The 2D HMQC-ROESY experiment is an hybrid inverse experiment consisting of an initial HMQC pulse train followed by a ROESY mixing sequence. In the first step, magnetization is transferred from the X nucleus (13C or 15N) to the directly-bonded proton nuclei via ¹J(CH). In the second step, polarization transfer is achieved in the transverse plane via NOE. Similar results are obtained from the analog 2D HSQC-ROESY experiment.

Easy implementation on any AVANCE spectrometer equipped with an inverse probehead.

The basic sequence of the 2D HMQC-ROESY experiment is based in the four-pulse 2D HMQC experiment in which a ROESY mixing sequence (for instance, low-power continuous wave) is inserted prior to acquisition. A BIRD-recovery cluster is used as a preparation period in order to reduce the large unwanted 1H-X (typically, 12C or 14N) magnetization ( 92JACS1115 ). Carbon decoupling is optionally applied during proton acquisition.

Improved results can be obtained from the gradient enhanced version (see ge-2D HMQC-ROESY experiment).

The 2D HMQC-ROESY experiment can be recorded in routine/automation modes. The experiment is basically optimized as described for the 2D HMQC experiment. The most important paramter to optimize is the mixing time length. More details on practical implementation of 2D HMQC-ROESY experiments on AVANCE spectrometers can be found in

Tutorials: 2D inverse experiments

Tutorials: 2D gradient-based inverse experiments

The HMQC-ROESY spectrum correlates chemical shifts of heteronucleus X (F1 dimension) and protons (F2 dimension) via the direct heteronuclear coupling ¹J(XH). Two different cross-peaks are present for each X resonance: The direct 1H-X NOE connectivites and the NOE 1H-X connectivities due to the cumulative transfer ¹J(XH) + 1H-1H NOE.  The same NOE effects can also be detected by a 2D HMQC-NOESY, 2D HSQC-ROESY and 2D HSQC-NOESY experiments.

Comparison of different 2D inverse correlations have been carried out ( 90JMR488-87 ).

A 3D HMQC-ROESY experiment is easily designed by incorporating a second variable evolution period between the HMQC and the ROESY mixing period. On the other hand, a very similar pulse sequence is used for the w1-X-filtered 2D ROESY experiment by fixing the variable period in the HMQC block of this 3D HMQC-ROESY experiment.

Related experiments:

2D Inverse experiments

2D Inverse gradient-enhanced experiments