Adhesion and Structural Changes of PEGylated Lipid Nanocarriers on Silica Surfaces

: PEGylated lipid nanoparticles have a continuously expanding range of applications, particularly within pharmaceutical areas. Hereby, it is shown with the help of the Quartz Crystal Microbalance with Dissipation monitoring (QCM-D) and other surface sensitive techniques that, at room temperature, PEGylated liposomes and lipodisks adhere strongly to silica surfaces resulting in the displacement of the hydration layer of silica and the formation of immobilized nanoparticle ﬁlms. Furthermore, it is shown that drastic changes in the structure of the immobilized ﬁlms occur if the temperature is increased to >35 ◦ C. Thus, intact immobilized PEGylated liposomes rupture and spread, even in the gel phase state; immobilized lipodisks undergo complete separation of their components (bilayer forming lipids and PEGylated lipids) resulting in a monolayer of adsorbed PEGylated lipids; and PEGylated supported lipid bilayers release part of the water trapped between the lipid membrane and the surface. It is hypothesized that these changes occur mainly due to the changes in the conﬁguration of PEG chains and a drastic decrease of the afﬁnity of the polymer for water. The observed phenomena can be applied, e.g., for the production of defect-free supported lipid bilayers in the gel or liquid ordered phase states.


Introduction
Lipid nanocarriers are well established for drug delivery and versatile in their selfassembled structures for many purposes [1]. To increase the colloidal stability of the particles, as well as to prolong their circulation lifetime in vivo, polyethyleneglycol (PEG) grafted lipids or surfactants are commonly added to the preparations [2,3]. This PEGylation strategy has proven useful for a broad range of nanocarriers, including liposomes [4], lipodisks [5], and micelles [6].
Unfortunately, besides the desired increased colloidal stability and prolonged blood survival time, the PEGylation of nanocarriers may lead to some unwanted side effects. For instance, considerable attention has been given to the tendency of PEGylated drug nanocarriers to provoke the production of anti-PEG antibodies, which in turn may result in reduced functionality and toxicity issues [7,8]. Another less recognized and often overlooked problem is that the presence of PEG can result in unwanted interactions between the nanocarriers and certain solid surfaces, such as those composed of silica or the chemically identical quartz. These interactions can lead to biased results from investigations based on spectroscopic analyses with quartz cuvettes and measurements employing Quartz Crystal Microbalance with Dissipation monitoring (QCM-D) in combination with silica sensors [9]. Strategies to avoid or mitigate the PEG-surface interactions are therefore needed. Further, a thorough understanding of the factors affecting the interactions opens up for applications in which the PEG-mediated adsorption is controlled and utilized to obtain surface-immobilized nanocarriers, develop materials for purification/separation, or exploited to produce supported lipid bilayers.

Preparation of Liposomes and Lipodisks
The desired lipids were weighed, or pipetted from stock solutions in chloroform or methanol, and subsequently dissolved in chloroform. A lipid film was obtained by evaporation of the organic solvent, first with a gentle stream of Nitrogen then removing the residual solvent in a vacuum oven from Lab-Line Instruments (Melrose Park, IL, USA) over night.
The lipid film was suspended in either phosphate buffered saline (10 mM, 150 mM NaCl, pH = 7.4) or HEPES buffer (10 mM, 150 mM NaCl, pH = 7.4). The standard protocol for preparation of liposomes and lipodisks consisted of at least 5 and up to 10 freezethawing cycles (freezing with liquid Nitrogen and thawing with a water bath at 60 • C) followed by 31 (liposomes) or 21 (disks) times of extrusion through a 100 nm pore size filter from Whatman plc (Kent, UK).
The lipodisks reported in Section 3.1.1 were prepared by simple hydration of the lipid films in HEPES buffer (20 mM, 150 mM NaCl, pH = 7.4) for 3 h at 70 • C with intermittent mixing. The dispersion was kept at 70 • C and extruded 20 times through a 100 nm pore size filter from Whatman plc (Kent, UK).

QCM-D Characterizations
The interactions of the different liposomes and lipodisks on various surfaces was monitored with the help of a Quartz Crystal Microbalance with Dissipation monitoring from Q-sense (QCM-D E1, Gothenburg, Sweden). The lipid concentration was set to 1 g/L for all experiments unless stated otherwise. Silica (Q-sense, Gothenburg, Sweden) sensors were used. The frequency and dissipation signals were monitored at the fundamental sensor frequency (5 MHz), as well as the 3rd, 5th, 7th, 9th, 11th, and 13th overtones.
The sensors were cleaned before each experiment according to the procedure suggested by the provider. Briefly, the silica sensors were first cleaned in a UV/Ozone chamber from BioForce Nanosciences Inc. (Ames, IA, USA), then immersion of the sensors for 30 min into a 2% SDS-solution followed by rinsing the sensor with Milli-Q water and drying it with nitrogen and then an additional 30 min treatment in the UV/ozone chamber.
The sensors were mounted into the QCM-D at a controlled temperature and rinsed with PBS until equilibration was reached. After a stable baseline was obtained the system was loaded with the liposomes or lipodisks with a flow rate of 150 µL/min until a stable signal was obtained. For experiments with temperature cycling, the temperature was programmed in accordance with the settings shown in Table 1. In order to account for the effect of temperature on the background signal, the same program was run on a bare silica sensor on PBS. The data obtained with immobilized liposomes or disks was then corrected by subtraction of the values obtained on bare silica.
The mass density of the immobilized films was calculated from the QCM-D data using the linear equation proposed by Agmo Hernández et al. [21]: where n is the overtone number, f 0 is the fundamental oscillation frequency of the quartz crystal, t q and ρ q are the thickness and density of the quartz crystal, m d is the adsorbed mass surface density, µ 1 and η 1 are elastic modulus and the viscosity, respectively, of the adsorbed layer. A plot of ∆ f n vs. n∆D at different values of n should have the y-intercept equal to − m d f 0 t q ρ q (i.e., -m d /(17.7 ng −1 Hz −1 cm 2 ) for a 5 MHz crystal). Thus the mass density of surface adsorbed layer could be calculated.

NPS/QCM-D
Simultaneous nanoplasmonic sensing and QCM-D experiments were performed using the Acoulyte instrument by Insplorion AB (Gothemburg, Sweden) coupled to a QCM-D QWM 401 window module (Q-Sense, Gothemburg Sweden) connected to the QCM-D E1 instrument. Details concerning the coupled NPS/QCM-D measurements can be found in Ferhan et al. [22]. Liposomes were loaded at a concentration of 0.5 mM and a flow of 150 µL/min until a stable signal was obtained with both techniques. The shift in centroid position in the extinction spectrum was monitored.

MP-SPR
The multi-parametric surface plasmon resonance (MP-SPR) measurements reported here correspond to the same experiments previously discussed by Zetterberg et al. [20]. Experimental details can be therefore found there. Briefly, experiments were performed with a SPR Navi 220A (BioNavis, Tampere, Finland) using silica coated gold plasmon surfaces on glass substrates. The surface plasmon resonance was monitored at wavelengths 670 and 785 nm for a scanning interval between 39 • and 78 • . The temperature was held at 21 • C. The lipodisks (0.25 mM) were injected at 50 µL/min to two parallel surface areas of the sensor. After 10 min, the sensors were rinsed with PBS. The bound mass was calculated from the following equation [23]: where δ is the decay length of the intensity of the evanescent field associated with the SPR excitation (109 and 154 nm for wavelengths 670 and 785 nm, respectively), S is the bulk sensitivity parameter, dn/dC is the refractive index increment (0.14 mL/g), as calculated from reported values for lipids and PEG and ∆deg is the measurement response. Equation (2) applies only for films much thinner than the decay wavelength δ, a condition that is fulfilled if adsorption of a lipodisk monolayer is assumed.

Results and Discussion
3.1. Lipodisks 3.1.1. Adsorption on Silica at 21 • C Exposure of a silica QCM-D sensor to a 0.25 mM (total lipid) DSPC:DSPE-PEG lipodisk suspension at 21 • C resulted in the adhesion of lipodisks to the surface ( Figure 1) The resulting film could not be removed even after extensive rinsing with buffer, suggesting an irreversible attachment. Noteworthy, repetitions of the experiment resulted in almost exactly the same final surface coverage. This finding is in contrast with previous results observed with active covalent immobilization via amine coupling of lipodisks to NHSactivated gold surfaces, where the degree of surface coverage varied greatly between experiments [21]. Irreversible adhesion of lipodisks was also observed on a silica MP-SPR sensor under the same experimental conditions (Figure 1). amount of water in the film while the latter measures only the dry mass, the results indicate that the water content in the immobilized film increases with increasing PEG-length, while the amount of immobilized lipids decreases. These results agree with what is expected given that the steric repulsion between lipodisks will increase with increasing PEG-length, leading to a more sparse distribution of lipodisks on the surface, decreasing thus the lipid content and increasing the contribution of water to the total film mass. A clearer picture concerning the distribution and orientation of the lipodisks on the surface can be elucidated from the results of the MP-SPR measurements. These suggest that the lipodisk film thickness is in the thin-film range (between 6-10 nm, see Figure S1 in the Supplementary Material) [24], and is thus much smaller than the diameter of the lipid part of the lipodisks as determined by cryo-TEM (25.4, 26 and 23.1 nm for disks stabilized by DSPE-PEG1000, DSPE-PEG2000 and DSPE-PEG5000 respectively [20]). This indicates that the lipodisks adsorb parallel to the surface, in contrast with the perpendicular orientation observed in previous reports for disks covalently bound to NHS-activated gold surfaces using amine coupling [21]. This conclusion is further supported by the rather large value of the Δf/ΔD ratio obtained on silica as compared with the value obtained in covalent coupling experiments (for DSPE-PEG2000 stabilized disks on the 3rd overtone: 20 × 10 6 Hz vs. 4.2 × 10 6 Hz, respectively), meaning that a more rigid film is formed on silica, agreeing with lipodisks lying flat on the surface.
The estimated film thickness, together with the large difference between the determined wet and dry masses, and the not negligible value of the dissipation factors measured with the QCM-D, suggests that the film cannot consist only of lipids, but relatively large amounts of water are likely to be trapped in between the lipodisks and the surface, as well as between the lipodisks.
In summary, it can be safely assumed from the results that the lipodisks are oriented parallel to the surface and separated from it by a thin water layer. Figure 2 shows a schematic illustration of the proposed arrangement of lipodisks on the surface. The thickness of the film, is, according to Figure S1 in the Supporting Information, likely to be independent of the PEG-lipid used. On the other hand, and as mentioned above, the data presented As observed in Figure 1, the size of the PEG chains affected the weight of the formed film. In the QCM-D experiments, the surface-bound mass was highest for the longest PEGchain (PEG5000). The opposite was observed in the MP-SPR experiments. Given that the main difference between the QCM-D and the MP-SPR is that the former measures also the amount of water in the film while the latter measures only the dry mass, the results indicate that the water content in the immobilized film increases with increasing PEG-length, while the amount of immobilized lipids decreases. These results agree with what is expected given that the steric repulsion between lipodisks will increase with increasing PEG-length, leading to a more sparse distribution of lipodisks on the surface, decreasing thus the lipid content and increasing the contribution of water to the total film mass.
A clearer picture concerning the distribution and orientation of the lipodisks on the surface can be elucidated from the results of the MP-SPR measurements. These suggest that the lipodisk film thickness is in the thin-film range (between 6-10 nm, see Figure S1 in the Supplementary Materials) [24], and is thus much smaller than the diameter of the lipid part of the lipodisks as determined by cryo-TEM (25.4, 26 and 23.1 nm for disks stabilized by DSPE-PEG1000, DSPE-PEG2000 and DSPE-PEG5000 respectively [20]). This indicates that the lipodisks adsorb parallel to the surface, in contrast with the perpendicular orientation observed in previous reports for disks covalently bound to NHS-activated gold surfaces using amine coupling [21]. This conclusion is further supported by the rather large value of the ∆f /∆D ratio obtained on silica as compared with the value obtained in covalent coupling experiments (for DSPE-PEG2000 stabilized disks on the 3rd overtone: 20 × 10 6 Hz vs. 4.2 × 10 6 Hz, respectively), meaning that a more rigid film is formed on silica, agreeing with lipodisks lying flat on the surface.
The estimated film thickness, together with the large difference between the determined wet and dry masses, and the not negligible value of the dissipation factors measured with the QCM-D, suggests that the film cannot consist only of lipids, but relatively large amounts of water are likely to be trapped in between the lipodisks and the surface, as well as between the lipodisks.
In summary, it can be safely assumed from the results that the lipodisks are oriented parallel to the surface and separated from it by a thin water layer. Figure 2 shows a schematic illustration of the proposed arrangement of lipodisks on the surface. The thickness of the film, is, according to Figure S1 in the Supporting Information, likely to be independent of the PEG-lipid used. On the other hand, and as mentioned above, the data presented in Figure 1 suggest that the space between disk increases with increasing PEG length, due, most likely, to a stronger steric repulsion between immobilized disks. Physchem 2021, 1, FOR PEER REVIEW 6 in Figure 1 suggest that the space between disk increases with increasing PEG length, due, most likely, to a stronger steric repulsion between immobilized disks. The fact that the immobilized film forms spontaneously and is irreversibly attached to the silica substrate indicates a rather high affinity between the lipodisks and the surface. Indeed, experiments performed with low concentrations of lipodisks (down to 1 µM total lipid concentration) resulted always in complete coverage of the surface upon long enough (up to ~24 h) measurement times (see Figure S2 in the Supplementary Material), further indicating a very high affinity of the particles for the surface at 21 °C Previous experiments performed with PEG-micelles [25] have shown a similar high affinity between highly PEGylated nanocarriers and silica. Figure 3 shows the results from experiments probing adhesion of DSPC:DSPE-PEG2000 lipodisks (80:20) to silica at different temperatures. The concentration of lipid was 500 µM in all cases. Note that the same batch of lipodisks was used for all the experiments summarized in the figure. The collected data reveals some interesting and somewhat unexpected temperature effects. We will first focus on the behavior in the interval between 21 °C and 37 °C. It is observed that the initial increase in temperature (up to 27 °C) results in a decrease of the recorded mass. This can be interpreted as either a decrease in the surface coverage, or a decrease in the water content of the adsorbed film. Given that the affinity of the lipodisks to the surface is rather high according to the results presented above, the second explanation is more likely. Interestingly, increasing the temperature to 32 °C resulted in the formation of an immobilized layer that spontaneously seemed to detach from the surface, as illustrated by the fact that the recorded mass suddenly starts decreasing without any action being taken by the experimenter. Rinsing with buffer does not seem to affect this apparent detachment process. This behavior is even more marked at 37 °C, where a rather fast spontaneous adhesion is followed by an apparent spontaneous detachment of the immobilized film. Noteworthy, after this attachment-detachment process the surface remained inactive for lipodisk adhesion, as flowing a fresh lipodisk suspension over the surface resulted only in a negligible amount of disks attaching. These results suggest that at temperatures ≥ 32 °C the immobilized lipodisks are transformed into a different kind of immobilized structures, with much smaller mass density and the ability to protect the surface against further lipodisk adsorption. It is plausible to assume that these structures are built from PEG-lipids that remain on the surface after the lipodisk detachment. In other words, the results can be explained if it is considered that a few PEGylated lipids are left behind, while the rest of the disk departs from the surface, either as a disk with a lower PEG-content than before the attachment, or as another kind of structure (e.g., a PEGylated vesicle), as illustrated in Figure 4. It has been previously shown that, at this temperature, PEG chains in water tend to acquire an amphiphilic coil-like conformation [26]. Our results suggest that a strong attraction arises when the coil-like conformation becomes dominant resulting in the "pulling out" of PEGylated lipids from lipodisks. This hypothesis will be discussed further in the following sections. The fact that the immobilized film forms spontaneously and is irreversibly attached to the silica substrate indicates a rather high affinity between the lipodisks and the surface. Indeed, experiments performed with low concentrations of lipodisks (down to 1 µM total lipid concentration) resulted always in complete coverage of the surface upon long enough (up to~24 h) measurement times (see Figure S2 in the Supplementary Materials), further indicating a very high affinity of the particles for the surface at 21 • C Previous experiments performed with PEG-micelles [25] have shown a similar high affinity between highly PEGylated nanocarriers and silica. The collected data reveals some interesting and somewhat unexpected temperature effects. We will first focus on the behavior in the interval between 21 • C and 37 • C. It is observed that the initial increase in temperature (up to 27 • C) results in a decrease of the recorded mass. This can be interpreted as either a decrease in the surface coverage, or a decrease in the water content of the adsorbed film. Given that the affinity of the lipodisks to the surface is rather high according to the results presented above, the second explanation is more likely. Interestingly, increasing the temperature to 32 • C resulted in the formation of an immobilized layer that spontaneously seemed to detach from the surface, as illustrated by the fact that the recorded mass suddenly starts decreasing without any action being taken by the experimenter. Rinsing with buffer does not seem to affect this apparent detachment process. This behavior is even more marked at 37 • C, where a rather fast spontaneous adhesion is followed by an apparent spontaneous detachment of the immobilized film. Noteworthy, after this attachment-detachment process the surface remained inactive for lipodisk adhesion, as flowing a fresh lipodisk suspension over the surface resulted only in a negligible amount of disks attaching. These results suggest that at temperatures ≥ 32 • C the immobilized lipodisks are transformed into a different kind of immobilized structures, with much smaller mass density and the ability to protect the surface against further lipodisk adsorption. It is plausible to assume that these structures are built from PEG-lipids that remain on the surface after the lipodisk detachment. In other words, the results can be explained if it is considered that a few PEGylated lipids are left behind, while the rest of the disk departs from the surface, either as a disk with a lower PEG-content than before the attachment, or as another kind of structure (e.g., a PEGylated vesicle), as illustrated in Figure 4. It has been previously shown that, at this temperature, PEG chains in water tend to acquire an amphiphilic coil-like conformation [26]. Our results suggest that a strong attraction arises when the coil-like conformation becomes dominant resulting in the "pulling out" of PEGylated lipids from lipodisks. This hypothesis will be discussed further in the following sections.

Effect of Temperature
working with different lipodisk batches. It has been previously reported that, at these specific temperatures, the PEG silica interaction results in non-monotonic adsorption isotherms dominated by large concentration ranges in which negative adsorption is observed [26], which can be interpreted as a net repulsion between the polymer and the surface. The fact that at these temperatures no stable adsorption of PEGylated particles can be observed is in line with these observations.  To further investigate the role of temperature, experiments were performed in which the lipodisks were immobilized on the silica sensor at 21 °C and then subjected to a temperature cycle as described in the methods section. The calculated immobilized mass (after correction for temperature effects on the background signal) is shown in Figure 5. As can be seen, an initial slight decrease in temperature results in a small increase in the im- working with different lipodisk batches. It has been previously reported that, at these specific temperatures, the PEG silica interaction results in non-monotonic adsorption isotherms dominated by large concentration ranges in which negative adsorption is observed [26], which can be interpreted as a net repulsion between the polymer and the surface. The fact that at these temperatures no stable adsorption of PEGylated particles can be observed is in line with these observations.  To further investigate the role of temperature, experiments were performed in which the lipodisks were immobilized on the silica sensor at 21 °C and then subjected to a temperature cycle as described in the methods section. The calculated immobilized mass (after correction for temperature effects on the background signal) is shown in Figure 5. As can be seen, an initial slight decrease in temperature results in a small increase in the im- Interestingly, the experiments performed at 15 • C and 40 • C do not follow the trend observed for the rest of the experiments (Figure 3). At 15 • C, a sparsely coated surface is obtained, and the immobilized disks are easily washed away by rinsing, in contrast with what is observed at other temperatures. On the other hand, at 40 • C, no interaction at all was recorded during the experiment. Both observations were reproducible, even when working with different lipodisk batches. It has been previously reported that, at these specific temperatures, the PEG silica interaction results in non-monotonic adsorption isotherms dominated by large concentration ranges in which negative adsorption is observed [26], which can be interpreted as a net repulsion between the polymer and the surface. The fact that at these temperatures no stable adsorption of PEGylated particles can be observed is in line with these observations.
To further investigate the role of temperature, experiments were performed in which the lipodisks were immobilized on the silica sensor at 21 • C and then subjected to a temperature cycle as described in the methods section. The calculated immobilized mass (after correction for temperature effects on the background signal) is shown in Figure 5. As can be seen, an initial slight decrease in temperature results in a small increase in the immobilized mass. However, upon heating, a rather sudden drop in the measured mass occurs at a temperature~33.5 • C. At temperatures ≥35 • C no disks are left on the surface, although some minor mass changes are observed. Decreasing the temperature does not result in the recovery of the original signal, meaning that no new disks adsorb on the surface and indicating that the latter is coated by a thin film not clearly detected by the instrument. mobilized mass. However, upon heating, a rather sudden drop in the measured mass occurs at a temperature ~33.5 °C. At temperatures ≥35 °C no disks are left on the surface, although some minor mass changes are observed. Decreasing the temperature does not result in the recovery of the original signal, meaning that no new disks adsorb on the surface and indicating that the latter is coated by a thin film not clearly detected by the instrument.
These observations agree with the experiments performed at different fixed temperatures described above (Figure 3). Taken together, the results indicate that major structural changes of the immobilized material take place when the temperature is increased beyond ~32 °C. In addition to the investigations performed with lipodisks, QCM-D experiments were carried out with repeated application of DSPE-PEG2000 micelles to a silica sensor ( Figure 6). The collected data indicate that the interaction between the micelles and the silica surface is clearly reduced when a second dose of micelles is applied to the sensor. Furthermore, it is not possible to wash of the micelles even after extend times of rinsing the sensor with buffer solution. The reason for this observation is again hypothesized to be that PEG-lipids remain on the sensor after the washing step, and thus reduce the possibility for interactions with subsequently added DSPE-PEG2000 micelles.  These observations agree with the experiments performed at different fixed temperatures described above (Figure 3). Taken together, the results indicate that major structural changes of the immobilized material take place when the temperature is increased beyond 32 • C.
In addition to the investigations performed with lipodisks, QCM-D experiments were carried out with repeated application of DSPE-PEG2000 micelles to a silica sensor ( Figure 6). The collected data indicate that the interaction between the micelles and the silica surface is clearly reduced when a second dose of micelles is applied to the sensor. Furthermore, it is not possible to wash of the micelles even after extend times of rinsing the sensor with buffer solution. The reason for this observation is again hypothesized to be that PEG-lipids remain on the sensor after the washing step, and thus reduce the possibility for interactions with subsequently added DSPE-PEG2000 micelles.
Physchem 2021, 1, FOR PEER REVIEW 8 mobilized mass. However, upon heating, a rather sudden drop in the measured mass occurs at a temperature ~33.5 °C. At temperatures ≥35 °C no disks are left on the surface, although some minor mass changes are observed. Decreasing the temperature does not result in the recovery of the original signal, meaning that no new disks adsorb on the surface and indicating that the latter is coated by a thin film not clearly detected by the instrument. These observations agree with the experiments performed at different fixed temperatures described above (Figure 3). Taken together, the results indicate that major structural changes of the immobilized material take place when the temperature is increased beyond ~32 °C. In addition to the investigations performed with lipodisks, QCM-D experiments were carried out with repeated application of DSPE-PEG2000 micelles to a silica sensor ( Figure 6). The collected data indicate that the interaction between the micelles and the silica surface is clearly reduced when a second dose of micelles is applied to the sensor. Furthermore, it is not possible to wash of the micelles even after extend times of rinsing the sensor with buffer solution. The reason for this observation is again hypothesized to be that PEG-lipids remain on the sensor after the washing step, and thus reduce the possibility for interactions with subsequently added DSPE-PEG2000 micelles.

The Effect of the Hydration Layer on the Interaction of Lipodisks with Silica
The fact that the release of the lipodisks at 37 • C results in an immobilized film that is not clearly detected by the QCM-D suggests that the PEG chains are strongly and directly bound to the silica surface. This in turn suggests that the PEG-silica interaction is strong enough to remove the hydration layer on the silica surface. Monovalent counterions at the surface are also likely released. We hypothesized therefore that generating a thicker and more strongly bound hydration layer on silica would hinder the attachment of PEGylated particles to the surface. The effect of the hydration layer on silica and the lipid aggregates was investigated by means of QCM-D experiments in which the HEPES buffer containing 150 mM NaCl was substituted for HEPES buffer containing 75 mM CaCl 2 . As can be deduced from the data presented in Figure 7, the buffer change resulted in a markedly different adsorption behavior. In buffer containing 150 mM NaCl the lipodisks attached to the silica sensor and formed a stable layer that could not be washed off by the buffer (Figure 7a). However, repeating the experiment with a sample dispersed in a CaCl 2 -containing buffer resulted in frequency and dissipation data indicating a negligible interaction between the lipodisks and the silica sensor (Figure 7b). Similar experiments with lipodisks containing DSPE-PEG5000 instead of DSPE-PEG2000 (Supplementary Materials Figure S3) showed the same trend.
interaction between the sensor and the micelles is measured. The vertical black reference lines indicate the start of the rinsing (t = 0.5 h) and the second injection of the micelles solution (t = 16.5 h). The grey horizontal lines indicate the maximum dissipation and minimum frequency shift after the first application of micelles. T = 21 °C.

The Effect of the Hydration Layer on the Interaction of Lipodisks with Silica
The fact that the release of the lipodisks at 37 °C results in an immobilized film that is not clearly detected by the QCM-D suggests that the PEG chains are strongly and directly bound to the silica surface. This in turn suggests that the PEG-silica interaction is strong enough to remove the hydration layer on the silica surface. Monovalent counterions at the surface are also likely released. We hypothesized therefore that generating a thicker and more strongly bound hydration layer on silica would hinder the attachment of PEGylated particles to the surface. The effect of the hydration layer on silica and the lipid aggregates was investigated by means of QCM-D experiments in which the HEPES buffer containing 150 mM NaCl was substituted for HEPES buffer containing 75 mM CaCl2. As can be deduced from the data presented in Figure 7, the buffer change resulted in a markedly different adsorption behavior. In buffer containing 150 mM NaCl the lipodisks attached to the silica sensor and formed a stable layer that could not be washed off by the buffer (Figure 7a). However, repeating the experiment with a sample dispersed in a CaCl2-containing buffer resulted in frequency and dissipation data indicating a negligible interaction between the lipodisks and the silica sensor (Figure 7b). Similar experiments with lipodisks containing DSPE-PEG5000 instead of DSPE-PEG2000 (Supplementary Materials Figure S3) showed the same trend. The presence of the multivalent calcium ions obviously has an inhibitory effect on the binding of the lipodisks to the silica surface. This suggests that the thicker Stern layers (on both, the lipodisks and, perhaps more importantly, on silica) and stronger hydration forces arising from the presence of multivalent ions [27,28], prevent or decrease, the strength of the interaction between PEG and silica. The stronger hydration repulsive force thereby results in an unfavorable interaction between lipodisks and silica in the presence of calcium ions.
Unlike the well-known calcium triggered fusion process reported with liposomes, neither aggregation nor fusion of the lipodisks was induced by the addition of calcium ions, as confirmed by DLS measurements (Supplementary Materials Figure S4).

Liposomes
Given the unique adhesion behavior of lipodisks onto silica surfaces, we set out to investigate how PEGylation of liposomes affect their interaction with silica substrates. It The presence of the multivalent calcium ions obviously has an inhibitory effect on the binding of the lipodisks to the silica surface. This suggests that the thicker Stern layers (on both, the lipodisks and, perhaps more importantly, on silica) and stronger hydration forces arising from the presence of multivalent ions [27,28], prevent or decrease, the strength of the interaction between PEG and silica. The stronger hydration repulsive force thereby results in an unfavorable interaction between lipodisks and silica in the presence of calcium ions.
Unlike the well-known calcium triggered fusion process reported with liposomes, neither aggregation nor fusion of the lipodisks was induced by the addition of calcium ions, as confirmed by DLS measurements (Supplementary Materials Figure S4).

Liposomes
Given the unique adhesion behavior of lipodisks onto silica surfaces, we set out to investigate how PEGylation of liposomes affect their interaction with silica substrates. It is well known that non-PEGylated liposomes in the liquid disordered phase state tend to rupture and spread on silica surfaces [29,30] leading to the formation of supported lipid bilayers (SLBs). Liposomes in the gel phase state usually adhere as intact liposomes, while liposomes containing cholesterol have been reported to present mixed behaviors (sometimes adhering as intact liposomes and sometimes spreading), depending on the specific conditions of the experiments [9]. Hereby we investigate the effect of PEGylation on the liposome-silica interactions for liposomes in the liquid disordered, gel, and liquid ordered phase states.

Liposomes in the Liquid Disordered Phase State
As mentioned above, liposomes formed by a lipid membrane in the liquid disordered phase state usually adhere and spread on silica surfaces. Although the process has mainly been studied using small sonicated liposomes [29], it has been shown that the same applies for larger extruded liposomes based on POPC [9]. Figure 8 indeed shows that extruded POPC liposomes initially adhere on the QCM-D silica sensor and rupture and spread after a few seconds (as evidenced by the drop in frequency and dissipation values). The coating of the surface seems to be incomplete, as adhesion of intact liposomes (as evidenced by changes in both frequency and dissipation factor) is still observed. However, these intact liposomes are rinsed away when clean buffer is introduced. Prolonged rinsing (several hours, results not shown) resulted often in the signal stabilizing at a frequency change of ca −25 Hz and small values for the dissipation factor (<<1·10 −6 ), suggesting that a supported lipid bilayer remains on the surface.
As mentioned above, liposomes formed by a lipid membrane in the liquid disordered phase state usually adhere and spread on silica surfaces. Although the process has mainly been studied using small sonicated liposomes [29], it has been shown that the same applies for larger extruded liposomes based on POPC [9]. Figure 8 indeed shows that extruded POPC liposomes initially adhere on the QCM-D silica sensor and rupture and spread after a few seconds (as evidenced by the drop in frequency and dissipation values). The coating of the surface seems to be incomplete, as adhesion of intact liposomes (as evidenced by changes in both frequency and dissipation factor) is still observed. However, these intact liposomes are rinsed away when clean buffer is introduced. Prolonged rinsing (several hours, results not shown) resulted often in the signal stabilizing at a frequency change of ca −25 Hz and small values for the dissipation factor (<<1·10 −6 ), suggesting that a supported lipid bilayer remains on the surface.
Performing the experiments with liposomes modified with 4 moL% of PEGylated lipid (Figure 8) resulted in a slower adhesion process, likely due to steric repulsion between adhered and dispersed liposomes. After a few minutes the liposomes eventually ruptured and spread, and no further liposome adhesion was observed. Prolonged rinsing had no effect on the signal obtained. The final values of frequency and dissipation factor changes (−30 Hz and 2·10 −6 , respectively), suggest a structure heavier and softer than that of a supported POPC bilayer. Applying the same temperature cycle as for the lipodisks (Figure 9), resulted in a decrease in mass as the temperature increased, with a sharp drop at ~35 °C. As for the case of the lipodisks, decreasing the temperature did not result in the recovery of the original mass. The results again suggest that an irreversible change in the immobilized structure takes place at temperatures > 32 °C. To verify that the effect of temperature is coupled to the presence of PEG lipids and does not arise from the background correction or any other artifact, the same temperature cycle and the same background correction were applied to an SLB formed by pure POPC. As observed in Figure 9, the effect of temperature is in this case the opposite: the mass Performing the experiments with liposomes modified with 4 moL% of PEGylated lipid (Figure 8) resulted in a slower adhesion process, likely due to steric repulsion between adhered and dispersed liposomes. After a few minutes the liposomes eventually ruptured and spread, and no further liposome adhesion was observed. Prolonged rinsing had no effect on the signal obtained. The final values of frequency and dissipation factor changes (−30 Hz and 2·10 −6 , respectively), suggest a structure heavier and softer than that of a supported POPC bilayer. Applying the same temperature cycle as for the lipodisks (Figure 9), resulted in a decrease in mass as the temperature increased, with a sharp drop at~35 • C. As for the case of the lipodisks, decreasing the temperature did not result in the recovery of the original mass. The results again suggest that an irreversible change in the immobilized structure takes place at temperatures > 32 • C.
To verify that the effect of temperature is coupled to the presence of PEG lipids and does not arise from the background correction or any other artifact, the same temperature cycle and the same background correction were applied to an SLB formed by pure POPC. As observed in Figure 9, the effect of temperature is in this case the opposite: the mass increases with increasing temperature (likely because more water enters the space between the membrane and the surface), and this increase is reversible (the mass returns to the initial value when the temperature decreases). Thus, it can be concluded that the observed effect of temperature is coupled to the presence of PEG on the immobilized structures.
increases with increasing temperature (likely because more water enters the space between the membrane and the surface), and this increase is reversible (the mass returns to the initial value when the temperature decreases). Thus, it can be concluded that the observed effect of temperature is coupled to the presence of PEG on the immobilized structures.

Liposomes in the Gel Phase State
Both pure DPPC and DPPC:DSPE-PEG2000 (96:4) liposomes in the gel-phase state adhered spontaneously to the silica sensor and remained bound even after extensive rinsing ( Figure 10). The main difference between the behavior of the PEGylated and the non-PEGylated liposomes was the larger frequency and dissipation changes observed for the latter, likely because the liposomes can pack more tightly on the surface. Interestingly, for both compositions a peak in the monitored dissipation factor can be observed in the initial stages of the adhesion process. This peak is not reflected in the changes in oscillation frequency. This suggests structural rearrangements of the liposomes occurring at the surface, with the immobilized films becoming more rigid over time. These rearrangements seem to be faster in the case of PEG-containing liposomes. Applying the previously described temperature program to the layer of immobilized liposomes resulted in interesting differences between the PEGylated and non-PEGylated

Liposomes in the Gel Phase State
Both pure DPPC and DPPC:DSPE-PEG2000 (96:4) liposomes in the gel-phase state adhered spontaneously to the silica sensor and remained bound even after extensive rinsing ( Figure 10). The main difference between the behavior of the PEGylated and the non-PEGylated liposomes was the larger frequency and dissipation changes observed for the latter, likely because the liposomes can pack more tightly on the surface. Interestingly, for both compositions a peak in the monitored dissipation factor can be observed in the initial stages of the adhesion process. This peak is not reflected in the changes in oscillation frequency. This suggests structural rearrangements of the liposomes occurring at the surface, with the immobilized films becoming more rigid over time. These rearrangements seem to be faster in the case of PEG-containing liposomes.
served effect of temperature is coupled to the presence of PEG on the immobilized structures.

Liposomes in the Gel Phase State
Both pure DPPC and DPPC:DSPE-PEG2000 (96:4) liposomes in the gel-phase state adhered spontaneously to the silica sensor and remained bound even after extensive rinsing ( Figure 10). The main difference between the behavior of the PEGylated and the non-PEGylated liposomes was the larger frequency and dissipation changes observed for the latter, likely because the liposomes can pack more tightly on the surface. Interestingly, for both compositions a peak in the monitored dissipation factor can be observed in the initial stages of the adhesion process. This peak is not reflected in the changes in oscillation frequency. This suggests structural rearrangements of the liposomes occurring at the surface, with the immobilized films becoming more rigid over time. These rearrangements seem to be faster in the case of PEG-containing liposomes. Applying the previously described temperature program to the layer of immobilized liposomes resulted in interesting differences between the PEGylated and non-PEGylated Applying the previously described temperature program to the layer of immobilized liposomes resulted in interesting differences between the PEGylated and non-PEGylated DPPC liposomes ( Figure 11). As seen in the figure, in the absence of PEG lipids the liposomes seem to swell as the temperature increases and finally some of them rupture and spread at a temperature corresponding to the main phase transition temperature of the lipids (41 • C). On the other hand, the PEGylated liposome layer decreases in mass as soon as the temperature starts increasing, and there is an abrupt drop in mass, suggesting vesicle rupture and spreading at 35 • C. Note that the signal remains fairly stable after this point. Indeed, repetitions of the experiments resulted in reproducible final values when the liposomes were PEGylated, whereas non-PEGylated DPPC liposomes showed large variations between experiments. This observation can be interpreted as a complete rupture of the liposomes and formation of a supported lipid bilayer in the presence of PEG, while, for non-PEGylated liposomes, whole intact liposomes remain on the surface, even after repeated temperature cycles (data not shown). This observation together with the fact that the rupture process occurs at a lower temperature, strongly suggest that PEGylation of the liposomes facilitates their rupture and spreading on the silica surface. This phenomenon has been previously exploited in our laboratory to produce supported DPPC bilayers in the gel-phase state [31,32]. The results from peptide binding experiments performed on these supported structures suggest that the formed bilayers are essentially defect free. To our knowledge, these are the only studies so far that report on the successful formation of supported lipid bilayers in the gel-phase state via vesicle fusion.
icle rupture and spreading at 35 °C. Note that the signal remains fairly stable after this point. Indeed, repetitions of the experiments resulted in reproducible final values when the liposomes were PEGylated, whereas non-PEGylated DPPC liposomes showed large variations between experiments. This observation can be interpreted as a complete rupture of the liposomes and formation of a supported lipid bilayer in the presence of PEG, while, for non-PEGylated liposomes, whole intact liposomes remain on the surface, even after repeated temperature cycles (data not shown). This observation together with the fact that the rupture process occurs at a lower temperature, strongly suggest that PEGylation of the liposomes facilitates their rupture and spreading on the silica surface. This phenomenon has been previously exploited in our laboratory to produce supported DPPC bilayers in the gel-phase state [31,32]. The results from peptide binding experiments performed on these supported structures suggest that the formed bilayers are essentially defect free. To our knowledge, these are the only studies so far that report on the successful formation of supported lipid bilayers in the gel-phase state via vesicle fusion. In order to test whether the same phenomenon would be observed with other lipids in the gel phase state, we repeated the experiments substituting DPPC for DSPC. As for the other liposomes studied, the adhesion of PEGylated liposomes was slightly slower than that of non-PEGylated liposomes ( Figure 12). However, in contrast with the results obtained with other compositions, the final shift in oscillation frequency was mostly unaffected suggesting a similar degree of coverage regardless of the presence of PEG-lipids. Another remarkable fact is that after the peak in dissipation, observed right after adhesion, the dissipation signal from PEGylated DSPC liposomes drops steadily, suggesting a continuous "hardening" of the immobilized film. In order to test whether the same phenomenon would be observed with other lipids in the gel phase state, we repeated the experiments substituting DPPC for DSPC. As for the other liposomes studied, the adhesion of PEGylated liposomes was slightly slower than that of non-PEGylated liposomes ( Figure 12). However, in contrast with the results obtained with other compositions, the final shift in oscillation frequency was mostly unaffected suggesting a similar degree of coverage regardless of the presence of PEG-lipids. Another remarkable fact is that after the peak in dissipation, observed right after adhesion, the dissipation signal from PEGylated DSPC liposomes drops steadily, suggesting a continuous "hardening" of the immobilized film.
Interestingly, experiments performed with coupled/simultaneous QCM-D and NPS ( Figure 13) showed that the acoustic and the optical signals behave in opposite ways after liposome immobilization. While the wet mass recorded by the QCM-D drops steadily over time, the dry mass (proportional to the shift in centroid position in NPS) continuously increases. This apparent discrepancy can be explained if it is assumed that the liposomes rearrange on the surface in such a way that increasingly more PEG lipids bind to the surface (resulting in an increase in the NPS signal over time) and that in this process water is released from the surface-liposome interspace, resulting in a decrease of the QCM-D signal. Furthermore, the peak observed in the QCM-D signal is not observed in the NPS trace suggesting again a structural rearrangement in which only water is displaced. Interestingly, experiments performed with coupled/simultaneous QCM-D and NPS ( Figure 13) showed that the acoustic and the optical signals behave in opposite ways after liposome immobilization. While the wet mass recorded by the QCM-D drops steadily over time, the dry mass (proportional to the shift in centroid position in NPS) continuously increases. This apparent discrepancy can be explained if it is assumed that the liposomes rearrange on the surface in such a way that increasingly more PEG lipids bind to the surface (resulting in an increase in the NPS signal over time) and that in this process water is released from the surface-liposome interspace, resulting in a decrease of the QCM-D signal. Furthermore, the peak observed in the QCM-D signal is not observed in the NPS trace suggesting again a structural rearrangement in which only water is displaced. Applying the temperature program to immobilized DSPC-based liposomes resulted in the QCM-D mass densities illustrated in Figure 14. As in the case of DPPC, a sudden drop in the immobilized mass is observed at a temperature corresponding to the phase transition temperature of the lipid (~55 °C) when working with non-PEGylated liposomes. For PEGylated liposomes, the immobilized mass slowly starts decreasing at around 30 °C. This decrease gets continuously faster after 40 °C and, finally, a sudden drop of the mass is observed at 53 °C. The results suggest that, as in the case of DPPC, the liposomes start  Interestingly, experiments performed with coupled/simultaneous QCM-D and NPS ( Figure 13) showed that the acoustic and the optical signals behave in opposite ways after liposome immobilization. While the wet mass recorded by the QCM-D drops steadily over time, the dry mass (proportional to the shift in centroid position in NPS) continuously increases. This apparent discrepancy can be explained if it is assumed that the liposomes rearrange on the surface in such a way that increasingly more PEG lipids bind to the surface (resulting in an increase in the NPS signal over time) and that in this process water is released from the surface-liposome interspace, resulting in a decrease of the QCM-D signal. Furthermore, the peak observed in the QCM-D signal is not observed in the NPS trace suggesting again a structural rearrangement in which only water is displaced. Applying the temperature program to immobilized DSPC-based liposomes resulted in the QCM-D mass densities illustrated in Figure 14. As in the case of DPPC, a sudden drop in the immobilized mass is observed at a temperature corresponding to the phase transition temperature of the lipid (~55 °C) when working with non-PEGylated liposomes. For PEGylated liposomes, the immobilized mass slowly starts decreasing at around 30 °C. This decrease gets continuously faster after 40 °C and, finally, a sudden drop of the mass is observed at 53 °C. The results suggest that, as in the case of DPPC, the liposomes start Applying the temperature program to immobilized DSPC-based liposomes resulted in the QCM-D mass densities illustrated in Figure 14. As in the case of DPPC, a sudden drop in the immobilized mass is observed at a temperature corresponding to the phase transition temperature of the lipid (~55 • C) when working with non-PEGylated liposomes. For PEGylated liposomes, the immobilized mass slowly starts decreasing at around 30 • C. This decrease gets continuously faster after 40 • C and, finally, a sudden drop of the mass is observed at 53 • C. The results suggest that, as in the case of DPPC, the liposomes start rupturing while still in the gel phase. Similarly to DPPC, the signals obtained after liposome rupturing are very stable and reproducible when working the PEGylated liposomes, suggesting the formation of a stable supported lipid bilayer in the gel phase state.
The observed fact that PEGylation enhances liposome rupture and spreading on silica surfaces when the temperature is >35 • C is likely to arise from a high affinity of PEG to silica. Although the mechanisms by which liposomes rupture and spread on hydrophilic surfaces are still discussed, it is generally accepted that the process can only occur if the attractive forces between the surface and the membrane are strong enough to deform the liposomes up to the point of rupture [33,34]. Our results suggest that inclusion of PEG does increase the strength of the attractive interactions, and this increase is high enough to induce rupture when the temperature is above~35 • C. Indeed, it has been previously shown [35] that, at this temperature, the conformation of PEG adsorbed on silica changes (the polymer stretches on the surface) due to a high affinity of the polymer for the surface. As mentioned above, the fact that, even at room temperature, the optical (NPS) signal increases while the QCM-D signal decreases when both are measured simultaneously for DSPC-DSPEPEG2000 liposomes is in line with the liposomes flattening on the surface, leading to a curved, stressed edge where rupture can eventually occur ( Figure 15).
Physchem 2021, 1, FOR PEER REVIEW 14 rupturing while still in the gel phase. Similarly to DPPC, the signals obtained after liposome rupturing are very stable and reproducible when working the PEGylated liposomes, suggesting the formation of a stable supported lipid bilayer in the gel phase state. The observed fact that PEGylation enhances liposome rupture and spreading on silica surfaces when the temperature is >35 °C is likely to arise from a high affinity of PEG to silica. Although the mechanisms by which liposomes rupture and spread on hydrophilic surfaces are still discussed, it is generally accepted that the process can only occur if the attractive forces between the surface and the membrane are strong enough to deform the liposomes up to the point of rupture [33,34]. Our results suggest that inclusion of PEG does increase the strength of the attractive interactions, and this increase is high enough to induce rupture when the temperature is above ~35°C. Indeed, it has been previously shown [35] that, at this temperature, the conformation of PEG adsorbed on silica changes (the polymer stretches on the surface) due to a high affinity of the polymer for the surface. As mentioned above, the fact that, even at room temperature, the optical (NPS) signal increases while the QCM-D signal decreases when both are measured simultaneously for DSPC-DSPEPEG2000 liposomes is in line with the liposomes flattening on the surface, leading to a curved, stressed edge where rupture can eventually occur ( Figure 15). The question remains concerning why liposomes break while, in the case of lipodisks, the PEGylated lipids seem to be instead detached from the aggregates. A possibility  The observed fact that PEGylation enhances liposome rupture and spreading on silica surfaces when the temperature is >35 °C is likely to arise from a high affinity of PEG to silica. Although the mechanisms by which liposomes rupture and spread on hydrophilic surfaces are still discussed, it is generally accepted that the process can only occur if the attractive forces between the surface and the membrane are strong enough to deform the liposomes up to the point of rupture [33,34]. Our results suggest that inclusion of PEG does increase the strength of the attractive interactions, and this increase is high enough to induce rupture when the temperature is above ~35°C. Indeed, it has been previously shown [35] that, at this temperature, the conformation of PEG adsorbed on silica changes (the polymer stretches on the surface) due to a high affinity of the polymer for the surface. As mentioned above, the fact that, even at room temperature, the optical (NPS) signal increases while the QCM-D signal decreases when both are measured simultaneously for DSPC-DSPEPEG2000 liposomes is in line with the liposomes flattening on the surface, leading to a curved, stressed edge where rupture can eventually occur ( Figure 15). The question remains concerning why liposomes break while, in the case of lipodisks, the PEGylated lipids seem to be instead detached from the aggregates. A possibility The question remains concerning why liposomes break while, in the case of lipodisks, the PEGylated lipids seem to be instead detached from the aggregates. A possibility would be that the energy cost of pulling out several PEG-lipids at once from the liposomes is larger than the energy cost of deforming and breaking the membrane. Alternatively, it could be proposed that the former process is kinetically hindered (as several PEG-lipids would need to be detached at once) while the latter can occur much faster. However, this would mean that the release of the bilayer lipids from lipodisks at this temperature would be very slow, which is not the case. A more likely explanation is that, as the amount of PEG in the liposomes is much lower than in the disks, the resulting open bilayer would have enough free space to adsorb on the surface (contrary to the case of lipodisks where most of the surface is covered by PEG-lipids) even if the PEG-lipids are eventually pulled out of the membrane. It can also be speculated that this behavior is linked to the reported transition from amphiphilic helical to hydrophobic coil-like configurations of PEG at 35 • C [26]. In the case of lipodisks, the local concentration of PEG near the surface is very high and can therefore result in the formation of aggregates when the affinity of the polymer for water decreases. The formation of these aggregates may cause the "pulling-out" of the PEGylated lipids from the lipodisks membrane when the temperature reaches 35 • C. In the case of liposomes, the local concentration of PEG is much lower, and it is therefore possible that no such aggregation occurs, leaving thus the PEG-lipids incorporated into the membrane.

Liposomes in the Liquid Ordered Phase (DSPC:Cholesterol)
As for liposomes in the liquid disordered (i.e., POPC liposomes) and gel phase (i.e., DPPC and DSPC liposomes) states, inclusion of PEG-lipids resulted in a slower adhesion process when working with liposomes containing cholesterol, i.e., liposomes in the liquid ordered phase state ( Figure 16). No liposome rupture was observed even at prolonged times. The peak in dissipation observed for gel phase liposomes is also appreciated in the liquid ordered phase, suggesting that structural rearrangements occur close to the surface. Upon subjecting the immobilized liposome films to the temperature program ( Figure 17), it was observed that while non-PEGylated liposomes were barely affected by the temperature change, PEGylated liposomes rupture and spread reproducibly when the temperature reaches ca 33 • C. Given that no phase transition is expected for liposomes of the studied composition, the results suggest that PEG-silica interactions are responsible for this behavior.
high and can therefore result in the formation of aggregates when the affinity of the polymer for water decreases. The formation of these aggregates may cause the "pulling-out" of the PEGylated lipids from the lipodisks membrane when the temperature reaches 35 °C. In the case of liposomes, the local concentration of PEG is much lower, and it is therefore possible that no such aggregation occurs, leaving thus the PEG-lipids incorporated into the membrane.

Liposomes in the Liquid Ordered Phase (DSPC:Cholesterol)
As for liposomes in the liquid disordered (i.e., POPC liposomes) and gel phase (i.e., DPPC and DSPC liposomes) states, inclusion of PEG-lipids resulted in a slower adhesion process when working with liposomes containing cholesterol, i.e., liposomes in the liquid ordered phase state ( Figure 16). No liposome rupture was observed even at prolonged times. The peak in dissipation observed for gel phase liposomes is also appreciated in the liquid ordered phase, suggesting that structural rearrangements occur close to the surface. Upon subjecting the immobilized liposome films to the temperature program (Figure 17), it was observed that while non-PEGylated liposomes were barely affected by the temperature change, PEGylated liposomes rupture and spread reproducibly when the temperature reaches ca 33 °C. Given that no phase transition is expected for liposomes of the studied composition, the results suggest that PEG-silica interactions are responsible for this behavior.

Conclusions
From the results presented above it is clear that PEGylated liposomes and lipodisks spontaneously attach to silica surfaces at room temperature, forming immobilized layers consisting of either intact liposomes (if using liposomes in the gel or liquid ordered phase states), supported lipid bilayers (in the case of liposomes in the liquid disordered phase state), or intact lipodisks bound parallel to the surface. The characteristics of the formed

Conclusions
From the results presented above it is clear that PEGylated liposomes and lipodisks spontaneously attach to silica surfaces at room temperature, forming immobilized layers consisting of either intact liposomes (if using liposomes in the gel or liquid ordered phase states), supported lipid bilayers (in the case of liposomes in the liquid disordered phase state), or intact lipodisks bound parallel to the surface. The characteristics of the formed layers are very reproducible (in terms e.g., of surface coverage and film thickness) for a given composition of the lipid nanoparticles, and the attachment seems to be driven by a high affinity between the PEG chains and the silica surface. Interestingly, the results also show that increasing the temperature leads to irreversible changes in the nature of the supported layers. These changes occur when the temperature reaches~35 • C, i.e., the same temperature at which previous reports have suggested that the configuration of PEG in solution changes from helical to coil-like and the affinity of the polymer to water decreases drastically [26] while its affinity for silica increases [35]. While in aqueous solutions of PEG the change from helical to coil-like conformations results in a decrease in affinity to silica, likely because a strong repulsion arises between the polymer and the hydration layer on the surface, we show in this work that, for immobilized PEGylated structures, the opposite occurs: i.e., the coil-like conformation gives rise to a strong attraction between the polymer and the surface, resulting in liposome rupture and the "pulling out" of PEGylated lipids from lipodisks. An explanation for this apparent discrepancy is provided by the experiments performed in the presence of calcium. According to the obtained results, when attaching onto silica at room temperature the PEG chains are likely to remove/replace the hydration layer on the surface. Thus, once the temperature is increased to the point where the affinity between PEG and water is low, it is favorable for PEG to adsorb even more strongly onto the already water-depleted silica surface, thus minimizing its interactions with water. This hypothesis is further supported by the fact that immobilizing the particles at room temperature and then increasing the temperature well above 40 • C does not result in a recovery of the bare surface (meaning that the polymer remains adsorbed on the surface), whereas attempts to perform the immobilization directly at 40 • C results in no interaction at all (meaning that the polymer is repelled from the surface, as the hydration layer has not been removed).
The described phenomena has already found applications in, e.g., the production of supported lipid bilayers in the gel phase [31,32] (Figure 18). Future applications may include sorting of nanoparticles (e.g., separating them by degree of PEGylation), enrichment of certain proteins or molecules of interest tagged with PEG, and passivation of quartz and other silica-like surfaces to avoid unwanted interactions (as proposed in recent work from our laboratory [15]).
Physchem 2021, 1, FOR PEER REVIEW 17 and other silica-like surfaces to avoid unwanted interactions (as proposed in recent work from our laboratory [15]).

Institutional Review Board Statement: Not applicable.
Informed Consent Statement: Not applicable.

Data Availability Statement:
The data presented in this study is contained within the article or Supplementary Materials. versity of Technology, Sweden) are gratefully acknowledged for assistance in the collection and evaluation of MP-SPR data. Insplorion AB (Gothemburg, Sweden) is acknowledged for providing access to the Acoulyte instrument and for assistance with the interpretation of the NPS data. Valuable assistance from Xinchen Zhang and Dimitrios Georgouvelas with the experimental work is greatly appreciated.

Conflicts of Interest:
The authors declare no conflict of interest.