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A sulfur-aromatic gate latch is essential for opening of the Orai1 channel pore

Sulfur-aromatic interactions occur in the majority of protein structures, yet little is known about their functional roles in ion channels. Here, we describe a novel molecular motif, the M101 gate latch, which is essential for gating of human Orai1 channels via its sulfur-aromatic interactions with the F99 hydrophobic gate. Molecular dynamics simulations of different Orai variants reveal that the gate latch is mostly engaged in open but not closed channels. In experimental studies, we use metal-ion bridges to show that promoting an M101-F99 bond directly activates Orai1, whereas disrupting this interaction triggers channel closure. Mutational analysis demonstrates that the methionine residue at this position has a unique combination of length, flexibility, and chemistry to act as an effective latch for the phenylalanine gate. Because sulfur-aromatic interactions provide additional stabilization compared to purely hydrophobic interactions, we infer that the six M101-F99 pairs in the hexameric channel provide a substantial energetic contribution to Orai1 activation.


Introduction
The opening and closing of ion channels constitute an important means by which extracellular signals are translated into the activation of specific intracellular signaling cascades. Critical to this process is tight control of the channel gate, which forms an ion-proof barrier at rest and permits ion conduction when activated. In this study, we describe an essential molecular motif involving a sulfur-aromatic interaction that plays a critical role in the gating of Ca 2+ release-activated Ca 2+ (CRAC) channels formed by Orai1. CRAC channels are activated by the engagement of cell surface receptors that activate phospholipase C through G-proteins or tyrosine kinase cascades to cleave phosphatidylinositol 4,5-bisphosphate (PIP 2 ) and produce soluble inositol 1,4,5-trisphosphate (IP 3 ). The ensuing depletion of endoplasmic reticulum (ER) Ca 2+ stores activates the ER Ca 2+ sensors, STIM1 and STIM2, which translocate to the junctional ER to interact with and activate CRAC channels encoded by the Orai1-3 proteins. During this process, STIM1, which is thought to be compactly folded at rest, adopts an extended multimeric conformation to expose the Orai1-activating domain (CAD), making it available for binding to Orai1 channels at ER-plasma membrane junctions (Prakriya and Lewis, their emergence as drug targets for inflammatory diseases (Stauderman, 2018) and spurred strong interest in elucidating the molecular underpinnings of the gating mechanism (Yeung et al., 2020).
Crystal structures of the highly homologous Drosophila melanogaster Orai (dOrai) and recent concatemer-based studies have shown that Orai channels are formed by six subunits (Cai et al., 2016;Hou et al., 2012;Liu et al., 2019;Yen et al., 2016). Each of these protomers has four transmembrane domains (TMs) which are together arranged in three concentric layers, with TMs 2-4 surrounding a narrow pore lined by six TM1 helices (Figure 1; Hou et al., 2012). Previous studies support a model wherein STIM1 binding to the cytosolic surface of Orai1 initiates a conformational wave throughout the protein (Yeung et al., 2020;Zhou et al., 2019), ultimately culminating in rotation of the pore helices to activate a hydrophobic gate in the outer pore . Together with a modest dilation of the outer pore (Yeung et al., 2018), the displacement of F99 residues away from the pore axis lowers the overall energetic penalty in this region to permit pore hydration and ion conduction ( Figure 1A; Yamashita et al., 2017). Although the hydrophobic gate also involves the neighboring residue V102 located one turn above (McNally et al., 2012;Yeung et al., 2017), and may even extend to L95 located below, for simplicity, we will refer to the hydrophobic gate as the 'F99 gate' because F99 is the residue whose movement has been shown to directly contribute to pore opening .
The nature of the proximal signal that facilitates displacement of the F99 gate away from the pore axis during channel activation is not known. However, one crucial relay along the gating pathway to the pore is a cluster of tightly packed hydrophobic residues at the interface between the pore helices and its surrounding TM2/3 ring (Yeung et al., 2018). In the crystal structure of dOrai,  (Yeung et al., 2018), which moves F171 (hOrai1 F99) away from the pore axis and decreases the free energy barrier in the hydrophobic stretch for ion permeation. For simplicity, TMs 2-4 are not shown. (B) A cluster of hydrophobic residues (shown as gray spheres) between the TM1 pore helices and the TM3 segment. The selectivity filter E178 (hOrai1 E106, orange) and hydrophobic gate residues V174 (hOrai1 V102, purple) and F171 (hOrai1 F99, green) in the pore are also shown. Four TM1 helices and two TM3 helices are shown for clarity. (C) Position of M101 within the hydrophobic cluster. F171 (hOrai1 F99) is also shown within the context of the hexameric channel and relative to the hydrophobic cluster residues. Residues M173 (hOrai1 M101) and F259 (hOrai1 F187) are depicted as blue and red spheres, respectively. The F171 gate is shown as green sticks. hOrai1 numbering is shown in parentheses.
this hydrophobic cluster at the TM1-TM3 interface is formed by the TM1 residues with dOrai residue numbering L168, M173, M176 and TM3 residues F259, I263, L266 (equivalent to human Orai1 L96, M101, M104, F187, V191, L194) ( Figure 1B,C). We previously showed that mutations that lower the hydrophobicity or reduce the side-chain size of these residues lead to loss-of-function channel phenotypes, suggesting that the interwoven hydrophobic interactions in this region function as a rigid relay during allosteric gating by STIM1 (Yeung et al., 2018). In the current study, we identify an additional novel function for one of these residues, M101 ( Figure 1C), whose robust sulfuraromatic interaction with the F99 channel gate actively stabilizes the pore in its open configuration.

Molecular dynamics simulations reveal sulfur-aromatic interactions involving the hydrophobic gate in activated states
To better understand the molecular mechanisms underlying F99 gate opening, we began our studies by carefully mapping the movements of F99 in molecular dynamics (MD) simulations of gain-of-function (GOF) and loss-of-function (LOF) dOrai mutants ( Figure 2). Although there are now several available structures of activating mutants (Hou et al., 2018;Liu et al., 2019), we performed simulations using the 3.35 Å crystal structure of Drosophila melanogaster Orai ([PDB ID:4HKR]; Hou et al., 2012) because it remains the most complete, highest-resolution structure and has been utilized in previous MD studies (Bonhenry et al., 2019;Dong et al., 2019). Further, given the high sequence identity between dOrai and human Orai1 (hOrai1) within the transmembrane domains, channel phenotypes identified using MD simulations in dOrai are likely to be translatable to electrophysiological results in hOrai1.
For our simulations, we took advantage of mutations at a well-studied gating locus, H134 on TM2 (equivalent to dOrai H206), to model inactive, partially active, or fully active channels. The histidine side-chain of H134 faces the non-pore-lining surface of TM1 and has been suggested to stabilize the closed channel state by acting as a steric brake at the TM1-TM2/3 ring interface (Yeung et al., 2018;Figure 2-figure supplement 1A). Previous studies have described several interesting GOF or LOF mutations at hOrai1 H134 that either inhibit or constitutively activate Orai1 gating (Frischauf et al., 2017;Yeung et al., 2018). Compared to WT channels, the LOF mutant hOrai1 H134Y (dOrai H206Y) conducts small, non-selective Orai1 currents when co-expressed with STIM1, reflecting a defect in STIM1-mediated gating (Yeung et al., 2018). A second mutant, hOrai1 H134Q (dOrai H206Q), is modestly active at rest but can be further gated by STIM1. By contrast, a third mutant, hOrai1 H134C (dOrai H206C), is one of the most strongly active variants, displaying similar properties as STIM1-gated channels even without STIM1, including inward-rectifying, Ca 2+ -selective currents and displacement of the F99 gate (Bulla et al., 2019;Frischauf et al., 2017;Yeung et al., 2018). The channel activities of these mutants, as measured by electrophysiology (Figure 2-figure supplement 1B), correlate well with metrics such as the extent of pore helix rotation, outer pore dilation, and pore hydration observed in MD simulations (Figure 2-figure supplement 2B; [see also Yeung et al., 2018]).
Within these dOrai H206 simulations, we looked for conformational changes in the TM1-TM3 hydrophobic cluster that correlated with pore opening for potential clues on the molecular mechanism of channel gate opening. The time trajectories of dOrai across all variants showed that most of the residues in the hydrophobic stack display spatial fluctuations of small amplitude, consistent with their role as a rigid relay from TM3 to TM1. However, intriguingly, in simulations of the active variants H206Q/C (equivalent to hOrai1 H134Q/C), the M173 (hOrai1 M101) side-chain was uniquely flexible and reversibly sampled rotamers that deviated from the crystal structure ( Figure 2C,D, . We observed that the flexibility of M173 allowed it to interact with the hydrophobic gate residue, F171 (hOrai1 F99) of neighboring subunits ( Figure 2C,D). Specifically, the M173-F171 distance often reached 4-6 Å ( Figure 2E), sufficiently close for direct contact between the two sidechains. This finding is notable as sulfur-aromatic interactions involving Met and Phe residues are known to play distinctive roles in protein function, often by stabilizing protein structures (Valley et al., 2012;Weber and Warren, 2019). Because the M173-F171 interaction was preferentially seen only in the activating mutants and not in WT or LOF mutants ( , respectively. Distances were measured from the sulfur of the methionine and the center of mass of the phenylalanine ring. The mean and standard error of mean of M173-F171 distances over simulation repeats are 7.4 ± 0.1 Å for WT, 6.4 ± 0.2 Å for H206C, 6.6 ± 0.1 Å for H206Q, and 7.9 ± 0.1 Å for H206Y. Compared to closed WT and H206Y channels, constitutively active dOrai mutants H206Q/C show a greater proportion of M173-F171 interactions within the sulfur-aromatic interaction distance of 3-7 Å . By contrast, M173-    videos 1 and 2), we considered the possibility that this interaction may promote the opening of the channel gate in the activating mutants.
To investigate this hypothesis, we examined how interactions between M173 and F171 correlated with metrics of channel activity in WT, H206Y, H206Q, and H206C channels ( Figure 2G-K). Previous studies have concluded that sulfur-aromatic interactions occur at distances less than 7 Å , with a peak distance of » 5 Å (Gó mez- Tamayo et al., 2016;Valley et al., 2012). Therefore, we quantified the interactions between M173 (hOrai1 M101) with the hydrophobic gate F171 (hOrai1 F99) as well as with its normal 'resting state' partner in the hydrophobic stack, F259 (hOrai1 F187 in TM3), by measuring distances between the sulfur atom on M173 and the center of mass of the aromatic rings of F171 and F259 ( Figure 2E,F). This analysis showed that the distance between M173 and F259 oscillated between 4 and 7 Å , with an average value of 5.46 ± 0.04 Å (WT), 5.38 ± 0.05 Å (H206Y), 5.65 ± 0.06 Å (H206Q), and 5.65 ± 0.04 Å (H206C). These values indicate that the interaction of the M173 side-chain with F259 within the TM1-TM3 hydrophobic stack is relatively stable and maintained across open and closed variants ( Figure 2F).
By contrast, the distance between M173 and F171 showed much larger variability and depended on channel activity. In closed WT and LOF H206Y (hOrai1 H134Y) channels, there was a broad distribution of F171-M173 distances from 5 Å to 10 Å ( Figure 2A,B,E). In the activated channels H206Q and H206C, however, the distribution was markedly shifted toward shorter distances, with a peak between 4 and 7 Å , centered at 6.6 ± 0.1 Å for H206Q and 6.4 ± 0.2 Å for H206C ( Figure 2C-E). These distances imply the presence of a stable sulfur-aromatic interaction between M173 and F171 in the open variants. Importantly, the M173-F171 interaction distance was correlated with several metrics of channel activation, including pore helix rotation, pore hydration, and pore diameter across all dOrai variants ( Figure 2G-K), with shorter interaction distances most strongly associated with F171 rotation. The increased magnitude of counterclockwise angular rotations of F171 C a in the activated mutants also correlated well with those of M173, suggesting that as the channel opens, M173 rotates along with F171 to enable it to contact F171 on the adjacent helix ( While the Met-Phe interactions described above may be mediated by side-chain fluctuations, rigid body motions of the TM1 backbone may also contribute to these interactions. To assess this possibility, we quantified the distances between the C b of M173 and the center of the F171 and F259 rings in the different H206 mutants (Figure 2-figure supplement 2E,F). Compared to the sulfur atom distances, C b measurements are likely to be driven more by pore helix rotation because the M173 C b is closer to the center of the TM1 helix. In WT and H206Y channels, M173 is predominantly facing TM3 as part of the TM1-TM3 hydrophobic clamp, so that C b is closer to F259 and farther away from F171. However, in the activated states of the H206Q/C channels, the TM1 rotation angle distribution displayed an additional peak corresponding to distances closer to F171 and farther from F259 ( . This result suggests that the TM1 helix is sufficiently mobile to display conformational alterations at the M173 C b position between open and closed states. By contrast, as already indicated above, no differences were seen in the distance measured from the sulfur atom to the F259 ring ( Figure 2F), indicating that the M173 side-chain exhibits sufficient flexibility and that the sulfur atom is intrinsically drawn toward the F259 ring.

Enhancing the M101-F99 interaction boosts F99C/M101C Orai1 channel activity
The finding that M173-F171 (hOrai1 M101-F99) interactions are augmented in MD simulations of active channel states led us to consider whether artificially forcing an interaction between M101 and F99 in hOrai1 via a metal-ion bridge can directly activate the channel. Metal-ion bridges in double cysteine mutants have been exploited in many studies of ion channel gating to probe the conformational changes underlying gating and to stabilize channels in specific states (Holmgren et al., 1996;Li et al., 2010;Loussouarn et al., 2001;McNally et al., 2012;Puljung and Zagotta, 2011;Rulísek and Vondrásek, 1998). We therefore introduced cysteines at F99 and M101 in hOrai1 and examined the effects of applying the thiol-reactive divalent ion Cd 2+ in F99C/M101C Orai1 channels overexpressed in HEK293-H cells without STIM1 ( Figure 3A).
F99C/M101C channels are partially open at baseline, producing non-selective CRAC currents (V rev = À5.4 ± 2.7 mV) in line with previous results indicating that the F99C mutation disrupts the hydrophobic barrier in the pore . Strikingly, Cd 2+ administration dramatically enhanced this F99C/M101C current with a slow time course over tens of seconds ( Figure 3C,E,F). Over the 40 s application of 5 mM Cd 2+ , the non-selective F99C/M101C Orai1 current increased 12fold over the baseline current ( Figure 3C,D). Washout of Cd 2+ by 20 mM Ca 2+ Ringer's solution caused an additional rapid increase in the current ( Figure 3C,E,F). Previous reports have shown that application of Cd 2+ to the single F99C mutant results in strong blockade of Orai1 currents when F99C residues are oriented in a pore-facing configuration (McNally et al., 2009;Yamashita et al., 2017). Thus, we reasoned that the rapid current increase in the F99C/M101C double mutant following washout of Cd 2+ arises from the removal of Cd 2+ block by the permeating Ca 2+ ions. The Cd 2+mediated potentiation was stable and could only be reversed by reducing agent bis(2-mercaptoethylsulfone) (BMS) ( Figure 3C,E,F), indicating that the trapping of Cd 2+ between the introduced cysteine residues is destabilized only by directly disrupting the coordinating thiol groups.
WT and single cysteine mutants F99C and M101C did not exhibit Cd 2+ -dependent current enhancement (McNally et al., 2009), indicating that cysteines at both positions are required for the potentiation effect. Further, when STIM1 was co-expressed, the extent of Cd 2+ -induced current potentiation was dramatically reduced ( Figure 3D). Because STIM1 stabilizes F99 is an activated state with F99 facing away from the pore and toward M101, we reasoned that the additional gating induced by a Cd 2+ bridge between F99C and M101C is diminished in the STIM1-bound state of Orai1. However, one caveat to this interpretation is that STIM1 does not activate the F99C/M101C channels strongly (I = À1.49 pA/pF at baseline versus À3.17 pA/pF following STIM1 binding). Thus, we cannot formally out that the smaller degree of STIM1-activated Cd 2+ potentiation of F99C/ M101C channels is due to unknown indirect effects such as stabilization of the channel in an intermediate state where the Cd 2+ -binding site is obscured. Nevertheless, the robust potentiation of F99C/ M101C activity in STIM1-free channels is strong indication of the importance of M101-F99 interaction for pore opening.
Increasing the Cd 2+ dose from 5 mM to 500 mM dramatically increased the extent of channel potentiation in F99C/M101C channels, up to 150 times the baseline amplitude at 300 mM Cd 2+ (- Figure 3E,G). However, even at 500 mM Cd 2+ potentiation did not reach saturation. Further increases could not be quantified because Cd 2+ precipitated out of the 20 mM Ca 2+ Ringer's solution at higher concentrations. In order to distinguish whether the Cd 2+ potentiation site is close to the pore or away from it, we varied the permeant ion concentration, reasoning that a site located in or close to the pore would be highly sensitive to the concentration of permeant ions. Specifically, current potentiation is expected to decline at higher concentrations of permeant Ca 2+ ions due to a knockoff effect of Cd 2+ by Ca 2+ ions. As predicted for a Ca 2+ -permeable channel, F99C/M101C channels conducted more baseline current when the external Ca 2+ concentration was raised from 20 to 110 mM Ca 2+ ( Figure 3F). However, when applied in the 110 mM Ca 2+ solution, Cd 2+ induced significantly less current potentiation than that in 20 mM Ca 2+ solution ( Figure 3F,G), indicating that raising the permeant ion concentration diminishes Cd 2+ -induced gating. Based on this result, we conclude that Ca 2+ flux in the pore competes with Cd 2+ binding at its potentiation site and thus the Cd 2+ binding site is located close to the pore where it is influenced by permeant ions.
To test whether the gating induced by Cd 2+ is also seen with other thiol-reactive probes, we tested the effects of Zn 2+ , a slightly smaller metal ion that, like Cd 2+ , can also coordinate with thiol groups (Yellen et al., 1994). Administration of Zn 2+ also elicited potentiation of Orai1 current (Figure 3-figure supplement 1), suggesting that the potentiation effect is not unique to Cd 2+ but arises due to bridging of F99C to M101C via a thiol-reactive divalent ion. These results are consistent with the hypothesis that the M101-F99 interaction stabilizes the open state.
Stabilizing the M101-F187 interaction promotes pore closure in M101C/F187C Orai1 channels If stabilizing a M101-F99 interaction augments channel activation, does facilitating the resting state interaction between M101 and F187 (as seen in the closed channel crystal structure) favor the closed state? We tested this idea using the hOrai1 M101C/F187C mutant. We have previously shown that Orai1 F187C is a Ca 2+ -selective, constitutively active mutant (Yeung et al., 2018). Similarly, the M101C/F187C double cysteine mutant was also constitutively active and highly Ca 2+ selective ( Figure 4B). Strikingly, when 5 mM Cd 2+ was applied to M101C/F187C, the current was almost  completely inhibited ( Figure 4B). This current decrease was uniform across the voltage ramp (V rev = 41.0 ± 6.3 mV without Cd 2+ and V rev = 35.8 ± 8.9 mV with 5 mM Cd 2+ ; p=0.65), which suggests that it arises from channel inhibition rather than pore block. In addition, the reversibility of the effect by BMS is consistent with that of a cysteine-mediated mechanism ( Figure 4B). The rapid Cd 2+ -induced inhibition was only seen in the double Cys mutants. Neither the single F187C nor double M101A/F187C and M101C/H134S mutants showed any effect with Cd 2+ (Figure 4C), indicating that cysteines are required at both F187 and M101 for inducing channel closure. In contrast to the strong dependence on the permeant ion concentration seen for the Cd 2+ -mediated potentiation of F99C/M101C channels, Cd 2+ -induced channel closure in the M101C/F187C mutant was largely insensitive to the permeant ion concentration. Specifically, Cd 2+ blockade in 110 mM Ca 2+ Ringer's was not notably different than that seen in 20 mM Ca 2+ solution ( Figure 4E,F), suggesting that the inhibition site is likely not in the pore. This conclusion is also supported by the strikingly different Cd 2+ sensitivities of Cd 2+ inhibition on M101C/F187C channels versus potentiation in F99C/M101C channels. Whereas inhibition in M101C/F187C channels quickly reached saturation with increasing Cd 2+ with an apparent K d of~0.3 mM ( Figure 4F), potentiation in the F99C/ M101C channels did not reach saturation even at 500 mM Cd 2+ ( Figure 3G). The latter effect is likely due to a knockoff effect of the permeant Ca 2+ ions on Cd 2+ occupancy at the potentiation site between F99C and M101C. Application of Zn 2+ also induced channel closure in M101C/F187C channels, suggesting that the inhibition effect is generalizable to other thiol-reactive metals (Figure 3figure supplement 1). We conclude that stabilizing the resting interaction between M101 and F187 evokes pore closure, presumably by releasing the F99 gate into its pore-facing configuration ( Figure 4A).

M101 is essential for STIM1-mediated Orai1 channel activation
If the sulfur-aromatic interaction is critical for gate opening, then mutations of M101 to other amino acids that cannot support sulfur-aromatic interactions should disrupt channel function. Consistent with this hypothesis, nearly every substitution that we tested, including M101G/A/S/T/C/V/L/I, yielded LOF channels that lost gating by STIM1 ( Figure 5A,B). Notably, mutations of M101 to Leu or Ile, which have comparable or even greater hydrophobicity as the native Met, also produced channels that could not be activated by STIM1 ( Figure 5A,B). The plasma membrane fluorescence of Orai1-YFP was similar across the mutants, indicating that reduced channel expression is not the cause of the smaller currents. Moreover, with the exception of some polar and charged substitutions (M101Q/N/D/K/E), no difference was seen in co-localization of the YFP-tagged Orai1 mutants with CFP-CAD nor in E-FRET between the two proteins ( Figure 5-figure supplement 1), indicating that loss of gating was not due to gross changes in the ability of the Orai1 variants to interact with STIM1. Introduction of the M101L mutation into the constitutively active H134S and constitutively conducting V102C mutants also attenuated currents in these mutants ( Figure 5-figure supplement  2). This latter result in V102C is not entirely unexpected since previous studies have indicated that the V102C mutant also shows greater spontaneous counter-clockwise fluctuations of the F99 gate region compared to WT channels, consistent with models showing that gate opening and pore hydration are intimately coupled in CRAC channels Yeung et al., 2018).
The one exception to the LOF effect induced by mutations at M101 was the Phe mutant, which surprisingly produced a GOF phenotype. M101F was not only normally gated by STIM1 ( Figure 5A), but was also modestly active and Ca 2+ -selective (V rev = 44.9 ± 5.7 mV) at rest in the absence of STIM1 ( Figure 5C). Interestingly, the M101F substitution was able to confer channel activity to LOF mutant H134W ( Figure 5-figure supplement 2) which cannot be gated by STIM1 (Yeung et al., 2018), suggesting that the effect of M101F is directly on the F99 gate. As will be discussed further below, we postulate that the constitutive activity of M101F likely arises from interactions of the introduced Phe side-chain with F99 and F187 created by the introduced aromatic ring at M101. Collectively, these M101 mutants demonstrate that hydrophobicity alone is not enough for channel function and reaffirm the conclusion that the sulfur-containing Met residue at position 101 mediates a specialized function in Orai1 gating in addition to its role in the hydrophobic cluster.
In contrast to the LOF Orai1 phenotypes of mutations at M101, mutation of F187 to smaller residues including Gly, Ala, Ser, and Cys produced GOF channels with inwardly rectifying CRAC channel-like current-voltage relationships. Large and hydrophobic F187 substitutions including Tyr and Trp, on the other hand, remained closed in the absence of STIM1 ( Figure 5-figure supplement 3).
Based on these results, we conclude that the large, hydrophobic side-chain of F187 on TM3 is required for stabilizing the closed state of the channel. However, because M101C channels are not constitutively open, we surmise that F187 may prevent spontaneous pore opening through mechanisms beyond its interaction with M101, potentially involving other residues of the TM1-TM3 hydrophobic stack. Without additional these interactions, the pore transitions into a Ca 2+ -selective state that is similar to the one evoked by STIM1 binding. Loss of the gate latch prevents channel opening by stabilizing the gate in its closed position The experimental results showing that loss of the sulfur-aromatic gate latch compromises channel gating led us to hypothesize that M101 LOF mutations stabilize the F99 gate in the closed pore-facing orientation, resulting in diminished pore hydration at the channel gate. To address this hypothesis, we performed MD simulations of dOrai M173L (LOF hOrai1 M101L) and dOrai M173F (GOF hOrai1 M101F) to investigate the effects of the mutations on pore hydration and orientation of the F99 gate. These simulations revealed that the M173L channel displayed significantly smaller spontaneous counter-clockwise pore helix rotations than the WT channel ( Figure 6D), with the angular position of F171 shifted by 10 ± 1˚for M173L channels and 17 ± 1˚for WT channels as measured with respect to the crystallographic orientation of the F171 side-chain in our coordinate system (30.6˚, [PDB ID:4HKR]; Hou et al., 2012). The decrease in pore helix rotation of M173L was accompanied by markedly lower hydration of the hydrophobic stretch of the pore ( Figure 6B). By contrast, M173F channels, which are modestly active in the absence of STIM1 (Figure 5C), showed a statistically significant increase in the extent of pore helix rotation relative to WT ( Figure 6D) and a similar level of pore hydration as WT channels ( Figure 6B). Examination of the simulation trajectories showed that the introduced Leu, which is both shorter and more hydrophobic than the native Met, spends the majority of the simulation time in the hydrophobic cluster at the TM1-TM3 interface and away from F171, suggesting that it cannot interact with F171 to facilitate pore opening ( Figure 6-video 1). Quantification of the M173L-F171 distance as measured from the C b atom of M173 indicated a subtle but clear shift towards larger distances in this variant. This shift was accompanied by an increase in the interaction propensity between M173L and F259 ( Figure 6E,F and Figure 6-video 1). By contrast, in simulations of M173F channels, we observed that the Phe side-chain, which is shorter and less flexible than the native Met at position 173, results in a bridge between F171 and the TM3 residue F259, causing F171 to be displaced away from the pore and increasing pore helix rotation ( Figure 6-video 2). We conclude that the M173L mutation stabilizes F99 in a pore-facing configuration, and that the resulting decrease in pore hydration relative to WT channels in the hydrophobic stretch contributes to the LOF phenotype of the M101L mutant.

Discussion
Ion channel gates come in a variety of shapes and sizes, including bulky amino acids that cause steric blockade, reversible salt bridges that form electrostatic barriers, and hydrophobic residues that impede pore hydration. Recent progress in membrane protein purification, high-resolution structural biology techniques, and molecular dynamics studies has permitted detailed examination of the structural and energetic landscape within channel pores. We now know that many ion channels operate, at least in part, by hydrophobic gating, wherein energetically unfavorable interactions between water molecules and nonpolar pore-lining residues lead to a dewetted stretch in the pore that presents an energetic barrier to ion conduction (Aryal et al., 2015).
The hydrophobic gate of store-operated Orai1 channels is formed by two rings of pore-facing nonpolar residues, V102 and F99, which together preclude ion flow in the resting state (McNally et al., 2012;Yamashita et al., 2017). In this study, we identified a unique feature of Orai1 channels, the M101 gate latch, which facilitates displacement of the F99 gate to allow ion permeation. Sulfur-aromatic interactions are prevalent across diverse groups of proteins and have been shown to be essential in stabilizing protein folding and facilitating oxidation-dependent conformational changes (Gó mez- Tamayo et al., 2016;Valley et al., 2012;Weber and Warren, 2019). More recently, a systematic survey of all protein structures available in the Protein Data Bank reported that up to 40% of all proteins involved a methionine bridging two aromatic residues in Aro-Met-Aro formations, albeit with less well-defined functional roles than simple Met-aromatic interactions (Weber and Warren, 2019). To our knowledge, the methionine gate latch in CRAC channels is the first reported example of a Met-aromatic interaction involved in ion channel gating.
MD simulations indicated that, contrary to our previous predictions of its role in a conformationally constrained hydrophobic clamp (Yeung et al., 2018), M101 retains a considerable amount of flexibility. Most notably, direct M101-F99 contact was strongly correlated with metrics of pore opening (Figure 2), suggesting that M101 acts as a bridge between the F99 gate and an F187 'anchor' on TM3 to keep the channel gate open. We validated this concept experimentally by introducing double cysteine mutants that can be bridged by Cd 2+ . In the F99C/M101C double mutant, formation of a Cd 2+ bridge between the cysteines at F99 and M101 resulted in robust activation of Orai1 current (Figure 3). This effect is reminiscent of Cd 2+ bridging between cysteines introduced at G98 and F99, which also potentiates Orai1 current by tethering F99C in a deflected state away from the pore . The opposite is true for the M101C/F187C double mutant, where Cd 2+ disrupts the constitutive activation of the mutant, presumably by forming a bridge between M101C and F187C. The formation of the M101C-Cd 2+ -F187C bond likely destabilizes the open state of the F99 gate, freeing F99, and causing it to revert into its closed pore-facing configuration to close the channel (Figure 4).
Consistent with an essential role for the M101 gate latch in opening the gate, none of the tested mutations at M101 supported STIM1-mediated Orai1 activation. Even the substitutions that are most similar to the native Met (e.g. Leu, Ile, Cys) in their hydrophobicity and which preserve the a atoms for all pore-lining residues (hOrai1 numbering in brown). Average distribution of water oxygen atoms (B) and Na + and Cl À ions (C) along the pore axis. The P values from a two-sided Welch's t-test of mean water oxygen count at z = 15 Å across all simulation repeats indicate a significant difference with respect to WT for M173L (1.2 Â 10 À2 , p<0.05) but not for M173F (1.1 Â 10 À1 ). (D) Relative distributions of the radial angle of residue 171 defined as the angle between the pore axis, the center of mass of the two helical turns centered at residue 171, and the C a atom of residue 171 in the different mutants. The mean and standard error of mean of F171 radial angle over simulation repeats are 41 ± 1˚for M173L and 48 ± 1˚for M173F. The P values from a two-sided Welch's t-test for each system indicate significant differences (p<0.05) between the mean of these distributions with respect to WT simulations (6.1 Â 10 À24 , 5.2 Â 10 À3 ). The black solid line represents the angle observed in the closed dOrai crystal structure 4HKR. (E-F) Distribution of distances between M173 with F171 (d 3 ) and M173 with F259 (d 4 ), respectively. Distances were measured from the C b of the methionine and the center of mass of the phenylalanine ring. The mean and standard error of mean of M173-F171 distances over simulation repeats are 6.5 ± 0.1 Å for WT, 6.9 ± 0.1 Å for M173L, and 6.6 ± 0.1 Å for M173F. In (F), M173-F259 distances over simulation repeats are 6.1 ± 0.1 Å for WT, 6.0 ± 0.1 Å for M173L, and 5.8 The online version of this article includes the following video(s) for figure 6: Figure 6-video 1. MD simulation trajectory of the LOF mutant M173L dOrai. https://elifesciences.org/articles/60751#fig6video1 Figure 6-video 2. MD simulation trajectory of the GOF mutant M173F dOrai. https://elifesciences.org/articles/60751#fig6video2 ability of Orai1 to bind STIM1 failed to be activated by co-expressed STIM1 ( Figure 5A). These findings indicate that a combination of hydrophobicity and the presence of the sulfur atom in Met is necessary for the M101 latch function. The only exception to the loss of channel activity was the M101F mutant, which elicited a modest GOF phenotype. We speculate that the gate opening of this mutant may arise due to direct edge-to-face or face-to-face p-p stacking interactions among the three aromatic rings (F99, M101F, F187) as suggested by the simulations ( Figure 6H) to promote displacement of the gate.
M101 is endowed with a unique combination of features that allow it to fulfill its specialized role as a latch for stabilizing the open state of the gate. First, M101 is well situated on the non-pore facing surface of TM1 towards TM3 in closed channels and is oriented towards F99 of a neighboring subunit when TM1 rotates counterclockwise and the pore dilates. Second, Met is longer and more flexible than Leu or Ile, allowing it to interact with both F187 on TM3 and F99 in the pore. Third, and most importantly, the sulfur atom in methionine provides an additional energetic contribution that is stronger than a purely hydrophobic interaction with F99 (Reid et al., 1985;Valley et al., 2012). In solution, the energy associated with each Met-Phe bond in ab initio simulations using dimethyl sulfide and benzene as proxies of sulfur-aromatic interactions is estimated to be 2.0-2.9 kcal/mol (Gó mez-Tamayo et al., 2016), providing an upper bound to the free energy of the interaction. The true free energy of the M101-F99 association however, is likely to be significantly lower due to constraints within the Orai1 protein environment. Moreover, in the proposed gating mechanism, it is the difference in free energy between the contacts formed in open and closed states that is relevant for the gating transition.
To better estimate the contribution of the Met-Phe contacts to the gating equilibrium in Orai1, we exploited the fact that in simulations of dOrai, the open and closed channel states sample both contact and non-contact separations. The analysis in Figure 2E shows four distributions of M173-F171 distances, of two open (H206Q and H206C) and two closed channel variants (WT and H206Y). Assuming that each of these distributions approaches equilibrium, we can convert the distance distributions to potential of mean-force profiles ( Figure 7B) using a relationship derived from the Boltzmann equation (see Materials and methods). In the open state modeled by H206Q/C channels, this analysis indicates a free energy minimum at 5-6 Å that is associated with the sulfur-aromatic interaction ( Figure 7B).
The energetic contribution of the interaction to channel opening ( Figure 7C) can be quantified from the relative probability distributions of the M173-F171 distances (d 1 ) in closed and open states. Using a distance of d = 7 Å as the cutoff (Gó mez- Tamayo et al., 2016;Valley et al., 2012), we transformed these continuous probability profiles into discrete states corresponding to contact versus non-contact Met-Phe states. For the closed and open channels modeled by the above variants, the relative occupancy of the contact and non-contact states can be estimated from the ratio of the cumulative probabilities above and below the 7 Å cutoff. This ratio is~0.8 for WT channels,~0.5 for H206Y channels,~2.2 for H206Q channels, and~3 for H206C channels. Based on these ratios, the relative preference (P contact /P non-contact ) for Met-Phe interactions is approximately 0.8:1 in the closed (WT) state and 3:1 in the open (H206C) state.
Because free energy is conserved in the thermodynamic cycle in Figure 7C, it follows that: where DG 1 , DG 2 , DG 3 , and DG 4 are the free energy changes for the transitions defined in Figure 7C.
Rearranging the terms leads to: where DG 2 -DG 1 corresponds to the relative stabilization of the contact state upon channel opening, and DG 4 -DG 3 corresponds to the relative stabilization of the open state upon making contact.
DG 1 and DG 2 in Figure 7C can be calculated from the relationship: where P contact and P non-contact are the probabilities of the Met-Phe distances being smaller and larger than the 7 Å cutoff, respectively. Substituting values obtained in the previous analysis, we get 0.13 kcal/mol for DG 1 and À0.65 kcal/mol for DG 2 . Therefore, the DDG for stabilization of the open state by the gate latch contact is~0.8 kcal/mol, a value that is commensurate with the magnitude of thermal energy at physiological temperatures. Assuming that the contributions of the individual Met-Phe interactions are additive, this analysis implies that the six Met-Phe interactions contribute approximately~5 kcal/mol per channel. However, the 0.8 kcal/mol estimate could reflect in part cooperative interactions between multiple gate latch pairs rather than individual interactions, so that the actual energetic contribution to pore opening may be lower than this 5 kcal/mol estimate.
How do these estimates compare to the overall free energy change required for Orai1 channel activation? Although we currently do not know the total free energy change associated with Orai1 gating, comparison with the estimated activation energies for the Shaker potassium channel (14 kcal/mol) (Chowdhury and Chanda, 2012) and the BK channel (24 kcal/mol) (Chowdhury and Chanda, 2013) suggests that this estimate of the M101-F99 interaction energy may be critical for the overall Orai1 gating process. Furthermore, because F99 is on the face of TM1 opposite to M101, the formation of the proposed latch interactions between neighboring TM1 helices would be expected to promote correlated TM1 helix rotations to induce cooperative opening of the channel gate. These considerations indicate that M101 is well positioned, with the suitable length and added sulfur group, to interact with F187 and F99 act as an effective gate latch to facilitate opening and closing of the F99 channel gate.
From a functional standpoint, the finding M101 that promotes pore opening by stabilizing the channel gate into the open configuration likely has important implications for CRAC channel gating. Activation of CRAC channels occurs in a highly nonlinear manner with respect to STIM1 binding, resulting in abrupt switching of closed channels from a long-lasting silent state into a high open probability (P O ) channel state (Prakriya and Lewis, 2006;Yen and Lewis, 2018). The M101-F99 interaction allows for conformational changes in one TM1 subunit to be transmitted to a neighboring subunit because the M101 gate latch stabilizes the rotated state of the neighboring F99 while also keeping its own TM1 in a rotated conformation. This synergistic interaction could promote cooperative pore opening across the entire channel once one or more subunits are flipped into the active state. Once the pore is opened, the M101-F99 interaction can help maintain Orai1 channel's characteristic high-P O state governing the induction of downstream cellular pathways. Routines developed by R. S. Lewis (Stanford) on the Igor Pro software (Wavemetrics) were employed for stimulation, data acquisition and analysis. Data are corrected for the liquid junction potential of the pipette solution relative to Ringer's in the bath (À10 mV). The holding potential was +30 mV. The standard voltage stimulus consisted of a 100 ms step to -100 mV followed by a 100 ms ramp from -100 to +100 mV applied at 1 s intervals. I CRAC was typically activated by passive depletion of ER Ca 2+ stores by intracellular dialysis of 8 mM BAPTA. All currents were acquired at 5 kHz and low pass filtered with a 1 kHz Bessel filter built into the amplifier. All data were corrected for leak currents collected in 100-200 mM LaCl 3 .

Data analysis
Analysis of current amplitudes was typically performed by measuring the peak currents during the À100 mV pulse. Specific mutants were categorized as gain-of-function if their currents exceeded 2 pA/pF, which is more than ten times the current density of WT Orai1 without STIM1. Reversal potentials were measured from the average of several leak-subtracted sweeps in each cell. Fractional inhibition of current was quantified as: Inhibition=(1-I b /I Ctrl ), where I b is the Orai1 current in the presence of Cd 2+ , and I Ctrl is the Orai1 current prior to application of the blocker (Cd 2+ ).

FRET microscopy
HEK293-H cells transfected with Orai1-YFP and CFP-CAD DNA constructs were imaged using widefield epifluorescence microscopy on an IX71 inverted microscope (Olympus, Center Valley, PA). Cells were imaged with a 60X oil immersion objective (UPlanApo NA 1.40), a 175 W Xenon arc lamp (Sutter, Novatao, CA), and excitation and emission filter wheels (Sutter, Novato, CA). At each time point, three sets of images (CFP, YFP, and FRET) were captured on a cooled EM-CCD camera (Hamamatsu, Bridgewater, NJ) using optical filters specific for the three images as previously described. Image acquisition and analysis was performed with SlideBook software (Imaging Innovations Inc, Denver, CO). Images were captured at exposures of 100-500 ms with 1 Â 1 binning. Lamp output was attenuated to 25% by a 0.6 ND filter in the light path to minimize photobleaching. All experiments were performed at room temperature. FRET analysis was performed as previously described (Navarro-Borelly et al., 2008). The microscope-specific bleed-through constants (a = 0.12; b = 0.008; c = 0.002 and d = 0.33) were determined from cells expressing cytosolic CFP or YFP alone. The apparent FRET efficiency was calculated from background-subtracted images using the formalism (Zal and Gascoigne, 2004): where F c = I DA aIAA -dI DD. I DD , I AA , and I DA refer to the background subtracted CFP, YFP, and FRET images, respectively. The instrument dependent G factor had the value 1.85 ± 0.1. E-FRET analysis was restricted to cells with YFP/CFP ratios in the range of 2-6 to ensure that E-FRET was compared across identical acceptor to donor ratios, and measurements were restricted to regions of interest drawn at the plasma membrane.

Confocal microscopy
HEK293-H cells expressing various Orai1-YFP mutants and CFP-CAD were imaged on an Andor XDI Revolution spinning-disk confocal microscope equipped with a 100X oil immersion objective. Cells were maintained at 37˚C with 5% CO 2 . Fluorophores were excited with 445 nm (CFP) and 515 nm (YFP) laser diodes with the intensity of laser light attenuated to 15-40% for CFP and 5-30% for YFP. Images were obtained at 512 Â 512 pixels at an exposure of 200-500 ms per frame and a slice thickness of 0.8 mm. An average of four frames was used for each image. Images analysis was performed using NIH ImageJ software (NIH, Bethesda, MD).

Molecular dynamics simulations
Molecular models were constructed using the crystal structure of the Drosophila melanogaster Orai1 channel (4HKR) (Hou et al., 2012). Missing residues of the M1-M2 loop (amino acids 181 to 190) and the M2-M3 loop (amino acids 220 to 235) were modeled de novo using MODELLER (Fiser and Sali,