High resolution low noise optical polarimeter

• US 5,477,327 A
• Filed: 12/15/1993
• Issued: 12/19/1995
• Est. Priority Date: 12/15/1993
• Status: Expired due to Fees

• Current Assignee: Bergman Research Group, Inc.
• Original Assignee: Bergman Research Group, Inc.
• Inventors: Bergman, John D.
• Primary Examiner(s): Rosenberger, Richard A.
• Assistant Examiner(s): VIERRA EISENBERG, JASON D
• Application Number:
  US08/168,119
• Time in Patent Office: 734 Days
• Field of Search: 356/364, 356/367, 356/368, 356/332, 356/333, 356/335, 128/633, 128/664
• US Class Current: 356/367
• CPC Class Codes: G01J 4/04 Polarimeters using electric detection means G01J4/02 takes precedence
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence

Abstract

Two linearly polarized beams of monochromatic laser light are amplitude modulated with low frequency sinusoids. The first laser is modulated with a sinusoid 90° out of phase from the second laser. The two beams of laser light have their polarization axis fixed and separated by 45°. These two beams are then collimated and combined into one composite beam using simple optics. This composite beam is then allowed to pass through an optically active substance of a calibrated path length. The laser radiation exiting the sample is passed through a optical notch pass filter, reducing any signal that may be present from any polarized ambient light by passing only light of the laser'"'"'s frequency. The composite beam then passes into a beam splitting polarizing cube. This cube has the function of separating the beam into two orthogonal polarization components. The two beams of light exiting the cube are focused onto silicon photoelectric detectors. The cube is oriented such that one of the cube'"'"'s transmission axis is aligned to coincide with the polarization axis of one of the lasers. The current from the detectors is converted into a voltage. The resulting detector voltages are then AC coupled to remove any DC component of the voltage, leaving only signal. These voltages are then subtracted using an instrumentation grade operational amplifier. The subtracted signal is phase shifted in direct proportion to solution concentration. Setting the ratio of laser signal amplitudes greater than unity can further amplify this phase shift to produce high instrument sensitivity.

Claims

1. A polarimeter comprising in combination:

first and second means for emitting respective first and second amplitude modulated linearly polarized beams of monochromatic light having a polarization axis, said first amplitude modulated linearly polarized beam of monochromatic light with said polarization axis non-collinear with said polarization axis of said second amplitude modulated linearly polarized beam of monochromatic light, said amplitude modulation including imposition of a sinusoid on both said beams, said first amplitude modulated linearly polarized beam of monochromatic light modulated with said imposed sinusoid out of phase from said imposed sinusoid on said second amplitude modulated linearly polarized beam of monochromatic light;

an optical path including a transparent, optically active sample of known length in said optical path;

means for combining said first and second amplitude modulated linearly polarized beams of monochromatic light and emitting said combined beam into said optical path;

means for separating said combined beam into two orthoganal polarization components in said optical path;

first and second photoelectric detectors for detecting said two orthoganal polarization components and emitting respective signals proportional to said components;

means for subtracting said respective signals from said first and second photoelectric detectors for removing common mode noise and obtaining a received amplitude modulated sinusoid; and

,

means for comparing phase of said received amplitude modulated sinusoid with phase of said imposed sinusoids on respective first and second amplitude modulated linearly polarized beams of monochromatic light obtaining a phase difference proportional to polarization rotation within said sample.

2. A polarimeter according to claim 1 and further wherein:

said means for separating said combined beam into said two orthogonal polarization components includes a beam splitting polarizing cube having a transmission axis.

3. A polarimeter according to claim 2 and further wherein:

said means for combining said first and second amplitude modulated linearly polarized beams of monochromatic light includes simple optics having spherical lenses.

4. A polarimeter according to claim 2 and further wherein:

said beam splitting polarizing cube is oriented with respect to said first and second amplitude modulated linearly polarized beams of monochromatic light such that said beam splitting polarizing cube having a transmission axis is aligned to coincide with said polarization axis of one of said amplitude modulated linearly polarized monochromatic light beams.

5. A polarimeter according to claim 1 and further wherein:

said first amplitude modulated linearly polarized beam of monochromatic light has said polarization axis offset 45°

from said polarization axis of said second amplitude modulated linearly polarized beam of monochromatic light.

6. A polarimeter according to claim 1 and further wherein:

means modulating said first and second amplitude modulated linearly polarized beams of monochromatic light include said imposed sinusoids of a frequency less than 100 Hz.

7. A polarimeter according to claim 1 and further including:

an optical notch filter in said optical path between said transparent, optically active sample and said photoelectric detectors for passing light only of said monochromatic light.

8. A polarimeter according to claim 1 and further including:

means for converting said respective signals from said first and second photoelectric detectors to electrical voltages.

9. A polarimeter according to claim 8 and further wherein:

said resulting detector voltages are AC coupled to remove any DC component of said voltage.

10. A polarimeter according to claim 1 and further wherein:

said means for subtracting said signals from said first and second photoelectric detectors constitutes an instrumentation grade operational amplifier.

11. A polarimeter according to claim 1 and further including:

means for setting an amplitude ratio of said imposed sinusoids on said first and second amplitude modulated linearly polarized beams of monochromatic light greater than unity whereby said means for comparing further amplifies said phase difference to produce high instrument sensitivity.

12. A process for polarimetry comprising the steps of:

emitting respective first and second amplitude modulated linearly polarized beams of monochromatic light having a polarization axis, said first amplitude modulated linearly polarized beam of monochromatic light having said polarization axis non-collinear with said polarization axis of said second amplitude modulated linearly polarized beam of monochromatic light, said amplitude modulation including imposition of a sinusoid on both said beams;

said first amplitude modulated linearly polarized beam of monochromatic light modulated with said imposed sinusoid out of phase from said imposed sinusoid on said second amplitude modulated linearly polarized beam of monochromatic light;

combining said first and second amplitude modulated linearly polarized beams of monochromatic light;

emitting said combined beam into an optical path including a transparent optically active sample of known length in said optical path;

placing means for separating said combined beam into two orthoganal polarization components in said optical path;

providing first and second photoelectric detectors for detecting said two orthoganal polarization components and emitting a signal proportional to said components;

subtracting said signals from said first and second photoelectric detectors for removing common mode noise and obtaining a received amplitude modulated sinusoid; and

,

comparing phase of said received amplitude modulated sinusoid with phase of said imposed sinusoids on said respective first and second amplitude modulated linearly polarized beams of monochromatic light obtaining a phase difference proportional to polarization rotation within said sample.

13. A process for polarimetry according to claim 12 including the further steps of:

setting an amplitude ratio of said imposed sinusoids on said first and second amplitude modulated linearly polarized beams of monochromatic light greater than unity whereby said process further amplifies said phase difference to produce high instrument sensitivity.

14. A process for polarimetry according to claim 12 and including the further steps of:

emitting said first amplitude modulated linearly polarized beam of monochromatic light with said polarization axis offset 45°

from said polarization axis of said second amplitude modulated linearly polarized beam of monochromatic light.

15. A process for polarimetry according to claim 12 including the further steps of:

modulating said first and second amplitude modulated linearly polarized beams of monochromatic light with said imposed sinusoids that are 90°

out of phase.

16. A process for polarimetry according to claim 15 including the further steps of:

modulating said first and second amplitude modulated linearly polarized beams of monochromatic light with said imposed sinusoids of a frequency less than 100 Hz.

17. A process for polarimetry according to claim 12 and further wherein:

said combining said first and second amplitude modulated linearly polarized beams of monochromatic light constitutes providing simple optics having spherical lenses; and

,

routing said beams through said simple optics.

18. A process for polarimetry according to claim 12 including the further steps of:

providing an optical notch filter between said sample and said photoelectric detectors for passing light only of said monochromatic light.

19. A process for polarimetry according to claim 12 and further wherein:

said separating said combined beam constitutes orienting a beam splitting polarizing cube with respect to said first and second light beams such that said beam splitting polarizing cube has a transmission axis aligned to coincide with said polarization axis of one of said first and second amplitude modulated linearly polarized beams of monochromatic light; and

routing said beams through said beam splitting polarizing cube.

20. A process for polarimetry according to claim 12 including the further steps of:

converting said signal from said first photoelectric detectors to electrical voltages.

21. A process for polarimetry according to claim 20 including the further steps of:

AC coupling said signal from said first and second photoelectric detectors to remove any DC component of said voltage.

22. A process for polarimetry according to claim 12 and further wherein:

said subtracting said signals from said first and second photoelectric detectors constitutes providing an instrumentation grade operational amplifier; and

,

routing said signals through said instrumentation grade operational amplifier.