The HMBC experiment provides 1H-13C correlations over multiple bonds and is essential for assigning small molecules. The main drawback to the HMBC is that it does not identify the length of the correlation and in some cases may be ambiguous. A recent publication describes a method, called i-HMBC, for distinguishing two bond HMBC correlations from longer ones.
Tuesday, May 2, 2023
Wednesday, April 6, 2022
NUS for HMBC and LR-HSQMBC experiments
Non Uniform Sampling (NUS) of multidimensional NMR data can greatly reduce the time taken to record a spectrum by recording only a subset of the normal data. A variety of algorithms are available to reconstruct the omitted data based on the data that was recorded. The most commonly used algorithm is Iterative Soft Thresholding (IST). Most implementations of the IST algorithm rely on the peaks in the detected dimension being phased correctly and positive. For most modern experiments this is not a problem, but in the HMBC experiment it is not possible to phase the peaks. For this reason I have not recommended using NUS with HMBCs. The LR-HSQMBC experiment, however, can be phased and I recommend using NUS with it. In this post, spectra recorded with different levels of NUS were recorded to determine how NUS affects HMBC and LR-HSQMBC experiments.
Wednesday, December 1, 2021
Testing the NOAH BSC sequence
One of the many recent innovations to make acquiring NMR data faster is the NOAH technique. NOAH concatenates several pulse sequences behind a single relaxation delay to reduce the total acquisition time. Various combinations of experiments are available, but perhaps the most useful is the NOAH_BSC variant which provides a gCOSY, 13C HSQC and 13C HMBC. In this post the NOAH_BSC spectra are compared with those collected using the standard Facility parameters.
Friday, February 5, 2021
Constant time
Collecting multi-dimensional spectra requires recording chemical shift information via the use of an incremented delay. Since the length of the delay increases over the course of the experiment the signal is recorded at different times for each increment. This allows coupling in the indirect dimension to evolve, which broadens the peaks and decreases resolution. The "constant time" method was developed to eliminate this problem.