Abstract
Strong coupling of nuclear spins, which is achieved when their scalar coupling 2πJ2πJ<math><mrow><mn>2</mn><mi>π</mi><mi>J</mi></mrow></math> is greater than or comparable to the difference ΔωΔω<math><mrow><mi>Δ</mi><mi>ω</mi></mrow></math> in their Larmor precession frequencies in an external magnetic field, gives rise to efficient coherent longitudinal polarization transfer. The strong coupling regime can be achieved when the external magnetic field is sufficiently low, as ΔωΔω<math><mrow><mi>Δ</mi><mi>ω</mi></mrow></math> is reduced proportional to the field strength. In the present work, however, we demonstrate that in heteronuclear spin systems these simple arguments may not hold, since heteronuclear spin-spin interactions alter the ΔωΔω<math><mrow><mi>Δ</mi><mi>ω</mi></mrow></math> value. The experimental method that we use is two-field nuclear magnetic resonance (NMR), exploiting sample shuttling between the high field, at which NMR spectra are acquired, and the low field, where strong couplings are expected and at which NMR pulses can be applied to affect the spin dynamics. By using this technique, we generate zero-quantum spin coherences by means of a nonadiabatic passage through a level anticrossing and study their evolution at the low field. Such zero-quantum coherences mediate the polarization transfer under strong coupling conditions. Experiments performed with a 13C13C<math><mrow><msup><mi></mi><mn>13</mn></msup><mi>C</mi></mrow></math>-labeled amino acid clearly show that the coherent polarization transfer at the low field is pronounced in the 13C13C<math><mrow><msup><mi></mi><mn>13</mn></msup><mi>C</mi></mrow></math> spin subsystem under proton decoupling. However, in the absence of proton decoupling, polarization transfer by coherent processes is dramatically reduced, demonstrating that heteronuclear spin-spin interactions suppress the strong coupling regime, even when the external field is low. A theoretical model is presented, which can model the reported experimental results.