Cooperative Stabilization of Close-Contact Zones Leads to Sensitivity and Selectivity in T-Cell Recognition

T cells are sensitive to 1 to 10 foreign-peptide-MHC complexes among a vast majority of self-peptide-MHC complexes, and discriminate selectively between peptide-MHC complexes that differ not much in their binding affinity to T-cell receptors (TCRs). Quantitative models that aim to explain this sensitivity and selectivity largely focus on single TCR/peptide-MHC complexes, but T cell adhesion involves a multitude of different complexes. In this article, we demonstrate in a three-dimensional computational model of T-cell adhesion that the cooperative stabilization of close-contact zones is sensitive to one to three foreign-peptide-MHC complexes and occurs at a rather sharp threshold affinity of these complexes, which implies selectivity. In these close-contact zones with lateral extensions of hundred to several hundred nanometers, few TCR/foreign-peptide-MHC complexes and many TCR/self-peptide-MHC complexes are segregated from LFA-1/ICAM-1 complexes that form at larger membrane separations. Previous high-resolution microscopy experiments indicate that the sensitivity and selectivity in the formation of closed-contact zones reported here are relevant for T-cell recognition, because the stabilization of close-contact zones by foreign, agonist peptide-MHC complexes precedes T-cell signaling and activation in the experiments.


Introduction
T cells recognize foreign peptides that are bound to major histocompatibility complexes (MHCs) on apposing cell surfaces among a vast majority of self peptides [1]. This recognition is highly sensitive and selective: T cells can be sensitive to between 1 and 10 foreign-peptide-MHC complexes [2][3][4][5], and discriminate selectively between foreignpeptide-MHC and self-peptide-MHC complexes that differ not strongly in their binding affinity to T-cell receptors [6][7][8][9]. Such selectivity is typically seen to require kinetic proof-reading in TCR binding, which involves a series of biochemical transformations in TCR/peptide-MHC complexes [10][11][12][13][14][15]. Kinetic proofreading focuses on individual TCR binding events and single TCR/peptide-MHC complexes, but T cells interact with apposing cells via many complexes. Increasing the concentration of self-peptide-MHCs has been shown to increase the response of T cells to foreign-peptide-MHCs [16,17], which points to a cooperativity between TCR/self-peptide-MHC and TCR/foreign-peptide-MHC complexes in T-cell recognition. The formation of these TCR complexes occurs at close contact of about 15 nm, while the longer LFA-1/ICAM-1 complexes form at larger cell-cell separations of about 40 nm [18]. High-resolution microscopy experiments showed that TCR/foreign-peptide-MHC complexes stabilize close-contact zones during the scanning of antigen-presenting cells by T cells [19]. The stabilization of the close-contact zones is independent of the actin cytoskeleton and of TCR-induced signaling and, thus, appears to precede and initiate T-cell signaling and activation.
In this article, we investigate the interplay of few TCR/foreign-peptide-MHC and many TCR/self-peptide-MHC and LFA-1/ICAM-1 complexes in a computational model of T-cell adhesion. The longer LFA-1/ICAM-1 complexes tend to segregate from the shorter TCR/MHC complexes because the membranes need to curve to compensate the length mismatch, which costs bending energy. The TCR/foreign-peptide-MHC and TCR/selfpeptide-MHC complexes therefore form in close-contact zones that are separated from domains of LFA-1/ICAM-1 complexes. Figure 1A illustrates adhesion in the absence of foreign-peptide-MHC complexes and at a binding energy of TCR/self-peptide-MHC complexes at which close-contact zones are not stable. The adhesion is then mediated only by LFA-1/ICAM-1 complexes (grey dots). In Figure 1B, the addition of just three foreignpeptide-MHC complexes with larger binding energy to TCRs leads to a close-contact zone that is cooperatively stabilized by few TCR/foreign-peptide-MHC complexes (black dots) and many TCR/self-peptide-MHC complexes (light grey dots). We systematically varied the binding energies of the TCR/self-peptide-MHC and TCR/foreign-peptide-MHC complexes and find that the cooperative stabilization of close-contact zones occurs selectively at a rather sharp threshold value of the TCR/foreign-peptide-MHC binding energy. in the presence of three foreign-peptide MHCs with binding energy U f = 12 k B T to TCRs. In (A), the binding energy U s = 5.9 k B T of the 270 self-peptide-MHCs is not sufficient to stabilize a close-contact zone of the adhering membranes. The adhesion is therefore mediated by LFA-1/ICAM-1 complexes (grey dots) with a concentration of about 100/µm 2 . The close-contact zone in (B) is cooperatively stabilized by 3 TCR/foreign-petide-MHC complexes (black dots) and many TCR/self-peptide-MHC complexes (light grey dots).

Adhesion Scenario with a Single Type of Peptide-MHC Complexes
We first consider an adhesion scenario in which TCRs can only bind to one type of peptide-MHC complexes. This scenario corresponds to T-cell adhesion on supported membranes that contain one type of peptide-MHCs and ICAM-1 [19][20][21]. In our model, the two adhering membranes are discretized into apposing patches that can contain single proteins. The proteins diffuse along the membranes by hopping from patch to patch, and bind to proteins at apposing membrane patches if the separation of the patches is within 15 ± 0.5 nm for TCR/MHC complexes and within 40 ± 0.5 nm for LFA-1/ICAM-1 complexes. The membrane bending energy associated with variations in the membrane separation depends on the effective bending rigidity κ = κ 1 κ 2 /(κ 1 + κ 2 ) of the two membranes with rigidities κ 1 and κ 2 [22,23]. We used the value κ = 20 k B T in accordance with typical values of the bending rigidities of lipid membranes [24,25] and plasma membranes [26,27] between 10 and 40 k B T. Our membranes consist of 100 × 100 patches with a projected area of 15 × 15 nm 2 and, thus, have a total projected area of 1.5 × 1.5 µm 2 . In the adhesion scenario with one type of peptide-MHC complexes, the T-cell membrane contains 270 TCR and 270 LFA-1 proteins, and the apposing membrane contains 270 peptide-MHC and 270 ICAM-1 proteins. The total concentration of all four protein species is therefore 120/µm 2 . We adjusted the binding energy of LFA-1/ICAM-1 complexes to 9.5 k B T, which leads to a concentration of the complexes of about 100/µm 2 [20] for small numbers of TCR/peptide-MHC complexes, and systematically varied the binding energy U of the TCR/peptide-MHC complexes. For each value of U, we ran six Monte Carlo (MC) simulations with a length of 2 × 10 8 t o where t o is the time associated with a MC step. In a MC step, we attempt to shift the separation of each pair of apposing membrane patches and to translate each protein and each pair of apposing binding partners to a nearest-neighbor patch along the membrane in independent substeps. To sample the equilibrium adhesion behavior, we discarded the initial 4 × 10 7 MC steps of the MC simulations during which the adhering membranes relax into equilibrium from different initial conformations (see Methods for details). Figure 2A shows how the average number of TCR/peptide-MHC complexes depends on the binding energy U of the complexes. The number of TCR/peptide-MHC com-plexes increases strongly at a binding energy U of about 6.0 k B T at which a close-contact zone begins to be stabilized by the TCR/peptide-MHC complexes. At binding energies U ≥ 6.5 k B T, the probability for such a close-contact zone is 1 (see Figure 2B), which means that a close-contact zone of TCR/peptide-MHC complexes is continuously present in the equilibrated simulations. The lifetime of the close-contact zone therefore becomes equal to the length T o = 1.6 × 10 8 t o of the equilibrated trajectory parts over which these quantities were measured (see Figure 2D). The probability and lifetime of close-contact zones were calculated from simulation conformations at intervals of 2 × 10 5 t o in the equilibrated trajectory parts. We define a close-contact event as a contiguous sequence of conformations (i) that contains pairs of apposing membrane patches with separation less than 20 nm in each conformation and (ii) in which TCR/peptide-MHC complexes are present in at least one conformation in the sequence. The probability of close-contact zones is the fraction of conformations that are part of close-contact events. This definition of close-contact zones takes into account that the instantaneous number of TCR/peptide-MHC complexes in a small close-contact zone with few complexes can briefly drop to 0 because of fluctuations in the number of complexes from binding and unbinding events. The average area of the close-contact zones grows for binding energies U ≥ 6.0 k B T at which the number of TCR/peptide-MHC increased (see Figure 2C).

Adhesion Scenarios with Two Types of Peptide-MHC Complexes
We now consider adhesion scenarios in which TCRs can bind to two types of peptide-MHCs with different binding energies: to "self-peptide-MHCs" with binding energy U s , or to "foreign-peptide-MHCs" with larger binding energy U f . This situation corresponds to T-cell adhesion on supported membranes that contain self-peptide-MHCs, agonist foreign-peptide-MHCs, and ICAM-1 [16], and mimicks the interplay of self-and foreignpeptide-MHC complexes in the adhesion of T cells to antigen-presenting cells. In our simulation systems, we either have three foreign-peptide-MHCs and 267 self-peptide-MHCs, or one foreign-peptide-MHC and 269 self-peptide-MHCs. The concentration of foreign-peptide-MHCs is thus 1.3/µm 2 or 0.4/µm 2 , respectively, for the membrane area 1.5 × 1.5 µm 2 of our simulations. As before, the numbers of TCRs, LFA-1 proteins, and ICAM-1 proteins are 270 each, and the binding energy of LFA-1/ICAM-1 complexes is 9.5 k B T. We assume that the self-peptide-MHCs alone do not stabilize a close-contact zone and chose the three values U s = 4.0, 5.5, and 5.9 k B T for the binding energy of TCR/selfpeptide-MHC complexes, which are below the threshold value of about 6.0 k B T for stable contact zones with one type of peptide-MHCs (see Figure 2).  Figure 3 shows how the probability and lifetime of close-contact zones depend on the binding energy U f of the TCR/foreign-peptide-MHC complexes. In our simulations with three foreign-peptide-MHCs, the lifetime of close-contact zones increases rather strongly at threshold values of U f that depend on the binding energy U s of the TCR/selfpeptide-MHC complexes. For U s = 4.0 k B T, the lifetime of the close-contacts zones increases from 0.023 ± 0.005 T o at U f = 12 k B T to 0.30 ± 0.14 T o at U f = 13 k B T and, thus, by a factor of 13 ± 7 with an increase of 1 k B T in U f . For U s = 5.5 k B T, the lifetime increases by a factor of 10 ± 3 from 0.012 ± 0.001 These increases in the lifetimes of close-contact zones by a factor of about 10 for an increase of 1 k B T in the binding energy U f for the three foreign-peptide-MHCs are significantly larger than the increases in the lifetimes of the individual complexes. In our simulations, the lifetimes of TCR/peptide-MHC complexes is proportional to exp[U/k B T], irrespective of the stability of the closecontact zones in which these complexes form (see Figure 4B), and thus increases by a factor of 2.7 with an increase of 1 k B T in the binding energy U. For large values of U f , the close-contact zones contain three TCR/foreign-peptide-MHC complexes and on average about 21 TCR/self-peptide-MHC complexes for U s = 5.9 k B T, about five TCR/selfpeptide-MHC complexes for U s = 5.5 k B T, and on average about 0.5 TCR/self-peptide-MHC complexes for U s = 4.0 k B T (see Figures 1B, 4A, and 5A,B). The close-contact zones thus are jointly stabilized by TCR/foreign-peptide-MHC and TCR/self-peptide-MHC complexes for U s = 5.9 k B T and 5.5 k B T, and predominantly by the TCR/foreign-peptide-MHC complexes for U s = 4.0 k B T. The threshold value of U f at which the lifetime of the close-contact zones increases rather strongly is reduced by about 2.5 to 3 k B T for an increase of U s from 4.0 to 5.9 k B T (see Figure 3B). In our simulations with one foreign-peptide-MHC complex, the lifetime of closecontact zones increases by about a factor of 3 with an increase of 1 k B T in U f in the range from U f = 12 k B T to 15 k B T, which was comparable to the increase in the lifetime of the TCR/foreign-peptide-MHC complex with U f . However, the lifetimes of the close-contact zones is about a factor 40 larger than the lifetime of the TCR/foreign-peptide-MHC complex in this range of U f values, which reflects the cooperative stabilization of close-contact zones by the TCR/self-peptide-MHC complexes with binding energy U s = 5.9 k B T in our simulations. For large values U f ≥ 15 k B T, the close-contact zones contain between 10 and 12 TCR/self-peptide-MHC complexes, besides the single TCR/foreign-peptide-MHC complex in these simulations (see Figures 4A and 5C).

Discussion
Our simulation results indicate that the cooperative stabilization of close-contact zones is sensitive to few TCR/foreign-peptide-MHC complexes. In our simulations with three foreign-peptide-MHCs, a clear stabilization of close-contact zones occurs within rather narrow windows of about 2 k B T in the binding energy U f of the TCR/foreign-peptide-MHC complexes (see Figure 3). These narrow 2 k B T windows imply selectivity between TCR/peptide-MHC complexes at both sides of the windows and, thus, between peptide-MHC complexes that differ by only 2 k B T in their binding energies. In our adhesion scenario with 3 foreign-peptide-MHCs and the binding energy U s = 5.5 k B T of TCR/self-peptide-MHC complexes, for example, the probability and lifetime of close-contact zones change significantly in the 2 k B T window from about U f = 10.5 k B T to 12.5 k B T. TCR/foreignpeptide-MHC complexes with a binding energy U f ≥ 12.5 k B T lead to highly probable and long-lived close-contact zones in this scenario, in contrast to complexes with binding energy U f ≤ 10.5 k B T. To estimate physical time-scales for this adhesion scenario, let us assume that a binding energy U f = 12.5 k B T corresponds to a TCR/foreign-MHCpeptide complex with a typical lifetime of 1 s [21,28]. According to the regression line for the lifetime TCR/MHC-peptide complexes shown in Figure 4B, the time step t o of our MC simulations then corresponds to a physical time of 1 µs, and the average lifetime of close-contact zones of about 0.3 T o 0.5 × 10 8 t o at U f = 12.5 k B T corresponds to 50 s. In contrast, the average lifetime of close-contact zones at U f = 10.5 k B T is then only 1 s. In addition, the average probability of close-contact zones at U f = 10.5 k B T is about 6% and, thus, signicantly smaller than the probability of 89% at U f = 12.5 k B T. These changes in the probability and lifetime of close-contact zones are large compared to the change by a factor of about seven in the lifetime of individual TCR/MHC-peptide complexes for an increase of 2 k B T in the binding energy. In the adhesion scenario with one foreign-peptide-MHC, a comparable increase in the probability of the close-contact zones occurs within a wider window of 4 k B T from about U f = 11 k B T to U f = 15 k B T (see Figure 3A).
In our adhesion scenario with three foreign-peptide-MHCs, the window of U f values in which the stabilization of the close-contact zones occurs depends on the binding energy U s of TCR/self-peptide-MHC complexes. At the binding energy U s = 4.0 k B T, closecontact zones are predominantly stabilized by TCR/foreign-peptide-MHC complexes alone. TCR/self-peptide-MHC complexes only form with low probability and, thus, do not contribute significantly to the stabilization. At the binding energies U s = 5.5 k B T and U s = 5.9 k B T, the close-contact zones are jointly stabilized by TCR/foreign-peptide-MHC and TCR/self-peptide-MHC complexes, and the stabilization window is shifted to smaller values of U f . The joint stabilization of close-contact zones by TCR/foreign-peptide-MHC and TCR/self-peptide-MHC complexes is in line with experimental findings that self-peptide-MHCs increase and facilitate the response of T cells to agonist foreign-peptide-MHCs [16,17]. The cooperativity of self-peptide-MHCs and foreign-peptide-MHCs has been suggested to result from positive selection of naive T cells with TCRs that interact with self-peptide-MHCs on antigen-presenting cells in the thymus [17]. This positive selection is balanced by negative selection to ensure that T cells are not activated by self-peptide-MHCs alone [29].
The membrane separation in closed-contact zones varies between about 10 nm and 20 nm in our simulations (see Figures 1B and 5). Proteins with extracellular protrusions larger than 25 nm such as CD45 therefore are rather clearly excluded from these closecontact zones as suggested in the kinetic-segregation model of T-cell activation. In this model, the size-based segregation of the inhibitory tyrosine phosphatase CD45 from TCR complexes in close-contact zones triggers T-cell signaling and activation [30][31][32][33]. Our simulation results can also be seen to connect to the serial-engagement model that suggests that foreign-peptide-MHC complexes bind to many different TCRs [34,35]. The lifetimes of close-contact zones in our simulations are much larger than the lifetime of the individual TCR/foreign-peptide-MHC complexes that stabilize the close-contact zones, which implies many binding and unbinding events of foreign-peptide-MHC complexes during the lifetime of a close-contact zone.
While the lifetimes of TCR/peptide-MHC complexes depend only on the binding energy U in our simulations, the two-dimensional binding constant K 2D is also affected by the distribution P(l) of local membrane separations. The two-dimensional binding constant can be calculated as K 2D = k 2D (l)P(l)dl where k 2D (l) is the binding constant as a function of the separation l [36]. In our model, k 2D (l) is equal to a 2 exp[U/k B T] for separations l within the binding range 15 ± 0.5 nm of TCR/peptide-MHC complexes, where a 2 = 15 × 15 nm 2 is the area of a membrane patch, and is equal to 0 for separations l outside this binding range [37]. In large close-contact zones of our simulations, about 20% of the membrane patches are within the binding range of TCR/peptide-MHC complexes. The two-dimensional binding constant of these complexes therefore is , which is about 10 µm 2 for the binding energy U = 12.5 k B T of the example above. Within the domains of LFA-1/ICAM-1 complexes, the binding constant K 2D for TCR/peptide-MHC complexes is 0 simply because the distribution P(l) of local membrane separations within these domains does not allow for the binding of TCR/peptide-MHC complexes.
TCR/peptide-MHC and LFA-1/ICAM-1 complexes tend to segregate in our model because the membranes need to curve to compensate the length mismatch [38]. Experiments in the last years highlight the importance of size and length in the segregation of complexes and proteins in membrane adhesion [39][40][41][42][43]. In particular the clustering of the initially randomly distributed TCRs [44] during T-cell adhesion has been a focus in understanding T-cell activation [45][46][47][48][49][50]. Our previous simulations and calculations indicate that the curvature-mediated segregation into domains of LFA-1/ICAM-1 complexes and close-contact zones of TCR/peptide-MHC complexes occurs for concentrations [LFA-1/ICAM-1] > c k B T/κ(∆l) 2 (1) of LFA-1/ICAM-1 complexes with length difference ∆l to TCR/peptide-MHC complexes and the numerical prefactor c = 0.65 ± 0.15 [22,51,52]. For the κ = 20 k B T and ∆l = 25 nm as in our model, the critical concentration of segregation at the right-hand side of this inequality is about 50/µm 2 . The concentration [LFA-1/ICAM-1] 100/µm 2 in our model is clearly larger than this critical concentration, in agreement with the concentrations of LFA-1/ICAM-1 complexes measured in the immunological synapse of T cells on supported membranes [20]. In the adhesion of T cells to antigen-presenting cells, other complexes with comparable length to TCR/peptide-MHC complexes such as complexes of CD2 [53], CD80/CD28 complexes [54], and complexes of the co-receptors CD4 or CD8 with MHC may contribute to the segregation and the stabilization of close-contact zones. CD2 has been reported to enhance the response of T cells to antigens [53]. At sufficiently high concentrations, CD2 complexes more recently have been found to form peripheral domains in the immunological synapse of T cells on supported membranes [55]. In our T-cell adhesion model, other complexes with comparable length to TCR/peptide-MHC complexes can be seen to affect the stabilization of close-contact zones analogously to TCR/self-peptide-MHC complexes.
High-resolution microscopy of T-cell adhesion shows that close-contact zones form at the tips of microvilli that protrude from T cells during the scanning of antigen-presenting cells [19]. These tips have a width of about 500 nm, which is larger or comparable to the width of the close-contact zones in our simulations. Close-contact zones at the microvilli tips stabilized by TCR/foreign-peptide-MHC remain after the drug-induced disassembly of the actin cytoskeleton of the T cells, which indicates that the stabilization of the closecontact zones observed in the experiments is independent of cytoskeletal forces. With intact cytoskeleton, T cells exert forces that likely play a role in bringing the cell surfaces to distances of about 40 nm, at which the LFA-1/ICAM-1 can form, against the repulsion of glycocalyx components longer than 40 nm [18]. Our simulations indicate that the nucleation of close-contact zones within the domains of LFA-1/ICAM-1 is rather fast and, thus, does not require force. However, transversal forces on TCR/foreign-peptide-MHC complexes observed in recent experiments [56], which are presumably induced by lateral motion of microvilli, may contribute to T-cell signaling and activation [28,[57][58][59][60][61].

Methods
In our computational model of T-cell adhesion, the two adhering membrane segments are discretized into 100 × 100 apposing pairs of membrane patches [62]. The patches at opposing boundaries of the membrane segments are connected by periodic boundary conditions. Each membrane patch can contain a single protein. Our MC simulations consist of MC moves in which we attempt (1) to shift the separation of a pair of apposing membrane patches, (2) to translate a single protein to a nearest-neighbor patch, and (3) to translate a pair of apposing partner proteins to a nearest-neighbor pair of apposing patches. In the MC moves (1), a pair i of apposing patches is selected randomly, and the local separation l i of the patches is attempted to be shifted to l i + δl where δl is a random length that is distributed uniformly between −0.5 nm and 0.5 nm. In the MC moves (2), a single protein is randomly selected and attempted to be shifted to one of the four nearest-neighbor patches in the discretized membranes, provided this patch is not occupied by another protein. In the MC moves (3), a pair of apposing partner proteins, i.e., a pair of LFA-1 and ICAM-1 proteins or a pair of TCR and peptide-MHC proteins located in two apposing membrane patches, is selected randomly and independently of the separation of the patches, and is attempted to be shifted to a nearest-neighbor pair of apposing, unoccupied membrane patches. All three types of MC moves can lead to the binding or unbinding of protein complexes. The MC moves (2) lead to the diffusion of single proteins, and the MC moves (3) to the diffusion of bound protein complexes. To correctly capture the lifetimes of bound complexes, unrealistic MC moves of type (2) in which a bound protein would directly hop into a new complex at a neighboring site are excluded.
The MC moves are accepted or rejected with probabilities that depend on the energy change ∆E associated with the move. We use the standard Metropolis criterion in which MC moves are accepted with probability 1 for ∆E < 0, i.e., if the moves decrease the overall energy, and with probability exp[−∆E/k B T] for ∆E > 0. The energy change of MC moves of type (1) associated with changes in the bending energy of the membrane is calculated from the discretized effective bending energy of the two membranes 1 and 2 with effective bending rigidity κ = κ 1 κ 2 /(κ 1 + κ 2 ) and the discretized Laplacian ∆ d l i = l i1 + l i2 + l i3 + l i4 − 4l i [22,23]. Here, l i is the membrane separation of the apposing pair i of membrane patches, and l i1 to l i4 are the membrane separations at the four nearest-neighbor pairs of patches around pair i. In our model, the linear size a of the membrane patches is a = 15 nm as in our previous model for the cooperative binding of CD47 in the adhesion of giant plasma membrane vesicles [27]. The energy decrease and increase associated with binding and unbinding events, respectively, is simply determined from the binding energy of the complexes. In our model, an apposing pair of TCR and peptide-MHC proteins is bound if the separation l i of the apposing pair i of membrane patches, in which the proteins are located, is within 15 ± 0.5 nm. The binding energy of the TCR complexes is U f for complexes with foreign-peptide-MHCs proteins and U s for complexes with self-peptide-MHCs. An apposing pair of LFA-1 and ICAM-1 is bound with binding energy 9.5 k B T if the separation of the membrane patches is within 40 ± 0.5 nm. A single MC step consists of 100 × 100 attempted moves of type (1), N attempted moves of type (2), where N is the total number of proteins in both membranes, and M attempted moves of type (3), where M is the instantaneous number of apposing partner proteins. A single MC trajectory consists of of 2 × 10 8 MC steps. The dwell times of TCR/MHC complexes as well as the numbers of binding and unbinding events were computed on the fly during the second halves of the trajectories, i.e., from 10 8 MC moves. For each set of parameter values in our adhesion scenarios, we ran six MC simulations with different initial conformations. In three of the six MC runs, the separations l i of the apposing membrane patches were initially distributed randomly in the intervals from 14.5 to 40.5 nm, from 13.5 to 41.5 nm, and from 12.5 to 42.5 nm, respectively. With these initial distributions of membrane separations, both TCR/peptide-MHC complexes and the LFA-1/ICAM-1 complexes were formed at the beginning of the MC trajectories. In the three other of the six MC runs, the initial membrane separations l i were distributed randomly in the intervals from 39.5 to 40.5 nm, from 38.5 to 41.5 nm, and from 37.5 to 42.5 nm, respectively. In these MC runs, the membrane adhesion is initially mediated only by the LFA-1/ICAM-1 complexes. In all MC runs, the proteins were initially distributed uniformly within the membranes. The MC simulations relax into equilibrium from these different initial conformations within the first 4 × 10 7 MC steps of the MC simulations. We have therefore discarded these MC steps in our analysis of the equilibrium adhesion behavior.
Our three-dimensional, computational model is related to previous models that have been used to investigate the formation and temporal evolution of domain patterns in the immunological synapse of T cells [63][64][65][66]. A difference is the smaller size of the membrane patches in the simulations presented here, which allows for a higher resolution of the membrane shape and fluctuations within and between the close-contact zones of TCR/peptide-MHC complexes. In other models of the pattern formation, the proteins have been described with continuous distributions, and not as single molecules [67][68][69][70].

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