Suppose A is a non-singular matrix. AT is the transpose matrix of A. Therefore, the eigenvalue of A can be expressed as:
S-1AS=Λ
(S-1AS)T=ΛT
(AS)TS-T=STATS-T=Λ
So, AT and A share the same eigenvalue and eigenvector.
Here, x is the base eigenvector of A. Hence, span{x} is the eigenvector of...
Hi.
Are there someone working on Metallothionein? Maybe we can discuss on something because I am Electronic Engineering Student who work on the Bio-Sensor.
Edit: removed e-mail
Welcome.!
I think the \varpi coordinate should be normalized, if you want to have a good comprehension. When \varpi increase, it can not obey the SPPs but the free gas plasmons dispersion in upper band.
because E=-\nabla\varphi.
from upper equation \varphi=C1Z+C2;
so E=-C1=E0, it is independence with the position. So, I can said when Z=0 or somewhere z<1/2a, E=E0.
by the way, maybe it could be \epsilonE0 because of the continuity at the boundary.
So sorry, lots of confusion.
thank you very much!
But if I apply the Laplace Equation:
curl2φ=0, because φ is independence of x and y. So:
φ=C1Z+C2.
when Z increase to infinitude. E=-curlφ=-C1 =E0.
Suppose the midst of conductor layer is Z=0. when z=0, it always E=E0. But it should be 0, where am I wrong?
A 1-D metal put inside a E0 electric field just like shown in following figure.
--> |- <-- +| -->
--> |- <-- +| -->
--> |- <-- +| --> E0
--> |- <-- +| -->
--> |- <-- +| -->
Suppose the positive charge density of δ1, the negative charge density δ2, δ1=-δ2...