In the top trace, broadband 1H decoupling is applied with a 100% duty cycle. This is most common for the collection of 13C NMR data. It is applied during the acquisition time to decouple protons and during the recycle delay to take advantage of any nuclear Overhauser enhancement. In the second trace, decoupling is applied only during the acquisition time to decouple protons but not during the recycle delay. This is called inverse gated decoupling and is often used when collecting NMR data for nuclei like 15N or 29Si which have negative gyromagnetic ratios and hence negative nuclear Overhauser effects. In the third trace the decoupling is applied only during the recycle delay but not during the acquisition time. This is called gated decoupling and is used when a fully coupled spectrum is desired while still taking advantage of any nuclear Overhauser enhancement. The bottom trace shows an example of inverse gated decoupling applied to an X nucleus while observing protons. For examples of this, click here and here.
Showing posts with label gated decoupling. Show all posts
Showing posts with label gated decoupling. Show all posts
Thursday, May 1, 2008
Modes of Heteronuclear Broadband Decoupling
In talking to many novice NMR users over the years, I have often been discouraged to learn that some do not even realize that they are using heteronuclear broadband decoupling when they run (for example) a 13C spectrum. They do not question why their signals are singlets or even realize why they may not be singlets if 1H decoupling is not used. It is for this reason I have added this BLOG post. Heteronuclear broadband decoupling is the irradiation of one nuclide while observing another nuclide. It is normally applied using multiple pulse decoupling schemes such as WALTZ 16 or GARP. These schemes effectively allow the decoupling to be efficient over a range of frequencies (sometimes even the entire chemical shift range!) with a minimum of power. The figure below shows some common modes of heteronuclear decoupling.In the top trace, broadband 1H decoupling is applied with a 100% duty cycle. This is most common for the collection of 13C NMR data. It is applied during the acquisition time to decouple protons and during the recycle delay to take advantage of any nuclear Overhauser enhancement. In the second trace, decoupling is applied only during the acquisition time to decouple protons but not during the recycle delay. This is called inverse gated decoupling and is often used when collecting NMR data for nuclei like 15N or 29Si which have negative gyromagnetic ratios and hence negative nuclear Overhauser effects. In the third trace the decoupling is applied only during the recycle delay but not during the acquisition time. This is called gated decoupling and is used when a fully coupled spectrum is desired while still taking advantage of any nuclear Overhauser enhancement. The bottom trace shows an example of inverse gated decoupling applied to an X nucleus while observing protons. For examples of this, click here and here.
In the top trace, broadband 1H decoupling is applied with a 100% duty cycle. This is most common for the collection of 13C NMR data. It is applied during the acquisition time to decouple protons and during the recycle delay to take advantage of any nuclear Overhauser enhancement. In the second trace, decoupling is applied only during the acquisition time to decouple protons but not during the recycle delay. This is called inverse gated decoupling and is often used when collecting NMR data for nuclei like 15N or 29Si which have negative gyromagnetic ratios and hence negative nuclear Overhauser effects. In the third trace the decoupling is applied only during the recycle delay but not during the acquisition time. This is called gated decoupling and is used when a fully coupled spectrum is desired while still taking advantage of any nuclear Overhauser enhancement. The bottom trace shows an example of inverse gated decoupling applied to an X nucleus while observing protons. For examples of this, click here and here.
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