• Laser & Optoelectronics Progress
  • Vol. 59, Issue 18, 1800001 (2022)
Bo Cao1、2, Huiqun Cao3、*, Danying Lin1, Junle Qu1, and Bin Yu1、**
Author Affiliations
  • 1Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education and Guangdong Province, Center for Biomedical Optics and Photonics, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, Guangdong , China
  • 2College of Electronics and Information Engineering, Shenzhen University, Shenzhen 518060, Guangdong , China
  • 3College of Chemistry and Environmental Engineering, Shenzhen University, Shenzhen 518060, Guangdong , China
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    DOI: 10.3788/LOP202259.1800001 Cite this Article Set citation alerts
    Bo Cao, Huiqun Cao, Danying Lin, Junle Qu, Bin Yu. Research Progress of Double-Helix Point Spread Function Engineering and Its Application[J]. Laser & Optoelectronics Progress, 2022, 59(18): 1800001 Copy Citation Text show less
    3D intensity distribution[15]. (a) Standard PSF; (b) DH-PSF
    Fig. 1. 3D intensity distribution[15]. (a) Standard PSF; (b) DH-PSF
    Schematic of the DH-PSF system[17]
    Fig. 2. Schematic of the DH-PSF system[17]
    Transfer function[10]. (a) DH-PSF using LG model light superposition; (b) high-efficiency DH-PSF initial estimation distribution; (c) high-efficiency DH-PSF distribution; (d)-(f) corresponding LG modal cloud distribution
    Fig. 3. Transfer function[10]. (a) DH-PSF using LG model light superposition; (b) high-efficiency DH-PSF initial estimation distribution; (c) high-efficiency DH-PSF distribution; (d)-(f) corresponding LG modal cloud distribution
    Influence of number and distribution of vortex singularities in the pupil on the PSF[19]. (a) Left column shows the pupil phase function (phase mask) with an increasing number of vortex singularities N and constant spacing d between them, the corresponding PSF at focal plane are shown in the right column; (b) change of the phase mask (left) and PSF at focus (right) as the spacing d increasing with a constant N= 9
    Fig. 4. Influence of number and distribution of vortex singularities in the pupil on the PSF[19]. (a) Left column shows the pupil phase function (phase mask) with an increasing number of vortex singularities N and constant spacing d between them, the corresponding PSF at focal plane are shown in the right column; (b) change of the phase mask (left) and PSF at focus (right) as the spacing d increasing with a constant N= 9
    Relationship between DH-PSF rotation and total number of the Fresnel zones in the spiral mask[22]. (a) N=2; (b) N=6
    Fig. 5. Relationship between DH-PSF rotation and total number of the Fresnel zones in the spiral mask[22]. (a) N=2; (b) N=6
    Image results[9]. (a) Rotating PSF; (b) standard PSF; (c) reconstructed PSF; (d) reconstructed MTF
    Fig. 6. Image results[9]. (a) Rotating PSF; (b) standard PSF; (c) reconstructed PSF; (d) reconstructed MTF
    Flowchart of the dual-channel complementary PSF engineering digital optical system[11]
    Fig. 7. Flowchart of the dual-channel complementary PSF engineering digital optical system[11]
    Depth estimation and restored imaging technology[11].(a) Scene objects recovered from cubic phase channels for image segmentation; (b) average axial distance of each car taken from the depth estimation channel after segmenting the objects within the scene
    Fig. 8. Depth estimation and restored imaging technology[11].(a) Scene objects recovered from cubic phase channels for image segmentation; (b) average axial distance of each car taken from the depth estimation channel after segmenting the objects within the scene
    Microscope image of the fabricated DH-metalens [18]
    Fig. 9. Microscope image of the fabricated DH-metalens [18]
    Experimental setup and characterization of the DH-metalens[18]. (a) Schematic of the experimental setup; (b) theoretically calculated and experimentally obtained relationship curves between the rotation angle (θ) and the imaging defocus (d) at wavelength of 750 nm; (c)-(f) rotation of DH-PSF images at different defocus positions; (g) relationship curves between θ and d at wavelengths of 730, 790, 860 nm, the insets are two DH-PSF images at a wavelength of 730 nm
    Fig. 10. Experimental setup and characterization of the DH-metalens[18]. (a) Schematic of the experimental setup; (b) theoretically calculated and experimentally obtained relationship curves between the rotation angle (θ) and the imaging defocus (d) at wavelength of 750 nm; (c)-(f) rotation of DH-PSF images at different defocus positions; (g) relationship curves between θ and d at wavelengths of 730, 790, 860 nm, the insets are two DH-PSF images at a wavelength of 730 nm
    Design diagram of dual-aperture metasurface depth imaging system[24]
    Fig. 11. Design diagram of dual-aperture metasurface depth imaging system[24]
    Schematic of the image acquisition setup[25]
    Fig. 12. Schematic of the image acquisition setup[25]
    Flowchart of the image acquisition and reconstruction[25]
    Fig. 13. Flowchart of the image acquisition and reconstruction[25]
    Imaging results of the three-dimensional object scene[25]. (a) Nominal image; (b) DH-PSF encoded image; (c) decoded image
    Fig. 14. Imaging results of the three-dimensional object scene[25]. (a) Nominal image; (b) DH-PSF encoded image; (c) decoded image
    Schematic of the single-shot three-dimensional fluorescence microscope[26]
    Fig. 15. Schematic of the single-shot three-dimensional fluorescence microscope[26]
    The conventional image and the extended depth-of-field recovered image produced by DH-PSF, the DH-PSF produces the extended depth-of-field recovered image, which is verified by the observation results of F-actin in BPAE cells[26]. (a)(b) Images captured by using the conventional Gaussian PSF, the two images are captured at different depths (1500 nm apart); (c) raw image acquired by the DH-PSF (N=6); (d) recovered object image shown in Fig.16(c); (a1)-(d1) enlarged images of ROI1 area; (a2)-(d2) enlarged images of ROI2 area
    Fig. 16. The conventional image and the extended depth-of-field recovered image produced by DH-PSF, the DH-PSF produces the extended depth-of-field recovered image, which is verified by the observation results of F-actin in BPAE cells[26]. (a)(b) Images captured by using the conventional Gaussian PSF, the two images are captured at different depths (1500 nm apart); (c) raw image acquired by the DH-PSF (N=6); (d) recovered object image shown in Fig.16(c); (a1)-(d1) enlarged images of ROI1 area; (a2)-(d2) enlarged images of ROI2 area
    Experimental setup for three dimensional tracking of moving fluorescent particles[13]
    Fig. 17. Experimental setup for three dimensional tracking of moving fluorescent particles[13]
    Fluorescent microsphere tracking in three dimensions[13]. (a) Standard PSF image; (b) DH-PSF image; (c) 3D locations of four microspheres; (d)-(f) X-Y, X-Z, and Y-Z projections of the microspheres’ 3D locations
    Fig. 18. Fluorescent microsphere tracking in three dimensions[13]. (a) Standard PSF image; (b) DH-PSF image; (c) 3D locations of four microspheres; (d)-(f) X-Y, X-Z, and Y-Z projections of the microspheres’ 3D locations
    3D tracking of a quantum dot-labeled structure in a live cell[28]
    Fig. 19. 3D tracking of a quantum dot-labeled structure in a live cell[28]
    3D trajectory of a single mRNP in a yeast cell[29]
    Fig. 20. 3D trajectory of a single mRNP in a yeast cell[29]
    Schematic of the DDCM system[38]
    Fig. 21. Schematic of the DDCM system[38]
    Simultaneous three-dimensional tracing of three fluorescent beads[38]
    Fig. 22. Simultaneous three-dimensional tracing of three fluorescent beads[38]
    Schematic of 2π-DH-PSF system and its application in 3D trajectory[40]. (a) Optical setup and 3D stereograms of two defocused 2π-DH-PSF combinations; (b) 3D trajectory of fluorescent microspheres in Hela cells; (c) 3D trajectory of fluorescent microspheres in saliva
    Fig. 23. Schematic of 2π-DH-PSF system and its application in 3D trajectory40. (a) Optical setup and 3D stereograms of two defocused 2π-DH-PSF combinations; (b) 3D trajectory of fluorescent microspheres in Hela cells; (c) 3D trajectory of fluorescent microspheres in saliva
    Schematic of the DH-PSF microscopy using light-sheet illumination[41]
    Fig. 24. Schematic of the DH-PSF microscopy using light-sheet illumination41
    DH-PSF microscopy enhanced by light sheet excitation[41]. (a) DH-PSF obtained from light sheet fluorescence microscopy; (b) DH-PSF of epi-illumination microscopy; (c) intensity profile of the cross section for the two straight lines in Fig.25(a) and Fig.25(b); (d) three-dimensional trajectory of single fluorescent bead; (e) linear fitting of the 3D MSD of single fluorescent bead
    Fig. 25. DH-PSF microscopy enhanced by light sheet excitation[41]. (a) DH-PSF obtained from light sheet fluorescence microscopy; (b) DH-PSF of epi-illumination microscopy; (c) intensity profile of the cross section for the two straight lines in Fig.25(a) and Fig.25(b); (d) three-dimensional trajectory of single fluorescent bead; (e) linear fitting of the 3D MSD of single fluorescent bead
    Schematic of the TILT3D system[42]
    Fig. 26. Schematic of the TILT3D system[42]
    Applications of TILT3D in cell biology[42]
    Fig. 27. Applications of TILT3D in cell biology[42]
    DH-PSF imaging system and 3D super-resolution imaging[16]. (a) Detection path of the single-molecule DH-PSF setup; (b) typical calibration curve between angle of two lobes and axial position; (c) images of a fluorescent bead at different axial positions; (d) single molecule image of DCDHF-V-PF4-azide with high concentration in a thick PMMA sample
    Fig. 28. DH-PSF imaging system and 3D super-resolution imaging[16]. (a) Detection path of the single-molecule DH-PSF setup; (b) typical calibration curve between angle of two lobes and axial position; (c) images of a fluorescent bead at different axial positions; (d) single molecule image of DCDHF-V-PF4-azide with high concentration in a thick PMMA sample
    3D localization of a single molecule[16]
    Fig. 29. 3D localization of a single molecule[16]
    Schematic of the DH-PSF-assisted STED microscopic optical path[68]
    Fig. 30. Schematic of the DH-PSF-assisted STED microscopic optical path[68]
    Three dimensional imaging of a group of 100-nm diameter beads immobilized in a PDMS[68]. (a) Confocal image; (b) corresponding STED image; (c) STED image processed by deconvolution; (d) corresponding DH images recorded at five points in Fig.31(c); (e) image of fluorescent bead at focal plane and corresponding depth map, scale bar is 500 nm
    Fig. 31. Three dimensional imaging of a group of 100-nm diameter beads immobilized in a PDMS[68]. (a) Confocal image; (b) corresponding STED image; (c) STED image processed by deconvolution; (d) corresponding DH images recorded at five points in Fig.31(c); (e) image of fluorescent bead at focal plane and corresponding depth map, scale bar is 500 nm
    Schematic of MSIMH system[70]
    Fig. 32. Schematic of MSIMH system[70]
    Imaging comparison of mitochondria in living cells by wide-field microscope and MSIMH[70]. (a) Wide-field image of mitochondria at z= 0; (b) wide-field image of mitochondria at z=-1000 nm; (c) MSIMH 3D imaging of mitochondria at z=0
    Fig. 33. Imaging comparison of mitochondria in living cells by wide-field microscope and MSIMH[70]. (a) Wide-field image of mitochondria at z= 0; (b) wide-field image of mitochondria at z=-1000 nm; (c) MSIMH 3D imaging of mitochondria at z=0
    Schematic of HMSIM system[71]
    Fig. 34. Schematic of HMSIM system[71]
    Flowchart of the image reconstruction process[71]
    Fig. 35. Flowchart of the image reconstruction process[71]
    Postprocessing of each rodlike sub-image[71]
    Fig. 36. Postprocessing of each rodlike sub-image[71]
    Schematic of RESCH system and RESCH fluorescent images[72]. (a) Sketch of the RESCH optical path; (b) DH-filtered image of a 100-nm diameter fluorescent bead, the circular hole is a synthetic pinhole at the corresponding defocus
    Fig. 37. Schematic of RESCH system and RESCH fluorescent images[72]. (a) Sketch of the RESCH optical path; (b) DH-filtered image of a 100-nm diameter fluorescent bead, the circular hole is a synthetic pinhole at the corresponding defocus
    Confocal and RESCH images of microtubules[72]. (a) The first row is confocal images recorded at axial steps of 200 nm, the second row is RESCH images at corresponding position; (b) confocal image and RESCH images of another sample
    Fig. 38. Confocal and RESCH images of microtubules[72]. (a) The first row is confocal images recorded at axial steps of 200 nm, the second row is RESCH images at corresponding position; (b) confocal image and RESCH images of another sample
    Schematic diagram and characterization of the MRESCH[73]. (a) Optical configuration of MRESCH; (b) intensity distribution of the DH-PSF at different positions along z-axis; (c) relationship between the two lobe rotation angles of the DH-PSF and position along z-axis
    Fig. 39. Schematic diagram and characterization of the MRESCH[73]. (a) Optical configuration of MRESCH; (b) intensity distribution of the DH-PSF at different positions along z-axis; (c) relationship between the two lobe rotation angles of the DH-PSF and position along z-axis
    Schematic of reconstruction process of MRESCH[73]. (a) Raw images of MRESCH; (b) double helix point with digital pinhole; (c) image reconstruction process of MRESCH
    Fig. 40. Schematic of reconstruction process of MRESCH[73]. (a) Raw images of MRESCH; (b) double helix point with digital pinhole; (c) image reconstruction process of MRESCH
    saMMM setup and DH-PSF modulated through the GL phase plate[74]
    Fig. 41. saMMM setup and DH-PSF modulated through the GL phase plate[74]
    Monitoring simultaneously Ca2+ dynamics from 113 foci on cultured expressing jRGECO1 neurons[74]
    Fig. 42. Monitoring simultaneously Ca2+ dynamics from 113 foci on cultured expressing jRGECO1 neurons[74]
    Schematic of holographic optical tweezer (HOT) and DH-PSF system and detail images. (a) Experimental setup integrated with HOT system and DH-PSF system[79]; (b) DH-PSF distribution; (c) DH-PSF phase mask; (d) brightfield image; (e) corresponding off-axis darkfield DH-PSF image
    Fig. 43. Schematic of holographic optical tweezer (HOT) and DH-PSF system and detail images. (a) Experimental setup integrated with HOT system and DH-PSF system[79]; (b) DH-PSF distribution; (c) DH-PSF phase mask; (d) brightfield image; (e) corresponding off-axis darkfield DH-PSF image
    Schematic of experimental setup for two-photon polymerization with single exposure[81]
    Fig. 44. Schematic of experimental setup for two-photon polymerization with single exposure[81]
    SEM images of polymerized double-helix microstructures[81]. (a) Double-helix microstructure array; (b)(c) top and side views of single double-helix microstructure
    Fig. 45. SEM images of polymerized double-helix microstructures[81]. (a) Double-helix microstructure array; (b)(c) top and side views of single double-helix microstructure
    Experimental setup and conceptual design of the holograms for fabricating and detecting double-helical microstructures[82]
    Fig. 46. Experimental setup and conceptual design of the holograms for fabricating and detecting double-helical microstructures[82]
    Diameters of double-helical microstructures to different topological charges[82]
    Fig. 47. Diameters of double-helical microstructures to different topological charges[82]
    Bo Cao, Huiqun Cao, Danying Lin, Junle Qu, Bin Yu. Research Progress of Double-Helix Point Spread Function Engineering and Its Application[J]. Laser & Optoelectronics Progress, 2022, 59(18): 1800001
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