Archimedean screw in driven chiral magnets
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 q B ⊥ ( t ) ⊥ q , which is spatially homogeneous but oscillating in time, induces a net rotation of the texture around {q} q . This ro...
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Published in | SciPost physics Vol. 11; no. 1; p. 009 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
SciPost
01.07.2021
|
Online Access | Get full text |
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Summary: | 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 q
B
⊥
(
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}}
v
screw
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}|^2
v
screw
∝
|
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}}
v
screw
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_\bot
B
⊥
,
forming a `time quasicrystal’ which oscillates in space and time for
moderately strong drive. |
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ISSN: | 2542-4653 2542-4653 |
DOI: | 10.21468/SciPostPhys.11.1.009 |