Probe, Sample, and Instrument (PSI): The Hat-Trick for Fluorescence Live Cell Imaging

: Cell Imaging Platforms (CIPs) are research infrastructures offering support to a number of scientiﬁc projects including the choice of adapted ﬂuorescent probes for live cell imaging. What to detect in what type of sample and for how long is a major issue with ﬂuorescent probes and, for this, the “hat-trick” “Probe–Sample–Instrument” (PSI) has to be considered. We propose here to deal with key points usually discussed in CIPs including the properties of ﬂuorescent organic probes, the modality of cell labeling, and the best equipment to obtain appropriate spectral, spatial, and temporal resolution. New strategies in organic synthesis and click chemistry for accessing probes with enhanced photophysical characteristics and targeting abilities will also be addressed. Finally, methods for image processing will be described to optimize exploitation of ﬂuorescence signals. stage


Introduction
Since the 1960s, the discovery of fluorescent proteins [1,2] has boosted live cell imaging studies and, consequently, technological developments for microscopy including simultaneous resolution improvement [3][4][5][6] and detector sensitivity [7,8]. In the early 2000s, European and also French (Infrastructure en Biologie, Santé et Agronomie, IBiSA) policies were established to identify emerging cell imaging platforms (CIPs) in which equipment, human resources, and skills are mutualized to facilitate broad access to advanced technologies. Economic reasons have also driven sharing strategies since the price for a commercial live cell imaging system starts around 100 k€ for a basic plate reader and reaches 1 M€ for a fully equipped STimulated Emission Depletion (STED) nanoscope. Frequently, CIPs are at the crossroads between molecular and cellular biology, chemistry, informatics, and engineering. By taking advantage of the diversity of projects and biological models studied on the Norman IBiSA CIP, the so-called PRIMACEN (Plate-forme de Recherche en IMAgerie CEllulaire de Normandie), On one hand, there is a large diversity of chemical and biomolecular strategies to construct new fluorescent probes with enhanced properties and specificities. In this review, we will focus only on organic fluorescent dyes including small organic fluorophores and fluorescent proteins; other fluorophores such as metal complexes [9][10][11], lanthanide complexes [12][13][14] and nanoparticles [15][16][17], fluorescent polymers [18,19], quantum dots [20][21][22], carbon dots [23], and nanoparticles [24,25] will not be detailed. On the other hand, localization or tracking of molecules, organelles, or cells in living cells, tissues, or organisms, without perturbing cellular processes, is an ongoing, fascinating research area [26]. Many methods for fluorescent labeling including diffusion of cell-permeable probes [27], uptake [28,29], injection [30], chemical and enzymatic reactions [31,32], genetic manipulation [31,32], and virus transfection [33] are now available. Indeed, the final choice of the labeling strategy depends on the cellular target but also on the experimental conditions, i.e., in vitro, ex vivo, or in vivo studies. In addition, probes and methods of labeling should also be adapted to prokaryotes or eukaryotes and to the presence of autofluorescence, siliceous structures, or walls. Finally, for live cell imaging, a dye should be excitable with a low-power light source and be detected with high-and stable-performance equipment but should not be cytotoxic and not bleach rapidly upon irradiation [34]. From nanoscopy to light sheet microscopy, there is a large variety of imaging systems and devices with spatial and temporal resolution ranges [6,[35][36][37][38][39]. These instruments are also adapted to the type of living sample and to the detection of low-to high-intensity signals. Therefore, photophysics of fluorescent organic probes, methods for cell and tissue labeling with a focus on click chemistry, progress in synthesis of small fluorescent organic molecules, and instrumental requirements for appropriate probe excitation and signal detection/analysis will be successively described in this review in the context of the PSI triad. On one hand, there is a large diversity of chemical and biomolecular strategies to construct new fluorescent probes with enhanced properties and specificities. In this review, we will focus only on organic fluorescent dyes including small organic fluorophores and fluorescent proteins; other fluorophores such as metal complexes [9][10][11], lanthanide complexes [12][13][14] and nanoparticles [15][16][17], fluorescent polymers [18,19], quantum dots [20][21][22], carbon dots [23], and nanoparticles [24,25] will not be detailed. On the other hand, localization or tracking of molecules, organelles, or cells in living cells, tissues, or organisms, without perturbing cellular processes, is an ongoing, fascinating research area [26]. Many methods for fluorescent labeling including diffusion of cell-permeable probes [27], uptake [28,29], injection [30], chemical and enzymatic reactions [31,32], genetic manipulation [31,32], and virus transfection [33] are now available. Indeed, the final choice of the labeling strategy depends on the cellular target but also on the experimental conditions, i.e., in vitro, ex vivo, or in vivo studies. In addition, probes and methods of labeling should also be adapted to prokaryotes or eukaryotes and to the presence of autofluorescence, siliceous structures, or walls. Finally, for live cell imaging, a dye should be excitable with a low-power light source and be detected with high-and stable-performance equipment but should not be cytotoxic and not bleach rapidly upon irradiation [34]. From nanoscopy to light sheet microscopy, there is a large variety of imaging systems and devices with spatial and temporal resolution ranges [6,[35][36][37][38][39]. These instruments are also adapted to the type of living sample and to the detection of low-to high-intensity signals. Therefore, photophysics of fluorescent organic probes, methods for cell and tissue labeling with a focus on click chemistry, progress in synthesis of small fluorescent organic molecules, and instrumental requirements for appropriate probe excitation and signal detection/analysis will be successively described in this review in the context of the PSI triad. Fluorescence proceeds through three successive steps, i.e., (1) absorption of a photon to reach nonstabilized excited states (Franck Condon states), (2) stabilization of the excited state by vibrational relaxation and internal conversion (IC) to populate the lowest excited state (Kasha State), and (3) radiative decay resulting in the emission of a photon. The absorption efficiency is described by the molar extinction coefficient ε defined by the Beer-Lambert law (Equation (1)). The ε value ranges from 10 4 cm −1 ·mol −1 ·L, for the less absorbing chromophores, to 10 6 for the commonly used fluorophores, depending of the nature of the transition involved.
A= ε(λ)lc (1) In Equation (1), A is the absorbance as a function of ε(λ), the molar extinction coefficient; l is the cuvette length in cm; and c is the concentration of the chromophore.
As the absorption process is extremely fast (<10 −15 s) [42], the molecules are considered motionless during the process leading to transient excited states (Figure 2A, Step 1). These states feature the same conformation as fundamental states but with distinct molecular orbital configurations. They quickly stabilize by vibrational relaxation leading to conformation change and then to internal conversion ( Figure 2A, Step 2) to the lowest excited energy state from which fluorescence will arise (Figure 2A, Step 3). The efficiency of the emission process is described by the fluorescence quantum yield (φF), which is the ratio between the number of emitted and absorbed photons (0 < φF < 1; Equation (2)). Indeed, the excited state may also decay through nonradiative processes such as internal conversion (IC) (Figure 2A, Step 4), resulting in heat release or intersystem crossing (ISC) (Figure 2A, Step 5) to populate the triplet state (T1). Perrin-Jablonski diagram containing three singlet states S0, S1, S2 and a triplet state T1. (B) UV-visible absorption and emission spectra. Molecular coordinates refer to molecular conformational evolution occurring during photophysical processes. ε molar extinction, IC internal conversion, ISC intersystem crossing, k F fluorescence rate constant, k ic internal conversion rate constant, ϕ F fluorescence quantum yield.
Fluorescence proceeds through three successive steps, i.e., (1) absorption of a photon to reach nonstabilized excited states (Franck Condon states), (2) stabilization of the excited state by vibrational relaxation and internal conversion (IC) to populate the lowest excited state (Kasha State), and (3) radiative decay resulting in the emission of a photon. The absorption efficiency is described by the molar extinction coefficient ε defined by the Beer-Lambert law (Equation (1)). The ε value ranges from 10 4 cm −1 ·mol −1 ·L, for the less absorbing chromophores, to 10 6 for the commonly used fluorophores, depending of the nature of the transition involved.
A= ε(λ)lc (1) In Equation (1), A is the absorbance as a function of ε(λ), the molar extinction coefficient; l is the cuvette length in cm; and c is the concentration of the chromophore.
As the absorption process is extremely fast (<10 −15 s) [42], the molecules are considered motionless during the process leading to transient excited states (Figure 2A, Step 1). These states feature the same conformation as fundamental states but with distinct molecular orbital configurations. They quickly stabilize by vibrational relaxation leading to conformation change and then to internal conversion ( Figure 2A, Step 2) to the lowest excited energy state from which fluorescence will arise (Figure 2A, Step 3). The efficiency of the emission process is described by the fluorescence quantum yield (ϕ F ), which is the ratio between the number of emitted and absorbed photons (0 < ϕ F < 1; Equation (2)). Indeed, the excited state may also decay through nonradiative processes such as internal conversion (IC) (Figure 2A, Step 4), resulting in heat release or intersystem crossing (ISC) (Figure 2A, Step 5) to populate the triplet state (T 1 ). Equation (2) shows fluorescence quantum yield as a function of the deactivation kinetics of the excited state; subscript F denotes fluorescence, IC denotes internal conversion, and ISC denotes intersystem crossing.
The "Kasha rule" states that fluorescence arises only from the lowest exited state of singlet spin multiplicity; therefore, the emission spectrum and quantum yield do not depend on the excitation wavelength, as higher states decay to the lowest excited state. It also implies that a fluorophore features only one fluorescence band arising from the "Kasha state". The overall efficiency of a fluorophore can be represented using the brightness β accounting for the ability to both absorb and emit photons (Equation (3)).
Equation (3) gives the brightness as a function of ε(λ) and ϕ F. The absorption and emission spectra also give access to another property: the "Stokes shift", which is the difference between the absorption band of higher wavelength and the emission band ( Figure 2B). The Stokes shift corresponds also to the energy difference between absorption and emission caused by the stabilization of the excited state before emission; it has to be expressed in cm −1 or eV (Equation (4)) to compare the energy of absorption and emission at different wavelengths, since wavelength is inversely proportional to energy. This property is also important in fluorescence microscopy; in this case, the direct wavelength difference in nanometers is more convenient to define the emission and the absorption spectral windows.
The Stokes shift is very significant in terms of the photophysical properties of a fluorophore: A small Stokes shift means that the electron density of the excited state is similar to that of the fundamental state. A large Stokes shift is evidence of a strong reorganization and stabilization of the chromophores at its excited state due to environmental or internal effects.

Small Organic Fluorophore Classification and Structure-Fluorescence Relationship
A classification to briefly outline the nature of the most common fluorescence transitions in relation to the structure of small organic fluorophores can be established ( Figure 3): -Apolar chromophores in which local state emission occurs with no electron donor and accepting groups. Due to this absence, electrons remain localized at the excited state. Local state emission features small Stokes shifts, and can present vibronic structures and symmetry if the π-conjugated system is very rigid. The most common apolar fluorophores are perylenes, anthracenes, rubrenes, and pyrenes. -Push-pull chromophores possessing strong electron donor and accepting groups. These groups favor electron delocalization along all of the π-conjugated system, leading to significant electron density change or internal charge transfer (iCT) at excited states manifested by large Stokes shifts. As iCT excited states are more polar than fundamental states, the Stokes shift increases with the polarity of the solvent. The most common push-pull fluorophores are coumarins [43]. -Cyanine chromophores featuring an electron delocalization along a π-conjugated system with an odd number of atoms. They usually possess a thoroughly delocalized charge and small Stokes shifts. The most common cyanine fluorophores are cyanines, squaraines, xanthenes, and bodipy [44]. As fluorescence efficiency and spectral shape are very sensitive to the environment, fluorescence microscopy is an ideal technique to probe and monitor biological environment parameters [46] such as polarity [47,48], viscosity [49][50][51], hydrophilicity, pH [52], redox potential [53], membrane potential [54,55], and protein mobility (fluorescence recovery after photobleaching (FRAP)) [56] in living cells [57]. The fluorescence properties of a fluorophore can also be impacted by the presence of other chromophores in close vicinity through spatial energy transfers such as FRET (Förster Resonance Energy Transfer) and PET (Photoinduced Electron Transfer) [40][41][42]. These energy transfer mechanisms have been widely used to design fluorescent bioprobes [58,59].

Fluorescent Proteins (FPs)
Green fluorescent protein (GFP) from the jellyfish Aequora victoria was discovered in 1962 [60], followed by homologs from diverse marine animals including sea anemone [61], copepod [61], and lancelet [62]. Proteins of the GFP family consist of ~220-240 amino acid residues with 11 β-sheets that form a barrel with a distorted helix inside [2]. At the very center of the β-barrel, 3 amino acid residues of the helix form the chromophore of FPs at positions 65, 66, and 67 (numbering in reference to the GFP of Aequorea victoria). A two-step reaction with cyclization of the protein backbone at positions 65-67 followed by dehydrogenation of Cα-Cβ of Tyr66 with molecular oxygen is responsible for the formation of the chromophore. Thus, the chromophore is a two-ring structure representing a conjugated π-system that is large, polarized, and planar enough to absorb and emit light within the visible range [2]. Tyr66 and Gly67 are strictly conserved among natural GFP-like proteins while the residue at position 65 can vary. The side chains of amino acids located inside the barrel play essential roles in chromophore formation and the fine-tuning of spectral properties of cyan, green, and red natural FPs. Variations of these side chains can dramatically alter the excitation and emission spectra [2].

Fluorescent Proteins (FPs)
Green fluorescent protein (GFP) from the jellyfish Aequora victoria was discovered in 1962 [60], followed by homologs from diverse marine animals including sea anemone [61], copepod [61], and lancelet [62]. Proteins of the GFP family consist of~220-240 amino acid residues with 11 β-sheets that form a barrel with a distorted helix inside [2]. At the very center of the β-barrel, 3 amino acid residues of the helix form the chromophore of FPs at positions 65, 66, and 67 (numbering in reference to the GFP of Aequorea victoria). A two-step reaction with cyclization of the protein backbone at positions 65-67 followed by dehydrogenation of Cα-Cβ of Tyr66 with molecular oxygen is responsible for the formation of the chromophore. Thus, the chromophore is a two-ring structure representing a conjugated π-system that is large, polarized, and planar enough to absorb and emit light within the visible range [2]. Tyr66 and Gly67 are strictly conserved among natural GFP-like proteins while the residue at position 65 can vary. The side chains of amino acids located inside the barrel play essential roles in chromophore formation and the fine-tuning of spectral properties of cyan, green, and red natural FPs. Variations of these side chains can dramatically alter the excitation and emission spectra [2].
The natural diversity of excitation-emission spectra was further extended via mutagenesis. Today, violet, blue, cyan, green, yellow, orange, red, and far-red monomeric FPs cover almost the whole visible spectrum [2,[62][63][64] (Figure 4). This modern palette is additionally enriched by a number of FP variants (T-Sapphire, mAmetrine, mKeima) with large Stokes shift of more than 100 nm [2]. In addition to monomeric FPs, generation of tandem versions of dimeric FPs (dTomato) [65] or tetrameric FPs (Katushka) [66,67] also exists.   In the last decades, advanced fluorescence imaging techniques such as fluorescence lifetime, two-photon microscopy, and nanoscopies have emerged. Using spectroscopic properties of fluorophores, these approaches lead to higher 3D resolution and possibly reduce photodamage to biological samples (see also Section 4).

Fluorescence Lifetime Imaging Microscopy (FLIM)
Fluorescence lifetime imaging microscopy (FLIM) is an imaging technique which allows mapping of the fluorescence signal as a function of fluorescence lifetime [68][69][70][71][72]. Fluorescence  In the last decades, advanced fluorescence imaging techniques such as fluorescence lifetime, two-photon microscopy, and nanoscopies have emerged. Using spectroscopic properties of fluorophores, these approaches lead to higher 3D resolution and possibly reduce photodamage to biological samples (see also Section 4).

Fluorescence Lifetime Imaging Microscopy (FLIM)
Fluorescence lifetime imaging microscopy (FLIM) is an imaging technique which allows mapping of the fluorescence signal as a function of fluorescence lifetime [68][69][70][71][72]. Fluorescence lifetime corresponds to the duration of the existence of a molecule at excited states, in particular at the lowest exited state S 1 . As absorption is considered immediate, the fluorescence lifetime depends mostly on the nature of the Kasha state and de-excitation processes. The fluorescence lifetime is denoted by τ (Equation (5)) and is expressed as a function of the deactivation kinetics of the excited state (i.e., of the fluorescence rate k F , intersystem crossing rate k ISC , and internal conversion rate k IC ).
Time-resolved fluorescence measurement provides additional information in comparision with steady-state microscopy as it allows for discriminating several emissions within the same spectral window. The most straightforward time-resolved experiment is the time-gated technique, which involves using a delay between excitation and detection to selectively remove the short-living biological background fluorescence; this technique requires chromophores featuring long-living luminescence, which can be achieved using long-living fluorescence (above 5 ns) [73], phosphorescence [74], lanthanide emission [75], or excimer emission [76]. Time-resolved fluorescence microscopy can be even more selective when using sets of luminophores with very distinctive lifetimes, allowing multiplexing, i.e., separation of several luminescence spectra as functions of fluorescence lifetime [77].
As fluorescence depends both on the nature of the Kasha state and on the competition between several de-excitation processes, fluorescence lifetime is very sensitive to the environment. It allows for measurement of the oxygen concentration [78,79], viscosity [49,80], and pH [81,82].
Fluorescence lifetime imaging can be performed with endogenous (tryptophan, NADH, flavins, porphyrins, melanin, liposfuscin, collagen, etc.) and exogenous fluorophores (small organic fluorophores, FPs, nanoparticles, etc.). Autofluorescence lifetime imaging may provide information on the morphological structure of cells and tissues but the weak and nonspecific fluorescence originating from a variety of endogenous fluorophores limits applications of this method. In contrast, the advantages of exogenous probes are their (i) large structural and spectral diversities, (ii) wide range of fluorescence lifetimes from picoseconds to milliseconds, and (iii) numerous applications in cells, tissues, and whole organs [68]. Notably, due to their organic origin, the majority of small organic fluorophores and FPs have similar characteristics including fluorescence lifetimes within the range of 0.1-4 ns. In addition, both types of molecules share applications in fluorescence lifetime studies including background/autofluorescence elimination and the FLIM-FRET approach [68,83].

Fluorescent Organic Probes in Two-Photon (2P) Microscopy
2P photon absorption is the simultaneous absorption of two photons to populate an excited state of a chromophore ( Figure 5); this is a nonlinear optical phenomenon which depends on the hyperpolarizability of chromophores [84,85]. After excitation, the molecule evolves in a similar way to when exposed to classical excitation, featuring the same fluorescence quantum yield and the same emission spectrum shape. The simultaneous nature of this absorption leads to two main consequences. On one hand, the energy of each photon is half the energy used in one-photon excitation, meaning that the wavelength is doubled in two-photon excitation compared to in classical excitation. As a matter of fact, excitation of fluorochromes and collection of photons within the biological transparency windows are much easier and lead to deeper tissue penetration and less photodamage to living cells ( Figure 5). On the other hand, the simultaneity of photon absorption implies a nonlinear probability for photon absorption, which depends on the square of incident light intensity. The square dependence allows us to better restrict the excitation to a focal volume that determines a better control of the excitation depth [86,87]. Two-photon absorbing molecules have been developed [88,89] allowing images of deeper inside a tissue (>100 µm) to be obtained with higher spatial resolution and longer observation time. Although many "one-photon" dyes can also be excited under two-photon irradiation conditions, their structure is not optimized for this technique as they have a small two-photon absorption cross section. The particular design of two-photon probes has been well rationalized by theoretical approaches [85]. It was shown that electron delocalization plays the main role in two-photon absorption. Indeed, privileged chromophores for two-photon absorption are highly polarizable molecules featuring strong internal charge transfer upon irradiation ( Figure 6). They feature both long conjugation systems and strong electron donating and withdrawing groups to create the strongest electron delocalization. Chromophore geometry may also play a determining role. In particular, quadrupolar, octupolar, or cyanine structures increase 2P absorption thanks to resonances with low energy states ( Figure 6) [85,90]. In addition to these synthetic small organic molecules, FPs are also suitable for 2P absorption. However, the 2P optimum excitation wavelength and maximum brightness of FPs cannot, in general, be deduced from 1P properties because (i) the chromophore of FPs is not centrosymmetric and (ii) there is an enhancement of certain vibronic transitions in the 2P absorption spectrum of FPs [91]. Compared with a small fluorescent organic molecule in solution, the chromophore of FPs is On the other hand, the simultaneity of photon absorption implies a nonlinear probability for photon absorption, which depends on the square of incident light intensity. The square dependence allows us to better restrict the excitation to a focal volume that determines a better control of the excitation depth [86,87]. Two-photon absorbing molecules have been developed [88,89] allowing images of deeper inside a tissue (>100 µm) to be obtained with higher spatial resolution and longer observation time. Although many "one-photon" dyes can also be excited under two-photon irradiation conditions, their structure is not optimized for this technique as they have a small two-photon absorption cross section. The particular design of two-photon probes has been well rationalized by theoretical approaches [85]. It was shown that electron delocalization plays the main role in two-photon absorption. Indeed, privileged chromophores for two-photon absorption are highly polarizable molecules featuring strong internal charge transfer upon irradiation ( Figure 6). They feature both long conjugation systems and strong electron donating and withdrawing groups to create the strongest electron delocalization. Chromophore geometry may also play a determining role. In particular, quadrupolar, octupolar, or cyanine structures increase 2P absorption thanks to resonances with low energy states ( Figure 6) [85,90]. On the other hand, the simultaneity of photon absorption implies a nonlinear probability for photon absorption, which depends on the square of incident light intensity. The square dependence allows us to better restrict the excitation to a focal volume that determines a better control of the excitation depth [86,87]. Two-photon absorbing molecules have been developed [88,89] allowing images of deeper inside a tissue (>100 µm) to be obtained with higher spatial resolution and longer observation time. Although many "one-photon" dyes can also be excited under two-photon irradiation conditions, their structure is not optimized for this technique as they have a small two-photon absorption cross section. The particular design of two-photon probes has been well rationalized by theoretical approaches [85]. It was shown that electron delocalization plays the main role in two-photon absorption. Indeed, privileged chromophores for two-photon absorption are highly polarizable molecules featuring strong internal charge transfer upon irradiation ( Figure 6). They feature both long conjugation systems and strong electron donating and withdrawing groups to create the strongest electron delocalization. Chromophore geometry may also play a determining role. In particular, quadrupolar, octupolar, or cyanine structures increase 2P absorption thanks to resonances with low energy states ( Figure 6) [85,90]. In addition to these synthetic small organic molecules, FPs are also suitable for 2P absorption. However, the 2P optimum excitation wavelength and maximum brightness of FPs cannot, in general, be deduced from 1P properties because (i) the chromophore of FPs is not centrosymmetric and (ii) there is an enhancement of certain vibronic transitions in the 2P absorption spectrum of FPs [91]. Compared with a small fluorescent organic molecule in solution, the chromophore of FPs is In addition to these synthetic small organic molecules, FPs are also suitable for 2P absorption. However, the 2P optimum excitation wavelength and maximum brightness of FPs cannot, in general, be deduced from 1P properties because (i) the chromophore of FPs is not centrosymmetric and (ii) there is an enhancement of certain vibronic transitions in the 2P absorption spectrum of FPs [91].
Compared with a small fluorescent organic molecule in solution, the chromophore of FPs is buried within a complex protein environment that influences the photophysical properties of the chromophore through electrostatic interactions. In particular, the internal electric field inside the β-barrel influences the 2P properties of FPs, including the cross section [91,92]. Recently, blue-shifted green fluorescent protein homologs have been shown to be 2.5 times brighter than the commonly used enhanced GFP under 2P excitation [92].

Fluorescent Organic Probes in Nanoscopy
A general restriction of fluorescence imaging is the Abbe light diffraction limit. Very simply, if the distance between two emitting fluorophores is shorter than half the wavelength used, it is impossible to isolate the emission of each molecule, making the image blurred. To bypass this limit, super-resolution fluorescence imaging techniques were implemented to individually isolate the emission of each fluorophore. These techniques are generally classified into two main categories: fluorescence depletion and stochastic approaches [6,93]. STimulated Emission Depletion (STED) nanoscopy is the most widespread fluorescence depletion technique, and uses stimulated emission to prevent the spontaneous emission of fluorescence in the vicinity of target fluorophores. Practically, STED relies on two distinct excitations: a diffraction-limited classical excitation followed by a structured toroidal excitation, which depopulates the excited state of fluorophores by stimulated emission at the periphery of the first excitation circle. Consequently, depopulation allows for retaining only the fluorescence of fluorophores at the very center of the irradiation (Figure 7) [94][95][96]. buried within a complex protein environment that influences the photophysical properties of the chromophore through electrostatic interactions. In particular, the internal electric field inside the β-barrel influences the 2P properties of FPs, including the cross section [91,92]. Recently, blue-shifted green fluorescent protein homologs have been shown to be 2.5 times brighter than the commonly used enhanced GFP under 2P excitation [92].

Fluorescent Organic Probes in Nanoscopy
A general restriction of fluorescence imaging is the Abbe light diffraction limit. Very simply, if the distance between two emitting fluorophores is shorter than half the wavelength used, it is impossible to isolate the emission of each molecule, making the image blurred. To bypass this limit, super-resolution fluorescence imaging techniques were implemented to individually isolate the emission of each fluorophore. These techniques are generally classified into two main categories: fluorescence depletion and stochastic approaches [6,93]. STimulated Emission Depletion (STED) nanoscopy is the most widespread fluorescence depletion technique, and uses stimulated emission to prevent the spontaneous emission of fluorescence in the vicinity of target fluorophores. Practically, STED relies on two distinct excitations: a diffraction-limited classical excitation followed by a structured toroidal excitation, which depopulates the excited state of fluorophores by stimulated emission at the periphery of the first excitation circle. Consequently, depopulation allows for retaining only the fluorescence of fluorophores at the very center of the irradiation (  The other family of nanoscopy methods is the stochastic approach in which fluorophores are initially in a dark state (nonfluorescent state) ( Figure 8). Few spatially separated molecules are then activated, localized by the emitted fluorescence, and then deactivated. Several cycles of activation/deactivation are used to map the biological sample ( Figure 8). The fluorescence switching process can be induced in several ways. The first strategy is called Photo-Activated Localization Microscopy (PALM) and may use "dark-state" fluorophores requiring irradiation to become fluorescent [97,98]. After fluorescence signal detection, fluorophores are photobleached under irradiation and other "dark-state" fluorophores are activated. In a second method, named Binding Activated Localization Microscopy or Points Accumulation for Imaging in Nanoscale Topography (BALM/PAINT), dark-state fluorophores are briefly activated only during interaction with a specific substrate [99]. An alternative to the PALM technique is the STochastic Optical Reconstruction Microscopy (STORM) using photoswitchable dyes whose fluorescence can be triggered or inhibited by light irradiation [100][101][102]. The other family of nanoscopy methods is the stochastic approach in which fluorophores are initially in a dark state (nonfluorescent state) ( Figure 8). Few spatially separated molecules are then activated, localized by the emitted fluorescence, and then deactivated. Several cycles of activation/deactivation are used to map the biological sample ( Figure 8). The fluorescence switching process can be induced in several ways. The first strategy is called Photo-Activated Localization Microscopy (PALM) and may use "dark-state" fluorophores requiring irradiation to become fluorescent [97,98]. After fluorescence signal detection, fluorophores are photobleached under irradiation and other "dark-state" fluorophores are activated. In a second method, named Binding Activated Localization Microscopy or Points Accumulation for Imaging in Nanoscale Topography (BALM/PAINT), dark-state fluorophores are briefly activated only during interaction with a specific substrate [99]. An alternative to the PALM technique is the STochastic Optical Reconstruction Microscopy (STORM) using photoswitchable dyes whose fluorescence can be triggered or inhibited by light irradiation [100][101][102]. Recent developments of small fluorescent organic probes for nanoscopies will be discussed in Section 4.2. For FPs, new variants of so-called photocontrollable FPs have been engineered, notably for nanoscopies, and can be classified into three forms [103,104]: -Photoactivatable FPs (PAFPs) which undergo activation from a nonfluorescent (dark) state to a fluorescent state (PATagRFP, PAmKate, …). -Photoswitchable (also called photoconvertible) FPs (PSFPs) that can be converted from one fluorescent state to another (Dendra2, mEos2, …).

Strategies for Labeling Living Samples with Fluorescent Probes
In addition to their photophysical properties, fluorescent organic probes should have essential physicochemical properties for easy use with living samples. The membrane permeability of small organic fluorophores depends on their lipophilicity, their molecular weight, the number of hydrogen bond donors/acceptors, and their charge [105]. Therefore, cell-permeant probes are preferred but cell loading could also be achieved by other techniques that involve iontophoresis, ejection of a substance from a pipette by the application of current, or pressure injection using intracellular micropipettes [106]. Once inside the cell, probes should be well-retained within the cell or, in some cases, need the support of multidrug resistance protein family inhibitors to reduce extrusion [107]. The sensitivity and specificity of the small fluorescent organic probe determine the use concentration and consequently limit cytotoxicity or physiological modifications. For FPs, the expression level of a fusion construct (protein of interest-FP) should be good enough to obtain a sufficient signal for reliable imaging and not too high in order to avoid interfering with the biochemistry of a living cell. In transient transfection (introduction of fusion-construct-containing plasmid in cells), the expression level may vary among transfected cells. For robust and reproducible experiments, stable cell lines (integration of the transfected plasmid into the target cell genome) are preferred [2]. Finally, photostability of the fluorescent organic probe is directly responsible for the duration of the experiment and the frequency of image acquisition.
The aim of this section is not to propose a comprehensive and extensive catalog but rather to underline through mostly, but not exclusively, in situ examples the required characteristics of fluorescent organic probes with regard to applications and type of living samples (Table 1). Thanks to their easy access, isolated cells offer the greatest possibilities for cellular and intracellular labeling and they will be firstly described. Although most labeling methods for isolated cells may be applicable to other type of samples, adaptation or complementary strategies have also been developed to reach similar targets in tissues, organs, and organisms. Recent developments of small fluorescent organic probes for nanoscopies will be discussed in Section 4.2. For FPs, new variants of so-called photocontrollable FPs have been engineered, notably for nanoscopies, and can be classified into three forms [

Strategies for Labeling Living Samples with Fluorescent Probes
In addition to their photophysical properties, fluorescent organic probes should have essential physicochemical properties for easy use with living samples. The membrane permeability of small organic fluorophores depends on their lipophilicity, their molecular weight, the number of hydrogen bond donors/acceptors, and their charge [105]. Therefore, cell-permeant probes are preferred but cell loading could also be achieved by other techniques that involve iontophoresis, ejection of a substance from a pipette by the application of current, or pressure injection using intracellular micropipettes [106]. Once inside the cell, probes should be well-retained within the cell or, in some cases, need the support of multidrug resistance protein family inhibitors to reduce extrusion [107]. The sensitivity and specificity of the small fluorescent organic probe determine the use concentration and consequently limit cytotoxicity or physiological modifications. For FPs, the expression level of a fusion construct (protein of interest-FP) should be good enough to obtain a sufficient signal for reliable imaging and not too high in order to avoid interfering with the biochemistry of a living cell. In transient transfection (introduction of fusion-construct-containing plasmid in cells), the expression level may vary among transfected cells. For robust and reproducible experiments, stable cell lines (integration of the transfected plasmid into the target cell genome) are preferred [2]. Finally, photostability of the fluorescent organic probe is directly responsible for the duration of the experiment and the frequency of image acquisition.
The aim of this section is not to propose a comprehensive and extensive catalog but rather to underline through mostly, but not exclusively, in situ examples the required characteristics of fluorescent organic probes with regard to applications and type of living samples (Table 1). Thanks to their easy access, isolated cells offer the greatest possibilities for cellular and intracellular labeling and they will be firstly described. Although most labeling methods for isolated cells may be applicable to other type of samples, adaptation or complementary strategies have also been developed to reach similar targets in tissues, organs, and organisms.

Fluorescent Labeling to Monitor Cell Viability
Monitoring cell viability is one of the earlier applications of fluorescent probes and is mainly based on plasma membrane integrity (Table 1). To facilitate membrane permeation, probes such as fluorescein diacetate (FDA) or calcein have been designed with an organic complex acetoxymethylester group (AM, R: -CH 2 OCOCH 3 ) [108]. Outside the cell, the probe is not fluorescent and penetrates the cell membrane thanks to the AM group, which is then cleaved by endogeneous esterases [109]. Once the AM is removed, the probe is strongly fluorescent and trapped within the cell, although leakage can be observed over time. FDA is a low-cost and easy-to-use probe, but is, unfortunately, poorly retained in cells. Consequently, cells are often lysed before fluorescence measurement through plate readers to obtain the full signal [110,111]. Calcein is also frequently used for cell viability purposes but has the drawback of being sensitive to light exposure, and rapid photobleaching may limit experimental duration. To refine the experimental procedure by monitoring the ratio of living and dead cells, calcein is usually combined with a cell-impermeant DNA-intercalating agent such as propidium iodide or ethidium bromide that reaches their target only in cells with fragmented plasma membranes. More recently, a new generation of ready-to-use reagents (Nuc family) for dead or live cells has emerged which exhibits a very low basal fluorescence and emits a very bright fluorescence signal when bound to DNA [112,113].

Fluorescent Labeling for Cell Tracking
Cell tracking is associated with short and long time lapses for which the ability of the probe to be retained in the cell is an essential criterion (Table 1). Due to reactivity with the thiol group of cellular macromolecules, FDA-derived probes commercially known as the Cell Tracker family are frequently used to perform short time lapses [114]. Cell trackers label the entire cytoplasm but cell loading might depend on the cell type or cell metabolism. To reduce photocytotoxicity induced by repetitive light exposure, near-red probes such as Red or Deep Red CytoTracker are preferred because they are excited with low-energy radiation (see also Section 2.5). Lipophilic tracers including long-chain dialkylcarbocyanines such as 1,1 -dioctadecyl-3,3,3 3 -tetramethylindocarbocyanine perchlorate (DiI) or the CellVue family finely and intensively stain membrane structures [115,116] and could represent convenient markers for long-term tracking. Alternatively, a new technology has been recently developed to stably incorporate a red fluorescent dye containing hydrophobic aliphatic chains into the lipids of plasma membrane [117]. Note that nonorganic probes such as Quantum Dots may also be used for cell tracking but will not be detailed here.

Fluorescent Labeling to Identify Membrane, Organelles, and Macromolecules
Indirect staining of membranous elements by using lectins that reversibly bind to glycoproteins, glycolipids, or polysaccharides is a very simple and convenient strategy (Table 1) [118]. In particular, wheat germ agglutinin (WGA) is a protein that recognizes N-acetylglucosamine and N-acetylneuraminic acid residue present at the cell surface of numerous eukaryotes and prokaryotes [119]. A broad range of fluorescent Alexa-WGA conjugates is commercially available but their labeling intensity and photostability are associated with photophysical characteristics of the fluorochrome [120,121]. Therefore, short-term incubation with fluorescent WGA conjugates induces a bright cellular outline including processes and intercellular connections [114,122]. Due to membrane internalization and vesicle recycling processes, fluorescent lectins can also be detected and followed in intracellular compartments or elements over time [122]. Nevertheless, considering the large distribution of the target residues, WGA could not be considered a discriminating marker.
Nuclear, mitochondrial, and cytosolic nucleic acids could be labeled in living cells with rarer cell-permeant probes (Table 1). Historically, the Hoechst intercalant DNA family was used but it has spectral drawbacks with a high-energy UV peak of excitation that is phototoxic to cells and a broad emission, a source of spectral contamination during multilabeling experiments [123]. However, Hoechst dyes are now conjugated to various molecules to tether them to DNA [124]. More recently, a new generation of cyanine probes called the SYTO ® family offers a large diversity of both ex/em wavelength couples and DNA/RNA affinities. Consequently, cellular localization of the nucleus in the case of counter-staining and multiplex fluorescent signals and/or specific nucleic acid detection are now facilitated by the use of SYTO ® probes [113].
Labeling and tracking organelles in living cells is not a trivial issue (Table 1). As a striking example, localization of actively respiring mitochondria with organic dyes needs particular attention. Containing a thiol-reactive chloromethyl moiety, dyes from the "Mitotracker" family are widely used nowadays to follow mitochondria within a cell or from cell to cell [125]. Mitochondria have been shown to display the capacity to be transferred between cell types, notably in the context of cancer [126]. Co-culture experiments with a combination of Mitotracker and vital dye have been recently performed and clearly identify the transfer of mitochondria from donor cells to target cells [127]. Although there is a broad variety of fluorescent Mitotrackers, differential signal intensity and differential distribution may be noted between them. In particular, localization of mitochondria is different with Mitotracker Green FM compared with Mitotracker Red CMXRos in PC12 cells ( Figure 9) and more cell leakage is observed for Mitotracker Red. On the contrary, there is potentially more cytotoxicity with Mitotracker Green labeling during long time lapses as we observed through videomicroscopy. As previously mentioned, the aim of this section is not to propose a catalog of fluorescent probes for living cells but to note that there are numerous dyes or strategies to label other organelles including lysosomes, peroxisomes, endosomes, endoplasmic reticulum, or Golgi apparatus. Among these strategies, the BacMam method with insect baculovirus (CellLight ® ), available for most organelles, leads to the introduction of a fluorescent protein which is a specific marker of the organelle [33]. For lysosomes, probes such as Lysotrackers or Lysosensors take advantage of the acidity/pH of these organelles for fluorescent labeling [128]. More recently, new organic fluorescent probes with high photostability have been developed to follow lysosome (peptide-based and Atto) and mitochondrion (NHS ester and Atto) dynamics and interaction during super-resolution time-lapse experiments [129].
Chemosensors 2018, 6, x 12 of 45 emission, a source of spectral contamination during multilabeling experiments [123]. However, Hoechst dyes are now conjugated to various molecules to tether them to DNA [124]. More recently, a new generation of cyanine probes called the SYTO ® family offers a large diversity of both ex/em wavelength couples and DNA/RNA affinities. Consequently, cellular localization of the nucleus in the case of counter-staining and multiplex fluorescent signals and/or specific nucleic acid detection are now facilitated by the use of SYTO ® probes [113].
Labeling and tracking organelles in living cells is not a trivial issue (Table 1). As a striking example, localization of actively respiring mitochondria with organic dyes needs particular attention. Containing a thiol-reactive chloromethyl moiety, dyes from the "Mitotracker" family are widely used nowadays to follow mitochondria within a cell or from cell to cell [125]. Mitochondria have been shown to display the capacity to be transferred between cell types, notably in the context of cancer [126]. Co-culture experiments with a combination of Mitotracker and vital dye have been recently performed and clearly identify the transfer of mitochondria from donor cells to target cells [127]. Although there is a broad variety of fluorescent Mitotrackers, differential signal intensity and differential distribution may be noted between them. In particular, localization of mitochondria is different with Mitotracker Green FM compared with Mitotracker Red CMXRos in PC12 cells ( Figure 9) and more cell leakage is observed for Mitotracker Red. On the contrary, there is potentially more cytotoxicity with Mitotracker Green labeling during long time lapses as we observed through videomicroscopy. As previously mentioned, the aim of this section is not to propose a catalog of fluorescent probes for living cells but to note that there are numerous dyes or strategies to label other organelles including lysosomes, peroxisomes, endosomes, endoplasmic reticulum, or Golgi apparatus. Among these strategies, the BacMam method with insect baculovirus (CellLight ® ), available for most organelles, leads to the introduction of a fluorescent protein which is a specific marker of the organelle [33]. For lysosomes, probes such as Lysotrackers or Lysosensors take advantage of the acidity/pH of these organelles for fluorescent labeling [128]. More recently, new organic fluorescent probes with high photostability have been developed to follow lysosome (peptide-based and Atto) and mitochondrion (NHS ester and Atto) dynamics and interaction during super-resolution time-lapse experiments [129].  To reduce light-induced cellular stress, a new family of near-infrared or infrared fluorophores named silicon rhodamine probes (SiR probes) has been recently developed for DNA, cytoskeleton protein, and lysosome detection (Table 1) (see also Section 4.1 for chemical structure and advantages) [130]. Depending on the cell type, SiR probes might be excluded and, consequently, cell loading could be weak. Therefore, concomitant incubation with verapamil, a broad-spectrum efflux pump inhibitor, may improve fluorescent staining with SiR probes [131]. An alternative strategy to obtain an intense and long-term fluorescent signal is to infect cells with lentivectors known as Cyto-Tracers™ that expressed fluorochrome-fusion tracer proteins [132]. Therefore, these vectors produce fluorescent proteins that are specifically integrated into organelles or cellular targets and used for tracer dynamic studies [132].
To visualize glycan and lipids in cells for which, in contrast to proteins, genetically encoded reporters are not possible, click chemistry has been recently adapted to overcome the lack of methods (Table 1) [133]. The principle of click chemistry consists of cultivating cells in the presence of non-natural metabolite derivatives that carry "clickable" functions such as azide or alkyne groups ( Figure 10A). These derivatives must cross the cell membrane and be accepted by the biosynthetic machinery of the cell [134]. Once metabolized and presented on the cell surface, the azide (or alkyne)-containing molecule can be visualized through a bioorthogonal ligation reaction with a fluorescent reporter using cuprous Cu(I) ions as catalyst ( Figure 10). Numerous derivatives have been synthesized to date and been used to label various molecules in animal cells, bacteria, yeast, and plant cells, and they are now widely used for glycobiology, especially to study the function of carbohydrates or glycomolecules in living systems. For example, lipopolysaccharides of Gram-negative bacteria can be labeled using an azide-modified analogue of 3-deoxy-D-manno-octulosonic acid (Kdo-N3) [135] and glycans were recently visualized with N-azidoacetylmannosamine in HEK293T cells [134]. The azide group is exploited for because it possesses a high reactivity, is stable in water, unreactive in biological samples, and does not perturb the structural conformation of the modified molecule. The prototypical click reaction termed as azide-alkyne cycloaddition ( Figure 10A) is one of the three main click reactions used for molecule labeling. In fact, two other reactions-the copper-free azide-alkyne cycloaddition between an azide group and a strained cyclooctyne and the Staudinger ligation between an azide group and a phosphine-are also commonly employed for labeling of biological molecules. These two last reactions are of major interest because they do not need to be catalyzed by copper and are thus effective for in vivo labeling. While these reactions are of main interest as they exhibit strong selectivity, the choice of reaction when initiating studies is of main importance as side effects such as copper toxicity, changes in membrane permeability, and unspecific or background labeling can be problematic. For example, alkynyl sugars worked better than the azide form for labeling in mouse [136], probably because azide sugars could be toxic at high concentrations. However, azide sugars showed no toxicity in plant cells [137]. Moreover, the alkynil fluorophore is also generally more efficient than the azide form but can lead to unspecific or high background labeling. Thus, the choice of the alkynil-azide couple is of main importance when choosing click chemistry for labeling.
Cellular localization and co-localization of molecules of interest require both cytological references (membrane, nucleus, etc.), also called counter-staining, and multiplex fluorescent signals. Consequently, it is necessary to activate as many excitation wavelengths as fluorescent probes. However, special attention has to be paid on spectral overlapping of emitting light to avoid any artifactual detection of fluorescence, i.e., detection of emitted light by fluorochrome #1 in channel detection of fluorochrome #2. In addition, autofluorescence may be present in samples such as plants [138] and microalgaes [139] and its spectral characterization through λΛ scan (excitation/emission) is essential to choosing the appropriate fluorescent probe(s). Multilabeling experiments also suggest that a sequential mode of acquisition (one by one) may increase the duration of acquisition and the duration of light exposure, leading consequently to phototoxicity and photobleaching (see also Section 5). One of the most common ways to study the functional role of a protein is to incorporate in a cell a vector with genetic material tagged with a fluorescence sequence (Table 1). Besides the impact of the fluorescent tag size on the function of the protein of interest, many transfection strategies are used and have to be considered regarding their efficiency and their cytotoxicity. Lipofectant agents (transient pores in the cell membrane induced by calcium phosphate, cationic lipids, etc.) or electroporation (or electropermeabilization; increase in cell membrane permeability induced by an electrical field) are two main methods used to induce penetration of a plasmid into targeted cells. As one example, GFP-chromogranin A (CgA-GFP) is expressed in living COS-7 cells after transfection with lipofectamine and allows the tracking of secretory granules during granulogenesis [140]. More recently, a liposomal carrier system has been developed and offers a high yield of transfection combined with very low toxicity in mammalian cells [141]. Targeted introduction of a DNA sequence could also be performed with a modified insect cell baculovirus that infects and expresses genes in mammalian cells [113]. However, depending on the cell type, cytotoxicity and a poor yield of infection can be observed. Alternatively, new types of fusion protein-tag platforms including tetracysteine tag [142], SNAP/CLIP-tag [143,144], and HaloTag [145] have emerged more recently [146]. In these methods, the tag can be conveniently labeled with small organic fluorophores added to the incubation medium of living cells. For the tetracysteine system, a short peptide sequence (6 to 12 amino acid binding motifs) is genetically introduced into the sequence of a target protein. This sequence can specifically react with cell-permeant biarsenical fluorophores (FIAsH-EDT2 and ReASH) [147]. Similar in size to FPs, SNAP/CLIP-tag and HaloTag are self-labeling enzymes. SNAP and CLIP, variants of the human O 6 -alkylguanine-DNA alkytransferase (AGT), are used to visualize cellular proteins with fluorescent O 6 -benzylguanine and O 2 -benzylcytosine substrates, respectively One of the most common ways to study the functional role of a protein is to incorporate in a cell a vector with genetic material tagged with a fluorescence sequence (Table 1). Besides the impact of the fluorescent tag size on the function of the protein of interest, many transfection strategies are used and have to be considered regarding their efficiency and their cytotoxicity. Lipofectant agents (transient pores in the cell membrane induced by calcium phosphate, cationic lipids, etc.) or electroporation (or electropermeabilization; increase in cell membrane permeability induced by an electrical field) are two main methods used to induce penetration of a plasmid into targeted cells. As one example, GFP-chromogranin A (CgA-GFP) is expressed in living COS-7 cells after transfection with lipofectamine and allows the tracking of secretory granules during granulogenesis [140]. More recently, a liposomal carrier system has been developed and offers a high yield of transfection combined with very low toxicity in mammalian cells [141]. Targeted introduction of a DNA sequence could also be performed with a modified insect cell baculovirus that infects and expresses genes in mammalian cells [113]. However, depending on the cell type, cytotoxicity and a poor yield of infection can be observed. Alternatively, new types of fusion protein-tag platforms including tetracysteine tag [142], SNAP/CLIP-tag [143,144], and HaloTag [145] have emerged more recently [146]. In these methods, the tag can be conveniently labeled with small organic fluorophores added to the incubation medium of living cells. For the tetracysteine system, a short peptide sequence (6 to 12 amino acid binding motifs) is genetically introduced into the sequence of a target protein. This sequence can specifically react with cell-permeant biarsenical fluorophores (FIAsH-EDT2 and ReASH) [147]. Similar in size to FPs, SNAP/CLIP-tag and HaloTag are self-labeling enzymes. SNAP and CLIP, variants of the human O 6 -alkylguanine-DNA alkytransferase (AGT), are used to visualize cellular proteins with fluorescent O 6 -benzylguanine and O 2 -benzylcytosine substrates, respectively [144]. In particular, single-molecule imaging of SNAP-tagged fusion proteins has been developed with Dy 549 and CF 640 coupled benzylguanines [148]. HaloTag is a modified bacterial hydrolase enzyme designed to fuse to a protein of interest and to facilitate visualization of its subcellular localization. This HaloTag technology is based on the formation of a specific and irreversible covalent bond (chloroalkane linker) between the HaloTag protein fusion and synthetic ligands that carry a variety of functionalities including a fluorescent group for in vitro cellular imaging (TMR, diAcFAM, Oregon Green, Coumarin, or Alexa Fluor 488) [149].

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Cell Metabolism Due to their high sensitivity and fast response time, small-molecule-based nonratiometric/ratiometric fluorescence sensor systems for monitoring cell activity variations are widely used nowadays [58]. The binding affinity of the probe for its target is characterized by the dissociation constant (K D ), expressed in nM, that may also be dependent on pH and ionic strength [128]. Nonratiometric probes do not emit fluorescence (or emit low fluorescence) in the absence of the target molecule while ratiometric ones exhibit differential light emission/absorption whether they are coupled or not to the analyte [128]. When quantification is required, ratiometric organic probes are usually used to limit interference from the subcellular microenvironment, instrumental parameters, local concentration of the probe, and photobleaching, and to therefore provide effective internal referencing [58]. Related to their design, four classes of ratiometric probes have been identified so far including internal charge transfer (ICT; cation sensing), excited-state intramolecular proton transfer (ESIPT; fluoride, acetate, metal ion sensing), fluorescence resonance energy transfer (FRET; metal cation sensing) and through-bond energy transfer (TBET; metal cation sensing), and monomer-excimer formation (metal ions, phosphate, nucleic acid sensing) [58]. However, the use of ratiometric probes has a direct impact on the choice of instrument since efficient simultaneous detection or excitation is mandatory. Note that cell loading could be facilitated by dispersing agents that will increase the bioavailability of the probe [150]. There are a number of ratiometric Ca 2+ ion indicators including Fura-2 and Indo-1 AM [151,152]. For simplicity of use, notably for Ca 2+ studies on cell populations using plate readers or confocal microscopes, the nonratiometric probe Fluo-4 AM might be preferred [153,154]. For plant samples such as pollen tubes and root hairs, a cell lysis solution is needed to improve Fluo-4 AM loading [155]. Many ratiometric and nonratiometric indicators for sodium (CoroNa, SBFI) [156], zinc (FluoZin-1, FluoZin-3) [157], and magnesium (Mag-Fura-2, Magnesium Green, KMG-20-AM, and KMG-27-AM) [158] are also available. JC-1 (tetraethylbenzimidazolylcarbocyanine iodide) revealed mitochondrial activity through ratiometric monitoring of membrane potential. When mitochondrial membrane potential is high, suggesting healthy hyperpolarized mitochondria, the dye form aggregates and emits a red fluorescence with a maximum peak at 590 nm. When mitochondrial membrane potential is low (depolarization), JC-1 has predominantly a monomer form and emits green fluorescence with a peak of emission at 530 nm [159]. Cell metabolism is also followed by monitoring cellular stress revealed by organic probes (H2DCFDA, Luminol, RedocSensor, MTT) for reactive oxygen species (ROS) detection [160,161], boronobenzo[b]quinolizinium derivatives for H 2 O 2 [162], Si-rhodamine deoxylactam-based near-infrared fluorescent probe for nitric oxide (NO) [163], or by determining apoptosis with fluorescent marker fluorescein isothiocyanate carbobenzoxy-valyl-alanyl-aspartyl-[O-methyl]-fluoromethylketone (FITC-VAD-FMK) for the detection of caspase activity [110]. The combination of a cell-permeant fluorescent polymer thermometer called NN-AP2.5, which notably consists of a thermosensitive poly(N-n-propylacrylamide) unit, with FLIM leads to intracellular temperature monitoring between 28 • C and 38 • C in Hela cells [164].
Consequently, there is a huge range of small fluorescent organic molecules available for cell metabolism studies and the choice of probe should be driven by their selectivity and specificity described in the literature and technical notes. Cellular environment considerations may also increase the difficulty of the choice since intracellular factors including pH, concentration of competing metals, ionic strength, preference for hydrophobic regions, and binding constants influence specificity and sensitivity of fluorescent dyes. In particular, fluorescence generated by Zn 2+ and Ca 2+ probes within cells may also result from nonselective binding to labile and protein-bound as well as membrane-bound metals and/or from nonspecific affinity for other divalent cations [165].
An alternative to organic probes for detection of cell activity is the recent development of a number of biosensors with numerous genetic constructions mostly related to the GFP protein family [166] (Table 1). This approach includes a vector transfection step of genetically encoded FRET biosensor(s) [167]. Biosensor expression offers many possibilities to study molecular mechanisms in living cells including calcium, PKA, and ERK activities through FLIM-FRET experiments [168,169]. With the development of lifetime imaging systems and new fluorescent proteins, simultaneous use of two FLIM-FRET biosensors within one sample is allowed [169,170]. The biosensor strategy may bypass difficulties like probe penetration and autofluorescence in plants or microalgae [171]. In addition, photoactivation-induced specific expression of biosensors in a group of cells, in cells, and in subcellular compartments offers a new perspective in cell biology studies [172]. In the context of oocyte development, photoactivation of a subpopulation of microtubule subunits contributed to understanding of the comprehensive dynamics of microtubules within the mouse egg spindle [173].

Strategies of Labeling Living Cells within Organotypic Slices or Organs
Living organs and cultured organotypic slices offer the possibility to study cell responses within a microenvironment in which connections between cells and interactions with the extracellular matrix or vascular networks are preserved. Consequently, direct access to probes is sometimes limited and cell labeling may be more difficult (Table 1). While extended time of incubation could be sufficient for some cell-permeant fluorescent probes, others cannot be used. In particular, a high level of plasma and extracellular esterase activity render the classical acetoxymethyl (AM) probes ineffective for monitoring intracellular events ex vivo or in vivo [108]. Because widefield microscopes do not have any way to eliminate out-of-focus light, samples thicker than 10-20 µm may have dramatically reduced image quality. Consequently, confocal micro-and macroscopy, equipped with a pinhole in the detection path, as well as 2P microscopy whose excitation is restricted to the tiny focal volume, are preferred over wide-field microscopy for thicker samples. Live-or dead-cell fluorescent markers probes such as Syto 61, Sytox Orange, TO-PRO-3, or YO-PRO-1 may be used for cell viability or counterstaining [174,175]. However, cell metabolism indicators such as ROS would give more informative data on the real state of the sample rather than a simple calcein labeling [176]. As a nonratiometric Ca 2+ sensor, Oregon Green 488 BAPTA-1, which presents a high absorptivity (~93%), is more efficiently excited by a 488 nm laser line than are other Ca 2+ dyes (~45% of maximum absorptivity for fluo-3 and calcium green indicators) [128]. Consequently, less laser power is necessary to measure calcium variations in brain slices, reducing phototoxicity and photobleaching [177,178]. More recently, variations of Ca 2+ concentrations have been monitored with a calcium biosensor (TN L15) through FLIM-FRET experiments in neurons of hippocampal slices [179]. In contrast, cell markers previously described for isolated cells such as CMFDA or DiI have been successively used in several types of samples including cerebellar slices to study neuronal migration during development [111,177,180]. Both probes exhibit intense fluorescence signals and photostability since time lapses of up to 12 h have be performed with dry, long working distance objective (for more details see also Section 5.2) through confocal macroscopy [111]. Fluorescent lectins such as IB4 derived from Griffona simplicifolia seeds also penetrate tissues efficiently. As one example, IB4 selectively stains parenchymal microglia and endothelial cells and thus provides a simple one-step method to label brain slices [175]. Another strategy is to use a virus such as the herpes simplex virus (HSV) that will infect targeted cell types under the control of specific gene promoter. Infected cells will consequently express fluorescent proteins including biosensors in brain slices [180,181]. Alternative to transfer techniques such as microinjection, biolistic gene gun, viral infection, lipofection, and transgenic technology that are not suitable for gene transfer into a single cell or a small number of cells, a method with local application of plasmid solution and a small current injection (electroporation) was developed to study axon morphology of individual cortical neurons in organotypic slice cultures [182]. To label organ vascular pathways, one possibility is to inject tracers directly in the blood or lymphatic circulation of living organisms. Ligating is then necessary to remove the organ and to reduce leakage from the vessels as it was performed for ex vivo observation of rat heart labeled with FITC-dextran through confocal macroscopy ( Figure 11) [183]. Ligating is then necessary to remove the organ and to reduce leakage from the vessels as it was performed for ex vivo observation of rat heart labeled with FITC-dextran through confocal macroscopy ( Figure 11) [183]. Figure 11. Ex vivo cartography of cardiac blood vasculature. Intravenous injection of fluorescein isothiocyanate (FITC)-dextran was performed in anaesthetized animals (for experimental procedures, please see [183]). After ligating, the heart was removed and directly placed on the stage of a confocal macroscope for imaging. FITC-dextran labeled blood circulation. Scale bar: 1 mm.

Strategies for Labeling Living Cells within an Organism
The strategy of labeling, together with the strategy of access for imaging, should be adapted to the type of organism (unicellular organisms, larvae, embryos, pups, plants, insects, adult rodents, etc.) and possibly to the type of target organ within the organism (Table 1). Some strategies will require anesthesia and invasive methods such as surgery (skin sectioning, laparotomy, cranial window, etc.) to access to the area of interest (muscle, embryos, intestine, heart, brain, etc.). Other strategies of labeling and observation are noninvasive, but they may need anesthesia and are limited to organism restraint or immobilization and hair shaving. In addition, spectral characteristics of the probe might be driven by the thickness and the transparency of tissues. As a general principle, the use of long wavelengths, as for near-infrared or infrared probes, results in reduced scatter losses and, consequently, increased tissue penetration and deeper imaging. As an example, a new cyanine-based NIR fluorescent probe was recently developed for the detection of Zn 2+ in zebrafish [184]. Regarding the instruments, confocal macroscopy, fibered confocal microscopy, two-photon microscopy, and light sheet fluorescence microscopy (LSFM) are technologies of choice for imaging organisms. In LSFM, a thin excitation light sheet illuminates a single plane of the specimen via an illumination objective. The emitted fluorescence signals are detected by a second objective which is mounted perpendicular to the illumination axis. A specimen holder is automatically moved to obtain images, plane by plane, throughout the whole sample, and resulting image stacks are used for 3D reconstruction [36]. Therefore, large field of view, rapid acquisition with detectors such as Electron-Multiplication CCD cameras (EM-CCD) and scientific Complementary Metal Oxide Semiconductor (sCMOS) cameras (see also Section 5.3), good signal-to-noise ratio (SNR), and undamaged sample above or below the focal plane are LSFM features particularly adapted to studying living transparent specimens such as growing plants, drosophila larvae, and zebrafish [36,185].

Injection of Fluorescent Probes and Labeled Cells
As described in Section 3.2, fluorescent probes can be injected through the vascular pathway and systemic circulation to reach organs in organisms. After surgery, the probe can also be injected directly within the organ or organism (Table 1). To trace the neural circuit, Levy et al. [186] injected Alexa 488-WGA lectin directly within the mouse cerebellum. Injection of Figure 11. Ex vivo cartography of cardiac blood vasculature. Intravenous injection of fluorescein isothiocyanate (FITC)-dextran was performed in anaesthetized animals (for experimental procedures, please see [183]). After ligating, the heart was removed and directly placed on the stage of a confocal macroscope for imaging. FITC-dextran labeled blood circulation. Scale bar: 1 mm.

Strategies for Labeling Living Cells within an Organism
The strategy of labeling, together with the strategy of access for imaging, should be adapted to the type of organism (unicellular organisms, larvae, embryos, pups, plants, insects, adult rodents, etc.) and possibly to the type of target organ within the organism (Table 1). Some strategies will require anesthesia and invasive methods such as surgery (skin sectioning, laparotomy, cranial window, etc.) to access to the area of interest (muscle, embryos, intestine, heart, brain, etc.). Other strategies of labeling and observation are noninvasive, but they may need anesthesia and are limited to organism restraint or immobilization and hair shaving. In addition, spectral characteristics of the probe might be driven by the thickness and the transparency of tissues. As a general principle, the use of long wavelengths, as for near-infrared or infrared probes, results in reduced scatter losses and, consequently, increased tissue penetration and deeper imaging. As an example, a new cyanine-based NIR fluorescent probe was recently developed for the detection of Zn 2+ in zebrafish [184]. Regarding the instruments, confocal macroscopy, fibered confocal microscopy, two-photon microscopy, and light sheet fluorescence microscopy (LSFM) are technologies of choice for imaging organisms. In LSFM, a thin excitation light sheet illuminates a single plane of the specimen via an illumination objective. The emitted fluorescence signals are detected by a second objective which is mounted perpendicular to the illumination axis. A specimen holder is automatically moved to obtain images, plane by plane, throughout the whole sample, and resulting image stacks are used for 3D reconstruction [36]. Therefore, large field of view, rapid acquisition with detectors such as Electron-Multiplication CCD cameras (EM-CCD) and scientific Complementary Metal Oxide Semiconductor (sCMOS) cameras (see also Section 5.3), good signal-to-noise ratio (SNR), and undamaged sample above or below the focal plane are LSFM features particularly adapted to studying living transparent specimens such as growing plants, drosophila larvae, and zebrafish [36,185].

Injection of Fluorescent Probes and Labeled Cells
As described in Section 3.2, fluorescent probes can be injected through the vascular pathway and systemic circulation to reach organs in organisms. After surgery, the probe can also be injected directly within the organ or organism (Table 1). To trace the neural circuit, Levy et al. [186] injected Alexa 488-WGA lectin directly within the mouse cerebellum. Injection of DiI/3,3 -dioctadecyloxacarbocyanine perchlorate, DiO, in the mesenchym of chick embryo offers the possibility to follow dynamics of tissue deformation during hindlimb development [187]. More simply, organs can only be bathed in a solution of fluorescent probes for several minutes. Observation through intravital microscopy of exposed submandibular gland acini incubated with Mitotracker revealed synchronization of mitochondrial metabolic oscillations [188]. In xenograft protocols, cells could be labeled before injection in an organism and consequently be easily imaged or even tracked later on. Injection of SiR700-labeled antibody-containing HKBMM cells in mouse induces a tumor that can consequently be detected through in vivo imaging [189].

Transfection through Electroporation and Transgenic Organisms
There are two approaches to labeling organisms with fluorescent proteins ( Table 1). The first one consists of injecting a plasmid expressing a tagged protein into an organism followed by electroporation to allow the vector to penetrate targeted cells. Microinjection of a GFP-tagged plasmid into the lateral ventricle of the embryonic rat brain (E15.5 or E18.5) followed by electroporation (5 electric pulses, 50 V, 50 ms) revealed p57(Kip2) effects on neurogenesis and gliogenesis [190]. The second approach is to obtain through genetic engineering transgenic organisms with total or targeted expression of proteins or biosensors [191].

Click Chemistry in Living Organisms
The principle of click chemistry developed in cultured cells has been recently applied to living organisms to accumulate small molecules at a potential site of injury ( Table 1). As an illustration of in vivo application, Tetrazine (Tz) or Azide (Az) alginate gels were firstly injected intramuscularly or into the mouse mammary fat pad [192]. Then, intravenous injections of Cy5-trans-cyclooctene (TCO) or Cy7-dibenzocyclooctyne (DBCO) induced respective fluorescence emission in Tz and Az gels, revealing click chemistry reactions [192]. In addition to azide-alkyne cycloadditions, thiol-ene click reactions are also widely used to form hydrogels-delivery vehicles of cells and therapeutics including small-molecule drugs, peptides, or proteins [193]. Reactions of thiol-containing macromolecules (polyethylene glycol, etc.) with alkenes (vinyl sulfone, maleimides, norbornene, etc.) may occur in situ [194] and time release of fluorescent cargo molecules (albumin, IgG, etc.) is notably dependent on thiol composition [195]. These data suggest new perspectives for click chemistry in disease treatment including controlled drug delivery.
In plant glycobiology, click chemistry represents a very powerful tool to study the cell wall-the complex matrix made of carbohydrate and proteins which ensures the mechanical integrity of plant tissue but also permits cell expansion after physical and enzymatic modification and determines cell shape [196] (Figure 10B).
To date, click labeling of plant cell wall has been used to study pectic polysaccharides [135] (Figure 12A), an unknown wall component in root hair tips [197], and monolignol in secondary cell wall [198,199]. These studies showed that fucose alkyne is successfully incorporated, metabolized, and labeled in plant cell wall pectic polysaccharide Rhamnogalacturonan I [200] (Figure 12(A2)). Moreover, the labeling of rhamnogalacturonane II (RG-II) with Kdo-N3 (Figure 12(A1)) demonstrated that incorporation of Kdo-N3 occurs in RG-II, a highly complex pectic component, through the endogenous biosynthetic machinery of the cell, and co-localization with calcofluor white (cellulose-binding dye) demonstrated that RG-II exists throughout the primary cell wall. Finally, pulse labeling experiments validate metabolic click-mediated labeling with Kdo-N3 as an excellent tool to study the synthesis and redistribution of RG-II in cell wall.
The recent development of new click-compatible sugar analogues-glucose, galactose, fucose, arabinose, rhamnose, and sucrose [137,201]-allows a good opportunity to develop this technique and to improve our knowledge on polysaccharide biosynthesis and function as soon as the current limitations of the method can be bypassed. In fact, click chemistry relies on the reaction of azides and/or alkynes and uses copper as a catalyst; thus, it does not allow dynamic imaging of living cells as copper is toxic for cells. Hopefully, alternative methods, termed "copper-free click chemistry", are currently being developed and have been successfully used to detect sugar analogues in living organisms using cyclooctyne ( Figure 12B). For instance, the difluorinated cyclooctyne (DIFO) possesses ring strain and electron-withdrawing fluorine substituents that together promote dipolar cycloaddition with azides without the use of copper. The kinetics of the reaction are comparable to those of the copper-catalyzed reaction and it proceeds within minutes on living cells with no apparent toxicity. This method has been successfully used to label glycan in Chinese Hamster Ovary (CHO) cells [133] in mouse [202] and in plant [137] with no apparent toxicity, and allows us to consider new promising and attractive applications for direct imaging of glycan in living cells. possesses ring strain and electron-withdrawing fluorine substituents that together promote dipolar cycloaddition with azides without the use of copper. The kinetics of the reaction are comparable to those of the copper-catalyzed reaction and it proceeds within minutes on living cells with no apparent toxicity. This method has been successfully used to label glycan in Chinese Hamster Ovary (CHO) cells [133] in mouse [202] and in plant [137] with no apparent toxicity, and allows us to consider new promising and attractive applications for direct imaging of glycan in living cells.

Progress in Synthesis of Organic Fluorescent Probes
Nature produces few fluorescent secondary metabolites such as umbelliferone (coumarin skeleton), flavanols, curcumin, and hypericin which have been employed (natively or after modification) for bioimaging ( Figure 13A) [203,204]. Since the discovery of natural Green Fluorescent Protein (GFP), many others have been discovered; however, they are now being

Progress in Synthesis of Organic Fluorescent Probes
Nature produces few fluorescent secondary metabolites such as umbelliferone (coumarin skeleton), flavanols, curcumin, and hypericin which have been employed (natively or after modification) for bioimaging ( Figure 13A) [203,204]. Since the discovery of natural Green Fluorescent Protein (GFP), many others have been discovered; however, they are now being engineered, allowing the production of differently colored proteins (see also Section 2.3).
To expend the library of fluorescent molecules, synthetic chemists have generated numerous new fluorescent scaffolds such as bimanes, bodipys, cyanines, squaraines, and xanthenes (fluorescein and rhodamines), to name the most well known ( Figure 13B,C) [205][206][207][208]. These small molecules have had a huge impact on modern Life Sciences as they have allowed observation of living organisms, thanks to the development of bioimaging [208].
To further improve the photophysical characteristics of fluorescent molecules including brightness and photostability, concomitantly with new imaging approaches, new chemical strategies have been formed [209], taking into account that an ideal fluorophore ("the fluorescent grail") should absorb and emit light with maximum efficiency, be photo-and chemically stable in biological medium, be of the smallest possible size, and be nontoxic [210].
As the size of the fluorophore matters if one wants to limit perturbations brought to the observed system, the very small bimane fluorophore has been developed and mostly used for accurate measurements of dynamics of proteins by FRET [211].
With a larger size, bodipy fluorophores presenting a rigid neutral system have been widely used thanks to their easy functionalization with maleimides or NHS esters, allowing introduction of targeting or hydrosolubilizing moieties. The bodipys are usually photostable and present a high quantum yield, but with a small Stokes shift. They can be found in commercially available dyes such as ER-or Lyso-trackers (Table 1) [212].
The cyanine family represents a very important class of fluorophores with multiple colors up to NIR, allowing multiplexing, FRET, or derivatization as chemosensors for analytes. They, however, generally suffer from photobleaching and small Stokes shift [213,214]. Cyanines can be found in commercially available dyes such as Mitotrackers (Table 1).
Squaraine-type dyes are characterized by the presence of a four-membered ring bearing two ketones (squaric acid) out of which one or two may be enolized. The substitution of this cycle by electron-donating substituents, usually aromatic rings, makes the donor-acceptor-donor cyanin-type structure (see Figure 5). Due to their very rigid structure, they present an exceptionally high extinction coefficient, a large two-photon absorption cross section, and a very short Stokes shift; however, they usually suffer from instability in biological medium due to nucleophilic attack. To circumvent this issue, squaraine protected by a rotaxane ring has been developed, leading to very bright and stable dyes for cell imaging [215,216].

Development of Small Near-Infrared Organic Molecules to Reduce Fine Cytotoxicity and to Image Thicker Samples
Among the synthetic modifications of known fluorophores, evolution of the skeleton of fluorescein is representative of the recent impact of chemistry on the conception of dyes. Indeed, fluorescein is a relatively simple tricyclic molecule possessing two phenols, with absorption and emission wavelengths of around 490 and 510 nm ( Figure 13C). The replacement of phenols by amines or dialkylamines led to the development of the rhodamine dye family with absorption/emission wavelengths of 543/565 nm for rhodamine B ( Figure 13C) [217]. Modifications of the skeleton with the introduction of silicon in rhodamines led to the development of Sila-Rhodamines (SiR) as powerful near-infrared (NIR) probes [218][219][220]. The replacement of O by Si in rhodamines leads to a red shift of both absorption and emission wavelengths resulting from a lowering of the excited state energy levels. Further modifications of substituents on the nitrogen atoms led to the development of Janelia Fluor [221] (azetidine) and Potomac dyes (azepane) [220], which have superior brightness and stability to SiR. Similarly, replacement of O by phosphorus atom in rhodamines led to the development of Nebraska dyes [222] or others [223] also displaying NIR fluorescence ( Figure 13C).
Some of the fluorescent dyes used for bioimaging have high affinity for a specific organelle due to their nature (polarity, charge, etc.) or to the presence of a targeting agent. Among the commercially available and widely used markers, specific stains can be found for cell nucleus (DAPI or Hoechst 33342), acidic organelles (Lysotrackers), endoplasmic reticulum (ERtrackers), or mitochondria (Mitotracker). They can also be chemically modified to act as a profluorophore that an enzymatic or chemical reaction will convert back into the fluorophore (leading to an OFF → ON

Development of Small Near-Infrared Organic Molecules to Reduce Fine Cytotoxicity and to Image Thicker Samples
Among the synthetic modifications of known fluorophores, evolution of the skeleton of fluorescein is representative of the recent impact of chemistry on the conception of dyes. Indeed, fluorescein is a relatively simple tricyclic molecule possessing two phenols, with absorption and emission wavelengths of around 490 and 510 nm ( Figure 13C). The replacement of phenols by amines or dialkylamines led to the development of the rhodamine dye family with absorption/emission wavelengths of 543/565 nm for rhodamine B ( Figure 13C) [217]. Modifications of the skeleton with the introduction of silicon in rhodamines led to the development of Sila-Rhodamines (SiR) as powerful near-infrared (NIR) probes [218][219][220]. The replacement of O by Si in rhodamines leads to a red shift of both absorption and emission wavelengths resulting from a lowering of the excited state energy levels. Further modifications of substituents on the nitrogen atoms led to the development of Janelia Fluor [221] (azetidine) and Potomac dyes (azepane) [220], which have superior brightness and stability to SiR. Similarly, replacement of O by phosphorus atom in rhodamines led to the development of Nebraska dyes [222] or others [223] also displaying NIR fluorescence ( Figure 13C).
Some of the fluorescent dyes used for bioimaging have high affinity for a specific organelle due to their nature (polarity, charge, etc.) or to the presence of a targeting agent. Among the commercially available and widely used markers, specific stains can be found for cell nucleus (DAPI or Hoechst 33342), acidic organelles (Lysotrackers), endoplasmic reticulum (ERtrackers), or mitochondria (Mitotracker). They can also be chemically modified to act as a profluorophore that an enzymatic or chemical reaction will convert back into the fluorophore (leading to an OFF → ON signal), thus acting as chemosensors for analytes or as proof of biological activity (Table 1). Among these fluorophores, epicocconone, an azaphilone natural product isolated from the Epicoccum nigrum fungus, emerged as a profluorescent natural product that has been extensively used for protein staining on electrophoresis gels and for bioimaging [224] (Figure 14). Due to its water solubility, low molecular weight, nontoxicity, and cell permeability, epicocconone showed strong potential for live cell imaging [89,113]. The chemical synthesis, guided by DFT and photophysical studies, led to the development of a synthetic analogue with improved photostability and to epicocconone-hemicyanine hybrids with NIR emission [225][226][227][228][229][230][231].
Chemosensors 2018, 6, x 22 of 45 signal), thus acting as chemosensors for analytes or as proof of biological activity (Table 1). Among these fluorophores, epicocconone, an azaphilone natural product isolated from the Epicoccum nigrum fungus, emerged as a profluorescent natural product that has been extensively used for protein staining on electrophoresis gels and for bioimaging [224] (Figure 14). Due to its water solubility, low molecular weight, nontoxicity, and cell permeability, epicocconone showed strong potential for live cell imaging [89,113]. The chemical synthesis, guided by DFT and photophysical studies, led to the development of a synthetic analogue with improved photostability and to epicocconone-hemicyanine hybrids with NIR emission [225][226][227][228][229][230][231]. In bioimaging, epicocconone and its naphtyl analogue were compared through one-photon (1P) and two-photon (2P) advanced light microscopy studies using PC12 cells [113]. Results obtained with the synthetic analogue on PC12 cells showed more interesting characteristics than the natural product in terms of band sharpness, fluorescent intensity, photobleaching (fluorescence is only 25% weaker after a 30 min acquisition), and Stokes shift in 1P and 2P microscopies ( Figure 15A). The synthetic analogue did not label the nucleus of the PC12 cell but induced a moderate labeling of plasma and nuclear membranes and of filamentous structures in the cytoplasm, and an intense labeling of numerous intracellular vesicle-like structures around the nucleus ( Figure 15B). The skeleton of epicocconone could be further modified by making epicoccone-hemicyanine hybrids, based on an internal charge transfer (ICT) between different hemicyanine groups as electron donors and the naphtylketoenol group of the previous synthetic analogue as electron In bioimaging, epicocconone and its naphtyl analogue were compared through one-photon (1P) and two-photon (2P) advanced light microscopy studies using PC12 cells [113]. Results obtained with the synthetic analogue on PC12 cells showed more interesting characteristics than the natural product in terms of band sharpness, fluorescent intensity, photobleaching (fluorescence is only 25% weaker after a 30 min acquisition), and Stokes shift in 1P and 2P microscopies ( Figure 15A). signal), thus acting as chemosensors for analytes or as proof of biological activity (Table 1). Among these fluorophores, epicocconone, an azaphilone natural product isolated from the Epicoccum nigrum fungus, emerged as a profluorescent natural product that has been extensively used for protein staining on electrophoresis gels and for bioimaging [224] (Figure 14). Due to its water solubility, low molecular weight, nontoxicity, and cell permeability, epicocconone showed strong potential for live cell imaging [89,113]. The chemical synthesis, guided by DFT and photophysical studies, led to the development of a synthetic analogue with improved photostability and to epicocconone-hemicyanine hybrids with NIR emission [225][226][227][228][229][230][231]. In bioimaging, epicocconone and its naphtyl analogue were compared through one-photon (1P) and two-photon (2P) advanced light microscopy studies using PC12 cells [113]. Results obtained with the synthetic analogue on PC12 cells showed more interesting characteristics than the natural product in terms of band sharpness, fluorescent intensity, photobleaching (fluorescence is only 25% weaker after a 30 min acquisition), and Stokes shift in 1P and 2P microscopies ( Figure 15A). The synthetic analogue did not label the nucleus of the PC12 cell but induced a moderate labeling of plasma and nuclear membranes and of filamentous structures in the cytoplasm, and an intense labeling of numerous intracellular vesicle-like structures around the nucleus ( Figure 15B). The skeleton of epicocconone could be further modified by making epicoccone-hemicyanine hybrids, based on an internal charge transfer (ICT) between different hemicyanine groups as electron donors and the naphtylketoenol group of the previous synthetic analogue as electron The synthetic analogue did not label the nucleus of the PC12 cell but induced a moderate labeling of plasma and nuclear membranes and of filamentous structures in the cytoplasm, and an intense labeling of numerous intracellular vesicle-like structures around the nucleus ( Figure 15B). The skeleton of epicocconone could be further modified by making epicoccone-hemicyanine hybrids, based on an internal charge transfer (ICT) between different hemicyanine groups as electron donors and the naphtylketoenol group of the previous synthetic analogue as electron acceptor (Figure 14). Unlike epicocconone or its naphtyl analogue, this epicocconone-hemicyanine hybrid is natively fluorescent with emission wavelengths red-shifted to the NIR region. It was shown that the hybrids have in general a large Stokes shift (about 80 nm) and an emission maximum ranging from 715 to 795 nm, depending on the nature of the hemicyanine moiety [225].

Development of Organic Probes to Increase Resolution in Microscopy
In wide-field and confocal microscopy, a single fluorophore can only be precisely localized if it is separated by a few hundred nanometers from others, due to the diffraction of light (see also Section 2.3). With regards to emission depletion and stochastic reconstruction principles, photophysical properties of probes have been recently reassessed to find the most valuable chromophores [232].

Development of Organic Probes for STED Nanoscopy
When used in a STED nanoscopy set up, fluorophores are exposed to the high intensity of the laser beam (see also Section 5) used to narrow the fluorescence into a very small volume; therefore, one of the key parameters of a STED fluorophore is photostability. A variety of mechanisms may lead to photodamage as excited-state absorption can produce chemically unstable upper energy states. Degradation is even more pronounced if triplet states are involved due to their long lifetime and their ability to generate highly reactive ROS and radicals [233]. These latter reactive species lead also to biological photodamage [234,235]. Other photobleaching effects are isomerization, oxidations, or reductions often leading to blue-emitting photoproducts, or the formation of twisted states. All these effects lower the fluorescence quantum yield. Another parameter is the Stokes shift, as the STED irradiation wavelength has to be different enough from the fluorophore excitation wavelength to avoid excitation of the fluorophore during the depletion step [96]. Therefore, when choosing a fluorophore, the equipment specification also has to be taken into consideration as the fluorescence wavelength should match the STED depletion wavelength [236]. The photophysical properties of many available fluorophores were assessed for STED nanoscopy [96]. In order to be effective and to avoid a strong fluorescent background, nanoscopy probes have to be specific. On the one hand, some fluorophores can be activated only by interaction with specific biomolecules; for example, a ruthenium complex was used to image DNA [237]. On the other hand, STED probes can be fluorophore-targeting agent conjugates, the most widespread targeting agents being antibodies even though they necessitate working with fixed cells. Live cell imaging requires a targeting agent able to internalize in cells, such as taxanes that allow the imaging of tubulin in living tissues [238], and biarsenical dyes [147], benzylguanines/benzylcytosine [144,239], and synthetic ligands [149] that were used for tetracysteine tag, SNAP/CLIP, and HaloTag fusion protein labeling, respectively. The stability of fluorophores, and, hence, their efficacy, also depends on their cellular environment as biological processes may damage excited chromophores. A good answer can be to localize fluorophores in hydrophobic cell compartments [240] or to encapsulate them in protecting fluorogen-activating peptides (FAPs) [241]. Hell's group from the Max Planck Institute for Biophysical Chemistry (Göttingen, Germany) is currently undertaking molecular engineering to provide optimized fluorophores. While these molecules have been, at this point, only assessed on fixed cells due the use of immunolabeling, they seem very promising for live cell imaging ( Figure 13). Rhodamines were modified to improve their photostability and their ability to internalize in cells ( Figure 16A).  [109,110,175] isolated cell or multi cell layers permeation acetate derivatives of fluorescein (FDA) [110,111] organ permeation Syto 61, Sytox Orange, TO-PRO-1/3 [173,174] Cell tracking isolated cell/organ/organism permeation/injection CellTracker/DiI/Cyto-Tracers/WGA [114,116,176,179,185,186] isolated cell incorporation in lipid membrane CellVue, CytoID Red [115][116][117] isolated cell/organ/organism infection (lentivectors) Cyto-Tracers [132] organ/organism injection Dextran-conjugated/SiR [182,188] organism transfection/electroporation Plasmid contruction [140,141] Identification of membrane, organelles and macromolecules plasma membrane isolated cell/organ/organism reversible binding WGA [114,122] plasma membrane organ reversible binding IB4 [174] cytoskeleton isolated cell/organ permeation SiR-Actin/Tubulin/Taxanes [130,131,237] nucleus isolated cell or multi cell layers permeation Hoechst/SYTO/Nuc/dinuclear RuII-based complex 1 4+ [112,113,123,124,237] mitochondria isolated cell/organ/organism permeation Mitotracker [125][126][127]187] lysosome isolated cell/organ/organism permeation Lysotracker, SiR-Lysosome [128][129][130][131] glycan isolated cell/organ/organism click chemistry azide or alkyl monosaccharide [133,134,201] plant primary cell wall isolated cell/organ/organism click chemistry azide or alkyl monosaccharide [135,137,197,200] plant secondary cell wall isolated cell/organ/organism click chemistry azide or alkyl monolignol [198] Cellular activity potential membrane activity isolated cell permeation JC-1 [160] ionic indicator isolated cell or multi cell layers permeation fluo-4 (Ca 2+ ), SBFI (Na 2+ ), Fluo-Zin, KMG-20/27 [151][152][153][154][156][157][158] ionic indicator multilayers, organ permeation oregon green (Ca 2+ ) [176,177] ROS detection isolated cell or multi cell layers permeation H2DCFDA, RedocSensor, SiR-NO, . . . [160][161][162][163] caspase activity isolated cell or multi cell layers permeation FITC-ZVAD-FMK [110] plamid contruction/Biosensors isolated cell transfection GFP family or derivative protein [140,165] plamid contruction/Biosensors organ/organism transfection by electroporation GFP family or derivative protein [181,189,190] pathway signal transduction isolated cell infection (bacculovirus) BacMam system [113] pathway signal transduction isolated cell transfection FRET Biosensors [166][167][168][169][170][171] pathway signal transduction organ infection (HSV) Biosensors [179,180] Chemosensors 2018, 6, 40

of 45
The best improvements were obtained through the introduction of side chains bearing phosphonates or hydroxyl groups and substitution of the lateral aromatic ring ( Figure 13A). On the other hand, rigidification of the amino moieties improves fluorescence by preventing the formation of twisted low-emitting states [242]. Hell's group also modified coumarins and higher stability was obtained by introducing a new photostable electron-withdrawing group based on an original betaine structure [243] (Figure 16B). These coumarins are of particular interest as they feature high Stokes shift due to their "push-pull" nature, allowing two-color STED images when combined with rhodamines. The best improvements were obtained through the introduction of side chains bearing phosphonates or hydroxyl groups and substitution of the lateral aromatic ring ( Figure 13A). On the other hand, rigidification of the amino moieties improves fluorescence by preventing the formation of twisted low-emitting states [242]. Hell's group also modified coumarins and higher stability was obtained by introducing a new photostable electron-withdrawing group based on an original betaine structure [243] (Figure 16B). These coumarins are of particular interest as they feature high Stokes shift due to their "push-pull" nature, allowing two-color STED images when combined with rhodamines. Although only one STED wavelength is applied, the fluorophores are discriminated thanks to their very distinct excitation wavelengths. The quest for new optimized chromophores leads to exploring new chemical structures, e.g., a phosphole P-oxide-based chromophore showed promising photostability for application as a STED probe [244] ( Figure 16C). The stability of fluorophores can be improved by encapsulation with dendrimers [245] or rotaxanes [215] which prevent reaction of excited-state chromophores with biological molecules. An alternative approach to more photostable structures consists of healing bleached chromophores thanks to antifading agents. These agents can be triplet states, or redox or radical quenchers used as additives during fluorescence imaging. However, their efficiency is related to their ability to interact quickly with bleached chromophores; this requires a high concentration which can disturb biological media. This could also be achieved by directly attaching the photostabilizing agent to the fluorophores to obtain self-healing chromophores [246]. Plasmonic nanoparticles can also be used to improve STED nanoscopy, as they have the ability to concentrate the light electromagnetic field in their vicinity. As a result, they allow a reduction in the power of irradiation depletion used to switch off the fluorescence of grafted fluorophores, including less photodamage to biological tissues [247].

Development of Organic Probes for Stochastic Approaches
As described previously (Section 2, Figure 8), stochastic techniques are classified into two main categories: those using photoactivable fluorophores, which are then destroyed under irradiation, and those relying on switchable fluorophores, which can be reversibly activated and deactivated. Among the first category, the PALM technique was introduced in 2006, and is based on the use of photoactivable fluorescent proteins (Pa-GFP, Pa-mcherry) or photoactivable "small molecule" fluorophores [248] (Figure 17A). In the second category, the STORM technique relies on reversible photoswitching; it was originally developed using Cy5 fluorophores reversibly switched off to a dark state thanks to a photo-triggered reaction with biological thiols [100,249,250]. This approach can be generalized to the majority of cyanine fluorophores commonly used in classical fluorescence imaging. Other common fluorophores derived from rhodamine were also used, the dark state being generated from diverse mechanisms like photoredox reaction or the formation of long-living triplet states [251]. However, these small molecules systems are limited due to their "switching fatigue"; to date, photoswitchable fluorescent proteins are the most stable photoswitching systems [252]. In an Although only one STED wavelength is applied, the fluorophores are discriminated thanks to their very distinct excitation wavelengths. The quest for new optimized chromophores leads to exploring new chemical structures, e.g., a phosphole P-oxide-based chromophore showed promising photostability for application as a STED probe [244] ( Figure 16C). The stability of fluorophores can be improved by encapsulation with dendrimers [245] or rotaxanes [215] which prevent reaction of excited-state chromophores with biological molecules. An alternative approach to more photostable structures consists of healing bleached chromophores thanks to antifading agents. These agents can be triplet states, or redox or radical quenchers used as additives during fluorescence imaging. However, their efficiency is related to their ability to interact quickly with bleached chromophores; this requires a high concentration which can disturb biological media. This could also be achieved by directly attaching the photostabilizing agent to the fluorophores to obtain self-healing chromophores [246]. Plasmonic nanoparticles can also be used to improve STED nanoscopy, as they have the ability to concentrate the light electromagnetic field in their vicinity. As a result, they allow a reduction in the power of irradiation depletion used to switch off the fluorescence of grafted fluorophores, including less photodamage to biological tissues [247].

Development of Organic Probes for Stochastic Approaches
As described previously (Section 2, Figure 8), stochastic techniques are classified into two main categories: those using photoactivable fluorophores, which are then destroyed under irradiation, and those relying on switchable fluorophores, which can be reversibly activated and deactivated. Among the first category, the PALM technique was introduced in 2006, and is based on the use of photoactivable fluorescent proteins (Pa-GFP, Pa-mcherry) or photoactivable "small molecule" fluorophores [248] (Figure 17A). In the second category, the STORM technique relies on reversible photoswitching; it was originally developed using Cy5 fluorophores reversibly switched off to a dark state thanks to a photo-triggered reaction with biological thiols [100,249,250]. This approach can be generalized to the majority of cyanine fluorophores commonly used in classical fluorescence imaging. Other common fluorophores derived from rhodamine were also used, the dark state being generated from diverse mechanisms like photoredox reaction or the formation of long-living triplet states [251]. However, these small molecules systems are limited due to their "switching fatigue"; to date, photoswitchable fluorescent proteins are the most stable photoswitching systems [252]. In an effort to close this gap, new fluorophores based on diarylethene structures selected for their photochromic behavior were synthesized by Hell's group [253] (Figure 17B).  Figure 17B). Small organic fluorophores are complementary to bioengineered fluorescent proteins. Small molecules may lack solubility, or suffer from uncontrolled biodistribution or enzymatic instability. One of the main challenges with small molecules is targeting. Indeed, monoclonal antibodies are the most commonly used targeting agent for small molecules in fixed cells due to their high specificity; however, they are not able to internalize in living cells. Therefore, other targeting agents have been developed to cope with this problem, such as lectins [122], or drugs like Paclitaxel [238]. On one hand, FPs directly expressed inside cells do not present this problem, but require bioengineering preliminary work to obtain appropriate proteins; the introduction of such large tags may modify the activity or the structure of imaged proteins. On the other hand, small molecules are easier to modify, and can be built as a platform combining both imaging and biological properties or other functionalities, i.e., "Fluorescent False Neurotransmitters" [254], photoclick labeling dyes [255], and profluorescent ligands of genetically encoded tags [256,257].

Generation, Collection, Detection, and Analysis of the Fluorescence Signal from Living Samples
As proposed by the PSI triad concept with interrelationship between pillars, general improvement of the fluorescence signal is the result of better probes detected with adapted and efficient instruments. Consequently, specialist knowledge of light sources, objectives, detectors, and image processing is also essential to optimize live cell imaging.

Light Sources
Originating from a light source that can be a mercury/xenon arc lamp, a light-emitting diode (LED), or a continuous or pulsed laser, photons are absorbed by the probe that emits in return a signal of fluorescence. Considering the adverse effects of phototoxicity [258] and photobleaching on cell activity and time-lapse duration, a comparison of light source characteristics is presented here ( Table 2). A first group of sources with low light power is represented by supercontinuum sources. Supercontinuum lasers, also called "white lasers", which result from the dispersion of a continuous laser (1032 nm) into a nonlinear material (crystal fiber), offer a broad spectral band of light emission (250-1100 nm) with low laser power (<5 mW) [259]. A second group of light sources with moderate to high (5-500 mW) light power is represented by gas lasers, arc lamps, diode lasers, and LEDs [260]. The third group comprises depletion lasers for STED nanoscopy and solid-state lasers like Ti-sapphire lasers dedicated to two-photon absorption applications. Tunable pulsed Ti-sapphire lasers emit light in the range of 680 to 1080 nm with high power (up to 4 W) [261]. Consequently, electro-or acousto-optic modulators (EOM and AOM) are necessary to reduce the light power which is delivered to living samples. Therefore, phototoxicity and photobleaching are significantly reduced Small organic fluorophores are complementary to bioengineered fluorescent proteins. Small molecules may lack solubility, or suffer from uncontrolled biodistribution or enzymatic instability. One of the main challenges with small molecules is targeting. Indeed, monoclonal antibodies are the most commonly used targeting agent for small molecules in fixed cells due to their high specificity; however, they are not able to internalize in living cells. Therefore, other targeting agents have been developed to cope with this problem, such as lectins [122], or drugs like Paclitaxel [238]. On one hand, FPs directly expressed inside cells do not present this problem, but require bioengineering preliminary work to obtain appropriate proteins; the introduction of such large tags may modify the activity or the structure of imaged proteins. On the other hand, small molecules are easier to modify, and can be built as a platform combining both imaging and biological properties or other functionalities, i.e., "Fluorescent False Neurotransmitters" [254], photoclick labeling dyes [255], and profluorescent ligands of genetically encoded tags [256,257].

Generation, Collection, Detection, and Analysis of the Fluorescence Signal from Living Samples
As proposed by the PSI triad concept with interrelationship between pillars, general improvement of the fluorescence signal is the result of better probes detected with adapted and efficient instruments. Consequently, specialist knowledge of light sources, objectives, detectors, and image processing is also essential to optimize live cell imaging.

Light Sources
Originating from a light source that can be a mercury/xenon arc lamp, a light-emitting diode (LED), or a continuous or pulsed laser, photons are absorbed by the probe that emits in return a signal of fluorescence. Considering the adverse effects of phototoxicity [258] and photobleaching on cell activity and time-lapse duration, a comparison of light source characteristics is presented here ( Table 2). A first group of sources with low light power is represented by supercontinuum sources. Supercontinuum lasers, also called "white lasers", which result from the dispersion of a continuous laser (1032 nm) into a nonlinear material (crystal fiber), offer a broad spectral band of light emission (250-1100 nm) with low laser power (<5 mW) [259]. A second group of light sources with moderate to high (5-500 mW) light power is represented by gas lasers, arc lamps, diode lasers, and LEDs [260]. The third group comprises depletion lasers for STED nanoscopy and solid-state lasers like Ti-sapphire lasers dedicated to two-photon absorption applications. Tunable pulsed Ti-sapphire lasers emit light in the range of 680 to 1080 nm with high power (up to 4 W) [261]. Consequently, electro-or acousto-optic modulators (EOM and AOM) are necessary to reduce the light power which is delivered to living samples. Therefore, phototoxicity and photobleaching are significantly reduced with supercontinuum lasers. High-power solid-state lasers may induce large phototoxicity and photobleaching but in a restricted focal volume due to the two-photon principle. In contrast, they have the advantages of emitting red and near-infrared photons that are less cytotoxic. Probe and living sample preservations could also be optimized by reducing the pixel time, i.e., limiting the duration of laser impact on a pixel through an increase in rotation speed for spinning disk microscopy [262] or scanning speed (resonant scanner) in confocal/2P microscopy [36]. Exposure of living samples to light is also a major issue in nanoscopy approaches. For STED nanoscopy, the power of the depletion laser might be deleterious for cellular structures [122]. However, depletion with new wavelengths in near-infrared or with pulsed infrared lasers is preferred for live cell imaging [263]. The applications of stochastic nanoscopies to living samples are for the moment limited by the duration of the acquisition [264]. Structured illumination microscopy (SIM), which is compatible with most standard fluorophores, offers interesting resolutions between 50 and 100 nm but can also be limited in time resolution due to numerous pattern acquisitions [264]. Power measurements were obtained with a power meter (Thorlabs PM100D + S170C Sensor) in the absence of objective. * power measurement at 488 nm; ** power measurement at 800 nm; *** power measurement at 592 nm.

Objectives
For observation of living samples (isolated cells, tissue slices, organs, or organisms) and fluorescence signal collection, the choice or the strain of the objective is a major issue. Dry, multi-immersion, oil, water, and glycerol objectives are available ( Figure 18) [263]. The first rule is to respect as much as possible the refractive index between the aqueous incubation medium of the sample and the immersion medium of the objective. Consequently, water (n = 1.33) and glycerol (n = 1.3) objectives are more adapted for live cell imaging [265]. Due to repetitive movements or medium evaporating during long-time/multiposition acquisitions, dry objectives are nevertheless preferred despite their poor optical characteristics. More recently, commercial recurring refilled water systems have been developed to optimize water-objective images during long time lapses at 37 • C. The second rule is to consider the numerical aperture (NA) of the objective with regard to the requirements of signal collection, resolution, working distance (WD), and depth of field (DF). For high photon collection and high resolution, objectives with large NA (1.2 < NA < 1.49) are preferred in particular for intracellular localization purposes ( Figure 18) [266]. Some objectives are also equipped with a correction collar to limit image aberration due to fluctuations in cover glass thickness, temperature, and specimen inhomogeneities [267]. In contrast, small NA (0.02 < NA < 0.8) objectives with large WD and DF are used for tissue slice or organism studies ( Figure 18) [111,268]. It is also interesting to verify that the emission spectrum of the fluorescent probe completely fits with the transmission curve of the objective. Finally, autofocus systems might be helpful for mid-length and long time lapses [269]. For nanoscopy, new objectives with WD and DF up to 300 and 150 µm now facilitate STED approaches in living tissues [269]. Therefore, depending on the type of sample and the scientific question, the choice of the objective is crucial to appropriately detecting the fluorescence signal of interest.

Objectives
For observation of living samples (isolated cells, tissue slices, organs, or organisms) and fluorescence signal collection, the choice or the strain of the objective is a major issue. Dry, multi-immersion, oil, water, and glycerol objectives are available ( Figure 18) [263]. The first rule is to respect as much as possible the refractive index between the aqueous incubation medium of the sample and the immersion medium of the objective. Consequently, water (n = 1.33) and glycerol (n = 1.3) objectives are more adapted for live cell imaging [265]. Due to repetitive movements or medium evaporating during long-time/multiposition acquisitions, dry objectives are nevertheless preferred despite their poor optical characteristics. More recently, commercial recurring refilled water systems have been developed to optimize water-objective images during long time lapses at 37 °C. The second rule is to consider the numerical aperture (NA) of the objective with regard to the requirements of signal collection, resolution, working distance (WD), and depth of field (DF). For high photon collection and high resolution, objectives with large NA (1.2 < NA < 1.49) are preferred in particular for intracellular localization purposes ( Figure 18) [266]. Some objectives are also equipped with a correction collar to limit image aberration due to fluctuations in cover glass thickness, temperature, and specimen inhomogeneities [267]. In contrast, small NA (0.02 < NA < 0.8) objectives with large WD and DF are used for tissue slice or organism studies ( Figure 18) [111,268]. It is also interesting to verify that the emission spectrum of the fluorescent probe completely fits with the transmission curve of the objective. Finally, autofocus systems might be helpful for mid-length and long time lapses [269]. For nanoscopy, new objectives with WD and DF up to 300 and 150 µm now facilitate STED approaches in living tissues [269]. Therefore, depending on the type of sample and the scientific question, the choice of the objective is crucial to appropriately detecting the fluorescence signal of interest.

Detectors
Depending of the type of imaging system (wide-field, spinning disk, confocal, 2P, nanoscopy, etc.), single-point or array detectors are used for fluorescence signal detection [7]. Different key parameters have to be considered for each type of sensor. Single-point detectors such as photomultiplier tubes (PMTs) and hybrid photodetectors (HPDs) have to be compared with regard to their quantum efficiency (QE), their signal-to-noise ratio (SNR) value, and their time response [7]. Since HPDs combine the advantages of the vacuum technology of PMT and avalanche photodiode semiconductor diode (APD) technology, they offer low-light detection (×1.3-1.4), especially for single molecule detection, excellent timing resolution (×2-3), and noise close to 0 [269]. Due to semiconductor diode technology, a photon counting mode is also available with HPD, allowing direct fluorescence quantification [270]. In contrast to single-point detectors, there is a large diversity of array detectors that can be distributed into three groups: Charge-Coupled Device cameras (CCD), Electron-Multiplication CCD cameras (EM-CCD), and scientific Complementary Metal Oxide Semiconductor (sCMOS) cameras [270]. For live cell imaging, criteria such as frame rate, QE, SNR, and pixel size are generally compared to reach appropriate temporal and spatial resolution. CCD cameras appeared almost 50 years ago with continuous development since then for time response and QE. Consequently, EM-CCD cameras were developed for the detection of low fluorescence signals, in particular for in vivo applications with back-illuminated sensors [271]. Nowadays, sCMOS cameras allow larger field of view than other sensors, small pixel size, and a very good SNR [272]. With a rapid frame rate, they are fast sensors compared with CCD and EM-CCD cameras and have equivalent or lower QE [270]. Taken together, scientific requirements such as spatial and temporal resolution and low fluorescence signal may be decisive for the choice of array detector.

Instrument Performance
As described in the above paragraphs, light sources, objectives, scanners, and detectors are key elements for appropriate live cell imaging with fluorescent probes. Consequently, the stability and performance of these elements during acquisition are essential to obtaining experimental reproducibility and repeatability of confident measurements [273]. Thus, regular control of laser power, field illumination, and detector sensitivity over time is a requirement of performing successful experiments. In the context of acquisition of one shot or short time lapses, field illumination and detector sensitivity should be stable (Table 3). Table 3. Potential instrumental instabilities during one-time acquisition, and short and long time lapses. In contrast, instability of laser power may appear in mid-length or long time lapses [273]. Similarly, environmental and room temperature as well as xyz positioning may vary during mid-length and long time-lapses. Please note that variations of temperature are often responsible for variations of stage drifts [273,274]. Such variations can be controlled by introducing focus-keeping systems for long-term monitoring, limiting loss of information [267]. When required, saturation of the local atmosphere with CO 2 (5%) can be achieved by an automatic gas mixer or home-made systems. Variations of environmental temperature and CO 2 concentration induce biological artifacts that can lead to misinterpretation of the results.

Image Processing
Imaging living samples together for as long as possible while preserving the fluorescence signal from photobleaching is a major issue. In this context, compromises of intensity of light sources, time of exposure or time of scanning, and signal amplification methods are mandatory. These compromises generally lead to degradation of the image quality with an increase of the noise and, consequently, a decrease in SNR. The degradation can be assumed, giving priority to biological sample integrity and long life of the fluorescent probe. However, to overcome the noise, image processing through deconvolution has several advantages leading to an increase in SNR, contrast, and resolution ( Figure 19). Thus, deconvolution is of main importance in nanoscopy but also in confocal and wide-field microscopy with algorithms that integrate the characteristics of the optical system (objective, NA, immersion medium, etc.). Nevertheless, successful deconvolution requires rigorous backward imaging acquisition with appropriate sampling in x, y, and z dimensions according to the Nyquist criterion. In addition, pitfalls of acquisition such as mechanical drift and shift, spectral crosstalk of fluorescent probes, and saturation of the signal must be strictly eliminated.
Degradation of image quality should, however, be limited for tracking experiments, in particular in organotypic slices, organs, and organisms due to the risk of lost cells, organelles, or molecules during time lapse. Consequently, detection of "objects" over time should be improved through commercial or open source image processing programs [275]. In particular, deconvolution and combination of morphologic filters (erosion, dilatation, etc.) facilitate the efficiency of automatic or semi-automatic tracking [268]. However, home-made strategies with dedicated algorithms are often necessary to fully match with the expected results [276,277]. mid-length and long time-lapses. Please note that variations of temperature are often responsible for variations of stage drifts [273,274]. Such variations can be controlled by introducing focus-keeping systems for long-term monitoring, limiting loss of information [267]. When required, saturation of the local atmosphere with CO2 (5%) can be achieved by an automatic gas mixer or home-made systems. Variations of environmental temperature and CO2 concentration induce biological artifacts that can lead to misinterpretation of the results.

Image Processing
Imaging living samples together for as long as possible while preserving the fluorescence signal from photobleaching is a major issue. In this context, compromises of intensity of light sources, time of exposure or time of scanning, and signal amplification methods are mandatory. These compromises generally lead to degradation of the image quality with an increase of the noise and, consequently, a decrease in SNR. The degradation can be assumed, giving priority to biological sample integrity and long life of the fluorescent probe. However, to overcome the noise, image processing through deconvolution has several advantages leading to an increase in SNR, contrast, and resolution ( Figure 19). Thus, deconvolution is of main importance in nanoscopy but also in confocal and wide-field microscopy with algorithms that integrate the characteristics of the optical system (objective, NA, immersion medium, etc.). Nevertheless, successful deconvolution requires rigorous backward imaging acquisition with appropriate sampling in x, y, and z dimensions according to the Nyquist criterion. In addition, pitfalls of acquisition such as mechanical drift and shift, spectral crosstalk of fluorescent probes, and saturation of the signal must be strictly eliminated.
Degradation of image quality should, however, be limited for tracking experiments, in particular in organotypic slices, organs, and organisms due to the risk of lost cells, organelles, or molecules during time lapse. Consequently, detection of "objects" over time should be improved through commercial or open source image processing programs [275]. In particular, deconvolution and combination of morphologic filters (erosion, dilatation, etc.) facilitate the efficiency of automatic or semi-automatic tracking [268]. However, home-made strategies with dedicated algorithms are often necessary to fully match with the expected results [276,277].

Conclusions
One of the roles of CIPs is to support researchers from both the public and private sectors in their choice of adapted fluorescent probe for their scientific projects. In addition, CIPs closely work

Conclusions
One of the roles of CIPs is to support researchers from both the public and private sectors in their choice of adapted fluorescent probe for their scientific projects. In addition, CIPs closely work with research laboratories that develop new strategies to improve the fluorescence properties of probes including targeting and adaptation to advanced imaging technologies (2P microscopy, STED nanoscopy, etc.).
The progress made in chemistry, optics, electronics, and fluorescence microscopy techniques has allowed the frontiers of bioimaging of living samples to be pushed back. Chemistry has been and is still needed to provide molecules with higher stability and with photophysical properties compatible with the use of high-energy lasers. While conventional 1P and 2P microscopies are routinely used in bioimaging, many techniques are now being developed for nanoscopy that will allow a deeper understanding of biological processes. The progress of DFT calculations and the development of new synthetic methodologies allow the synthesis of rationally designed small fluorescent organic molecules, in particular, modification of a basic skeleton or introduction of new substituents aiming at gaining brightness, photostability, and selectivity in bioimaging along with tuning absorption and emission wavelengths.
For fluorescent labeling, both the bioavailability of the probe and the type of living sample have to be considered. Consequently, the method of labeling may be determined by the "cellular environment", i.e., isolated cells, cells within an organotypic slice or organ, or cells within an organism. For that, a large diversity of labeling strategies from simple diffusion of cell-permeant probes to engineered fluorescent proteins expressed by animals, plants, or micro-organisms is available. Click chemistry that results from the ligation of non-natural metabolite derivatives with a fluorescent reporter is now widely used to visualize specific molecules, such as glycan and lipids, for which genetically encoded reporters are not possible.
Beyond classical spectral specifications of light sources and detectors to excite and to detect, respectively, a fluorescent probe, it is important to pay particular attention to instruments in the context of living samples. As a matter of fact, the tricky issue is to use low light power to preserve the sample as much as possible and to limit the photobleaching as much as possible while reaching appropriate spatial and/or temporal resolution. Consequently, the brightness and photostability of the fluorescent probes are preponderant parameters. In addition, we have shown in this review that the choices and performance of the instruments including the light sources (supercontinuum, diode, gas, and solid-state lasers) and the detectors (PMT, HyD, sCMOS, CCD, or EM-CCD), together with the mode of acquisition (resonant scanner, spinning disk), are crucial for live cell imaging. Light power can also be further reduced by developing specific post-acquisition image processing procedures such as deconvolution to achieve similar SNR and spatial resolution but with lower light exposure. Taken together, the concept of the Probe-Sample-Instrument (PSI) triad aims to identify the criteria that will help in making the appropriate choice of fluorescent organic probe for living cell studies.