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Appendix A<br />
The Derivatives of the DSM Energy<br />
The first and second derivatives of the DSM energy model with respect to c is found recalling that<br />
and<br />
DSM<br />
( ) ( )<br />
( ) ( ) 2Tr<br />
E c = E D + 2TrFD δ , (A-1)<br />
E D = E D0 + DF + 0 + TrDF, + +<br />
(A-2)<br />
n<br />
D = c ( D −D ), (A-3)<br />
+<br />
∑<br />
i=<br />
1<br />
The two terms in Eq. (A-1) is evaluated one by one:<br />
and<br />
∂E<br />
∂c<br />
( D )<br />
x<br />
i<br />
i<br />
0<br />
D δ = 3DSD −2DSDSD −D. (A-4)<br />
= Tr DF − Tr DF + Tr DF + Tr DF−Tr DF −Tr<br />
DF (A-5)<br />
x 0 0 x x x<br />
0 0<br />
∂<br />
∂F<br />
∂D<br />
2TrFDδ<br />
= 2Tr Dδ<br />
+ 2TrF<br />
∂c ∂c ∂c<br />
x x x<br />
∂Dδ<br />
= 2TrFD<br />
x δ + 2Tr F ,<br />
∂c<br />
x<br />
δ<br />
(A-6)<br />
where<br />
∂D<br />
∂<br />
δ<br />
c x<br />
= 3DSD + 3D SD −2DSDSD −2DSD SD −2D SDSD −D . (A-7)<br />
The second derivative is found in the same manner<br />
∂<br />
where<br />
2<br />
E<br />
∂c<br />
x<br />
( D )<br />
∂c<br />
y<br />
x x x x x x<br />
= 2TrDF + TrDF + TrDF −TrDF −TrDF −TrDF −TrDF, (A-8)<br />
0 0 x y y x 0 x x 0 y 0 0 y<br />
2<br />
2<br />
∂<br />
∂ δ ∂ δ ∂ δ<br />
2Tr δ = 2Tr D x + 2Tr D y + 2Tr<br />
D<br />
x y y x x y<br />
FD F F F , (A-9)<br />
∂c ∂c ∂c ∂c ∂c ∂c<br />
2<br />
∂ D<br />
∂c<br />
∂c<br />
x<br />
δ<br />
y<br />
= 3D SD + 3D SD −2DSD SD −2D SDSD −2DSD SD<br />
y x x y y x y x x y<br />
−2DSDSD−2DSDSD −2 DSDSD.<br />
y x x y x y<br />
(A-10)<br />
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