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Michaël Deschamps

Publications and source records attributed to Michaël Deschamps.

4 recordsLinked to original sources

Three-dimensional through-bond homonuclear-heteronuclear correlation experiments for quadrupolar nuclei in solid-state NMR applied to (27)Al-O-(31)P-O-(27)Al networks.

We present here the first 3D homonuclear/heteronuclear correlation experiment applied to quadrupolar nuclei and making use of the sole scalar J-coupling. This experiment, based on the 2D-Homonuclear-Heteronuclear Single Quantum Correlation (H-HSQC) experiment, uses a relayed transfer from the (27)Al central transition to neighbouring (31)P spins and to the central transition of a second (27)Al. It confirms the correlation map characterizing the two (27)Al and the (31)P NMR signatures of (27)Al-O-(31)P-O-(27)Al chemically bonded molecular motifs.

Algorithms↗

Through-bond homonuclear correlation experiments in solid-state NMR applied to quadrupolar nuclei in Al-O-P-O-Al chains.

Through-bond homonuclear correlation experiments can be realised in solids between spins of type X, separated by four chemical bonds, in X-O-Y-O-X motifs, provided a J coupling between X and Y exists: central transitions of quadrupolar 27Al spins can be correlated via the J2 scalar coupling between 27Al (X) and 31P (Y) in materials featuring Al-O-P-O-Al motifs.

Journal Article↗

Cooling overall spin temperature: protein NMR experiments optimized for longitudinal relaxation effects.

In experiments performed on protonated proteins at high fields, 80% of the NMR spectrometer time is spent waiting for the (1)H atoms to recover their polarization after recording the free induction decay. Selective excitation of a fraction of the protons in a large molecule has previously been shown to lead to faster longitudinal relaxation for the selected protons [K. Pervushin, B. Vögeli, A. Eletsky, Longitudinal (1)H relaxation optimization in TROSY NMR spectroscopy, J. Am. Chem. Soc. 124 (2002) 12898-12902; P. Schanda, B. Brutscher, Very fast two-dimensional NMR spectroscopy for real-time investigation of dynamic events in proteins on the time scale of seconds, J. Am. Chem. Soc. 127 (2005) 8014-8015; H.S. Attreya, T. Szyperski, G-matrix Fourier transform NMR spectroscopy for complete protein resonance assignment, Proc. Natl. Acad. Sci. USA 101 (2004) 9642-9647]. The pool of non-selected protons acts as a "thermal bath" and spin-diffusion processes ("flip-flop" transitions) channel the excess energy from the excited pool to the non-selected protons in regions of the molecule where other relaxation processes can dissipate the excess energy. We present here a sensitivity enhanced HSQC sequence (COST-HSQC), based on one selective E-BURP pulse, which can be used on protonated (15)N enriched proteins (with or without (13)C isotopic enrichment). This experiment is compared to a gradient sensitivity enhanced HSQC with a water flip-back pulse (the water flip-back pulse quenches the spin diffusion between (1)H(N) and (1)H(alpha) spins). This experiment is shown to have significant advantages in some circumstances. Some observed limitations, namely sample overheating with short recovery delays and complex longitudinal relaxation behaviour are discussed and analysed.

Magnetic Resonance Spectroscopy↗

Residual dipolar couplings and some specific models for motional averaging.

The measurement of residual dipolar couplings (RDCs) from partially oriented molecules is now widely used to provide restraints for NMR structure determination. Bond vibrations, random angular fluctuations around bond vectors and conformational exchange all influence the magnitude of the experimental RDCs. The effect that angular fluctuations have upon the magnitude of RDCs is quantitatively compared using three new models (elliptic, uni-dimensional, and equally populated two site jump) and three established models (static, isotropic motion in a cone and free diffusion about a fixed symmetry axis: Woessner's model) for motional averaging in the limit that the amplitude of motion beta < or = (max)15-20 degrees. The influence of the different motional models on the value of R(obs) determined from the distribution of RDCs is explored. The consequences of the different types of angular motion for the accurate determination of bond vector orientation, with respect to the alignment tensor, A, is investigated. The extent to which motion influences the magnitude of RDCs is compared to some non-dynamic factors affecting RDC size.

Anisotropy↗