IP Library › Granted Patent US 9,719,852
Granted Patent B2
US 9,719,852 · App. 14/711,582 · Granted Aug 1, 2017

System and method for compensating light source drift at different wavelengths with a single reference channel in a light measuring device

Inventor: Zhiling Xu (West Windsor, NJ)
Assignee: DATACOLOR HOLDING AG
G01J3/0254G01J3/10G01J3/28G01J2003/2866
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Quick Facts
Patent No.
US 9,719,852
App. No.
14/711,582
Granted
Aug 1, 2017
Kind
B2
Abstract

In accordance with a broad aspect of the present invention the system and method described are directed to correcting with a single reference channel thermally dependent spectrum shifts of a light source used with a spectrophotometer. In one embodiment of the system and method described, a light measuring device uses the measured light intensity values to generate a correction coefficient for use in correcting measured light from an object under analysis.

Claims (170)

1. A computer implemented method to compensate temperature induced light source drift in a spectrophotometer using a light measuring device having a processor, a memory, a light source configured to emit broad band light, a sample sensor configured to output a sample signal in response to light being incident upon the sensor, a reference sensor configured to output a reference signal in response to light being incident upon the reference sensor, and a calibration measurement application stored in the memory and executable by the processor, the method comprising the steps of:

emitting a plurality of flashes of light from the light source such that the light is incident on a reference target and a calibration target,

measuring, for each of the plurality of light flashes, the intensity of each wavelength of the light reflected off a calibration target using the sample sensor, and the intensity of the light reflected off a reference target using the reference sensor;

transforming the measured values into a compensation coefficient value based on the relationship between the sample sensor measurement and the reference sensor measurement at each wavelength;

obtaining a sample measurement of the intensity at different wavelengths of light reflected off of a sample under analysis with the sample sensor and a reference measurement of the intensity of light reflected off of the reference target;

generating a corrected sample measurement according to a compensation algorithm that incorporates the compensation coefficient; and

outputting the corrected sample signal.

2. The method of claim 1 , wherein the compensation algorithm is:

I

c

⁡

(

λ

)

=

I

⁡

(

λ

)

+

k

⁡

(

λ

)

*

[

I

⁡

(

λ

)

I

W

⁡

(

λ

)

]

*

(

T

1

-

T

0

)

where I(λ) is the measured sample signal at wavelength λ when the object is obtained, k(λ) is the transformed coefficient value at wavelength λ, T 1 is the measured reference channel signal when the object is measured, T 0 is a measured reference signal value obtained during the measuring step, I W (λ) is a measured sample signal value obtained during the measuring step and where I c (λ) is the corrected sample signal.

3. The method of claim 2 , wherein I W (λ) and T 0 are derived from the measurements obtained in the measuring step.

4. The method of claim 2 , wherein I W (λ) and T 0 are selected from among the values obtained in the measuring step.

5. The method of claim 2 , further comprising the step of:

generating a reflectance R(λ) value of the object based on I C (λ), according to the following:

R (λ)= I C (λ) R W (λ)/ I W (λ).

6. The method of claim 1 , wherein the transforming step includes performing a linear regression on the sample and reference signals at each wavelength to generate the compensation coefficient.

7. The method of claim 1 , where the light source is an LED.

8. The method of claim 1 , where the sample sensor is a spectrophotometer.

9. The method of claim 1 , where the light source is subject to thermally dependent spectrum shift.

10. The method of claim 1 , wherein the reference sensor is selected from a broadband sensor, a narrowband sensor, a single band sensor, or a multiband sensor.

11. The method of claim 1 , wherein the reference target is part of the inside surface of an integrating sphere.

12. A system for compensating thermally dependent light source drift in a spectrophotometer, the system comprising:

a. a spectrophotometer having a processor, a memory, a light source configured to emit broad-band light, a sample sensor configured to output a sample signal in response to light being incident upon the sensor, a reference sensor configured to output a reference signal in response to light being incident upon the reference sensor,

b. the processor of the spectrophotometer configured by code executing therein to implement the steps of:

emitting a plurality of flashes of light from the light source such that the light is incident on a reference target and a calibration target,

measuring for each of the plurality of light flashes, the intensity at each wavelength of the light reflected off a calibration target using the sample sensor and the intensity of the light reflected off a reference target using the reference sensor;

transforming the measured values into a compensation coefficient based on the relationship between the signal channel measurement and the reference channel measurement at each wavelength;

obtaining a sample measurement of the intensity at different wavelengths of light reflected off of a sample under analysis with the sample sensor and a reference measurement of the intensity of light reflected off of the reference target;

generating a corrected sample signal according to:

I

c

⁡

(

λ

)

=

I

⁡

(

λ

)

+

k

⁡

(

λ

)

*

[

I

⁡

(

λ

)

I

W

⁡

(

λ

)

]

*

(

T

1

-

T

0

)

where I(λ) is the measured sample signal at wavelength λ when the object is measured, k(λ) is the generated coefficient at wavelength λ, T 1 is the measured reference channel signal when the object is measured, T 0 is a reference signal value obtained from the measuring step, I W (λ) is a measured sample signal value obtained from the measuring step and where I c (λ) is the corrected sample signal; and

outputting the corrected sample signal.

13. The method of claim 12 , wherein I W (λ) and T 0 are the average values of the measurements obtained in the measuring step.

14. The method of claim 13 , further comprising the step of:

generating a reflectance R(λ) value of the object based on I C (λ), according to the following:

R (λ)= I C (λ) R W (λ)/ I W (λ).

15. The method of claim 12 , wherein I W (λ) and T 0 are selected from among the values obtained in the measuring step.

16. The method of claim 12 , wherein the transforming step includes performing a linear regression on the sample and reference signals at each wavelength to generate the compensation coefficient.

17. The method of claim 12 , where the light source is an LED.

18. The method of claim 12 , wherein in the reference target is an integrating sphere.

19. A system for compensating thermally dependent light source drift in a spectrophotometer, the system comprising:

a. a spectrophotometer having a processor, a memory, a light source configured to emit broad-band light, a sample sensor configured to output a sample signal in response to light being incident upon the sensor, a reference sensor configured to output a reference signal in response to light being incident upon the reference sensor,

b. the processor of the spectrophotometer configured by code executing therein to implement the steps of:

accessing a calibration coefficient from the memory;

obtaining a sample measurement of the intensity at different wavelengths of light reflected off of a sample under analysis with the sample sensor and a reference measurement of the intensity of light reflected off of the reference target;

generating a corrected sample signal according to:

I

c

⁡

(

λ

)

=

I

⁡

(

λ

)

+

k

⁡

(

λ

)

*

[

I

⁡

(

λ

)

I

W

⁡

(

λ

)

]

*

(

T

1

-

T

0

)

where I(λ) is the measured sample signal at wavelength λ when the object is measured, k(λ) is the generated coefficient at wavelength λ, T 1 is the measured reference channel signal when the object is measured, T 0 is a reference signal value obtained from the measuring step, I W (λ) is a measured sample signal value obtained from the measuring step and where I c (λ) is the corrected sample signal; and

outputting the corrected sample signal.

20. The system for compensating thermally dependent light source drift in a spectrophotometer of claim 19 , wherein the calibration coefficient value stored in the memory is determined according to the steps of:

emitting a plurality of flashes of the light from the light source such that the light is incident on a reference target and a calibration target,

measuring for each of the plurality of light flashes the intensity each wavelength of light reflected off a calibration target using the sample sensor the intensity of the light reflected off a reference target using the reference sensor;

transforming the measured values into a compensation coefficient based on the relationship between the signal channel measurement and the reference channel measurement at each wavelength.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 22, 2018
From: DATACOLOR HOLDING AG
To: DATACOLOR AG EUROPE
Reel/Frame 044689/0305 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 13, 2015
From: XU, ZHILING
To: DATACOLOR HOLDING AG
Reel/Frame 035633/0176 →
Continuity (1)
Related Publication 20160334274A1 · Nov 17, 2016