Protein quantitation device

Patent metadata

Field	Value
Publication number	US-10948403-B2
Application number	US-201816151732-A
Country	US
Kind code	B2
Filing date	Oct 4, 2018
Priority date	Oct 6, 2017
Publication date	Mar 16, 2021
Grant date	Mar 16, 2021

Abstract

Systems for protein quantitation using a Fabry-Perot interferometer. In one arrangement, a quantitation device includes an infrared source, a sample holder, and a Fabry-Perot interferometer positioned to receive infrared radiation from the source passing through a sample on the sample holder. A band pass optical filter sets the working range of the interferometer, and radiation exiting the interferometer falls on a detector that produces a signal indicating the intensity of the received radiation. A controller causes the interferometer to be tuned to a number of different resonance wavelengths and receives the intensity signals, for determination of an absorbance spectrum.

First claim

What is claimed is:

1. A device for measuring absorption of light by a sample, the device comprising:
a source of infrared radiation;
a sample holder positioned to place a sample in a location to receive infrared radiation from the source;
a Fabry-Perot interferometer positioned to receive infrared radiation originating from the source and passing through the sample, the Fabry-Perot interferometer comprising a pair of spaced-apart reflective surfaces, at least one of which is movable to change the spacing between the reflective surfaces;
a detector positioned to receive infrared radiation from the Fabry-Perot interferometer and to produce an output signal indicating the intensity of the infrared radiation received at the detector;
a first band pass optical filter positioned in an optical path of the device such that infrared radiation in a first wavelength band from the source passes through the first band pass optical filter before reaching the detector;
a second band pass optical filter that passes infrared radiation in a second wavelength band different from the first wavelength band;
a mechanism for removing the first band pass optical filter from the optical path and placing the second band pass filter in the optical path such that infrared radiation from the source passes through the second band pass optical filter before reaching the detector; and
a controller coupled to the source, the Fabry-Perot interferometer, and the detector, the controller including a processor programmed to:
cause the Fabry-Perot interferometer to be tuned to a series of different resonant wavelengths with the first band pass optical filter in place in the optical path;
receive the output signal of the detector at each of the series of resonant wavelengths; and
record an absorbance spectrum indicating the absorbance of the sample as a function of infrared radiation wavelength.

2. The device of claim 1 , wherein the source of infrared radiation is a micromachined resistive source.

3. The device of claim 1 , wherein the source of infrared radiation is hermetically sealed.

4. The device of claim 1 , wherein the Fabry-Perot interferometer is a micromachined Fabry-Perot interferometer.

5. The device of claim 1 , further comprising an optical system positioned to direct infrared radiation passing through the sample toward an entrance aperture of the Fabry-Perot interferometer.

6. The device of claim 1 , wherein the detector is a pyroelectric detector.

7. The device of claim 1 , wherein the source is modulated at a predetermined measurement frequency.

8. The device of claim 7 , further comprising a lock-in amplifier that receives the signal from the detector, enabling lock-in detection of the infrared radiation intensity.

9. The device of claim 1 , wherein the series of wavelengths is a first series of wavelengths and the absorbance spectrum is a first absorbance spectrum, and wherein the processor of the controller is further programmed to:
cause the Fabry-Perot interferometer to be tuned to a second series of different resonant wavelengths with the second band pass optical filter in place in the optical path;
receive the output signal of the detector at each of the second series of resonant wavelengths; and
record a second absorbance spectrum indicating the absorbance of the sample as a function of infrared radiation wavelength within the range of wavelengths passed by the second band pass optical filter.

10. The device of claim 9 , wherein the processor of the controller is further programmed to combine the first and second absorbance spectra into a composite absorbance spectrum, covering a wider wavelength range than either the first or second absorbance spectrum alone.

11. A device for measuring absorption of infrared radiation by a sample, the device comprising:
a source of infrared radiation;
a sample holder positioned to place a sample in a location to receive infrared radiation from the source;
a first Fabry-Perot interferometer positioned to receive infrared radiation originating from the source and passing through the sample, the first Fabry-Perot interferometer comprising a pair of spaced-apart reflective surfaces, at least one of which is movable to change the spacing between the reflective surfaces;
a first detector positioned to receive infrared radiation from the first Fabry-Perot interferometer and to produce an output signal indicating the intensity of the infrared radiation received at the first detector;
a first band pass optical filter positioned in an optical path of the device such that infrared radiation from the source passes through the first band pass optical filter before reaching the first detector, the first band pass optical filter passing a first band of infrared radiation wavelengths;
a second Fabry-Perot interferometer positioned to receive infrared radiation originating from the source and passing through the sample, the second Fabry-Perot interferometer comprising a pair of spaced-apart reflective surfaces, at least one of which is movable to change the spacing between the reflective surfaces;
a second detector positioned to receive infrared radiation from the second Fabry-Perot interferometer and to produce an output signal indicating the intensity of the infrared radiation received at the second detector;
a second band pass optical filter positioned in an optical path of the device such that infrared radiation from the source passes through the second band pass optical filter before reaching the second detector, the second band pass optical filter passing a second band of infrared radiation wavelengths different from the first; and
a controller coupled to the source, the first and second Fabry-Perot interferometers, and the first and second detectors, the controller including a processor programmed to:
cause each of the first and second Fabry-Perot interferometers to be tuned to a respective series of different resonant wavelengths;
receive the output signals of the respective detectors at each of the series of resonant wavelengths; and
record an absorbance spectrum indicating the absorbance of the sample as a function of infrared radiation wavelength within the range of wavelengths passed by the first and second band pass optical filters.

12. The device of claim 11 , further comprising a beam splitter that directs a first portion of the infrared radiation passing through the sample to the first Fabry-Perot interferometer and passes a second portion of the infrared radiation passing through the sample to the second Fabry-Perot interferometer, such that both the first and second Fabry-Perot interferometers receive infrared radiation from the sample simultaneously.

13. The device of claim 11 , further comprising an optical switch that directs infrared radiation passing through the sample to the first Fabry-Perot interferometer when the optical switch is in a first position and directs infrared radiation passing through the sample to the second Fabry-Perot interferometer when the optical switch is in a second position, such that at most one of the first and second Fabry-Perot interferometers receives infrared radiation from the sample at any one time.

14. The device of claim 13 , wherein the optical switch comprises a movable mirror.

15. The device of claim 11 , further comprising a heater proximate the sample holder.

16. A method of protein quantitation, the method comprising:
directing infrared radiation to a sample from an infrared radiation source, at least some of the infrared radiation passing through the sample;
directing infrared radiation having passed

Assignees

• Bio Rad Laboratories

Inventors

• Thrush Evan
• Swihart Steven
• Strong William
• Marlowe Trey
• Lu Li

Classifications

• G02B5/281

  designed for the infrared light · CPC title

• G01N2201/0438

  Linear motion, sequential · CPC title

• G01N2021/3572

  Preparation of samples, e.g. salt matrices · CPC title

• G01N2021/0339

  Holders for solids, powders · CPC title

• G01N21/3563

  for analysing solids; Preparation of samples therefor · CPC title