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Recovering Invisible Signals by Two‐Field NMR Spectroscopy
Authors:Samuel F. Cousin  Dr. Pavel Kadeřávek  Baptiste Haddou  Dr. Cyril Charlier  Thorsten Marquardsen  Jean‐Max Tyburn  Dr. Pierre‐Alain Bovier  Dr. Frank Engelke  Dr. Werner Maas  Prof. Dr. Geoffrey Bodenhausen  Dr. Philippe Pelupessy  Prof. Dr. Fabien Ferrage
Affiliation:1. Department of Chemistry, Ecole Normale Supérieure, PSL Research University, Paris, France;2. Sorbonne Universités, UPMC Univ Paris 06, LBM, Paris, France;3. CNRS, UMR 7203 LBM, Paris, France;4. CNRS, UMR, 8640 Pasteur, Paris, France;5. Laboratory of Chemical Physics, NIDDK, NIH, Bethesda, MD, USA;6. Bruker BioSpin GmbH, Rheinstetten, Germany;7. Bruker BioSpin, Wissembourg Cedex, France;8. Bruker BioSpin AG, F?llanden, Switzerland;9. Bruker BioSpin, Billerica, MA, USA
Abstract:Nuclear magnetic resonance (NMR) studies have benefited tremendously from the steady increase in the strength of magnetic fields. Spectacular improvements in both sensitivity and resolution have enabled the investigation of molecular systems of rising complexity. At very high fields, this progress may be jeopardized by line broadening, which is due to chemical exchange or relaxation by chemical shift anisotropy. In this work, we introduce a two‐field NMR spectrometer designed for both excitation and observation of nuclear spins in two distinct magnetic fields in a single experiment. NMR spectra of several small molecules as well as a protein were obtained, with two dimensions acquired at vastly different magnetic fields. Resonances of exchanging groups that are broadened beyond recognition at high field can be sharpened to narrow peaks in the low‐field dimension. Two‐field NMR spectroscopy enables the measurement of chemical shifts at optimal fields and the study of molecular systems that suffer from internal dynamics, and opens new avenues for NMR spectroscopy at very high magnetic fields.
Keywords:chemical exchange  high-field NMR spectroscopy  kinetics  nuclear magnetic resonance  low-field NMR spectroscopy
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