Time resolved raman spectroscopy

• US 8,325,337 B2
• Filed: 07/14/2008
• Issued: 12/04/2012
• Est. Priority Date: 07/13/2007
• Status: Active Grant

• Current Assignee: Purdue Research Foundation (Purdue University)
• Original Assignee: Purdue Research Foundation (Purdue University)
• Inventors: Sinfield, Joseph V., Colic, Oliver
• Primary Examiner(s): NGUYEN, SANG H
• Application Number:
  US12/668,844
• Publication Number:
  US 20110261354A1
• Time in Patent Office: 1,604 Days
• Field of Search: 356300-301, 356/319, 356/326, 356/328, 356/73, 600/473, 600/476, 378/37, 435/287.2, 250/203.2, 250/201.3
• US Class Current: 356/301
• CPC Class Codes: G01J 3/02 Details
• CPC Class Codes: G01J 3/0202 Mechanical elements; Supports for optical elements
• CPC Class Codes: G01J 3/021 using plane or convex mirrors, parallel phase plates, or particular reflectors
• CPC Class Codes: G01J 3/0218 using optical fibers
• CPC Class Codes: G01J 3/027 Control of working procedures of a spectrometer; Failure detection; Bandwidth calculation
• CPC Class Codes: G01J 3/0291 Housings; Spectrometer accessories; Spatial arrangement of elements, e.g. folded path arrangements
• CPC Class Codes: G01J 3/44 Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
• CPC Class Codes: G01N 21/64 Fluorescence; Phosphorescence
• CPC Class Codes: G01N 21/65 Raman scattering

Abstract

System, method, and apparatus for determining the composition of a sample of material. In one embodiment, the method pertains to the counting of photons that were inelastically scattered by the sample, and for minimizing the effects of fluorescent or phosphorescent photons. In yet another embodiment of the invention, a sample is illuminated by a repetitive pulse of monochromatic light, and the resultant scattered photons from the samples are collected and counted during a predetermined integration period. Yet other embodiments pertain to a low-cost, computer-controlled system for repetitively counting inelastically scattered photons so as to create a Raman histogram and a Raman spectrogram of the photons.

Claims

1. A method for determining the composition of a sample, comprising:

providing a controller and a source of pulsed light and a sensor receiving photons and providing an electrical signal corresponding to each received photon;

repetitiously illuminating the sample with a pulse of light from the source, wherein some of the source photons from each pulse are scattered by the sample;

substantially eliminating the elastically scattered photons and collecting the Raman-shifted inelastically scattered photons;

preparing a time histogram of the number of collected Raman-shifted photons, the histogram dividing a predetermined period of time into a plurality of counting bins arranged in sequential order, each bin containing a natural number corresponding to the number of Raman-shifted photons collected during the corresponding time interval, one of the bins having the largest natural number; and

determining by the controller the composition of the sample by analyzing the photons collected earlier in time than the one bin and ignoring the photons collected later in time than the one bin.

2. The method of claim 1 which further comprises starting the period of time after a predetermined delay time, the delay time corresponding to transmission delays associated with the sensor.

3. The method of claim 2 wherein said providing includes a second sensor providing a second electrical signal corresponding to the receipt by the second sensor of a photon, and which further comprises:

splitting the pulse;

directing a split portion of the pulse to the second sensor; and

beginning the delay time by the second electrical signal.

4. The method of claim 1 which further comprise beginning the period of time by the counting of a photon by the sensor.

5. The method of claim 1 wherein the source of light is a Q switched laser.

6. The method of claim 1 wherein the sensor is a photo-multiplier tube.

7. The method of claim 1 wherein the source is a monochromatic source of coherent light.

8. The method of claim 1 wherein the source of light is monochromatic with a wavelength more than about 500 nanometers and less than about 600 nanometers.

9. The method of claim 1 which further comprises rejecting the scattered photons that are not within a predetermined frequency band before said counting.

10. The method of claim 1 wherein the source is a monochromatic source, said collecting is at a first frequency, and which further comprises:

illuminating the sample with a second pulse of light having a beginning and an ending, wherein some of the source photons of the second pulse are scattered by the sample;

substantially eliminating the elastically scattered photons and collecting the inelastically scattered photons of the second pulse at a second frequency different than the first frequency;

counting the Raman-shifted inelastically scattered photons by the sensor at the second frequency during a second predetermined period of time; and

stopping said counting before collecting a statistically significant sample of non-Raman shifted photons.

11. The method of claim 1 wherein the period of time is less than about six times the period of the pulse.

12. The method of claim 1 which further comprises not counting Raman-shifted inelastically scattered photons that have a frequency that is less than a first lower frequency or greater than a second higher frequency.

13. The method of claim 1 wherein the sensor converts each collected photon to a corresponding electrical signal, and which further comprises not counting a photon if the magnitude of the corresponding electrical signal does not exceed a predetermined intensity threshold.

14. The method of claim 1 wherein said eliminating includes eliminating anti-Stokes shifted inelastically scattered photons and said collecting is of Stokes-shifted inelastically scattered photons.

15. An apparatus for determining the composition of a sample comprising:

a repetitive source of pulsed light at a source wavelength;

a chamber for receiving the sample;

a probe for directing the pulsed light onto the sample and collecting the photons scattered by the sample;

a controllable photon filter receiving the collected photons and substantially eliminating photons not within a selectable frequency band defined between a first selectable lower frequency and a second selectable higher frequency, the photon filter substantially eliminating photons at the source wavelength;

an electrical filter having an intensity threshold;

a photon counting sensor for receiving Raman-shifted inelastically scattered photons from said photon filter and providing a plurality of electrical signals each in response to a different one of the corresponding plurality of received photons, said sensor further counting only the photons within the frequency band having corresponding electrical signals that exceed the intensity threshold of the electrical filter; and

a controller having a plurality of memory bins and being operably connected to said source, said filter, and said sensor;

wherein said controller receives the count of photons from a first pulse, stores the count as a first count signal in a first memory bin associated with the first frequency band.

16. The apparatus of claim 15 wherein said photon filter is an electronically controllable monochromator.

17. The apparatus of claim 15 wherein the count signal comprises the counting of individual photons as a function of time.

18. The apparatus of claim 15 wherein the count signal is a natural number.

19. The apparatus of claim 15 wherein the count signal is acquired during a period of summation, and the period ends before the receipt of a statistically significant quantity of fluorescence photons or phosphorescence photons on said sensor.

20. The apparatus of claim 19 wherein said sensor has a rise time and a peak in response to receiving a photon, and the period of summation ends before the peak.

21. The apparatus of claim 19 wherein said sensor has a rise time in response to receiving a photon, and the period of summation ends during the rising period.

22. The apparatus of claim 19 wherein the period of summation is triggered by the receipt of photons by the sensor.

23. The apparatus of claim 15 wherein said source is a monochromatic Q switched laser.

24. The apparatus of claim 23 wherein said laser emits light having a wavelength greater than about 500 nanometers and less than about 600 nanometers.

25. The apparatus of claim 15 wherein said probe includes a first optical path for providing the light onto the sample and a second optical path for collecting the scattered photons, the second optical path including a long-pass filter.

26. The apparatus of claim 15 wherein said source includes a beam splitter, and the pulsed signal is a split portion of the pulse of light.

27. The apparatus of claim 26 wherein said controller receives a split portion of the pulse of light, said controller beginning a period of summation corresponding to receiving the split portion of light, the count signal being acquired during the period of summation.

28. The apparatus of claim 15 wherein the pulsed signal corresponds to the start of the pulse, said controller being operably coupled to said source and receiving the pulsed signal, said controller beginning a period of summation corresponding to receiving the pulsed signal, the count signal being acquired during the period of summation.

29. The apparatus of claim 15 wherein the count signal is acquired during a period of summation, the pulse of light has a time width, and the period of summation is greater than about four times the time width of the pulse.