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Effects of high pressure, magnetic fields, and substitutions - ICMR ...

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Symmetry <strong>and</strong> L<strong>and</strong>au theory (Kenzelmann, Mostovoy)<br />

Lowest order coupling Φ em<br />

(P,M) between FE polarization, P, <strong>and</strong> <strong>magnetic</strong><br />

modulation, M, that is invariant upon time reversal <strong>and</strong> spatial inversion:<br />

t -> -t : P -> P <strong>and</strong> M -> -M Φ em<br />

quadratic in M<br />

x -> -x: P -> -P <strong>and</strong> M -> M Φ em<br />

~ P <strong>and</strong> ∇M (Lifshits invariant), P uniform<br />

for cubic symmetry: Φ em<br />

= const P* [ M(∇*M) – (M*∇)M ]<br />

Φ e<br />

= P 2 /(2χ e<br />

) =><br />

P = const χ e<br />

[ M(∇*M) – (M* ∇)M ]<br />

Spiral <strong>magnetic</strong> order: M = m 1<br />

e 1<br />

cos(Qx) + m 2<br />

e 2<br />

sin(Qx) + m 3<br />

e 3<br />

Average polarization: = const χ e<br />

m 1<br />

m 2<br />

[ e 3<br />

× Q ]<br />

Sinusoidal <strong>magnetic</strong> order: m 1<br />

or m 2<br />

=0 => = 0

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