Electromagnetics in deterministic and stochastic bianisotropic media
Electromagnetics in deterministic and stochastic bianisotropic media
Electromagnetics in deterministic and stochastic bianisotropic media
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Well-posedness<br />
Theorem<br />
Time-doma<strong>in</strong> problems<br />
Under suitable regularity assumptions on the data, (28) is weakly / mildly<br />
/ strongly / classically well-posed.<br />
The underly<strong>in</strong>g space is H0(curl, O) × H(curl, O), where<br />
H(curl, O) := {u ∈ (L 2 (O)) 3 : curl u ∈ (L 2 (O)) 3 }.<br />
For bounded O, H0(curl, O) is the space<br />
{u ∈ H(curl, O) : n × u|∂O = 0}.<br />
The first component of the underly<strong>in</strong>g space <strong>in</strong>corporates the perfect<br />
conductor boundary condition for the electric field.<br />
I. G. Stratis (Maths Dept, NKUA) Collège de France November 18, 2011 36 / 95