Submitted:
04 November 2026
Posted:
05 November 2026
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Abstract
Accurate spatiotemporal patterns of gene expression orchestrated by transcription factors (TFs) are fundamental to developmental progression. As such, the knowledge of biophysical properties of transcription factors (TFs) is crucial for understanding the mechanism of gene regulation. While fluorescence intensity, a commonly accessible parameter, gives an idea about relative bulk concentration, it provides an incomplete picture of eukaryotic transcriptional regulation owing to the involvement of a multitude of other factors in the process. The bulk concentration of TFs is composed of populations with distinct diffusivities, such as freely diffusing population with high diffusivity, DNA-bound population with low diffusivity, and population with intermediate diffusivity likely representing mobile clusters; each playing disparate but crucial roles in gene regulation. Biophysical parameters such as the diffusivity, concentrations of the distinct populations, as well as their spatiotemporal dynamics can shed light on mechanisms of TF mediated gene regulation. Here, we provide a detailed workflow spanning sample collection, sample preparation, image acquisition, and image analysis to quantify the aforementioned parameters in live Drosophila embryos using raster image correlation spectroscopy (RICS). The pipeline can be used to characterize the populations with distinct diffusivities and their variations over space and time for any protein of interest tagged with a fluorescent protein. In addition to the cross-correlation between a TF and DNA to characterize the TF-DNA binding, this pipeline can be extended to study protein-protein interactions by the cross-correlation between multiple proteins of interest by making use of spectrally distinct fluorescent tags. This quantitative approach is expected to enhance our mechanistic understanding of protein-based signaling networks.
Keywords:
drosophila embryos
; live imaging
; image analysis
; raster image correlation spectroscopy
; TF-DNA binding
; absolute concentration
Introduction
Transcription factors (TFs) play a crucial role in metazoan development by regulating spatiotemporal pattern of gene expression. This is achieved by TFs binding to the cis-regulatory elements in the DNA containing transcription factor binding sites. A quantitative description of the spatiotemporal dynamics is integral to understand the mechanism of transcriptional regulation. Recent advances in genome editing and live imaging have enabled the real time monitoring of TF expression patterns. The intensity obtained from such images provides an idea about the relative bulk concentration of the TFs. However, in eukaryotes, DNA is wrapped around histones forming nucleosome which act as a barrier to TF-DNA binding. As a result, chromatin structure also plays a role in TF occupancy [1,2]. Recent studies have also found that TFs may form transcriptional hubs that might enhance transcription by facilitating TF-DNA binding by increasing the local concentrations [3,4,5,6] and that TFs also form mobile clusters which might provide an efficient search mechanism for locating target genes [5,7]. As such, these clusters also serve as determinants of TF-DNA binding, and thereby gene regulation. Thus, although intensity measurements are easily attainable and generally reveal the spatial pattern of TF expression and relative changes over time, they do not give a complete picture of TF activity and binding. On the other hand, although recent advances in single-molecule imaging provided insights into the dynamics of transcription factors at transcriptional hubs, they do not tell us how the bulk-level properties of TFs are interpreted in hub formation, DNA binding, and thereby in gene expression. Measuring biophysical properties of the TFs, such as diffusion, binding, and absolute concentration allow us to chart out distinct TF subpopulations by their mobilities. In particular, quantification of the spatiotemporal dynamics of the freely diffusing, DNA-bound, and slowly-moving cluster subpopulations of TFs provides maps between bulk-level properties and binding, a crucial relationship for understanding TF-driven gene regulation.
Raster image correlation spectroscopy (RICS) analysis [8,9,10,11,12,13], a derivative of fluorescence correlation spectroscopy [14], allows the quantification of the properties using live embryo time series images acquired during the desired developmental stage [5,15,16]. Confocal images built by raster-scanning have a fast-scanning direction (pixel-to-pixel) and a slow-scanning direction (line retracing). RICS analysis uses intensity fluctuations of fluorescent protein-tagged molecules, correlated in time and space, to build an autocorrelation function (ACF) in two dimensions, corresponding to the fast (Δx) and slow (Δy) scanning directions. The amplitude of the ACF, A, is inversely proportional to the fluorescent protein concentration, while the shape of the ACF, especially in the slow direction, is determined by the fraction of fluorescent protein that is freely diffusible vs. that which is immobile. Furthermore, cross-correlations in the fluctuations between different fluorescent proteins, one tagged to a TF of interest and the other to His2Av, allow us to calculate the fraction of the TF that is bound to the same structure as the His2Av (likely to be DNA [17,18]). Therefore, RICS allows us to quantify not only the absolute concentration of GFP molecules, but also the fraction freely diffusible, the fraction immobile, and the fraction correlated to His2Av. This approach can be used to construct dose/response relationship between the concentrations of free and immobile TF populations which can elucidate how TF binding and thereby gene expression as well as the formation of clusters is dictated by free TF concentrations. Application of this approach in early Drosophila embryos improved our mechanistic understanding of timeline of activity of the pioneer factors Zelda and GAGA factor during zygotic genome activation [15], transcriptional interpretation of Dorsal and Bicoid morphogen gradients [5,16], and formation of DNA-bound and mobile clusters of the morphogen Dorsal [5].
Here, we provide a detailed workflow encompassing all the steps starting from Drosophila embryo collection, embryo preparation, embryo mounting, selection of microscope parameters, image acquisition and image analysis. This workflow can be easily followed to quantify the absolute concentrations and DNA binding of any protein of interest from live embryo images with sufficient spatial and temporal resolutions to enhance our understanding of the protein behavior and transcriptional regulation. This can be extended to find the cross-correlation between multiple proteins to study the protein-protein interactions in cellular signaling.
Materials
Fly lines
- Fly line having the protein of interest tagged with a fluorescent protein and histone tagged with a spectrally distinct fluorescent protein
- For tagged His2Av, existing stocks such as w[*]; P{w[+mC]=His2Av-mRFP1}II.2 (BDCS# 23651) for RFP tagged His2Av or w[*]; P{w[+mC]=His2Av-EGFP.C}2/SM6a (BDSC# 24163) for GFP tagged His2Av can be used. Lines with His2Av tagged with BFP are also available in the fly community [19].
Embryo collection
- Vials with molasses media (Archon Scientific, Catalog # B20101)
- Embryo Collection Cages (Flystuff® Drosophila Embryo Collection Cages, Genesee Scientific Catalog # 59-105)
- Petri dish (VWR Catalog # 10799-192)
- Grape juice agar
- Active dry yeast (VWR Catalog # 470303-062)
- Incubator that can be set to 25 °C
- Deionized water
Dechorionation
- Mesh basket with 1” inside diameter (Flystuff® Drosophila Mesh Baskets, Genesee Scientific Catalog # 46-102)
- Mesh with pore size 120 µm (Flystuff® Drosophila Mesh, Genesee Scientific Catalog # 57-102)
- Paint brush (size 1-2)
- Deionized water
- Bleach (Clorox® Concentrated Germicidal Bleach, VWR Catalog # 89501-620)
Sample mounting
- Paint brush (size 1-2)
- Stereo microscope
- Hair loop (prepared by looping a human hair and attaching it to a pipette tip with a piece of tape)
- Glass bottom dish, 35 mm Dish, No. 1.5 Coverslip, 20 mm Glass Diameter, Uncoated (Mattek, VWR Catalog # MSPP-P35G1520C)
- Deionized water
- Low melting point agarose (IBI Scientific, VWR Catalog # IB70050)
- Clear double-sided tape (Scotch, VWR Catalog # 500026-846)
- Heptane (VWR Catalog # MK513910)
- Microscope slides 75×25×1 mm (VWR Catalog # 16004-422)
- Cover glass 50×24×0.2 mm
- TetraSpeck beads (0.1 µm, T7279, Invitrogen)
- Ethanol (VWR Catalog # EM-EX0276-4S)
Imaging
-
Confocal microscope (LSM 900, Carl Zeiss, Germany) with
- ○
- 40x objective (C-Apochromat 40x/1.2 water immersion Korr objective)
- ○
- Lasers depending on the fluorescent proteins (488 nm laser for GFP and 561 nm laser for RFP)
- ZEN Microscopy Software
Image visualization and analysis
- Fiji (ImageJ)
- MATLAB R2024a (MathWorks)
Methods
Generation of fly lines
The protein of interest should be tagged with a fluorescent protein, preferably endogenously using techniques like CRISPR-Cas9 genome editing. We have shown that in attempts to generate fly lines with fluorescent protein tagged Dorsal, the presence of a DsRed marker in the 3’UTR of dorsal led to a reduction in dl mRNA levels, disrupted target gene expression, and reduced the viability of the fly lines [20]. Therefore, scarless removal of the selectable marker [21] is recommended to minimize locus disruption and to ensure wildtype behavior of the protein of interest.
If cross-correlation between two proteins is required, the proteins should be tagged with spectrally distinct fluorescent proteins. For observing nuclear morphology essential for proper staging, nuclear segmentation, and determining the DNA-bound population by cross-correlation, His2Av should be tagged with a fluorescent protein. The fly line with the tagged fluorescent protein of interest can be mated with a line having histone tagged with a spectrally distinct fluorescent protein such as w[*]; P{w[+mC]=His2Av-mRFP1}II.2 (BDCS# 23651) for RFP tagged His2Av or w[*]; P{w[+mC]=His2Av-EGFP.C}2/SM6a (BDSC# 24163) for GFP tagged His2Av to obtain embryos containing both the proteins.
Throughout this text, we will use the imaging of ventral midline of embryos expressing Dorsal-mNeonGreen and His2Av-RFP [5,20] as an example, unless otherwise specified.
Fly husbandry
- Flies are harvested on a standard cornmeal-molasses-yeast diet at a 25 °C incubator in room with 12 h light/dark cycle
- Embryo collection cages are set with flies required to produce embryos containing desired proteins of interest tagged with fluorescent proteins two days before imaging (Figure 1A)
- Yeast paste is prepared by adding and mixing deionized water with active dry yeast
- The grape juice agar plates are streaked with yeast paste (grape juice plate streaked with yeast paste are referred to as plates henceforth)
- The plate is placed on the bottom of the cage for oviposition
- The plates are changed twice every day for two days before imaging is started
- To remove any older eggs which are often retained by the females before deposition, a plate is placed in the cage for an hour of pre-egg laying session
- After one hour the plate is replaced with another plate to collect embryos for two hours.
- After the embryo collection, the plate is removed and replaced with another plate
- The deposited embryos should be appropriately aged by placing the plate in an incubator at 25 °C so the desired stage for the experiments is reached. For nuclear cycle 14, the embryos should be aged at 25 °C for two hours (Figure 1B).
Embryo preparation
- Mesh is placed inside mesh baskets for embryo collection
- After aging, the embryos are transferred to the mesh basket and rinsed with deionized water from a wash bottle that filters out any residual yeast paste (Figure 1C)
- A Petri dish is filled three-quarters full with fresh bleach
- The embryos contained in the mesh basket is submerged in the bleach for 30 seconds for dechorionation
- After 30 seconds, the embryos in the mesh basket are rinsed with about 250 ml deionized water from a wash bottle to make sure all the residual bleach is removed
- The mesh containing the washed and dechorionated embryos is removed from the basket (Figure 1D)
Embryo mounting
The embryos can be immobilized in either in microscope slides with coverslips (Figure 1E) or in a glass bottom dish (Figure 1F) depending on the nature of the acquisitions and the confocal microscope used. The microscope slides are convenient for both upright and inverted microscopes whereas the glass bottom dishes are preferred for inverted microscopes. The following steps are monitored using a stereo microscope.
Using slide with coverslip:
- To attach the coverslip and ensure the embryo does not get deformed between the slide and coverslip, two layers of the double-sided tape are attached to both ends of the slide, approximately half an inch from the edge, excess tape is cut to match the slide width
- Heptane glue is prepared by submerging 5 cm of double-sided tape in about 5 ml heptane contained in a glass vial and shaken overnight at room temperature to dissolve the glue from the tape [22]
- About 100 µl of the heptane glue is applied on the slide in a thin layer in the area between the tapes on the same side as the tape
- Dechorionated embryos are transferred from the mesh to the heptane glue layer on the slide using a paintbrush
- About 5 µl of deionized water is pipetted on each embryo
- The embryos are covered with a coverslip
Using glass bottom dish:
- The dechorionated embryos are transferred from the mesh to the glass bottom dish using a paintbrush
- Each embryo is covered with 3-5 µl of 1% low melting point agarose solution stored at 42 °C
- The agarose is allowed to solidify for about one minute
- Once the agarose pads covering the embryos are solidified, a thin layer of water is poured over the solidified agarose to avoid drying
If dorsoventral orientation is relevant, the desired side of the embryo to be imaged (dorsal or ventral or an intermediate coordinate) should face the coverslip which can be ensured by rotating the embryo using the paintbrush or a hair loop.
Image acquisition
- Appropriate immersion medium is used on the objective. In this case, a drop of water is pipetted on the 40x/1.2 objective
- The sample in the slide or glass bottom dish is placed on the microscope stage
- The focus is adjusted to view the surface of an embryo at appropriate stage
-
Imaging parameters are selected
- ○
- Image is acquired by raster scanning where the laser moves unidirectionally, forming the image by linear scanning followed by line retracing
- ○
- Frame size 1024 pixels by 1024 pixels
- ○
- Pixel size of 31.95 nm obtained at 5x zoom
- ○
- Pixel dwell time of 2.06 µs, which results in a frame time of 5.06 s
- ○
- 0.2% laser power are selected for both 488 nm laser and 561 nm laser. Laser power should be selected based on the intensity observed in both the channels for the proteins of interest and should be balanced to improve the signal-to-noise ratio but minimize photobleaching.
- The focus is adjusted to view the nuclei on the surface of the embryo.
- Time series acquisition is started after selecting the microscope parameters.
- Time series acquisition of at least 12 frames is taken per region of interest (ROI)
- If a longer time course is needed, the ROI can be moved to a different part of the embryo expected to have similar behavior as those in the current ROI
-
Owing to the higher surface area of the embryo along anteroposterior (AP) direction compared to that in the dorsoventral (DV) direction, it is possible to move the ROI to a location along the AP direction after each acquisition.
- ○
- For ubiquitously expressed proteins, this enables long time course to be obtained with minimal photobleaching
- ○
- If the protein shows DV variation but no AP variation, a similar long time course is enabled by moving along the AP direction. And for observing the spatial variation along DV, embryos mounted at different DV coordinate need to be imaged
- ○
- If the protein shows AP variation but no DV variation, by changing the location of the ROI, the spatial variation along AP is obtained. If a long time course is needed at a particular AP position, photobleaching correction should be considered if a high laser power is used.
Image acquisition and analysis for the determination of Point Spread Function
- 70% ethanol is added to diffraction-limited TetraSpeck beads for a 1:1000 dilution.
- The beads are uniformly suspended by sonicating in water bath for 20 minutes.
-
The suspension is mounted following the same procedure as embryos:
- ○
- Using glass bottom dish: 5 µl of the suspension is added to the glass bottom dish and it is allowed to dry. 1% low melting point agarose solution is added over the dried sample and allowed to solidify. Then a thin layer of water is added over the agarose.
- ○
- Using slide with coverslip: 5 µl of the suspension is add to a slide and it is allowed to dry. 5 µl of water is added over the dried sample and covered with a coverslip.
- Same objective and microscope settings are used to obtain the images as mentioned in the point 4 of Image acquisition.
- An ROI is selected in which the beads are sparsely distributed far apart one another.
- z-stack is acquired with the imaging volume extending beyond the beads on both sides to include regions with minimal fluorescence signal. Each slice is separated by 0.05 microns, yielding around 80 slices in total.
- Three acquisitions are taken per batch of the mounted beads by repositioning the ROI to previously unimaged areas.
- The acquisition is repeated for three batches of mounted beads.
-
For the PSF analysis, open the “run_fitPSF3D.m” file. The script calls the function “fitPSF3D.m” which loads the images in the specified file path, detects the fluorescent beads in the specified channel, fits a 3D Gaussian function to each bead, and saves the fitted parameters in the specified output folder path.
- ○
- The beads are detected in the average z projection image. The center of each bead (x and y coordinates) and the z-slice with the maximum intensity for each bead are used as an initial guess for the Gaussian fitting using lsqcurvefit. The fitted parameters include the bead center coordinates along each axis, standard deviations along each axis, amplitude, and background intensity. These parameters for each .czi file are saved in separate .mat files in the output folder. An average z-projection image for each CZI file is also saved as a .tif file.
Image analysis
- Open the “sc_main.m” file. This script will run the code to load the images, segment nuclei from the images, calculate the ACFs and CCFs, and fit a series of biophysical models to the ACFs and CCFs.
- The top of “sc_main.m” contains a series of editable options, including the image path and filename, size of the point spread function (PSF), background subtraction and image stabilization flags, the sliding window size for image grouping and averaging, and the channel numbers for the data and mask channels. A guess of the diffusivity of mobile components can also be chosen. The default values for everything except the image path and filename are pre-filled.
- The first block of code loads the image series. If the background subtraction and stabilization flags are set to “true,” these processes will also occur in this block of code. If the image series is tiled, the frames from each tile will be grouped into separate elements of a cell variable in Matlab.
- In the second block of code, the nuclei are segmented in the image. To increase robustness, groups of 7-12 frames are averaged together and the segmentation is performed on the averaged image. The nuclear segmentation mask is eroded by 0.5 microns to provide a conservative estimate of the nuclei, decreasing the probability of false positives. Similarly, the complement of the pre-eroded mask is the cytoplasmic mask, which is then also eroded by 0.5 microns to provide a conservative estimate of the cytoplasm.
- In the next block of code, the ACFs and CCF are calculated for each time point. The time points may consist of different tiles in the image or of groups of 7-12 image frames. ACFs are calculated for the total, nuclear, and cytoplasmic fractions of the data channel, and for the nuclear fraction of the nuclear channel. The CCF between the data and nuclear channel is calculated for the nuclear fraction.
-
The next block of code fits the ACFs, or portions of the ACFs, to three models, resulting in estimated parameters:
- ○
- First, the fast direction of each ACF is fit to a Gaussian-shaped model of the PSF. This allows us to infer the amplitude of each ACF, which in turn allows us to infer absolute concentrations of the fluorescent species.
- ○
- Second, each full ACF is fit to a pure diffusion model, allowing us to estimate an effective overall diffusivity. This model is typically inaccurate as most species contain a mixture of mobile and immobile components.
- ○
- Third, each full ACF is fit to a two-component model, which accounts for a potential mixture of a single mobile component and one immobile component. This model estimates the fraction of the immobile component and the diffusivity of the mobile component. This fit may not accurately identify the diffusivity, as in some cases, it is unidentifiable. It is recommended to set a moderate value of the diffusivity, such as 3-5 μm2/s.
- The next block of code fits the CCF to a model specific to the CCF. As the CCF includes cross-correlation between a TF and histone, and likely represents TF bound to DNA, this model assumes a near-zero diffusivity. This model includes corrections for differences in volume and centroid location of the PSFs of the two imaged wavelengths. This model allows us to estimate the fraction of the TF that is bound to DNA.
-
The final block of code produces a plot of the results
- ○
- For single time point acquisitions, the resulting plots include the ACFs and the CCF, and annotates the plots with the estimated model parameters (absolute concentration, diffusivity, immobile fraction, DNA-bound fraction).
- ○
- For time course acquisitions, the resulting plots include the estimated model parameters as functions of time.
- The final output data, including nuclear segmentation masks, ACFs, CCFs, image metadata (czi path and filename, image size, time step, pixel dwell time, etc.) and the chosen analysis flags (background subtraction, stabilization, etc), are stored as a structure variable. A separate structure variable, which also stores the image metadata and chosen flags, is produced that contains the estimated parameters. These two structures are kept separate due to the large size of the ACFs and CCFs stored in the first structure variable.
- If multiple image series are analyzed, the above structure variables for each image series should concatenated for visualization purposes (see below).
- Visualization of results
- To produce a plot of averages of the estimated parameters from either multiple time course acquisitions, or multiple acquisitions at different spatial locations, run “sc_extract_RICS_timecourse.m” or “sc_extract_RICS_spatialorientation.m”, respectively.
- For visualization of time courses, run “sc_extract_RICS_timecourse.m”. This script will first load the concatenated structure variable containing the time courses of estimated parameters (including absolute concentration, diffusivity, immobile fraction, DNA-bound fraction of the TF). In the beginning of the script, you must specify the path to a mat file containing this structure variable. The script then calls “extract_RICS_timecourse”, which outputs a structure variable that contains the time course of estimated parameters, averaged across all embryos. Error bars are also calculated. You can set a flag to have the error bars represent standard deviation or standard error of the mean. You can also set a flag to have the script plot the averaged time courses.
- For visualization of spatial variation, run “sc_extract_RICS_timecourse.m”. This script largely parallels the script discussed in the previous point. It will first load the concatenated structure variable containing the estimated parameters (including absolute concentration, diffusivity, immobile fraction, DNA-bound fraction of the TF) for each RICS acquisition. In the beginning of the script, you must specify the path to a mat file containing this structure variable. You must also supply the spatial location for each acquisition. The script outputs a structure variable that contains the estimated parameters, binned into different spatial locations. Error bars for each bin are also calculated. As with the previous script, you can set a flag to have the error bars represent standard deviation or standard error of the mean. You can also set a flag to have the script plot the binned values of the parameters.
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Figure 1.
Sample preparation for imaging. A Population cage with a desired fly line for embryo collection on grape juice plates streaked with yeast paste. B Grape juice plate is removed from the cage after the embryos have been collected. C The collected embryos are washed form the plate into a mesh basket using deionized water and dechorionated using bleach. D The mesh with the washed dechorionated embryos is removed from the basket. E The dechorionated embryos can be mounted on a slide and covered with a coverslip. F The dechorionated embryos can be mounted on a glass bottom dish and embedded in low melt agarose (left) and then covered with deionized water (right). Depending on the experimental requirements and microscope setup either method E or F can be used for embryo mounting.
Figure 1.
Sample preparation for imaging. A Population cage with a desired fly line for embryo collection on grape juice plates streaked with yeast paste. B Grape juice plate is removed from the cage after the embryos have been collected. C The collected embryos are washed form the plate into a mesh basket using deionized water and dechorionated using bleach. D The mesh with the washed dechorionated embryos is removed from the basket. E The dechorionated embryos can be mounted on a slide and covered with a coverslip. F The dechorionated embryos can be mounted on a glass bottom dish and embedded in low melt agarose (left) and then covered with deionized water (right). Depending on the experimental requirements and microscope setup either method E or F can be used for embryo mounting.

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