Abstract
In chiral magnets a magnetic helix forms where the
magnetization winds around a propagation vector
{q}q.
We show theoretically that a magnetic field B_\bot(t) \bot qB⊥(t)⊥q, which is
spatially homogeneous but oscillating in time, induces a net rotation of
the texture around {q}q.
This rotation is reminiscent of the motion of an Archimedean screw and
is equivalent to a translation with velocity
v_{\text{screw}}vscrew
parallel to q. Due to the coupling to a Goldstone mode, this
non-linear effect arises for arbitrarily weak B_\bot(t)B⊥(t) with
v_{\text{screw}} \propto |{ B_\perp}|^2vscrew∝|B⊥|2
as long as pinning by disorder is absent. The effect is resonantly
enhanced when internal modes of the helix are excited and the sign of
v_{\text{screw}}vscrew
can be controlled either by changing the frequency or the polarization
of B_\bot(t)B⊥(t). The Archimedean screw can be used to transport spin and
charge and thus the screwing motion is predicted to induce a voltage
parallel to q. Using a combination of numerics and Floquet spin wave
theory, we show that the helix becomes unstable upon increasing B_\botB⊥,
forming a `time quasicrystal’ which oscillates in space and time for
moderately strong drive.
Funder
Deutsche Forschungsgemeinschaft
Subject
General Physics and Astronomy
Cited by
8 articles.
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