Method and apparatus for the detection of terahertz radiation absorption
The invention is a method and apparatus for the detection of terahertz radiation. In one embodiment, frequency modulated spectroscopy is performed on a swept source of coherent far infrared electromagnetic radiation that is focused on a target. A beam of radiation passes through a cell in which the target is housed, losing energy as certain frequencies are absorbed by contaminants in the target. A detector is positioned to determine how much energy is lost by the radiation (e.g., which frequencies fail to transmit through the cell), thereby indicating the presence of contaminants in the target.
1. A system for
detecting contaminants in a sample, comprising:
a concentrator for concentrating molecules of the contaminants in said sample; and
a terahertz radiation detection system coupled to the concentrator for receiving the concentrated molecules for analysis, wherein the concentrator is coupled to the detection system by a sonic orifice.
2. A system for detecting contaminants in a sample, comprising:
a concentrator for concentrating molecules of the contaminants in said sample;
a terahertz radiation detection system coupled to the concentrator for receiving the concentrated molecules for analysis, the detection system comprising
a radiation source for generating frequency modulated far infrared radiation;
a low-pressure cavity coupled to the radiation source for receiving said sample; and
a radiation detector coupled to the low-pressure cavity.
3. The system of claim 2 , wherein the low-pressure cavity has one or more far infrared transmissive walls to allow the frequency modulated far infrared radiation to pass therethrough.
4. The system of claim 2 , wherein the radiation detector is cryogenically cooled.
5. The system of claim 2 , wherein the low-pressure cavity has:
a sample chamber for receiving said sample;
a vacuum chamber,
a terahertz transmissive window positioned between the sample chamber and the vacuum chamber; and
a conductive grating disposed within the vacuum chamber.
6. The system of claim 5 , wherein the low-pressure cavity further comprises:
a lid having a reflective surface positioned opposite to the terahertz transmissive window.
7. The system of claim 6 , wherein the lid is coupled to an actuator for controlling the position of the lid.
8. The system of claim 5 , wherein the low-pressure cavity further comprises:
a collector positioned proximate to an end of the conductive grating for intercepting an electron beam passed over the conductive grating.
9. The system of claim 8 , wherein the collector is coupled to a measurement device for measuring the energy of the electron beam.
10. The system of claim 9 , wherein the measurement device is an ammeter circuit.
11. The system of claim 5 , wherein the sample chamber further comprises:
a sample tube for containing a liquid in which said sample is suspended.
12. The system of claim 5 , wherein the low-pressure cavity further comprises:
an input pipe coupled to for sample chamber for collecting radiation from
an environment outside of the low-pressure cavity and funneling said radiation into the sample chamber.
13. The detector of claim 5 , wherein the sample chamber further comprises:
a sample tube for containing a liquid in which said sample is suspended.
14. The system of claim 2 , wherein the radiation source is an IMPATT multiplier.
15. A detector for detecting contaminants in a sample comprising:
a radiation source for generating frequency modulated terahertz radiation;
a low-pressure cavity coupled to the radiation source for containing said sample; and
a radiation detector coupled to the low-pressure cavity for measuring absorption of radiation by said sample for determining whether said contaminant is in said sample.
16. The detector of claim 15 , wherein the low-pressure cavity has one or more far infrared transmissive walls to allow the frequency modulated far infrared radiation to pass therethrough.
17. The detector of claim 15 , wherein the radiation detector is cryogenically cooled.
18. The detector of claim 15 , wherein the low-pressure cavity comprises: a sample chamber for receiving said sample;
a vacuum chamber,
a terahertz transmissive window positioned between the sample chamber and the vacuum chamber; and
a conductive grating disposed within the vacuum chamber.
19. The detector of claim 18 , wherein the sample chamber has:
a lid having a reflective surface positioned opposite to the terahertz transmissive window.
20. The detector of claim 19 , wherein the lid is coupled to an actuator for controlling the position of the lid.
21. The detector of claim 18 , wherein the low-pressure cavity further comprises; a collector positioned proximate to an end of the conductive grating for intercepting an electron beam passed over the conductive grating.
22. The detector of claim 21 , wherein the collector is coupled to a measurement device for measuring the energy of the electron beam.
23. The detector of claim 22 , wherein the measurement device is an ammeter circuit.
24. The detector of claim 18 , wherein the low-pressure cavity further comprises:
an input pipe coupled to the sample chamber for collecting radiation from an environment outside of the low-pressure cavity and funneling said radiation into the sample chamber.
25. The detector of claim 15 , wherein the radiation source is an IMPATT multiplier.
26. A method for detecting contaminant molecules in a sample, comprising:
introducing the sample into a first portion of a low-pressure cavity;
applying terahertz radiation to the sample; and
observing the interaction of the terahertz radiation with the sample, for detecting the presence of the contaminant molecules.
27. The method of claim 26 , further comprising:
concentrating the sample to enhance contaminant molecule density prior to introducing the sample into the low-pressure cavity.
28. The method of claim 26 , wherein the sample is introduced into the first portion of the low-pressure cavity in a gaseous state.
29. The method of claim 28 , wherein the step of observing the interaction of the terahertz radiation with molecules in the sample comprises:
providing a conductive grating disposed in a second portion of the low-pressure cavity, wherein the second portion of the low-pressure cavity is physically isolated from the first portion by a terahertz transmissive window; and
passing an electron beam over the conductive grating, in close proximity to the conductive grating; and
determining the amount of energy lost by the electron beam.
30. The method of claim 28 , wherein the step of observing the interaction of the terahertz radiation with molecules in the sample:
providing a conductive grating disposed in a portion of the low-pressure cavity;
passing an electron beam over the conductive grating, in close proximity to the conductive grating;
funneling radiation from an environment outside of the low-pressure cavity into the low-pressure cavity; and
determining the amount of energy gained by the electron beam.
31. The method of claim 26 , wherein the sample is introduced into the low-pressure cavity in a liquid state.
32. The method of claim 31 , wherein the step of observing the interaction of the terahertz radiation with molecules in the sample comprises:
introducing a portion of the sample into a first liquid to form a first liquid solution;
inserting the first liquid solution into a container disposed within the first portion of the low-pressure cavity;
observing the rotational spectrum of the molecules in the first liquid solution;
introducing a portion of the sample into a second liquid to form a second liquid solution, wherein the second liquid contains at least one binding agent for binding to the molecules in the sample;
inserting the second liquid solution into the container disposed within the first portion of the low-pressure cavity; and
observing the rotational spectrum of the molecules in the second liquid solution; and
comparing the rotational spectra of the first and second liquid solutions.
33. The method of claim 32 , wherein the step of observing the rotational spectra of the first and second liquid solutions comprises:
providing a conductive grating disposed in a second portion of the low-pressure cavity, wherein the second portion of the low-pressure cavity is physically isolated from the first portion by a terahertz transmissive window;
passing an electron beam over the conductive grating, in close proximity to the conductive grating; and
determining the amount of energy lost by the electron beam.
34. The method of claim 26 , wherein the step of applying terahertz radiation to the sample comprises modulating the frequency of the terahertz radiation.