Raman spectrometer having interferometer with optical substraction filters

• US 5,247,343 A
• Filed: 11/01/1991
• Issued: 09/21/1993
• Est. Priority Date: 11/01/1991
• Status: Expired due to Term

• Current Assignee: Thermo Nicolet Corporation (Thermo Fisher Scientific Incorporated)
• Original Assignee: Nicolet Instrument Corporation (Thermo Fisher Scientific Incorporated)
• Inventors: Burch, Robert V.
• Primary Examiner(s): Turner, Samuel A.
• Application Number:
  US07/786,521
• Time in Patent Office: 690 Days
• Field of Search: 356/346, 356/352, 356/301
• US Class Current: 356/451
• CPC Class Codes: G01J 2003/1213 Filters in general, e.g. dichroic, band
• CPC Class Codes: G01J 3/44 Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
• CPC Class Codes: G01J 3/453 by correlation of the amplitudes

Abstract

A spectrometer for Raman spectrometry has a radiation source which provides a beam of radiation directed onto a sample, sample collection optics which directs the radiation from the sample as an input beam into an interferometer, the output beam of the interferometer being focused onto a detector, and filters interposed in the input and output beams of the interferometer. The filters are preferably holographic notch filters. Optical subtraction occurring in the interferometer as a result of the filters provides enhanced attenuation of the Rayleigh line of the reflected radiation while substantially passing the Raman lines, with the two filters achieving attenuation of the Rayleigh line equivalent to that obtained by several comparable filters stacked together.

Claims

1. Apparatus for Raman spectrometry comprising:

(a) a source of a beam of electromagnetic radiation at a selected wavelength suitable for Raman spectrometry and means for directing the beam from the source onto a sample;

(b) sample collection optics means for collecting the radiation reflected from the sample into a beam;

(c) an interferometer mounted to receive the beam from the sample collection optics means as its input beam and to provide a modulated output beam;

(d) a detector capable of detecting the wavelengths of the radiation reflected from the sample, and optics means for focusing the output beam from the interferometer onto the detector;

(e) a first filter interposed in the input beam to the interferometer at a position adjacent to the interferometer and a second filter interposed in the output beam from the interferometer at a position adjacent to the interferometer, the filters constructed to provide substantial attenuation of the wavelength of the Rayleigh line reflected from the sample while substantially passing the Raman lines reflected from the sample, the two filters arranged to provide optical subtraction in the interferometer of wavelengths at the Rayleigh line.

2. The apparatus of claim 1 wherein the filters comprise holographic notch filters.

3. The apparatus of claim 2 wherein the interferometer is a Michelson interferometer.

4. The apparatus of claim 2 including means for mounting the holographic notch filter in the input beam to allow tilting of the filter with respect to the input beam of the interferometer.

5. The apparatus of claim 2 including means for mounting the first holographic notch filter for tilting with respect to the input beam and means for mounting the second holographic notch filter for selective tilting with respect to the output beam of the interferometer.

6. A method of filtering the Rayleigh line of the radiation reflected from a sample which is collected and passed as the input beam to an interferometer, wherein the output beam of the interferometer is passed to and focused on a detector, comprising the steps of:

(a) interposing a notch filter in the input beam of the interferometer having an attenuation notch centered approximately at the Rayleigh line of the reflected radiation from the sample; and

(b) interposing a notch filter in the output beam of the interferometer having an attenuation notch centered approximately at the Rayleigh line of the reflected radiation, wherein the two filters are arranged at positions adjacent to the interferometer to provide optical subtraction in the interferometer of wavelengths at the Rayleigh line.

7. The method of claim 6 wherein the notch filters comprise holographic notch filters.

8. The method of claim 7 further including the step of tilting at least one of the holographic notch filters to tune the position of the notch with respect to the Rayleigh line of the reflected radiation.

9. The method of claim 6 including the step of tilting at least one of the notch filters to tune the position of the notch with respect to the Rayleigh line of the reflected radiation.