$$ f(u) = e^{(-(3.15987540437407e-36)*(99446621081482098*u1 + 99446621081482098*u2 + 99446621081482098*u3 + 49723310540741049*u4 + 99446621081482098*u5 + 165744368469136820*u6 + 198893242162964181*u7 +298339863244446264)^2 - (3.15987540437407e-38)*(1790039179466677674*u1 - 2983398632444462490*u2 - 2983398632444462490*u3 - 1491699316222231245*u4 - 2983398632444462490*u5 - 2320421158567915270*u6 - 1988932421629641660*u7 - 994466210814820830)^2 - (3.15987540437407e-38)*(1790039179466677674*u1 + 2983398632444462715*u2 + 2320421158567915470*u3 - 1491699316222231245*u4 - 2983398632444462490*u5 - 2320421158567915270*u6 + 1988932421629641810*u7 - 994466210814820830)^2 - (3.15987540437407e-38)*(1790039179466677674*u1 + 2983398632444462715*u2 + 2320421158567915470*u3 - 1491699316222231245*u4 + 4972331054074104450*u5 - 2320421158567915270*u6 + 1988932421629641810*u7 - 994466210814820830)^2 - (3.15987540437407e-38)*(1790039179466677674*u1 + 2983398632444462715*u2 + 2320421158567915470*u3 + 4475097948666693960*u4 + 4972331054074104450*u5 + 5635308527950651670*u6 + 1988932421629641810*u7 - 994466210814820830)^2 - (3.15987540437407e-38)*(1790039179466677674*u1 + 2983398632444462715*u2 + 4972331054074104450*u3 + 4475097948666693960*u4 + 4972331054074104450*u5 + 5635308527950651670*u6 + 1988932421629641810*u7 - 994466210814820830)^2 - (3.15987540437407e-36)*(99446621081482098*u1 + 99446621081482098*u2 + 99446621081482098*u3 + 49723310540741049*u4 + 99446621081482098*u5 + 165744368469136820*u6 - 198893242162964166*u7 - 397786484325928347*u8 + 298339863244446264)^2 - (3.15987540437407e-36)*(99446621081482098*u1 + 99446621081482098*u2 + 99446621081482098*u3 + 49723310540741049*u4 + 99446621081482098*u5 + 165744368469136820*u6 + 198893242162964181*u7 + 397786484325928347*u8 + 298339863244446264)^2)}$$
I also tried to use simplify_full() command in sage to simplify it which gives me a simplified form. My code for taylor expansion is as follows:
PLM = f(u)
Taylor_Expansion = []
#Taylor series is expanded at the origin i.e. (0,0,0,0,0,0,0,0)
b1=0;b2=0;b3=0;b4=0;b5=0;b6=0;b7=0;b8=0;
for n1 in [0..sum_limit]:
for n2 in [0..sum_limit]:
for n3 in [0..sum_limit]:
for n4 in [0..sum_limit]:
for n5 in [0..sum_limit]:
for n6 in [0..sum_limit]:
for n7 in [0..sum_limit]:
for n8 in [0..sum_limit]:
#const1 is the part of the Taylor series without partial derivatives term
const1 = ((u1 - b1)^n1*(u2-b2)^n2*(u3-b3)^n3*(u4-b4)^n4*(u5-b5)^n5*(u6-b6)^n6*(u7-b7)^n7*(u8-b8)^n8)/(factorial(n1)* factorial(n2)*factorial(n3)*factorial(n4)*factorial(n5)*factorial(n6)*factorial(n7)*factorial(n8))
f = PLM.full_simplify()
if n8>0:
for dif8 in [1..n8]:
f = derivative(f,u8)
if n7>0:
for dif7 in [1..n7]:
f = derivative(f,u7)
if n6>0:
for dif6 in [1..n6]:
f = derivative(f,u6)
if n5>0:
for dif5 in [1..n5]:
f = derivative(f,u5)
if n4>0:
for dif4 in [1..n4]:
f = derivative(f,u4)
if n3>0:
for dif3 in [1..n3]:
f = derivative(f,u3)
if n2>0:
for dif2 in [1..n2]:
f = derivative(f,u2)
if n1>0:
for dif1 in [1..n1]:
f = derivative(f,u1)
ff = f
#const2 is the term with partial derivatives and after evaluation at point (0,0,0,0,0,0,0,0)
const2 = ff.substitute(u1=b1,u2=b2,u3=b3,u4=b4,u5=b5,u6=b6,u7=b7,u8=b8)
eqn = const1*const2
Taylor_Expansion.append(eqn)