SYSTEM AND METHOD FOR HOLOGRAPHIC IMAGING OF A SINGLE PLANE OF AN OBJECT

Abstract

A system and method to produce a hologram of a single plane of a three dimensional object includes an electromagnetic radiation assembly to elicit electromagnetic radiation from a single plane of said object, and an assembly to direct the elicited electromagnetic radiation toward a hologram-forming assembly. The hologram-forming assembly creates a hologram that is recorded by an image capture assembly and then further processed to create maximum resolution images free of an inherent holographic artifact.

Claims

1. A holographic method for detecting interference of electromagnetic waves emitted exclusively from a single plane of a three dimensional object, the method comprising: receiving, at an optical arrangement, electromagnetic waves from the three dimensional object; for each point of a plurality of points in the single plane of the three dimensional object: forming, in the optical arrangement, a first beam of electromagnetic waves and a second beam of electromagnetic waves from electromagnetic waves emitted exclusively from said each point; and detecting exclusively a pattern of interference between the first beam and the second beam; and reconstructing a hologram using the detected patterns corresponding to the plurality of points in the single plane.

2. The method of claim 1 in which the electromagnetic waves are light.

3. The method of claim 2 in which the electromagnetic waves are fluorescent light, luminescent light, or reflected light.

4. (canceled)

5. (canceled)

6. (canceled)

7. The method of claim 2, in which the electromagnetic waves are incoherent light.

8. The method of claim 1, wherein the electromagnetic waves emitted from the single plane are used to create an image.

9. The method of claim 8, wherein the resolution of the image exceeds the Rayleigh or Abbe limit.

10. The method of claim 1, wherein the receiving includes initially collecting the electromagnetic waves from the object with a microscope objective in the optical arrangement.

11. The methods of claim 8, further comprising combining a series of single plane images to create a three dimensional image.

12. A holographic system for detecting interference of electromagnetic waves emitted exclusively from a single plane of a three dimensional object, the system comprising: an optical arrangement configured to: receive electromagnetic waves from the three dimensional object; for each point of a plurality of points in the single plane of the three dimensional object, form a respective first beam of electromagnetic waves and a respective second beam of electromagnetic waves from electromagnetic waves emitted exclusively from said each point; and a detector configured to: for each point of a plurality of points in the single plane of the three dimensional object, detect exclusively a pattern of interference between the respective first beam and the respective second beam; and reconstruct a hologram using the detected patterns corresponding to the plurality of points in the single plane.

13. The system of claim 12 in which the electromagnetic waves are light.

14. The system of claim 13 in which the electromagnetic waves are fluorescent light, luminescent light and reflected light.

15. (canceled)

16. (canceled)

17. (canceled)

18. The system of claim 13, wherein the electromagnetic waves are incoherent light.

19. The system of claim 12, wherein the electromagnetic waves emitted from the single plane are used to create an image.

20. The system of claim 19, wherein the resolution of the image exceeds the Rayleigh or Abbe limit.

21. The system of claim 12, wherein the electromagnetic waves are initially collected with a microscope objective of the optical arrangement.

22. The systems of claim 19, wherein a series of single plane images is combined to create a three dimensional image.

23. A super-resolution optical microscope system, said system comprising: an optical system containing one or more conjugate image planes and a detection plane, with a spatial filter placed at a conjugate image plane; a microscope objective configured to receive light from an object and direct said light to the optical system, wherein the optical system is configured to receive the light from the microscope objective, spatially filter the received light at a conjugate image plane, and produce a hologram at the detection plane; and an image recording device configured to record the hologram at the detection plane.

24. A super-resolution optical microscope method, said method comprising: using a microscope objective configured to receive light from an object and direct said light to an optical system; using an optical system containing one or more conjugate image planes, with a spatial filter placed at a conjugate image plane common to all image planes in the system, to receive the light from the objective, spatially filter all the received light at a conjugate image plane, and to produce a hologram at a detection plane only from the spatially filtered light; and using an image recording device and simultaneous or subsequent image processing to render a final super-resolved image of the object.

25. The holographic system of claim 13, wherein a confocal technique is used to isolate, for each said point in the single plane of the three dimensional object, the electromagnetic waves emitted exclusively from said each point.

26. The holographic system of claim 25, further comprising a confocal pinhole at a conjugate plane between the object and the detection plane in the optical arrangement, wherein the confocal technique includes operating the confocal pinhole to isolate electromagnetic waves emitted exclusively from said each point, and wherein the conjugate plane containing the confocal pinhole is common to the image planes of both the first and second beams formed from the electromagnetic waves emitted from each said point.

27. The holographic system of claim 25, further comprising a spinning disk at a conjugate plane between the object and the detection plane in the optical arrangement, wherein the confocal technique includes operating the spinning disk to isolate electromagnetic waves emitted exclusively from said each point, and wherein the conjugate plane containing the spinning disk is common to the image planes of both the first and second beams formed from the electromagnetic waves emitted from each said point.

28. The holographic system of claim 25, further comprising a camera including the detector, wherein the confocal technique includes adjusting the camera while scanning respective multi-photon excitation spots throughout the object.

29. The holographic system of claim 25, wherein the recorded interference patterns and reconstructed holograms have sharper intensity or phase modulation than those of systems that record multiple planes of an object in one recording.

30. The holographic system of claim 25, wherein the holographic system is a FINCH holographic system, and wherein the detected interference patterns and reconstructed holograms are free from artifacts caused by super-imposition of other planes of the object caused inherently by the FINCH system.

31. The holographic system of claim 25, wherein the holographic system is configured to create interference patterns in which a single detected interference pattern is processable to one or more final images without requiring recording and co-processing of multiple phase shifted interference patterns.

32. The holographic system of claim 25, wherein the interference patterns are recorded at a maximum signal-to-noise ratio that is higher than that of holographic systems that cause multiple planes of the object to create interference patterns on the detector or holographic systems that do not block light from all undesired object planes from reaching the detector.

33. The holographic system of claim 25, wherein the interference patterns are recorded using a maximum dynamic range of the detector as compared to systems that allow multiple planes of the object to create interference patterns on the detector or systems that do not fully block light from all undesired object planes from reaching the detector.

34. The holographic system of claim 26, wherein the confocal pinhole is additionally used to filter an excitation electromagnetic wave that is projected into the object to elicit the electromagnetic waves that are received from the object.

35. The holographic system of claim 27, wherein the spinning disk is additionally used to filter an excitation electromagnetic wave that is projected into the object to elicit the electromagnetic waves that are received from the object.

36. The holographic system of claim 13, wherein the emitted electromagnetic waves are elicited by a multi-photon excitation electromagnetic wave.

37. The holographic system of claim 13, wherein the holographic system is a FINCH holographic system, and wherein the holographic system is configured to confer an improved axial resolution compared to a classical imaging system, by virtue of attenuation of intensity in a reconstructed FINCH hologram plane of residual light from out-of-focus object planes due to sub-optimal beam overlap of two differentially focused beams in a FINCH interference pattern of an out-of-focus object point.

38. The holographic method of claim 2, wherein the forming a first beam of electromagnetic waves and a second beam of electromagnetic waves comprises using a confocal technique to isolate, for each said point in the single plane of the three dimensional object, the electromagnetic waves emitted exclusively from said each point.

39. The holographic method of claim 38, wherein the confocal technique comprises using a confocal pinhole arranged at a conjugate plane between the object and the detection plane to isolate electromagnetic waves emitted exclusively from said each point, wherein the conjugate plane containing the confocal pinhole is common to the image planes of both the first and second beams formed from the electromagnetic waves emitted from each said point.

40. The holographic method of claim 38, wherein the confocal technique comprises using a spinning disk at a conjugate plane between the object and the detection plane in the optical arrangement to isolate electromagnetic waves emitted exclusively from said each point, wherein the conjugate plane containing the spinning disk is common to the image planes of both the first and second beams formed from the electromagnetic waves emitted from each said point.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0011] FIG. 1 (Prior Art) is a schematic of a general FINCH system incorporating a relay subsystem containing a conjugate image plane.

[0012] FIG. 2 is a schematic of a FINCH system with a removable spinning Nipkow disk at the conjugate image plane inside a relay subsystem, according to a preferred embodiment of the present invention.

[0013] FIG. 3 is a schematic of a FINCH system viewing single plane of an object away from the focal plane of the first lens in the FINCH system, showing the modified locations of the conjugate image planes, according to a preferred embodiment of the present invention.

DETAILED DESCRIPTION OF THE DRAWINGS

[0014] With reference to the detailed discussion of the drawings, it is emphasized that the drawings and descriptions are meant to present the composition and operating principles to a sufficient degree to enable a fundamental understanding of the method and system of the invention. Thus certain details such as polarization sensitive optics and compound lens assemblies are represented in the most simplified form to present a clear and readily understood schematic, appropriate to enable one skilled in the art to appreciate the system and method.

[0015] FIG. 1 is a schematic depicting prior art, in this case a FINCH microscope system, and is included to serve as background information to illustrate the concepts discussed further in the description of the invention. A single infinitesimal point 100 located at the front focal plane 118 of the objective lens 101 is considered as an ideal object, with real objects considered as the sum of many single points. After excitation light is introduced into the object 100 from the excitation source 120 by means of the dichroic mirror 119, light emanates from the object 100 and travels a distance z.sub.s 110 to the objective lens 101, which possess focal length f.sub.0. From the objective, the light travels a distance 111 z.sub.1 through the objective back pupil 102 and then a further distance 112 equal to the focal length f.sub.R1 of the first relay lens 103, before reaching the first relay lens 103. The light travels a further distance 113, equal to the sum of the first relay lens focal length and the second relay lens 105 focal length f.sub.R2, before reaching the second relay lens 105. From there 155 the light travels a further distance 114 equal to f.sub.R2 to the polarization sensitive optical assembly (PSOA) 106. It is noted that the two relay lenses comprise a 4f optical relay, which duplicates at its output plane (just before 106) the light distribution that impinged on its input plane at 102, scaled by the magnification ratio f.sub.R2/f.sub.R1. This effectively negates the distance between the objective lens back pupil and the PSOA 106 which actually creates the hologram, and is critical to ensure concentricity of the co-propagating beams 160 produced by 106. The relay pair also contains a conjugate real image plane 104 at a distance of f.sub.R1 after the first relay lens and f.sub.R2 before the second relay lens. The PSOA 106, which possesses two polarization dependent lens functions, focuses part of the light to a focal plane 107 located a distance 115 of f.sub.d1 from the PSOA 106, and part of the light to a focal plane 109 located a distance 117 of f.sub.d2 away from 106. This is equivalent to a single lens located at the position of 106 having two focal lengths f.sub.d1 and f.sub.d2. This differential focusing procedure effectively splits the light beam coming from each object point into two co-propagating, concentric beams with different spherical wavefront curvatures. The two beams are equivalent in spatial size at a single plane known as the hologram plane 108 located a distance 116 z.sub.h away from 106 and the interference between the two beams is captured there as a hologram. The collected hologram is then processed computationally by well-known methods to result in the final image. It is readily understood that all conjugate image planes are at the back focal planes of 103 and 106 only in cases in which the object 100 is at the front focal plane of the objective 101, i.e. z.sub.s=f.sub.0; if z.sub.sf.sub.0, the conjugate image planes change their location in space according to well-known laws of optics. It follows then that the plane z.sub.h 108 only contains perfectly size-matched beams from the objects originating in the front focal plane of 101. Objects not in that front focal plane create perfectly size matched pairs of beams at different planes after the PSOA 106. Thus perfectly overlapped holograms and subsequently maximum resolution final images can only be obtained from a single object plane at one time.

[0016] FIG. 2 depicts one preferred embodiment of the invention, in which a spinning Nipkow disk 200 is inserted between the relay lenses of a system otherwise identical to that described in FIG. 1. As in the system described in U.S. Pat. No. 6,147,798 B2, the Nipkow disk is placed on a rail and can be inserted into or removed from the optical path. It is placed at the internal conjugate image plane 104 of the relay, as in the standard arrangement of a confocal microscope. It can readily be seen that the disk isolates the light emanating from the object portion in the objective focal plane and creates perfectly size matched and overlapped holograms at the plane z.sub.h that will attain maximum possible resolution and avoid the image reversal problem as described in the background of the invention.

[0017] FIG. 3 depicts another preferred embodiment of the invention, in which the disk is translated along the optical axis to a conjugate image plane corresponding to an object plane not at the objective focal plane, and in which the recording plane for the hologram is also translated along the optical axis of the system to a plane at which the two differential beams from the PSOA 106 are size matched and can thus produce maximal resolution final images after processing. All other optics remain in the same location. In this case the object point considered is further away from the objective than the objective focal plane, and the emitted light must travel a distance 304 z.sub.s before encountering the objective. However the conjugate plane 300 inside the relay system is moved closer to the first relay lens 103, and the effective focal planes 301 and 303 of the PSOA 106 are moved to locations that are different distances 305 f.sub.d1 and 307 f.sub.d2 away from 106. The optimal recording plane 302 is also moved to a distance z.sub.h 306 away from 106. In this way a maximum resolution final image may be produced from a point away from the front focal plane of the objective, again without the image reversal problem. It is noted that analogous changes in the locations of the conjugate image planes happen in the opposite direction if the object is closer to the objective than the objective focal plane, with the difference that the conjugate image planes move further away from the first relay lens instead of closer to it. Additionally, in either case the camera need not be moved, but the optical path length may be changed by means of translating corner cube mirrors and similar optics to match the beam sizes at the detection plane.

REFERENCES CITED

U.S. Patent Documents

[0018]

TABLE-US-00001 8,009,340 B2 August 2011 Rosen 8,179,578 B2 May 2012 Rosen et al. 8,542,421 B2 September 2013 Rosen et al. 8,405,890 B2 March 2013 Rosen 6,147,798 B2 November 2000 Brooker et al.

Other Publications

[0019] Siegel et al., in Optics Express, Vol. 20, p. 19822 (2012). [0020] Jost, et al., in Annu. Rev. Mater. Res. Vol/43, pp 261-282 (2013).