Method and apparatus for selecting wavelengths for optical measurements of a property of a molecular analyte

Patent metadata

Field	Value
Publication number	US-9714900-B2
Application number	US-201314397810-A
Country	US
Kind code	B2
Filing date	Apr 29, 2013
Priority date	Apr 30, 2012
Publication date	Jul 25, 2017
Grant date	Jul 25, 2017

Abstract

A system and optimization algorithm for determining the preferred operational wavelengths of a device configured for measurement of molecular analytes in a sample. Operational wavelengths are determined by solving a system of equations linking empirically defined functions representative of these analytes, spectrally dependent coefficients corresponding to these analytes, path lengths traversed by waves probing the analytes at wavelengths corresponding to the absorption level described by the functions representative of these analytes, and, optionally, a cost-function taking into account at least one of spectral separation between the operational wavelengths, manufacturability of wave source(s) producing wave(s) at operational wavelength(s), and the noise factor associated with the operation of such wave source(s).

First claim

What is claimed is:

1. A method for determining a spectral regime of operation of a spectrometric device that is cooperated with a sample, the device enabled to generate optical waves and configured to measure a property of a material component of the sample, the method comprising:
receiving at a user-input device, optical data obtained with light from a set of light sources of said spectrometric device and representing spectrally-dependent characteristics of M material components of the sample to be measured with the spectrometric device having at least one optical detector, M being greater than 1;
forming a first system of equations that expresses the optical data as functions of at least
i) respectively corresponding concentrations of the M material components in the sample and
ii) spectrally-dependent paths of optical waves through the sample, the optical waves respectively corresponding to the M material components;

forming a second system of equations including the first system of equations and additional equations employing at least one parameter representing operational utility of the device; and
solving said second system of equations, with a programmable processor, to calculate such N wavelengths of operation of the device that a spectrally-dependent figure of merit is locally optimized at the wavelengths of operation, wherein to solve said second system of equations a number N of calculated wavelengths of operation smaller than the number M of the material components is required, and wherein said spectrally-dependent figure of merit includes propagation of variance,
and
transforming said set of light sources by replacing at least one light source from said set to form a transformed set of light sources that generate light at said N of calculated wavelengths.

2. A method according to claim 1 , wherein said receiving includes receiving optical data representing, for each of the M material components, two or more of an attenuation coefficient, a scattering coefficient, a coefficient of anisotropy, a fluorescence parameter, an index of refraction, and a parameter representing a quantum response of the M material components to impinging optical waves.

3. A method according to claim 2 , wherein said attenuation coefficient includes a molar attenuation coefficient.

4. A method according to claim 1 , wherein said M material components include two or more of molecular analytes, cells, protein, hemoglobin, glucose, lipids, chromophore, hyperpolarized gas, carbon dioxide, carbon monoxide, and oxygen, and water.

5. A method according to claim 1 , wherein said receiving includes receiving optical data that represent spectrally-dependent light scattering properties of each of the M material components of the sample.

6. A method according to claim 1 , wherein said receiving includes receiving optical data representing spectral dependences of a chosen characteristic of each of the M material components of a sample that contains blood, at least the M material components including blood analyte.

7. A method according to claim 1 , wherein said receiving includes acquiring, with the at least one optical detector, pulses of said optical waves transmitted in a defined sequence and correlating a sequence of acquired pulses with a sequence of transmitted pulses.

8. A method according to claim 1 , wherein said forming of a second system of equations includes forming a matrix equation that includes a matrix coefficient representing one or more of
i) a cost of manufacture of the device that operates at a wavelength of operation from the N wavelengths of operation,
ii) an error associated with determination of said paths of optical waves, and
iii) a figure of merit associated with operational noise of the device at said wavelength of operation.

9. A method according to claim 8 , wherein said forming of a second system of equations includes forming a matrix equation that includes a matrix coefficient representing a figure of merit associated with operational noise of the device, which operational noise is calculated as a function of a change in light scattering of the M components as a wavelength of the optical waves is varied.

10. A method according to claim 1 , wherein said solving includes optimizing the figure of merit that further includes at least one of a parameter representing manufacturing cost of the device, a parameter representing a size of the device, and a parameter representing power consumption of the device.

11. A method according to claim 1 , wherein said solving includes solving the second system of equations to determine first and second wavelengths of operation one of which is shorter that an isosbestic wavelength corresponding to said M material components and another is longer than said isosbestic wavelength.

12. A method according to claim 1 , wherein said solving includes employing an iterative algorithm comprising at least one of a simulated annealing algorithm, a gradient descent algorithm, and a linear programming algorithm.

13. A method according to claim 1 , wherein said forming of a first system of equations includes defining a first system of equations representing said spectrally-dependent characteristics as a functions of respectively-corresponding concentrations parameters representing said material components in the sample, wherein said concentrations parameters include at least two of a cell count, a protein count, a hemoglobin level, a glucose level, a lipid level, percent of a chromophore, a gas concentration; a carbon dioxide concentration, an oxygen concentration a percent content of water, and a pH level.

14. A method according to claim 1 , wherein said spectrally-dependent figure of merit represents operational cost of employing the device.

15. A method according to claim 1 , wherein said spectrally-dependent figure of merit further represents a number of said at least one optical detector and a parameter of placement of said at least one optical detector with respect to the sample.

16. An apparatus for determining a spectral regime of operation of a spectrometric device, the system comprising:
a tangible storage medium containing optical data representing spectrally-dependent characteristics of M material components of a sample to be measured with the spectrometric device having at least one optical detector, M being greater than 1;
a microprocessor in operable communication with the tangible storage medium, the microprocessor being configured to receive an input associated with an identification of M material components of the sample; and
a tangible non-transitory computer-readable medium on which are stored computer instructions that, when the instructions are executed by the microprocessor, cause the microprocessor to:
receive, from the tangible storage medium, said optical data;
form a first system of equations that expresses said optical data as functions of at least
i) respectively corresponding concentrations of the M material components in the sample and
ii) spectrally-dependent paths of optical waves through the sample, the optical waves respectively corresponding to the M material components;
form a second system of equations including the first system of equations and additional equations employing at least one parameter representing operational utility of the device; and
solve said second system of equations with a programmable processor, to calculate such N wavelengths of operation of the device that a spectrally-dependent figure of merit is locally optimized at the wavelengths of operation, wherein to solve said second system of equations a number

Assignees

• Mayo Foundation

Inventors

• Haider Clifton R
• Gilbert Barry K
• Delp Gary S

Classifications

• A61B5/1455

  using optical sensors, e.g. spectral photometrical oximeters · CPC title

• A61B5/1495

  Calibrating or testing of in-vivo probes · CPC title

• G01J2003/104

  Monochromatic plural sources · CPC title

• G01N21/21

  Polarisation-affecting properties (G01N21/19 takes precedence) · CPC title

• G01N21/49

  within a body or fluid · CPC title