Enhancing emission of excited radiation in an analytical sample subjected to exciting radiation

• US 5,317,378 A
• Filed: 02/15/1991
• Issued: 05/31/1994
• Est. Priority Date: 02/19/1990
• Status: Expired due to Term

• Current Assignee: Perkinelmer Incorporated
• Original Assignee: Perkinelmer Incorporated
• Inventors: Bennett, Robert, Mould, Henry M.
• Primary Examiner(s): McGraw, Vincent P.
• Assistant Examiner(s): Hantis, K. P.
• Application Number:
  US07/656,266
• Time in Patent Office: 1,201 Days
• Field of Search: 356/317, 356/318, 356/417, 356/446-448, 356/236, 356/301, 356/346, 250/228
• US Class Current: 356/301
• CPC Class Codes: G01N 2021/0367 Supports of cells, e.g. pivotable
• CPC Class Codes: G01N 2021/052 Tubular type; cavity type; multireflective
• CPC Class Codes: G01N 2021/516 Multiple excitation of scattering medium, e.g. by retro-reflected or multiply reflected excitation rays
• CPC Class Codes: G01N 2021/651 Cuvettes therefore
• CPC Class Codes: G01N 2021/655 Stimulated Raman
• CPC Class Codes: G01N 21/03 Cuvette constructions

Abstract

A spherical sample cell (FIG. 4A) bears an external inwardly specular laye defining a hollow imaging mirror 11D and an optical aperture 11E. The mirror acts as an integrator of both the exciting radiation for irradiating the sample and the resulting excited radiation to be analysed, the former entering and the latter exiting through the aperture 11E. Optical integration resulting from multiple internal reflections provides multifold increase in excited radiation compared with bare cells, which is of particular advantage in Raman spectrophotometry. Alternatively, the mirror may be provided in two complementary halves in a two-part cell-holder, in which case any conventional sample cell that fits within the mirror may be used. Spectrophotometers adapted for use with the sample cell or the cell holder as well as methods based on them are described.

Claims

1. An analytical optical sample-cell within which a fluid sample will in operation be subjected to exciting radiation at the sample station of an analytical instrument for the purpose of enabling the excited radiation emitted by the sample to be analysed, the fluid sample being pervious to both radiations, comprising:

a) a hollow imaging mirror having an inner imaging surface which in operation surrounds the sample and acts as a specular optical integrator by virtue of the fact that the said mirror enables both radiations to be multiply reflected within the sample;

b) a hollow bulbous fluid-sample retaining part defined by a wall having a small filling orifice, an outer surface to which the inner imaging surface of the hollow imaging mirror adheres and a substantially co-extensive inner surface adapted to enclose the sample completely except for the small filling orifice, via which the bulbous part may be filled with fluid sample by means of a syringe, the wall of the bulbous part being pervious to both radiations; and

c) a single optical aperture in said mirror through which the exciting radiation will be admitted and the excited radiation will exit, the area of the actual imaging surface of the said mirror being between 51 and 98 percent of the total area represented by the sum of the area covered by the imaging surface and the area of the optical aperture, said sum being substantially equal to the area of said outer surface of the bulbous part, excluding the filling orifice area.

2. An optical sample-cell as claimed in claim 1, wherein the area of the imaging surface is between 80 and 97 percent of the said total area.

3. An optical sample-cell as claimed in claim 1, wherein the imaging surface of the hollow imaging mirror is the inner surface of a suitable coating on the outer surface of the wall defining the bulbous part.

4. An optical sample-cell as claimed in claim 3, wherein the coating is a thin vacuum-evaporated aluminium layer.

5. An optical sample-cell as claimed in claim 1, wherein the volume enclosed by the inner surface of the bulbous part is between 0.08 and 0.4 cc.

6. An optical sample-cell as claimed in claim 5, wherein the volume enclosed by the inner surface of the bulbous part is between 0.1 cc and 0.3 cc.

7. An optical sample-cell as claimed in claim 1, wherein the wall thickness of the hollow bulbous part is between 0.1 mm and 0.2 mm.

8. An optical sample-cell as claimed in claim 1, wherein the optical sample-cell includes registration means to facilitate the proper orientation of the optical aperture when the optical sample-cell is in situ at the sample station of an analytical instrument used to analyse the excited radiation.

9. An optical sample-cell as claimed in claim 1, wherein the imaging surface of the hollow imaging mirror is spherical and the outer surface of the wall defining the hollow bulbous part is also spherical.

10. An optical sample-cell as claimed in claim 1, wherein the wall defining the hollow bulbous part integrally extends into a slender elongated filling stem having a small bore representing the filling orifice.

11. An optical sample-cell as claimed in claim 10, wherein the filling stem is integral with registration means which when engaged by co-operating means provided at the sample station of an analytical instrument will enable the single optical aperture to be properly orientated relatively to the optical means provided in said instrument for the collection of the excited radiation.

12. An optical sample-cell as claimed in claim 11, wherein the registration means is in the form of a projection extending radially from the filling stem.

13. A spectrophotometer which in operation co-operates with an analytical optical sample-cell as claimed in claim 1, comprising:

a) a spectrophotometer having an aperture stop and an optical collecting system for collecting the excited radiation issuing in operation from the optical aperture of the optical sample-cell and transferring it to the aperture stop of the spectrophotometer;

b) optical sample-cell locating means to ensure the proper location of the optical aperture of the optical sample-cell relative to the optical collecting means; and

c) a laser and co-operating light deflecting means adapted to direct a beam of exciting radiation through the central region of said optical aperture in such orientation as to permit a large plurality of internal reflections to be set up within the hollow imaging mirror of the optical sample-cell.

14. A spectrophotometer as claimed in claim 13, wherein the locating means enables the positioning of the optical aperture to be adjusted independently in the three orthogonal x,y, and z axes.

15. A spectrophotometer as claimed in claim 13, wherein the optical sample-cell as claimed in claim 1 further includes registration means which in operation is engaged by the optical sample-cell locating means, whereby to ensure repeatability of the proper operative orientation of the sample-cell aperture.

16. An optical holder for a plain analytical sample-cell in which there are distinguished a first sample-retaining cell portion, within which a fluid sample will in operation be subjected to exciting radiation at the sample station of an analytical instrument for the purpose of enabling the excited radiation emitted by the sample to be analysed, and a second cell portion for filling and handling the cell, said second portion longitudinally extending from the first cell portion, the first cell portion and the sample being transparent to both radiations, said optical holder comprising:

a) two relatively displaceable co-operating members which in operation are eased apart by the user for interposing a filled sample cell as aforesaid therebetween and then are gently pressed together for nesting the sample cell therebetween;

b) a complementary part of a hollow imaging mirror in each member within which part a first cell portion as aforesaid will be nested as the members are pressed together;

c) a single optical aperture in one of the two complementary parts, through which the exciting radiation will be admitted and the excited radiation will exit;

d) a complementary part in each member of sample cell positioning means that will engage a second sample-cell portion as aforesaid as the members are pressed together; and

e) co-operating registration means in each member ensuring that when the members are brought into close abutment with the sample cell nested therebetween the two complementary mirror parts define a complete hollow imaging mirror acting as a specular integrator by virtue of the fact that the said mirror enables in operation both radiations to be multiply reflected within it and hence within the sample and the complementary sample cell positioning parts define a complete sample-cell positioning means which engages the second sample cell portion and locates the first sample cell portion within the hollow imaging mirror.

17. An optical holder for a plain analytical sample-cell as claimed in claim 16, wherein each relatively displaceable member is in the general form of a parallelepipedal slab having an abutment face for providing a close abutment between the members and the associated complementary part of the hollow imaging mirror is a specular surface in a cavity of the member.

18. An optical holder for a plain analytical sample-cell as claimed in claim 17, wherein the cavity in each slab extends so as to extend from a region of the abutment face of the slab into the thickness of the slab.

19. An optical holder for a plain analytical sample-cell as claimed in claim 18, wherein the specular surface is a replicated-from-master surface in a layer adherent to the surface of the cavity.

20. An optical holder for a plain analytical sample-cell as claimed in claim 19, wherein each complementary part of the sample cell positioning means is a rectilinear groove provided in each slab extending from the cavity, and the complete sample-cell positioning means is a channel, that will be formed by the co-operation between the grooves as the displaceable members are brought into abutment.

21. An optical holder for a plain analytical sample-cell as claimed in claim 16, wherein the volume enclosed by the hollow imaging mirror is between 0.08 cc and 0.4 cc.

22. An optical holder for a plain analytical sample-cell as claimed in claim 16, wherein the volume enclosed by the hollow imaging mirror is between 0.1 and 0.3 cc.

23. An optical holder for a plain analytical sample-cell as claimed in claim 16, wherein the hollow imaging mirror is spherical.

24. A spectrophotomer which in operation co-operates with an optical holder for a plain analytical sample-cell as claimed in claim 16, comprising:

a) a spectrophotometer having an aperture stop and an optical collecting system for collecting the excited radiation issuing in operation from the optical aperture of an optical holder as aforesaid and transferring it to the aperture stop of the spectrophotometer;

b) locating means for ensuring the proper location of the optical-holder single optical aperture relative to the optical collecting system; and

c) a laser co-operating with light deflecting means to direct a laser beam of exciting radiation through the central region of said optical aperture in such orientation as to permit a large plurality of internal reflections to be set up within the hollow imaging mirror of the optical holder.

25. A spectrophotometer as claimed in claim 24, wherein the optical holder is integral with a co-operating spectrophotometer by virtue of the fact that the displaceable member including the optical aperture is predeterminedly fixed relatively to the optical collecting system and thus inherently includes the said locating means.

26. A spectrophotometer as claimed in claim 24, wherein the locating means is in the form of a structure into which the co-operating members of optical holder may be slid in abutment and retained therein with the optical aperture in a predetermined optically correct location with respect to the optical collecting system.

27. A spectrophotometer as claimed in claim 24, comprising means for adjusting the power of the laser beam and means for adjusting the cross-section of the laser beam.

28. A spectrophotometer as claimed in claim 24, comprising a filter for attenuating unwanted excited radiation and maximising desired excited radiation, the filter being located in close proximity to the aperture stop of the spectrophotometer.

29. A spectrophotometer as claimed in claim 24, wherein the spectrophotometer is a Raman Fourier Transform spectrophotometer and the aperture stop of the spectrophotometer is the Jacquinot stop.

30. As spectrophotometer as claimed in claim 24, wherein the optical collecting system includes means for adjusting the optical matching between the effective source of the excited radiation and the aperture stop of the spectrophotometer by permitting the image and object distances to be independently adjusted.

31. A spectrophotometer as claimed in claim 24, wherein the optical collecting system includes means for selecting as the effective source the region within the hollow imaging mirror accessed through the optical aperture where the concentration of excited radiation is more advantageous.

32. A method of spectrophotometry comprising the steps of:

a) injecting a fluid sample in an analytical optical sample-cell comprising a hollow imaging mirror having an inner imaging surface surrounding the sample and thus acting as a specular optical integrator, except for an area not significantly larger than that occupied by an optical aperture, by virtue of the fact that the said mirror enables, in the performance of this method, both exciting radiation impinging upon the sample and excited radiation emitted by the sample to be multiply reflected within the sample;

b) locating the analytical optical sample-cell at the sample station of a suitable spectrophotometer having an aperture stop;

c) irradiating the sample with a narrow beam of exciting radiation directed through the optical aperture of the hollow imaging mirror along such path as will cause the beam to undergo multiple reflections in the volume within said mirror;

d) imaging a chosen zone of near optimum energy density from within the hollow imaging mirror close to the optical aperture onto the aperture stop of said suitable spectrophotometer and thus collecting the radiation excited in the molecules of the sample that is available at the chosen zone as a result of the multiple reflections taking place within the hollow imaging mirror and transferring it to said aperture stop with an advantageously predetermined optical matching, the said zone thus representing the effective source of excited radiation; and

e) analysing by means of said suitable spectrophotometer the excited radiation collected.

33. A method as claimed in claim 32, wherein the narrow beam of exciting radiation is a laser beam.

34. A method as claimed in claim 33, wherein the power and the cross-section of the laser beam are adjusted in relation to the sample volume so that excessive temperatures leading to loss or disintegration of the sample are avoided.

35. A method as claimed in claim 32, wherein the method is a method of Raman Fourier Transform spectrophotometry and the spectrophotometer is a Raman Fourier Transform spectrophotometer.

36. A method of spectrophotometry comprising the steps of:

a) filling a plain analytical sample-cell with a fluid sample to be analysed;

b) placing the plain analytical sample-cell between relatively displaceable co-operating members of an optical holder for said cell, each member comprising a complementary part of a hollow imaging mirror provided with an optical aperture in one of the parts;

c) urging the said parts to abut with the plain analytical sample-cell nesting within the hollow imaging mirror;

d) locating the optical holder at the sample station of a suitable spectrophotometer having an aperture stop;

e) irradiating the sample with a narrow beam of exciting radiation directed through the central region of the optical aperture along such path as will cause the beam to undergo multiple reflections within the volume of said hollow imaging mirror;

f) imaging a zone of near optimum high energy density from within the hollow imaging mirror close to the optical aperture onto the aperture stop of said suitable spectrophotometer and thus collecting the radiation excited from the molecules of the sample that is available at the chosen zone as a result of the multiple reflections taking place within the hollow imaging mirror and transferring it onto said aperture stop with an advantageously predetermined optical matching, the said zone thus representing the effective source of stimulated radiation; and

g) analysing by means of the spectrophotometer the excited radiation collected.

37. A method as claimed in claim 36, wherein the narrow beam of exciting radiation is a laser beam.

38. A method as claimed in claim 37 wherein the power and the cross-section of the laser beam are adjusted in relation to the sample volume so that excessive temperatures leading to loss or disintegration of the sample are avoided.

39. A method as claimed in claim 36, wherein the method is a method of Raman Fourier Transform spectrophotometry and the spectrophotometer is a Raman Fourier Transform spectrophotometer.