PARTICLE CHARACTERIZATION

Abstract

A particle characterization apparatus is disclosed comprising: a sample cell for holding a sample, a light source for producing a light beam for illuminating the sample in the sample cell, thereby producing scattered light by the interaction of the light beam with the sample; a focussing lens for focussing the light beam within the sample; and a detector for detecting the backscattered light along a detection optical path that intersects the focussed light beam within the sample. The intersection of the light beam and the detection optical path in the sample define a detection region. The apparatus comprises an optical arrangement for varying the volume of the detection region.

Claims

1. A particle characterization apparatus comprising: a sample cell for holding a sample; a light source for producing a light beam for illuminating the sample in the sample cell, thereby producing scattered light by the interaction of the light beam with the sample; a focussing lens for focussing the light beam within the sample; and a detector for detecting the scattered light along a detection optical path that intersects the focussed light beam within the sample, the intersection of the focussed light beam and the detection optical path in the sample defining a detection region, wherein the apparatus comprises an optical arrangement for varying the volume of the detection region and the focussing lens is moveable, so as to vary a location of a focal plane of the light beam and detection optical path in the sample with movement of the focussing lens so as to vary the position of the detection region within the sample.

2. (canceled)

3. The apparatus of claim 1, wherein the optical arrangement for varying the volume of the detection region is operable to vary the light beam width incident on the focussing lens.

4. The apparatus of claim 3, wherein the optical arrangement for varying the light beam width incident on the focussing lens comprises a beam expander.

5. The apparatus of claim 4, wherein the beam expander comprises a moveable lens, operable to vary the light beam width incident on the focussing lens with movement of the moveable lens.

6. The apparatus of claim 5, wherein the beam expander further comprises a fixed lens between the light source and the moveable lens.

7. The apparatus of claim 6, wherein the beam expander is operable to produce a collimated output beam of variable width.

8. The apparatus of claim 6, wherein the fixed lens comprises a diverging lens.

9. The apparatus of claim 6, wherein the fixed lens comprises a converging lens.

10. The apparatus of claim 5, wherein the moveable lens comprises a converging lens.

11. The apparatus of claim 1, wherein the focussing lens focuses the detection optical path within the sample

12-13. (canceled)

14. The apparatus of claim 1, wherein the optical arrangement for varying the light beam width incident on the focussing lens comprises: a converging lens between the focussing lens and light source causing the light beam to be convergent at the focussing lens, and a mount operable to move the focussing lens so as to vary the distance between the focussing lens and the converging lens.

15. The apparatus of claim 14, wherein the converging lens is a fixed lens.

16. The apparatus of claim 11, wherein the detection optical path comprises an optical fibre.

17. The apparatus of claim 16, wherein the optical fibre comprises a single mode fibre.

18. The apparatus of claim 16, further comprising a coupling lens arranged to couple the detection optical path to the optical fibre.

19. The apparatus of claim 18, wherein the coupling lens comprises a graded refractive index lens.

20. The apparatus of claim 14, wherein the focussing lens comprises a focus tuneable lens.

21. The apparatus of claim 14, wherein the apparatus is operable to perform a dynamic light scattering measurement using an output from the detector.

22. The apparatus of claim 21, wherein the apparatus comprises a processor for performing the dynamic light scattering measurement.

23. A method of performing a dynamic light scattering measurement, comprising: adjusting a location and a volume of a detection region in a sample cell in response to a concentration of particles within a sample held by the sample cell; illuminating the sample with a light beam, thereby producing scattered light by the interaction of the light beam with the sample; detecting scattered light along a detection optical path that intersects the focussed light beam within the sample at the detection region; deriving characteristics of particles within the sample from the detected scattered light by performing dynamic light scattering analysis.

24. The method of claim 23, wherein adjusting the location and volume of the detection region comprises moving the detection region closer to the nearest wall of the sample cell and reducing the volume of the detection region.

25. The method of claim 24, wherein the adjusting is in response to a concentration of particles that is greater than a first predetermined threshold.

26. The method of claim 23, wherein adjusting the location and volume of the detection region comprises moving the detection region further from the nearest wall of the sample cell, and increasing the volume of the detection region.

27. The method of claim 26, wherein the adjusting is in response to a concentration of particles that is lower than a second predetermined threshold.

28. The method of claim 23, further comprising providing an estimated concentration of particles within the sample cell.

29. The method of claim 28, wherein the estimated concentration comprises a qualitative indicator of concentration.

30. The method of claim 23, further comprising measuring the concentration of particles within the sample.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0048] Embodiments of the invention will now be described, with reference to the accompanying drawings, in which:

[0049] FIG. 1 is a schematic diagram of a prior art NIBS arrangement with the detection region in a first position;

[0050] FIG. 2 is a schematic diagram of a prior art NIBS arrangement with the detection region in a second position;

[0051] FIG. 3 is a schematic diagram of an illumination optical path in accordance with an embodiment in which a moveable lens is configured to vary the width of an illumination beam that is incident on the focussing lens;

[0052] FIG. 4 is a schematic diagram of an illumination optical path in accordance with an embodiment in which a converging beam is incident on the moveable focussing lens;

[0053] FIG. 5 is a schematic diagram of the detection region illustrating a beam waist for two different beam widths at the focusing lens;

[0054] FIG. 6 is a schematic diagram of an embodiment of the invention, including the illumination optical path of FIG. 3; and

[0055] FIG. 7 is an outline flow diagram of a method of characterizing particles suspended in a sample, in accordance with an embodiment.

DETAILED DESCRIPTION OF THE INVENTION

[0056] Referring to FIGS. 1 and 2, a prior art NIBS arrangement 100 is shown, in which an illumination beam 106 is focussed on a sample 150 within a sample cell 110 by a focussing lens 130.

[0057] A detection optical path 108 receives light scattered from the illumination beam 106 by particles dispersed within the sample 150. The detection optical path 108 defines the field of view of a detector (not shown) for detecting the scattered light. The detection optical path 108 may receive light scattered at a narrow range of angles, centred on a specific scattering angle 103 along detection axis 109. The detection optical path 108 is also focussed within the sample 150 by the focussing lens 130.

[0058] The intersection of the illumination beam 106 and the detection optical path 108 define a detection region 120. The position of the detection region 120 within the sample cell 110 can be varied by moving the focussing lens 130, which varies the position of a focal plane 112 of the focussing lens 130 within the sample cell 110. As the focussing lens moves closer to the sample cell, the detection volume moves in the same direction, increasing a distance 102 between the detection region 120 and a cell wall through which the light beam 106 passes to illuminate the sample 150. In FIG. 1 the detection volume 120 is positioned closer to this wall of the sample cell 110 than is the case in FIG. 2.

[0059] As discussed above, this arrangement provides for adjustment of the position of the detection region 120, but does not enable adjustment of the volume of the detection region 120.

[0060] Referring to FIG. 3, an illumination optical path 200 is shown comprising a beam expander 175, focussing lens 130 and sample cell 110. The beam expander 175 is arranged to receive an illuminating light beam 106 from a light source (not shown), and to vary the width 161 of the illuminating light beam 106 incident on the focussing lens 130. The illuminating light beam 106 defines a light beam axis 104.

[0061] The beam expander 175 in this embodiment comprises a fixed lens 170 and a moveable lens 160. The fixed lens 170 is disposed between the light source and the moveable lens 160, and is a converging lens. The moveable lens 160 is moveable along the light beam axis 104. The range of movement of the moveable lens 160 may occupy a position on the light beam axis that is after a focal plane of the fixed lens 170, so that the light beam 106 incident on the moveable lens 160 is diverging.

[0062] The moveable lens 160 may be configured to collimate the diverging light beam 106 following the focal plane of the fixed lens 170, so that the beam expander 175 produces a collimated beam of light 106 of variable beam width (or diameter) 161 incident on the focussing lens 130.

[0063] There is a Fourier relationship between the plane 114 of the focussing lens 130 and the plane 164 of the moveable lens 160, such that an increased beam diameter 161 incident on the focussing lens 130 results in a tighter waist of focus within the focal plane 112 within the sample 150. Conversely, a narrower beam diameter 161 incident on the focussing lens 130 results in a broader waist of focus within the focal plane 112 within the sample 150. A narrower waist of focus equates to a smaller detection region 120, and broader waist equates to a larger detection region 120.

[0064] FIG. 5 illustrates the relationship between the width of the beam at the focussing lens 130 and the size of the detection region 120. The path of a beam 201 that is narrow at the focussing lens 130 is compared with the path of a beam 202 that is broader at the focussing lens 130. It can be seen that the detection axis 109 intersects with a longer illuminated region of the sample for the bream 201 than for the beam 202. It will be appreciate that the detection optical path is not confined to the axis 109, but the relationship is nevertheless clear.

[0065] Moving the moveable lens 160 further from the fixed lens 170 results in a larger beam diameter 161, which provides a narrower beam waist at the focal plane 112 of the focussing lens 130, within the sample 150. Such a narrow beam waist is particularly suitable for characterization of turbid samples 150 with high concentration of particles. A detection region 120 with a smaller volume may be positioned closer to a wall of the sample cell 110, reducing the probability of multiple scattering, which directly results in an increase in the maximum particle concentration that can be reliably characterized by the instrument. For a sample with a low concentration of particles, the size of the detection region 120 may be increased by moving the moveable lens 160 further away from the fixed lens 170, thereby increasing the beam width at the focussing lens 130. The focussing lens 130 can be adjusted to place the detection region nearer to the centre of the sample cell 110, away from the walls, so as to minimise scattering contributions from the walls.

[0066] The arrangement depicted in FIG. 3 provides for independent adjustment of the location of the detection region within the sample cell 110 (e.g. nearer or further from the wall facing the light source) and the volume of the detection region 120.

[0067] The focussing lens 130 may operate in the same way as described with reference to FIGS. 1 and 2, being moveable so as to vary the position of the focal plane 112 within the sample cell 110, and therefore to vary the position of the detection region 120.

[0068] Although the detection optical path is not shown in FIG. 3, it may be similar to that depicted in FIGS. 1 and 2, with the detection optical path passing through the focussing lens 130, so that the focus of the detection optical path is likewise moved with the focusing lens 130.

[0069] In an alternative embodiment the converging fixed lens 170 may be replaced by a diverging fixed lens. Furthermore, the moveable focussing lens 130 may be replaced by a fixed, focus tuneable lens (e.g. a deformable lens and/or a lens with tuneable refractive index).

[0070] Referring to FIG. 4, an alternative arrangement of an illumination optical path is shown, for use in an embodiment. The optical path comprises a beam expander 175, focussing lens 130 and sample cell 110. The focussing lens 130 and sample cell 110 may be as described with reference to FIG. 3.

[0071] The arrangement of FIG. 4 differs from that of FIG. 3 because in the arrangement of FIG. 4 the volume of the detection region 120 and the location of the detection region 120 are not independently adjustable. Instead, movement of the focussing lens 130 results in simultaneous adjustment of both the volume and location of the detection volume 120. This may be convenient, and provide a simpler arrangement with fewer moving parts.

[0072] The beam expander 175 in FIG. 4 comprises a first fixed lens 170 and a second fixed lens 180. The first fixed lens 170 is disposed between the second fixed lens 180 and the light source (not shown), and is a converging lens. The illuminating light beam 106 from the light source (which may be collimated) is incident on the first fixed lens 170. The second fixed lens 180 is positioned beyond the focal plane of the first fixed lens 170, between the first fixed lens 170 and the focussing lens 130, so the light beam 106 is diverging when it enters the second fixed lens 180. The second fixed lens 180 is arranged to produce a converging illumination beam at the moveable focussing lens 130. The width and taper of the illuminating beam 106 may be selected to provide a desired relationship between the position of the moveable focussing lens 130 (corresponding with a position of the detection region 120) and the volume of the detection region 120. In alternative arrangements, the first and second fixed lenses 170, 180 may be replaced by a single converging lens, or the first lens 170 could be a diverging lens.

[0073] Moving the focussing lens 130, closer to the beam expander 175 results in a broader beam incident on the focussing lens 130 resulting in a narrower beam waist within the sample 150 as the detection volume 120 is moved closer to the wall of the sample cell 110.

[0074] Referring to FIG. 6, an example embodiment 300 is shown comprising the illumination arrangement 200 from FIG. 3. The detection optical path 108 is similar to that shown in FIGS. 1 and 2, and is focussed within the sample cell 110 by the focussing lens 130. The detection optical path 108 is coupled to a detection optical fibre 307 by a lens 305 (which may be a graded refractive index or GRIN lens). The detection optical fibre 307 couples the detection optical path 108 to the detector 306. Similarly, the light source 302 may provide illumination via an illumination optical fibre 303, via a fibre-free space coupling lens 301 (which may be a GRIN lens).

[0075] The detector 306 may provide a signal to a processor (not shown) which may perform a dynamic light scattering analysis to characterize particles within the sample 150. A display may be provided for displaying the results of such an analysis to a user.

[0076] The illumination path, i.e., the beam 106, and the detection path 108 may pass through a common lens, i.e. the focussing lens 130 in the arrangement illustrated in FIG. 6. In alternative arrangements, the detection path 108 may pass through a separate lens from the illumination path 106, for example in order to defocus one path with respect to the other.

[0077] Referring to FIG. 7, an example method in accordance with an embodiment is shown. The method includes estimating or determining a concentration of particles within a sample 401. For instance, the concentration of particles within the fluid may be measured (e.g. by UV spectroscopy). Alternatively, the user may inspect the sample visually to determine a qualitative measure of particle concentration within the sample (e.g. to determine whether the sample appears turbid). A particle characterization instrument may be configured to automatically estimate the particle concentration, or a user may input an estimate of particle concentration.

[0078] Following the step 401 of estimating/determining particle concentration, the location and volume of the detection region is adjusted 402, for example in response to the concentration of particles in the sample.

[0079] Once the detection region is adjusted, the detection region is illuminated, and light scattered by interactions of the illuminating beam with the sample is detected 403 (e.g. at a detector). The illumination may take place along an optical path similar to those described above. Similarly, the detection may take place along an optical path like those described above.

[0080] The data obtained by detecting the scattered light is subsequently analysed 404 in accordance with well-known dynamic light scattering techniques, so as to determine characteristics of the particles of the sample from the detected scattered light. Such analysis may be performed using a processor, and the results may be displayed on a screen or recorded on a medium (e.g. a computer readable medium).

[0081] Although example embodiments have been depicted in which the detection optical path is configured to detect backscattered light, in other embodiments the detection optical path may be configured to detect forward scattered light (e.g. scattered at less than 90 degrees from the illumination light beam axis 104). Furthermore, an example has been described that uses an optical fibre to couple the detector and/or light source to the sample, it will be understood that the present invention is equally applicable to arrangements that use free space optics.

[0082] In the example embodiments a beam expander has been used to implement a variable volume detection region within the sample. However, any suitable optical assembly, optical component or components may be used to achieve this functionality. For example, a programmable or variable focal length lens may be used (e.g. having a variable refractive index or variable geometry). Alternatively, a plurality of detection paths may be used, each corresponding with a different detection volume, thereby avoiding the need to vary the width of the illuminating beam.

[0083] Embodiments have been described in which varying a beam width at the focussing lens is used to vary the detection region volume. In other embodiments, a focus tuneable lens may be used as the focussing lens, and the detection region volume may be varied by adjusting the focal length of the focus tuneable lens. The focus tuneable lens may be moveable, such that the location of the detection region can be adjusted independently of the detection region volume.

[0084] In some embodiments, both a variable beam width at the focussing lens and a focus tuneable focussing lens may be used.

[0085] Other variations and modifications will be apparent to the skilled person, and are intended to be within the scope of the invention, which is defined by the appended claims.