The pot lid is rotating around an axis along the surface of the table that is quickly rotating. This results in a secondary rotation which is perpendicular to the table. This is equivalent to the Bloch–Siegert shift and can be seen by watching the motion of the red dot.

The Bloch–Siegert shift is a phenomenon in quantum physics that becomes important for driven two-level systems when the driving gets strong (e.g. atoms driven by a strong laser drive or nuclear spins in NMR, driven by a strong oscillating magnetic field).

When the rotating-wave approximation (RWA) is invoked, the resonance between the driving field and a pseudospin occurs when the field frequency ${\displaystyle \omega }$ is identical to the spin's transition frequency ${\displaystyle \omega _{0}}$. The RWA is, however, an approximation. In 1940 Felix Bloch and Arnold Siegert showed that the dropped parts oscillating rapidly can give rise to a shift in the true resonance frequency of the dipoles.

Rotating wave approximation

In RWA, when the perturbation to the two level system is ${\displaystyle H_{ab}={\frac {V_{ab}}{2}}\cos {(\omega t)}}$, a linearly polarized field is considered as a superposition of two circularly polarized fields of the same amplitude rotating in opposite directions with frequencies ${\displaystyle \omega ,-\omega }$. Then, in the rotating frame(${\displaystyle \omega }$), we can neglect the counter-rotating field and the Rabi frequency is

${\displaystyle \Omega ={\sqrt {(\Omega _{0})^{2}+(\omega -\omega _{0})^{2}}}}$

where ${\displaystyle \Omega _{0}=|V_{ab}/2\hbar |}$ is the on-resonance Rabi frequency.

Bloch–Siegert shift

Consider the effect due to the counter-rotating field. In the counter-rotating frame (${\displaystyle \omega _{\mathrm {cr} }=-\omega }$), the effective detuning is ${\displaystyle \Delta \omega _{\mathrm {cr} }=\omega +\omega _{0}}$ and the counter-rotating field adds a driving component perpendicular to the detuning, with equal amplitude ${\displaystyle \Omega _{0}}$. 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

${\displaystyle \Delta \omega _{\mathrm {eff} }=\pm {\sqrt {\Omega _{0}^{2}+(\omega +\omega _{0})^{2}}}}$

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

${\displaystyle \omega _{\mathrm {res} }+\omega =\pm {\sqrt {\Omega _{0}^{2}+(\omega +\omega _{0})^{2}}}}$

and there are two solutions for ${\displaystyle \omega _{res}}$

${\displaystyle \omega _{\mathrm {res} }=\omega _{0}\left[1+{\frac {1}{4}}\left({\frac {\Omega _{0}}{\omega _{0}}}\right)^{2}\right]}$

and

${\displaystyle \omega _{\mathrm {res} }=-{\frac {1}{3}}\omega _{0}\left[1+{\frac {3}{4}}\left({\frac {\Omega _{0}}{\omega _{0}}}\right)^{2}\right].}$

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:

${\displaystyle \delta \omega _{\mathrm {B-S} }={\frac {1}{4}}{\frac {\Omega _{0}^{2}}{\omega _{0}}}}$

The counter-rotating frequency gives rise to a population oscillation at ${\displaystyle 2\omega }$, with amplitude proportional to ${\displaystyle (\Omega /\omega )}$, and phase that depends on the phase of the driving field.^[1] 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.^[2]

AC-Stark shift

The AC-Stark shift is a similar shift in the resonance frequency, caused by a non-resonant field of the form ${\displaystyle H_{\mathrm {or} }={\frac {V_{\mathrm {or} }}{2}}\cos {(\omega _{\mathrm {or} }t)}}$ 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: ${\displaystyle \delta \omega _{\mathrm {AC} }={\frac {1}{2}}{\frac {\Omega _{\mathrm {or} }^{2}}{(\omega _{0}-\omega _{\mathrm {or} })}}}$, with ${\displaystyle \Omega _{or}=|V_{or}/2\hbar |}$.

References

• L. Allen and J. H. Eberly, Optical Resonance and Two-level Atoms, Dover Publications, 1987.