Abstract
More than a decade ago genetically encoded calcium indicators (GECIs) entered the stage as new promising tools to image calcium dynamics and neuronal activity in living tissues and designated cell types in vivo. From a variety of initial designs two have emerged as promising prototypes for further optimization: FRET (Förster Resonance Energy Transfer)-based sensors and single fluorophore sensors of the GCaMP family. Recent efforts in structural analysis, engineering and screening have broken important performance thresholds in the latest generation for both classes. While these improvements have made GECIs a powerful means to perform physiology in living animals, a number of other aspects of sensor function deserve attention. These aspects include indicator linearity, toxicity and slow response kinetics. Furthermore creating high performance sensors with optically more favorable emission in red or infrared wavelengths as well as new stably or conditionally GECI-expressing animal lines are on the wish list. When the remaining issues are solved, imaging of GECIs will finally have crossed the last milestone, evolving from an initial promise into a fully matured technology.
INTRODUCTION
Genetically encoded calcium indicators (GECIs) have come of age. Since the first demonstration of FRET (Förster Resonance Energy Transfer)-based prototypical sensors such as the Cameleons (Miyawaki et al., 1997, 1999) and the first single fluorophore calcium sensors (), these two major classes have evolved high performance variants in which signal strength was optimized in iterative steps of improvements and validation. Among FRET based sensors Cameleons, which exploit the interaction of Calmodulin with the binding peptide M13 as a calcium sensing mechanism, saw several rounds of improvements of their signal strength (Nagai et al., 2004; ). Troponin C has been used as a more biocompatible alternative to Calmodulin in FRET sensors (). These sensors also underwent several rounds of engineering (Mank et al., 2006, 2008). Among single fluorophore sensors GCaMP type sensors (Nakai et al., 2001) became the most popular class, chosen from several initial architectures. Variants with ever increasing sensitivity to neuronal activity were generated (Ohkura et al., 2005, 2012a; Tian et al., 2009; ), as were blue and red emitting color variants (Zhao et al., 2011; ; Ohkura et al., 2012b). Finally, large scale mutagenesis and screening approaches have resulted in GECIs that match or even exceed the in vivo sensitivity of the synthetic calcium dye OGB-1, often referred to as a standard against which response properties of new GECIs were compared to (; Thestrup et al., 2014).
Genetically encoded calcium indicators finally made it possible to label specific types of neurons in vivo and even allowed targeting to subcellular compartments and repeated imaging of identified neurons over long periods of time. For several small genetically tractable organisms with strong body walls or cuticulae such as in Caenorhabditis elegans or Drosophila, which made access and loading of dyes from the outside challenging, expression of GECIs was the only feasible way to image neuronal activity. In many aspects imaging of GECIs has thus become a well-established technology that enables experiments that previously were not possible.
What is the ideal GECI for imaging neuronal physiology? Obviously this will depend on the experimental situation and the neuronal cell types to be imaged. Nevertheless, a number of general criteria may be derived that a GECI should strive to include in the ideal case. (i) It should be bright enough to identify expressing cells even at rest, allow an estimate of the amount of indicator expressed in a given cell after gene transfer, and possibly reveal fine details of its architecture. (ii) It should be readily expressed at sufficient levels by the standard methods for gene transfer and transgenesis. (iii) It should exhibit a linear relationship between the changes in free calcium and the fluorescence change of the indicator. (iv) For reporting neuronal activity it should be sensitive enough to faithfully report small calcium elevations due to firing of single action potentials (APs) in single trials in vivo, ideally at lower magnification and faster scanning rate to sample large numbers of neurons. (v) It should not perturb cells that express the indicator by buffering of physiological calcium or other unwanted biological side effects. (vi) It should minimize artifacts due to specimen movement, photobleaching, or other perturbing causes. (vii) Finally, it should have sufficiently fast binding kinetics to accurately follow calcium fluctuations, if it is used as a reporter of neuronal activity.
In view of these criteria we will discuss some of the current issues in quantifying neuronal signals with GECIs and point to some further desirable improvements to finally turn imaging of GECIs it into a mature, fully fledged technology for the study of neuronal function.
QUANTIFYING NEURONAL ACTIVITY WITH GECIs – DEALING WITH NON-LINEARITY
The biochemical and optical properties of the latest generation of GECIs rival and in some aspects even surpass those of synthetic calcium indicators (; Table 1). It is now possible to detect the somatic calcium influx associated with individual APs with high reliability in vivo. Even calcium signals following synaptic activation can now be monitored chronically in live animals (). Yet, in one point most GECIs are clearly inferior to their synthetic counterparts: linearity with respect to the actual calcium concentration. Indicator non-linearity renders the direct deduction of absolute changes in calcium from the relative changes in fluorescence challenging. Robust quantification with the commonly used calibration methods is only possible in the ‘linear’ regime of a calcium indicator (; Neher, 1995; Maravall et al., 2000; Yasuda et al., 2004), well below its Kd value (Figure 1A). Only in this range the fluorescence intensity (or fluorescence ratio) change ΔF/F or ΔR/R of the indicator is approximately proportional to the cellular Ca2+ concentration ([Ca2+]i). Most synthetic indicators with linear response curves (Hill coefficient ∼1) show a simple saturation function of ΔF/F or ΔR/R vs. [Ca2+]. The saturation fluorescence Fmax in response to [Ca2+] > > Kd is used together with the indicator fluorescence Fmin at zero [Ca2+] to calibrate the fluorescence response:
Table 1
| Indicator | Fluorophore(s) | Ca2+ sensing domain | in vitro KD (nM) | Hill slope | Rise (s) | Decay(s) | Single AP(ΔF/F or ΔR/R) | Description | Reference |
|---|---|---|---|---|---|---|---|---|---|
| Synthetic | |||||||||
| OGB | Oregon green | BAPTA | 260 | 1.48 | 0.24a 0.09b | 0.38a 2.11b | 10.0 ± 0.9%j 5.2 ± 0.9%k | High linearity; high baseline brightness; fast kinetics; acute usage (<12 h) | , , Tada et al. (2014) |
| Cal-520 | – | BAPTA | 320 | – | 0.06b | 0.69b | 18.8 ± 0.8%k | Latest generation synthetic indicator | Tada et al. (2014) |
| Single FP | |||||||||
| GCaMP3 | cpEGFP | Calmodulin | 345–660 | 2.1–2.5 | 0.08c | 0.61c 0.64d | 7.9 ± 2.8%j 17.4 ± 3.5%n | – | Tian et al. (2009), , |
| GCaMP5G | cpEGFP | Calmodulin | 450–460 | 2.5 | 0.15e | 0.61e | – | – | , |
| GCaMP5K | cpEGFP | Calmodulin | 189 | 3.8 | 0.06f | 0.27f | 3.6 ± 1.9%l | High affinity; High non-linearity | , |
| GCaMP6 | cpEGFP | Calmodulin | 158 | – | – | 0.46d | 27.9 ± 4.5%n | – | Ohkura et al. (2012b) |
| GCaMP8 | cpEGFP | Calmodulin | 200 | – | – | 0.43d | 37.8 ± 5.2%n | – | Ohkura et al. (2012b) |
| GCaMP6f | cpEGFP | Calmodulin | 375 | 2.27 | 0.14e 0.05f | 0.38e 0.14f | 19 ± 2.8%l | Medium–high affinity; low baseline brightness; faster kinetics | |
| GCaMP6m | cpEGFP | Calmodulin | 167 | 2.96 | 0.14e 0.08f | 0.87e 0.27f | 13 ± 0.9%l | High affinity; low baseline brightness; intermediate kinetics | |
| GCaMP6s | cpEGFP | Calmodulin | 144 | 2.90 | 0.16e 0.18f | 1.14e 0.55f | 23 ± 3.2%l | High affinity; low baseline brightness; slower kinetics | |
| FRET | |||||||||
| YC3.60 | ECFP/cpVenus | Calmodulin | 250 | 1.7 | 0.82g | 0.73g | 2.0 ± 0.09%k 5.5 ± 1.2%m | – | Nagai et al. (2004), , , Lütcke et al. (2010) |
| YC-Nano15 | ECFP/cpVenus | Calmodulin | 15.8 | 3.1 | – | ∼ 4h | 10.4 ± 1.9%m | High affinity; high baseline brightness; slower kinetics | , Thestrup et al. (2014) |
| TN-XXL | ECFP/cpCitrine | Troponin | 800 | 1.5 | 1.04g | 0.88g | 1.6 ± 0.3%n | – | Mank et al. (2008), Thestrup et al. (2014) |
| Twitch2B | mCerulean3/ cpVenus | Troponin | 200 | 1.31 | – | 2.11i | 26.5 ± 3.8%o | High linearity; high baseline brightness; slower kinetics | Thestrup et al. (2014) |
| Twitch3 | ECFP/cpCitrine | Troponin | 250 | 1.42 | – | 2.05i | 5.7 ± 0.7%p | High linearity; high baseline brightness; slower kinetics | Thestrup et al. (2014) |
Comparison of current generation genetically encoded calcium indicators (GECIs) for in vivo usage with OGB.
Overview of parameters describing the function of the commonly used GECIs, their predecessors and the ‘golden standard’ OGB.
KD measured by stop-flow measurement using purified protein.
Rise and decay:
aSingle exponential fit (τrise, τdecay), 40 APs (20 Hz) in drosophila larval neuromuscular junction (NMJ) .
bRise time (10-90), decay time constant from double exponential fit to single AP in acute brain slices of mouse barrel cortex Tada et al. (2014).
cHalf-rise time (t1/2), half-decay time (t1/2) for 10 APs (83Hz) in hippocampal slice culture Tian et al. (2009).
dSingle exponential fit (decay τ1/2), 1 AP in hippocampal slice culture Ohkura et al. (2012b).
eFull-rise time, half-decay time (t1/2), 20 Hz in drosophila larval NMJ .
fFull-rise time, half-decay time (t1/2) for single AP induced signals in mouse V1 in vivo or .
gSingle exponential fit (τrise, τdecay), 80 APs (40 Hz) in drosophila larval NMJ or Mank et al. (2008).
hSingle exponential fit (τdecay), for 10 APs (20 Hz) in mouse brain .
iSingle exponential fit (τdecay), for 10 APs (83 Hz) in dissociated hippocampal culture Thestrup et al. (2014).
Single AP ΔF/F or ΔR/R measured in:
jMouse M1 or S1 in vivo or Tian et al. (2009).
kMouse barrel cortex in vivoLütcke et al. (2010) and Tada et al. (2014).
lMouse V1 in vivo.
mMouse cortex, acute brain slices Lütcke et al. (2010) or .
nHippocampal slice culture Mank et al. (2008) and Ohkura et al. (2012b).
oAcute cortical slice Thestrup et al. (2014).
pDissociated hippocampal culture Thestrup et al. (2014).
FIGURE 1
However, if the Hill coefficient of the binding curve diverges strongly from 1 the assumptions underlying Eq.1 are violated (Figure 1A).
Owing to four cooperative calcium-binding sites in most GECIs, response curves frequently are highly non-linear. For example, Hill coefficients of recent GCaMP5 or six variants range from 2.5 to 4 (
An additional complication for the quantitative use of GECIs is that it is not clear if the non-linear relation of F or R and calcium is constant, especially considering the variable expression levels over time and between subjects. The result is that the same absolute change in calcium may lead to highly variable changes in fluorescence depending on the actual resting calcium concentration (Figure 1A). As a result of this variability, establishing a ‘ground truth’ of single AP-evoked fluorescence in order to infer spike rate and timing from the fluorescence data is challenging: since it is unclear from which resting calcium level single AP transients are arising, generalizing a single waveform of this unitary event to an entire population of cells can be problematic. Of course, when the indicator affinity is high enough so that the calcium changes of interest largely fall in the linear range of the indicator, reliable spike inference should be possible. Careful in situ calibrations of indicator fluorescence change vs. simultaneously measured cellular activity under realistic indicator expression levels and imaging conditions need to be performed in order to deduce reliable spike timings from non-linear GECI data. In these cases one should consider if more linear ratiometric GECIs would provide a better quantifiable alternative. To increase the accuracy of methods for calcium measurement and AP inference, reducing calcium-binding sites as performed with recent ratiometric “Twitch” calcium sensors (Thestrup et al., 2014) should be a design goal for other future GECI developments.
BUFFERING AND EXPRESSION LEVEL
All calcium indicators act as calcium buffers. Therefore, expression of any type of GECI will inadvertently change the spatio-temporal dynamics of this ubiquitous secondary messenger. The degree to which an exogenous buffer affects cellular free calcium ([Ca2+]i) is well understood and largely depends on three main factors: its mobility, affinity (including binding rates), and concentration (Zhou and Neher, 1993; Neher, 1995;
If one aims at monitoring neuronal activity, i.e., calcium signals associated with APs or synaptic activation, one can either choose to minimize the effect of exogenous buffer on endogenous calcium signaling by minimizing the indicator concentration, or to maximize the SNR of the readout of calcium activity by finding the indicator concentration that yields optimal SNR.
Under ideal (i.e., photon shot noise limited) conditions, the measure of confidence that one can attribute to a change in fluorescence given the intrinsic variability in the measurement due to the Poisson statistics of light detection (i.e., the SNR), is directly proportional to the indicator’s signal change over baseline fluorescence (i.e., ΔF or ΔR) and to the square root of the baseline fluorescence signal (Yasuda et al., 2004;
In the case of ratiometric indicators, the relative shot noise components of donor and emission fluorescence add so that for the same relative change in fluorescence ratio from a comparable baseline fluorescence level the SNR is worse than for single fluorophore GECIs that require only one noise-affected measurement. However, since FRET indicators are typically much brighter at rest this disadvantage is largely compensated (but see Wilt et al., 2013). Increasing the concentration of a calcium indicator increases F and thereby improves SNR because more fluorescent molecules become available. Yet, a larger buffer concentration will also lead to a smaller fluorescence change: When the indicator is trying to bind more calcium than is entering the cell while at the same time competing with endogenous calcium buffers, the number of indicator molecules changing their emission from the baseline level decreases. The amplitude (ΔF orΔR) and decay time constant (τ) of the calcium-dependent fluorescence change depend on the summed buffer capacity of the exogenous and endogenous buffers (
where κendo represents the buffer capacity of the endogenous buffers (fixed or mobile) and κdye represents the exogenous buffer capacity of the added calcium dye. The buffer capacity (or ‘binding ratio’) is the constant describing the fixed ratio between changes in free [Ca2+] and buffer-bound [CaB] calcium, which can be related to the effective dissociation constant (Kd) and concentration [B]tot of the respective buffer (Zhou and Neher, 1993; Neher, 1995):
What would be the optimal indicator concentration (or GECI expression level) to maximize SNR? F0 is proportional to κdye and by substitution in Eq. 2 one yields (
It follows that maximal SNR is achieved under ‘balanced loading’ conditions where the endogenous and exogenous buffer capacities are equal (κendo= κdye;
INDICATOR KINETICS
It had been noticed early on that the response kinetics of GECIs were slower than that of synthetic calcium dyes. Early prototypical Cameleon-1 had a measured on-rate kon of about 106 M-1 s-1 compared to essentially diffusion-limited on-rates of 108 M-1 s-1 for fura-2 or fluo-3 (
Neurons in the mammalian CNS exhibit a wide range of firing rates, from sparse activity below 0.1 Hz (e.g., L2/3 cells in the barrel cortex,
FIGURE 2

Ratiometric imaging of neuronal activity in an awake mouse using the Twitch-2B calcium indicator. Two-photon imaging of layer II/III excitatory neurons, conditionally expressing Twitch-2B (CAG promoter, double-floxed inverted open reading frame, 28 days after transduction by AAV1) together with Cre-recombinase (CamKII promoter, AAV1), in V1 of an awake head-restrained mouse on a treadmill (see, e.g.,
RATIOING VERSUS SINGLE CHANNEL RECORDING
The two major classes of GECIs operate in different read-out modes. While single GFP-based sensors are imaged using a single channel for recording fluorescence, FRET-based indicators are ratiometric and require splitting the emitted light into two channels that are recorded separately and the ratio of the two emission channel intensities taken as a measure of calcium concentrations. An example of a ratiometric in vivo recording can be seen in Figure 2. The indicator Twitch-2B was expressed in mouse primary visual cortex and ratiometric imaging of the activities of a group of neurons performed in awake mice. Both types of procedures have distinct advantages and disadvantages. Recording with a single channel is simpler and allows collecting all photons emitted from a probe, without any loss from emission filters or beam splitters. Such probes also occupy less bandwidth of the spectral range, allowing more multiplexing and co-labeling of neuronal cell types with different colors. Ratiometric, FRET based probes use two fluorescent proteins as fluorophores, and therefore occupy a larger area of spectral bandwidth for a given sensor. Ratioing has, however, a number of advantages if quantification of neuronal activity is desired. The ratio formed between the two channels is, in principle, independent of expression levels. Thus, heterogeneities in indicator expression levels between cells, as occur with AAV-mediated gene delivery into the brain (
SEGMENTATION
The main objective of calcium imaging experiments is to monitor neuronal activity via variations in fluorescence. Having performed the experiment, the next step is to make sense of the fluorescence data. Traditional methods involve hand-picking a region of interest (ROI) in the anatomy and finding the fluorescence time-series within this ROI. This method can easily be implemented when sparse labeling makes it straight forward to manually segment the anatomical ROI and is particularly useful in experiments where the experimenter knows what particular ROIs are of interest in order to answer questions such as: Is this specific neuron active in my experiment?
In certain cases though, it is more appropriate to use an automated method to select ROIs, in particular when seeking an unbiased, large-throughput way of processing the data. These methods can be said to fall roughly into two categories, those that use anatomical information and those that use functional data for the segmentation. We briefly discuss both below.
Anatomical segmentation methods greatly rely on the specimen being imaged and the labeling of the tissue. Issues such as whether the calcium indicator is expressed in the nucleus or the cytoplasm, whether the labeling is dense or sparse and whether neurons are morphologically similar or vary widely in shape and size all enter the design of the particular algorithm. In regions where the morphology of the anatomy is homogenous, algorithms can be quite effective. Figure 3A shows an example from the optic tectum of a larval zebrafish expressing GCaMP5G under the pan-neuronal promoter elavl3. The neurons have their cytoplasm labeled, are densely packed and of similar size. In order to perform automated segmentation, the anatomical image is spatially filtered with a filter whose width is in the order of the diameter d of a typical neuron, for example a Gaussian filter with standard deviation d. This removes local spatial inhomogeneities and emphasizes the important features that will be used for segmentation. In this case these are the bright cytoplasms, which can be used to identify boundaries between cells and the dark nuclei which can be used to identify the centers of the cells (Figure 3B, left). One may then perform a watershed algorithm on this image that will identify the “ridges” in this image, namely the bright cytoplasms. This will segment the image into ROIs, many of which will be individual cells (Figure 3B, right). By placing constraints on the morphology of these ROIs, such as a lower and upper limit on their size it is possible to ensure that most of the ROIs that are kept are actual neurons. The fluorescence time-series for all the ROIs can then be extracted using these ROIs as masks. Figure 3C shows this process for the 627 automatically segmented neurons in Figure 3B. These algorithms are not perfect. As can be observed in Figure 3B, right, they will fail to identify bona-fide neurons and will identify ROIs that are not actual neurons (akin to type II and type I statistical errors, respectively). By placing further constraints, errors can be minimized, but simple algorithms like the ones described are able to correctly identify a large fraction of neurons within seconds. These methods have been used (
FIGURE 3

Segmentation and whole-brain imaging. (A) Head of a 7-day-old larval zebrafish that was embedded in agarose and was presented with a visual stimulus: a dot moving at constant speed from left to right of its visual field and then back to the left. The red square shows the area that was imaged at 7.5 Hz in the medial optic tectum. Scale bar = 250 μm. (B) Anatomical image of the region imaged, generated by summing all the frames acquired in one plane (left). The image can then be automatically segmented using the methods described in the text (right). In this case 627 neurons were identified. Scale bar = 50 μm. (C) Raster plot of the responses of the 627 automatically segmented neurons in (B). (D) The method of computing the correlation of the fluorescence time-series of a pixel with its eight neighboring pixels is shown. This image can be used as a basis for determining functionally active cells by determining a threshold (following a shuffling-control) followed by segmentation. (E) How similar is activity during behavior across different animals? This question was addressed by imaging the whole brain of 13 behaving larval zebrafish discretized in over 500 × 800 × 400 voxels and then morphing the brains onto a reference brain (Portugues et al., 2014). Functionally active units were segmented using correlation-based methods described in the text. For every active voxel, how far on average must one look in other brains to find a similarly active voxel, i.e., one displaying similar activity patterns? The figure shows that in regions such as the ventral hindbrain neuropil, the cerebellum and certain retinal ganglion cell arborization fields, the answer is surprisingly less than 1 μm. Ro, rostral; L, left; R, right; C, caudal; scale bar = 50 μm.
A second class of algorithms involves functional segmentation. This idea relies on the fact that pixels that belong to the same neuron will have highly correlated fluorescence time-series. Naturally, if a neuron is not active, the time-series of the pixels that comprise it will involve mainly independent noisy fluctuations that will exhibit low correlation. These algorithms will therefore identify contiguous regions that are active in a correlated way. Explicitly the algorithms work as follows. For every pixel one can compute the correlation of its time-series with the sum of the time-series of its eight closest neighbors (in the case of 2D segmentation). This can be repeated for every pixel in the image, such that the result is an anatomical image of correlation values. In Figure 3D we perform this analysis for the same dataset as Figures 3B,C. This image can then be further processed in one of two ways (potentially following spatial filtering). The easiest way is to perform a threshold operation (set a threshold and set to 0 all the pixels with values below the threshold) and then identify particles within the thresholded image. In this case the threshold can be set either by hand, or more rigorously, by performing a shuffling control, comparing the distributions of the un-shuffled and the shuffled correlations and using the correlation value that implements a certain confidence interval of choice (i.e., this correlation value is 20 times more common in the un-shuffled versus the shuffled data).
Alternatively, the correlation image can be used to determine the seeds of a region-growing algorithm. The first step is to look for local maxima in the correlation image. The highest maximum is then used as a seed of the first ROI, and neighboring pixels are added to the ROI if their correlation with the already existing pixels in the ROI exceeds a threshold, which should ideally be determined by again performing a shuffled control. This process is repeated until no more pixels are aggregated and then one proceeds to the second highest maximum, which becomes the seed of the second ROI. It is once more possible to place constraints on the size and shape of these ROIs to ensure that certain requirements are met, for example, that they have the morphology of neurons. This method will only produce active ROIs, as opposed to the anatomical segmentation mentioned before, and has been recently used in (Portugues et al., 2014) to automatically identify 3D ROIs throughout the brains or larval zebrafish.
In the case of the dataset shown in Figures 3A–D, this method would not work particularly well to identify individual neurons, because many contiguous neurons are active and would be clumped into the same ROI. On the other hand, using this algorithm will identify activity in regions which are not morphologically different from their anatomical surrounding, such as neuropil.
No single method is superior to the others and which one should be implemented depends on many factors, such as the biological questions that need to be answered, the specific expression pattern of the indicator or the signal to noise of the measurement. These are by no means the only algorithms possible. Functional segmentation can be performed using maximum DF/F instead of correlation with neighboring pixels as a measure of activity and then centering ROIs that are the size and shape of typical neurons on the spatial locations of maxima that exceed a threshold (
CHRONIC IMAGING
Neuronal circuits adapt in response to sensory experience, mature during development and change due to disease processes in time scales which vary from milliseconds to months. While fast events are easily captured with electrophysiology techniques and imaging of synthetic calcium dyes, events that extended more than a few hours in time were up to now hard or impossible to follow due to technical limitations. Long term imaging of structural changes within the nervous system (see e.g.,
WHOLE-BRAIN IMAGING
The dream of a systems’ neuroscientist is to be able to record the spiking activity (the membrane potential would even be more preferable) of all the neurons in a brain while the animal is actively engaged in a behavior. Recent studies now show that this is a very real possibility, at least in certain model organisms.
The nematode C. elegans and the larval zebrafish are transparent organisms, small enough so that a large fraction of their nervous system fits within the field of view of an objective. They have cells that on average range from 3 to 10 microns in diameter, although C. elegans have 302 and zebrafish in the order of 150,000. Traditional approaches involving point scanning microscopy required several presentations of the same experimental paradigm per plane in order to determine the calcium response properties of the cells in the imaging plane. However, the signal to noise properties of the latest GECIs (
Scanning microscopy nevertheless has its limitations. The activity during single trial learning, for example, cannot be observed in every imaging plane. The nuclear targeting of calcium indicators and the implementation of more recently developed volumetric imaging techniques such as fast z-scanning with piezos (
OFF-TARGET EFFECTS OF GECIs
A major problem for previous GECIs has been that SNR-optimal indicator concentrations often could not be reached without leading to obvious signs of deterioration of cell health or compromises on indicator function. Indeed, already early versions of Cameleons showed sensor inactivation or formation of aggregates when expressed in transgenic mice (
FIGURE 4

Biocompatibility and off-target effects of GECIs. (A) Long-term high-level expression of a GECI (GCaMP6s) leads to breakdown of nuclear exclusion of the indicator. The number of ‘filled’ cells is a function of time after viral transduction (middle panel). Cells with ‘filled’ nucleus show atypical functional responses (right panel): neurons in primary visual cortex with ‘filled’ nuclei lose their orientation selectivity in response to moving grating stimulation. (B) GCaMP3 expression at moderate levels (∼15 μM) in CA1 neurons in rat hippocampal slice culture does not affect the early phase of long-term potentiation (LTP) in the short run. [Figures reproduced from
Either by means of changed expression strategies or serendipitous improvement of indicator properties, general cytotoxicity of the GCaMP family of indicators appears to have been reduced over time. Constitutive expression of GCaMP2 in mice led to unwanted phenotypes like cardiac hypertrophy (Tallini et al., 2006), whereas similar effects have not been noted for later conditional or neuron-specific GCaMP2, GCaMP3, and GCaMP5 transgenic mouse lines (
Stably or conditionally expressing animal models greatly simplify imaging by rendering invasive acute transfection methods unnecessary and by improving the repeatability of experiments. Probably even more importantly, they ameliorate issues resulting from the unavoidable ramping up of expression after viral transduction that render long-term chronic imaging of the same cell-populations problematic. Chronic imaging of stably expressing neuronal populations is indispensable, though, to study experience-dependent plasticity on the single cell level. Changes in intracellular calcium determine the sign and amplitude of synaptic plasticity (Shouval et al., 2002). GECI overexpression has therefore always been suspected to affect neuronal plasticity. While plastic changes during learning have now repeatedly been observed using chronic GECI expression over weeks (
REASONS FOR RED
The most recent optimization efforts in the field of GECI engineering are centered on expanding the spectral palette of high-performance GECIs. While indicators emitting in the blue range of the visible spectrum have been developed as well (Zhao et al., 2011), most work so far focused on the development of viable probes emitting in the red (Ohkura et al., 2012b;
CONCLUSION
Genetically encoded calcium indicators have come a long way since the presentations of the initial designs. Cycles of iterative improvements, biophysical, and structural analysis and testing have led to variants with ever increasing signal strength. Recent engineering efforts have also aimed at both lowering calcium buffering by the sensors and improving linearity of responses. Finally, large-scale mutagenesis and screening approaches have resulted in high performance variants in both FRET-based and GCaMP indicator families. In particular, these latter efforts provide a viable example for improving some of the other genetically encoded sensors that neuroscience is interested in, for example sensors of membrane potential. With the remaining issues clarified, as pointed out in this article, imaging of GECIs will finally become a tremendously valuable and mature set of tools for analyzing neuronal circuits and their plasticity and pathology.
Statements
Acknowledgments
Ruben Portugues would like to that Michael B. Orger and Claudia E. Feierstein for help with collecting data and extremely useful discussions. Tobias Rose, Pieter M. Goltstein, and Oliver Griesbeck acknowledge Pia Sipilä for support and helpful discussion. We all would like to thank the Max-Planck-Society for support.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
buffering, calcium, fluorescent protein, FRET, imaging, neuronal activity, segmentation
Citation
Rose T, Goltstein PM, Portugues R and Griesbeck O (2014) Putting a finishing touch on GECIs. Front. Mol. Neurosci. 7:88. doi: 10.3389/fnmol.2014.00088
Received
19 August 2014
Accepted
29 October 2014
Published
18 November 2014
Volume
7 - 2014
Edited by
Yoshiyuki Yamada, University of Geneva, Switzerland
Reviewed by
Johannes Hirrlinger, University of Leipzig, Germany; David J. Margolis, Rutgers University, USA
Copyright
© 2014 Rose, Goltstein, Portugues and Griesbeck.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Oliver Griesbeck, Max-Planck-Institute of Neurobiology, Am Klopferspitz 18, 82152 Martinsried, Germany e-mail: griesbeck@neuro.mpg.de
This article was submitted to the journal Frontiers in Molecular Neuroscience.
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