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Identifying and Overcoming Artifacts in (1) H-Based Saturation Transfer NOE NMR Experiments

[Image: see text] Magnetization transfer experiments are versatile nuclear magnetic resonance (NMR) tools providing site-specific information. We have recently discussed how saturation magnetization transfer (SMT) experiments could leverage repeated repolarizations arising from exchanges between lab...

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Detalles Bibliográficos
Autores principales: Grün, J. Tassilo, Kim, Jihyun, Jayanthi, Sundaresan, Lupulescu, Adonis, Kupče, E̅riks, Schwalbe, Harald, Frydman, Lucio
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10037324/
https://www.ncbi.nlm.nih.gov/pubmed/36877814
http://dx.doi.org/10.1021/jacs.2c13087
Descripción
Sumario:[Image: see text] Magnetization transfer experiments are versatile nuclear magnetic resonance (NMR) tools providing site-specific information. We have recently discussed how saturation magnetization transfer (SMT) experiments could leverage repeated repolarizations arising from exchanges between labile and water protons to enhance connectivities revealed via the nuclear Overhauser effect (NOE). Repeated experience with SMT has shown that a number of artifacts may arise in these experiments, which may confound the information being sought – particularly when seeking small NOEs among closely spaced resonances. One of these pertains to what we refer to as “spill-over” effects, originating from the use of long saturation pulses leading to changes in the signals of proximate peaks. A second, related but in fact different effect, derives from what we describe as NOE “oversaturation”, a phenomenon whereby the use of overtly intense RF fields overwhelms the cross-relaxation signature. The origin and ways to avoid these two effects are described. A final source of potential artifact arises in applications where the labile (1)Hs of interest are bound to (15)N-labeled heteronuclei. SMT’s long (1)H saturation times will then be usually implemented while under (15)N decoupling based on cyclic schemes leading to decoupling sidebands. Although these sidebands usually remain invisible in NMR, they may lead to a very efficient saturation of the main resonance when touched by SMT frequencies. All of these phenomena are herein experimentally demonstrated, and solutions to overcome them are proposed.