.
• Primary Examiner(s): Bryant, Casey
• Application Number:
  US14/054,599
• Publication Number:
  US 20140043612A1
• Time in Patent Office: 490 Days
• Field of Search: 250/336.1, 250/338.1, 250/339.06, 250/339.07
• US Class Current: 250/339.07
• CPC Class Codes: A61B 5/0507 using microwaves or terahertz waves
• CPC Class Codes: G01J 3/10 Arrangements of light sources specially adapted for spectrometry or colorimetry
• CPC Class Codes: G01J 3/42 Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry beam switching arrangements G01J3/08
• CPC Class Codes: G01J 3/427 Dual wavelengths spectrometry
• CPC Class Codes: G01J 3/4531 Devices without moving parts
• CPC Class Codes: G01N 21/3581 using far infrared light; using Terahertz radiation
• CPC Class Codes: G01N 21/3586 by Terahertz time domain spectroscopy [THz-TDS]
• CPC Class Codes: G01N 21/39 using tunable lasers

Abstract

An apparatus for analyzing, identifying or imaging an target including first and second laser beams coupled to a pair of photoconductive switches to produce CW signals in one or more bands in a range of frequencies greater than 100 GHz focused on and transmitted through or reflected from the target; and a detector for acquiring spectral information from signals received from the target and using a multi-spectral heterodyne process to generate an electrical signal representative of some characteristics of the target. The lasers are tuned to different frequencies and a frequency shifter in the path of one laser beam allows the terahertz beam to be finely adjusted in one or more selected frequency bands.

Claims

1. A method for analyzing, identifying, or imaging a target, said method comprising:

providing first and second lasers, said first laser having a tunable frequency and configured to produce a first output beam and said second laser having a tunable frequency and configured to produce a second output beam, said first output beam and said second output beam having different frequencies, wherein the frequency of the first output beam is coarsely adjustable by temperature adjustment of the first laser and the frequency of the second output beam is coarsely adjustable by temperature adjustment of the second laser;

producing a first composite output beam from a first portion of said first output beam and a first portion of said second output beam;

producing a second composite output beam from a second portion of said first output beam and a second portion of said second output beam, wherein the second portion of the first output beam is coupled to a frequency control element for controllably finely adjusting the frequency of the second portion of the first output beam to finely adjust a frequency difference between the first composite output beam and the second composite output beam;

generating CW signals in the range of frequencies from 100 GHz to over 2 THz using said second composite output beam;

causing said CW signals to be substantially simultaneously focused on or through said target;

acquiring a spectral information signal from said target; and

generating an electrical signal representative of a characteristic of said target based on said spectral information signal and said first composite output beam.

2. A method as defined in claim 1, wherein producing said second composite output beam from said second portion of said first output beam and said second portion of said second output beam includes controllably adjusting the frequency of said second portion of said first output beam by a tunable reference oscillator coupled to the frequency control element such that said second composite output beam has said adjustable frequency difference with respect to said first composite output beam.

3. A method as defined in claim 2, wherein generating said CW signals includes activating a first photoconductive switch using said second composite output beam.

4. A method as defined in claim 3, wherein generating said electrical signal includes activating a second photoconductive switch using said first composite output beam.

5. A method as defined in claim 4, wherein the tunable reference oscillator is coupled to a lock-in amplifier coupled to the second photoconductive switch.

6. A method as defined in claim 3, further comprising biasing the first photoconductive switch using a “

lock-in”

amplifier with a modulated bias voltage.

7. A method as defined in claim 1, further comprising sweeping the CW signals by activating a first photoconductive switch by the second composite optical beam, and sweeping the frequency of one of said first and second lasers.

8. A method as defined in claim 7, further comprising performing a heterodyne down conversion of the acquired spectral information from the target by activating a second photoconductive switch by the first composite optical beam.

9. A method as defined in claim 1, further comprising:

storing a spectral signature of a compound;

sweeping the CW signals over at least one frequency band in the range of frequencies from 100 GHz to 1.5 THz; and

subsequently determining whether the spectral signature of the compound is present in the acquired spectral information by tuning the frequency of the CW signals in frequency increments of less than 100 MHz.

10. A method as defined in claim 1, further comprising providing first and second thermoelectric coolers coupled to the first and second lasers, respectively, for independently coarsely tuning each of the first and second lasers over a wavelength range of about 5 nm intervals or step sizes of about 0.01 nm.

11. A method as defined in claim 1, wherein the frequency control element comprises a frequency shifter coupled to the second portion of the first output beam from the first laser for tuning the frequency of the second portion of the first output beam from the first laser over at least a portion of the frequency range between 0 and 10 GHz.

12. A method as defined in claim 11, further comprising providing a reference oscillator coupled to the frequency shifter for tuning the frequency of the second portion of the first output beam from the first laser with a frequency interval or step size less than 1 MHz.

13. A method as defined in claim 11, further comprising providing a reference oscillator coupled to the frequency shifter for tuning the frequency of the second portion of the first output beam from the first laser.

14. A method as defined in claim 13, wherein the reference oscillator has an adjustable frequency interval or step size between 1 Hz and 1 GHz.

15. A method as defined in claim 13, wherein the terahertz variation in the intensity of a mixing or difference signal between the frequencies of the first and second lasers, in combination with the terahertz modulation of the conductance in photoconductive semiconductor material as a result of a terahertz current flow in an antenna used to receive a terahertz signal from the sample to acquire the spectral information from the target results in a heterodyning and down conversion of the received terahertz signal to a baseband frequency equal to the frequency of the reference oscillator.

16. A method as defined in claim 1, wherein the frequency control element comprises a frequency shifter coupled to the second portion of the first output beam from the first laser for tuning the frequency of the second portion of the first output beam from the first laser with an adjustable frequency interval or step size between 1 Hz and 1 GHz.

17. A method as defined in claim 1, wherein the frequency control element comprises a frequency modulator coupled to the second portion of the first output beam from the first laser for tuning the frequency of the second portion of the first output beam from the first laser, wherein the frequency modulator has an electronically adjustable bias for tuning the frequency of the second portion of the first output beam from the first laser.

18. A method as defined in claim 17, wherein the frequency modulator performs a frequency shift of the second portion of the first output beam from the first laser.

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

first and second lasers, said first laser having a tunable frequency and configured to produce a first output beam and said second laser having a tunable frequency and configured to produce a second output beam, said first output beam and said second output beam having different frequencies, wherein a first portion of said first output beam and a first portion of said second output beam produce a first composite output beam configured to be swept over a frequency band as the frequency of at least one of the first and second lasers is swept;

a frequency shifting element coupled to a reference oscillator and positioned to receive a second portion of said first output beam to controllably shift the frequency of said second portion of said first output beam;

a beam combiner coupled to an output the frequency shifting element and to a second portion of the second output beam to produce a second composite beam, wherein the frequency shifting element is configured to controllably finely adjust the frequency of the second portion of the first output beam to finely adjust a frequency difference between the first composite output beam and the second composite output beam;

a first photoconductive switch activated by said second composite output beam to produce CW signals in the range of frequencies from 100 GHz to over 2 THz;

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

a second photoconductive switch activated by said first composite output beam and positioned with respect to the target so as to acquire a spectral information signal from the target, and to generate, based on said spectral information and said first composite output beam and heterodyne down conversion, an electrical signal representative of a characteristic of said target.

20. The apparatus of claim 19, wherein the frequency shifting element comprises a frequency modulator coupled to the second portion of the first output beam from the first laser for tuning the frequency of the second portion of the first output beam from the first laser and having an electronically adjustable bias for tuning the frequency of the second portion of the first output beam from the first laser.

21. The apparatus of claim 20, wherein the frequency modulator performs a frequency shift of the second output beam from the first laser.

22. The apparatus of claim 19, wherein the reference oscillator is configured for tuning the frequency of the second portion of the first output beam from the first laser with a frequency interval of step size less than 1 MHz.

23. The apparatus of claim 19, wherein the reference oscillator is configured for tuning the frequency of the second portion of the first output beam from the first laser.