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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...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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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 |
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author | Grün, J. Tassilo Kim, Jihyun Jayanthi, Sundaresan Lupulescu, Adonis Kupče, E̅riks Schwalbe, Harald Frydman, Lucio |
author_facet | Grün, J. Tassilo Kim, Jihyun Jayanthi, Sundaresan Lupulescu, Adonis Kupče, E̅riks Schwalbe, Harald Frydman, Lucio |
author_sort | Grün, J. Tassilo |
collection | PubMed |
description | [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. |
format | Online Article Text |
id | pubmed-10037324 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-100373242023-03-25 Identifying and Overcoming Artifacts in (1) H-Based Saturation Transfer NOE NMR Experiments Grün, J. Tassilo Kim, Jihyun Jayanthi, Sundaresan Lupulescu, Adonis Kupče, E̅riks Schwalbe, Harald Frydman, Lucio J Am Chem Soc [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. American Chemical Society 2023-03-06 /pmc/articles/PMC10037324/ /pubmed/36877814 http://dx.doi.org/10.1021/jacs.2c13087 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Grün, J. Tassilo Kim, Jihyun Jayanthi, Sundaresan Lupulescu, Adonis Kupče, E̅riks Schwalbe, Harald Frydman, Lucio Identifying and Overcoming Artifacts in (1) H-Based Saturation Transfer NOE NMR Experiments |
title | Identifying and Overcoming Artifacts in (1) H-Based
Saturation Transfer NOE NMR Experiments |
title_full | Identifying and Overcoming Artifacts in (1) H-Based
Saturation Transfer NOE NMR Experiments |
title_fullStr | Identifying and Overcoming Artifacts in (1) H-Based
Saturation Transfer NOE NMR Experiments |
title_full_unstemmed | Identifying and Overcoming Artifacts in (1) H-Based
Saturation Transfer NOE NMR Experiments |
title_short | Identifying and Overcoming Artifacts in (1) H-Based
Saturation Transfer NOE NMR Experiments |
title_sort | identifying and overcoming artifacts in (1) h-based
saturation transfer noe nmr experiments |
url | 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 |
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