Structures of riboswitch RNA reaction states by mix-and-inject XFEL serial crystallography.

Riboswitches are structural RNA elements that are generally located in the 5' untranslated region of messenger RNA. During regulation of gene expression, ligand binding to the aptamer domain of a riboswitch triggers a signal to the downstream expression platform. A complete understanding of the structural basis of this mechanism requires the ability to study structural changes over time. Here we use femtosecond X-ray free electron laser (XFEL) pulses to obtain structural measurements from crystals so small that diffusion of a ligand can be timed to initiate a reaction before diffraction. We demonstrate this approach by determining four structures of the adenine riboswitch aptamer domain during the course of a reaction, involving two unbound apo structures, one ligand-bound intermediate, and the final ligand-bound conformation. These structures support a reaction mechanism model with at least four states and illustrate the structural basis of signal transmission. The three-way junction and the P1 switch helix of the two apo conformers are notably different from those in the ligand-bound conformation. Our time-resolved crystallographic measurements with a 10-second delay captured the structure of an intermediate with changes in the binding pocket that accommodate the ligand. With at least a 10-minute delay, the RNA molecules were fully converted to the ligand-bound state, in which the substantial conformational changes resulted in conversion of the space group. Such notable changes in crystallo highlight the important opportunities that micro- and nanocrystals may offer in these and similar time-resolved diffraction studies. Together, these results demonstrate the potential of 'mix-and-inject' time-resolved serial crystallography to study biochemically important interactions between biomacromolecules and ligands, including those that involve large conformational changes.

A thermodynamic framework for Mg2+ binding to RNA.

We present a model describing how Mg(2+) binds and stabilizes specific RNA structures. In this model, RNA stabilization arises from two energetically distinct modes of Mg(2+) binding: diffuse- and site-binding. Diffusely bound Mg(2+) are electrostatically attracted to the strong anionic field around the RNA and are accurately described by the Poisson-Boltzmann equation as an ensemble distributed according to the electrostatic potentials around the nucleic acid. Site-bound Mg(2+) are strongly attracted to specifically arranged electronegative ligands that desolvate the ion and the RNA binding site. Thus, site-binding is a competition between the strong coulombic attraction and the large cost of desolvating the ion and its binding pocket. By using this framework, we analyze three systems where a single site-bound Mg(2+) may be important for stability: the P5 helix and the P5b stem loop from the P4-P6 domain of the Tetrahymena thermophila group I intron and a 58-nt fragment of the Escherichia coli 23S ribosomal RNA. Diffusely bound Mg(2+) play a dominant role in stabilizing these RNA structures. These ions stabilize the folded structures, in part, by accumulating in regions of high negative electrostatic potential. These regions of Mg(2+) localization correspond to ions that are observed in the x-ray crystallographic and NMR structures of the RNA. In contrast, the contribution of site-binding to RNA stability is often quite small because of the large desolvation penalty. However, in special cases, site-binding of partially dehydrated Mg(2+) to locations with extraordinarily high electrostatic potential can also help stabilize folded RNA structures.

Translational repression of the Escherichia coli alpha operon mRNA: importance of an mRNA conformational switch and a ternary entrapment complex.

Ribosomal protein S4 represses synthesis of the four ribosomal proteins (including itself) in the Escherichia coli alpha operon by binding to a nested pseudoknot structure that spans the ribosome binding site. A model for the repression mechanism previously proposed two unusual features: (i) the mRNA switches between conformations that are "active" or "inactive" in translation, with S4 as an allosteric effector of the inactive form, and (ii) S4 holds the 30 S subunit in an unproductive complex on the mRNA ("entrapment"), in contrast to direct competition between repressor and ribosome binding ("displacement"). These two key points have been experimentally tested. First, it is found that the mRNA pseudoknot exists in an equilibrium between two conformers with different electrophoretic mobilities. S4 selectively binds to one form of the RNA, as predicted for an allosteric effector; binding of ribosomal 30 S subunits is nearly equal in the two forms. Second, we have used S4 labeled at a unique cysteine with either of two fluorophores to characterize its interactions with mRNA and 30 S subunits. Equilibrium experiments detect the formation of a specific ternary complex of S4, mRNA pseudoknot, and 30 S subunits. The existence of this ternary complex is unambiguous evidence for translational repression of the alpha operon by an entrapment mechanism.

Recognition of 16S rRNA by ribosomal protein S4 from Bacillus stearothermophilus.

Protein S4 is essential for bacterial small ribosomal subunit assembly and recognizes the 5' domain (approximately 500 nt) of small subunit rRNA. This study characterizes the thermodynamics of forming the S4-5' domain rRNA complex from a thermophile, Bacillus stearothermophilus, and points out unexpected differences from the homologous Escherichia coli complex. Upon incubation of the protein and RNA at temperatures between 35 and 50 degrees C under ribosome reconstitution conditions [350 mM KCl, 8 mM MgCl2, and 30 mM Tris (pH 7.5)], a complex with an association constant of > or = 10(9) M(-1) was observed, more than an order of magnitude tighter than previously found for the homologous E. coli complex under similar conditions. This high-affinity complex was shown to be stoichiometric, in equilibrium, and formed at rates on the order of magnitude expected for diffusion-controlled reactions ( approximately 10(7) M(-1) x s(-1)), though at low temperatures the complex became kinetically trapped. Heterologous binding experiments with E. coli S4 and 5' domain RNA suggest that it is the B. stearothermophilus S4, not the rRNA, that is activated by higher temperatures; the E. coli S4 is able to bind 5' domain rRNA equally well at 0 and 37 degrees C. Tight complex formation requires a low Mg ion concentration (1-2 mM) and is very sensitive to KCl concentration [- partial differential[log(K)]/partial differential(log[KCl]) = 9.3]. The protein has an unusually strong nonspecific binding affinity of 3-5 x 10(6) M(-1), detected as a binding of one or two additional proteins to the target 5' domain RNA or two to three proteins binding a noncognate 23S rRNA fragment of the approximately same size. This binding is not as sensitive to monovalent ion concentration [- partial differential[log(K)]/partial differential(log[KCl]) = 6.3] as specific binding and does not require Mg ion. These findings are consistent with S4 stabilizing a compact form of the rRNA 5' domain.

Thermal methods for the analysis of RNA folding pathways.

Once a model of the secondary structure of an RNA has been deduced, thermal melting analysis can be used to determine whether the model accounts for all intramolecular interactions of the RNA, or whether noncanonical and tertiary interactions make the structure more stable than predicted, or link parts of the structure in unexpected ways. It is also useful to determine the pH, salt, and temperature ranges under which the RNA adopts a stably folded structure, or to analyze unfolding pathways. This unit discusses sample preparation, instrumentation, and theoretical background. It also provide a sample analysis of tRNA unfolding.

Structural preordering in the N-terminal region of ribosomal protein S4 revealed by heteronuclear NMR spectroscopy.

Protein S4, a component of the 30S subunit of the prokaryotic ribosome, is one of the first proteins to interact with rRNA in the process of ribosome assembly and is known to be involved in the regulation of this process. While the structure of the C-terminal 158 residues of Bacillus stearothermophilus S4 has been solved by both X-ray crystallography and NMR, that of the N-terminal 41 residues is unknown. Evidence suggests that the N-terminus is necessary both for the assembly of functional ribosomes and for full binding to 16S RNA, and so we present NMR data collected on the full-length protein (200 aa). Our data indicate that the addition of the N-terminal residues does not significantly change the structure of the C-terminal 158 residues. The data further indicate that the N-terminus is highly flexible in solution, without discernible secondary structure. Nevertheless, structure calculations based on nuclear Overhauser effect spectroscopic data combined with (15)N relaxation data revealed that two short segments in the N-terminus, S(12)RRL(15) and P(30)YPP(33), adopt transiently ordered states in solution. The major conformation of S(12)RRL(15) appears to orient the arginine side chains outward toward the solvent in a parallel fashion, while that of P(30)YPP(33) forms a nascent turn of a polyproline II helix. These segments contain residues that are highly conserved across many prokaryotic species, and thus they are reasonable candidates respectively for sites of interaction with RNA and other ribosomal proteins within the intact ribosome.

Stabilization of RNA tertiary structure by monovalent cations.

The effects of monovalent cations (Li(+), Na(+), K(+), Rb(+), Cs(+), and NH4(+)) on the thermal stability of RNA tertiary structure were investigated by UV melting. We show that with the RNA used here (nucleotides 1051-1108 of Escherichia coli 23 S rRNA with four base substitutions), monovalent cations and Mg(2+) compete in stabilizing the RNA tertiary structure, and that the competition takes place between two boundaries: one where Mg(2+) concentration is zero and the other where it is maximally stabilizing ("saturating"). The pattern of competition is the same for all monovalent cations and depends on the cation's ability to displace Mg(2+) from the RNA, its ability to stabilize tertiary structure in the absence of Mg(2+), and its ability to stabilize tertiary structure at saturating Mg(2+) concentrations. The stabilizing ability of a monovalent cation depends on its unhydrated ionic radius, and at a low monovalent cation concentration and saturating Mg(2+), there is a (calculated) net release of a single monovalent cation/RNA molecule when tertiary structure is denatured. The implications are that under these conditions there is at least one binding site for monovalent cations on the RNA, the site is specifically associated with formation of stable tertiary structure, K(+) is the most effective of the tested cations, and Mg(2+) appears ineffective at this site. At high ionic strength, and in the absence of Mg(2+), stabilization of tertiary structure is still monovalent-cation specific and ionic-radius dependent, but a larger number of cations ( approximately eight) are released upon RNA tertiary structure denaturation, and NH(4)(+) appears to be the most effective cation in stabilizing tertiary structure under these conditions. In the majority of the experiments, methanol was added as a cosolvent to the buffer. Its use allowed the examination of the behavior of monovalent ions under conditions where their effects would otherwise have been too weak to be observed. Methanol stabilizes tertiary but not secondary structure of the RNA. There was no evidence that it either causes qualitative changes in cation-binding properties of the RNA or a change in the pattern of monovalent cation/Mg(2+) competition.

Mg(2+) binding to tRNA revisited: the nonlinear Poisson-Boltzmann model.

Our current understanding of Mg(2+) binding to RNA, in both thermodynamic and structural terms, is largely based on classical studies of transfer RNAs. Based on these studies, it is clear that magnesium ions are crucial for stabilizing the folded structure of tRNA. We present here a rigorous theoretical model based on the nonlinear Poisson-Boltzmann (NLPB) equation for understanding Mg(2+) binding to yeast tRNA(Phe). We use this model to interpret a variety of experimental Mg(2+) binding data. In particular, we find that the NLPB equation provides a remarkably accurate description of both the overall stoichiometry and the free energy of Mg(2+) binding to yeast tRNA(Phe) without any fitted parameters. In addition, the model accurately describes the interaction of Mg(2+) with localized regions of the RNA as determined by the pK(a) shift of differently bound fluorophores. In each case, we find that the model also reproduces the univalent salt-dependence and the anticooperativity of Mg(2+) binding. Our results lead us to a thermodynamic description of Mg(2+) binding to yeast tRNA(Phe) based on the NLPB equation. In this model, Mg(2+) binding is simply explained by an ensemble of ions distributed according to a Boltzmann weighted average of the mean electrostatic potential around the RNA. It appears that the entire ensemble of electrostatically bound ions superficially mimics a few strongly coordinated ions. In this regard, we find that Mg(2+) stabilizes the tertiary structure of yeast tRNA(Phe) in part by accumulating in regions of high negative electrostatic potential. These regions of Mg(2+) localization correspond to bound ions that are observed in the X-ray crystallographic structures of yeast tRNA(Phe). Based on our results and the available thermodynamic data, there is no evidence that specifically coordinated Mg ions have a significant role in stabilizing the native tertiary structure of yeast tRNA(Phe) in solution.

The RNA-binding domain of ribosomal protein L11 recognizes an rRNA tertiary structure stabilized by both thiostrepton and magnesium ion.

Antibiotics that inhibit ribosomal function may do so by one of several mechanisms, including the induction of incorrect RNA folding or prevention of protein and/or RNA conformational transitions. Thiostrepton, which binds to the 'GTPase center' of the large subunit, has been postulated to prevent conformational changes in either the L11 protein or rRNA to which it binds. Scintillation proximity assays designed to look at the binding of the L11 C-terminal RNA-binding domain to a 23S ribosomal RNA (rRNA) fragment, as well as the ability of thiostrepton to induce that binding, were used to demonstrate the role of Mg(2+), L11 and thio-strepton in the formation and maintenance of the rRNA fragment tertiary structure. Experiments using these assays with both an Escherichia coli rRNA fragment and a thermostable variant of that RNA show that Mg(2+), L11 and thiostrepton all induce the RNA to fold to an essentially identical tertiary structure.

Contributions of basic residues to ribosomal protein L11 recognition of RNA.

The C-terminal domain of ribosomal protein L11, L11-C76, binds in the distorted minor groove of a helix within a 58 nucleotide domain of 23 S rRNA. To study the electrostatic component of RNA recognition in this protein, arginine and lysine residues have been individually mutated to alanine or methionine residues at the nine sequence positions that are conserved as basic residues among bacterial L11 homologs. In measurements of the salt dependence of RNA-binding, five of these mutants have a reduced value of - partial differentiallog(K(obs))/ partial differentiallog[KCl] as compared to the parent L11-C76 sequence, indicating that these residues interact with the RNA electrostatic field. These five residues are located at the perimeter of the RNA-binding surface of the protein; all five of them form salt bridges with phosphates in the crystal structure of the complex. A sixth residue, Lys47, was found to make an electrostatic contribution to binding when measurements were made at pH 6.0, but not at pH 7.0; its pK in the free protein must be <6.5. The unusual behavior of Lys47 is explained by its burial in the hydrophobic core of the free protein, and unburial in the RNA-bound protein, where it forms a salt bridge with a phosphate. The contributions of these six residues to the electrostatic component of binding are not additive; thus the magnitude of the salt dependence cannot be used to count the number of ionic interactions in this complex. By interacting with irregular features of the RNA backbone, including an S-turn, these basic residues contribute to the specificity of L11 for its target site.

The interpretation of Mg(2+) binding isotherms for nucleic acids using Poisson-Boltzmann theory.

Magnesium ions play a crucial role in the structural integrity and biological activity of nucleic acids. Experimental thermodynamic descriptions of Mg(2+) interactions with nucleic acids in solution have generally relied on the analyses of binding polynomials to estimate the energetic contributions of diffuse and site-bound ions. However, since ion binding is dominated by long-range electrostatic forces, such models provide only a phenomenological description of the experimental Mg(2+) binding data and provide little insight into the actual mechanism of the binding equilibria. Here, we present a rigorous theoretical framework based on the non-linear Poisson-Boltzmann (NLPB) equation for understanding diffuse ion interactions that can be used to interpret experimental Mg(2+) binding isotherms. As intuitively expected, in the NLPB model binding is simply the total accumulation of the ion around the nucleic acid. Comparing the experimental data to the calculated curves shows that the NLPB equation provides a remarkably accurate description of Mg(2+) binding to linear polynucleotides like DNA and poly(A x U) without any fitted parameters. In particular, the NLPB model explains two general features of magnesium binding; the strong dependence on univalent salt concentration, and its substantial anticooperativity. Each of these effects can be explained by changes in the Mg(2+) distribution around the polyion under different solution conditions. In order to more fully understand these different aspects of magnesium binding, the free energy of Mg(2+) binding, DeltaGMg, is calculated and partitioned into several salt-dependent contributions: the change in the electrostatic interaction free energy of the charges, DeltaDeltaGE.D (including Mg(2+)-phosphate, Mg(2+)-Mg(2+), Mg(2+)-Na(+), Na(+)-Na(+), Na(+)-phosphate interactions, and similar contributions for Cl(-)) and the cratic free energies of (re)organizing the MgCl2 and NaCl atmospheres, DeltaG(Mg)org and DeltaDeltaG(Na)org, respectively. For the systems studied here, DeltaGMg is strongly influenced by entropic free energy changes in the distributions of both NaCl and MgCl2, DeltaG(Mg)org and DeltaDeltaG(Na)org. From this analysis, we also raise the possibility that coions added with the magnesium salt might play an important role in the overall stability of nucleic acids under some conditions.

Themes in RNA-protein recognition.

Atomic resolution structures are now available for more than 20 complexes of proteins with specific RNAs. This review examines two main themes that appear in this set of structures. A "groove binder" class of proteins places a protein structure (alpha-helix, 310-helix, beta-ribbon, or irregular loop) in the groove of an RNA helix, recognizing both the specific sequence of bases and the shape or dimensions of the groove, which are sometimes distorted from the normal A-form. A second class of proteins uses beta-sheet surfaces to create pockets that examine single-stranded RNA bases. Some of these proteins recognize completely unstructured RNA, and in others RNA secondary structure indirectly promotes binding by constraining bases in an appropriate orientation. Thermodynamic studies have shown that binding specificity is generally a function of several factors, including base-specific hydrogen bonds, non-polar contacts, and mutual accommodation of the protein and RNA-binding surfaces. The recognition strategies and structural frameworks used by RNA binding proteins are not exotically different from those employed by DNA-binding proteins, suggesting that the two kinds of nucleic acid-binding proteins have not evolved independently.

Refining the overall structure and subdomain orientation of ribosomal protein S4 delta41 with dipolar couplings measured by NMR in uniaxial liquid crystalline phases.

Prokaryotic protein S4 initiates assembly of the small ribosomal subunit by binding to 16 S rRNA. Residues 43-200 of S4 from Bacillus stearothermophilus (S4 Delta41) bind to both 16 S rRNA and to a mRNA pseudoknot. In order to obtain structure-based insights regarding RNA binding, we previously determined the solution structure of S4 Delta41 using NOE, hydrogen bond, and torsion angle restraints. S4 Delta41 is elongated, with two distinct subdomains, one all helical, the other including a beta-sheet. In contrast to the high resolution structures obtained for each individual subdomain, their relative orientation was not precisely defined because only 17 intersubdomain NOE restraints were determined. Compared to the 1.7 A crystal structure, when the sheet-containing subdomains are superimposed, the helical subdomain is twisted by almost 45 degrees about the long axis of the molecule in the solution structure. Because variations in subdomain orientation may explain how the protein recognizes multiple RNA targets, our current goal is to determine the orientation of the subdomains in solution with high precision. To this end, NOE assignments were re-examined. NOESY experiments on a specifically labeled sample revealed that one of the intersubdomain restraints had been misassigned. However, the revised set of NOE restraints produces solution structures that still have imprecisely defined subdomain orientations and that lie between the original NMR structure and the crystal structure. In contrast, augmenting the NOE restraints with N-H dipolar couplings, measured in uniaxial liquid crystalline phases, clearly establishes the relative orientation of the subdomains. Data obtained from two independent liquid crystalline milieux, DMPC/DHPC bicelles and the filamentous bacteriophage Pf1, show that the relative orientation of the subdomains in solution is quite similar to the subdomain orientation in the crystal structure. The solution structure, refined with dipolar data, is presented and its implications for S4's RNA binding activity are discussed.

A complete conformational map for RNA.

A simple stereochemical framework for understanding RNA structure has remained elusive to date. We present a comprehensive conformational map for two nucleoside-5',3'-diphosphates and for a truncated dinucleotide derived from a grid search of all potential conformers using hard sphere steric exclusion criteria to define allowed conformers. The eight-dimensional conformational space is presented as a series of two-dimensional projections. These projections reveal several well-defined allowed and disallowed regions which correlate well with data obtained from X-ray crystallography of both large and small RNA molecules. Furthermore, the two-dimensional projections show that consecutive and ribose ring-proximal torsion angles are interdependent, while more distant torsion angles are not. Remarkably, using steric criteria alone, it is possible to generate a predictive conformational map for RNA.

Crystal structure of a conserved ribosomal protein-RNA complex.

The structure of a highly conserved complex between a 58-nucleotide domain of large subunit ribosomal RNA and the RNA-binding domain of ribosomal protein L11 has been solved at 2.8 angstrom resolution. It reveals a precisely folded RNA structure that is stabilized by extensive tertiary contacts and contains an unusually large core of stacked bases. A bulge loop base from one hairpin of the RNA is intercalated into the distorted major groove of another helix; the protein locks this tertiary interaction into place by binding to the intercalated base from the minor groove side. This direct interaction with a key ribosomal RNA tertiary interaction suggests that part of the role of L11 is to stabilize an unusual RNA fold within the ribosome.

Protein-RNA sequence covariation in a ribosomal protein-rRNA complex.

Comparative sequence analysis has successfully predicted secondary structure and tertiary interactions in ribosomal and other RNAs. Experiments presented here ask whether the scope of comparative sequence-based predictions can be extended to specific interactions between proteins and RNA, using as a system the well-characterized C-terminal RNA binding domain of ribosomal protein L11 (L11-C76) and its 58 nucleotide binding region in 23S rRNA. The surface of L11-C76 alpha-helix 3 is known to contact RNA; position 69 in this helix is conserved as serine in most organisms but varies to asparagine (all plastids) or glutamine (Mycoplasma). RNA sequence substitutions unique to these groups of organisms occur at base pairs 1062/1076 or 1058/1080, respectively. The possibility that rRNA base pair substitutions compensate for variants in L11 alpha-helix 3 has been tested by measuring binding affinities between sets of protein and RNA sequence variants. Stability of the RNA tertiary structure, as measured by UV melting experiments, was unexpectedly affected by a 1062/1076 base pair substitution; additional mutations were required to restore a stably folded structure to this RNA. The results show that the asparagine variant of L11-C76 residue 69 has been compensated by substitution of a 1062/1076 base pair, and plausibly suggest a direct contact between the amino acid and base pair. For some of the protein and RNA mutations studied, changes in binding affinity probably reflect longer-range adjustments of the protein-RNA contact surface.

RNA binding strategies of ribosomal proteins.

Structures of a number of ribosomal proteins have now been determined by crystallography and NMR, though the complete structure of a ribosomal protein-rRNA complex has yet to be solved. However, some ribosomal protein structures show strong similarity to well-known families of DNA or RNA binding proteins for which structures in complex with cognate nucleic acids are available. Comparison of the known nucleic acid binding mechanisms of these non-ribosomal proteins with the most highly conserved surfaces of similar ribosomal proteins suggests ways in which the ribosomal proteins may be binding RNA. Three binding motifs, found in four ribosomal proteins so far, are considered here: homeodomain-like alpha-helical proteins (L11), OB fold proteins (S1 and S17) and RNP consensus proteins (S6). These comparisons suggest that ribosomal proteins combine a small number of fundamental strategies to develop highly specific RNA recognition sites.

The solution structure of ribosomal protein S4 delta41 reveals two subdomains and a positively charged surface that may interact with RNA.

S4 is one of the first proteins to bind to 16S RNA during assembly of the prokaryotic ribosome. Residues 43-200 of S4 from Bacillus stearothermophilus (S4 Delta41) bind specifically to both 16S rRNA and to a pseudoknot within the alpha operon mRNA. As a first step toward understanding how S4 recognizes and organizes RNA, we have solved the structure of S4 Delta41 in solution by multidimensional heteronuclear nuclear magnetic resonance spectroscopy. The fold consists of two globular subdomains, one comprised of four helices and the other comprised of a five-stranded antiparallel beta-sheet and three helices. Although cross-linking studies suggest that residues between helices alpha2 and alpha3 are close to RNA, the concentration of positive charge along the crevice between the two subdomains suggests that this could be an RNA-binding site. In contrast to the L11 RNA-binding domain studied previously, S4 Delta41 shows no fast local motions, suggesting that it has less capacity for refolding to fit RNA. The independently determined crystal structure of S4 Delta41 shows similar features, although there is small rotation of the subdomains compared with the solution structure. The relative orientation of the subdomains in solution will be verified with further study.

The crystal structure of ribosomal protein S4 reveals a two-domain molecule with an extensive RNA-binding surface: one domain shows structural homology to the ETS DNA-binding motif.

We report the 1.7 A crystal structure of ribosomal protein S4 from Bacillus stearothermophilus. To facilitate the crystallization, 41 apparently flexible residues at the N-terminus of the protein have been deleted (S4Delta41). S4Delta41 has two domains; domain 1 is completely alpha-helical and domain 2 comprises a five-stranded antiparallel beta-sheet with three alpha-helices packed on one side. Domain 2 is an insertion within domain 1, and it shows significant structural homology to the ETS domain of eukaryotic transcription factors. A phylogenetic analysis of the S4 primary structure shows that the likely RNA interaction surface is predominantly on one side of the protein. The surface is extensive and highly positively charged, and is centered on a distinctive canyon at the domain interface. The latter feature contains two arginines that are totally conserved in all known species of S4 including eukaryotes, and are probably crucial in binding RNA. As has been shown for other ribosomal proteins, mutations within S4 that affect ribosome function appear to disrupt the RNA-binding sites. The structure provides a framework with which to probe the RNA-binding properties of S4 by site-directed mutagenesis.