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Wang X, Yan T, Wang L, Wang N, Yang X, Wang X, Cai H, Yuan Z, Ma X, Chen X. Ultra-low-cost and high-fidelity NIR-II confocal laser scanning microscope with Bessel beam excitation and SiPM detection. BIOMEDICAL OPTICS EXPRESS 2024; 15:4786-4794. [PMID: 39346982 PMCID: PMC11427194 DOI: 10.1364/boe.531266] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 05/29/2024] [Revised: 07/10/2024] [Accepted: 07/11/2024] [Indexed: 10/01/2024]
Abstract
Confocal laser scanning microscopy (CLSM) is one of the most important imaging tools in the biomedical field, and near-infrared-II (NIR-II, 900-1700nm) fluorescence imaging technology has also made fruitful research progress in deep imaging in recent years. The NIR-II based CLSM has problems such as an expensive detector and reduced image resolution caused by long wavelength excitation. Here, by simultaneously using a low-cost silicon photomultiplier (SiPM) as a detector and a Bessel beam as an excitation, we developed an ultra-low-cost and high-fidelity NIR-II confocal laser scanning microscope. The use of SiPM reduces the cost of the NIR-II fluorescence detection module in CLSM, while enabling the detection of ultra-broadband fluorescence signals spanning visible to NIR-II regions. The introduction of the Bessel beam compensates to some extent for the weakening of spatial resolution caused by the increase in the wavelength of light in the NIR region. Experimental results show that the use of the Bessel beam can improve the resolution by 12% when observing thin samples. With the increase of sample thickness, the imaging resolution of the Bessel beam at NIR-II wavelengths is better than that of the Gaussian beam at NIR-I wavelengths at the penetrable depth of the NIR-I light. At deeper depths, the imaging resolution and imaging depth of Bessel beam CLSM is superior to Gaussian beam CLSM at the same excitation power.
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Affiliation(s)
- Xinyu Wang
- Center for Biomedical-photonics and Molecular Imaging, Advanced Diagnostic-Therapy Technology and Equipment Key Laboratory of Higher Education Institutions in Shaanxi Province, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
- Engineering Research Center of Molecular and Neuro Imaging, Ministry of Education & Xi’an Key Laboratory of Intelligent Sensing and Regulation of trans-Scale Life Information, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
| | - Tianyu Yan
- Center for Biomedical-photonics and Molecular Imaging, Advanced Diagnostic-Therapy Technology and Equipment Key Laboratory of Higher Education Institutions in Shaanxi Province, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
- Engineering Research Center of Molecular and Neuro Imaging, Ministry of Education & Xi’an Key Laboratory of Intelligent Sensing and Regulation of trans-Scale Life Information, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
| | - Lin Wang
- School of Computer Science and Engineering, Xi’an University of Technology, Xi’an, Shaanxi 710048, China
| | - Nan Wang
- Center for Biomedical-photonics and Molecular Imaging, Advanced Diagnostic-Therapy Technology and Equipment Key Laboratory of Higher Education Institutions in Shaanxi Province, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
- Engineering Research Center of Molecular and Neuro Imaging, Ministry of Education & Xi’an Key Laboratory of Intelligent Sensing and Regulation of trans-Scale Life Information, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
| | - Xiaoli Yang
- School of Control Science and Engineering, Shandong University, Jinan, Shandong 150061, China
| | - Xiaodong Wang
- Shaanxi Institute of Medical Device Quality Inspection, Xi’an, Shaanxi 712046, China
| | - Hu Cai
- Shaanxi Institute of Medical Device Quality Inspection, Xi’an, Shaanxi 712046, China
| | - Zhen Yuan
- Faculty of Health Sciences, University of Macau, Macau 999078, China
| | - Xiaopeng Ma
- School of Control Science and Engineering, Shandong University, Jinan, Shandong 150061, China
| | - Xueli Chen
- Center for Biomedical-photonics and Molecular Imaging, Advanced Diagnostic-Therapy Technology and Equipment Key Laboratory of Higher Education Institutions in Shaanxi Province, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
- Engineering Research Center of Molecular and Neuro Imaging, Ministry of Education & Xi’an Key Laboratory of Intelligent Sensing and Regulation of trans-Scale Life Information, School of Life Science and Technology, Xidian University, Xi'an, Shaanxi 710126, China
- Innovation Center for Advanced Medical Imaging and Intelligent Medicine, Guangzhou Institute of Technology, Xidian University, Guangzhou, Guangdong 510555, China
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Han M, Smith D, Kahro T, Stonytė D, Kasikov A, Gailevičius D, Tiwari V, Ignatius Xavier AP, Gopinath S, Ng SH, John Francis Rajeswary AS, Tamm A, Kukli K, Bambery K, Vongsvivut J, Juodkazis S, Anand V. Extending the Depth of Focus of an Infrared Microscope Using a Binary Axicon Fabricated on Barium Fluoride. MICROMACHINES 2024; 15:537. [PMID: 38675348 PMCID: PMC11052387 DOI: 10.3390/mi15040537] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/06/2024] [Revised: 04/05/2024] [Accepted: 04/15/2024] [Indexed: 04/28/2024]
Abstract
Axial resolution is one of the most important characteristics of a microscope. In all microscopes, a high axial resolution is desired in order to discriminate information efficiently along the longitudinal direction. However, when studying thick samples that do not contain laterally overlapping information, a low axial resolution is desirable, as information from multiple planes can be recorded simultaneously from a single camera shot instead of plane-by-plane mechanical refocusing. In this study, we increased the focal depth of an infrared microscope non-invasively by introducing a binary axicon fabricated on a barium fluoride substrate close to the sample. Preliminary results of imaging the thick and sparse silk fibers showed an improved focal depth with a slight decrease in lateral resolution and an increase in background noise.
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Affiliation(s)
- Molong Han
- Optical Sciences Centre and ARC Training Centre in Surface Engineering for Advanced Materials (SEAM), School of Science, Computing and Engineering Technologies, Swinburne University of Technology, Hawthorn, VIC 3122, Australia; (M.H.); (D.S.); (S.H.N.); (S.J.)
| | - Daniel Smith
- Optical Sciences Centre and ARC Training Centre in Surface Engineering for Advanced Materials (SEAM), School of Science, Computing and Engineering Technologies, Swinburne University of Technology, Hawthorn, VIC 3122, Australia; (M.H.); (D.S.); (S.H.N.); (S.J.)
| | - Tauno Kahro
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Dominyka Stonytė
- Laser Research Center, Physics Faculty, Vilnius University, Sauletekio Ave. 10, 10223 Vilnius, Lithuania; (D.S.); (D.G.)
| | - Aarne Kasikov
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Darius Gailevičius
- Laser Research Center, Physics Faculty, Vilnius University, Sauletekio Ave. 10, 10223 Vilnius, Lithuania; (D.S.); (D.G.)
| | - Vipin Tiwari
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Agnes Pristy Ignatius Xavier
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
- School of Electrical and Computer Engineering, Ben Gurion University of the Negev, P.O. Box 653, Beer-Sheva 8410501, Israel
| | - Shivasubramanian Gopinath
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Soon Hock Ng
- Optical Sciences Centre and ARC Training Centre in Surface Engineering for Advanced Materials (SEAM), School of Science, Computing and Engineering Technologies, Swinburne University of Technology, Hawthorn, VIC 3122, Australia; (M.H.); (D.S.); (S.H.N.); (S.J.)
| | | | - Aile Tamm
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Kaupo Kukli
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
| | - Keith Bambery
- Infrared Microspectroscopy (IRM) Beamline, ANSTO—Australian Synchrotron, Clayton, VIC 3168, Australia (J.V.)
| | - Jitraporn Vongsvivut
- Infrared Microspectroscopy (IRM) Beamline, ANSTO—Australian Synchrotron, Clayton, VIC 3168, Australia (J.V.)
| | - Saulius Juodkazis
- Optical Sciences Centre and ARC Training Centre in Surface Engineering for Advanced Materials (SEAM), School of Science, Computing and Engineering Technologies, Swinburne University of Technology, Hawthorn, VIC 3122, Australia; (M.H.); (D.S.); (S.H.N.); (S.J.)
- Tokyo Tech World Research Hub Initiative (WRHI), School of Materials and Chemical Technology, Tokyo Institute of Technology, 2-12-1, Ookayama, Meguro-ku, Tokyo 152-8550, Japan
| | - Vijayakumar Anand
- Optical Sciences Centre and ARC Training Centre in Surface Engineering for Advanced Materials (SEAM), School of Science, Computing and Engineering Technologies, Swinburne University of Technology, Hawthorn, VIC 3122, Australia; (M.H.); (D.S.); (S.H.N.); (S.J.)
- Institute of Physics, University of Tartu, 50411 Tartu, Estonia; (T.K.); (A.K.); (V.T.); (A.P.I.X.); (S.G.); (A.S.J.F.R.); (A.T.); (K.K.)
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Hung ST, Kalisvaart D, Smith C. Image scanning microscopy: a vectorial physical optics analysis. OPTICS EXPRESS 2024; 32:1524-1539. [PMID: 38297702 DOI: 10.1364/oe.500957] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/18/2023] [Accepted: 11/30/2023] [Indexed: 02/02/2024]
Abstract
Image scanning microscopy (ISM) achieves resolution beyond the diffraction limit by a factor of 2. However, prior ISM research predominantly employs scalar diffraction theory, neglecting critical physical effects such as polarization, aberrations, and Stokes shift. This paper presents a comprehensive vectorial ISM point spread function (PSF) model that accounts for these phenomena. By considering the effect of polarization in emission and excitation paths, as well as aberrations and Stokes shift, our model provides a more accurate representation of ISM. We analyze the differences between scalar and vectorial theories in ISM and investigate the impact of pinhole size and aberration strength on resolution. At a numerical aperture of 1.2, the full width half maximum (FWHM) discrepancy between scalar and vectorial ISM PSFs can reach 45 nm, representing a 30% deviation from the vectorial model. Additionally, we explore multiphoton excitation in ISM and observe increased FWHM for 2-photon and 3-photon excitation compared to 1-photon excitation. The FWHM of the 2-photon excitation ISM PSF increases by 20% and the FWHM of the 3-photon excitation ISM PSF increases by 28% compared to the 1-photon excitation ISM. In addition, we found that the optimal sweep factor for 2-photon ISM is 1.22, and the optimal sweep factor of 3-photon ISM is 1.12 instead of the 2 predicted by the one-photon scalar ISM theory. Our work improves the understanding of ISM and contributes to its advancement as a high-resolution imaging technique.
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Sheppard CJR, Castello M, Tortarolo G, Zunino A, Slenders E, Bianchini P, Vicidomini G, Diaspro A. Signal strength and integrated intensity in confocal and image scanning microscopy. JOURNAL OF THE OPTICAL SOCIETY OF AMERICA. A, OPTICS, IMAGE SCIENCE, AND VISION 2023; 40:138-148. [PMID: 36607082 DOI: 10.1364/josaa.477240] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/03/2022] [Accepted: 11/28/2022] [Indexed: 06/17/2023]
Abstract
The properties of signal strength and integrated intensity in a scanned imaging system are reviewed. These properties are especially applied to confocal imaging systems, including image scanning microscopy. The integrated intensity, equal to the image of a uniform planar (sheet) object, rather than the peak of the point spread function, is a measure of the flux in an image. Analytic expressions are presented for the intensity in the detector plane for a uniform volume object, and for the resulting background. The variation in the integrated intensity with defocus for an offset point detector is presented. This axial fingerprint is independent of any pixel reassignment. The intensity in the detector plane is shown to contain the defocus information, and simple processing of the recorded data can improve optical sectioning and background rejection.
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Yin W, Yang Y, Yang R, Yao B. Tunable depth of focus with modified complex amplitude modulation of an optical field. APPLIED OPTICS 2022; 61:3502-3509. [PMID: 35471448 DOI: 10.1364/ao.453313] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/07/2022] [Accepted: 03/22/2022] [Indexed: 06/14/2023]
Abstract
Bessel beams have nondiffraction and self-healing properties in the propagation direction and are widely used in particle optical manipulation and optical microscopy. Bessel beams can be generated by axicons or spatial light modulators, which can produce a zero-order or high-order Bessel beam with different parameters depending on the specific application. The modulation of Bessel beams achieved in the spatial spectrum domain by optimization algorithms has a low light energy utilization rate due to the small effective modulation region. We propose a Bessel-like beam phase generation algorithm based on an improved iterative optimization algorithm directly in the spatial domain to achieve a tunable modulation of the beam's length and the axial center position. The optimization time is reduced from minutes to seconds relative to the genetic algorithm, providing a new means of modulation for different applications in various fields.
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Temma K, Oketani R, Lachmann R, Kubo T, Smith NI, Heintzmann R, Fujita K. Saturated-excitation image scanning microscopy. OPTICS EXPRESS 2022; 30:13825-13838. [PMID: 35472987 DOI: 10.1364/oe.455621] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/04/2022] [Accepted: 03/27/2022] [Indexed: 06/14/2023]
Abstract
Image scanning microscopy (ISM) overcomes the trade-off between spatial resolution and signal volume in confocal microscopy by rearranging the signal distribution on a two-dimensional detector array to achieve a spatial resolution close to the theoretical limit achievable by infinitesimal pinhole detection without sacrificing the detected signal intensity. In this paper, we improved the spatial resolution of ISM in three dimensions by exploiting saturated excitation (SAX) of fluorescence. We theoretically investigated the imaging properties of ISM, when the fluorescence signals are nonlinearly induced by SAX, and show combined SAX-ISM fluorescence imaging to demonstrate the improvement of the spatial resolution in three dimensions. In addition, we confirmed that the SNR of SAX-ISM imaging of fluorescent beads and biological samples, which is one of the challenges in conventional SAX microscopy, was improved.
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Kratz J, Geisler C, Egner A. ISM-assisted tomographic STED microscopy. OPTICS EXPRESS 2022; 30:939-956. [PMID: 35209272 DOI: 10.1364/oe.445441] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/08/2021] [Accepted: 12/23/2021] [Indexed: 06/14/2023]
Abstract
Stimulated emission depletion (STED) microscopy theoretically provides unlimited resolution. However, in practice the achievable resolution in biological samples is essentially limited by photobleaching. One method which overcomes this problem is tomographic STED (tomoSTED) microscopy. In tomoSTED microscopy, one-dimensional depletion patterns facing in different directions are successively applied in order to acquire a highly-resolved image in two dimensions. In this context, the number of addressed directions depends on the desired angular homogeneity of the point spread function or the optical transfer function and thus on the resolution increase as compared to diffraction-limited imaging. At a reasonable angular homogeneity the light dose and thus bleaching can be reduced, as compared to conventional STED microscopy. Here, we propose and demonstrate for the first time, to our knowledge, that the number of required depletion pattern orientations can be reduced by combining tomoSTED microscopy with the concept of image scanning microscopy (ISM). With our realization of an ISM-tomoSTED microscope, we show that approximately a factor of 2 lower number of orientations are required to achieve the same resolution and image quality as in tomoSTED microscopy.
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Improving Multiphoton Microscopy by Combining Spherical Aberration Patterns and Variable Axicons. PHOTONICS 2021. [DOI: 10.3390/photonics8120573] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
Abstract
Multiphoton (MP) microscopy is a well-established method for the non-invasive imaging of biological tissues. However, its optical sectioning capabilities are reduced due to specimen-induced aberrations. Both the manipulation of spherical aberration (SA) and the use of axicons have been reported to be useful techniques to bypass this limitation. We propose the combination of SA patterns and variable axicons to further improve the quality of MP microscopy images. This approach provides enhanced images at different depth locations whose quality is better than those corresponding to the use of SA or axicons separately. Thus, the procedure proposed herein facilitates the visualization of details and increases the depth observable at high resolution.
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The Development of Microscopy for Super-Resolution: Confocal Microscopy, and Image Scanning Microscopy. APPLIED SCIENCES-BASEL 2021. [DOI: 10.3390/app11198981] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
Optical methods of super-resolution microscopy, such as confocal microscopy, structured illumination, nonlinear microscopy, and image scanning microscopy are reviewed. These methods avoid strong invasive interaction with a sample, allowing the observation of delicate biological samples. The meaning of resolution and the basic principles and different approaches to superresolution are discussed.
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Sheppard CJR, Castello M, Tortarolo G, Slenders E, Deguchi T, Koho SV, Bianchini P, Vicidomini G, Diaspro A. Pixel reassignment in image scanning microscopy with a doughnut beam: example of maximum likelihood restoration. JOURNAL OF THE OPTICAL SOCIETY OF AMERICA. A, OPTICS, IMAGE SCIENCE, AND VISION 2021; 38:1075-1084. [PMID: 34263763 DOI: 10.1364/josaa.426473] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/31/2021] [Accepted: 06/06/2021] [Indexed: 06/13/2023]
Abstract
In image scanning microscopy, the pinhole of a confocal microscope is replaced by a detector array. The point spread function for each detector element can be interpreted as the probability density function of the signal, the peak giving the most likely origin. This thus allows a form of maximum likelihood restoration, and compensation for aberrations, with similarities to adaptive optics. As an example of an aberration, we investigate theoretically and experimentally illumination with a vortex doughnut beam. After reassignment and summation over the detector array, the point spread function is compact, and the resolution and signal level higher than in a conventional microscope.
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Sheppard CJR. Structured illumination microscopy and image scanning microscopy: a review and comparison of imaging properties. PHILOSOPHICAL TRANSACTIONS. SERIES A, MATHEMATICAL, PHYSICAL, AND ENGINEERING SCIENCES 2021; 379:20200154. [PMID: 33896206 DOI: 10.1098/rsta.2020.0154] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Accepted: 12/10/2020] [Indexed: 05/19/2023]
Abstract
Structured illumination microscopy and image scanning microscopy are two microscopical tech- niques, rapidly increasing in practical application, that can result in improvement in transverse spatial resolution, and/or improvement in axial imaging performance. The history and principles of these techniques are reviewed, and the imaging properties of the two methods compared. This article is part of the Theo Murphy meeting issue 'Super-resolution structured illumination microscopy (part 1)'.
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MESH Headings
- Animals
- Humans
- Image Processing, Computer-Assisted/methods
- Image Processing, Computer-Assisted/statistics & numerical data
- Imaging, Three-Dimensional/methods
- Imaging, Three-Dimensional/statistics & numerical data
- Light
- Microscopy, Confocal/methods
- Microscopy, Confocal/statistics & numerical data
- Microscopy, Fluorescence/methods
- Microscopy, Fluorescence/statistics & numerical data
- Microscopy, Fluorescence, Multiphoton/methods
- Microscopy, Fluorescence, Multiphoton/statistics & numerical data
- Optical Phenomena
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Affiliation(s)
- Colin J R Sheppard
- Nanoscopy and NIC@IIT, Istituto Italiano di Tecnologia, Via Enrico Melen, 83 Edificio B, 16152 Genova, Italy
- Molecular Horizons, School of Chemistry and Molecular Biology, University of Wollongong, Wollongong 2522, New South Wales, Australia
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