C4′/H4′ selective, non-uniformly sampled 4D HC(P)CH experiment for sequential assignments of 13C-labeled RNAs
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A through bond, C4′/H4′ selective, “out and stay” type 4D HC(P)CH experiment is introduced which provides sequential connectivity via H4′(i)–C4′(i)–C4′(i−1)–H4′(i−1) correlations. The 31P dimension (used in the conventional 3D HCP experiment) is replaced with evolution of better dispersed C4′ dimension. The experiment fully utilizes 13C-labeling of RNA by inclusion of two C4′ evolution periods. An additional evolution of H4′ is included to further enhance peak resolution. Band selective 13C inversion pulses are used to achieve selectivity and prevent signal dephasing due to the of C4′–C3′ and C4′–C5′ homonuclear couplings. For reasonable resolution, non-uniform sampling is employed in all indirect dimensions. To reduce sensitivity losses, multiple quantum coherences are preserved during shared-time evolution and coherence transfer delays. In the experiment the intra-nucleotide peaks are suppressed whereas inter-nucleotide peaks are enhanced to reduce the ambiguities. The performance of the experiment is verified on a fully 13C, 15N-labeled 34-nt hairpin RNA comprising typical structure elements.
KeywordsRNA resonance assignment HCP Selective pulses Four-dimensional NMR Non-uniform sampling
With the advent of several new classes of non-coding RNAs (e.g. siRNA, miRNAs) research has been heavily focused on understanding the role of RNA in cellular processes during normal and diseased states (Esteller 2011), through exploring its structure–function relationship (Briones et al. 2009; Mercer et al. 2009). Over the years, in conjunction with isotope labeling techniques, several NMR approaches (Varani et al. 1996; Wijmenga and van Buuren 1998; Furtig et al. 2003; Flinders and Dieckmann 2006) proved to be highly useful in expanding our knowledge about RNA structure, its basic structural motifs, catalysis and interactions with small molecules or proteins. However, precise structural determination of even moderately sized RNAs can still be problematic. In addition to low proton density in RNAs, these biopolymers comprise only four different nucleotides. Effectively, chemical shift dispersion is inherently low, which entails severe spectral overlaps. For non-coding RNAs a frequent lack of base stacking results in even increased crowding in the NMR spectra. Moreover, similar chemical shifts are observed for many nucleotides having similar chemical environment in helical secondary structures. Recently, automated assignment approach involving no isotope labeling (Aeschbacher et al. 2013) was proposed that requires peak lists from 2D TOCSY, 2D NOESY and natural abundance 1H–13C HSQC spectra. However, difficulty may arise while assigning regions/nuclei with irregular or limited statistics. In addition, chemical shift degeneracy or low dispersion still remain a bottleneck for such approaches. This suggests that new high dimensional techniques, resembling 4D/5D methods employed for intrinsically disordered proteins (Zawadzka-Kazimierczuk et al. 2012; Stanek et al. 2013b; Bermel et al. 2013) can be explored for the assignment of poorly resolved resonances in RNAs.
The sequential resonance assignment in RNA is usually achieved using through-space NOE-type (Nikonowicz and Pardi 1993) and/or through-bond HCP (Marino et al. 1994) experiments. The efficacy of both types of experiments is severely affected due to spectral crowding and overlaps, which increases dramatically with the size of RNA. To increase the peak resolution, experiments having HCP concatenated with HCCH-TOCSY were also proposed (Marino et al. 1995; Ramachandran et al. 1996), however, their application remained limited due to significant relaxation losses during TOCSY mixing time and limited resolution owing to relatively short maximum evolution times. In account of this, high resolution 4D C(aro),C(ribo)-NOESY experiment (Stanek et al. 2013a) was recently reported which aimed at providing the intra and inter-nucleotide (sequential) NOE correlations in RNA. As NOE interactions are largely dependent on conformations, ambiguities and gaps may arise during the assignment of NOESY spectrum, preventing the possible correlation of genuine peaks that may be present in the spectrum. These ambiguities can largely be resolved if the spectral analysis is complemented by some through-bond experiments. For example, the 3D HCP experiment, which provides sequential connectivity via intervening 31P nuclei, i.e. correlating H4′(i)–C4′(i)–P(i) with P(i)–C4′(i−1)–H4′(i−1), has been successful in many applications. However, it suffers from severe spectral overlaps (see Fig. S1a–d in Supplementary Materials) and relies on quite poor resolution of 31P dimension. In principle the peaks can be resolved in 31P dimension but in practice it is limited by its low chemical shift dispersion (~1.8 ppm) (see Fig. S1e), which makes unambiguous assignment of peaks a challenging task even for moderately sized RNAs. Additionally, in this experiment it is very difficult to unambiguously assign intra- and inter-nucleotide peaks (see Fig. S1b, c), especially when it relates to the most crowded, H4′C4′, region among sugar carbons. The possibility of sequential correlation through other sugar carbons, i.e. C3′(i−1) and C5′(i) is also hampered due to weak 31P–C3′/5′ couplings making such peaks either absent or too weak; the problem is further augmented by peak overlaps and presence of H5′/H5″ doublets. Clearly, more advanced approaches are needed to achieve an unambiguous sequential assignment in RNAs.
Since, as it was shown earlier for nucleic acids (Fiala et al. 1998, 2000), the dominant 1H–13C dipolar relaxation mechanism is significantly attenuated for zero- and double-quantum coherences, MQ coherences are preserved during the frequency labeling of both C4′ evolution periods. In the first MQ1 period (see Fig. 2), the coherence starts from H4′ in sugars and is transferred to C4′ via non-refocused INEPT. H4′ and C4′ are then brought into a MQ state and the shared-evolution of chemical shifts of H4′ (t 1) and C4′ (t 2) is performed in a constant-time manner by shifting the corresponding hard 180° pulses within the MQ1 period. In order to evolve C4′–P couplings and achieve a coherence transfer, a 180° pulse on 31P is applied simultaneously with the C4′ inversion pulse on 13C channel. During this period (τa), the evolution due to homonuclear carbon coupling (C4′–C3′ and C4′–C5′) is refocused by two cosine modulated IBURP-2 (Geen and Freeman 1991) pulses (P in Fig. 2) which selectively and simultaneously invert the frequency bands of C3′ and C5′ ribose sugar carbons. Since C2′ carbons share the same spectral region as of C3′, inversion of later also inverts the C2′ carbons. Effectively, the use of inversion pulses lead to an indirect selection of C4′ and hence H4′ during the MQ1 period. The next 90° pulse on H4′ and ∆ delay refocus the C4′ anti-phase to H4′ whereas the subsequent 90° pulses on C4′ and 31P transfer the coherence onto 31P.
In the next SQ period magnetization on 31P is brought into transverse plane and 31P–13C couplings are evolved. In the middle of this period a C4′ selective cosine modulated IBURP-2 pulse (Q in Fig. 2) is employed to prevent dephasing due to Pi–C3′i−1 and Pi–C5′i couplings and achieve selectivity for P → C4′ transfer.
The coherence transfer efficiency and hence the intensities are dependent on 3 J (C4′, P) values (discussed later in the text). The experiments are performed at various J values, however at ~10 Hz we found the least loss of number of resonances in the spectrum. The transverse relaxation rate (R) is estimated experimentally for 31P and intensities for both types of peaks are plotted (see Fig. S2 in Supplementary Materials), with increasing transfer delay (τb). A suitable delay (~38 ms for this study) is chosen to maximize the inter-nucleotide peak intensities, which in turn also minimizes the intra-nucleotide terms, especially in the cases where 3 J (C4′i, Pi) ≈ 3 J (Pi,C4′i−1).
In the consecutive block MQ2, the coherence is forward transferred to C4′(i) where its chemical shifts are indirectly recorded (t 3) preserving the MQ coherences similarly to the MQ1 block in the sequence. During the same period (τc) refocusing of P–C4′ couplings is also achieved by application of a 180° pulse on 31P in synchrony with the moving 180° pulse on 13C channel. Another 180° pulse is centrally placed on 1H channel to refocus its chemical shift evolution. Again, the use of C3′/C5′ selective IBURP-2 pulses (P in Fig. 2) prevents the evolution due to C4′–C3′/5′ homonuclear couplings and indirectly selects C4′/H4′. Finally, an in-phase coherence is generated on H4′ spins by refocused INEPT transfer during ∆ period.
The inversion profiles for shaped pulses were simulated and tested using Spinach library (Hogben et al. 2011) on MATLAB®. Gradients and phase cycling are employed to eliminate undesired coherences and improve the C4′/H4′ selectivity of experiment. After P → C4′ transfer period, spin-lock pulses (SLx, SLy) are employed (W in Fig. 2) to dephase any remaining transverse water magnetization. The experiment complements the set of recently reported high dimensional experiments, 5D HCP-CCH COSY (Krahenbuhl et al. 2014) and 4D-NUS C(aro),C(ribo)-NOESY (Stanek et al. 2013a), dedicated for sequential resonance assignment in RNAs.
To achieve higher dimensionality with reasonable resolution in the indirectly detected dimensions, non-uniform sampling (NUS) was employed. Using NUS we are able to acquire 4D HC(P)CH experiment with high evolution times: 20 ms (t 1), 14 ms (t 2) and 14 ms (t 3). The processing of 4D NUS data was accomplished by the home-written software package Signal Separation Algorithm (SSA) (Stanek et al. 2012), which can be downloaded free of charge for non-commercial purposes from the website http://nmr.cent3.uw.edu.pl.
To conclude, we have introduced a through-bond, C4′/H4′ selective, non-uniformly sampled 4D HC(P)CH experiment for sequential assignments in RNAs. The incorporated indirect dimensions, along with the replacement of evolution of 31P by 13C4′, significantly enhanced the spectral dispersion. NUS was employed to achieve high resolution in all the indirectly detected dimensions. Band selective inversion pulses were used to prevent signal modulation due to C4′–C3′, C4′–C5′ couplings and to indirectly select the C4′/H4′ region. Experiment involved the suppression of intra-nucleotide peaks, as a result, the number of ambiguities were further reduced. We have demonstrated that the C4′/H4′ selectivity and attenuated relaxation of MQ coherences partially compensated the sensitivity losses entailing the increased dimensionality. Despite lower sensitivity, the proposed experiment clearly outperforms the conventional HCP experiment, which suffers from critical overlap in the “linking” 31P dimension. The experiment is proposed as a complementary tool to 3D/4D NOESY experiments and augments the set of high dimensional experiments aimed at improving resolution and reducing ambiguities during resonance assignments in RNAs with poor chemical shift dispersion.
This work was supported by TEAM project operated within the Foundation for Polish Science. S.S. and W.K. thank Polish National Science Centre for the financial support with the Grant No. 2013/11/N/ST4/01827. The research was co-financed from Polish budget funds for science for years 2013–2014, the project No. IP2012 057872 (J.S.). M.C. and J.P. thank Slovenian Research Agency (ARRS, P1-242 and J1-6733). The study was carried out at the Biological and Chemical Research Centre, University of Warsaw, established within the project co-financed by European Union from the European Regional Development Fund under the Operational Programme Innovative Economy.
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