Method for acquiring a spectrum

Patent metadata

Field	Value
Publication number	US-10788427-B2
Application number	US-201815951549-A
Country	US
Kind code	B2
Filing date	Apr 12, 2018
Priority date	Apr 14, 2017
Publication date	Sep 29, 2020
Grant date	Sep 29, 2020

Abstract

The invention is an iterative method for acquiring a spectrum of a particle that is subjected to an illumination. It may in particular be a Raman spectrum. The method includes successively acquiring spectra that are what are called elementary spectra. These elementary spectra are combined to form a combined spectrum, which may be obtained by summing said elementary spectra. With each elementary spectrum is associated an acceptance criterion that is representative of a variation between said elementary spectrum and the elementary spectra acquired beforehand. Depending on this acceptance criterion, the elementary spectrum is either rejected, or accepted, in which case it is added to the combined spectrum. The invention makes it possible to guard against a degradation of the particle under the effect of an excessive exposure to said illumination.

First claim

The invention claimed is:

1. A method for acquiring a spectrum representative of a particle, comprising the following steps:
illuminating the particle with a light source;
detecting, using a photodetector, light radiation emitted or scattered by said particle under effect of the illuminating and acquiring a first elementary spectrum from the detected light radiation;
performing, in order, steps of:
i) forming a combination spectrum from the acquired first elementary spectrum;
ii) acquiring a current elementary spectrum;
iii) taking into account a reference spectrum;
iv) determining an acceptance criterion of the current elementary spectrum, the acceptance criterion corresponding to a deviation between the current elementary spectnim and the reference spectrum;
v) depending on the acceptance criterion:
accepting the current elementary spectrum and updating the combination spectrum by adding the current elementary spectrum to the combination spectrum resulting from step i), or to the combination spectrum resulting from a preceding iteration of steps ii) to v,
or rejecting the current elementary spectrum;

vi) reiterating steps ii) to v) if an iteration termination criterion has not been reached, otherwise exiting from the iteration and proceeding to step vii); and
vii) determining the spectrum representative of the particle, depending on the combination spectrum obtained in v) of a final iteration before exiting.

2. The method according to claim 1 , wherein, after the first iteration of steps ii) to v), the reference spectrum is an average spectrum, representative of an average of elementary spectra forming the combination spectrum resulting from the preceding iteration.

3. The method according to claim 2 , wherein the average spectrum is established on the basis of a normalization of elementary spectra forming the combination spectrum, depending on an acquisition time of each elementary spectrum forming the combination spectrum taken into account in each iteration.

4. The method according to claim 1 , wherein, in step iv), the acceptance criterion is determined on the basis of a subtraction of the reference spectrum and of the current elementary spectrum.

5. The method according to claim 4 , wherein the subtraction is normalized by an indicator of noise in the reference spectrum and in the current elementary spectrum.

6. The method according to claim 1 , wherein the reference spectrum is the first elementary spectrum, acquired in step i), or an elementary spectrum acquired in a preceding iteration.

7. The method according to claim 1 , wherein the reference spectrum is a spectrum deteimined a priori.

8. The method according to claim 1 , wherein the reference spectrum includes one or more regions of interest of the current elementary spectrum.

9. The method according to claim 8 , wherein the acceptance criterion is established via a comparison of the current elementary spectrum, in at least one selected region of interest, with the reference spectrum.

10. The method according to claim 1 , wherein, in step v), the combination spectrum is updated with a sum of:
the current elementary spectrum and the combination spectrum resulting from step i) or the combination spectrum resulting from the preceding iteration, or
the current elementary spectrum, to which processing is applied, and the combination spectnim resulting from step i) or the combination spectrum resulting from the preceding iteration.

11. The method according to claim 10 , wherein the sum is a weighted sum.

12. The method according to claim 1 , wherein, in step vi), the iteration termination criterion corresponds:
a preset number of iterations, and/or
to the obtainment of a preset number of rejections of current elementary spectra, and/or
to the obtainment of a preset number of events in the combination spectrum resulting from step v).

13. The method according to claim 1 , wherein, in step ii), each current elementary spectrum is acquired with a same acquisition time.

14. The method according to claim 1 , wherein, following a first iteration of steps ii) to v), step ii) includes a step of determining an acquisition time of the current elementary spectrum, depending on [[the]] a value of an acceptance criterion resulting from step iii) of the preceding iteration.

15. The method according to claim 1 , wherein the light source generates an illuminating beam that propagates as far as to the particle, and, following a first iteration of steps ii) to v), step ii) includes a step of determining a power of the illuminating beam depending on a value of the acceptance criterion resulting from step iv) of the preceding iteration.

16. The method according to claim 1 , wherein the photodetector is a Raman spectrometer, the acquired first elementary spectrum and each current elementary spectrum being a Raman spectrum representative of the particle.

17. The method according to claim 1 , wherein the photodetector is a fluorescence spectrometer, the acquired first elementary spectrum and each current elementary spectrum being a fluorescence spectrum of the particle.

18. A device for analyzing a particle, including:
a light source;
a holder configured to receive the particle;
a photodetector configured to detect a response signal, emitted by the particle when the particle is illuminated by the light source, and to form a spectrum therefrom; and
a processor that is configured to implement steps i) to vii) of the method according to claim 1 , on the basis of a plurality of elementary spectra acquired by the photodetector, so as to form a spectrum representative of the particle.

Assignees

• Commissariat Energie Atomique

Inventors

• Baritaux Jean-Charles
• Schultz Emmanuelle
• Rebuffel Veronique

Classifications

• G01N21/6486

  Measuring fluorescence of biological material, e.g. DNA, RNA, cells (G01N21/6428 takes precedence) · CPC title

• G01J3/4412

  Scattering spectrometry (particle sizing by light scattering G01N15/0205; optical velocimetry of particles G01P5/20, G01P5/26) · CPC title

• G01N21/65 Primary

  Raman scattering · CPC title

• G01N2021/656

  Raman microprobe · CPC title