The 2014 Nobel Prize in chemistry was awarded for the groundbreaking advancement of superresolution microscopy, which surpasses the fundamental diffraction limit of spatial resolution.1^–4 Among these remarkable technologies, structured illumination microscopy (SIM) stands out as a unique and highly compatible approach that can provide ultrahigh temporal and spatial resolution. SIM can be mainly categorized into two types: two-dimensional structured illumination microscopy (2DSIM)5^–8 and three-dimensional structured illumination microscopy (3DSIM).9^–11 2DSIM, also known as traditional SIM, extends the resolution beyond the diffraction limit by a factor of 2 in the x−o−y plane by utilizing 2D patterned illumination and subsequent reconstruction algorithms7^,12^–16 2DSIM has emerged as a powerful imaging technique that facilitates rapid and time-lapse visualization of diverse biological processes. However, because the illumination pattern of 2DSIM is not modulated axially, its axial resolution is the same as that of wide-field microscopy, leading to significant reconstruction errors when imaging thick specimens with defocus background. In stark contrast, 3DSIM with axial-modulated illumination can effectively double the axial resolution. This enables superresolution imaging in all three dimensions (x−y−z), enhancing the discernment of subcellular structures with unparalleled clarity and accuracy, particularly in deeper regions of the specimen. Unlike traditional 2DSIM images,17^,18 which are flat and lack depth information, 3D imaging aims to recreate the spatial characteristics of the subject, providing a more realistic and immersive representation.

Various implementations have been developed to realize the structured illumination and polarization modulation of the 3DSIM system, whose crucial device includes phase grating9^,19 and a ferroelectric liquid crystal spatial light modulator (FLC-SLM). Phase grating5^,9^,20 with a fixed linear polarizer is rotating and laterally translated to control the direction, phase, and polarization of the structured light, but the imaging speed is limited by the mechanical rotation (∼1s) and transversal movement (∼10ms) of the phase grating, and the incompatibility of phase grating period and interference frequency at different excitation wavelengths poses a challenge for multicolor imaging. FLC-SLM applies electric fields to the crystal layer and realizes the modulation of the optical field, which plays a crucial role by acting as a digital grating, replacing the traditional transmission phase grating. However, FLC-SLM cannot continuously display patterns, which requires constant switching of images and precise timing synchronization. Then, the response time of ferroelectric liquid crystal phase retarders is normally milliseconds, which will extremely drag the imaging speed and cause motion artifacts. What is more, Pizza wave plates are unable to adjust the zeroth-order light, necessitating a separate light path for its introduction and separate adjustment of its polarization angle when using SLMs, posing a difficulty in constructing an SLM-based 3DSIM system.

The digital micromirror device (DMD) is a kind of SLM that utilizes the electromechanical rotation of micromirrors to modulate the light field reflecting off DMD. Its fast response speed, low cost, and wide availability make it a popular choice for projectors and scientific research instruments. As each micromirror is controlled in the binary form corresponding to on and off states, DMD can also become a digital reflection grating when loading with a specific pattern and thus can provide a rapid switch of structured illumination patterns for 3DSIM. Compared with FLC-SLM-based 3DSIM, DMD-based 3DSIM possesses the following advantages in the interference SIM system. First, after loading pattern images, DMD maintains a working state and does not require a refresh cycle, as FLC-SLM does, which greatly simplifies the timing control of the SIM system. Then, DMD has a higher switching speed, with the latest products capable of switching speeds up to 23 kHz/1 bit (DLP9500, TI), making it more suitable for fast imaging of live cells. In addition, due to the nature of the coating on the DMD surface, DMD can preserve the polarization state of reflected light the same as the incident light. With an electro-optic modulator (EOM) capable of switching speeds up to the order of nanoseconds, DMD enables ultrafast imaging with minimal motion artifacts. All of these aspects show the greater potential and inspired us to combine DMD and EOM to build a 3DSIM system. (Section S1 in the Supplementary Material shows the comparison of three representative SIM methods with various polarization control schemes, and Sec. S2 in the Supplementary Material shows the polarization extinction ratio of DMD-based SIM with three polarization control schemes.) Overall, SIM, with its remarkable capabilities and flexibility, combined with the distinct advantages offered by DMDs, holds tremendous potential for advancing superresolution microscopy techniques.

In this work, we present a novel and high-speed autopolarization synchronization modulation 3DSIM system, leveraging the autopolarization-maintenance capability of DMD, in conjunction with the polarization modulation capability of EOM for the first time, we believe. By harnessing these advanced technologies, our developed system demonstrates exceptional superresolution imaging capabilities in all three dimensions (x−y−z) and in imaging speed, while enabling the precise determination of fluorescent dipole orientations. Through extensive experimentation, we successfully imaged a diverse array of subcellular structures, including the nuclear pore complex, microtubules, actin filaments, and mitochondria in animal cells. Moreover, we extended the application of our 3DSIM system to investigate highly scattering plant cell ultrastructures, examining cell walls in oleander leaves, hollow structures in black algal leaves, and features within the root tips of corn tassels. Notably, in a mouse kidney slice, the actin filaments exhibited a pronounced polarization effect, which was effectively captured and visualized using our 3DSIM approach. Overall, our innovative DMD-based 3DSIM technique offers a rapid, precise, and versatile platform for superresolution imaging, facilitating a range of significant biological discoveries and providing a reliable foundation for the advancement of next-generation 3DSIM.

An optical schematic for the 3DSIM setup is shown in Fig. 1(a). An excitation laser beam of 561 nm was polarized via a Glan–Taylor polarizing prism and modulated by a polarization rotator composed of an EOM and a quarter-wave plate. With linearly polarized light incident on the polarization rotator, output polarization can be rotated in azimuth at a speed up to 250 kHz by adjusting the liquid crystal retardation of the EOM. The emergent light was collimated and expanded to a diameter of 13 mm via a beam expander and then illuminated on the pattern generator DMD, a 1920pixel×1080-pixel SLM, at an incidence angle of 12 deg directed by mirrors. Each pixel of the DMD can tilt along the diagonal of the square micromirror, and the tilt direction of each micromirror is dictated by the binary contents of the CMOS memory cell associated with each micromirror. A binary value of 1 results in a micromirror landing in the ON state direction and a binary value of 0 results in a micromirror landing in the OFF state direction. Therefore, when a specific periodic binary fringe is loaded on the DMD, the DMD works as a pattern generator, and the diffracted beams converging through lens 1 can form 0th and ±1st order beams perpendicular to the periodic binary fringe. The custom-built spatial mask consisting of one central 0.6 mm diameter pinhole with an attenuation filter and six symmetrical 0.6 mm diameter pinholes is located in a pupil plane of L1 and can screen out the wanted seven diffraction beams and adjust the intensity ratio of the 0th and ±1st beams. The intensity of order 0 was 75% of that of ±1st orders to strengthen the highest lateral frequency information components. The 0th and ±1st order diffraction beams were refocused to the center and two points near the opposite edges of the back focal plane of the objective lens through a 4f system consisting of lens 2 and lens 3 via a polarization-preserving dichroic mirror coating with minimal transmission retardance at the excitation wavelength to maintain the desired polarization state of the illumination beam.21 The objective recollimated the three beams and made them approach the sample and intersect with each other to produce a 3D pattern of excitation intensity with both axial and lateral structures in the focal plane of the objective. The fluorescence emitted from the sample was gathered by the same objective and passed through the same polarization-preserving dichroic mirror, a tube lens, and an emission filter to a water-cooled sCMOS camera with 82% peak quantum efficiency to detect the emission fluorescence. The follow-up instrument is discussed in Sec. S3 in the Supplementary Material.

The acquisition of 3D data involved the use of five pattern phases spaced evenly at intervals of 2π/5, three pattern orientations separated by 60 deg, and an axial step size of 125 nm. The phase and orientation of the illumination stripe were controlled by rotating and laterally translating the pattern in the DMD. When patterns in Fig. 1(b) were preloaded onto the DMD controller circuit board, the DMD served as a grating, enabling precise and reproducible control of the position of the stripes formed by interference in the sample along the direction of its pattern wave vectors under the accurate determination of pattern wave vectors. We employed a piezoelectric translator (NanoMax 300, Thorlabs) controlled by closed-loop feedback from a capacitive position sensor to allow axial movement of the sample holder to the objective lens. And, the acquired data spanned an axial range that typically extended slightly above and below the region of interest. In certain cases where special requirements for high-speed imaging exist, sCMOS cameras can be operated in the rolling shutter mode (synchronous readout trigger mode), where exposure is triggered at the beginning of each frame and progresses row by row until the entire frame is captured. The synchronization of optical system components is crucial for proper functioning and performance. In our system, the differential amplifier (Model 302RM, Conoptics) of EOM for polarization rotating, DMD pattern switching and displaying, the trigger for the sCMOS camera to exposure in synchronous read-out mode, and trigger for the piezoelectric translator to move along axial direction were all precisely synchronized by a LabVIEW-based program running on a data acquisition equipment (PCIe-6738, National Instruments). The time sequence of the synchronization of the DMD-based 3DSIM is in Sec. S4 in the Supplementary Material.

Because of the characteristics of the optical system, the optical transfer function (OTF) has a leaky-cone shape.9 This causes a defocus background and limitation in the z axis. Through a shifted spectrum to fill the OTF, 3DSIM achieves the double enhancement in the x−y−z axis, as shown in Figs. 2(a) and 2(b). When the three beams interface in the specimen plane S(x,y,z), the emission light distribution Cθ,φ(x,y,z) with illumination angle θ and phase φ can be expressed as Cθ,φ(x,y,z)=[S(x,y,z)·Iθ,φ(x,y,z)]⊗OTF(x,y,z),(1)where Iθ,φ(x,y,z) is the excitation illumination light and OTF(x,y,z) is the leaky-cone OTF of the 3DSIM system.

Different from 2D-SIM, which has 0th and 1st harmonics, the illumination light of 3DSIM can be composited into the 0th, 1st, and 2nd harmonics, and can be expressed as22Iθ,φ(x,y,z)=I0[1+2m2+4m·cospzz·cos(pxx+pyy+φ)+2m2cos(2pxx+2pyy+2φ)],(2)where (x,y,z) are the vector bases of x−y−z in 3D space. We can see that only the firstst harmonic (4m·cos2πpzz) is relevant to the z axis, and the other harmonics (1+2m2 and 2m2) are only relevant to the x−y axis. So, let m0=1+2m2, m1z(z)=4m·cos2πpzz (let m1=4m) and m2=2m2 to simplify the expression. The Fourier transform of illumination light is Iθ,φ(kx,ky,kz)=I0{m0δ(kx,ky,kz)+m1δ(kx−px,ky−py,kz−pz)ejφ+m1δ(kx−px,ky−py,kz+pz)ejφ+m1δ(kx+px,ky+py,kz−pz)e−jφ+m1δ(kx+px,ky+py,kz+pz)e−jφ+m2δ(kx+2px,ky+2py,kz)e−j2φ+m2δ(kx+2px,ky+2py,kz)e−j2φ}.(3)

So, the 3D Fourier transform of emission light distribution Cθ,φ(x,y,z) can be expressed as $$\begin{gathered} Cθ,φ(kx,ky,kz)= \\ I0{m0S(kx,ky,kz)+m1S(kx−px,ky−py,kz−pz)ejφ+m1S(kx−px,ky−py,kz+pz)ejφ+m1S(kx+px,ky+py,kz−pz)e−jφ+m1S(kx+px,ky+py,kz+pz)e−jφ+m2S(kx+2px,ky+2py,kz)e−j2φ+m2S(kx−2px,ky−2py,kz)e−j2φ}. \end{gathered}$$(4)

Normally, we set the three illumination angles of θ1, θ2=θ1+2π/3, and θ3=θ1+4π/3 to improve the isotropy of reconstruction. In each illumination angle, we can resolve the 0th, ±1st, and ±2nd bands [i.e., S(kx,ky,kz), S(kx±px,ky±py,kz−pz)+S(kx±px,ky±py,kz+pz), and S(kx±2px,ky±2py,kz)] through the five images of phase (typically φ1=0, φ2=2π/5, φ3=4π/5, φ4=6π/5, φ5=8π/5) using the matrix separation method, [Cθ,φ1(k)Cθ,φ2(k)Cθ,φ3(k)Cθ,φ4(k)Cθ,φ5(k)]=I0M[S(kx,y,kz)·OTF(k)[S(kx−px,ky−py,kz−pz)+S(kx−px,ky−py,kz+pz)]·OTF(k)[S(kx+px,ky+py,kz−pz)+S(kx+px,ky+py,kz+pz)]·OTF(k)S(kx−2px,ky−2py,kz)·OTF(k)S(kx+2px,ky+2py,kz)·OTF(k)],(5)where k=(kx,ky,kz), M=[m0m1ejφ1m1e−jφ1m2ej2φ1m2e−j2φ1m0m1ejφ2m1e−jφ2m2ej2φ2m2e−j2φ2m0m1ejφ3m1e−jφ3m2ej2φ3m2e−j2φ3m0m1ejφ4m1e−jφ4m2ej2φ4m2e−j2φ4m0m1ejφ5m1e−jφ5m2ej2φ5m2e−j2φ5]is the separation matrix, so the five bands B0(k), B±1(k), and B±2(k) of 0th, ±1st, and ±2nd can be expressed as [B0(k)B−1(k)B+1(k)B−2(k)B+2(k)]=1I0A−1[Cθ,φ0(k)Cθ,φ1(k)Cθ,φ2(k)Cθ,φ3(k)Cθ,φ4(k)],(6)where [·]−1 is the symbol of the matrix inverse transform. Then, the five components should be shifted into the correct spectrum position on the x−o−y plane, so the combined spectrum can be expressed as Combined0(k)=∑n=−22F{F−1[Bn(k)·e−jn2π(px,py)]},(7)where F[·] and F−1[·] denote the 3D Fourier transform and Fourier inverse transform. Then, we use a notch filter23 and two steps of filters using Open-3DSIM to make the spectrum smooth and even and reduce the artifacts. The detailed steps are dismissed here and can be seen in Open-3DSIM.24 When Combined0(k) is notched and filtered, it can be expressed as Combined1(k). Thus, the final 3DSIM result S3DSIM(x,y,z) is S3DSIM(x,y,z)=F−1[Combined1(k)].(8)

The detailed algorithm flow is shown in Fig. 2(c).

Together with our recently published Open-3DSIM software,24 we have made all the hardware components and control mechanisms openly available in this study as a complementary open-source hardware counterpart. We have opened the detailed hardware devices in Sec. S5 in the Supplementary Material and the LabVIEW program in GitHub repository (available at: https://github.com/Cao-ruijie/DMD-3DSIM-hardware) to control the sequence of DMD, sCMOS camera, EOM, and piezoelectric translation platform for reproduction and development of the 3DSIM system (S6 in the Supplementary Material). Given the widespread utilization of DMD technology in digital light processing and its cost-effectiveness as a consumer product, we anticipate that our initiatives will significantly support the community in devising diverse adaptations and iterations, capitalizing on the foundation established by our open hardware approach.

To quantify the enhanced resolution and qualify the optical sectioning capability of our 3DSIM approach, we initially imaged 100 nm fluorescent beads using a raw-frame exposure time of 15 ms and a volume time of 6.75 s (29 sections, 15 frames/section, and 125 nm sectioning step). A comparison was made between the wide-field (WF) image and 3DSIM image, as depicted in Fig. 3(a). In the magnified view of the region outlined by the blue rectangle, the 3DSIM image successfully resolves three adjacent beads that are indistinguishable in the WF image, highlighting a significant improvement in lateral resolution. Furthermore, the x−o−z cross-sectional images of the isolated beads at the bottom left of Fig. 3(a) demonstrate the enhanced optical sectioning capability of 3DSIM, effectively eliminating out-of-focus background both above and below the focal plane. The WF and 3DSIM intensity profiles of the fluorescent beads along the white line in the x−o−y and x−o−z planes are illustrated at the bottom right of Fig. 3(a). In addition, the image decorrelation method25 was used to assess the resolution. The results revealed a lateral resolution of 263 nm in WF [Fig. 3(b)] and 133 nm in 3DSIM [Fig. 3(c)], showcasing a nearly twofold enhancement compared to WF. We also used PFSj26 on the images of the beads in Fig. 3(a) to evaluate the axial resolution of our system and found that 3DSIM can achieve a twofold resolution improvement in the axial direction, from 601 nm to 300 m. Subsequently, dot-like samples of nuclear pore complex resembling fluorescent beads were imaged under the same acquisition timing settings. Figure 3(c) showcases the WF and 3DSIM images of the nuclear pore complex within the cell nucleus. Similarly, 3DSIM improves the resolution in all three dimensions compared to WF and effectively eliminates the defocus of the background, enabling a comprehensive interpretation of the entire nuclear structure.

We utilized 3DSIM to image more intricate subcellular structures with finely detailed 3D features encompassed mitochondrial cristae and outer membranes, microtubule proteins, and actin filaments. Figures 4(a) and 4(b) show WF and 3DSIM images showcasing the mitochondrial cristae and outer membrane, respectively. It can be seen that the 3DSIM image provides a distinct view of the intricate internal structure of the mitochondrial cristae, while WF cannot [see Fig. 4(a)]. Furthermore, the 3DSIM image of the mitochondrial outer membrane exhibits higher resolution compared to WF, with a reduced impact in the defocused background [see Fig. 4(b)]. Furthermore, we conducted imaging of two linear subcellular structures, namely actin and tubulin. Figure 4(c) shows the imaging results for tubulin in COS7, where individual microtubules can be traced and observed throughout the entire cell volume, and many parallel microtubules can be distinctly resolved as separate entities. These findings demonstrate the superior capability of 3DSIM in revealing fine details and enhancing resolution for subcellular structures. In addition, we introduce polarization dimension27^–29 on the x−o−y plane, namely, polarized superresolution 3DSIM imaging techniques (p3DSIM), to investigate the subcellular structure of actin filament in U2OS with unprecedented resolution and polarization sensitivity in Fig. 4(d). p3DSIM offers a clearer insight into the orientation and alignment of the actin filaments: the ensemble orientation of the dipoles is approximately parallel to the direction of the filaments, contributing to a deeper understanding of their functional organization within the cellular context. It is noteworthy that with intensity calibration, the dipole orientation will be more accurately resolved by 3DSIM, and Sec. S7 in the Supplementary Material shows the intensity calibration of different angles in our 3DSIM system. What is more, we performed the comparison among WF, 2DSIM, and 3DSIM to demonstrate the advantage of 3DSIM in Sec. S8 in the Supplementary Material, and the comparison between DMD-based 3DSIM (DMD-3DSIM) and SLM-based 3DSIM(SLM-3DSIM) in Sec. S9 in the Supplementary Material.

We employed 3DSIM to image thick plant and animal tissues with a stronger defocus background. Figures 5(a)–5(c) present the WF and 3DSIM results of oleander leaves, black algal leaves, and corn tassels, respectively. In the 3DSIM images, distinct features become apparent that were not observable in conventional WF images. These include the 3D distribution of cell walls in oleander leaves, the hollow structures within black algal leaves, and the periodic aggregation and dispersion of structures in the root tips of corn tassels. In addition, we further analyzed the orientation of fluorescent dipoles within actin filaments in the mouse kidney tissue slice in Fig. 5(d). In the maximum projection image obtained from WF of the mouse kidney slices, the presence of out-of-focus scattered signals and the inability to distinguish in-focus information resulted in a less pronounced visualization of the filamentous structure. However, 3DSIM endows it with superior optical sectioning capabilities, presenting a clear representation of actin filaments, due to the higher resolution. Moreover, we utilized polar 3DSIM to investigate again the alignment of fluorescent dipoles within actin filaments in 8.5μm-depth mouse kidney tissue sections. Our findings demonstrated a prevailing parallel orientation of the dipoles relative to the filament axis. In addition, Figs. 5(g)–5(j) and Sec. S10 in the Supplementary Material show the spatial distribution of these samples in a 3D manner, effectively highlighting the advantages of 3DSIM in enhancing resolution and removing the out-of-focus background. Furthermore, Supplementary Video 1 of black algal leaves and Supplementary Video 2 of actin filaments in the mouse kidney tissue slice accompany the paper, illustrating the 3D reconstruction capabilities of 3DSIM, and providing a detailed visualization of angles of view.

Lastly, we use different 3D deconvolution algorithms to prove that computational superresolution technology can further improve the 3D resolution of our 3DSIM approach. We use 3D Richardson–Lucy (RL3D) deconvolution30 for the postprocessing of the 3DSIM image of 100 nm beads as shown in Fig. 6(a), finding that RL3D can further improve 3D resolution compared with 3DSIM, as the profiles in Fig. 6(b) show. We use sparse deconvolution31 to do the postprocessing of 3DSIM results of clathrin-coated pits (CCPs) in Fig. 6(c). Although 3DSIM can interpret the 3D hollow structure of CCPs, sparse deconvolution can make the hollow structure clearer. This is consistent with the physiological structure of CCPs,32 and similar results were reported with 3D single-molecule localization microscopy.33 Then, we use MRA deconvolution34 for the processing of tubulin structure of the low signal-to-noise ratio in Fig. 6(d). We can find that the artifacts of 3DSIM caused by the defocus and noise can be greatly suppressed using MRA, with an improved 3D resolution. These results show that our solution is suitable for many postprocessing algorithms, which can further improve the resolution and quality of 3DSIM reconstruction.

First, due to the limitation of experimental conditions (we do not have a live cell incubation system in our custom-built microscope), our current DMD-based 3DSIM setup can only perform single-color imaging with a fixed specimen. But we can further introduce other lasers to incident DMD at different angles to realize multicolor imaging without change for the most part of the system, as referred to in our proposed four-color DMD-based SIM concept.35 Meanwhile, regarding the potential applications of DMD-3DSIM for real-time and dynamic live cell imaging, it is better to equip the system with a microscope body and live cell incubator for spatial and temporal stability. And the fast switch of EOM and DMD exploits the potential to conduct the imaging of fast-moving living cells with the help of these improvements.

Second, in our DMD-based 3DSIM system, we conducted tests to measure the maximal data acquisition speed for single-layer 3DSIM with varying field-of-view (FOV) sizes in synchronous readout trigger mode (Sec. S11 in the Supplementary Material). We can achieve the maximum 24frame/s imaging when the FOV is 512×512 in 3DSIM modality, which depends largely on the readout and exposure time of the sCMOS because the switching time of DMD and EOM is several magnitudes higher than sCMOS. Furthermore, we performed 3DSIM imaging of tubulin in COS7 cells at the maximum illumination power with progressively decreasing exposure times (Fig. S6 in the Supplementary Material). However, when exposure times are further reduced (indicating faster imaging), the acquired raw data may exhibit inadequate signal-to-noise ratios, resulting in excessive reconstruction artifacts or even rendering the reconstruction impossible. Hence, we conclude that several other factors can influence the acquisition speed of multilayer 3DSIM data in practical experiments, even with the coordinated optimization of hardware and software. These include the characteristics of the illumination source (laser power and stability are crucial, as they affect signal-to-noise ratios), sample characteristics (fluorescent samples with high and stable brightness perform better in fast imaging), and sample mounting and stability (any instability in the sample stage can lead to a longer acquisition time).

Third, although we have used various deconvolution algorithms to optimize the images (both sparse and MRA deconvolution use the 2D OTF without considering the complex defocus background), advanced 3D algorithms36^,37 are still required to faithfully reconstruct and optimize low signal-to-noise ratio data acquired from high-speed live cell imaging.

In summary, we demonstrated our DMD-based 3DSIM system as a fast and reliable tool for subcellular structures, tissue architectures, and fluorescent dipole imaging with a 3D spatial resolution twice that of WF, and a computational superresolution algorithm can further improve the resolution of our system. Our system features the advantages of fast switching and accurate polarization modulation, opening up a new avenue for exploration and providing an invaluable tool for unraveling the complex mechanisms underlying fundamental biological processes.

Yaning Li is a PhD student in the Department of Biomedical Engineering, College of Future Technology, Peking University, China. Her research interests include two-dimensional and three-dimensional structured illumination microscopy based on digital micro-mirror devices.

Ruijie Cao received his BS degree from Nanjing Normal University in 2022. Currently, he is a PhD candidate in the College of Future Technology, Peking University. His research interests include hardware and software of structure illumination microscopy.

Wei Ren received his BS degree from North University of China in 2020. Currently, he is a PhD candidate in the Department of Biomedical Engineering, Peking University. His research interests include super-resolution microscopy and mitochondrial dynamics.

Yunzhe Fu received his BS degree from Nanjing University of Science and Technology in 2021. Currently, he is a PhD student in the Department of Biomedical Engineering, Peking University. His research interests include the study of multiple subcellular organelle interactions using multimodal ultrafast low phototoxicity super-resolution microscopy.

Yiwei Hou received his BS degree from the University of Electronic Science and Technology of China in 2022. Currently, he is a PhD student in the Department of Biomedical Engineering, Peking University. His research interests include computational fluorescence imaging and structured illumination microscopy.

Suyi Zhong received her BE degree from Central South University in 2018 and her ME degree from Tsinghua University in 2021. Currently, she is a PhD student at the College of Future Technology, Peking University, Beijing, China. Her research interests include light-sheet microscopy and lensfree microscopy.

Karl Zhanghao received his BS degree from Peking University in 2012 and his PhD from Peking University and Georgia Institute of Technology. He is a research assistant professor in the Department of Biomedical Engineering, Southern University of Science and Technology. His research interests include super-resolution microscopy, multidimensional live-cell imaging, and fluorescence polarization microscopy.

Meiqi Li is an engineer at the School of Life Sciences, Peking University, China. She received her PhD from the Department of Biomedical Engineering at Peking University, and her BS degree in automation from the Harbin Institute of Technology. Her research is focused on structured illumination microscopy and fluorescence polarization microscopy.

Peng Xi is a Boya professor at the College of Future Technology, Peking University, China. His research interest is on optical super-resolution microscopy. He has been awarded the National Distinguished Young Scholar and the fellow of IAAM. He is the chief scientist of the Key R&D Plan of the Ministry of Science and Technology. He has published over 90 scientific journal papers on high impact journals including Nature, Nature Methods, etc., with > 6000 citations.