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Atomic-level information about the structure and dynamics of biomolecules is critical for an understanding of their function. Nuclear magnetic resonance (NMR) spectroscopy provides unique insights into the dynamic nature of biomolecules and their interactions, capturing transient conformers and their features. However, relaxation-induced line broadening and signal overlap make it challenging to apply NMR spectroscopy to large biological systems. Here we took advantage of the high sensitivity and broad chemical shift range of 19 F nuclei and leveraged the remarkable relaxation properties of the aromatic 19 F- 13 C spin pair to disperse 19 F resonances in a two-dimensional transverse relaxation-optimized spectroscopy spectrum. We demonstrate the application of 19 F- 13 C transverse relaxation-optimized spectroscopy to investigate proteins and nucleic acids. This experiment expands the scope of 19 F NMR in the study of the structure, dynamics, and function of large and complex biological systems and provides a powerful background-free NMR probe.

In this study, a set of nuclear magnetic resonance experiments, some of them commonly used in the study of (13)C-labeled proteins and/or nucleic acids, is applied for the structure determination of uniformly (13)C-enriched carbohydrates. Two model substances were employed: one compound of low molecular weight [(UL-(13)C)-sucrose, 342 Da] and one compound of medium molecular weight ((13)C-enriched O-antigenic polysaccharide isolated from Escherichia coli O142, ~10 kDa). The first step in this approach involves the assignment of the carbon resonances in each monosaccharide spin system using the anomeric carbon signal as the starting point. The (13)C resonances are traced using (13)C-(13)C correlations from homonuclear experiments, such as (H)CC-CT-COSY, (H)CC-NOESY, CC-CT-TOCSY and/or virtually decoupled (H)CC-TOCSY. Based on the assignment of the (13)C resonances, the (1)H chemical shifts are derived in a straightforward manner using one-bond (1)H-(13)C correlations from heteronuclear experiments (HC-CT-HSQC). In order to avoid the (1) J CC splitting of the (13)C resonances and to improve the resolution, either constant-time (CT) in the indirect dimension or virtual decoupling in the direct dimension were used. The monosaccharide sequence and linkage positions in oligosaccharides were determined using either (13)C or (1)H detected experiments, namely CC-CT-COSY, band-selective (H)CC-TOCSY, HC-CT-HSQC-NOESY or long-range HC-CT-HSQC. However, due to the short T2 relaxation time associated with larger polysaccharides, the sequential information in the O-antigen polysaccharide from E. coli O142 could only be elucidated using the (1)H-detected experiments. Exchanging protons of hydroxyl groups and N-acetyl amides in the (13)C-enriched polysaccharide were assigned by using HC-H2BC spectra. The assignment of the N-acetyl groups with (15)N at natural abundance was completed by using HN-SOFAST-HMQC, HNCA, HNCO and (13)C-detected (H)CACO spectra.

Three improved ¹³C-spinlock experiments for side chain assignments of isotope labelled proteins in liquid state are presented. These are based on wide bandwidth spinlock techniques that have become possible with contemporary cryogenic probes. The first application, the H(C(ali)C(aro))H-TOCSY, is an HCCH-TOCSY in which all CHn moieties of a protein are detected in a single experiment, including the aromatic ones. This enables unambiguous assignment of aromatic and aliphatic amino acids in a single, highly sensitive experiment. In the second application, the ¹³C-detected C(all)-TOCSY, magnetization transfer comprises all carbons--aliphatic, aromatic as well as the carbonyl carbons--making the complete carbon assignment possible using one spectrum only. Thirdly, the frequently used HC(CCO)NH experiment was redesigned by replacing the long C-carbonyl refocused INEPT transfer step by direct ¹³C-¹³C-TOCSY magnetization transfer from side chain carbons to the backbone carbonyls. The resulting HC(CCO)NH experiment minimizes relaxation losses because it is shorter and represents a more sensitive alternative particularly for larger proteins. The performance of the experiments is demonstrated on isotope labeled proteins up to the size of 43 kDa.

Using the case of the catalytic domain of MMP-12 in complex with the known inhibitor CGS27023A, a recently assembled 3D (15)N-edited/(14)N,(12)C-filtered ROESY experiment is used to monitor and distinguish protein amide protons in fast exchange with bulk water from amide protons close to water molecules with longer residence times, the latter possibly reflecting water molecules of structural or functional importance. The (15)N-edited/(14)N,(12)C-filtered ROESY spectra were compared to the original (15)N-edited/(14)N,(12)C-filtered NOESY and the conventional amide-water exchange experiment, CLEANEX. Three protein backbone amide protons experiencing direct dipolar cross relaxation with water in the (15)N-edited/(14)N,(12)C-filtered ROESY spectrum were assigned. In an ensemble of six crystal structures, two conserved water molecules within 3 Å of the three amide protons were identified. These two water molecules are buried into cavities in the protein surface and thus sufficiently slowed down by the protein topology to account for the observed dipolar interaction. Structural analysis of an ensemble of six crystal structures ruled out any exchange-relayed contributions for the amide-water interactions of interest.

We present here a set of (13)C-direct detected NMR experiments to facilitate the resonance assignment of RNA oligonucleotides. Three experiments have been developed: (1) the (H)CC-TOCSY-experiment utilizing a virtual decoupling scheme to assign the intraresidual ribose (13)C-spins, (2) the (H)CPC-experiment that correlates each phosphorus with the C4' nuclei of adjacent nucleotides via J(C,P) couplings and (3) the (H)CPC-CCH-TOCSY-experiment that correlates the phosphorus nuclei with the respective C1',H1' ribose signals. The experiments were applied to two RNA hairpin structures. The current set of (13)C-direct detected experiments allows direct and unambiguous assignment of the majority of the hetero nuclei and the identification of the individual ribose moieties following their sequential assignment. Thus, (13)C-direct detected NMR methods constitute useful complements to the conventional (1)H-detected approach for the resonance assignment of oligonucleotides that is often hindered by the limited chemical shift dispersion. The developed methods can also be applied to large deuterated RNAs.

The N7 of purine nucleotides presents one of the most dominant metal ion binding sites in nucleic acids. However, the interactions between kinetically labile metal ions like Mg(2+) and these nitrogen atoms are inherently difficult to observe in large RNAs. Rather than using the insensitive direct (15)N detection, here we have used (2)J-[(1)H,(15)N]-HSQC (Heteronuclear Single Quantum Coherence) NMR experiments as a fast and efficient method to specifically observe and characterize such interactions within larger RNA constructs. Using the 27 nucleotides long branch domain of the yeast-mitochondrial group II intron ribozyme Sc.ai5gamma as an example, we show that direct N7 coordination of a Mg(2+) ion takes place in a tetraloop nucleotide. A second Mg(2+) ion, located in the major groove at the catalytic branch site, coordinates mainly in an outer-sphere fashion to the highly conserved flanking GU wobble pairs but not to N7 of the sandwiched branch adenosine.

Recent advances in instrumentation and isotope labeling methodology allow proteins up to 100 kDa in size to be studied in detail using NMR spectroscopy. Using 2H/13C/15N enrichment and selective methyl protonation, we show that newly developed 13C direct detection methods can be used to rapidly yield proton and carbon resonance assignments for the methyl groups of Val, Leu, and Ile residues. We present a highly sensitive 13C-detected CH3-TOCSY experiment that, in combination with standard 1H-detected backbone experiments, allows the full assignment of side chain resonances in methyl-protonated residues. Selective methyl protonation, originally developed by Kay and co-workers (Rosen, M. K.; Gardner, K. H.; Willis, R. C.; Parris, W. E.; Pawson, T.; Kay, L. E. J. Mol. Biol. 1996, 263, 627-636; Gardner, K. G.; Kay, L. E. Annu. Rev. Biophys. Biomol. Struct. 1998, 27, 357-406; Goto, N. K.; Kay, L. E. Curr. Opin. Struct. Biol. 2000, 10, 585-592), improves the nuclear relaxation behavior of larger proteins compared to their fully protonated counterparts, allows significant simplification of spectra, and facilitates NOE assignments. Here, we demonstrate the usefulness of the 13C-detected CH3-TOCSY experiment through studies of (i) a medium-sized protein (CbpA-R1; 14 kDa) with a repetitive primary sequence that yields highly degenerate NMR spectra, and (ii) a larger, bimolecular protein complex (p21-KID/Cdk2; 45 kDa) at low concentration in a high ionic strength solution. Through the analysis of NOEs involving amide and Ile, Leu, and Val methyl protons, we determined the global fold of CbpA-R1, a bacterial protein that mediates the pathogenic effects of Streptococcus pneumoniae, demonstrating that this approach can significantly reduce the time required to determine protein structures by NMR.

Echistatin is a potent antagonist of the integrins alpha(v)beta3, alpha5beta1 and alpha(IIb)beta3. Its full inhibitory activity depends on an RGD (Arg-Gly-Asp) motif expressed at the tip of the integrin-binding loop and on its C-terminal tail. Previous NMR structures of echistatin showed a poorly defined integrin-recognition sequence and an incomplete C-terminal tail, which left the molecular basis of the functional synergy between the RGD loop and the C-terminal region unresolved. We report a high-resolution structure of echistatin and an analysis of its internal motions by off-resonance ROESY (rotating-frame Overhauser enhancement spectroscopy). The full-length C-terminal polypeptide is visible as a beta-hairpin running parallel to the RGD loop and exposing at the tip residues Pro43, His44 and Lys45. The side chains of the amino acids of the RGD motif have well-defined conformations. The integrin-binding loop displays an overall movement with maximal amplitude of 30 degrees . Internal angular motions in the 100-300 ps timescale indicate increased flexibility for the backbone atoms at the base of the integrin-recognition loop. In addition, backbone atoms of the amino acids Ala23 (flanking the R24GD26 tripeptide) and Asp26 of the integrin-binding motif showed increased angular mobility, suggesting the existence of major and minor hinge effects at the base and the tip, respectively, of the RGD loop. A strong network of NOEs (nuclear Overhauser effects) between residues of the RGD loop and the C-terminal tail indicate concerted motions between these two functional regions. A full-length echistatin-alpha(v)beta3 docking model suggests that echistatin's C-terminal amino acids may contact alpha(v)-subunit residues and provides new insights to delineate structure-function correlations.

13C-only spectroscopy was used to measure multiple residual (13)C-(13)C dipolar couplings (RDCs) in uniformly deuterated and (13)C-labeled proteins. We demonstrate that (13)C-start and (13)C-observe spectra can be routinely used to measure an extensive set of the side-chain residual (13)C-(13)C dipolar couplings upon partial alignment of human ubiquitin in the presence of bacteriophages Pf1. We establish that, among different broadband polarization transfer schemes, the FLOPSY family can be used to exchange magnetization between a J coupled network of spins while largely decoupling dipolar interactions between these spins. An excellent correlation between measured RDCs and the 3D structure of the protein was observed, indicating a potential use of the (13)C-(13)C RDCs in the structure determination of perdeuterated proteins.

The assignment of the aliphatic (13)C resonances of trimeric Bacillus Subtilis chorismate mutase, a protein with a molecular mass of 44 kDa, consisting of three 127-residue monomers is presented by use of two-dimensional (2D) (13)C-start and (13)C-observe NMR experiments. These experiments start with (13)C excitation and end with (13)C observation while relying on the long transverse relaxation times of (13)C spins in uniformly deuterated and (13)C,(15)N-labeled large proteins. Gains in sensitivity are achieved by the use of a paramagnetic relaxation enhancement agent to reduce (13)C T(1) relaxation times with little effect on (13)C T(2) relaxation times. Such 2D (13)C-only NMR experiments circumvent problems associated with the application of conventional experiments for side-chain assignment to proteins of larger sizes, for instance, the absence or low concentration of the side-chain (1)H spins, the transfer of the side-chain spin polarization to the (1)H(N) spins for signal acquisition, or the necessity of a quantitative reprotonation of the methyl moieties in the otherwise fully deuterated side-chains. We demonstrate that having obtained a nearly complete assignment of the side-chain aliphatic (13)C resonances, the side-chain (1)H chemical shifts can be assigned in a semiautomatic fashion using 3D (15)N-resolved and (13)C-resolved NOESY experiments measured with a randomly partially protonated protein sample. We also discuss perspectives for structure determination of larger proteins by using novel strategies which are based on the (1)H,(1)H NOEs in combination with multiple residual dipolar couplings between adjacent (13)C spins determined with 2D (13)C-only experiments.