| Literature DB >> 29953344 |
Abstract
Fluorescence light microscopy is an indispensable approach for the investigation of cell biological mechanisms. With the development of cutting-edge tools such as genetically encoded fluorescent proteins and superresolution methods, light microscopy is more powerful than ever at providing insight into a broad range of phenomena, from bacterial fission to cancer metastasis. However, as with all experimental approaches, care must be taken to ensure reliable and reproducible data collection, analysis, and reporting. Each step of every imaging experiment, from design to execution to communication to data management, should be critically assessed for bias, rigor, and reproducibility. This Perspective provides a basic "best practices" guide for designing and executing fluorescence imaging experiments, with the goal of introducing researchers to concepts that will help empower them to acquire images with rigor.Entities:
Mesh:
Year: 2018 PMID: 29953344 PMCID: PMC6080651 DOI: 10.1091/mbc.E17-05-0276
Source DB: PubMed Journal: Mol Biol Cell ISSN: 1059-1524 Impact factor: 4.138
FIGURE 1:Imaging experiment workflow schematic.
Checklist of parameters to consider in image acquisition.
Check for autofluorescence using a “no transfection,” a “no antibody,” or a “no dye” control Control for antibody specificity with a no primary antibody control Reduce or account for bleed-through signal Account for or reduce photobleaching Monitor cell health and phototoxicity |
Confirm that the light source is fully aligned and evenly illuminating the sample Choose an appropriate objective lens (e.g., chromatically corrected) Minimize changes in filter sets to prevent shifts due to mechanical changes Check overlay and registration of channels in the software (use Tetraspeck beads) Monitor/control for lamp and/or laser intensity Double-check software settings/metadata before analysis: scaling, acquisition parameters, timestamps, etc. Use the correct size coverslip (most microscope objectives use no. 1.5 coverslips which are 0.17 mm thick), or use an objective lens with a correction collar adjusted to the thickness of your sample |
Avoid saturation Increase dynamic range to obtain best contrast Use the Shannon-Nyquist criterion for optimal spatial and temporal sampling Increase signal by
○ using bright, stable fluorophores ○ choosing a high NA objective ○ increasing light intensity (but watch out for photobleaching and phototoxicity) ○ choosing the optimal filter sets ○ matching refractive indices ○ using lowest magnification objective Decrease noise by
○ using cell culture media without phenol red or riboflavin ○ decreasing detector gain ○ eliminating ambient light ○ averaging frames on a laser scanning confocal |
Monitor factors such as temperature, carbon dioxide concentration, humidity, pH, and air circulation, where applicable Maintain consistent focus/Z-depth, light intensity, sample preparation from session to session |
FIGURE 2:Proper sampling is critical for obtaining highly resolved data. A Xenopus laevis stage 9 (7 hpf) embryo stained for tubulin and histone H3 with Alexa Fluor 488 and 568 was imaged on a Zeiss LSM 780 confocal with a 20×/1.0 NA water immersion objective. (A) Top panel shows the full field of view with no zoom; scale bar = 50 μm. Bottom panel shows an inset region of interest (ROI) as marked by the white box; scale bar = 20 μm. Images on the left were imaged at 512 pixels × 512 pixels. Images on the right were imaged using Shannon-Nyquist sampling at 3488 × 3488. The bottom-left image is an example of undersampling or aliasing. (B) Left panel shows the raw image acquired. Right panel shows an enhanced image, where the brightness of the entire image has been increased for both channels to allow for increased visibility.
Checklist of items to include in a detailed Methods section.
□ Microscope (Make, Model) □ Inverted or upright □ Objective: manufacturer, magnification, numerical aperture, immersion, correction (if any) □ Light source(s) □ Filters, dichroic mirrors, beam splitters □ Additional hardware used, e.g., stage motor, incubation chamber and set-up, Piezo stage or objective □ Acquisition software and settings □ Confocal, Multiphoton systems:
○ Detector type (PMT, NDD, etc.) ○ Laser line(s) used ○ Pixel resolution ○ PMT gain □ Widefield systems (with cameras):
Camera manufacturer, model Note if binning, gain was used □ Separate, detailed transfection and antibody staining protocols, including constructs used, antibody manufacturer(s) and concentrations □ For multi-channel acquisitions, note whether channels were acquired simultaneously or sequentially □ Strategy for selecting regions of interest (if any) □ Image processing steps (if any) □ Data analysis pipeline, including statistical methods (if any) □ Software used to make figures, including processing steps, if any (inversion, brightness & contrast, maximum intensity projection, etc.) |
FIGURE 3:For multichannel images, present each channel individually in grayscale and use color for merged images. Bovine pulmonary artery endothelial (BPAE) cells were stained with DAPI (4′,6-diamidino-2-phenylindole) to mark DNA and Alexa Fluor 488 phalloidin to mark actin microfilaments (Thermo Fisher; FluoCells Prepared Slide #1) and imaged on a Zeiss LSM 880 confocal with a 63×/1.4 NA oil immersion objective. Scale bar = 20 μm.
FIGURE 4:Alternative forms of representing three-dimensional data. An unstained Drosophila melanogaster eye (Carolina Biological Supply Company) was imaged on a Zeiss LSM 880 confocal microscope with a 20×/1.0 NA water immersion objective. Autofluorescence in the GFP channel was detected following excitation with the 488 nm argon laser. A 60-μm-thick z-stack (89 slices) was acquired. (A) A maximum intensity projection of the z-stack rendered by Zen software (RRID:SCR_013672). (B) Depth color coding of the z-stack (Zen), with blue indicating zero depth and red representing the deepest section (∼60 μm). (C) MIP of the z-stack tilted inside of a volume box, generated using Bitplane Imaris software (RRID:SCR_007370). Scale bars = 50 μm.