Optical activity detector for use with optically active compounds

• US 5,822,067 A
• Filed: 10/31/1997
• Issued: 10/13/1998
• Est. Priority Date: 01/31/1996
• Status: Expired due to Fees

• Current Assignee: Gary W. Yanik
• Original Assignee: Gary W. Yanik
• Inventors: Yanik, Gary W.
• Primary Examiner(s): Rosenberger, Richard A.
• Application Number:
  US08/962,017
• Time in Patent Office: 347 Days
• Field of Search: 356/364, 356/365, 356/366, 356/367, 356/368
• US Class Current: 356/368
• CPC Class Codes: G01N 21/05 Flow-through cuvettes G01N21/09 takes precedence; handling fluid samples G01N1/10
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence

Abstract

An improved optical rotation detector for detecting optically active molecular compounds in a sample solution using: a laser diode with the beam passing through an optical fiber or lens to improve its quality, a reference oscillator at frequency f, a first polarizer, a specially constructed flow cell to minimize mechanical birefringence and leaking in the cell'"'"'s optical windows, a second polarizer, and an improved detection scheme. The detection scheme includes a first and second photodetector for sensing first and second signals, where the first signal is light passed through the second polarizer and the second signal is light reflected off the second polarizer. A compensator circuit low pass filters the signals, inverts one signal and sums it with the other, and then notch filters off the undesired components to produce a compensated signal. The compensated signal then drives a lock-in amplifier which is driven by the reference oscillator to sense the amplitude modulated f frequency signal. This compensated signal indicates the optical activity of the sample, yet is immune to laser power fluctuations.

Claims

1. An improved optical rotation detector with components fixedly mounted and aligned on an operational bench, said components comprised of:

(I) a laser diode based light source system with a means selected from the group consisting of a fiber optic cable, a cylindrical focusing lens or multiple lenses and prisms for producing a near-gaussian laser beam;

(ii) a first glan-Thompson polarizing prism to improve the linear polarization ratio of said laser beam to at least 1000;

1;

(iii) a Faraday rotator utilizing a Terbium Gallium Garnet rod for affecting the polarization of said beam, said rotator being driven by an alternating current source, or reference oscillator, at frequency f;

(iv) a flow cell for directing a solvent and sample flow through said linearly polarized beam, said flow cell having a flow cell body with a central cavity;

a pair of sealing washers selected from the group consisting of chlorotrifluoroethylene, fluorinated ethylene propylene and tetrafluoroethylene a pair of synthetic fused silica hermetically sealed optical windows;

a pair of endcap means for containing said sealing and optical windows, each endcap means having mounting and alignment holes and an attachment means for sealably attaching each said endcap means to each flow cell body end, wherein said endcap and attachment means provides an improved flow cell for passing said laser beam through an optically active substance with minimal mechanical birefringence;

(v) a second glan-Thompson polarizing prism which is oriented 90 degrees from said first polarizing means in its ability to transmit polarized light, wherein said second polarizing means attenuates transmission of most of the polarized laser beam;

(vi) a photodetector for detecting a signal consisting of amplitude modulated light which is transmitted through said second polarizing means;

(vii) a compensator circuitry means for producing a compensated signal which attenuates contributions from frequencies other than f; and

(viii) a phase sensitive detector, or lock-in amplifier, as driven by said f frequency oscillator, for sensing the amplitude modulation of the compensated signal at frequency f.

2. The improved optical rotation detector of claim 1, wherein said compensator circuitry means is used to filter out interference and noise contributions from frequencies other than f, said circuitry including low pass and notch filters for filtering said photodetector signal.

3. The improved optical rotation detector of claim 1, wherein said means for producing a near-gaussian laser beam is a length of optical fiber cable.

4. The improved optical rotation detector of claim 1, wherein said means for producing a near-gaussian laser beam includes a cylindrical focusing lens mounted underneath the hermetically sealed optical window containing endcap and on the emitting aperture of the laser diode.

5. The improved optical rotation detector of claim 1, wherein said endcaps include a centralized donut shaped island with a surrounding moat wherein said optical windows are clamped to said endcaps and attached via glue being injected into said moat, wherein said clamps are removed after said glue hardens.

6. The improved optical rotation detector of claim 1, wherein said precision mounting fixture for said flow cell includes a "V" block mount for interfacably cradling said cylindrical flow cell and a top clamping bar which holds said flow cell in place and attaches to said mount, with said interface between said "V" block and said flow cell being machined so that a flow cell can be removed and replaced without further alignment of said detector components.

7. The improved optical rotation detector of claim 1, wherein said components are so ruggedly mounted and prealigned as to provide a system which can be operational for detecing samples within approximately 30-45 minutes for deployment.

8. The optical rotation detector of claim 1, wherein said pair of endcap means is formed from polyetheretherketone.

9. An improved optical rotation detector with components fixedly mounted and aligned on an operational bench, said components comprised of:

(I) a laser light source system with a means for producing a near-gaussian laser beam;

(ii) a first polarizing means to improve the linear polarization ratio of said laser beam to at least 1000;

1;

(iii) a Faraday rotator for affecting the polarization of said beam, said rotator being driven by an alternating current source, or reference oscillator, at frequency f;

(iv) a flow cell having a pair of hermetically sealed optical windows, said flow cell for directing a solvent and sample flow through said linearly polarized beam;

(v) a second polarizing means which is oriented 90 degrees from said first polarizing means in its ability to transmit polarized light, wherein said second polarizing means attenuates transmission of most of the polarized laser beam;

(vi) a first photodetector for detecting a signal consisting of amplitude modulated light which is transmitted through said second polarizing means, (vii) a compensator circuitry means for producing a compensated signal which attenuates contributions from frequencies other than f; and

(viii) a phase sensitive detector, or lock-in amplifier, as driven by said f frequency oscillator, for sensing the amplitude modulation of the compensated signal at frequency f;

(ix) a second photodetector positioned to detect light reflected from the entrance of said second polarizing means, and said compensator circuitry means is used to subtract out amplitude fluctuations from the laser light source and filter out interference and noise contributions from frequencies other than f, said circuitry including;

(I) at least one low pass filter for filtering said first and second photodetector signals;

(ii) a summing device for operationally subtracting said first and second photodetector signals; and

(iii) at least one notch filter for filtering unwanted signal components from the result.

10. The improved optical rotation detector of claim 9, wherein said compensator circuitry means is comprised of operational amplifiers configured to filter and process said photodetector signals.

11. The improved optical rotation detector of claim 10, wherein said compensator circuitry further includes at least one variable resistive device connected to allow controlled balancing of said subtraction operation of said first and second photodetector signals.

12. An improved optical rotation detector comprised of:

a laser diode light source system;

a first polarizing means to improve the linear polarization ratio of said laser beam;

a Faraday rotator;

a flow cell;

a second polarizing means which is oriented 90 degrees from said first polarizing means in its ability to transmit polarized light, wherein said second polarizing means attenuates transmission of most of the polarized laser beam;

a photodetector for detecting a signal consisting of amplitude modulated light which is transmitted through said second polarizing means;

a phase sensitive detector, or lock-in amplifier, as driven by said f frequency oscillator, for sensing the f frequency signal;

the improvement comprising;

(i) a means attached to said laser diode for producing a near-gaussian laser beam;

(ii) a cylindrically shaped flow cell means constructed to minimize mechanical birefringence and dispersion of transmitted light;

(iii) a machined "V"-block mount for precision alignment of said cylindrically shaped flow cell;

(iv) a second photodetector positioned to detect a signal consisting of laser light reflected from the entrance of said second polarizing means;

(v) compensator circuitry means for producing a compensated signal with attenuation of the interference and noise contributions from frequencies other than f.

13. The improved optical rotation detector of claim 12, wherein said compensator circuitry means consists of

(i) at least one low pass filter for filtering said first and second photodetector signals;

(ii) a summing device for operationally subtracting said first and second photodetector signals; and

(iii) at least one notch filter for filtering unwanted signal components from the summed result.

14. An improved optical rotation detector with components fixedly mounted and aligned on an operational bench, said components comprised of:

(I) a laser diode based light source system with a means selected from the group consisting of a fiber optic cable, a cylindrical focusing lens or multiple lenses and prisms for producing a near-gaussian laser beam;

(ii) a first glan-Thompson polarizing prism to improve the linear polarization ratio of said laser beam to at least 1000;

1;

(iii) a Faraday rotator utilizing a Terbium Gallium Garnet rod for affecting the polarization of said beam, said rotator being driven by an alternating current source, or reference oscillator, at frequency f;

(iv) a replaceable, cylindrically shaped flow cell means mounted on a precisioned mounting fixture, said flow cell being used for directing a solvent and sample flow through said linearly polarized beam, said flow cell means utilizing a fused quartz tube through its longitudinal center, said tube having a capillary as the main bore with said capillary being sized sufficiently larger than said beam so as to minimize scattering and subsequent depolarization of said beam;

(v) a second glan-Thompson polarizing prism which is oriented 90 degrees from said first polarizing means in its ability to transmit polarized light, wherein said second polarizing means attenuates transmission of most of the polarized laser beam;

(vi) a detector means for detecting said transmitted light; and

;

(v) compensator means for processing said detected signals.

15. The improved optical rotation detector of claim 14, wherein said detector means includes a photodetector and said compensator means includes circuitry for filtering unwanted components from said detected signal.

16. The improved optical rotation detector of claim 15, wherein said detector means includes a first and second photodetector, said compensator means including circuitry for filtering off unwanted components from said detected signals, and circuitry for subtracting said photodetector first signal from said second signal.