Conte Et Al. GIDRM 2006

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  • 8/12/2019 Conte Et Al. GIDRM 2006

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    RAPID MEASUREMENT OF 1 H 90 PULSE IN THE SOLID STATE NMR VIA

    CROSS POLARIZATION

    P. Conte, R. Spaccini, A. Piccolo

    Dip. di Scienze del Suolo della Pianta e dellAmbiente, via Universit 100, 80055 Portici (Na) ItalyE-Mail: [email protected]

    Cross polarization magic angle spinning (CPMAS) 13C NMR spectroscopy is based onthe excitation of carbons via proton nuclei. Namely, a 90 pulse applied on the protonsis followed by a spin lock sequence on both 1H and 13C in order to excite the carbons. Aproton decoupling sequence is then applied while the 13C signals are acquired. TheCPMAS 13C sequence is the basis of more complicated and powerful experiments suchas those based on the Lee-Goldburg decoupling. Key factors of the CPMAS 13C NMRspectroscopy are: 1. the matching of the Hartmann-Hahn condition, and, 2. the precision

    of the proton 90 pulse. If one of the two factors are not matched, NMR artefacts mayarise. The present work deals with the precise calibration of the proton 90 pulse viacross polarization on standard molecules and natural organic matter. The normal methodused to calibrate the proton 90 pulse via cross polarization is the use of an optimizationmethod on a standard system such as the simple glycine. Namely, the proton pulselength is varied until 13C NMR signals are undetected. The undetectability of the carbonsignals is due to the application of a proton pulse corresponding to a 180 1Hmagnetization inversion. The application of a 180 1H pulse prevents the 1H- 13C cross-polarization. The main disadvantages of the standard 90 pulse measurements arerelated to: 1. the NMR pulse trapezoidal shapes that shorten the real pulse length to beapplied in CPMAS 13C-NMR experiments, 2. the use of a recycle delay that can be

    inadequate as the proton pulse length is increased during the 90 proton pulsemeasurements, 3. the use of a simple organic standard that can have a NMR behaviourdifferent from that of the natural organic matter. In order to account for all theseproblems, a new method for proton 90 pulse calibration was developed. The classicalCPMAS 13C NMR pulse sequence was modified in order to apply a pulse train made byfour 90 pulses on protons. The use of such a modified sequence minimizes the errorsdue to the trapezoidal pulse shapes, and allows the application of a very short recycledelay, thereby shortening the 90 pulse measuring time. In fact, the 4x90 pulse traincorresponds to a rotation of 360 of the 1H magnetization. Being close to theequilibrium state, an unusually short recycle delay can be applied. Moreover, theabsence of 13C NMR signals is a confirmation that the correct 90 1H pulse wasmeasured. The modified 4x90 pulse sequence can be also used to rapidly measure thecorrect 90 1H pulse on natural organic matter (NOM), thereby preventing the use ofstandard organic systems that differ from NOM and can provide imprecise NOM 90 1Hpulses.