Effects of high pressure, magnetic fields, and substitutions - ICMR ...
Effects of high pressure, magnetic fields, and substitutions - ICMR ...
Effects of high pressure, magnetic fields, and substitutions - ICMR ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
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