Fourier tickling for homonuclear decoupling in NMR
View Patent ↗A method for high resolution NMR (=nuclear magnetic resonance) measurements using the application of excitation pulses and the acquisition of data points, whereby a dwell time Δt separates the acquisition of two consecutive data points, which is characterized in that one or more tickling rf (=radio frequency) pulses of duration τ p are applied within each dwell time Δt, and that the average rf field amplitude of each of the tickling rf pulses approximately fulfills the condition ω 1 =ω 1 τ p /Δt=πJ wherein J is the scalar J-coupling constant and ω 1 =γB 1 with γ being the gyromagnetic ratio and B 1 being the strength of the magnetic component of each tickling rf pulse. This method is effective in decoupling homonuclear couplings.
1. A method for high resolution NMR (=nuclear magnetic resonance) measurements, the method comprising the steps of:
a) applying an excitation pulse;
b) acquiring a first data point;
c) waiting a dwell time Δt;
d) applying, during step c), one or more tickling rf (=radio frequency) pulses of duration τ p , each tickling rf pulse having an average rf field amplitude between ω 1 =ω 1 τ p /Δt= π / 10 J and ω 1 =ω 1 τ p /Δt=10πJ, wherein J is a scalar J-coupling constant and ω 1 =γB 1 with γ being a gyromagnetic ratio and B 1 being a strength of a magnetic component of each tickling rf pulse; and
e) acquiring a second data point immediately following completion of step c), the dwell time Δt thereby separating acquisition of the first and the second data points.
2. The method of claim 1 , wherein an average rf field amplitude of each of the tickling rf pulses fulfills the condition: ω 1 =ω 1 τ p /Δt=πJ.
3. The method of claim 1 , wherein the duration τ p of the tickling pulses is between 0.1 μs and 20 μs.
4. The method of claim 3 , wherein the duration τ p of the tickling pulses is about 1 μs.
5. The method of claim 1 , wherein data points, acquired once in every dwell time Δt, are transformed into a spectrum by a Fourier transformation.
6. The method of claim 1 , wherein M tickling rf pulses of duration τ p are applied at will within each of multiple dwell times Δt, each tickling rf pulse within each dwell time At belonging to a different comb C m of tickling rf pulses, wherein m is a positive integer and 1≦m≦M, all tickling rf pulses belonging to a same comb C m being equidistant from each other.
7. The method of claim 6 , wherein a phase of each tickling rf pulse belonging to the same comb C m is shifted from one dwell time to a next by a constant factor.