Features of “All LNA” Duplexes Showing a New Type of Nucleic Acid Geometry

Förster, Charlotte; Eichert, André; Oberthür, Dominik; Betzel, Christian; Geßner, Reinhard; Nitsche, Andreas; Fürste, Jens P.

doi:https://doi.org/10.1155/2012/156035

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Volume 2012 | Article ID 156035 | https://doi.org/10.1155/2012/156035

Features of “All LNA” Duplexes Showing a New Type of Nucleic Acid Geometry

Charlotte Förster,^1,2André Eichert,^1,3Dominik Oberthür,⁴Christian Betzel,⁴Reinhard Geßner,²Andreas Nitsche,⁵and Jens P. Fürste¹

Academic Editor: Subhendu Sekhar Bag

Received13 Jan 2012

Accepted01 Mar 2012

Published14 May 2012

Abstract

“Locked nucleic acids” (LNAs) belong to the backbone-modified nucleic acid family. The 2′-O,4′-C-methylene-β-D-ribofuranose nucleotides are used for single or multiple substitutions in RNA molecules and thereby introduce enhanced bio- and thermostability. This renders LNAs powerful tools for diagnostic and therapeutic applications. RNA molecules maintain the overall canonical A-type conformation upon substitution of single or multiple residues/nucleotides by LNA monomers. The structures of “all” LNA homoduplexes, however, exhibit significant differences in their overall geometry, in particular a decreased twist, roll and propeller twist. This results in a widening of the major groove, a decrease in helical winding, and an enlarged helical pitch. Therefore, the LNA duplex structure can no longer be described as a canonical A-type RNA geometry but can rather be brought into proximity to other backbone-modified nucleic acids, like glycol nucleic acids or peptide nucleic acids. LNA-modified nucleic acids provide thus structural and functional features that may be successfully exploited for future application in biotechnology and drug discovery.

1. Introduction

Modified nucleic acids have great potential for applications in oligonucleotide-based drug design. As natural RNA and DNA molecules are highly sensitive towards nuclease digestion and often possess low thermal stability, great effort has been made to design nucleic acid modifications that stabilize RNA or DNA while simultaneously maintaining the overall Watson-Crick base pairing ability. Modified nucleic acids are indispensable for future applications comprising diagnostic and clinical approaches like the use of aptamers or the siRNA technology.

Extensive and challenging experiments and investigations have been undertaken to develop nucleotide analogues that maintain the overall A-RNA-type conformation and N-type sugar puckering, as such modifications are likely to allow the substitution of RNA without large changes in functionality. Considerable effort has been made in the synthesis and characterization of 2′-O-methyl-RNAs [1], 2′-F-RNAs [2], phosphoramidate-RNAs [3], and the “locked” nucleic acid family [4]. By using locked nucleotide building blocks containing the 2′-O,4′-C-methylene-β-D-ribofuranose (LNA) modification, a significant increase in thermostability can be observed in accordingly substituted RNAs. For example, the melting temperature of modified RNA helices can be increased by +2 to +10°C per LNA monomer substitution.

To understand the stabilizing effects of LNA-substituted RNAs, numerous structural investigations have been performed during the past years to investigate their conformation in detail. These studies provided insights in the local geometric parameters of mix-mer LNA-RNA helices and of LNA-RNA heteroduplexes. The 2′-O,4′-C-methylene-β-D-ribofuranose LNA-RNA mix-mer duplexes maintain mainly the overall A-type nucleic acid conformation [5]. On the other hand, the 2′-O,4′-C-α-L-ribofuranose LNA modification is used in DNA substitution, as this modification preserves the overall B-type nucleic acid geometry of DNA [6]. Thus, there are two powerful nucleotide modifications with great potential in drug design, the 2′-O,4′-C-methylene-β-D-ribofuranose nucleotides (LNA) for RNA substitution and the 2′-O,4′-C-methylene-α-L-ribofuranose nucleotides to modify DNA.

The structure of heteroduplexes, consisting of one fully modified LNA strand hybridized to either RNA or to DNA, revealed the following: the RNA conformation is maintained upon hybridizing a 2′-O,4′-C-methylene-β-D-ribofuranose LNA strand to RNA, whereas a mixed N- and S-type sugar puckering is induced by hybridizing a 2′-O,4′-C-methylene-β-D-ribofuranose LNA to DNA [7]. The B-type conformation is maintained by using a 2′-O,4′-C-methylene-α-L-ribofuranose LNA strand targeted to DNA [6]. It is generally accepted that the 2′-O,4′-C-methylene-β-D-ribofuranose “locks” the LNA in the C3′-endo conformation. This approach is used to direct the geometry of the phosphate backbone in a manner to orient the duplex towards a more efficient base stacking.

Even though the 2′-O,4′-C-methylene-β-D-ribofuranose LNA-RNA mix-mer duplexes maintain the overall A-type nucleic acid conformation, molecular dynamics simulations [8] and a crystal structure [9] of “all” LNA duplexes, consisting exclusively of 2′-O,4′-C-methylene-β-D-ribofuranose building blocks, yielded insights into a novel nucleic acid geometry. An “all LNA” duplex shows alterations in the local and overall helical parameters as compared to natural RNA and can rather be compared to other modified nucleic acids, like glycol nucleic acids (GNAs) [10], peptide nucleic acids (PNAs) [11], or homo-DNA [12]. An LNA duplex appears as a right-handed, antiparallel helix that maintains the canonical Watson-Crick base pairing and the 2′-exo conformation for all nucleotides. Nevertheless, the LNA duplex shows a considerable decrease in the helical twist, roll and propeller twist, which facilitates a widening of the major groove and a decrease of the minor groove dimensions. These alterations induce a large hollow cave in the middle of the duplex that is obvious in a projection perpendicular to the helical axis. Due to an enlarged helical rise and the unwinding of the helix, which results from the decrease in the twist angle parameters, the LNA duplex possesses an increased helical pitch. The unique nucleic acid geometry of “all LNA” helices apparently induces a more efficient and stable base stacking, which contributes to the higher thermostability of LNAs and LNA-modified nucleic acids. Interestingly, the structure of an RNA/LNA heteroduplex [13] is a geometric intermediate between the RNA and the “all LNA” conformation.

2. Material and Methods

2.1. Crystallization of the LNA Helices

The 7mer LNA helix was derived from the E. coli tRNA^Ser isoacceptor with the data base “Compilation of tRNA sequences and sequences of tRNA genes” ID RS 1661 [14] and represents the sequence of the aminoacyl stem microhelix that has been crystallized previously possessing the sequence 5′-(G-G-U-G-A-G-G-)-3′ and 5′-(C-C-U-C-A-C-C-)-3′ [15]. The LNA helix contained exclusively 2′-O,4′-C-methylene-β-D-ribofuranose building blocks. The base sequence of the RNA was maintained for further comparative studies, except for the U to T and the C to m⁵C exchange used in standard LNA synthesis. The chemically synthesized single strands with the sequences 5′-(G-G-T-G-A-G-G-3′ and 5′-(m⁵C-m⁵C-T-m⁵C-A-m⁵C-m⁵C-3′ were purchased from IBA (Göttingen, Germany) with HPLC purification grade. Crystals were grown within 3-4 days using 40 mM sodium cacodylate, pH 5.5, 20 mM cobalt hexamine, 80 mM sodium chloride, 20 mM magnesium chloride, and 10% (v/v) MPD with equilibration against 1 mL 33–41% (v/v) MPD at 21°C using the hanging drop vapour diffusion technique [16].

2.2. Diffraction Data Collection and Structure Determination and Refinement

Data collection of the LNA crystals was performed at the ELETTRA synchrotron (Trieste, Italy) beam line XRD-1 at a wavelength of 1.0 Å and a temperature of 100 K. The crystal diffracted up to 1.9 Å resolution [16]. The corresponding -microhelix was measured at the DESY synchrotron (Hamburg, Germany) at a wavelength of 0.8123 Å, 100 K temperature, and diffracted up to 1.2 Å [16]. All data were analyzed and processed using the programs from the HKL-2000 suite [17]. Molecular replacement calculations were performed using the program PHASER [18] within the CCP4i program suite [19]. The RNA structure was solved by molecular replacement using an artificially constructed RNA. The LNA structure was solved by using a model built from the previously solved microhelix structure but exchanging the riboses by 2′-O,4′-C-methylene-β-D-ribofuranose residues [9]. Standard LNA nucleotides were used for model building, which comprises the standard U to T and C to m⁵C substitutions in LNA as compared to RNA. Refinement calculations were done applying the program REFMAC [20], and electron density maps were calculated using FFT [21], as implemented in the CCP4i package [19]. Data and refinement statistics are shown in Table 1. The program X3DNA [22] was used to calculate the local and overall geometrical parameters. Structure representations and graphical analysis of helices were performed with the programs COOT [23] and PYMOL [24].

3. Results and Discussion

We analysed the crystal structure of a “locked” nucleic acid duplex [9], which contains exclusively 2′-O,4′-C-methylene-β-D-ribofuranose nucleotides (Figure 1), in comparison to the structures of the naturally occurring RNA as well as to other backbone-modified nucleic acids like glycol nucleic acids (GNAs) or peptide nucleic acids (PNAs).

(a)

(b)

The LNA helix structure reveals a nucleic acid duplex geometry that significantly differs from the canonical A-type RNA structure (Figure 2, Tables 2 and 3). The structure of the LNA duplex appears as a stretched helical ladder with altered local and overall geometric parameters. The observed geometry can be rather compared to that of glycol nucleic acids (GNAs) [25], peptide nucleic acids (PNAs) [26, 27], or homo-DNAs [12]. We detected a notable decrease in several local and overall helical parameters in the LNA helix, like the twist, roll and propeller twist, as compared to a corresponding RNA molecule (Table 2). This results in a widening of the major groove, a decrease in helical winding and an increased helical pitch. The major groove dimensions in the LNA duplex showed values of around 24-25 Å in diameter, as compared to 16 Å observed for the canonical A-RNA duplex. Concomitantly, the minor groove of LNA duplexes is narrower (about 15 Å) than that of standard RNA helices (19 Å). On the other hand, the slide and rise values are slightly increased in the LNA helices. Moreover, the shift of the base pairs in the LNA duplex results in an empty tunnel running through the center of the helix.

(a)

(b)

In the LNA helix, the low twist angle of 26° and the large pitch of 14 base pairs per turn lead to an unwinding of the duplex, as compared to RNA, which possesses a twist of 32° and a pitch of 11 base pairs per turn. The helical rise of LNA falls into a range of 2.8–3.0 Å, whereas the helical rise in RNA is 2.6 Å. Due to the increased rise and the unwinding of the helix, the LNA possessed an enlarged helical pitch of 39 Å, as compared to 29 Å in RNA helices. The backbone torsion angles resembled the sc⁻, ap⁺, sc⁺, sc⁺ ap, sc⁻, and ap⁺ conformation for the α, β, γ, δ, ε, ζ, and χ angles with the sugar puckering being in the 2′-exo conformation. The phosphate-phosphate distances are in the region of 5.6 Å as compared to 6.0 Å for RNA. It is conceivable that the altered helical parameters in LNA duplexes provide an enhancement in nucleotide stacking, leading towards stronger - interactions of the base pairs.

It is well accepted that the extensive hydration of the RNA minor groove plays an important role in the structure/function relationship [28]. As the specific hydration pattern of RNA is governed by the 2′-hydroxyl group, it has been questioned whether the 2′-O,4′-C-methylene-β-D-ribofuranose in LNA allows a comparable hydration as described for RNAs. Therefore, we focussed our investigations on analyzing the arrangement of the solvent molecules surrounding the LNA duplex. We observed that the distribution of water molecules in the LNA minor groove follows the general pattern known for RNA hydration, as the bridged 2′ oxygen atoms in the 2′-O,4′-C-methylene-β-D-ribofuranose moieties serve as hydrogen bond acceptors similar to the 2′-hydroxyl residues in RNA. An example for the LNA hydration is shown in Figure 3.

Interestingly, the structure of an RNA/LNA hybrid helix represents a geometric intermediate between RNA and “all LNA” helices. In Figure 4, we present the structure of idealized RNA as compared to the RNA/LNA hybrid (PDB ID: 1H0Q) and to the “all LNA” duplex (PDB ID: 2X2Q) as Calladine-Drew plot. To better visualize the overall geometry in this figure, the helices were extended to 22 base pairs for RNA, to 25 base pairs for RNA/LNA, and to 28 base pairs for LNA showing two full helical turns each [9]. For an overall comparison of A-RNA and B-DNA helices to the conformation of different backbone-modified nucleic acid types, like GNA and PNA (Figure 5), we displayed the selected nucleic acid helices with a total length of 46 base pairs (Figure 6). We illustrate the natural DNA and RNA and the synthetic GNA (PDB ID: 2JJA) and PNA (PDB ID: 1PUP) as compared to the LNA (PDB ID: 2X2Q) duplex structure. The standard A- and B-type nucleic acid conformations are paraphrased by the RNA and DNA helices. The GNA shows the structure of a helical ribbon with only one large minor groove and completely lacks the major groove, which is instead a convex surface [25]. The PNA resembles the helix with a wide and deep major groove concomitant with a narrow and shallow minor groove [26, 27]. The weakly twisted right-handed homo-DNA structure has been described to explain the inability of allo-, altro-, and glucanosyl-nucleotides to form stable base pairing systems (picture not shown) [12]. In the middle of Figure 6 we present the extended structure of the LNA duplex, which represents the unusual geometry, which can rather be brought into vicinity of GNA, PNA, and homo-DNA than to the natural nucleic acid duplexes DNA and RNA. The LNA helix, however, possesses a pitch of 39 Å with 14 base pairs per helical turn and an average rise of 2.8 Å. DNA and RNA show an average pitch of 30 Å and 34 Å, respectively, as compared to mean values of 60 Å, 58 Å, and 53 Å found for GNA, PNA, and homo-DNA. (Figure 6, Table 3, no data shown for homo-DNA). Conclusively, regarding the geometry of the LNA duplex in total, this helix resembles a more natural nucleic acid, when compared to the other backbone-modified duplexes.

(a)

(b)

(c)

(a)

(b)

(c)

(d)

Figure 6

Overall helical structures of natural nucleic acids (RNA and DNA) and of synthetic, modified nucleic acids (LNA, GNA, and PNA). All helices were extended to a total of 46 base pairs. The helices were constructed by using the following structures: DNA (idealized), RNA (idealized), LNA (PDB ID: 2X2Y), GNA (PDB ID: 2JJA), and PNA (PDB ID: 1PUP). Phosphate oxygen atoms are shown in blue, phosphates in yellow, and all other atoms are presented in grey. Top picture shows the side view of the duplexes and the bottom picture presents a projection along the helical axis.

As has been reviewed [4], an increase of the melting temperature between +2° to +10°C can be observed per LNA building block added in strands hybridized to RNA. The short 7 bp LNA duplex, derived from the microhelix for this study, exhibits a melting temperature of above 90°C, whereas the corresponding RNA has a value of 45.0°C [9]. We have previously investigated the melting temperature of another LNA 7mer helix in comparison to its natural RNA counterpart [29]. Similarly, the LNA duplex possesses a value of 84.3°C, whereas its corresponding RNA helix melts at 22.4°C. The drastic shift in thermostability in both LNAs as compared to the RNAs corresponds to an average of 4.5°C per nucleotide building block, which is consistent with the reviewed observations [4]. Thus, the thermostability data and the structure properties of LNAs provide new perspectives for future nucleic acid drug applications, which is an encouraging outlook.

Considering that the increase in values by substituting natural nucleic acids with single or multiple nucleotides by LNA residues seems to be a summative property, the challenge of using LNAs as tools in nucleic acid stabilization becomes obvious. Nearly any natural nucleic acid can be modified by introducing single and multiple LNA building blocks or even complete LNA duplexes, thereby stepwise increasing the thermostability depending on the number of introduced LNA residues. Depending on the particular requirements, any nucleic acid can thus be stabilized at will with little or no loss of function. In this respect, LNA substitution may serve as a reliable method to stabilize nucleic acids, in particular aptamers, for clinical applications.

An upcoming challenge is to stabilize aptamer stem regions by introducing LNA portions without affecting the loop regions that are usually essential for target binding and specificity. Several reports in the literature highlight a forthcoming application of LNA-substituted aptamers with retained or even improved ligand-binding capacity. An exciting example is the use of LNA modifications within hammerhead ribozymes that improve the overall cleaving capacity [30]. In addition, LNA modifications have successfully been introduced into antisense oligonucleotides and DNAzymes that were targeted to functionally selected binding sites and inhibited HIV-1 expression [31]. A third example describes a G-quadruplex thrombin aptamer, which retained the biological activity to a varying extent depending on the nucleotide positions that were LNA modified [32]. These selected reports are a snapshot of numerous studies demonstrating the great potential of LNA substitutions in functional nucleic acids and possible therapeutic applications. The crystal structure of the “all locked” nucleic acid helix contributes to the understanding of the structure/function relationship and the high thermostability of these molecules. In summary LNAs possess an encouraging potential for the development of new stabilized nucleic acids and will promote future applications in diagnostics, drug discovery, and clinical therapy [4].

Acknowledgments

This work was supported by the BiGRUDI network of the Robert Koch Institute (Berlin) financed by the Bundesministerium für Bildung und Forschung. A. Eichert was member of the Dahlem Research School of the Free University Berlin and funded by the Friedrich-Ebert-Stiftung, Germany, and is now supported by a DFG fellowship. We gratefully acknowledge the ELETTRA synchrotron, Trieste, Italy, and the DESY synchrotron, Hamburg, Germany for providing beam time and Ursula Erikli for copyediting the paper.

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Copyright © 2012 Charlotte Förster et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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