Bloch–Siegert shift

Bloch–Siegert shift

Consider the effect due to the counter-rotating field. In the counter-rotating frame (${\displaystyle {\omega }_{\mathrm{c}\mathrm{r}}=-\omega }$), the effective detuning is ${\displaystyle \mathrm{\Delta }{\omega }_{\mathrm{c}\mathrm{r}}=\omega +{\omega }_0}$ and the counter-rotating field adds a driving component perpendicular to the detuning, with equal amplitude ${\displaystyle {\mathrm{\Omega }}_0}$. The counter-rotating field effectively dresses the system, where we can define a new quantization axis slightly tilted from the original one, with an effective detuning

${\displaystyle \mathrm{\Delta }{\omega }_{\mathrm{e}\mathrm{f}\mathrm{f}}=\pm \sqrt{{\mathrm{\Omega }}_0^2+(\omega +{\omega }_0{)}^2}}$

Therefore, the resonance frequency (${\displaystyle {\omega }_{\mathrm{r}\mathrm{e}\mathrm{s}}}$) of the system dressed by the counter-rotating field is ${\displaystyle \mathrm{\Delta }{\omega }_{\mathrm{e}\mathrm{f}\mathrm{f}}}$ away from our frame of reference, which is rotating at ${\displaystyle -\omega }$

${\displaystyle {\omega }_{\mathrm{r}\mathrm{e}\mathrm{s}}+\omega =\pm \sqrt{{\mathrm{\Omega }}_0^2+(\omega +{\omega }_0{)}^2}}$

and there are two solutions for ${\displaystyle {\omega }_{\mathrm{r}\mathrm{e}\mathrm{s}}}$

${\displaystyle {\omega }_{\mathrm{r}\mathrm{e}\mathrm{s}}={\omega }_0\left[1+\frac{1}{4}{\left(\frac{{\mathrm{\Omega }}_0}{{\omega }_0}\right)}^2\right]}$

and

${\displaystyle {\omega }_{\mathrm{r}\mathrm{e}\mathrm{s}}=-\frac{1}{3}{\omega }_0\left[1+\frac{3}{4}{\left(\frac{{\mathrm{\Omega }}_0}{{\omega }_0}\right)}^2\right].}$

The shift from the RWA of the first solution is dominant, and the correction to ${\displaystyle {\omega }_0}$ is known as the Bloch–Siegert shift:

${\displaystyle \delta {\omega }_{\mathrm{B}-\mathrm{S}}=\frac{1}{4}\frac{{\mathrm{\Omega }}_0^2}{{\omega }_0}}$

The counter-rotating frequency gives rise to a population oscillation at ${\displaystyle 2\omega }$, with amplitude proportional to ${\displaystyle (\mathrm{\Omega }/\omega )}$, and phase that depends on the phase of the driving field. Such Bloch–Siegert oscillation may become relevant in spin flipping operations at high rate. This effect can be suppressed by using an off-resonant Λ transition.

Applications

NMR

When homonuclear nuclear magnetic resonance decoupling is performed, Bloch–Siegert shifts may become significant due to the strength of the homonuclear decoupling field. Direct measurement of the homonuclear decoupling mean field strength can be achieved by measuring the resulting Bloch–Siegert shift.

MRI

The Bloch–Siegert shift is currently being widely investigated a potential encoding mechanism for MRI. The first significant use of the phenomenon in the MR imaging community was to perform mapping of the RF transmit field, by using the imaging system to measure the spatial phase accrual produced by an off-resonant RF pulse. Since then, it has been recognized that Bloch–Siegert shifts can be used in MRI sequences within imaging systems with a transmit field gradient to provide slice selection, phase encoding, and frequency encoding. The motivation for this research is to provide an alternative to conventional ${\displaystyle B_0}$ gradient encoding, which is currently used in clinical imaging systems but produces undesirable acoustic noise, peripheral nerve stimulation, and spatial design constraints.

AC-Stark shift

The AC-Stark shift is a similar shift in the resonance frequency, caused by a non-resonant field of the form ${\displaystyle H_{\mathrm{o}\mathrm{r}}=\frac{V_{\mathrm{o}\mathrm{r}}}{2}\cos ({\omega }_{\mathrm{o}\mathrm{r}}t)}$ perturbing the spin. It can be derived using a similar treatment as above, invoking the RWA on the off-resonant field. The resulting AC-Stark shift is: ${\displaystyle \delta {\omega }_{\mathrm{A}\mathrm{C}}=\frac{1}{2}\frac{{\mathrm{\Omega }}_{\mathrm{o}\mathrm{r}}^2}{({\omega }_0-{\omega }_{\mathrm{o}\mathrm{r}})}}$, with ${\displaystyle {\mathrm{\Omega }}_{or}=|V_{or}/2\hslash |}$.