Original Research ARTICLE
Supported Lipid Bilayers of Escherichia coli Extracted Lipids and Their Calcium Dependence
- Department of Environmental and Life Sciences, Toyohashi University of Technology, Toyohashi, Japan
Formation of supported lipid bilayer (SLB) and additional structures of Escherichia coli (E. coli) lipids were investigated with fluorescence microscopy and atomic force microscopy. Ca2+ in the aqueous phase with concentration above 2 mM was necessary for the formation of SLB. Additional lipid structures, string-like structures, the second lipid bilayer, and multilayer stacking appeared on the first layer SLB depending on Ca2+ concentration. The bridging effect of Ca2+ between the negatively charged E. coli lipid bilayers and substrate is the dominant factor determining the two-dimensional and three-dimensional morphology of the E. coli lipid bilayer membranes.
Two- and three-dimensional organization of lipid bilayer structures are essential processes in signal and material transportations through cell membranes (Kim, 2006; Rutter, 2006; Rothman, 2014). Artificial lipid membrane is widely used for studying cell membrane property, drug development, and biosensor (Hirano-Iwata et al., 2008). Supported lipid bilayers (SLBs) are a kind of artificial lipid membranes situated at solid-liquid interface (Tamm and McConnell, 1985; Castellana and Cremer, 2006; Tero, 2012; van Weerd et al., 2015). They are used to investigate the fundamental physicochemical properties and molecular distribution of lipid bilayers with atomic force microscopy (AFM) and fluorescence-microscope-based methods (El Kirat et al., 2010; Tero, 2012; Zhong and He, 2012). Morphology and physicochemical properties of lipid domains, and shape transformation of membranes have been studied in multicomponent SLBs (El Kirat et al., 2010; Goertz et al., 2011; Zhong and He, 2012; Kawakami et al., 2017; Sumitomo and Oshima, 2017; Tero et al., 2017; Kakimoto et al., 2018).
As a bacterial model cell system, reconstituted Escherichia coli (E. coli) cell membrane has been studied (Dodd et al., 2008; Merz et al., 2008; Lopes et al., 2010; Unsay et al., 2013; Lind et al., 2015; Phan and Shin, 2015; Hsia et al., 2016; Konarzewska et al., 2017; Márquez and Vélez, 2017). Understanding the bacterial membrane system helps in revealing the mechanism of molecular recognition and material transportation during bacterial infection for medical technology. The E. coli lipid extract contains three main phospholipids, phosphatidylethanolamine (PE), phosphatidylglycerol (PG), and cardiolipin (CA). Neutral PE is most abundant in the E. coli cell membranes, and anionic PG and CA make the membrane net negatively charged (Shokri and Larsson, 2004; Romantsov et al., 2007; Gidden et al., 2009; Sohlenkamp and Geiger, 2015; Lin and Weibel, 2016). In addition, CA exists in the high curvature region of membrane and plays a key role in antimicrobial peptide interaction (Khalifat et al., 2008; Lewis and McElhaney, 2009; Mileykovskaya and Dowhan, 2009; Schlame and Ren, 2009; Lopes et al., 2010; Unsay et al., 2013; Phan and Shin, 2015).
There are several previous studies on the formation of SLBs containing E. coli lipids such as polar lipid extract (PLE) or total lipid extract (TLE) (Dodd et al., 2008; Merz et al., 2008; Lopes et al., 2010; Unsay et al., 2013; Lind et al., 2015; Hsia et al., 2016; Konarzewska et al., 2017; Márquez and Vélez, 2017). Solid substrates, which are generally used for SLB formation, e.g., glass, oxidized layer on a Si wafer, and mica, are negatively charged. Because of the electrostatic repulsion between negatively charged E. coli lipids and the substrates, divalent cation such as Ca2+ is necessary to form SLB (Merz et al., 2008; Lind et al., 2015; Márquez and Vélez, 2017). Previous QCM and fluorescence microscope studies showed that ~2 mM Ca2+ is sufficient for the formation of E. coli lipid SLB (Merz et al., 2008; Lind et al., 2015; Márquez and Vélez, 2017). Divalent cations bridge negatively charged substances by effectively shielding electrostatic interaction (Rajendran et al., 2011; Ido et al., 2013), and also positively affect the SLB formation from lipid vesicles (Hansma and Laney, 1996; Rivetti et al., 1996; Reviakine and Brisson, 2000; Pastré et al., 2003; Seantier and Kasemo, 2009). Ca2+ also induces microstructure of lipid bilayers containing negatively charged lipids. For example, phase separation and membrane fusion of lipid bilayers containing phosphatidylserine is caused by Ca2+ (Silvius and Gagne, 1984a,b). In this study, we investigated microscopic two-dimensional and three-dimensional organization of lipid membranes comprising of PLE and their dependence on Ca2+ concentration ([Ca2+]) with fluorescence microscopy and AFM.
Materials and Methods
PLE [PE: PG: CA = 67: 23.2: 9.8 (wt/wt)] and lissamine rhodamine B-dipalmitoylphosphatidylethanolamine (Rb-DPPE, Ex/Em: 560/583 nm) were purchased from Avanti Polar Lipids, Inc., (Alabaster, AL, USA), and used without purification. The lipid ratio among PE, PG and CA corresponds to that in E. coli (Merz et al., 2008; Lopes et al., 2010; Lind et al., 2015). Chloroform solutions of PLE and Rb-DPPE were mixed in a glass vial. The solution was dried with a nitrogen gas stream followed by overnight evacuation. A buffer solution (120 mM KCl and 10 mM HEPES/KOH: pH 7.2) was added to the vacuum-dried lipid mixture film. A lipid vesicle suspension was then prepared by vortex at 45°C, freeze-thawing through five cycles, and extruding through 800 and 100 nm polycarbonate filters. SLB was prepared by the vesicle fusion method on a thermally oxidized SiO2/Si substrate precleaned by boiling in piranha solution (3:1 v/v mixture of conc. H2SO4 and 30% H2O2 aqueous solution). Caution: Piranha solution violently reacts with organic materials, and extreme care must be taken at all times during handling.
We mixed the extruded vesicle suspension and a Ca2+-containing buffer solution (10 mM CaCl2, 120 mM KCl, 10 mM HEPES/KOH: pH 7.2), and incubated the SiO2/Si substrate under [Ca2+] = 0–8 mM, at 45°C for 90 min. After the incubation, the excess vesicles in the liquid phase were washed out by serial exchanges of the vesicle suspension with buffer solution.
An epi-fluorescence microscope (epi-FM) (BX51WI, Olympus, Tokyo, Japan) was used for wide-field fluorescence and qualitative fluorescence recovery after photobleaching (FRAP) observations. AFM observation was performed using the PicoPlus 5500 (Keysight Technologies, Inc., Santa Rosa, CA, USA, formerly Molecular Imaging, Corp.) in the acoustic AC (tapping) mode in the buffer solution. A cantilever with a spring constant of 0.09 N/m (resonant frequency: 110 kHz; BL-AC40TS-C2, Olympus) was used. Topography, phase-shift image, and amplitude image were obtained simultaneously.
Results and Discussion
Figure 1 shows fluorescence images of the SiO2/Si substrates after incubated in the PLE-vesicle suspensions with 0, 2.0, 2.5, 3.0, and 5.0 mM Ca2+. With [Ca2+] = 0 mM (Figure 1A), almost no fluorescence intensity was obtained except for a few bright spots, which were adsorbed vesicles. When the substrate was incubated in the PLE-suspension with [Ca2+] = 2 mM, a circular region with a uniform fluorescence intensity existed (Figure 1B). The fluorescence intensity shows that single layer of SLB was formed in this region (Tero et al., 2017; Kakimoto et al., 2018). The surrounding gray region contained bright dots that had similar fluorescence intensity to the circular SLB region (Figure 1B, inset). They are assigned to small SLB patches. Coverage of the larger SLB region and the surrounding SLB did not change at longer incubation time.
Figure 1. Fluorescence images of SiO2/Si substrates after incubated in the PLE-vesicle suspensions with [Ca2+] = (A) 0, (B) 2.0, (C,D) 2.5, (E) 3.0, and (F) 5.0 mM. (B,E) Insert: magnified image of the dotted square region. Representative SLB patch is indicated with a white arrow in (B). The string-like structure and the region two times brighter than the surrounding are indicated with a white arrow and a black arrow in (E), respectively. Scale bars are 50 μm.
The surface morphology became heterogeneous with [Ca2+] = 2.5 mM: a circular SLB and smaller SLB patches similar to Figure 1B existed (Figure 1C), and additional brighter objects were also observed in the SLB region with a uniform fluorescence intensity (Figure 1D). The latter region covered almost the whole substrate surface with [Ca2+] = 3.0 mM (Figure 1E). There were two types of bright objects on SLB (Figure 1E, inset). One was string-like structures (indicated by a white arrow in Figure 1E). The other was brighter regions (indicated by a black arrow in Figure 1E) that had two times higher intensity than the surrounding, and had a plateau-like intensity profile. We assigned them to the second lipid bilayer stacking on the first SLB, based on the fluorescence intensity (Nabika et al., 2006; Tero et al., 2008). These structures disappeared with [Ca2+] = 5.0 mM, and much brighter objects were observed in a uniform fluorescence intensity (Figure 1F). They had at least four times higher fluorescence intensity than the surrounding that had similar intensity with the SLB region in Figure 1E. Similar fluorescence images to Figure 1F were obtained with higher [Ca2+] up to 8 mM (data not shown).
Figure 2 shows the FRAP process of PLE-SLBs with [Ca2+] = 2.0, 3.0, and 5.0 mM. FRAP is a fluorescence-microscope-based technique to measure lateral molecular diffusion in a lipid bilayer (Axelrod et al., 1976; Soumpasis, 1983). Fluorescent probes at a part of a sample are bleached with strong excitation light, and then the fluorescence intensity recovers if the probes diffuse. We investigated the fluidity and continuity of the SLB and the brighter objects observed in the fluorescence images in Figure 1. The fluorescence intensity of the small SLB patches with [Ca2+] = 2.0 mM (the gray region in Figure 1B) partially recovered at the peripheral of the bleached region (Figure 2A), but did not recovered in the majority of the bleached region. The result indicates that the SLB patches did not link each other. In the region with uniform fluorescence intensity (the circular bright region in Figure 1B), fluorescence intensity completely recovered. The fluorescence intensity recovered over time in PLE-SLB with [Ca2+] = 3.0 (Figure 2B). These results show that fluid and continuous SLB was formed in the region with uniform intensity. The fluorescence of the brighter objects, the string-like structure and the second layer of the bilayer membrane (Figure 1E), also recovered completely (Figure 2B). It indicates that these objects are linked with the SLB under them, and lipid molecules diffuse between them. In the PLE-SLB with [Ca2+] = 5.0 mM, FRAP proceeded both in SLB and the bright objects (Figure 2C).
Figure 2. Fluorescence recovery after photobleaching (FRAP) processes of PLE-SLBs with [Ca2+] = (A) 2.0 mM, (B) 3.0 mM, and (C) 5.0 mM. Scale bars are 50 μm.
Figure 3 shows AFM topographies and cross-section profiles obtained at various positions of PLE-SLB with [Ca2+] = 2.5 mM. As shown in Figures 1B,C, the sample with [Ca2+] = 2.5 mM contained all kinds of structures, the SLB patches, uniform SLB, the string-like structure and the second layer on SLB, which were observed in the fluorescence images of 2 mM and 3 mM Ca2+. Three types of structures were obtained with AFM observation: plateaus 4–5 nm in height and ~10–1,000 nm in width (Figure 3A); flat and uniform region (Figure 3B); network-like protrusions 2–3 nm in height (Figure 3C). The network-like protrusions were fragile, and disappeared after the same area was scanned repeatedly.
Figure 3. AFM topographies and cross-section profiles of PLE-SLB with [Ca2+] = 2.5 mM obtained at different positions, [(A) 2.0 μm × 2.0 μm, (B) 3.0 μm × 3.0 μm, (C) 2.0 μm × 2.0 μm] and the cross-section profile at the white line in each AFM topography.
The height of the plateaus in Figure 3A corresponds to the thickness of a single lipid bilayer membrane in AFM topographies (Tero, 2012). Therefore we attribute the plateaus to the SLB patches observed in Figures 1B–D, 2A. The SLB patches of the order of 1 μm in width were recognized in the fluorescence images (Figure 1). FRAP proceeded partially (Figure 2A), as some of these patches linked each other (Figure 3A). The AFM topography in Figure 3A shows that small SLB patches 10-100 nm in width existed, although they were not recognized in the optical images (Figure 1).
The flat region in Figure 3B corresponds to a continuous SLB in Figures 2B,C. The AFM topography shows that the SLB was defect-free on the order of micrometer in wide, and surface roughness was ~ 1 nm. We attribute the network-like protrusions in Figure 3C to the string-like structure in the fluorescence image in Figure 1C. We hypothesize that they are tubular bilayers or wrinkles in a SLB, but could not achieve detailed observation because they were easily decomposed by AFM scanning. In the AFM topographies, we did not find objects corresponding to the double bilayer region, which was two times brighter than the surrounding SLB in the fluorescence image (Figure 1E). It is because that the area fraction of the second bilayer is small (2.5% in Figure 1E). The AFM scanning area (2–3 μm) was smaller than the width of the second bilayer (~10 μm). Single or double bilayer is not recognized with AFM if they are similarly flat, unless the edge of the second bilayer is captured in the AFM scanning area.
Formation and morphology of the PLE-SLB significantly depended on [Ca2+]. PLE-bilayer is negatively charged at neutral pH because of PG and CA. In this study, PLE vesicles transformed to SLB and other structures on the SLB. SLB formation from vesicles proceeded through the processes of vesicle adsorption, fusion, rupture and spreading. With [Ca2+] = 0 mM, few lipid components existed on the SiO2/Si substrate (Figure 1A), which is negatively charged because of the dissociation of surface silanol group (Si-OH) (Ahmed, 1966; Tero, 2012). Electrostatic repulsion between the PLE vesicle and the substrate suppressed the vesicle adsorption process.
Divalent cations shield the electrostatic interaction more effectively than monovalent cations, and also bridge electronegative substances, e.g., DNA and a mica substrate (Rajendran et al., 2011; Ido et al., 2013). Addition of Ca2+ promoted the vesicle adsorption and SLB formation on the SiO2/Si substrate (Figure 1B). The result is consistent with previous studies, which showed at least ~2 mM of Ca2+ is necessary for the formation of PLE-SLB on SiO2/Si, mica, TiO2, indium tin oxide and gold (Dodd et al., 2008; Merz et al., 2008; Lopes et al., 2010; Unsay et al., 2013; Lind et al., 2015; Hsia et al., 2016; Konarzewska et al., 2017; Márquez and Vélez, 2017). In the previous studies of the bacterial mimic lipid bilayer, however, averaged response from the sample was mainly obtained using QCM and fluorescence microscopy (Dodd et al., 2008; Merz et al., 2008; Lopes et al., 2010; Unsay et al., 2013; Lind et al., 2015; Phan and Shin, 2015; Hsia et al., 2016; Konarzewska et al., 2017; Márquez and Vélez, 2017). The results in this study showed the heterogeneity of SLB especially at the threshold [Ca2+] around 2.5 mM. Density of adsorbed Ca2+ on substrates depends on [Ca2+] in the bulk solution. Fluorescence images in Figure 1 shows that Ca2+ of 2–2.5 mM induced formation of the negatively charged PLE-SLB, but was not enough for the formation of full-coverage SLB. Under the bulk concentration of [Ca2+] = 3 mM, sufficient amount of Ca2+ existed between the PLE-SLB and the substrate for bridging them in the whole substrate surface.
Generally only a single layer of lipid bilayer membrane is formed in the SLB formation from small unilamellar vesicles (Tero, 2012), unless a specific attraction is introduced between the first and second layer (Murray et al., 2009; Han et al., 2010). In this study, inter-lipid-bilayer bridging was caused by Ca2+ more than 2 mM, as well as the substrate-lipid-bilayer bridging, and thus additional PLE-derived structures appeared on the first layer PLE-SLB. More PLE existed with higher [Ca2+] (Figures 1D–F), and their structures depended on [Ca2+]. At [Ca2+] = 3 mM, the string-like structure and the second bilayer patch bound to the first layer PLE-SLB, and they were isolated from each other. At [Ca2+] = 5–8 mM, on the other hand, attraction between the additional lipid membranes became dominant, and multi-layer stacking or segregation of PLE bilayers occurred. They kept the lipid bilayer structure, and also physically connected to the first layer PLE-SLB, because fluorescence intensity recovered in the FRAP experiment (Figure 2C).
Figure 4 shows time course of fluorescence images of PLE-SLBs with [Ca2+] = 3 mM, observed just after the PLE-SLBs were prepared. The amount of the string-like structure on the uniform lipid bilayer decreased with time (Figure 4A). The area of the second bilayer also decreased with time, leaving the string-like structures (Figure 4B). These images provide information about the formation process of these additional structures on the first layer PLE-SLB. The second layer remained on the first layer because of the Ca2+-bridging effect, at the process of the spreading during the transformation from vesicles to a planar membrane. Some of the second layers desorbed remaining the string-like structure, which further converted to a uniform SLB. These structural conversions stopped when their adsorption amounts reached at the equilibrium of Ca2+-bridging effect depending on [Ca2+]. Therefore the brighter objects existed stably in Figures 2B,C.
Figure 4. Sequential fluorescence images of PLE-SLBs with [Ca2+] = 3.0 mM focusing to (A) the string-like structure and (B) the second bilayer two times brighter than the surrounding. The images of (A,B) were obtained from two samples independently. Scale bars are 10 μm.
Intracellular [Ca2+] in E. coli is approximately 0.1 μM (Gangola and Rosen, 1987). E. coli exists, however, in intestine of warm blood animal. Its extracellular fluid is kept at [Ca2+] in the order of mM (Berridge et al., 2000, 2003). Additionally, cell membrane surfaces are negatively charged. From the point of view of biotechnology, generally transformation of E. coli with plasmid DNA is conducted in a solution of [Ca2+] ≥10 mM (Mandel and Higa, 1970; Hanahan, 1983). Ca2+ facilitates insertion of plasmid DNA by suppressing electrostatic repulsion between membrane and DNA, and then bringing membrane pore formation. Figure 1F showed tendency that a PLE bilayers to take multilamellar stacking and aggregate states, rather than a planar single bilayer membrane, at [Ca2+] ≥5 mM. The results in this study revealed that the Ca2+ induced the adsorption of PLE bilayer on a negatively charged surface, and also caused structural conversions of the PLE bilayer depending on [Ca2+]. They will provide information for understanding fundamental processes of infection and transfection of E. coli.
In conclusion, we investigated the morphology and physical properties of PLE-SLBs in various [Ca2+] with fluorescence microscopy and AFM. Ca2+ facilitated vesicle adsorption and subsequent SLB formation on a negatively charged SiO2/Si substrate. Morphologies of the first layer SLB and additional structures on it were strongly affected by [Ca2+]. Electrostatic bridging effect of Ca2+ is the dominant factor of these phenomena. Understanding two-dimensional and three-dimensional inter-membrane structures is valuable to construct model bacterial membranes using SLB systems, and to reveal fundamental processes of bacterial membrane reactions in the field of biotechnology and medicine.
YK carried out the experiments, and analyzed the data. YK and RT designed the experiment and wrote the paper.
This work was supported by JSPS KAKENHI Grant Numbers JP15H03768 and JP15H00893, JST-CREST Grant Number JPMJCR14F3, and JST-A-STEP.
Conflict of Interest Statement
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Electronics-Inspired Interdisciplinary Research Institute (EIIRIS) Project, Toyohashi University of Technology, and Nation-wide Cooperative Research Projects, Research Institute of Electrical Communication, Tohoku University are acknowledged.
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Keywords: supported lipid bilayer, E. coli lipid, lipid organization, atomic force microscopy, fluorescence microscopy, fluorescence recovery after photobleaching
Citation: Kakimoto Y and Tero R (2018) Supported Lipid Bilayers of Escherichia coli Extracted Lipids and Their Calcium Dependence. Front. Mater. 5:48. doi: 10.3389/fmats.2018.00048
Received: 31 May 2018; Accepted: 31 July 2018;
Published: 21 August 2018.
Edited by:Nam-Joon Cho, Nanyang Technological University, Singapore
Reviewed by:M. Gabriella Santonicola, Sapienza Università di Roma, Italy
Jun-ichi Hotta, Yamagata University, Japan
Copyright © 2018 Kakimoto and Tero. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Ryugo Tero, email@example.com