Stable sheared A.C pair in DNA hairpins

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.

Hexamer oligonucleotide topology and assembly under solution phase NMR and theoretical modeling scrutiny

The entire family of noncomplementary hexamer oligodeoxyribonucleotides d(GCXYGC) (X and Y = A, G, C, or T) were assessed for topological indicators and equilibrium thermodynamics using a priori molecular modeling and solution phase NMR spectroscopy. Feasible modeled hairpin structures formed a basis from which solution structure and equilibria for each oligonucleotide were considered. ¹H and ³¹P variable temperature-dependent (VT) and concentration-dependent NMR data, NMR signal assignments, and diffusion parameters led to d(GCGAGC) and d(GCGGGC) being understood as exceptions within the family in terms of self-association and topological character. A mean diffusion coefficient D(298 K) = (2.0 ± 0.07) × 10⁻¹⁰ m² s⁻¹ was evaluated across all hexamers except for d(GCGAGC) (D(298 K) = 1.7 × 10⁻¹⁰ m² s⁻¹) and d(GCGGGC) (D(298 K) = 1.2 × 10⁻¹⁰ m² s⁻¹). Melting under VT analysis (T(m) = 323 K) combined with supporting NMR evidence confirmed d(GCGAGC) as the shortest tandem sheared GA mismatched duplex. Diffusion measurements were used to conclude that d(GCGGGC) preferentially exists as the shortest stable quadruplex structure. Thermodynamic analysis of all data led to the assertion that, with the exception of XY = GA and GG, the remaining noncomplementary oligonucleotides adopt equilibria between monomer and duplex, contributed largely by monomer random-coil forms. Contrastingly, d(GCGAGC) showed preference for tandem sheared GA mismatch duplex formation with an association constant K = 3.9 × 10⁵M⁻¹. No direct evidence was acquired for hairpin formation in any instance although its potential existence is considered possible for d(GCGAGC) on the basis of molecular modeling studies.

Folding of a DNA hairpin loop structure in explicit solvent using replica-exchange molecular dynamics simulations

Hairpin loop structures are common motifs in folded nucleic acids. The 5'-GCGCAGC sequence in DNA forms a characteristic and stable trinucleotide hairpin loop flanked by a two basepair stem helix. To better understand the structure formation of this hairpin loop motif in atomic detail, we employed replica-exchange molecular dynamics (RexMD) simulations starting from a single-stranded DNA conformation. In two independent 36 ns RexMD simulations, conformations in very close agreement with the experimental hairpin structure were sampled as dominant conformations (lowest free energy state) during the final phase of the RexMDs ( approximately 35% at the lowest temperature replica). Simultaneous compaction and accumulation of folded structures were observed. Comparison of the GCA trinucleotides from early stages of the simulations with the folded topology indicated a variety of central loop conformations, but arrangements close to experiment that are sampled before the fully folded structure also appeared. Most of these intermediates included a stacking of the C(2) and G(3) bases, which was further stabilized by hydrogen bonding to the A(5) base and a strongly bound water molecule bridging the C(2) and A(5) in the DNA minor groove. The simulations suggest a folding mechanism where these intermediates can rapidly proceed toward the fully folded hairpin and emphasize the importance of loop and stem nucleotide interactions for hairpin folding. In one simulation, a loop motif with G(3) in syn conformation (dihedral flip at N-glycosidic bond) accumulated, resulting in a misfolded hairpin. Such conformations may correspond to long-lived trapped states that have been postulated to account for the folding kinetics of nucleic acid hairpins that are slower than expected for a semiflexible polymer of the same size.

Spectroscopic and structural impact of a stem base-pair change in DNA hairpins: GTTC-ACA-GAAC versus GTAC-ACA-GTAC

Successive investigations over the last decade have revealed and confirmed a stable loop closure in a family of d-[GTAC-5Pur6N7N-GTAC] hairpins, where 5Pur6N7N is a AAA, GAG and AXC loop (X being any nucleotide). The trinucleotide loop is characterized by a well defined 5Pur-7N mispairing mode, and by upfield chemical shifts for three sugar protons of the apical nucleotide 6N. The GTTC-ACA-GAAC DNA hairpin, of interest for its likely involvement in Vibrio cholerae genome mutations, has now been investigated. The GTAC-ACA-GTAC DNA hairpin has also been studied because it is intermediate between the other structures, as it contains the loop of the hairpin under consideration and the stem of the above family. The two hairpins with the ACA loop are stable. They show the same mispairing mode and similar upfield shifts as the previous family, but GTTC-ACA-GAAC seems to be slightly less compact than any other. GTTC-ACA-GAAC is remarkable in that it exhibits a B(II) character for the phosphate-ester conformation at 8Gp9A, together with a swing of the upper hairpin into the major groove that, in particular, brings 6CH1' roughly as close to 7AH2 as to 6CH6. These unexpected structural features are qualitatively deduced from (1)H and (31)P NMR spectra, and confirmed by Raman spectroscopy. This comparative study shows that not only the loop sequence but also the stem sequence may control hairpin structures.

A mutational analysis of the 8-17 deoxyribozyme core

The 8-17 deoxyribozyme is a small RNA-cleaving DNA enzyme of significant applicative interest. We measured the kinetics of over 60 variants of 8-17, mutated within the "core" region. The data were analyzed according to a conceptual framework in which deleterious substitutions can either decrease the stability of the reaction's transition state, or favor unreactive ground-state conformations. In agreement with earlier in vitro evolution studies, the most severe functional effects were observed upon mutating four conserved residues, whose role was further explored by replacing them with non-standard nucleotides. Removal or modification of individual functional groups on the A6 and G7 bases suggested that these residues are involved in a close-contact interaction and form a network of functionally important hydrogen bonds. Mutagenesis of residues C13 and G14 was less revealing, but argued strongly against a role of C13 as a general acid/base catalyst. The use of non-standard nucleotides also led to the identification of one deoxyribozyme variant that, under some ionic conditions, is substantially more active than the wild-type construct. Finally, the effects of mutations in the intramolecular "core stem" correlated only in part with changes in helical stability, suggesting that a stable stem is required but not sufficient for optimal activity.

Oligodeoxynucleotides having a loop consisting of 3'-deoxy-4'-C-(2-hydroxyethyl)thymidines form stable hairpins

Components that form stable hairpin loops are highly useful for the development of functional DNA and RNA molecules. We have designed and synthesized a sugar-modified thymidine analogue, 3'-deoxy-4'-C-(2-hydroxyethyl)thymidine (X), as a nucleosidic loop component stabilizing the hairpin structure. The ODNs I-1-4, 5'-d[CGAACG-X(n)-CGTTCG]-3' (I-1, n = 1; I-2, n = 2; I-3, n = 3; I-4, n = 4), forming the hairpin loop structures, of which the loop moiety consisted of the analogue X, and also the corresponding unmodified ODNs II-1-4, 5'-d[CGAACG-T(n)-CGTTCG]-3' (II-1, n = 1; II-2, n = 2;II-3, n = 3; II-4, n = 4), having a thymidine loop, were synthesized by the phosphoramidite method. The melting temperatures (T(m)) of the ODNs I-1-4 containing X in the loop moiety at 5 microM were 67.1, 68.1, 73.0, and 69.3 degrees C, respectively, and those of the control natural ODNs II-1-4 were 65.3, 67.0, 69.2, and 68.8 degrees C, respectively. Thus, the ODNs I-1-4 formed a more thermally stable hairpin than the corresponding unmodified ODNs II-1-4 having an equal number of loop residues. The hairpin structures of the modified ODNs I-1-4 and the unmodified ODNs II-1-4 were investigated by CD spectroscopy and molecular mechanics calculations. These results showed that the 4'-branched nucleoside X can stabilize hairpin structures when it is present in the loop moiety, probably due to the flexibility of the one-carbon-elongated 4'-branched structure.

The nature of actinomycin D binding to d(AACCAXYG) sequence motifs

Earlier studies by others had indicated that actinomycin D (ACTD) binds well to d(AACCATAG) and the end sequence TAG-3' is essential for its strong binding. In an effort to verify these assertions and to uncover other possible strong ACTD binding sequences as well as to elucidate the nature of their binding, systematic studies have been carried out with oligomers of d(AACCAXYG) sequence motifs, where X and Y can be any DNA base. The results indicate that in addition to TAG-3', oligomers ending with XAG-3' and XCG-3' all provide binding constants > or =1 x 10(7) M(-1) and even sequences ending with XTG-3' and XGG-3' exhibit binding affinities in the range 1-8 x 10(6) M(-1). The nature of the strong ACTD affinity of the sequences d(A1A2C3C4A5X6Y7G8) was delineated via comparative binding studies of d(AACCAAAG), d(AGCCAAAG) and their base substituted derivatives. Two binding modes are proposed to coexist, with the major component consisting of the 3'-terminus G base folding back to base pair with C4 and the ACTD inserting at A2C3C4 by looping out the C3 while both faces of the chromophore are stacked by A and G bases, respectively. The minor mode is for the G to base pair with C3 and to have the same A/chromophore/G stacking but without a looped out base. These assertions are supported by induced circular dichroic and fluorescence spectral measurements.

Sheared-type G(anti).C(syn) base-pair: a unique d(GXC) loop closure motif

Stable DNA loop structures closed by a novel G.C base-pair have been determined for the single-residue d(GXC) loops (X=A, T, G or C) in low-salt solution by high-resolution nuclear magnetic resonance (NMR) techniques. The closing G.C base-pair in these loops is not of the canonical Watson-Crick type, but adopts instead a unique sheared-type (trans Watson-Crick/sugar-edge) pairing, like those occurring in the sheared mismatched G.A or A.C base-pair, to draw the two opposite strands together. The cytidine residue in the closing base-pair is transformed into the rare syn domain to form two H-bonds with the guanine base and to prevent the steric clash between the G 2NH(2) and the C H-5 protons. Besides, the sugar pucker of the syn cytidine is still located in the regular C2'-endo domain, unlike the C3'-endo domain adopted for the pyrimidines of the out-of-alternation left-handed Z-DNA structure. The facile formation of the compact d(GXC) loops closed by a unique sheared-type G(anti).C(syn) base-pair demonstrates the great potential of the single-stranded d(GXC) triplet repeats to fold into stable hairpins.

Unusual DNA duplex and hairpin motifs

Single-stranded DNA or double-stranded DNA has the potential to adopt a wide variety of unusual duplex and hairpin motifs in the presence (trans) or absence (cis) of ligands. Several principles for the formation of those unusual structures have been established through the observation of a number of recurring structural motifs associated with different sequences. These include: (i) internal loops of consecutive mismatches can occur in a B-DNA duplex when sheared base pairs are adjacent to each other to confer extensive cross- and intra-strand base stacking; (ii) interdigitated (zipper-like) duplex structures form instead when sheared G*A base pairs are separated by one or two pairs of purine*purine mismatches; (iii) stacking is not restricted to base, deoxyribose also exhibits the potential to do so; (iv) canonical G*C or A.T base pairs are flexible enough to exhibit considerable changes from the regular H-bonded conformation. The paired bases become stacked when bracketed by sheared G.A base pairs, or become extruded out and perpendicular to their neighboring bases in the presence of interacting drugs; (v) the purine-rich and pyrimidine-rich loop structures are notably different in nature. The purine-rich loops form compact triloop structures closed by a sheared G*A, A*A, A*C or sheared-like G(anti)*C(syn) base pair that is stacked by a single residue. On the other hand, the pyrimidine-rich loops with a thymidine in the first position exhibit no base pairing but are characterized by the folding of the thymidine residue into the minor groove to form a compact loop structure. Identification of such diverse duplex or hairpin motifs greatly enlarges the repertoire for unusual DNA structural formation.

Proton NMR studies of 5'-d-(TC)(3) (CT)(3) (AG)(3)-3'--a paperclip triplex: the structural relevance of turns

In this study, we present the results of structural analysis of an 18-mer DNA 5'-T(1)C(2)T(3)C(4)T(5)C(6)C(7)T(8)C(9)T(10)C(11)T(12)A(13)G(14)A(15)G(16)A(17)G(18)-3' by proton nuclear magnetic resonance (NMR) spectroscopy and molecular modeling. The NMR data are consistent with characteristics for triple helical structures of DNA: downfield shifting of resonance signals, typical for the H3(+) resonances of Hoogsteen-paired cytosines; pH dependence of these H3(+) resonance; and observed nuclear Overhauser effects consistent with Hoogsteen and Watson-Crick basepairing. A three-dimensional model for the triplex is developed based on data obtained from two-dimensional NMR studies and molecular modeling. We find that this DNA forms an intramolecular "paperclip" pyrimidine-purine-pyrimidine triple helix. The central triads resemble typical Hoogsteen and Watson-Crick basepairing. The triads at each end region can be viewed as hairpin turns stabilized by a third base. One of these turns is comprised of a hairpin turn in the Watson-Crick basepairing portion of the 18-mer with the third base coming from the Hoogsteen pairing strand. The other turn is comprised of two bases from the continuous pyrimidine portion of the 18-mer, stabilized by a hydrogen-bond from a purine. This "triad" has well defined structure as indicated by the number of nuclear Overhauser effects and is shown to play a critical role in stabilizing triplex formation of the internal triads.

Looped out and perpendicular: deformation of Watson-Crick base pair associated with actinomycin D binding

Many anticancer drugs interact directly with DNA to exert their biological functions. To date, all noncovalent, intercalating drugs interact with DNA exclusively by inserting their chromophores into base steps to form elongated and unwound duplex structures without disrupting the flanking base pairs. By using actinomycin D (ActD)-5'-GXC/CYG-5' complexes as examples, we have found a rather unusual interaction mode for the intercalated drug; the central Watson-Crick X/Y base pairs are looped out and displaced by the ActD chromophore. The looped-out bases are not disordered but interact perpendicularly with the base/chromophore and form specific H bonds with DNA. Such a complex structure provides intriguing insights into how ligand interacts with DNA and enlarges the repertoires for sequence-specific DNA recognition.

Quadruple intercalated G-6 stack: a possible motif in the fold-back structure of the Drosophila centromeric dodeca-satellite?

The purine-rich strand d(GTACGGGACCGA)(n) of the Drosophila centromeric dodeca-satellite sequence is highly conserved and was found to form stable fold-back structures in which the homopurine 5'-GGGA-3' sequence was determined to play a crucial role. Here, we report the stable formation of the d(GGGA)(2) motif in the stem of a DNA hairpin closed by a single-residue d(ACC) loop. Similar to the zipper-like d(GGA)(2) motif observed in the human centromeric (TGGAA)(n) sequence, the central four guanosine bases in the d(GGGA)(2) motif do not pair, but interdigitate to form an elongated zipper-like quadruple-intercalated G-6 stack bracketed by sheared G.A base-pairs. Comparison between the current d(GGGA)(2) structure and the published crystal d(GAAA)(2) structure implies that the alignment of the unpaired purine bases plays an important role in determining the minor groove width of the purine-rich d(GPuPuA)(2) motif. Similarity between the zipper-like motifs possibly present in the Drosophila centromeric dodeca-satellite sequence and in the human centromeric (TGGAA)(n) sequence led us to propose that these special zipper-like motifs may constitute common cores in organizing eukaryotic centromeres.

Solution structure of a DNA double helix incorporating four consecutive non-Watson-Crick base-pairs

A series of DNA 21-mers containing a variety of the 4 x 4 internal loop sequence 5'-CAAG-3'/3'-ACGT-5' were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers exhibit excellent resolution in the NMR spectra and reveal many unusual NOEs (nuclear Overhauser effect) that allow for the detailed characterization of a DNA hairpin incorporating a track of four different non-Watson-Crick base-pairs in the stem. These include a wobble C.A base-pair, a sheared A.C base-pair, a sheared A.G base-pair, and a wobble G.T base-pair. Significantly different twisting angles were observed between the base-pairs in internal loop that results with excellent intra-strand and inter-strand base stacking within the four consecutive mismatches and the surrounding canonical base-pairs. This explains why it melts at 52 degrees C even though five out of ten base-pairs in the stem adopt non-Watson-Crick pairs. However, the 4 x 4 internal loop still fits into a B-DNA double helix very well without significant change in the backbone torsion angles; only zeta torsion angles between the tandem sheared base-pairs are changed to a great extent from the gauche(-) domain to the trans domain to accommodate the cross-strand base stacking in the internal loop. The observation that several consecutive non-canonical base-pairs can stably co-exist with Watson-Crick base-pairs greatly increases the limited repertoire of irregular DNA folds and reveals the possibility for unusual structural formation in the functionally important genomic regions that have potential to become single-stranded.

Zipper-like Watson-Crick base-pairs

A series of DNA heptadecamers containing the DNA analogues of RNA E-like 5'-d(GXA)/(AYG)-5' motifs (X/Y is complementary T/A, A/T, C/G, or G/C pair) were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers reveal excellent resolution in NMR spectra and exhibit many unusual nuclear Overhauser effects (NOEs) that allow for good characterization of an unusual zipper-like conformation with zipper-like Watson-Crick base-pairs; the potential canonical X.Y H-bonding is not present, and the central X/Y pairs are transformed instead into inter-strand stacks that are bracketed by sheared G.A base-pairs. Such phenomenal structural change is brought about mainly through two backbone torsional angle adjustments, i.e. delta from C2'-endo to C3'-endo for the sugar puckers of unpaired residues and gamma from gauche(+) to trans for the following 3'-adenosine residues. Such motifs are analogous to the previously studied (GGA)(2) motif presumably present in the human centromeric (TGGAA)(n) tandem repeat sequence. The novel zipper-like motifs are only 4-7 deg. C less stable than the (GGA)(2) motif, suggesting that inter-strand base stacking plays an important role in stabilizing unusual nucleic acid structures. The discovery that canonical Watson-Crick G.C or A.T hydrogen-bonded pairs can be transformed into stacking pairs greatly increases the repertoire for unusual nucleic acid structural motifs.

Conformational analysis of DNA-trinucleotide-hairpin-loop structures using a continuum solvent model

A number of trinucleotide sequences in DNA can form compact and stable hairpin loops that may have significance for DNA replication and transcription. The conformational analysis of these motifs is important for an understanding of the function and design of nucleic acid structures. Extensive conformational searches have been performed on three experimentally known trinucleotide hairpin loops (AGC, AAA, and GCA) closed by a four-base-pair stem. An implicit solvation model based on the generalized Born method has been employed during energy minimization and conformational search. In addition, energy-minimized conformers were evaluated using a finite-difference Poisson-Boltzmann approach. For all three loop sequences, conformations close to experiment were found as lowest-energy structures among several thousand alternative energy minima. The inclusion of reaction-field contributions was found to be important for a realistic conformer ranking. Most generated hairpin loop structures within approximately 5 kcal x mol(-1) of the lowest-energy structure have a similar topology. Structures within approximately 10 kcal x mol(-1) could be classified into about five structural families representing distinct arrangements of loop nucleotides. Although a large number of backbone torsion angle combinations were compatible with each structural class, some specific patterns could be identified. Harmonic mode analysis was used to account for differences in conformational flexibility of low-energy sub-states. Class-specific differences in the pattern of atomic fluctuations along the sequence were observed; however, inclusion of conformational entropy contributions did not change ranking of structural classes. For an additional loop sequence (AAG) with no available experimental structure, the approach suggests a lowest-energy loop topology overall similar to the other three loop sequences but closed by a different non-canonical base-pairing scheme.

CH/pi interactions in the crystal structure of TATA-box binding protein/DNA complexes

Crystal structures of TATA box-binding proteins (TBP) of various sources bound to their promoter DNA (TATA box) were analyzed with use of our program CHPI. A number of short CH/Csp2 contacts have been unveiled in these complexes at the boundary of TBP and the TATA box minor groove. The result was discussed in the context of the CH/pi interaction. Thus, the nature of nonpolar forces, reported in the past at the interface of the two components, has been attributed to the CH/pi interaction. Furthermore, many CH/pi contacts have been disclosed within the same strand of the promoter DNA. The structure of the TATA element, partially unwound and severely bent on complexation, seems to be stabilized by CH/pi interactions; H2' of the deoxyribose moiety and the methyl group in the thymine nucleotide play the primary role.

A DNA hairpin with a single residue loop closed by a strongly distorted Watson-Crick G x C base-pair

Our previous NMR and modeling studies have shown that the single-stranded 19mer oligonucleotides d(AGCTTATC-ATC-GATAA GCT) -ATC- and d(AGCTTATC-GAT-GATAAGCT) -GAT- encompassing the strongest topoisomerase II cleavage site in pBR322 DNA could form stable hairpin structures. A new sheared base-pair, the pyrimidine-purine C x A, was found to close the single base -ATC- loop, while -GAT- displayed a flexible loop of three/five residues with no stabilizing interactions. Now we report a structural study on -GAC-, an analog of -GAT-, derived through the substitution of the loop residue T by C. The results obtained from NMR, non-denaturing PAGE, UV-melting, circular dichroism experiments and restrained molecular dynamics indicate that -GAC- adopts a hairpin structure folded through a single residue loop. In the -GAC- hairpin the direction of the G9 sugar is reversed relative to the C8 sugar, thus pushing the backbone of the loop into the major groove. The G9 x C11 base-pair closing the loop is thus neither a sheared base-pair nor a regular Watson-Crick one. Although G9 and C11 are paired through hydrogen bonds of Watson-Crick type, the base-pair is not planar but rather adopts a wedge-shaped geometry with the two bases stacked on top of each other in the minor groove. The distortion decreases the sugar C1'-C1' distance between the paired G9 and C11, to 8 A versus 11 A in the standard B-DNA. The A10 residue at the center of the loop interacts with the G9 x C11 base-pair, and seems to contribute to the extra thermal stability displayed by -GAC- compared to -GAT-. Test calculations allowed us to identify the experimental NOEs critical for inducing the distorted G.C Watson-Crick base-pair. The preference of -GAC- for a hairpin structure rather than a duplex is confirmed by the diffusion constant values obtained from pulse-field gradient NMR experiments. All together, the results illustrate the high degree of plasticity of single-stranded DNAs which can accommodate a variety of turn-loops to fold up on themselves.

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.