Method of polarimetry and method of urinalysis using the same

• US 6,620,622 B1
• Filed: 06/27/2000
• Issued: 09/16/2003
• Est. Priority Date: 06/29/1999
• Status: Expired due to Fees

• Current Assignee: Matsushita Electric Industrial Company Limited (Panasonic Holdings Corporation)
• Original Assignee: Matsushita Electric Industrial Company Limited (Panasonic Holdings Corporation)
• Inventors: Kawamura, Tatsurou
• Primary Examiner(s): Warden, Jill
• Assistant Examiner(s): CROSS, LATOYA I
• Application Number:
  US09/604,406
• Time in Patent Office: 1,176 Days
• Field of Search: 436/164, 356/364, 356/367, 356/368, 250/225
• US Class Current: 436/164
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence

Abstract

According to the present invention, in a polarimetry for allowing a light to be incident upon a specimen with a spontaneous optical active substance, a polarized light is allowed to be incident upon the specimen while micro-vibrating the plane of vibration; a component having a specific plane of vibration is detected out of the polarized light through the specimen; a component with a certain angular frequency is extracted; and an angle of rotation attributed to the specimen is calculated based on 3 or more groups of data including a relative angle formed between the plane of vibration of the light incident upon the specimen and the plane of vibration of the light, and an intensity of the component with the angular frequency obtained at the relative angle. Consequently, the influence of noises mixed due to bubbles, particles and the like can be eliminated, thereby achieving a stable and highly accurate measurement in a shorter time.

Claims

1. A method of polarimetry for allowing a light to be incident upon a specimen to be detected containing a spontaneous optical active substance, and determining an optical rotation attributed to said spontaneous optical active substance when said light transmits through said specimen, comprising the steps of:

(a) allowing a polarized light having a known plane of vibration to be incident upon said specimen while micro-vibrating said plane of vibration by a modulation signal with an angular frequency of ω

;

(b) detecting a component having a specific plane of vibration out of said polarized light transmitted through said specimen by a photosensor;

(c) extracting a component with an angular frequency of ω

out of an output signal from said photosensor by phase sensitive detection using said modulation signal as a reference signal; and

(d) calculating an angle of rotation attributed to said specimen based on 3 or more groups of data including a relative angle formed between a plane of vibration of said light incident upon said specimen and said specific plane of vibration of the light to be detected by said photosensor, and an intensity of said component with an angular frequency of ω

obtained at said relative angle.

2. The method of polarimetry in accordance with claim 1, wherein in said step (a), said relative angle is varied by continuously rotating the plane of vibration of said polarized light incident upon said specimen.

3. The method of polarimetry in accordance with claim 1, wherein in said step (a), said relative angle is varied by discretely changing the plane of vibration of said polarized light incident upon said specimen.

4. The method of polarimetry in accordance with claim 1, wherein in said step (d), a linear regression formula is formed based on said data by using said relative angle as a criterion variable and using the intensity of said component with an angular frequency of ω

as a dependent variable, and an angle of rotation attributed to said specimen is calculated based on the regression formula obtained.

5. The method of polarimetry in accordance with claim 1, wherein in said step (a), said relative angle is varied by rotating the plane of vibration of said polarized light incident upon said specimen by the optical Faraday effect.

6. The method of polarimetry in accordance with claim 5, wherein in said step (d), a linear regression formula is formed based on said data by using a magnitude of a magnetic field for obtaining said relative angle or a current amount for generating said magnetic field as a criterion variable, and using the intensity of said component with an angular frequency of ω

as a dependent variable, and an angle of rotation attributed to said specimen is calculated based on the regression formula obtained.

11. The method of polarimetry in accordance with claim 4, wherein in said step (d), said regression formula is calculated by using a least squares method.

12. The method of polarimetry in accordance with claim 4, wherein step (d) comprises a step of estimating the measurement to be effective when reliability of said regression formula is higher than a predetermined value.

13. The method of polarimetry in accordance with claim 12, wherein a sum of squares of residuals S_E, a value D obtained by dividing said sum of squares of residuals S_E by the sum of squares of the intensity values of said component with an angular frequency of ω

, which is obtained by substituting data corresponding to the criterion variable of said regression formula, or a correlation coefficient R shown in the following formulae is used as criterion evaluation of said reliability;

$\begin{array}{c}{S}_E=\underset{i=1}{\overset{n}{\sum <br><br>}}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\left\{Y_i-\left(a+{\mathrm{bX}}_i\right)\right\}}^2\\ D=\frac{S_E}{\underset{i=1}{\overset{n}{\sum <br><br>}}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\left(a+{\mathrm{bX}}_i\right)}^2}<br><br><br><br>R=\frac{\underset{i=1}{\overset{n}{\sum <br><br>}}<br><br>\text{\hspace{1em}<br><br>}<br><br>\left[\left(X_i-\stackrel{\_}{X}\right)\times <br><br>\left(Y_i-\stackrel{\_}{Y}\right)\right]}{\sqrt{\underset{i=1}{\overset{n}{\sum <br><br>}}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\left(X_i-\stackrel{\_}{X}\right)}^2\times <br><br>\underset{i=1}{\overset{n}{\sum <br><br>}}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\left(Y_i-\stackrel{\_}{Y}\right)}^2}}\end{array}$

where the regression formula is expressed as Y=a+bX, X_i (i=1 to n) is the data for the criterion variable “

X”

of the regression formula, Y_i (i=1 to n) is the data for the dependent variable “

Y”

of the regression formula, {overscore (X)} is the mean value of X_i, and {overscore (Y)} is the mean value of Y_i.

14. A method of urinalysis for detecting a concentration of a spontaneous optical active substance in a urine by using said method of polarimetry in accordance with claim 1.

15. The method of polarimetry in accordance with claim 6, wherein in said step (d), said regression formula is calculated by using a least squares method.

17. The method of polarimetry in accordance with claim 6, wherein step (d) comprises a step of estimating the measurement to be effective when reliability of said regression formula is higher than a predetermined value.

7. A method of polarimetry for allowing a light to be incident upon a specimen to be detected containing a spontaneous optical active substance and a magneto-optical active substance and applying a magnetic field to said specimen, thereby rotating a plane of vibration of said light transmitting through said specimen by an optical Faraday effect, and determining an optical rotation attributed to said spontaneous optical active substance when said light transmits through said specimen based on a magnitude of rotation of said light caused by said magnetic field, comprising the steps of:

(a) allowing a polarized light having a known plane of vibration to be incident upon said specimen while micro-vibrating said plane of vibration by a modulation signal with an angular frequency of ω

;

(b) detecting a component having a specific plane of vibration out of said polarized light transmitted through said specimen by a photosensor;

(c) extracting a component with an angular frequency of ω

out of an output signal from said photosensor by phase sensitive detection using said modulation signal as a reference signal; and

(d′

) calculating an angle of rotation attributed to said specimen based on 3 or more groups of data including a magnitude of said magnetic field and an intensity of said component with an angular frequency of w obtained at said magnitude of said magnetic field.

8. The method of polarimetry in accordance with claim 7, wherein in said step (a), said plane of vibration of said light is continuously rotated by the optical Faraday effect.

9. The method of polarimetry in accordance with claim 7, wherein in said step (a), said plane of vibration of said light is discretely rotated by the optical Faraday effect.

10. The method of polarimetry in accordance with claim 7, wherein in said step (d′

), a linear regression formula is formed based on said data by using the magnitude of said magnetic field or a current amount for generating said magnetic field as a criterion variable and using the intensity of said component with an angular frequency of ω

as a dependent variable, and an angle of rotation attributed to said specimen is calculated based on the regression formula obtained.

16. The method of polarimetry in accordance with claim 10, wherein in said step (d′

), said regression formula is calculated by using a least squares method.

18. The method of polarimetry in accordance with claim 10, wherein step (d′

) comprises a step of estimating the measurement to be effective when reliability of said regression formula is higher than a predetermined value.

19. A method of urinalysis for detecting a concentration of a spontaneous optical active substance in a urine by using said method of polarimetry in accordance with claim 7.