Adherent cells avoid polarization gradients on periodically poled LiTaO3 ferroelectrics
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The response of fibroblast cells to periodically poled LiTaO3 ferroelectric crystals has been studied. While fibroblast cells do not show morphological differences on the two polarization directions, they show a tendency to avoid the field gradients that occur between polarization domains of the ferroelectric. The response to the field gradients is fully established after one hour, a time at which fibroblasts form their first focal contacts. If suspension cells, with a lower tendency to establish strong surface contacts are used, no influence of the field gradients is observed.
KeywordsFibroblast Cell adhesion Ferroelectrics Permanent dipole Polarization
When a particle, cell or microorganism approaches a surface, electrostatic interactions are among the first forces encountered [1, 2]. Especially for motile microorganisms, surface charge affects adhesion and extended Derjaguin, Landau, Verwey, Overbeek (DLVO) theory, in conjunction with electrostatic interactions, are used to describe observed experimental trends [1, 3]–. A series of studies by the Whitesides group show that an overall electrically neutral surface seems to be a prerequisite for an inert surface [7, 8]. Electrostatic interactions may still be involved even for formally neutral surfaces, such as self assembled monolayers (SAM) of ethylene glycol, as theory suggests that hydroxyl ions can accumulate on top of the SAM and thus form a negatively charged interface . Studies of electrostatic interactions between microorganisms or cells with surfaces in many cases rely on the presence of charged groups and differently charged surfaces are a result of a changed chemistry and it is desirable to experimentally access the impact and relevance of electrostatic contributions on adhesion phenomena. To restrict interaction studies to electrostatic contributions requires surfaces with constant surface energy and identical surface chemistry. Electrets with embedded charges in polytetrafluoroethylene are one option and recently used to correlate the polarity of the electret with the favorability of this substrate to be colonized by spores of the green algae Ulva linza. Another class of surfaces capable retaining a stable oxide surface but permit local alterations polarization are periodically poled inorganic ferroelectric materials. One of the characteristic features of the ferroelectrics is the presence of electrically reversible polarization. In a properly oriented ferroelectric sample, for example (001)-cut LiNbO3 crystal or (001)-grown BaTiO3 thin film, the polarization can be aligned perpendicular to the surface in the positive or negative direction. In this case, the abrupt change in the normal component of the spontaneous polarization on a ferroelectric surface results in the appearance of a bound polarization charge, which in ambient conditions is compensated by accumulation of ionic species or dipole molecules and through redistribution of mobile carriers in the bulk . This screening significantly affects the surface charge distribution and the surface potential and results in band bending . Similarly, charged surface states can pin the surface Fermi level resulting in a change in both the surface charge, the surface potential, and change the molecular band offsets . It has been shown recently that these electrically switchable properties of the ferroelectrics can be used to tailor surface reactivity. Several examples illustrating the effect of polarization on the photo-reduction rate of Ag+ ions, the sticking coefficients and interaction energies of alcohol and water molecules can be found in literature –, including the selective deposition of virus particles .
Regarding the effects of polarization on mammalian cells, several studies have shown that electrically active ceramics improve biological responses to artificial grafts in bones [21, 22]. It has been suggested that these effects are linked to the adaptation of bone in response to mechanical loading, since polarization effects have been observed in hydroxyapatite. However, the mechanism by which surface polarization affects cell response is yet to be elucidated and it still remains to be investigated if the preferential adsorption of proteins and ions plays a role. Another limitation is the use of different individual surfaces with a specific polarization state where subtle differences in adhesion behavior are difficult to assess. With the patterned material used in this study, a side-by-side comparison becomes possible and we can study if strong field gradients at boundaries between the polarized areas influence early cell adhesion - a key event regulating several biological responses. It is important to bear in mind that due to the high concentration of ions in cell culture medium, the Debye length is in the order of 1 nm. This means that only those parts of the cell that are very close to the surface will be in any way affected by the gradient fields. The unique approach of using periodically poled substrate domains allows the cells to select locations of different polarizations and field gradients without being significantly perturbed by chemical differences.
2.1 Preparation of single poled and periodically poled LiTaO3
2.2 Protein adsorption assay
Protein adsorption assays were carried out following established protocols . Alexa fluor 488 labeled fibrinogen was diluted in phosphate buffered solution (PBS) (both Invitrogen, Karlsruhe, Germany). Samples were immersed in 10 mL of filtered PBS for 1 min. Subsequently, 10 ml of 1 mg/mL fibrinogen solution was added and kept at room temperature for 30 min. Afterwards, the solution was continuously diluted with 500 mL deionized water and 500 mL Milli-Q water. The samples were dried and the protein layer was imaged by fluorescence microscopy using a Nikon TE-2000. The layer thickness was determined with X-ray photoelectron spectroscopy (XPS). The XPS device (Leybold-Heraeus MAX 200), equipped with a KαAl (1486.6 eV) anode measured the attenuation of Ta 4f signal from which the protein thickness was calculated.
2.3 Cell culture and adhesion
Cell adhesion on polarized LiTaO3 was evaluated in vitro using rat embryonic fibroblast cells expressing YFP-paxillin (REF52YFP, kindly provided by B. Geiger, Weizmann Institute, Israel). In previous studies, we showed that these cells form robust focal adhesions, which are paxillin-rich contacts mediated by integrins . The fibroblasts were cultured in a humidified incubator with 5% CO2 at 37°C. The initial culture medium used was Dulbecco’s modified Eagle medium (DMEM) supplemented with 10% fetal bovine serum, 1 mM L-glutamine, and 100 units/mL penicillin–streptomycin solution all purchased from Gibco (Invitrogen, Karlsruhe, Germany). The cells were harvested from tissue culture flasks by incubation with a 0.05% trypsin–EDTA solution for 5 min. Cells were then centrifuged and resuspended in complete media. Cells were seeded on the substrates at a density of 1 × 105 cells/mL.
Cell adhesion was also evaluated with the motile human leukemia cell line KG-1a. The KG-1a cells were cultured in RPMI-1640 medium supplemented with 10% fetal bovine serum, 1 mM L-glutamine, and 100 units/mL penicillin–streptomycin inside the same incubator. For adhesion experiments, KG-1a were directly taken from the culturing suspension and diluted with culture medium to 1 × 105 cells/mL.
2.3.3 Cell adhesion
Prior to adhesion experiments the substrates were cleaned by immersion in 3 mmol NaOH containing 10% p.a. ethanol. After a 30 min immersion in a sonication bath, samples were rinsed with ethanol and water. The substrates were affixed to the bottom of a custom-made petri dish where a hole of 5 mm in diameter was cut into the center of the dish. The adhesion and spreading of cells was followed by time-lapse video microscopy (Nikon TE-2000) inside a custom build incubation chamber under standard culture conditions (37° C, 5% CO2). Cells were imaged directly after seeding, at a time interval of 1 minute for the first two hours and then every 10 minutes up to 18 h of total incubation time with an automated microscope Nikon TE-2000. Time-lapse microscopy was carried out with a 10x Ph1 objective and static fluorescence imaging was performed with a 20x Ph1 objective (both Nikon, Tokyo, Japan). In the case of the fibroblast adhesion studies, several positions were observed simultaneously which was not possible for the weakly adherent leukemia cells because movement of the automated microscopy stage caused vibrations which caused immediate cell detachment. The fluorescence imaging of cell focal contacts was performed with a 20x phase contrast objective and a GFP/YFP filter.
2.3.4 Cell position analysis
Digital image analysis methods were applied to determine the preferential site for cells to adhere. Due to the unequal sizes of the two cell types and thus their relative size to the polarized domains of the substrate, the center of the nucleus was used as a measure of cell position on the substrate. The domains are visible in phase contrast microscopy as their optical properties change with polarization direction of the domains. The positions of cell nuclei were analyzed at different time points and related to the periodic pattern sequence A/B. The cell number along the periodicity was calculated by counting the number of cells within rectangular areas parallel to the stripes with a horizontal width of approximately 3.15 μm (5 px) across the full image. As the stripes had different widths, approximately 3.15 μm (5 px) relate to 1/7 of the width of the bright stripes (~35 px, 22 μm) and 1/8 of the dark stripes (~41 px, 25.8 μm).
3 Results and discussion
3.1 Protein adsorption on periodically poled LiTaO3
3.2 Cell adhesion on periodically poled LiTaO3
3.3 Cell response to polarization of periodically poled LiTaO3
Summarizing, adhesion and spreading of cells were investigated on poled and structured LiTaO3 surfaces and it was found that fibroblasts spread equally on homogeneously up (+) and down (-) poled substrates. Also, uniform spreading over up and down domain stripes was observed on periodically poled substrates. Random distribution of focal contacts over the domain stripes was confirmed by fluorescence microscopy of long term incubated YFP-paxillin REF52 fibroblasts. These results indicate that cell attachment and spreading were not affected by the polarization of the substrate. In contrast, analysis of the positions of the nuclei in the time lapse images revealed that during spreading fibroblasts preferably placed their nucleus in the middle of periodically poled domain stripes. This is the position on the surfaces where the lowest field gradients are present. In turn, the field gradient on the border of polarity domains is highest and these positions are less attractive. Kinetic analysis revealed that the positioning of the cell nucleus took place on the same timescale as the formation of cell focal contacts (30 min to 2 h). In the case of weakly adherent suspension cells KG-1a, the response was much weaker compared to fibroblasts. At present we can only speculate that the KG-1a response might be weaker due the larger distance of the nucleus to the surface for a suspension cell compared to an adherent fibroblast. Based on the short Debye length in the order of one nanometer, the weaker field strength could cause a weaker response. However, also the specific function of a particular cell type in the body might be connected with its ability to sense fields.
The fibrinogen adhesion data suggests that polarization-dependent surface chemistry can be excluded in the selective adhesion of these cells and the effects visible are due to the ferroelectric field present. Interestingly, isolated proteins , as some amino acids like cysteines , albeit in very low concentrations, have been seen to exhibit a preference for polar surfaces rather than domain walls. Adsorption from low concentration BSA solutions is higher on positively poled surfaces than on negatively poled ones . In comparison, our experimental conditions contained very high concentration of proteins and the sticky fibrinogen leads to a rapid formation of a proteinaceous overlayer that was found to be independent of the polarization. While the adsorption of molecules on polarized surfaces seems to be quite complex, the general notion that molecular interaction with the surfaces might depend on the fields present is supported by the observation that in the region of the ferroelectric domain boundaries the photo-reduction rate of AgNO3, HAuCl4, Pt(NO3)2 and other compunds is increased [23, 36]–. In addition it was found that nanowires of pure Ag, Au and Pt were grown along the predefined 1800 ferroelectric domain walls on c-cut congruent LiNbO3 and lead zirconate titanate [Pb(ZrxTi1-x)O3] single crystals. Thus, field gradients affect adsorption, chemical reactions, and crystal growth.
Less was so far known on interaction of cells with patterned, polarized substrates. Polarization-specific adhesion of cells does seem to occur under isothermal conditions and with minimal optical excitation, but cannot be attributed to the effect of pyroelectric or photoinduced charge . Our fibroblast adhesion experiments show that both, up and down poled domains, are equally preferred and the ferroelectric domain boundaries at which the strongest field gradients are present are avoided. However, no obvious morphological differences were seen in the middle of stripes of different polarization. This observation is in agreement with recent studies of Baxter et al. who found no long-term effect of polarization direction of non-structured hydroxyapatite-barium titanate ceramics on the morphology of adherent Saos-2 cells . In comparison to non-poled ones, Tarafder et al., however, observed fewer cell-cell attachments with the extension of filopodia on positively poled surfaces. These morphological differences went along with a delayed initial proliferation , irrespective of the sign of the surface charge. Research on osteoblast-like cells in some cases supports the preference of negatively charged surfaces , albeit in other cases contradicts this trend . To the best of our knowledge our study is the first on cell adhesion on microstructured, polarized surfaces and shows that the differences between surfaces with different polarization direction seems to be dominated by the strong influence of the high field gradients present at the domain boundaries. Especially the shift of the position of the nucleus of the cells is a so far an unknown observation. At present we can only speculate that electric signals that are connected with ion transport might be involved.
Summarizing, a detailed investigation on the adhesion of cells on structured, polarized ferroelectric samples was presented and we could for the first time show that cells actively reorient the position of their nucleus and avoid positions of high field gradients.
We acknowledge funding by the Sander Stiftung (Proposal 2010.079.1 and grant D10051281), the Biointerfaces programme of the Helmholtz society and by the National Science Foundation (NSF) through the Nebraska Materials Research Science and Engineering Center (NSF Grant No. 0820521).
- 4.Jucker BA, Harms H, Zehnder AJB: Adhesion of the positively charged bacterium Stenotrophomonas (Xanthomonas) maltophilia 70401 to glass and teflon. J Bacteriol 1996,178(18):5472–5479.Google Scholar
- 6.Van Loosdrecht MC, Lyklema J, Norde W, Schraa G, Zehnder AJ: The role of bacterial cell wall hydrophobicity in adhesion. Appl Environ Microbiol 1987,53(8):1893–1897.Google Scholar
- 10.Fridkin VM: Ferroelectric semiconductors. New York: Consultants Bureau; 1980:318.Google Scholar
- 22.Kobayashi T, McMahon AP, Kronenberg HM: Targeted expression of constitutively active BMP receptor 1A in chondrocytes causes lethal skeletal dysplasia with shortening of growth plate. J Bone Miner Res 2001, 16:S142-S142.Google Scholar
- 24.Zhang ZZ, Sharma P, Borca CN, Dowben PA, Gruverman A: Polarization-specific adsorption of organic molecules on ferroelectric LiNbO3 surfaces. Applied Physics Letter 2010,97(24):243702/1–247302/3.Google Scholar
- 33.Christophis C: Quantification of cell adhesion strength on artificial surfaces with a microfluidic shear force device. Doctor of natural sciences PhD. Heidelberg: Ruperto Carola University Heidelberg; 2011.Google Scholar
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