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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 />

91

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