Nonlinear vibrational microscopy

• US 6,108,081 A
• Filed: 04/19/1999
• Issued: 08/22/2000
• Est. Priority Date: 07/20/1998
• Status: Expired due to Term

• Current Assignee: Battelle Memorial Institute
• Original Assignee: Battelle Memorial Institute
• Inventors: Holtom, Gary R., Xie, Xiaoliang Sunney, Zumbusch, Andreas
• Primary Examiner(s): Evans, F. L.
• Application Number:
  US09/294,834
• Time in Patent Office: 491 Days
• Field of Search: 356/301, 356/317, 356/318
• US Class Current: 356/301
• CPC Class Codes: G01J 3/44 Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
• CPC Class Codes: G01N 2021/653 Coherent methods [CARS]
• CPC Class Codes: G01N 2021/656 Raman microprobe

Abstract

The present invention is a method and apparatus for microscopic vibrational imaging using coherent Anti-Stokes Raman Scattering or Sum Frequency Generation. Microscopic imaging with a vibrational spectroscopic contrast is achieved by generating signals in a nonlinear optical process and spatially resolved detection of the signals. The spatial resolution is attained by minimizing the spot size of the optical interrogation beams on the sample. Minimizing the spot size relies upon a. directing at least two substantially co-axial laser beams (interrogation beams) through a microscope objective providing a focal spot on the sample; b. collecting a signal beam together with a residual beam from the at least two co-axial laser beams after passing through the sample; c. removing the residual beam; and d. detecting the signal beam thereby creating said pixel. The method has significantly higher spatial resolution then IR microscopy and higher sensitivity than spontaneous Raman microscopy with much lower average excitation powers. CARS and SFG microscopy does not rely on the presence of fluorophores, but retains the resolution and three-dimensional sectioning capability of confocal and two-photon fluorescence microscopy. Complementary to these techniques, CARS and SFG microscopy provides a contrast mechanism based on vibrational spectroscopy. This vibrational contrast mechanism, combined with an unprecedented high sensitivity at a tolerable laser power level, provides a new approach for microscopic investigations of chemical and biological samples.

Claims

1. A method of creating a pixel, or spatially resolved image element, from at least two laser beams having first and second frequencies, the at least two laser beams spatially coincident on a sample producing a signal beam of a new frequency, the method comprising the steps of:

a. directing the at least two laser beams in a substantially co-axial relationship through a lens providing a common focal spot on the sample;

b. collecting the signal beam together with at least two residual beams from the at least two laser beams after passing through the sample;

c. removing the at least two residual beams; and

d. detecting the signal beam thereby creating said pixel.

2. The method as recited in claim 1, wherein said lens is an objective lens.

3. The method as recited in claim 2, further comprising the step of expanding the at least two laser beams for filling a back aperture of the objective lens.

4. The method as recited in claim 1, wherein said producing is with coherent anti-Stokes Raman scattering wherein a frequency difference between said at least two laser beams is in resonance with a vibrational frequency of the sample.

5. The method as recited in claim 4, wherein said at least two laser beams have wavelengths in the near infrared.

6. The method as recited in claim 1, wherein said producing is with sum frequency generation wherein a frequency of one of said at least two laser beams is in resonance with a molecular vibration of the sample.

7. The method as recited in claim 1, further comprising geometrically scanning said sample with respect to said common focal spot and obtaining a plurality of pixels and generating an image therefrom.

8. The method as recited in claim 1, further comprising scanning the common focal spot over the sample, by steering the at least two laser beams.

9. The method as recited in claim 1, further comprising changing the Raman vibrational frequency separation of at least two of the at least two pulsed laser beams for obtaining a vibrational property of the sample.

10. The method as recited in claim 1, wherein said vibrational frequency separation is less than 4000 cm^-1.

11. The method as recited in claim 1, further comprising the step of selecting a pulse width for the at least two laser beams, said pulse width infinite (continuous wave).

12. The method as recited in claim 1, further comprising the steps of

a. selecting a finite pulse width and pulsing at least one of said at least two laser beams with said finite pulse width;

and

b. causing at least one of the at least two laser beams to temporally overlap the pulse of finite pulse width.

13. The method as recited in claim 12, wherein said pulse width is less than infinite, but longer than 10 femtoseconds.

14. The method as recited in claim 12, wherein said pulse width is shorter than 1 picosecond.

15. A system for creating a pixel from at least two laser beams having first and second frequencies, the at least two laser beams spatially coincident on a sample producing a signal beam of a third frequency, the system comprising:

a. an optical director for directing the at least two laser beams in a substantially co-axial relationship through a microscope objective providing a focal spot on the sample

b. a lens for collecting the signal beam together with at least two residual beams from the at least two laser beams after passing through the sample;

c. a blocking filter for removing the at least two residual beams; and

d. a detector for detecting the signal beam thereby creating said pixel.

16. The system as recited in claim 15, wherein said lens is an objective lens.

17. The system as recited in claim 16, further comprising a telescope for expanding the at least two laser beams for filling a back aperture of the objective lens.

18. The system as recited in claim 15, wherein said signal beam is obtained from a frequency difference or a sum frequency.

19. The system as recited in claim 15, further comprising a scanner for geometrically scanning said sample with respect to said at least two laser beams and obtaining a plurality of pixels and generating an image therefrom.

20. The system as recited in claim 15, further comprising scanning the common focal spot over the sample, by steering the at least two laser beams.

21. The system as recited in claim 15, further comprising a separator control for changing the difference in frequency between separation of at least two of the at least two pulsed laser beams for obtaining a vibrational property of the sample.

22. The system as recited in claim 15, wherein said difference in frequency is less than 4000 cm^-1.

23. The system as recited in claim 15, wherein a pulse width of said at least two laser beams is less them is less than infinite, but longer than 1 nanosecond.

24. The system as recited in claim 23, wherein said pulse width is from about 1 nanosecond to 1 picosecond.

25. The system as recited in claim 23, wherein said pulse width is shorter than 1 picosecond.

26. An apparatus for coherent anti-Stokes Raman scattering microscopic imaging, comprising:

a. a pump wave laser that is a Ti;

S mode-locked laser amplified with a regenerative amplifier for generating a pump wave;

b. a second wave laser that is an optical parametric oscillator having a crystal of KNbO3 amplified with a portion of the pump wave;

c. at least one telescope for adjusting the size and collimation of the laser beams, and a dichroic beam combiner for making them substantially coaxial;

d. a microscope objective lens for focusing said pump wave laser and said second wave laser onto a sample; and

e. a blocking filter that passes a detection signal to a detector.

27. A method of creating a pixel with Coherent Anti-Stokes Raman scattering having at least two substantially co-axial pulsed laser beams separated by a Raman vibrational frequency coincident on a sample, wherein the frequency difference between the at least two co-axial pulsed laser beams corresponds to a vibrational molecular resonance of the sample, the method comprising the steps of:

a. directing the at least two co-axial pulsed laser beams through a microscope objective providing a focal spot on the sample;

b. collecting a pulsed signal beam together with a residual beams from the at least two co-axial pulsed laser beams after passing through the sample;

c. removing the residual beams; and

d. detecting the pulsed signal beam thereby creating said pixel.

28. The method as recited in claim 27, further comprising geometrically scanning said sample with respect to said pulsed signal beam and obtaining a plurality of pixels and generating an image therefrom.

29. The method as recited in claim 27, further comprising geometrically scanning said sample with respect to said common focal spot and obtaining a plurality of pixels and generating an image therefrom.

30. The method as recited in claim 27, further comprising scanning the common focal spot over the sample, by steering the at least two laser beams.

31. The method as recited in claim 27, further comprising changing the Raman vibrational frequency separation of at least two of the at least two pulsed laser beams for obtaining a vibrational property of the sample.

32. A system for creating a pixel with Coherent Anti-Stokes Raman scattering having at least two parallel pulsed laser beams separated by a Raman vibrational frequency coincident on a sample, wherein the frequency difference between the at least two parallel pulsed laser beams corresponds to a vibrational molecular resonance of the sample, the system comprising:

a. an optical director for directing the at least two parallel pulsed laser beams through a microscope objective providing a focal spot on the sample;

b. a collection lens for collecting a pulsed signal beam together with a residual beam from the at least two parallel pulsed laser beams after passing through the sample;

c. a blocking filter for removing the residual beam; and

d. a detector for detecting the pulsed signal beam thereby creating said pixel.

33. The system as recited in claim 32, further comprising a scanner for geometrically scanning said sample with respect to said pulsed signal beam and obtaining a plurality of pixels and generating an image therefrom.

34. The system as recited in claim 32, further comprising geometrically scanning said sample with respect to said common focal spot and obtaining a plurality of pixels and generating an image therefrom.

35. The system as recited in claim 32, further comprising scanning the common focal spot over the sample, by steering the at least two laser beams.

36. The system as recited in claim 32, further comprising a separator control for changing the Raman vibrational frequency separation of at least two of the at least two pulsed laser beams for obtaining a vibrational property of the sample.

37. A method of creating a pixel, or spatially resolved image element, from at least two laser beams having first and second frequencies, the at least two laser beams spatially coincident on a sample producing a signal beam of a new frequency, the method having the steps of:

a. directing the at least two laser beams through a lens providing a common focal spot on the sample;

b. collecting the signal beam together with at least two residual beams from the at least two laser beams after passing through the sample;

c. removing the at least two residual beams; and

d. detecting the signal beam thereby creating said pixel;

wherein the improvement comprises;

at least one of said at least two laser beams has a wavelength in the range of from deep red (0.7 micron) to near infrared (2 micron).

38. The method as recited in claim 37, wherein said at least two laser beams have wavelengths in the range of from deep red to near infrared.

39. The method as recited in claim 37, wherein said at least two laser beams are coaxial.

40. The method as recited in claim 39 wherein said at least two laser beams fill a back aperture of said lens thereby providing said common focal spot of a size of less than 10 micron.