Systems, methods, and apparatuses for optical systems in flow cytometers

Patent metadata

Field	Value
Publication number	US-10018553-B2
Application number	US-201715633613-A
Country	US
Kind code	B2
Filing date	Jun 26, 2017
Priority date	Feb 28, 2014
Publication date	Jul 10, 2018
Grant date	Jul 10, 2018

Abstract

The present set of embodiments relate to a system, method, and apparatus for an optical configuration in a flow cytometer that allows for independent adjustment of focusing for each light source. Such systems, methods, and apparatuses require a final focusing element to be moved near the beginning of the optical train and for each optical element coming after the final focusing element to be configured to accommodate converging light beams while minimizing the introduction of aberrations into those beams.

First claim

What is claimed:

1. An optical system, comprising:
a first optical subunit comprising a first radiation source in optical communication with a first converging element configured to convert radiation from the first radiation source into a first converging radiation beam having a width and an intensity profile across the width;
a second optical subunit comprising a second radiation source in optical communication with a second converging element configured to convert radiation from the second radiation source into a second converging radiation beam having a width and an intensity profile across the width,
the first and second optical subunits being independently adjustable; and
a dichroic element in optical communication with the first optical subunit and the second optical subunit,
the dichroic element being configured to (a) communicate the first converging radiation beam to a target region such that the intensity profile of the communicated first converging radiation beam is essentially unchanged following communication by the dichroic element, (b) communicate the second converging radiation beam to the target region such that the intensity profile of the communicated second converging radiation beam is essentially unchanged following communication by the dichroic element, or both (a) and (b).

2. The optical system of claim 1 , wherein the dichroic element comprises two or more prisms.

3. The optical system of claim 2 , wherein the two prisms are arranged to form a cube.

4. The optical system of claim 3 , wherein the dichroic element includes a wavelength-selective coating located between the two prisms.

5. The optical system of claim 1 , wherein the dichroic element is a long pass filter or a short pass filter.

6. The optical system of claim 1 , wherein at least one of the communicated first converging radiation beam and the communicated second converging radiation beam are not collimated.

7. The optical system of claim 1 , wherein the communicated first converging radiation beam has a width of from about 30 to about 70 micrometers.

8. The optical system of claim 1 , wherein the communicated second converging radiation beam has a width of from about 30 to about 70 micrometers.

9. The optical system of claim 1 , wherein one or both of the communicated first converging radiation beam and the communicated second converging radiation beam has a beam width of about 30-70 micrometers at an intensity of about 90%.

10. The optical system of claim 9 , wherein one or both of the communicated first converging radiation beam and the communicated second converging radiation beam has a beam width of about 40-60 micrometers at an intensity of about 90%.

11. The optical system of claim 1 , wherein at least one of the communicated first converging radiation beam and the second communicated converging radiation beam is characterized as having a flat top intensity profile.

12. The optical system of claim 1 , wherein at least one of the majority of the width of the communicated first converging radiation beam and the majority of the width of the communicated second converging radiation beam has an intensity of at least 90%.

13. The optical system of claim 12 , wherein the communicated first converging radiation beam has an intensity of at least 90% across at least about 50% of the width of the portion of the first converging radiation beam that has an intensity of at least 13.5%.

14. The optical system of claim 13 , wherein the communicated first converging radiation beam has an intensity of at least 90% across from about 60% to about 75% of the width of the portion of the first converging radiation beam that has an intensity of at least 13.5%.

15. The optical system of claim 1 , wherein one or both of the communicated first converging radiation beam and the communicated second radiation beam has a Gaussian intensity profile.

16. The optical system of claim 15 , wherein one or both of the communicated first converging radiation beam and the communicated second radiation beam has a focus at about 2 micrometers on the Gaussian axis.

17. The optical system of claim 1 , the optical system being configured to communicate a plurality of particles through the target region.

18. The optical system of claim 17 , wherein the target region is characterized as a capillary.

19. The optical system of claim 1 , wherein the communicated first converging radiation beam and the communicated second converging radiation beam are separated by a distance at the target region.

20. The optical system of claim 19 , wherein the distance is from about 80 to about 200 micrometers.

Assignees

• Life Technologies Corp

Inventors

• Kaduchak Gregory
• Smith Wesley
• Ward Michael

Classifications

• G01N2015/1438

  Using two lasers in succession · CPC title

• G01N15/1456

  without spatial resolution of the texture or inner structure of the particle, e.g. processing of pulse signals · CPC title

• G01N15/1459 Primary

  the analysis being performed on a sample stream · CPC title

• G01N15/1404 Primary

  Handling flow, e.g. hydrodynamic focusing · CPC title

• G01N15/1434

  Optical arrangements · CPC title