Comparison of <Superscript>13</Superscript>CH<Subscript>3</Subscript>, <Superscript>13</Superscript>CH<Subscript>2</Subscript>D,and <Superscript>13</Superscript>CHD<Subscript>2</Subscript> methyl labeling strategies in proteins

A comparison of three labeling strategies for studies involving side chain methyl groups in high molecular weight proteins, using ¹³CH₃,¹³CH₂D, and ¹³CHD₂ methyl isotopomers, is presented. For each labeling scheme, ¹H–¹³C pulse sequences that give optimal resolution and sensitivity are identified. Three highly deuterated samples of a 723 residue enzyme, malate synthase G, with ¹³CH₃,¹³CH₂D, and ¹³CHD₂ labeling in Ile δ1 positions, are used to test the pulse sequences experimentally, and a rationalization of each sequence’s performance based on a product operator formalism that focuses on individual transitions is presented. The HMQC pulse sequence has previously been identified as a transverse relaxation optimized experiment for ¹³CH₃-labeled methyl groups attached to macromolecules, and a zero-quantum correlation pulse scheme (¹³CH₃ HZQC) has been developed to further improve resolution in the indirectly detected dimension. We present a modified version of the ¹³CH₃ HZQC sequence that provides improved sensitivity by using the steady-state magnetization of both ¹³C and ¹H spins. The HSQC and HMQC spectra of ¹³CH₂D-labeled methyl groups in malate synthase G are very poorly resolved, but we present a new pulse sequence, ¹³CH₂D TROSY, that exploits cross-correlation effects to record ¹H–¹³C correlation maps with dramatically reduced linewidths in both dimensions. Well-resolved spectra of ¹³CHD₂-labeled methyl groups can be recorded with HSQC or HMQC; a new ¹³CHD₂ HZQC sequence is described that provides improved resolution with no loss in sensitivity in the applications considered here. When spectra recorded on samples prepared with the three isotopomers are compared, it is clear that the ¹³CH₃ labeling strategy is the most beneficial from the perspective of sensitivity (gains ≥2.4 relative to either ¹³CH₂D or ¹³CHD₂ labeling), although excellent resolution can be obtained with any of the isotopomers using the pulse sequences presented here.     

Direct amide <Superscript>15</Superscript>N to <Superscript>13</Superscript>C transfers for solid-state assignment experiments in deuterated proteins

The assignment of protein backbone and side-chain NMR chemical shifts is the first step towards the characterization of protein structure. The recent introduction of proton detection in combination with fast MAS has opened up novel opportunities for assignment experiments. However, typical 3D sequential-assignment experiments using proton detection under fast MAS lead to signal intensities much smaller than the theoretically expected ones due to the low transfer efficiency of some of the steps. Here, we present a selective 3D experiment for deuterated and (amide) proton back-exchanged proteins where polarization is directly transferred from backbone nitrogen to selected backbone or sidechain carbons. The proposed pulse sequence uses only ¹H–¹⁵N cross-polarization (CP) transfers, which are, for deuterated proteins, about 30% more efficient than ¹H–¹³C CP transfers, and employs a dipolar version of the INEPT experiment for N–C transfer. By avoiding H^N–C (H^N stands for amide protons) and C–C CP transfers, we could achieve higher selectivity and increased signal intensities compared to other pulse sequences containing long-range CP transfers. The REDOR transfer is designed with an additional selective π pulse, which enables the selective transfer of the polarization to the desired ¹³C spins.     

HNCO-based measurement of one-bond amide <Superscript>15</Superscript>N-<Superscript>1</Superscript>H couplings with optimized precision

A pair of 3D HNCO-based experiments have been developed with the aim of optimizing the precision of measurement of ¹J_NH couplings. Both pulse sequences record ¹J_NH coupling evolution during the entire constant time interval that ¹⁵N magnetization is dephasing or rephasing with respect to the directly bonded ¹³C′ nucleus, with ¹⁵N¹³C′ multiple quantum coherence maintained during the ¹³C′ evolution period. The first experiment, designed for smaller proteins, produces an apparent doubling of the ¹J_NH coupling without any accompanying increases in line width. The second experiment is a J-scaled TROSY-HNCO experiment in which the ¹J_NH coupling is measured by frequency difference between resonances offset symmetrically about the position of the downfield component of the ¹⁵N doublet (i.e. the TROSY resonance). This experiment delivers significant gains in precision of ¹J_NH coupling measurement compared to existing J-scaled TROSY-HNCO experiments. With the proper choice of acquisition parameters and sufficient sensitivity to acquire a 3D TROSY-HNCO experiment, it is shown that ¹J_NH couplings can be measured with a precision which approaches or exceeds the precision of measurement with which the frequency of the TROSY resonance itself can be determined.     

<Superscript>15</Superscript>N and <Superscript>13</Superscript>C- SOFAST-HMQC editing enhances 3D-NOESY sensitivity in highly deuterated,selectively [<Superscript>1</Superscript>H,<Superscript>13</Superscript>C]-labeled proteins

The ongoing NMR method development effort strives for high quality multidimensional data with reduced collection time. Here, we apply ‘SOFAST-HMQC’ to frequency editing in 3D NOESY experiments and demonstrate the sensitivity benefits using highly deuterated and ¹⁵N, methyl labeled samples in H₂O. The experiments benefit from a combination of selective T ₁ relaxation (or L-optimized effect), from Ernst angle optimization and, in certain types of experiments, from using the mixing time for both NOE buildup and magnetization recovery. This effect enhances sensitivity by up to 2.4× at fast pulsing versus reference HMQC sequences of same overall length and water suppression characteristics. Representative experiments designed to address interesting protein NMR challenges are detailed. Editing capabilities are exploited with heteronuclear ¹⁵N,¹³C-edited, or with diagonal-free ¹³C aromatic/methyl-resolved 3D-SOFAST-HMQC–NOESY–HMQC. The latter experiment is used here to elucidate the methyl-aromatic NOE network in the hydrophobic core of the 19 kDa FliT-FliJ flagellar protein complex. Incorporation of fast pulsing to reference experiments such as 3D-NOESY–HMQC boosts digital resolution, simplifies the process of NOE assignment and helps to automate protein structure determination.     

(3, 2)D <Superscript>1</Superscript>H, <Superscript>13</Superscript>C BIRD<Superscript>r,X</Superscript>-HSQC-TOCSY for NMR structure elucidation of mixtures: application to complex carbohydrates

Overlap of NMR signals is the major cause of difficulties associated with NMR structure elucidation of molecules contained in complex mixtures. A 2D homonuclear correlation spectroscopy in particular suffers from low dispersion of ¹H chemical shifts; larger dispersion of ¹³C chemical shifts is often used to reduce this overlap, while still providing the proton–proton correlation information e.g. in the form of a 2D ¹H, ¹³C HSQC-TOCSY experiment. For this methodology to work, ¹³C chemical shift must be resolved. In case of ¹³C chemical shifts overlap, ¹H chemical shifts can be used to achieve the desired resolution. The proposed (3, 2)D ¹H, ¹³C BIRD^r,X-HSQC-TOCSY experiment achieves this while preserving singlet character of cross peaks in the F₁ dimension. The required high-resolution in the ¹³C dimension is thus retained, while the cross peak overlap occurring in a regular HSQC-TOCSY experiment is eliminated. The method is illustrated on the analysis of a complex carbohydrate mixture obtained by depolymerisation of a fucosylated chondroitin sulfate isolated from the body wall of the sea cucumber Holothuria forskali.     

HNCA-TOCSY-CANH experiments with alternate <Superscript>13</Superscript>C-<Superscript>12</Superscript>C labeling: a set of 3D experiment with unique supra-sequential information for mainchain resonance assignment

Described here is a set of three-dimensional (3D) NMR experiments that rely on CACA-TOCSY magnetization transfer via the weak ³ \textJ_{\textCa\textCa} ^{ 3} {\text{J}}_{{{\text{C}}\alpha {\text{C}}\alpha }} coupling. These pulse sequences, which resemble recently described ¹³C detected CACA-TOCSY (Takeuchi et al. 2010) experiments, are recorded in ¹H₂O, and use ¹H excitation and detection. These experiments require alternate ¹³C-¹²C labeling together with perdeuteration, which allows utilizing the small ³ \textJ_{\textCa\textCa} ^{ 3} {\text{J}}_{{{\text{C}}\alpha {\text{C}}\alpha }} scalar coupling that is otherwise masked by the stronger ¹J_CC couplings in uniformly ¹³C labeled samples. These new experiments provide a unique assignment ladder-mark that yields bidirectional supra-sequential information and can readily straddle proline residues. Unlike the conventional HNCA experiment, which contains only sequential information to the ^{1 3} \textC^a ^{ 1 3} {\text{C}}^{\alpha } of the preceding residue, the 3D hnCA-TOCSY-caNH experiment can yield sequential correlations to alpha carbons in positions i−1, i + 1 and i−2. Furthermore, the 3D hNca-TOCSY-caNH and Hnca-TOCSY-caNH experiments, which share the same magnetization pathway but use a different chemical shift encoding, directly couple the ¹⁵N-¹H spin pair of residue i to adjacent amide protons and nitrogens at positions i−2, i−1, i + 1 and i + 2, respectively. These new experimental features make protein backbone assignments more robust by reducing the degeneracy problem associated with the conventional 3D NMR experiments.     

Automated amino acid side-chain NMR assignment of proteins using <Superscript>13</Superscript>C- and <Superscript>15</Superscript>N-resolved 3D [<Superscript>1</Superscript>H,<Superscript>1</Superscript>H]-NOESY

ASCAN is a new algorithm for automatic sequence-specific NMR assignment of amino acid side-chains in proteins, which uses as input the primary structure of the protein, chemical shift lists of (1)H(N), (15)N, (13)C(alpha), (13)C(beta) and possibly (1)H(alpha) from the previous polypeptide backbone assignment, and one or several 3D (13)C- or (15)N-resolved [(1)H,(1)H]-NOESY spectra. ASCAN has also been laid out for the use of TOCSY-type data sets as supplementary input. The program assigns new resonances based on comparison of the NMR signals expected from the chemical structure with the experimentally observed NOESY peak patterns. The core parts of the algorithm are a procedure for generating expected peak positions, which is based on variable combinations of assigned and unassigned resonances that arise for the different amino acid types during the assignment procedure, and a corresponding set of acceptance criteria for assignments based on the NMR experiments used. Expected patterns of NOESY cross peaks involving unassigned resonances are generated using the list of previously assigned resonances, and tentative chemical shift values for the unassigned signals taken from the BMRB statistics for globular proteins. Use of this approach with the 101-amino acid residue protein FimD(25-125) resulted in 84% of the hydrogen atoms and their covalently bound heavy atoms being assigned with a correctness rate of 90%. Use of these side-chain assignments as input for automated NOE assignment and structure calculation with the ATNOS/CANDID/DYANA program suite yielded structure bundles of comparable quality, in terms of precision and accuracy of the atomic coordinates, as those of a reference structure determined with interactive assignment procedures. A rationale for the high quality of the ASCAN-based structure determination results from an analysis of the distribution of the assigned side chains, which revealed near-complete assignments in the core of the protein, with most of the incompletely assigned residues located at or near the protein surface.     

<Superscript>1</Superscript>H, <Superscript>15</Superscript>N,and <Superscript>13</Superscript>C chemical shift assignments of the regulatory domain of human calcineurin

Calcineurin (CaN) plays an important role in T-cell activation, cardiac system development and nervous system function. Previous studies have demonstrated that the regulatory domain (RD) of CaN binds calmodulin (CaM) towards the N-terminal end. Calcium-loaded CaM activates the serine/threonine phosphatase activity of CaN by binding to the RD, although the mechanistic details of this interaction remain unclear. It is thought that CaM binding at the RD displaces the auto-inhibitory domain (AID) from the active site of CaN, activating phosphatase activity. In the absence of calcium-loaded CaM, the RD is disordered, and binding of CaM induces folding in the RD. In order to provide mechanistic detail about the CaM–CaN interaction, we have undertaken an NMR study of the RD of CaN. Complete ¹³C, ¹⁵N and ¹H assignments of the RD of CaN were obtained using solution NMR spectroscopy. The backbone of RD has been assigned using a combination of ¹³C-detected CON-IPAP experiments as well as traditional HNCO, HNCA, HNCOCA and HNCACB-based 3D NMR spectroscopy. A ¹⁵N-resolved TOCSY experiment has been used to assign Hα and Hβ chemical shifts.     

Speeding up direct <Superscript>15</Superscript>N detection: hCaN 2D NMR experiment

Experiments detecting low gyromagnetic nuclei have recently been proposed to utilize the relatively slow relaxation properties of these nuclei in comparison to ¹H. Here we present a new type of ¹⁵N direct-detection experiment. Like the previously proposed CaN experiment (Takeuchi et al. in J Biomol NMR 47:271–282, 2010), the hCaN experiment described here sequentially connects amide ¹⁵N resonances, but utilizes the initial high polarization and the faster recovery of the ¹H nucleus to shorten the recycling delay. This allows recording 2D ¹⁵N-detected NMR experiments on proteins within a few hours, while still obtaining superior resolution for ¹³C and ¹⁵N, establishing sequential assignments through prolines, and at conditions where amide protons exchange rapidly. The experiments are demonstrated on various biomolecules, including the small globular protein GB1, the 22 kDa HEAT2 domain of eIF4G, and an unstructured polypeptide fragment of NFAT1, which contains many SerPro sequence repeats.     

BEST and SOFAST experiments for resonance assignment of histidine and tyrosine side chains in <Superscript>13</Superscript>C/<Superscript>15</Superscript>N labeled proteins

Aromatic amino-acid side chains are essential components for the structure and function of proteins. We present herein a set of NMR experiments for time-efficient resonance assignment of histidine and tyrosine side chains in uniformly ¹³C/¹⁵N-labeled proteins. The use of band-selective ¹³C pulses allows to deal with linear chains of coupled spins, thus avoiding signal loss that occurs in branched spin systems during coherence transfer. Furthermore, our pulse schemes make use of longitudinal ¹H relaxation enhancement, Ernst-angle excitation, and simultaneous detection of ¹H and ¹³C steady-state polarization to achieve significant signal enhancements.     

An enhanced sensitivity methyl <Superscript>1</Superscript>H triple-quantum pulse scheme for measuring diffusion constants of macromolecules

We present a pulse scheme that exploits methyl ¹H triple-quantum (TQ) coherences for the measurement of diffusion rates of slowly diffusing molecules in solution. It is based on the well-known stimulated echo experiment, with encoding and decoding of TQ coherences. The size of quantifiable diffusion coefficients is thus lowered by an order of magnitude with respect to single-quantum (SQ) approaches. Notably, the sensitivity of the scheme is high, approximately ¾ that of the corresponding single quantum experiment, neglecting relaxation losses, and on the order of a factor of 4 more sensitive than a previously published sequence for AX₃ spin systems (Zheng et al. in JMR 198:271–274, 2009) for molecules that are only ¹³C labeled at the methyl carbon position. Diffusion coefficients measured from TQ- and SQ-based experiments recorded on a range of protein samples are in excellent agreement. We present an application of this technique to the study of phase-separated proteins where protein concentrations in the condensed phase can exceed 400 mg/mL, diffusion coefficients can be as low as ~10^?9 cm²s^?1 and traditional SQ experiments fail.     

Probing slow timescale dynamics in proteins using methyl <Superscript>1</Superscript>H CEST

Although ¹⁵N- and ¹³C-based chemical exchange saturation transfer (CEST) experiments have assumed an important role in studies of biomolecular conformational exchange, ¹H CEST experiments are only beginning to emerge. We present a methyl-TROSY ¹H CEST experiment that eliminates deleterious ¹H–¹H NOE dips so that CEST profiles can be analyzed robustly to extract methyl proton chemical shifts of rare protein conformers. The utility of the experiment, along with a version that is optimized for ¹³CHD₂ labeled proteins, is established through studies of exchanging protein systems. A comparison between methyl ¹H CEST and methyl ¹H CPMG approaches is presented to highlight the complementarity of the two experiments.     

HNHC: a triple resonance experiment for correlating the H2, N1(N3) and C2 resonances in adenine nucleobases of <Superscript>13</Superscript>C-, <Superscript>15</Superscript>N-labeled RNA oligonucleotides

A novel NMR pulse sequence has been developed that correlates the H2 resonances with the C2 and the N1 (N3) resonances in adenine nucleobases of ¹³C, ¹⁵N labeled oligonucleotides. The pulse scheme of the new 3D-HNHC experiment is composed of a ²J-¹⁵N-HSQC and a ¹J-¹³C-HSQC and utilizes large ²J(H2, N1(N3)) and ¹J(H2, C2) couplings. The experiment was applied to a medium-size ¹³C, ¹⁵N-labeled 36mer RNA. It is useful to resolve assignment ambiguities occurring especially in larger RNA molecules due to resonance overlap in the ¹H-dimension. Therefore, the missing link in correlating the imino H3 resonances of the uracils across the AU base pair to the H8 resonances of the adenines via the novel pulse sequence and the TROSY relayed HCCH-COSY (Simon et al. in J Biomol NMR 20:173–176 2001) is provided. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

Selective <Superscript>1</Superscript>H-<Superscript>13</Superscript>C NMR spectroscopy of methyl groups in residually protonated samples of large proteins

Methyl ¹³CHD₂ isotopomers of all methyl-containing amino-acids can be observed in residually protonated samples of large proteins obtained from [U-¹³C,¹H]-glucose/D₂O-based bacterial media, with sensitivity sufficient for a number of NMR applications. Selective detection of some subsets of methyl groups (Ala^β, Thr^γ2) is possible using simple ‘out-and-back’ NMR methodology. Such selective methyl-detected ‘out-and-back’ NMR experiments allow complete assignments of threonine γ2 methyls in residually protonated, [U-¹³C,¹H]-glucose/D₂O-derived samples of an 82-kDa enzyme Malate Synthase G. [U-¹³C,¹H]-glucose/D₂O-derived protein samples are relatively inexpensive and are usually available at very early stages of any NMR study of high-molecular-weight systems.     

Critical test of some computational methods for prediction of NMR <Superscript>1</Superscript>H and <Superscript>13</Superscript>C chemical shifts

Performance of 18 DFT functionals (B1B95, B3LYP, B3PW91, B97D, BHandHLYP, BMK, CAM-B3LYP, HSEh1PBE, M06-L, mPW1PW91, O3LYP, OLYP, OPBE, PBE1PBE, tHCTHhyb, TPSSh, wB97xD, VSXC) in combinations with six basis sets (cc-pVDZ, aug-cc-pVDZ, cc-pVTZ, aug-cc-pVTZ, IGLO-II, and IGLO-III) and three methods for calculating magnetic shieldings (GIAO, CSGT, IGAIM) was tested for predicting ¹H and ¹³C chemical shifts for 25 organic compounds, for altogether 86 H and 88 C atoms. Proton shifts varied between 1.03 ppm to 12.00 ppm and carbon shifts between 7.87 ppm to 209.28 ppm. It was found that the best method for calculating ¹³C shifts is PBE1PBE/aug-cc-pVDZ with CSGT or IGAIM approaches (mae?=?1.66 ppm), for ¹H the best results were obtained with HSEh1PBE, mPW1PW91, PBE1PBE, CAM-B3LYP, and B3PW91 functionals with cc-pVTZ basis set and with CSGT or IGAIM approaches (mae?=?0.28 ppm). We found that often larger basis sets do not give better results for chemical shifts. The best basis sets for calculating ¹H and ¹³C chemical shifts were cc-pVTZ and aug-cc-pVDZ, respectively. CSGT and IGAIM NMR approaches can perform really well and are in most cases better than popular GIAO approach.

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Graphical Abstract Mean absolute errors for ¹H and ¹³C chemical shifts and computational times of neutral toluene molecule with aug-cc-pVDZ basis set and CSGT approach

     

Resolution-optimized NMR measurement of <Superscript>1</Superscript>D<Subscript>CH</Subscript>, <Superscript>1</Superscript>D<Subscript>CC</Subscript> and <Superscript>2</Superscript>D<Subscript>CH</Subscript> residual dipolar couplings in nucleic acid bases

New methods are described for accurate measurement of multiple residual dipolar couplings in nucleic acid bases. The methods use TROSY-type pulse sequences for optimizing resolution and sensitivity, and rely on the E.COSY principle to measure the relatively small two-bond ²D_CH couplings at high precision. Measurements are demonstrated for a 24-nt stem-loop RNA sequence, uniformly enriched in ¹³C, and aligned in Pf1. The recently described pseudo-3D method is used to provide homonuclear ¹H-¹H decoupling, which minimizes cross-correlation effects and optimizes resolution. Up to seven ¹H-¹³C and ¹³C-¹³C couplings are measured for pyrimidines (U and C), including ¹D_C5H5, ¹D_C6H6, ²D_C5H6, ²D_C6H5, ¹D_C5C4, ¹D_C5C6, and ²D_C4H5. For adenine, four base couplings (¹D_C2H2, ¹D_C8H8, ¹D_C4C5, and ¹D_C5C6) are readily measured whereas for guanine only three couplings are accessible at high relative accuracy (¹D_C8H8, ¹D_C4C5, and ¹D_C5C6). Only three dipolar couplings are linearly independent in planar structures such as nucleic acid bases, permitting cross validation of the data and evaluation of their accuracies. For the vast majority of dipolar couplings, the error is found to be less than ±3% of their possible range, indicating that the measurement accuracy is not limiting when using these couplings as restraints in structure calculations. Reported isotropic values of the one- and two-bond J couplings cluster very tightly for each type of nucleotide.     

1-<Superscript>13</Superscript>C amino acid selective labeling in a <Superscript>2</Superscript>H<Superscript>15</Superscript>N background for NMR studies of large proteins

Isotope labeling by residue type (LBRT) has long been an important tool for resonance assignments at the limit where other approaches, such as triple-resonance experiments or NOESY methods do not succeed in yielding complete assignments. While LBRT has become less important for small proteins it can be the method of last resort for completing assignments of the most challenging protein systems. Here we present an approach where LBRT is achieved by adding protonated ¹⁴N amino acids that are ¹³C labeled at the carbonyl position to a medium for uniform deuteration and ¹⁵N labeling. This has three important benefits over conventional ¹⁵N LBRT in a deuterated back ground: (1) selective TROSY-HNCO cross peaks can be observed with high sensitivity for amino-acid pairs connected by the labeling, and the amide proton of the residue following the ¹³C labeled amino acid is very sharp since its alpha position is deuterated, (2) the ¹³C label at the carbonyl position is less prone to scrambling than the ¹⁵N at the α-amino position, and (3) the peaks for the 1-¹³C labeled amino acids can be identified easily from the large intensity reduction in the ¹H-¹⁵N TROSY-HSQC spectrum for some residues that do not significantly scramble nitrogens, such as alanine and tyrosine. This approach is cost effective and has been successfully applied to proteins larger than 40 kDa. Electronic Supplementary Material The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

<Superscript>1</Superscript>H, <Superscript>13</Superscript>C and <Superscript>15</Superscript>N backbone resonance assignment of the lamin C-terminal region specific to prelamin A

Lamins are the main components of the nucleoskeleton. They form a protein meshwork that underlies the inner nuclear membrane. Mutations in the LMNA gene coding for A-type lamins (lamins A and C) cause a large panel of human diseases, referred to as laminopathies. These diseases include muscular dystrophies, lipodystrophies and premature aging diseases. Lamin A exhibits a C-terminal region that is different from lamin C and is post-translationally modified. It is produced as prelamin A and it is then farnesylated, cleaved, carboxymethylated and cleaved again in order to become mature lamin A. In patients with the severe Hutchinson–Gilford progeria syndrome, a specific single point mutation in LMNA leads to an aberrant splicing of the LMNA gene preventing the post-translational processing of prelamin A. This leads to the accumulation of a permanently farnesylated lamin A mutant lacking 50 amino acids named progerin. We here report the NMR ¹H, ¹⁵N, ¹³CO, ¹³Cα and ¹³Cβ chemical shift assignment of the C-terminal region that is specific to prelamin A, from amino acid 567 to amino acid 664. We also report the NMR ¹H, ¹⁵N, ¹³CO, ¹³Cα and ¹³Cβ chemical shift assignment of the C-terminal region of the progerin variant, from amino acid 567 to amino acid 614. Analysis of these chemical shift data confirms that both prelamin A and progerin C-terminal domains are largely disordered and identifies a common partially populated α-helix from amino acid 576 to amino acid 585. This helix is well conserved from fishes to mammals.     

Simultaneous <Superscript>1</Superscript>H- or <Superscript>2</Superscript>H-, <Superscript>15</Superscript>N- and multiple-band-selective <Superscript>13</Superscript>C-decoupling during acquisition in <Superscript>13</Superscript>C-detected experiments with proteins and oligonucleotides

Significant resolution improvement in ¹³C,¹³C-TOCSY spectra of uniformly deuterated and ¹³C, ¹⁵N-labeled protein and ¹³C,¹⁵N-labeled RNA samples is achieved by introduction of multiple-band-selective ¹³C-homodecoupling applied simultaneously with ¹H- or ²H- and ¹⁵N-decoupling at all stages of multidimensional experiments including signal acquisition period. The application of single, double or triple band-selective ¹³C-decoupling in 2D-[¹³C,¹³C]-TOCSY experiments during acquisition strongly simplifies the homonuclear splitting pattern. The technical aspects of complex multiple-band homonuclear decoupling and hardware requirements are discussed. The use of this technique (i) facilitates the resonance assignment process as it reduces signal overlap in homonuclear ¹³C-spectra and (ii) possibly improves the signal-to-noise ratio through multiplet collapse. It can be applied in any ¹³C-detected experiment.     

TEDOR with adiabatic inversion pulses: Resonance assignments of <Superscript>13</Superscript>C/<Superscript>15</Superscript>N labelled RNAs

We have examined via numerical simulations the performance characteristics of different 15N RF pulse schemes employed in the transferred echo double resonance (TEDOR) experimental protocol for generating 13C-15N dipolar chemical shift correlation spectra of isotopically labelled biological systems at moderate MAS frequencies (omega(r) approximately 10 kHz). With an 15N field strength of approximately 30-35 kHz that is typically available in 5 mm triple resonance MAS NMR probes, it is shown that a robust TEDOR sequence with significant tolerance to experimental imperfections sa as H1 inhomogeneity and resonance offsets can be effectively implemented using adiabatic heteronuclear dipolar recoupling pulse schemes. TEDOR-based 15N-13C and 15N-13C-13C chemical shift correlation experiments were carried out for obtaining 13C and 15N resonance assignments of an RNA composed of 97 (CUG) repeats which has been implicated in the neuromuscular disease myotonic dystrophy.