We present phase correlation imaging (PCI) as a novel approach to study cell dynamics in a spatially-resolved manner. PCI relies on quantitative phase imaging time-lapse data and, as such, functions in label-free mode, without the limitations associated with exogenous markers. The correlation time map outputted in PCI informs on the dynamics of the intracellular mass transport. Specifically, we show that PCI can extract quantitatively the diffusion coefficient map associated with live cells, as well as standard Brownian particles. Due to its high sensitivity to mass transport, PCI can be applied to studying the integrity of actin polymerization dynamics. Our results indicate that the cyto-D treatment blocking the actin polymerization has a dominant effect at the large spatial scales, in the region surrounding the cell. We found that PCI can distinguish between senescent and quiescent cells, which is extremely difficult without using specific markers currently. We anticipate that PCI will be used alongside established, fluorescence-based techniques to enable valuable new studies of cell function.
Cells exhibit complex dynamic behavior across broad spatial and temporal scales1. In recent years, it has become increasingly clear that studying the cytoskeleton and its dynamic properties is central to understanding the physics of living cells throughout the cell cycle2. Actin, microtubules, and intermediate filaments are polymers that not only offer mechanical support to cells, but also act as tracks along which intracellular transport takes place3. Trafficking of vesicles and organelles along cytoskeletal structures inside cells is expected to be a combination of both diffusive and molecular-motor-driven processes4,5. In order to study the transport of discrete objects in the cell, e.g. vesicles, particle tracking has become a routine method6,7,8. However, the cell contains many extended objects or continuous media, such as actin filaments and microtubules, which, when viewed on scales larger than their mesh size, cannot be decomposed into discrete traceable objects. Thus, the spatiotemporal fluctuations of such continuous media cannot be investigated by particle tracking. To address this limitation, we have recently developed dispersion-relation phase spectroscopy (DPS)5,9,10 and dispersion-relation fluorescent spectroscopy (DFS)4,11, in which the continuous distribution of dry mass density or fluorophore density, respectively, is studied with a continuous model, in the frequency domain.
Currently the diffusion of fluorescently-tagged molecules is typically measured by fluorescence correlation spectroscopy (FCS)12,13,14,15,16,17 or fluorescence recovery after photobleaching (FRAP)18,19,20,21, in which the spatial scale is fixed by the excitation beam size. Image correlation spectroscopy (ICS)22, spatiotemporal image correlation spectroscopy (STICS)23, and raster image correlation spectroscopy (RICS)24 have been also successfully developed to infer information about fluorophore transport. STICS is complementary to ICS as it allows measuring velocity rather than just magnitude. RICS extends ICS to faster diffusion temporal scales. While very powerful, these methods are based on fluorescence imaging and, thus, are subject to phototoxicity and photobleaching limitations, which place a practical limitation on long time-scale studies. An ideal method for understanding spatiotemporal fluctuations in the living cell would cover broad scales, ~1–105 nm spatially and ~1–105 s temporally, which points to the need for label-free methods. In the past decade, quantitative phase imaging (QPI) has emerged as a promising approach to study cell structure and dynamics in a label-free manner25. Because it combines microscopy, interferometry, and holography, without exogenous contrast agents, QPI can be used to study cells over arbitrary time scales, from milliseconds to weeks26,27,28,29,30,31,32,33,34,35.
In this article, we present phase correlation imaging (PCI) as a label-free method based on QPI aimed at studying cell dynamics in a spatially-resolved manner. PCI outputs quantitative maps of the correlation time associated with fluctuations in the cell’s refractive index. We show that this information can reveal the diffusion coefficients of Brownian particles, without the need for particle tracking. The PCI investigation of cellular dynamics offers a detailed view of various compartments of the cell, such as in the nucleus, characterized by different time constants. PCI is extremely sensitive to mass density fluctuations at the femtogram scale26, which in turn report on the local dynamic properties of the cellular material. Here we show that PCI can quantify the change in actin dynamics when its polymerization is blocked by drugs and reveal that actin dynamics are subdominant at small spatial scales. Furthermore, we find that the distribution of correlation times is qualitatively different for quiescent and senescent cells, allowing us to classify these cell types with a label-free approach.
For imaging unlabeled live cells, we employed Spatial Light Interference Microscopy (SLIM)36,37,38,39, which is a QPI method based on phase contrast microscopy and white light illumination. Due to its broadband illumination, SLIM provides optical pathlength measurements with sub-nanometer sensitivity both spatially and temporally38. SLIM operates as an add-on module to a commercial phase contrast microscope (Fig. 1a), as described in more detail in Supplementary Information. In essence, our optical system makes the phase contrast objective ring appear tunable, such that one can control the phase shift between the scattered and unscattered field. In order to obtain a quantitative phase image, we record four intensity images corresponding to phase shifts that are π/2 apart40. Our SLIM system yields up to 12.5 quantitative phase images per second at 5.5 megapixels per frame. From the acquired time-lapse sequence, we calculate the correlation time at each pixel as illustrated in Fig. 1b and detailed in the Supplemental Information. The correlation time, τ0, is defined as the decay time of the temporal autocorrelation function associated with the phase fluctuations. The dynamics of the phase fluctuations report on the mass transport in the cell, as the phase map is linearly proportional to the dry mass density of the cell26,41. Large values of τ0 indicate slower processes, while short values denote fast dynamic regions in the cell. PCI carries the spirit of fluorescence lifetime imaging42, in the sense that it reveals information encoded in the time axis, which is not accessible from static imaging.
As illustrated in Fig. 1, the contrast in PCI and, thus, the ability to visually differentiate between various sub-cellular components, is determined by the difference in the dynamic properties of structures as well as the difference in optical path length. To demonstrate the ability of PCI to resolve fine sub-cellular structures, beyond what is visible from just phase images, we imaged A549 human adenocarcinoma alveolar basal epithelial cells and generated PCI maps (see Supplemental Information for details on the calculation). The cells were imaged in phenol red-free cell culture medium under physiological conditions (37° C and 5% CO2) with a 40X/0.75NA objective at an acquisition rate of 8 frames/s for up to 4 minutes (1,920 frames total). Representative quantitative phase images and the corresponding time correlation maps for A549 cells are shown in Fig. 1c–f. The correlation time maps, τ0(x, y), were obtained from the temporal autocorrelation function over sets of 100 phase images. Sliding the 100 frame set across the entire stack of 1,920 phase images, we obtain PCI maps that are time-resolved (see Supplemental movies S1 and S2). Figure 1e shows an example of a PCI map and Fig. 1f represents a more detailed image of the nuclear region selected in Fig. 1e. Clearly, the PCI maps are complementary to the phase images, as can be seen perhaps most noticeably in the nucleus. Low phase values can correspond to high τ0 values and vice versa, as the highest phase values are not necessarily the most stable. The complementarity between the SLIM and PCI maps can be seen on overlaid images in Supplementary Figs 1 and 2. The PCI maps show that the nucleus is much more fragmented from a dynamic point of view than can be glimpsed from the static, morphological images. The dynamics of nuclear material is a subject of intense research at the moment, especially in the context of gene expression43,44 and messenger RNA (mRNA) transport45,46. It is likely that PCI can become a valuable tool for studying such dynamics of crowded environments. Supplementary Videos 1 and 2 illustrate how PCI can provide complementary information to existing fluorescence approaches.
When applied to a suspension of particles under Brownian motion, we show that PCI yields the diffusion coefficient quantitatively. In order to demonstrate this capability, we imaged the Brownian motion of 1 μm polystyrene spheres in highly concentrated (99%) glycerol to mimic the viscous intracellular environment. We acquired 256 SLIM images with a 40X/0.75NA objective at an acquisition rate of 1 frame/s. Figure 2a shows a representative phase image from the time series and Fig. 2b the PCI map calculated from the entire time sequence. For Brownian motion, the dispersion relation dictates a quadratic relationship between the bandwidth, Γ, and spatial frequency, q, namely, Γ = Dq2 (see, e.g., ref. 5). Since the information is spatially-resolved in PCI, we pick a particular spatial frequency, q0, around which we band-pass the PCI map, retrieve the average bandwidth from the image, Γ0, and obtain the diffusion coefficient as . Specifically, we computed Γ from the PCI image, which was band-passed around q0 = 8 rad/μm, and plotted the histogram of these bandwidth values (see Fig. 2c). The mean Γ value from the distribution is Γ0 = 0.097 rad/s, as indicated in Fig. 2c. As a result, the diffusion coefficient from the PCI measurement is D = (1.56 +/− 0.15) × 10−3 μm2/s. For comparison, the dispersion relation4,5, Γ vs. q, is shown in Fig. 2d. The quadratic fit yields a value for the diffusion coefficient, D = (1.4 +/− 0.12) × 10−3 μm2/s, which agrees well with the PCI result. Furthermore, the PCI result agrees closely with an independent particle tracking result, which yielded D = 1.6 × 10−3 μm2/s5.
Furthermore, we applied PCI to quantifying the dynamics of A549 lung cancer cells (Fig. 3). Band-passing the PCI map around q0 = 6 rad/μm we obtained the histogram of Γ values and its mean, Γ0 = 4.92 rad/s, resulted in a diffusion coefficient D = 0.14 μm2/s (see Fig. 3c). The dispersion relation curve shows that, indeed, at short scales (2π/q0 ≤ 1 μm), the mass transport in the cell is diffusive. The fit with the quadratic function yielded D = 0.13 μm2/s, which compares very well with the PCI value. These results indicate that PCI can provide the diffusion coefficient of Brownian motion in both continuous and discrete media, without particle tracking or fluorescent markers. Our approach may become a useful complementary technique to methods such as fluorescent speckle imaging47.
Next we demonstrate that PCI can provide unique insight on cytoskeletal dynamics (Fig. 4). We studied the lamellipodia dynamic transformations in glial cells upon treatment with cytochalasin-D (cyto-D), which is known to inhibit actin polymerization48. The cell culture preparation is described in more detail in Supplemental Section 5. We collected two sets of 512 SLIM images, at 1 frame/s acquisition rate, one before and another immediately after the treatment. Figure 4a–f, respectively, show the results before and after the cyto-D treatment. The ruffling lamellipodia are highlighted by PCI as regions of high τ0 (Fig. 4b), indicating slow dynamics. The correlation time values, of tens of seconds (Fig. 4c) are consistent with the rates of actin polymerization previously reported in the literature, e.g., 24 s in ref. 47. It is interesting to note that large τ0 values are exhibited at large spatial scales, as dictated by the dispersion relation. This is exhibited in Fig. 4c, in which we low-passed filtered the image in Fig. 4b by blurring (convolving) it with a Gaussian kernel of 3 μm standard deviation. In this representation, the lamellipodia dynamic is evidenced as a “crown” surrounding the cell. Interestingly, after adding cyto-D, this region of high values disappeared completely, as shown in Fig. 4f. The visual difference between the treated and un-treated cells in the correlation time map is striking, with a shift from longer times at the edges in the untreated cells to longer times in the middle in the treated cells. The actin polymerization block leaves actin predominantly in the monomeric state, evidenced here by the complete loss of the large scale ruffling at the cell periphery. The reduction in polymeric actin is characterized by much faster transport, without large scales correlations. We should clarify that, although τ0 is computed at short spatial scales, the τ0-map may contain both large and small scale features. For example, if a medium is homogeneous, the resulting τ0-map is constant, characterized by zero-spatial frequency, although each τ0-value was calculated as a high-spatial frequency quantity.
We tested whether PCI is capable of distinguishing between subtle differences in the dynamics of quiescent and senescent cells. It is believed that cells in general and stem cells in particular, adopt the quiescent state to preserve key functional features49. Quiescent cells exit the cell cycle, but retain the ability to re-enter the cell cycle and undergo division. Therefore, during quiescence, cells (QC) can transit between a cycling and a resting state depending upon the signal they receive from the microenvironment. However, cellular senescence (SC) is distinct from QC, as it occurs in response to DNA damage or other cellular stress and, therefore, the cell cycle arrest is irreversible50. Typically senescent and quiescent cells are distinguished using the β-galactosidase assay, which requires fixation of cells51. Our label-free technique allows following the cells for long time periods and determining the timeline (phase of the cell cycle when the effect occurs, number of divisions before the treatment is effective) and status of cell cycle arrest (QC or SC) as a result of different treatment protocols50. Using SLIM, we imaged WI-38 human fibroblasts derived from lung tissue. The cells were assessed for QC and SC and compared with proliferating asynchronous cells. We imaged QC and SC cells, obtaining time-lapse stacks of 256 SLIM images, at 10 frames/s. We computed the correlation time maps for nine quiescent and nine senescent cell (see Supplemental Section 6 for details on the procedure). In Fig. 5a, we show the representative SLIM images of two different quiescent cells, and their respective correlation time maps, as indicated. Similarly, in Fig. 5b we show the SLIM images and their corresponding correlation time maps for two different senescent cells. The phase images and respective PCI maps for the additional seven quiescent and seven senescent cells are shown in Supplemental Figs S 3 and 4. To gain better insights into the nature of correlation times for the quiescent and senescent cells, we computed the probability density functions p(τ0) of the correlation time maps for each of the nine sets, which is normalized such that . The distributions associated with the QC and SC cells are shown in Fig. 6a,b, respectively (the τ-axis is logarithmic for simpler visualization). From these plots, it is evident that the distributions of τ0 (x, y) for SC cells are qualitatively broader than those of the QC cells. These findings suggest that SC cells are more likely to undergo slower intracellular trafficking than the QC counterparts. In order to quantify the spread, we computed the standard deviation (STD), inter-quartile range (IQR) and median absolute deviation (MAD) of τ0 (x, y) for each dataset (see Supplemental Section 6 for details). The median values over the nine sets for each group are shown in Fig. 6c. From these results, we can infer that senescent cells have greater variability in τ0 values, and thus higher probability of occurrence for longer correlation times. By comparison, such long-term processes are relatively rare in the quiescent cells, characterized by faster transient phenomena. These results underscore the ability of PCI for understanding the nature of temporal processes within quiescent and senescent cells and for studying cell phenotype classification.
Summary and Discussion
We introduced a new approach for studying cell dynamics in a spatially-resolved manner. Phase correlation imaging operates on a similar principle with FLIM, in the sense that it maps spatially a parameter of dynamic relevance, the correlation time, τ0(x, y). Of course, unlike FLIM, PCI is label-free, because it exploits fluctuations in quantitative phase images due to intracellular mass traffic. Qualitatively, the correlation maps reveal dynamic subdomains in the unlabeled cells, which are independent of the morphology maps obtained from single frames. However, perhaps the most appealing feature of PCI is that it provides quantitative information from dynamic systems. For example, PCI can be used to size particles undergoing Brownian motion, essentially converting the light microscope into a dynamic light scattering instrument. Furthermore, the size of the particles can be below the resolution limit of the microscope, because PCI does not require particle tracking.
Of course, like all QPI techniques, PCI provides noninvasive investigation at the expense of specificity. However, the SLIM instrument used here has the ability to overlay the correlation maps with the fluorescence channels present in the microscope, thus providing specific ques whenever needed. Note also that the correlation time calculation is based on the inherent assumption of wide-sense stationarity, meaning that the statistical properties of the second order statistics (autocorrelation, spectrum, their moments) do not change in time. Thus, the PCI measurement must be taken over time scales that are much shorter than any scale over which the cell undergoes massive dynamic, nonstationary changes. For example, during mitosis the τ-map should be extracted from time lapse data that is much faster than, say, the one-hour interval associated with cell division.
The τ0 maps associated with live cells are essentially high-spatial frequency representation of the dispersion relation and, as a result, reports on the diffusive component of the intracellular traffic. Thus, a map of diffusion coefficients can be obtained quantitatively. This type of diffusion-weighted imaging of cells has the potential to underscore inhomogeneity in the mass transport at the subcellular scale. It is particularly interesting that PCI is sensitive to the integrity of actin. We measured significant changes in the τ0 maps due to the cyto-D block and these modifications occur predominantly at large scales. These results indicate that PCI can contribute to the field of cytoskeleton dynamics, alongside established techniques, such as fluorescence speckle imaging44.
Due to the nanometer sensitivity to optical pathlength changes, PCI reports on extremely subtle changes in the cell dynamics map. As an example of this capability, we showed that PCI can distinguish between that quiescent and senescent cells based on their characteristic probability density of correlation time. Such assessment is essentially impossible based on morphology alone. The common method for classifying these two types of cells relies on specific fluorescent markers. Future studies will be dedicated to analyzing dynamic variability across cell populations, for example, during the differentiation process. It will be extremely interesting to study the interplay between morphology and dynamics, structure and function, during stem cell differentiation.
It has become apparent in the past decade that quantitative phase imaging (QPI) is emerging as a valuable approach to cell biology, especially due to its label-free operation and quantitative data. The ability to combine QPI with current fluorescent techniques will be crucial for its adoption in the main stream use. Such multimodal imaging provides the benefits of both worlds: specificity associated with fluorescence, with the absence of photoxicity and photobleaching QPI. One exciting avenue is to use fluorescence as a cue for the specific structure of interest and co-localize that structure in QPI. This way, the cell dynamic behavior can be monitored over arbitrarily large temporal scales.
Materials and Methods
Spatial Light Interference Microscopy (SLIM)
SLIM is an add-on module that transforms an existing phase contrast microscope into a quantitative phase imaging system. As detailed in the Supplemental Information, SLIM operates by effectively turning the objective pupil ring into a tunable phase shifter, modulating this filter 4 times in increments of quarter wavelength, and collecting independent intensity images. The final quantitative phase image is obtained by combining the 4 intensity frames. SLIM preserves the diffraction resolution and all the existing channels of the microscope (e.g., fluorescence).
Computing the correlation time maps
Using a time-lapse SLIM data set, the correlation time, τ0, is calculated at each pixel in the field of view via the variance of the temporal autocorrelation function, τ0(x, y)2 = <(x, y)>2 (see Supplemental Information for details). The bandwidth map is an entirely equivalent quantity that can be inferred from τ0 as Γ = 2π/τ0.
Dispersion-relation phase spectroscopy (DPS)
The dispersion relation connects the spatial and temporal frequencies associated with the fluctuations in a SLIM time series. Thus, the temporal bandwidth for each spatial mode, q, has the form Γ(q) = qΔv + Dq2. The fit with the linear and quadratic term in q, yield the width of the velocity distribution and the diffusion coefficient, respectively (see Supplemental information for details).
Live cell imaging
The specific procedure for each cell type is described in the Supplemental information.
How to cite this article: Ma, L. et al. Phase correlation imaging of unlabeled cell dynamics. Sci. Rep. 6, 32702; doi: 10.1038/srep32702 (2016).
This work was supported by the National Science Foundation (CBET-0939511 STC, DBI 14-50962 EAGER, IIP-1353368). The authors would like to thank Drs. H. Rex Gaskins and Matthew Leslie for preparing A549 lung cancer cells. LM acknowledges that this manuscript has been co-authored by UT-Battelle, LLC under Contract No. DE-AC05-00OR22725 with the U.S. Department of Energy. For more information, visit http://light.ece.illinois.edu/