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The (~(yz)) M ((z(yy))z) class Let Q' be the class of all (~(yz)) x ((z(yy))z) graph algebras and Id(E') the set of all identities satisfied in B'.
By recalling that: E x * θ r = Z * xx (θ r) H x * θ r + Z * xy (θ r) H y * θ r, E y * θ r = Z * yx (θ r) H x * θ r + Z * yy (θ r) H y * θ r, we may reach the following physical explanation : the in-cidenceofa magnetic ...
Additionally, z yy > 0is satisfied if the target shape is a convex, where we use simple expressions such as z yy = ∂ 2 z/∂y 2 . It is known that Z YY > 0holdsif z> 0and z yy > 0[3].
(8) and (9), x X is expressed as x X = 1 d 1 + d 2 + d 3 + d 4, (10) d 1 =1+ z 2 x + z 2 y, (11) d 2 = z ( z xx + z yy)= z tr H z, (12) d 3 = z 2 ( z xx z yy −z 2 xy)= z 2 det H z, (13) d 4 = z ( z 2 x z yy + z 2 y z xx − 2 z x z y z xy) ...
#4 (Eäã4 #F å¨ xj)*+,-xj x /$1 x)*+$1 /$ 1 2 3 4 5## $678 Eäã4 FGHI ô# æ # NO:PQ ~[\ZÅ[]cV b\']TX^]a[aTb'm]b'VV]~b ba un b'qc}Z]'YY]mT[']o [XU ^'bcXYZWa[mbcSXm[]TWXYb}b'.. b\']T[mTX^eU]['_]Tb_b\']T ...
By recalling that: E x * r = Z * xx ( r) H x * r + Z * xy ( r) H y * r, E y * r = Z * yx ( r) H x * r + Z * yy ( r) H y * r, we may reach the following physical explanation : the in- ...
Additionally, z yy > 0is satisfied if the target shape is a convex, where we use simple expressions such as z yy = 2 z/y 2 . It is known that Z YY > 0holdsif z> 0and z yy > 0[3
(8) and (9), x X is expressed as x X = 1 d 1 + d 2 + d 3 + d 4, (10) d 1 =1+ z 2 x + z 2 y, (11) d 2 = z ( z xx + z yy)= z tr H z, (12) d 3 = z 2 ( z xx z yy z 2 xy)= z 2 det H z, (13) d 4 = z ( z 2 x z yy + z 2 y z xx 2 ...
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