Electrorotation: A Spectroscopic Imaging Approach to Study the Alterations of the Cytoplasmic Membrane

Adalberto Bonincontro¹, Gianfranco Risuleo^2*

¹Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy.
²Dipartimento di Biologia e Biotecnologie, Sapienza Università di Roma, Rome, Italy.

DOI: 10.4236/ami.2015.51001                

Abstract

Electrorotation (ER) is a technique allowing the characterization of the surface properties of a variety of supra-molecular aggregates and living cultured cells as well as cellular organelles and biological materials in general. In particular, this technique allows measuring two important physical parameters of the cell membrane: specific capacitance and specific conductance. These parameters are strictly related to the structure/function relationships of the biological membrane; ER becomes thus a powerful means to investigate a number of phenomena involving the membrane integrity. These phenomena may originate from treatments with exogenous molecules and/or from pathological effects. Concerning these aspects, the study of the transfer of exogenous material (i.e. cat-anionic vesicles or liposomes) across the cell membrane assumes a high importance. This review is focused on the physical functioning principles of ER and on the quantitative analysis of the experimental measurements. This work also reports on different fields of application of ER with particular reference to data obtained in our laboratory. The investigation of the alterations of the cytoplasmic membrane function, as evidenced by this strategy, will be illustrated in detail.

Keywords

Electrorotation, Physical Principles, Membrane Dielectric Parameters, Molecular/Cell Biology

1. Introduction

The cytoplasmic membrane represents the bio-molecular structure allowing the cytoplasm matrix to communicate with the outer world. The transport of substances can be passive or active. In this latter case the cell is forced to expend energy in the process. The membrane is endowed of an intrinsicelectrical potential: therefore it works as a highly selective filter. Biological membranes participate to a number of transport mechanisms such as: passive osmosis and diffusion; endocytosis and exocytosis as well as transmembrane protein channels [1] .

In the light of what just presented, the membrane integrity plays a fundamental role in a number of cell functions such as metabolism, maintenance of the basal homeostasis and, although in an indirect manner, is also involved in cell differentiation and development. Recently, it has become clear the role of the cell membrane in “filtering” the paracrine apoptogenic and/or intrinsic death signals: therefore the efficient functioning of the cell membrane is essential for cell survival and correct proliferation [for a recent review see: 2 and references therein]. The complexity and multiplicity of the cell membrane is depicted in Figure 1.

Furthermore, the cytoplasmic membrane is primarily implicated in the penetration of exogenous material of the most diverse nature. Entry of this material occurs, just to give two examples, during the processes of gene transfer or drug delivery. Therefore, investigating the integrity and efficiency of the plasma membrane becomes of primary importance: with respect to this, electrorotation represents an excellent tool giving a quantitative idea about the intra-membrane traffic and possible membrane damages. This technique permits, in fact, the characterization of the surface properties of a variety of supra-molecular aggregates in the micrometric size range. The main application of this biophysical methodology is represented by the study of living cells as well as cellular organelles. Since ER allows measuring the two essential parameters of the cell membrane (specific capacitance and conductance), it constitutes a powerful means to investigate a number of phenomena related to the membrane integrity. Considering this particular aspect, it should be pointed out that these parameters are strictly linked to the structure/function relationships of the biological membrane. In addition, one of the major advantages of ER consists in the possibility of carrying out observations on single cells. The measurements are based on the light microscopy analysis of rotating cells in an electric field and take into consideration a sample of cells with respect to their “biological history”: metabolic status, dimensions and modes of treatment.

In this review we provide a clear and detailed critical description of the technique and discuss a number of applications to cells subjected to various forms of treatments, such as: exposure to chemicals, viruses and supra-molecular aggregates. The results discussed here refer essentially to data from our laboratory without disregarding the work of other research groups.

2. Materials

2.1. Cell Cultures

The stable murine fibroblasts 3T6 line was used in all experiments carried out in our laboratories. The cultures were maintained according to routine procedure. Culture medium was DMEM-10% newborn serum supplemented with glutamine and penicillin-streptomycin. All treatments, with natural substances and liposomes, were performed on cells plated 24 hours earlier. Treatments were continued for 24 hours, if not otherwise specified.

Figure 1. Schematic representation of a typical cell membrane. The image is freely available and not covered by copyright. It was obtained from the www at the following link: https://en.wikipedia.org/wiki/Cell_membrane#mediaviewer/File:Cell_membrane_detailed_diagram_en.svg, We acknowledge the work of the original author of this picture: LadyofHats.

Prior to the electrorotational measurements the cells were trypsinized to detach them from the Petri dish.

2.2. Cationic liposome preparation

The cationic liposomes used in this work were obtained adding to the zwitterionic phospholipid [1,2-dimyris- toyl-sn-glycero-3-phosphocholine, DMPC] the cationic gemini surfactant [(2S,3S)-2,3-dimetoxy-1,4-bis(N,N- dime-thylamine)-butane]. In the text the liposome will be defined as DMPC-G. The aqueous dispersions of liposomes were prepared by extrusion as previously described. For details see [3] -[5] .

3. Electrorotation

Theory and Experiments

An electric field, applied to cell suspensions, induces on each single cell an effective dipole moment deriving from the different polarizability between solvent and plasma membrane. The applied electric field used in this technique is rotating to induce a revolution of cells around an axis orthogonal to the direction of the electric field and to the dipole moment. The phenomenon is visualized by a “classical” imaging technique represented by optical microscopy.

In fact, if the mechanism of interfacial polarization is in phase with the electric field, the induced dipole moment is aligned. Increasing the frequency of the field, the polarization mechanism undergoes a phase delay (dielectric relaxation) causing a torque moment and the cells rotate in an anti-field fashion. One should take into consideration that major alterations of the overall structure of the membrane, as in necrotic cells, create an electrical short-circuit at membrane level and the cell ceases to rotate.

This phenomenon is generated in the range of approximately 10⁴ - 10⁶ Hz; if the frequency increases further, the electric field traverses the plasma membrane and the sense of rotation is inverted in a co-field fashion. The interface is now between membrane and cytoplasm. In the kHz range, another relaxation occurs associated to the double electrical layer formed by the counter-ions and the mechanisms of surface conductivity. The formation of the double electrical layer is due to the presence of counter-ions in the proximity of the cell charged surface.

These relaxations are known respectively as α, β and γ dispersions. However, only the β dispersion is directly related to the dielectric properties of the plasma membrane [6] [7] . The rotation period (T) of the cell depends on the frequency (f) of the applied field, according to equation (1), which describes a Debye-like relaxation:

(1)

where, f^* is the relaxation frequency and T_min is the corresponding value of the period. The experimental data must be analyzed by fitting according to equation (1) to obtain the relaxation frequency. As an example of this analysis, Figure 2 reports the typical dependence of the rotation period by the field frequency of a generic cell suspension in an osmolar sucrose solution. The value of f^* appearing in equation (1) depends on the solvent conductivity according to the expression (2):

(2)

where C and G are, respectively, the specific capacitance and specific conductance of the plasma membrane of a cell with a radius R, σ_e is the solvent conductivity and σ_i is the conductivity of the cytoplasm considered as homogeneous. Since in general σ_e << σ_i equation (2) becomes:

(3)

The experimental approach is based on the measurement of the relaxation frequency as a function of the con-

Figure 2. Typical correlation between rotation period of the cell and applied electric frequency. As an example the curve obtained from untreated cells rotating in an osmolar solution. The curve results from the best fit according to equation (1). The inset shows two typical spheroidal cells in suspension as they appear at optical microscope. The bar is 20 μ.

ductivity of the dispersing medium, from which C and G can be calculated by a linear fit taking into account the cell radius. Typically, four dispersing solutions are used: sucrose 300 mM and the same solution supplemented with three NaCl concentrations: (0.5; 1.0; 1.5 mM).

The Debye model mimics the cell as a sphere surrounded by a thin homogeneous layer simulating the plasma membrane. In comparison to the complexity of the real biological system, this model is rather coarse; however it proved to be very effective to evaluate even slight changes in the dielectric properties of the cell membrane. The capacitance C is influenced by the biochemical and physical properties of the membrane. The conductance G is informative of the membrane function in terms metabolism/ion-transport. Therefore, this simplified model is commonly accepted as a good tool to investigate the biological membrane conditions [6] -[12] .

According to equation (3) the four relaxation frequencies are dependent on solvent conductivity in a linear fashion: from the slope and the intercept, the plasma membrane parameters C and G can be directly obtained (Figure 3). To have a good statistical estimation of the absolute value of C and G, a reasonable number of cells (at least 15) must be taken into consideration. The electro rotation apparatus, used in our laboratory, is implemented with a video-recording system permitting an accurate off-line image analysis [3] . In this way the data acquisition time is considerably shorter, thus avoiding possible artifacts due to cell vitality failure deriving from a prolonged suspension time in sub-optimal conditions.

The rotating electrical field was generated superimposing four square waves out of phase by 90°, with respect to each other. The square pulses were applied to the copper mini-plate electrodes of the measuring cell, which form a central circular cavity with a volume of about 10 μl (Figure 4). The whole set up was glued onto a microscope slide. An objective a magnification of 33× and a focal length of 1 cm was used. The microscope was connected to a CCD camera producing a further magnification (20×).

Following this procedure the values of C and G are obtained with an error margin not lower than 10%. In any case these data must be compared with the one obtained from cells subjected to bio-stresses of various nature. Even though 10% approximation on a single measurement may seem very large, one should bear in mind that the variations of these parameters with cells exposed to different agents may be very large and far above 10%. The microscopic technique allows also an accurate measurement of the actual cell radius, avoiding the use of average literature data, which may alter the final experimental conclusions.

4. Overview and application of electrorotation in biological fields

The technique of electro rotation is a non-invasive biophysical strategy used to study a vast variety of biological systems such as membrane of prokaryotic and eukaryotic cells subjected to chemical and biological stresses as well as whole organisms, viruses, bacteria and cells [3] [11] -[21] . The electro rotational data are often supported by an additional electrokinetic technique known as dielectrophoresis where non uniform AC electric fields are used to produce a translational motion in charged or uncharged particles [22] [23] . However, the work presented here is specifically devoted to review the main fields of application of the ER strategy. A detailed list of biological systems investigated by ER is reported in Table 1 with the appropriate references. The Table evidences the flexibility of this technique. The subsequent sections of this review will report a recollection of data mainly obtained in our laboratory.

Figure 3. Relaxation frequency (f^*) as a function of the solvent conductivity (σ_e). Experi- mental data refer to the same sample reported in the legend of figure 2. The straight line was obtained by a best fit according to equation (3).

Figure 4. Schematic image of the four-electrode measuring cell. Square waves out of phase by 90˚ generate the rotating electrical field. The copper mini-plate electrodes form a central cir- cular cavity of about 10 μl and the whole set up is glued onto a microscope.

Table 1. Overview of the main biological systems investigated by electrorotation.

In this table, only the application of ER to biological systems is reported; however it should be pointed out that also interaction of synthetic materials, such as latex beads and liposomes, has been investigated.

5. Effect of natural substances of common use in popular medicine and/or as dietary supplements

5.1. Semi purified methanol extract of Neem oil

Neem oil is a natural mixture obtained from the seeds of Azadirachta indica (A. Juss) known as neem tree. The oil composition is heterogeneous depending upon growth habitat and environmental situation; this oil is normally considered a by-product of more valuable components [44] also as dietary supplements as recently reviewed in [45] . It contains high levels of many organic different compounds. Azadirachtin, possibly the most studied component, is a tetra-nor-triterpenoid active as pest and insect control. We prepared a methanol extract of the whole oil defined as MEX which is deprived of the terpenoid/limonoid moiety, and therefore of azadirachtin: we tested its biological properties and effects on cultured cells. The biological effects exhibited by MEX, obviously, are not attributable to azadirachtin but rather to other bio-active molecules whose nature is yet to be fully clarified. In any case, our partially purified mixtures have an anti-proliferative action on cultured mammalian cells and their administration appears to activate the apoptotic pathway [46] . It is commonly accepted by published work that the cell membrane is involved in the progression of the apoptotic death [2 and references therein]. Therefore, it becomes of primary interest the investigation of the membrane biophysical features. To ad- dress this specific point we conducted electrorotation experiments on cells treated with MEX. The experimental data were fitted according to equation (1) to determine the relaxation frequency. Measurements were routinely repeated at different conductivities of the solvent. The relaxation frequencies f^* are reported as a function of the solvent conductivity and, as expected from equation (3), they form a straight line (Figure 5). The average cell radius was estimated on a statistically significant number of cells and the dielectric parameters C and G were calculated (Table 2). While the C value is in good agreement with literature data, a discrepancy in the G value is monitored [47] [48] . This difference is attributable to the fact that fibroblasts are measured in conditions of high viability and proliferation: this may cause a higher intra-membrane ion transport. The results on cells treated with MEX are summarized in Table 2. It is evident that the treatment causes a significant increase of both parameters C and G. The increased C value denotes a higher polarizability of the membrane, while the effect on G strongly suggests highly enhanced ion permeability as compared to untreated cells. It should be also pointed out that cells exposed to MEX show a decrease of the radius size. One can speculate that this is principally due to the interaction of the oily moiety of MEX and the fatty component of the membrane: this could promote an overall re-arrangement of the plasma membrane. The alterations of C and G are directly related to this structural modification. Interestingly, these data recall previous results obtained in our laboratory by a different dielectric spectroscopic technique on viral infected and serum deprived cells [49] [50] . The higher polarizability and the enhanced ion permeability are suggestive of an increased membrane fluidity which may end in its damage [51] [52] .

A development of this study is represented by the investigation of the effects at membrane level deriving from the infection with murine polyomavirus (Py). The results are discussed in this following section.

5.2. Virus infection and membrane integrity

Murine polyomavirus is an extremely well-characterized model system used to investigate a variety of biologi-

Figure 5. Relaxation frequency (f^*) as a function of the solvent conductivity (σ_e). The straight lines result from the best fit according to equation (3) in the text. Control cells (lower line); MEX treated cells (upper line). The different slopes and intercepts evidence the effect of the treatment with MEX.

Table 2. Specific capacitance C and specific conductance G and radius R for control (line A) and MEX-treated samples (line B). These values are averaged on 20 different cells. The final concentration of MEX was 5 mg/ml.

cal phenomena: its genome is formed by a small double-stranded circular DNA molecule. Py relies completely on the metabolic machinery of the infected cell. The “classical” book edited by Tooze [53] possibly still represents the most complete work on DNA tumor viruses. In our laboratory, Py has also been used to test the cytotoxic and/or antiviral potential of substances of natural origin [46] [54] [55] .

A particular aspect of the productive infection is represented by the virion entry into the cell and by its interaction with the plasma membrane. Information on possible membrane damage consequent to virus penetration is not very abundant, even though reports have been published on the mode and effects of the viral proliferation on the plasma membrane [49] [56] -[58] . The results of electro rotation measurements performed on infected cells show that the viral proliferation induces a relevant increase of both membrane parameters C and G. Not surprisingly, this phenomenon is more evident at prolonged times post-infection (Table 3). However if the progression of the infection is reduced in the presence of MEX (Figure 6), which is a specific inhibitor of Py proliferation, the membrane parameters are not altered at the same extent (Table 4). An important observation is that the infection with Py increases significantly the parameter G; this indicates an augmentation of the intra-membrane ion transport which reflects an enhanced cell metabolism in response to the viral attack. This idea is also supported by the strong mitogenic action of the virus [53] . In experiments carried out in the presence of MEX, the C value returns to normal levels and also a very strong reduction of the effect on G is monitored. The overall explanation is clearly correlated with the inhibiting action of MEX on the progression of the viral infection.

The data discussed so far show that under a phenomenological point of view both the effect of MEX and the viral infection produce similar modification of the membrane dielectric parameters. Therefore, it becomes very

Table 3. Specific capacitance C and specific conductance G at different infection times with murine polyomavirus.

Table 4. Specific capacitance C and specific conductance G at different times of viral infection in the presence of MEX. The data at 72 hours are omitted since after this time of infection MEX is too toxic to provide reliable data.

Figure 6. Yield of progeny viral DNA in the control and MEX treated cells. Lane A: Electro- pherogram obtained from mock-infected control cells; Lane B: Progeny viral DNA yield; Lane C: Progeny viral DNA yield obtained in the presence of MEX. Viral DNA is indicated, when present, by the lower arrow. The higher arrow indicates contaminating cellular chromosomal DNA.

interesting to analyze the behavior a further natural substance: Resveratrol (RV), endowed with multiple biological actions.

5.3. Influence of Resveratrol on the Cell Membrane

Resveratrol is a poly-phenol non flavonoid compound belonging to the family of natural phytoalexins. This molecule is very abundant in red grapes (Vitis vinifera) and in highly pigmented vegetables and fruit such as pumpkin (Curcuma longa) or black mulberry (Morus nigra). The drug shows a great number of diverse biological activities behaving as anti-tumor, antioxidant, phyto-estrogen and antiviral. Its high antioxidant character has been demonstrated in several different situations. The antiviral action of RV has also been demonstrated in several pathological conditions [59] -[69] . The exposure to RV at low dosage does not show a significant cytotoxic effect. At higher doses, on the contrary, it is cytotoxic, possibly due to the fact that this drug is known to induce cell cycle arrest. Moreover, the mitochondrial pathway is activated and this eventually leads to apoptosis [70] [71] . An analogous action has been described for another potent antioxidant: curcumin, which is able to induce apoptosis in human cervical cancer cells [72] . Recent data from our laboratory demonstrate that the drug is promptly assumed by the cell, as shown by the propidium iodide uptake kinetics [31] [73] . We analyzed the action of RV by electro rotation to investigate putative effects on the cell membrane structure/function. The results of these measurements are reported in Table 5. Parallel cytofluorimetric experiments (Figure 7) show the presence of a small sub-population of necrotic cells. It should be kept in mind that these cells do not rotate and therefore are not “visible” by ER: hence they do not give any contribution to the C and G values. We also monitored a small fraction of apoptotic cells. Apoptotic cells do rotate up to a certain stage of the process [13] . However, their number is so small that the contribution to the ER data becomes irrelevant. It is evident (Table 5) that the effect on the two membrane parameters is quite different. After 24 hours of treatment no variation is monitored; while after 48 hours a very small effect on C is observed and, mainly, an evident and large increase of G occurs. Since C is strongly associated to the structure and morphology of the membrane one can conclude that no significant alterations occur. The enhancement of G implies, on the other hand, a dramatic increase of ion

Figure 7. Evaluation of apoptosis inducted by RV. Cell surface annexin V binding was stu- died by flow-cytometry at two different treatment times. At both times of treatment floating and adherent cells were collected and labeled with annexin V-FITC-conjugated. RV concen- tration, treatment times and percentage of apoptotic and necrotic cells are indicated. The re- ported values represent the mean of three independent experiments. The smaller panel indi- cates a schematic and typical cell distribution. Squares 1: Viable cells; 2: Necrotic cells; 3: Cells in advanced apoptosis; 4: Cells in early apoptosis.

Table 5. Specific capacitance C and specific conductance G for untreated 3T6 control and resveratrol treated cells.

transport across the membrane; therefore, the treatment with RV is seemingly associated to an enhanced cell metabolism as observed by other strategies in wholly diverse cell models [see for instance 73].

Electrorotation permits also the evaluation of the consequences at membrane level of supra-molecular aggregates such liposomes and vesicles potential tool for the delivery of “cargo” molecules. This is the topic discussed in the next section.

5.4. Liposome and cell membrane interactions

Liposomes are good tools for the delivery of drugs and biomacromolecules [74] . They present many advantages such as biocompatibility, ease of preparation, and high payload capacity. They have been also used as an alternative transfection means to viral vectors. Cationic liposome formulations were shown to be very promising carriers [75] . Liposomes have been shown to feature intrinsic tissue selectivity [76] -[78] . A key step for the biological effectiveness of a liposome formulation is represented by the pathway of intracellular internalization and consequent possible damages at membrane level. The internalization pathway is strongly influenced by diverse parameters, such as: size, shape, rigidity, charge, hydrophobic/hydrophilic balance, presence of specific ligands [79] -[81] . The initial interaction of cationic liposomes with the plasma membrane is of electrostatic nature; however, the general mechanisms of internalization and intracellular trafficking yet remain to be fully clarified. Two main questions of this interaction are represented: first by the adsorption onto the cell surface, followed by the a possible liposome fusion with the membrane. The second question is represented by the internalization into the cell. In addition to electrorotation [3] , we also used different experimental approaches to address these issues, i.e. atomic force microscopy (AFM), ξ potential, and laser scanning confocal microscopy (LSCM) as well as biomolecular/cellular techniques [32] . The results of the electrorotation measurements are visualized in Figure 8 which reports the linear trend of relaxation frequency for controls and liposome treated cells. Evident variations of the angular coefficient and intercept, reflecting a decrease of the membrane parameters C and G, can be observed unlike what was monitored in the formerly discussed experimental data. Obviously, these differences depend upon the type of interaction and the nature of the exogenous material to which the cell is exposed.

Figure 8. Relaxation frequency (f^*) as a function of the solvent conductivity (σ_e). The full circles refer to untreated control cells. Empty circles report the relaxation frequency of cells treated for 1 hour with DMPC-G liposomes. The straight lines were obtained from each relaxation frequency at the respective ion strength fitted according to equation (3).

The percent variations of the membrane parameters and the average cell radius are reported in Table 6. It is worth noting that the cell radius changes significantly as a consequence of the cell/liposome interaction. The decrease of the specific capacitance C may be attributed to different and non-mutually exclusive reasons: thickness and/or decrease of the membrane permittivity ε’ due to an overall misalignment of the polypeptide moiety; this misalignment implies a variation of the ion transport mechanisms. The increase of cell radius may simply derive from the intracellular liposome uptake; for an extensive discussion of this phenomenon see [3] .

The biophysical schematic representation of a cell is usually a sphere surrounded by a thin homogeneous shell, mimicking the plasma membrane [82] [83] . The outer structure of the cell membrane, however, is very different from an ideal smooth sphere. To this end one can adopt a form factor in the expression of the specific capacitance of a spherical condenser [as discussed in detail in the classical treatment reported in reference 10]. In any case, observations conducted by AFM corroborate the data that, interaction with liposomes brings about an overall smoothening of the effective cell surface [32] . Despite the apparent alterations of the membrane parameters discussed above, no evident effect on the overall cell viability is monitored [3] .

Electrorotation measurements conducted in the presence of endocytosis inhibitors such as bafilomycin A1 (inhibitor of the vacuolar proton pump) and chlorpromazine (that disrupts clathrin-dependent endocytotic mechanisms) give evidence that liposomes pass through the membrane and are not incorporated into the bi-layer [84] -[86] . In fact, in the presence of the inhibitors the variations of the membrane parameters and the cell radius R are drastically reduced (Table 7). Exposure to the sole endocytosis inhibitors, on the other hand, does not cause changes in the dielectric and geometric parameters of the cell membrane (Table 7, line C). In addition, measurements of ζ-potential are coherent with the data discussed above [32] . In fact, upon incubation with different concentrations of DMPC-G, the ζ-potential of the cells does not vary. These rules out that liposomes fuse with the plasma membrane. However the conclusive result about the intracellular location of the liposome is evidenced by LSCM of fluorescently labeled particle (Figure 9). Data clearly demonstrate that DMPC-Gs pene-

Figure 9. Z-stack confocal image of cells exposed to rhodamine-labeled liposomes. The image shows a single XY slice with two partially overlapping cells. The contour of the cell mem- brane (M) and of the nucleus (N) is symbolically indicated. It is evident that liposomes are confined to the cytoplasm area (C).

Table 6. The percent variations of the membrane parameters C and G and the average cell radius R, for the samples treated for 1 (A) or 4 (B) hours with DMPC-G. The average radius estimated on untreated control cells was 8.5 ± 0.3 μ.

Table 7. The percent variations of the membrane parameters C and G and the average cell radius R. (A) Interaction with DMPC-G. (B) Interaction with DMPC-G in presence of endocytosis inhibitors. (C) Effect of endocytosis inhibitors per se.

trate the plasma membrane and are located only within the cytoplasm.

6. Conclusive Remarks

This review article is mainly focused on the great potentials and flexibility of electro rotation. Trypsinization, necessary to detach the cells from the substrate, might actually influence the native membrane parameters. However this is of no consequence regarding the final significance of the measurements since both control and treated cells undergo the same experimental manipulation. Therefore, the final result of the experiment evidences the relative differences between the control and the treated cells. In any case the results are obtained from fully vital cells since non-viable cells do not rotate as discussed in detail. Data obtained by this strategy are summarized but in particular the results of our laboratory are discussed in greater detail. In any case, this review underlines how the synergy between this technique and other imaging and bio-molecular strategies can produce effective and stimulating results. Furthermore, the conclusive consideration is that the multidisciplinary efforts of biochemical-physicists and molecular-cellular biologists can pave the way to fruitful and innovative approaches in the field of life sciences.

NOTES

^*Corresponding author.

Conflicts of Interest

The authors declare no conflicts of interest.

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