result

Now, it is time to express [Graphics:../Images/index_gr_427.gif] in terms of the φ derivatives.

[Graphics:../Images/index_gr_428.gif]
[Graphics:../Images/index_gr_429.gif]
[Graphics:../Images/index_gr_430.gif]
(dim*Log[2*Pi])/2 - psi[0] + (ry[l1]*ry[u1])/2 - 
(o*ry[l1]*tp3[l2, u1, u2])/2 +
(o*ry[l1]*ry[l2]*ry[l3]*tp3[u1, u2, u3])/6 -
(o^2*tp3[l1, l2, l3]*tp3[u1, u2, u3])/6 +
(o^2*ry[l1]*ry[l2]*tp3[l3, l4, u1]*tp3[u2, u3, u4])/4 +
(o^2*tp4[l1, l2, u1, u2])/8 -
(o^2*ry[l1]*ry[l2]*tp4[l3, u1, u2, u3])/4 +
(o^2*ry[l1]*ry[l2]*ry[l3]*ry[l4]*tp4[u1, u2, u3, u4])/24

The coefficients of [Graphics:../Images/index_gr_431.gif] as a polynomial of [Graphics:../Images/index_gr_432.gif] are as follows.

[Graphics:../Images/index_gr_433.gif]
[Graphics:../Images/index_gr_434.gif]


Converted by Mathematica      July 21, 2003