Concentric spectrometer

• US 6,181,418 B1
• Filed: 03/12/1998
• Issued: 01/30/2001
• Est. Priority Date: 03/12/1998
• Status: Expired due to Term

• Current Assignee: X-Rite Switzerland GmbH (Danaher Corporation)
• Original Assignee: Gretagmacbeth, LLC (Danaher Corporation)
• Inventors: McMahan, Robert K., Weber, William L., Van Aken, Harold R., Palumbo, Perry A.
• Primary Examiner(s): Evans, F. L.
• Application Number:
  US09/041,233
• Time in Patent Office: 1,055 Days
• Field of Search: 356/307, 356/305, 356/326, 356/328
• US Class Current: 356/328
• CPC Class Codes: G01J 3/02 Details
• CPC Class Codes: G01J 3/0208 using focussing or collimating elements, e.g. lenses or mirrors; performing aberration correction
• CPC Class Codes: G01J 3/0218 using optical fibers
• CPC Class Codes: G01J 3/0256 Compact construction
• CPC Class Codes: G01J 3/0262 Constructional arrangements for removing stray light
• CPC Class Codes: G01J 3/0291 Housings; Spectrometer accessories; Spatial arrangement of elements, e.g. folded path arrangements
• CPC Class Codes: G01J 3/18 using diffraction elements, e.g. grating gratings per se G02B

Abstract

A concentric spectrometer which reduces stray light and re-entrant spectra within the spectrometer. The spectrometer includes a non-direct optical path between the entrance slit assembly and exit aperture. Dyson and Offner concentric optical configurations are used to eliminate third-order aberrations The concentric optical system includes a light trap which mitigates or eliminate stray light due to reflection of light incident on the exit aperture region but which does not impinge on the active area of a detector optically coupled to the exit aperture. A two-dimensional area array detector concurrently senses a spectral signal corresponding to an input optical radiation signal and a signal corresponding to zero-input radiation, and the spectral signal is corrected according to the zero-input radiation signal.

Claims

1. A spectrometer comprising:

an entrance aperture through which an optical radiation signal is received;

an exit aperture; and

an optical system that is monocentric and has a dispersion element, and that directs said optical radiation signal along a non-direct optical path from said entrance aperture to said exit aperture via said dispersion element which disperses said optical radiation signal according to wavelength.

2. The spectrometer according to claim 1, wherein said non-direct optical path is such that any dispersed radiation emergent from said dispersion element as a result of incidence on said dispersion element of said optical radiation being directed by said optical system to said dispersion element from said entrance aperture along said non-direct optical path does not impinge on said entrance aperture.

3. The spectrometer according to claim 1, wherein said optical system is symmetric about an optical axis, wherein said dispersion element spatially disperses said radiation according to wavelength along a dispersion direction, and wherein said entrance aperture and exit aperture are separated from and located on opposite sides of a plane which contains said optical axis and is parallel to said dispersion direction, thereby providing said non-direct optical path therebetween.

4. The spectrometer according to claim 1, wherein said optical radiation signal includes a plurality of optical input signals concurrently input into said entrance slit.

5. The spectrometer according to claim 4, wherein said entrance aperture is elongated to form an entrance slit and said plurality of optical signals are linearly oriented along said entrance slit.

6. The spectrometer according to claim 4, further comprising a plurality of optical fibers optically coupled to said entrance aperture, each optical fiber providing a respective one of said plurality of optical input signals.

7. The spectrometer according to claim 6, wherein said plurality of optical fibers are linearly oriented, and wherein regions of zero input radiation are between the fibers.

8. The spectrometer according to claim 1, wherein said optical system includes a spherical plano-convex lens, said dispersion element is a spherical concave diffraction grating, and wherein said spherical plano-convex lens and said spherical concave diffraction grating have coincident centers of curvature.

9. The spectrometer according to claim 1, wherein said optical system includes a concave mirror, said dispersion element is a convex diffraction grating, and wherein said concave mirror and convex diffraction grating have coincident centers of curvature.

10. The spectrometer according to claim 1, wherein said optical system provides linear dispersion of said optical radiation signal.

11. The spectrometer according to claim 1, wherein said optical system includes an optical filter.

12. The spectrometer according to claim 1, further comprising a detector optically coupled to said exit aperture to detect at least a portion of said optical radiation signal directed by said optical system to said exit aperture.

13. The spectrometer according to claim 12, wherein said entrance aperture is displaced from a predetermined plane to compensate for a corresponding displacement of the active area of said detector.

14. The spectrometer according to claim 1, wherein said optical system includes a lens, said dispersion element is a grating, and said lens has a radius of curvature greater than that for an image and object plane near a center of curvature given by the formula R_l=[(n−

1)/n]R_g, wherein R_l is the radius of curvature of said lens, n is the refractive index of the material of said lens, and R_g is the radius of curvature of said grating.

15. The spectrometer according to claim 12, wherein said optical system includes a refractive element and wherein said detector is placed in direct contact with said refractive element.

16. The spectrometer according to claim 12, wherein said optical system includes a light trap structure such that at least a portion of any of said optical radiation which traverses said non-direct optical path from said entrance aperture to said exit aperture and which impinges on said exit aperture along a direction not incident on said detector does not impinge on said entrance aperture by traversing said optical path in an opposite direction.

17. The spectrometer according to claim 16, wherein said optical system includes a spherical plano-convex lens which includes said light trap structure.

18. The spectrometer according to claim 17, wherein the planar surface of said plano-convex lens includes a bevel to provide said light trap structure.

19. The spectrometer according to claim 18, wherein said light trap structure includes a material that substantially absorbs optical radiation incident thereon.

20. The spectrometer according to claim 17, wherein said light trap structure includes a surface which provides substantially diffuse reflection for any optical radiation reflected therefrom.

21. The spectrometer according to claim 12, wherein the detector is a two-dimensional detector.

22. The spectrometer according to claim 21, wherein said optical radiation signal includes a plurality of optical input signals concurrently input into said entrance slit, and said two-dimensional detector is capable of concurrently detecting said plurality of optical input signals directed by said optical system to said exit aperture.

23. The spectrometer according to claim 22, wherein said optical radiation signal includes at least one region of zero input radiation input into said entrance slit concurrently with said plurality of optical input signal so, said two-dimensional detector capable of concurrently detecting said plurality of optical input signals and a signal corresponding to said zero input radiation region directed by said optical system to said exit aperture, the spectrometer further comprising a processor that corrects or compensates at least one detected said optical input signals according to said signal corresponding at least one region of zero input radiation.

24. The spectrometer according to claim 23, wherein said processor and said two-dimensional detector are both located on a common semiconductor substrate.

25. The spectrometer according to claim 21, wherein the two-dimensional detector is an area array of pixels located on a common semiconductor substrate.

26. A spectrophotometer comprising the spectrometer according to claim 1.

27. A method for correcting or compensating at least one spectral signal detected by a spectrometer which includes a two-dimensional detector, said method comprising the steps of:

sensing with said two-dimensional detector said at least one spectral signal and at least one zero-input radiation signal, each of said at least one spectral signal representing dispersion according to wavelength by the spectrometer of a respective input optical radiation signal coupled into the spectrometer, said zero-input radiation signal sensed at all area of said two-dimensional detector exterior to any region that detects any said input optical radiation signal input into the spectrometer;

processing said optical radiation signal and said zero-input radiation signal to correct said optical radiation signal.

28. The method according to claim 27, wherein a plurality of said input optical radiation signals are concurrently coupled into an entrance aperture of the spectrometer, and said at least one zero-input radiation signal corresponds to at least one region between said input optical radiation signals at the entrance slit.

29. The method according to claim 28, wherein said entrance aperture is elongated to form an entrance slit and said plurality of input optical signals are linearly oriented along said entrance slit.

30. The method according to claim 28, wherein each of said plurality of said input optical radiation signals is coupled into said entrance aperture via a respective one of a plurality of optical fibers.

31. The method according to claim 30, wherein said plurality of optical fibers are linearly oriented, and wherein said at least one zero-input radiation signal corresponds to at least one region between said optical fibers.

32. The method according to claim 27, wherein said processing step includes the step of analyzing said optical radiation signal in order to select a processing routine for correcting said at least one spectral signal.

33. The method according to claim 27, wherein the dispersion according to wavelength of each said at least one spectrum signal is detected by a contiguous set of pixels along a first dimension of said two-dimensional detector, each said at least one zero-input radiation signal detected by a contiguous set of zero-input pixels along said first dimension, and wherein said processing step includes the step of correcting a signal sample detected by a first pixel of said contiguous set of pixels according to a function of a zero-input signal sample detected by a second pixel of said zero-input pixels, said second pixel displaced from said first pixel in a second dimension perpendicular to said first dimension, and said first and second pixels having equal displacements relative to the first dimension.

34. The method according to claim 33, wherein said function is also a function of a zero-input signal sample detected by a third pixel of said zero-input pixels, said third pixel displaced from said second pixel in said first dimension.

35. The method according to claim 33, wherein said function is also a function of a zero-input signal sample detected by a third pixel of another of said contiguous set of zero-input pixels along said first dimension, said third pixel and said second pixel being located on opposite sides of said first pixel in said second dimension and having equal displacements relative to the first dimension.

36. The method according to claim 27, wherein said at least one spectrum signal is detected by a pixel array of said two-dimensional detector, said pixel array having columns of adjacent pixels arranged along a first direction of the dispersion according to wavelength and rows of adjacent pixels in a second direction perpendicular to said first direction, each said at least one zero-input radiation signal detected by a zero-input pixel array having columns of adjacent pixels arranged along said first direction and rows of adjacent pixels in the second direction, and wherein said processing step includes the step of correcting a first function of signal samples detected by a first row of pixels of said pixel array according to a second function of zero-input signal samples detected by a second row of pixels of said zero-input pixel array, said first row and said second row displaced in the second dimension and displaced equally with respect to the first dimension.

37. The method according to claim 36, wherein said first function represents a sum or average of signal samples detected by the first row of pixels, and said second function represents a sum or average of zero-input signal samples detected by the second row of pixels.

38. The method according to claim 36, wherein said first function is also a function of a third row of zero-input signal samples detected by the zero-input pixel arrays, said third pixel displaced from said second pixel in said first dimension.

39. The method according to claim 33, wherein said function is also a function of a zero-input signal sample detected by a third row of pixels of another zero-input pixel array, said third row of pixels and said second row of pixels being located on opposite sides of said first row of pixels in said second dimension.

40. The method according to claim 27, wherein the two-dimensional detector is an area array of pixels located on a common semiconductor substrate.

41. The method according to claim 27, wherein said sensing of said at least one spectral signal and said at least one zero-input radiation signal occurs concurrently.

42. A spectrometer comprising:

an entrance aperture through which a plurality of input optical radiation signals are concurrently received;

an exit aperture;

an optical system having a dispersion element, and which directs said plurality of input optical radiation signals along an optical path from said entrance aperture to said exit aperture via said dispersion element which spatially disperses each of said input optical radiation signals according to wavelength; and

a two-dimensional detector optically coupled to said exit aperture to detect at least a portion of each of said plurality of input optical radiation signals directed by said optical system to said exit aperture.

43. The spectrometer according to claim 42, wherein said optical path is such that any dispersed radiation emergent from said dispersion element as a result of incidence on said dispersion element of said optical radiation being directed by said optical system to said dispersion element from said entrance aperture along said optical path may impinge on said entrance aperture.

44. The spectrometer according to claim 42, wherein said optical system is monocentric and is symmetric about an optical axis, wherein said dispersion element spatially disperses said radiation according to wavelength along a dispersion direction, and wherein said entrance aperture and exit aperture are separated from said optical axis and are intersected by a plane which contains said optical axis and is parallel to said dispersion direction, thereby providing a direct optical path therebetween.

45. The spectrometer according to claim 42, wherein said optical path is a non-direct optical path between said entrance aperture and said exit aperture.

46. The spectrometer according to claim 45, wherein said non-direct optical path is such that any dispersed radiation emergent from said dispersion element as a result of incidence on said dispersion element of said optical radiation being directed by said optical system to said dispersion element from said entrance aperture along said non-direct optical path does not impinge on said entrance aperture.

47. The spectrometer according to claim 45, wherein said optical system is monocentric and is symmetric about an optical axis, wherein said dispersion element spatially disperses said radiation according to wavelength along a dispersion direction, and wherein said entrance aperture and exit aperture are separated from and located on opposite sides of a plane which contains said optical axis and is parallel to said dispersion direction, thereby providing said non-direct optical path therebetween.

48. The spectrometer according to claim 42, further comprising a plurality of optical fibers optically coupled to said entrance aperture, each optical fiber providing a respective one of said plurality of input optical radiation signals.

49. The spectrometer according to claim 48, wherein said entrance aperture is elongated to form an entrance slit and said plurality of optical signals are linearly oriented along said entrance slit.

50. The spectrometer according to claim 49, wherein regions of zero input radiation are between the fibers.

51. The spectrometer according to claim 42, wherein said optical system includes a spherical plano-convex lens, said dispersion element is a spherical concave diffraction grating, and wherein said spherical plano-convex tens and said spherical concave diffraction grating have coincident centers of curvature.

52. The spectrometer according to claim 42, wherein said optical system includes a concave mirror, said dispersion element is a convex diffraction grating, and wherein said concave mirror and convex diffraction grating have coincident centers of curvature.

53. The spectrometer according to claim 42, wherein said two-dimensional detector detects a signal corresponding to a region of zero-input radiation input into said entrance aperture concurrently with said plurality of input optical radiation signals, the spectrometer further compromising a processor that corrects or compensates at least one detected said input optical radiation signals according to said signal corresponding a region of zero-input radiation.

54. A spectrometer comprising:

an entrance aperture through which an input optical radiation signal is received;

a detector;

a concentric optical system symmetric about an optical axis and having a dispersion element, and which directs said optical radiation signal along an optical path from said entrance aperture to said detector via said dispersion element which spatially disperses said optical radiation signal according to wavelength; and

a light trap disposed such that optical radiation is prevented from producing reflected light which interferes with optical signals detected by said detector.

55. The spectrometer according to claim 54, wherein said light trap substantially prevents optical radiation which impinges proximate to an active area of said detector from reflecting back to said diffraction element or said entrance slit.

56. The spectrometer according to claim 54, wherein said light trap substantially prevents generation of stray light or re-entrant spectra.

57. The spectrometer according to claim 54, wherein said optical system includes a spherical plano-convex lens which includes said light trap.

58. The spectrometer according to claim 57, wherein the planar surface of said plano-convex lens includes a bevel to provide said light trap.

59. The spectrometer according to claim 57, wherein said light trap includes a material that substantially absorbs optical radiation incident thereon.

60. The spectrometer according to claim 57, wherein said light trap includes a surface which provides substantially diffuse reflection for any optical radiation reflected therefrom.

61. A spectrometer comprising:

an entrance slit assembly including an entrance slit and a plurality of optical fibers that each guide one of a respective plurality of input optical radiation signals into the spectrometer via the entrance slit;

a spherical plano-convex lens;

a concave diffraction grating having substantially parallel grooves, and having a common optical axis and substantially coincident center of curvature relative to said spherical plano-convex lens;

an exit aperture oriented such that said entrance aperture and said exit aperture are separated from and located on opposite sides of a plane which contains said optical axis and which is perpendicular to a direction along the parallel grooves of said concave diffraction grating, thereby providing a non-direct optical path between the entrance and exit apertures; and

a detector optically coupled to the exit aperture, and which senses a plurality of spectral signals each corresponding to one of the respective plurality of input optical signals directed by said spherical plano-convex lens to said concave diffraction grating, dispersed according to wavelength and directed to said spherical plano-convex lens by said diffraction grating, and directed by said spherical plano-convex lens to said exit aperture.

62. The spectrometer according to claim 61, wherein said detector concurrently senses said plurality of spectral signals.

63. A spectrometer comprising:

an entrance slit assembly including an entrance slit and a plurality of optical fibers that each guide one or a respective plurality of input optical radiation signals into the spectrometer via the entrance slit;

a concave mirror;

a convex diffraction grating having substantially parallel grooves, and having a common optical axis and substantially coincident center of curvature relative to said concave mirror;

an exit aperture oriented such that said entrance aperture and said exit aperture are separated from and located on opposite sides of a plane which contains said optical axis and which is perpendicular to a direction along the parallel grooves of said convex diffraction grating, thereby providing a non-direct optical path between the entrance and exit apertures; and

a detector optically coupled to the exit aperture, and which senses a plurality of spectral signals each corresponding to one or the respective plurality of input optical signals directed by said concave mirror to said convex diffraction grating, dispersed according to wavelength and directed to said concave mirror by said convex diffraction grating, and directed by said concave mirror to said exit aperture.

64. The spectrometer according to claim 63, wherein said detector concurrently senses said plurality of spectral signals.

65. A spectrometer comprising:

receiving means for receiving optical radiation into the spectroimeter;

transmitting means for transmitting an optical radiation spectrum according to wavelength of the optical radiation received by the receiving means;

means for directing said optical radiation along a non-direct optical path from said receiving means to said transmitting means and for dispersing said input optical radiation signal according to wavelength to generate the optical radiation spectrum; and

means for detecting at least a portion of said optical radiation spectnum transmitted by said transmitting means.

66. The spectrometer according to claim 65, wherein said means for receiving includes an entrance slit.

67. The spectrometer according to claim 65, wherein said means for directing includes a Dyson-type optical configuration.

68. The spectrometer according to claim 65, wherein said means for directing includes an Offner-type optical configuration.