Role of the closing base pair for d(GCA) hairpin stability: free energy analysis and folding simulations

Hairpin loops belong to the most important structural motifs in folded nucleic acids. The d(GNA) sequence in DNA can form very stable trinucleotide hairpin loops depending, however, strongly on the closing base pair. Replica-exchange molecular dynamics (REMD) were employed to study hairpin folding of two DNA sequences, d(gcGCAgc) and d(cgGCAcg), with the same central loop motif but different closing base pairs starting from single-stranded structures. In both cases, conformations of the most populated conformational cluster at the lowest temperature showed close agreement with available experimental structures. For the loop sequence with the less stable G:C closing base pair, an alternative loop topology accumulated as second most populated conformational state indicating a possible loop structural heterogeneity. Comparative-free energy simulations on induced loop unfolding indicated higher stability of the loop with a C:G closing base pair by ~3 kcal mol(-1) (compared to a G:C closing base pair) in very good agreement with experiment. The comparative energetic analysis of sampled unfolded, intermediate and folded conformational states identified electrostatic and packing interactions as the main contributions to the closing base pair dependence of the d(GCA) loop stability.     

RNA hairpin loop stability depends on closing base pair.

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type GGXAUAAUAYCC, where X and Y are CG, GC, AU, UA, GU, or UG. A nearest neighbor analysis of the data indicates the free energy change for loop formation at 37 degrees C, delta degrees Gl,37, averages 3.4 kcal/mol for hairpin loops closed with C.G, G.C, and G.U pairs. In contrast, delta G degree l,37 averages 4.6 kcal/mol for loops closed with A.U, U.A, or U.G pairs. Thus the stability of an RNA hairpin depends on the closing base pair. The hairpin with a GA mismatch that is formed by GGCGUAAUAGCC is more stable than the corresponding hairpin with an AA mismatch. Thus hairpin stability also depends on loop sequence. These effects are not included in current algorithms for prediction of RNA structure from sequence.     

Sequence dependence of the stability of RNA hairpin molecules with six nucleotide loops

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequence of the types GCGXUAAUYCGC and GGUXUAAUYACC with Watson-Crick loop closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.1 to 5.1 kcal/mol. These results agree with the model previously developed [Vecenie, C. J., and Serra, M. J. (2004) Biochemistry 43, 11813] to predict the stability of RNA hairpin loops: DeltaG degrees (37L(n) = DeltaG degrees (37i(n) + DeltaG degrees (37MM) - 0.8 (if first mismatch is GA or UU) - 0.8 (if first mismatch is GG and loop is closed on the 5' side by a purine). Here, DeltaG degrees (37i(n) is the free energy for initiating a loop of n nucleotides, and DeltaG degrees (37MM) is the free energy for the interaction of the first mismatch with the closing base pair. Thermodynamic parameters are also reported for hairpin formation in 1 M NaCl by RNA sequence of the types GACGXUAAUYUGUC and GGUXUAAUYGCC with GU base pair closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.6 to 5.3 kcal/mol. These results allow the development of a model for predicting the stability of hairpin loops closed by GU base pairs. DeltaG degrees (37L(n) (kcal/mol) = DeltaG degrees (37i(n) - 0.8 (if the first mismatch is GA) - 0.8 (if the first mismatch is GG and the loop is closed on the 5' side by a purine). Note that for these hairpins, the stability of the loops does not depend on DeltaG degrees (37MM). For hairpin loops closed by GU base pairs, the DeltaG degrees (37i(n) values, when n = 4, 5, 6, 7, and 8, are 4.9, 5.0, 4.6, 5.0, and 4.8 kcal/mol, respectively. The model gives good agreement when tested against six naturally occurring hairpin sequences. Thermodynamic values for terminal mismatches adjacent to GC, GU, and UG base pairs are also reported.     

Thermodynamic parameters for loop formation in RNA and DNA hairpin tetraloops.

We determined the melting temperatures (Tm) and thermodynamic parameters of 15 RNA and 19 DNA hairpins at 1 M NaCl, 0.01 M sodium phosphate, 0.1 mM EDTA, at pH 7. All these hairpins have loops of four bases, the most common loop size in 16S and 23S ribosomal RNAs. The RNA hairpins varied in loop sequence, loop-closing base pair (A.U, C.G, or G.C), base sequence of the stem, and stem size (four or five base pairs). The DNA hairpins varied in loop sequence, loop-closing base pair (C.G, or G.C), and base sequence of the four base-pair stem. Thermodynamic properties of a hairpin may be represented by nearest-neighbor interactions of the stem plus contributions from the loop. Thus, we obtained thermodynamic parameters for the formation of RNA and DNA tetraloops. For the tetraloops we studied, a free energy of loop formation (at 37 degrees C) of about +3 kcal/mol is most common for either RNA or DNA. There are extra stable loops with delta G degrees 37 near +1 kcal/mol, but the sequences are not necessarily the same for RNA and DNA. The closing base pair is also important; changing from C.G to G.C lowered the stability of several tetraloops in both RNA and DNA. These values will be useful in predicting RNA and DNA secondary structures.     

Thermodynamics of DNA hairpins: contribution of loop size to hairpin stability and ethidium binding.

A combination of calorimetric and spectroscopic techniques was used to evaluate the thermodynamic behavior of a set of DNA hairpins with the sequence d(GCGCTnGCGC), where n = 3, 5 and 7, and the interaction of each hairpin with ethidium. All three hairpins melt in two-state monomolecular transitions, with tm's ranging from 79.1 degrees C (T3) to 57.5 degrees C (T7), and transition enthalpies of approximately 38.5 kcal mol-1. Standard thermodynamic profiles at 20 degrees C reveal that the lower stability of the T5 and T7 hairpins corresponds to a delta G degree term of +0.5 kcal mol-1 per thymine residue, due to the entropic ordering of the thymine loops and uptake of counterions. Deconvolution of the ethidium-hairpin calorimetric titration curves indicate two sets of binding sites that correspond to one ligand in the stem with binding affinity, Kb, of approximately 1.8 x 10(6) M-1, and two ligands in the loops with Kb of approximately 4.3 x 10(4) M-1. However, the binding enthalpy, delta Hb, ranges from -8.6 (T3) to -11.6 kcal mol-1 (T7) for the stem site, and -6.6 (T3) to -12.7 kcal mol-1 (T7) for the loop site. Relative to the T3 hairpin, we obtained an overall thermodynamic contribution (per dT residue) of delta delta Hb = delta(T delta Sb) = -0.7(5) kcal mol-1 for the stem sites and delta delta Hb = delta(T delta Sb) = -1.5 kcal mol-1 for the loop sites. Therefore, the induced structural perturbations of ethidium binding results in a differential compensation of favorable stacking interactions with the unfavorable ordering of the ligands.     

A test of the model to predict unusually stable RNA hairpin loop stability

To investigate the accuracy of a model [Giese et al., 1998, Biochemistry37:1094-1100 and Mathews et al., 1999, JMol Biol 288:911-940] that predicts the stability of RNA hairpin loops, optical melting studies were conducted on sets of hairpins previously determined to have unusually stable thermodynamic parameters. Included were the tetraloops GNRA and UNCG (where N is any nucleotide and R is a purine), hexaloops with UU first mismatches, and the hairpin loop of the iron responsive element, CAGUGC. The experimental values for the GNRA loops are in excellent agreement (deltaG degrees 37 within 0.2 kcal/mol and melting temperature (TM) within 4 degrees C) with the values predicted by the model. When the UNCG hairpin loops are treated as tetraloops, and a bonus of 0.8 kcal/mol included in the prediction to account for the extra stable first mismatch (UG), the measured and predicted values are also in good agreement (deltaG degrees 37 within 0.7 kcal/mol and TM within 3 degrees C). Six hairpins with unusually stable UU first mismatches also gave good agreement with the predictions (deltaG degrees 37 within 0.5 kcal/mol and TM within 8 degrees C), except for hairpins closed by wobble base pairs. For these hairpins, exclusion of the additional stabilization term for UU first mismatches improved the prediction (AG degrees 37 within 0.1 kcal/mol and TM within 3 degrees C). Hairpins with the iron-responsive element loop were not predicted well by the model, as measured deltaG degrees 37 values were at least 1 kcal/mol greater than predicted.     

Stability of RNA hairpin loops closed by AU base pairs

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequence of the type GCAXUAAUYUGC, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates that the free energy of loop formation at 37 degrees C varies from 3.2 to 5.0 kcal/mol. These results combined with the model previously developed [Dale et al. (2000) RNA 6, 608] allow improvements in the model to predict the stability of RNA hairpin loops: DeltaG degrees (37L(n) = DeltaG degrees (37i(n)) + DeltaG degrees (37MM) - 0.8 (if first mismatch is GA or UU) - 0.8 (if first mismatch is GG and loop is closed on 5' side by a purine). Here, DeltaG degrees (37i(n) is the free energy for initiating a loop of n nucleotides, and DeltaG degrees (37MM) is the free energy for the interaction of the first mismatch with the closing base pair. Hairpins with GG first mismatches were found to vary in stability depending upon the orientation of the closing base pair (5' or 3' purine relative to the loop). The model gives good agreement when tested against four naturally occurring hairpin sequences.     

Protein loops on structurally similar scaffolds: database and conformational analysis

A general problem in comparative modeling and protein design is the conformational evaluation of loops with a certain sequence in specific environmental protein frameworks. Loops of different sequences and structures on similar scaffolds are common in the Protein Data Bank (PDB). In order to explore both structural and sequential diversity of them, a data base of loops connecting similar secondary structure fragments is constructed by searching the data base of families of structurally similar proteins and PDB. A total of 84 loop families having 2-13 residues are found among the well-determined structures of resolution better than 2.5 A. Eight alpha-alpha, 20 alpha-beta, 19 beta-alpha, and 37 beta-beta families are identified. Every family contains more than 5 loop motifs. In each family, no loops share same sequence and all the frameworks are well superimposed. Forty-three new loop classes are distinguished in the data base. The structural variability of loops in homologous proteins are examined and shown in 44 families. Motif families are characterized with geometric parameters and sequence patterns. The conformations of loops in each family are clustered into subfamilies using average linkage cluster analysis method. Information such as geometric properties, sequence profile, sequential and structural variability in loop, structural alignment parameters, sequence similarities, and clustering results are provided. Correlations between the conformation of loops and loop sequence, motif sequence, and global sequence of PDB chain are examined in order to find how loop structures depend on their sequences and how they are affected by the local and global environment. Strong correlations (R > 0.75) are only found in 24 families. The best R value is 0.98. The data base is available through the Internet.     

The Effects of Trinucleotide Repeats Found in Human Inherited Disorders on Palindrome Inviability in Escherichia Coli Suggest Hairpin Folding Preferences in Vivo

Unusual DNA secondary structures have been implicated in the expansion of trinucleotide repeat tracts that are associated with several human inherited disorders. We present evidence consistent with the folding of these trinucleotide repeats into hairpin loops at the center of a long DNA palindrome in vivo. Our assay utilizes a palindrome in bacteriophage λ, the center of which determines its ability to inhibit plaque formation in a manner that is consistent with folding into a hairpin or cruciform structure. We show that central inserts of even numbers of d(CAG)·d(CTG) repeats inhibit plaque formation more than do odd numbers. Both d(CAG)(2)·d(CTG)(2) and d(CGG)(2)·d(CCG)(2) central sequences behave like DNA sequences known to form two-base loops in vitro, suggesting that they may also form compact and stable loops. By contrast, repeats of d(GAC)·d(GTC) do not show any evidence consistent with unusual loop stability. These results agree with in vitro evidence that the unstable repeats can form hairpin secondary structures and suggest a favored position of folding. We discuss the potential roles of secondary structures, DNA replication and recombination in models of repeat tract expansion.     

Coupling of sequential transitions in a DNA double hairpin: energetics, ion binding, and hydration

In an effort to evaluate the relative contributions of sequence, ion binding, and hydration to the thermodynamic stability of nucleic acids, we have investigated the melting behavior of a double hairpin and that of its component single hairpins. Temperature-dependent UV absorption and differential scanning calorimetry techniques have been used to characterize the helix-coil transitions of three deoxyoligonucleotides: d(GTACT5GTAC), d(GCGCT5GCGC), and d(GCGCT5GCGCGTACT5GTAC). The first two oligomers melt with transition temperatures equal to 28 and 69 degrees C, respectively, in 10 mM dibasic sodium phosphate at pH 7.0. The Tm's are independent of strand concentration, strongly indicating the presence of single-stranded hairpin structures at low temperatures. The third oligomer, with a sequence corresponding to the joined sequences of the first two oligomers, melts with two apparently independent monomolecular transitions with Tm's of 41 and 69 degrees C. These transitions correspond to the melting of a double hairpin. In the salt range of 10-100 mM in NaCl, we obtain average enthalpies of 24 and 38 kcal/mol for the transitions in the single-hairpin molecules. Each transition in the double hairpin has an enthalpy of 32 kcal/mol. In addition, dtm/d log [Na+] for the transitions are 4.1 and 4.7 degrees C for the single hairpins and 12.6 and 11.2 degrees C for each transition in the double hairpin. The differential ion binding parameter between the double hairpin and that of the sum of single hairpins is roughly equal to 1.1 mol of Na+ ions/mol of double hairpin and is consistent with an increase in the electrostatic behavior of the stem phosphates of this molecule.     

Stable formation of a pyrimidine-rich loop hairpin in a cruciform promoter.

We have determined the solution structure of a TCC-loop hairpin in the cruciform promoter for the bacteriophage N4 virion RNA polymerase (N4 vRNAP). This hairpin and its complementary GGA-loop hairpin are extruded at physiological superhelical density and are required for vRNAP recognition. Contrary to its complementary GGA-loop, the three pyrimidines in the TCC-loop are all unpaired. However, with the help of two juxtaposed stem Watson-Crick G.C base-pairs, each nucleotide in the loop employs a special method to stabilize the hairpin structure. The resulting structures display extensive loop base-stacking rearrangement yet minor backbone distortion, which is largely accomplished through some loop zeta and alpha torsional angle changes. Consistent with the structural studies, UV melting of the GAAGCTCCGCTTC hairpin revealed a higher melting temperature (66 degrees C) than that of the GAACGTCCCGTTC hairpin (58 degrees C) with reversed stem G.C base-pairs, indicating significant contribution from the extra three loop-stem H-bonds. Thermodynamic parameters DeltaG degrees 25of the GAAGCTCCGCTTC hairpin and its complementary GAAGCGGAGCTTC hairpin are -4.1 and -4. 3 kcal/mol respectively, indicating approximately equal contribution of each hairpin to the cruciform formation of the N4 virion RNA polymerase promoter. No significant loop dynamics in the microsecond to millisecond NMR time-scale was observed, and the abundant well-defined exchangeable and non-exchangeable proton NOEs allowed us to efficiently determine a well-converged family for the final structures of the TCC-loop hairpin.     

The human T-cell lymphotropic virus type-I dimerization initiation site forms a hairpin loop, unlike previously characterized retroviral dimerization motifs

The formation of genomic RNA dimers during the retroviral life cycle is essential for optimal viral replication and infectivity. The sequences and RNA structures responsible for this interaction are located in the untranslated 5' leader RNA, along with other cis-acting signals. Dimer formation occurs by specific interaction between identical structural motifs. It is believed that an initial kissing hairpin forms following self-recognition by autocomplementary RNA loops, leading to formation of an extended stable duplex. The dimerization initiation site (DIS) of the deltaretrovirus human T-cell lymphotropic virus type-I (HTLV-I) has been previously localized to a 14-nucleotide sequence predicted to contain an RNA stem loop. Biochemical probing of the monomeric RNA structure using RNAse T1, RNAse V1, RNAse U2, lead acetate, and dimethyl sulfate has led to the generation of the first structural map of the HTLV-I DIS. A comprehensive data set of individual nucleotide modifications reveals that the structural motif responsible for HTLV-I RNA dimerization forms a trinucleotide RNA loop, unlike any previously characterized retroviral dimerization motif. Molecular modeling demonstrates that this can be formed by an unusual C:synG base pair closing the loop. Comparative phylogeny indicates that such a motif may also exist in other deltaretroviruses.     

Understanding the thermodynamic stability of an RNA hairpin and its mutant.

The thermodynamic stability of RNA hairpin loops has been a subject of considerable interest in the recent past (Wimberly et al., 1991). There have been experimental reports indicating that the hairpins with a C(UUCG)G loop sequence are thermodynamically very stable (Wimberly et al., 1991). We used the solution structure of GGAC(UUCG)GUCC (Cheong et al., 1990; Varani et al., 1991) as the starting conformation in our attempt to understand its thermodynamic stability. We carried out molecular dynamics/free energy simulations to understand the basis for the destabilization of the C(UUCG)G loop by mutating cytosine (C7)-->uracil. Because of the limited length of simulation and the presence of kinetic barriers (solvent intervention) to the uracil-->cytosine mutation, all of our computed free energy differences are based on multiple forward simulations. Based on these calculations we find that the cytosine-->uracil mutation in the loop destabilizes it by approximately 1.5kcal/mol relative to that of the reference state, an A-form RNA but with cytosine (C7) looped out. This is the same sign and magnitude as that observed in the thermodynamic studies carried out by Varani et al.(1991). We have carried out free energy component analysis to understand the effect of mutating the cytosine residue to uracil on the thermodynamic stability of the C(UUCG)G hairpin loops. Our calculations show that the most significant contribution to the stability is from the phosphate group linking U5 and U6, which favors the cytosine residue over uracil by about 6.0 kcal/mol. The residues U5, U6, and G8 in the loop region also contribute significantly to the stability. The contributions from the salt and solvent compensate each other, indicating the dynamic nature of interactions of the environment with the nucleic acid system and the coupling between these two components.     

Base pairing at the stem-loop junction in the SL1 kissing complex of HIV-1 RNA: a thermodynamic study probed by molecular dynamics simulation

The thermodynamics of the opening/closure process of a GC base pair located at the stem-loop junction of the SL1 sequence from HIV-1(Lai) genomic RNA was investigated in the context of a loop-loop homodimer (or kissing complex) using molecular dynamics simulation. The free energy, enthalpy and entropy changes for the closing reaction are 0 kcal x mol(-1), -11 kcal x mol(-1) and -0.037 kcal x mol(-1) x K(-1) at 300 degrees K respectively. Furthermore it is found that the free energy change is the same for the formation of a 11 nucleotide loop closed with UG and for the formation of a 9 nucleotide loop closed with GC. Our study evidences the high flexibility of the nucleotides at the stem-loop junction explaining the weak stability of this structure.     

Conformational analysis and clustering of short and medium size loops connecting regular secondary structures: a database for modeling and prediction.

Loops are regions of nonrepetitive conformation connecting regular secondary structures. We identified 2,024 loops of one to eight residues in length, with acceptable main-chain bond lengths and peptide bond angles, from a database of 223 protein and protein-domain structures. Each loop is characterized by its sequence, main-chain conformation, and relative disposition of its bounding secondary structures as described by the separation between the tips of their axes and the angle between them. Loops, grouped according to their length and type of their bounding secondary structures, were superposed and clustered into 161 conformational classes, corresponding to 63% of all loops. Of these, 109 (51% of the loops) were populated by at least four nonhomologous loops or four loops sharing a low sequence identity. Another 52 classes, including 12% of the loops, were populated by at least three loops of low sequence similarity from three or fewer nonhomologous groups. Loop class suprafamilies resulting from variations in the termini of secondary structures are discussed in this article. Most previously described loop conformations were found among the classes. New classes included a 2:4 type IV hairpin, a helix-capping loop, and a loop that mediates dinucleotide-binding. The relative disposition of bounding secondary structures varies among loop classes, with some classes such as beta-hairpins being very restrictive. For each class, sequence preferences as key residues were identified; those most frequently at these conserved positions than in proteins were Gly, Asp, Pro, Phe, and Cys. Most of these residues are involved in stabilizing loop conformation, often through a positive phi conformation or secondary structure capping. Identification of helix-capping residues and beta-breakers among the highly conserved positions supported our decision to group loops according to their bounding secondary structures. Several of the identified loop classes were associated with specific functions, and all of the member loops had the same function; key residues were conserved for this purpose, as is the case for the parvalbumin-like calcium-binding loops. A significant number, but not all, of the member loops of other loop classes had the same function, as is the case for the helix-turn-helix DNA-binding loops. This article provides a systematic and coherent conformational classification of loops, covering a broad range of lengths and all four combinations of bounding secondary structure types, and supplies a useful basis for modelling of loop conformations where the bounding secondary structures are known or reliably predicted.     

A semiflexible polymer model applied to loop formation in DNA hairpins

A statistical mechanical "zipper" model is applied to describe the equilibrium melting of short DNA hairpins with poly(dT) loops ranging from 4 to 12 bases in the loop. The free energy of loop formation is expressed in terms of the persistence length of the chain. This method provides a new measurement of the persistence length of single-stranded DNA, which is found to be approximately 1.4 nm for poly(dT) strands in 100 mM NaCl. The free energy of the hairpin relative to the random coil state is found to scale with the loop size with an apparent exponent of > or = 7, much larger than the exponent of approximately 1.5-1.8 expected from considerations of loop entropy alone. This result indicates a strong dependence of the excess stability of the hairpins, from stacking interactions of the bases within the loop, on the size of the loop. We interpret this excess stability as arising from favorable hydrophobic interactions among the bases in tight loops and which diminish as the loops get larger. Free energy profiles along a generalized reaction coordinate are calculated from the equilibrium zipper model. The transition state for hairpin formation is identified as an ensemble of looped conformations with one basepair closing the loop, and with a lower enthalpy than the random coil state. The equilibrium model predicts apparent activation energy of approximately -11 kcal/mol for the hairpin closing step, in remarkable agreement with the value obtained from kinetics measurements.     

NMR structures of (rGCUGAGGCU)2 and (rGCGGAUGCU)2: probing the structural features that shape the thermodynamic stability of GA pairs

The NMR structures of [see text] and [see text] are reported. The internal loop, [see text], is about 2 kcal/mol more stable than [see text] at 37 degrees C. The duplexes assemble into similar global folds characterized by the formation of tandem sheared GA pairs. The different stabilities of the loops are accompanied by differences in the local structure of the closing GU pairs. In the [see text] internal loop, the GU pairs form canonical wobble configurations with two hydrogen bonds, whereas in [see text], the GU pairs form a single hydrogen bond involving the amino group, GH22, and the carbonyl group, UO4. This pairing is similar to the GU closing pair of the 690 hairpin loop found in E. coli 16S rRNA. The [see text] and [see text] structures reveal how the subtle interplay between stacking and hydrogen bonding determines sequence dependent conformation and thermodynamic stability. Thus, this work provides structural and thermodynamic benchmarks for theoreticians in the ongoing effort to understand the sequence dependence of RNA physicochemical properties.     

Perturbation of DNA hairpins containing the EcoRI recognition site by hairpin loops of varying size and composition: physical (NMR and UV) and enzymatic (EcoRI) studies.

We have investigated loop-induced structural perturbation of the stem structure in hairpins d(GAATTCXnGAATTC) (X = A, T and n = 3, 4, 5 and 6) that contain an EcoRI restriction site in close proximity to the hairpin loop. Oligonucleotides containing either a T3 or a A3 loop were not hydrolyzed by the restriction enzyme and also showed only weak binding to EcoRI in the absence of the cofactor Mg2+. In contrast, hairpins with larger loops are hydrolyzed by the enzyme at the scission site next to the loop although the substrate with a A4 loop is significantly more resistant than the oligonucleotide containing a T4 loop. The hairpin structures with 3 loop residues were found to be thermally most stable while larger hairpin loops resulted in structures with lower melting temperatures. The T-loop hairpins are thermally more stable than the hairpins containing the same number of A residues in the loop. As judged from proton NMR spectroscopy and the thermodynamic data, the base pair closest to the hairpin loop did form in all cases studied. The hairpin loops did, however, affect the conformation of the stem structure of the hairpins. From 31P and 1H NMR spectroscopy we conclude that the perturbation of the stem structure is stronger for smaller hairpin loops and that the extent of the perturbation is limited to 2-3 base pairs for hairpins with T3 or A4 loops. Our results demonstrate that hairpin loops modulate the conformation of the stem residues close to the loop and that this in turn reduces the substrate activity for DNA sequence specific proteins.