| Schwarzschild black hole with cosmological constant Copyright © 2004-2008 by DigiArea Group . All rights reserved. Problem: Schwarzschild black hole with cosmological constant is 4-dimentional Lorentz manifold with constant Ricci curvature , timelike Killing vector field and group as a subgroup of the manifold isometry group (with spacelike orbits). For Schwarzschild metric calculate the following: - connetion 1-forms
- curvature 2-forms
- Riemannin tensor field
- Ricci tensor field
Verify that are Killing vector vields.
Schwarzschild metric restart: with(atlas): Constants: Constants(r[g],Lambda); ![{Pi, I, _Z, Catalan, Lambda, r[g], -I}](prod/atlas/Templates/images/schw4.gif)
Vector fields: Vectors(E[i],X,Y,Z); ![{X, Y, Z, E[i]}](prod/atlas/Templates/images/schw5.gif)
Differential p-forms: Forms(e[j]=1); ![{e[j]}](prod/atlas/Templates/images/schw6.gif)
Coframe 1-forms: Coframe(e[1]=d(t),e[2]=d(rho),e[3]=d(theta),e[4]=d(phi)); ![[e[1] = d(t), e[2] = d(rho), e[3] = d(theta), e[4] = d(phi)]](prod/atlas/Templates/images/schw7.gif)
Frame vector fields: Frame(E[i]); ![[E[1] = Diff(``,t), E[2] = Diff(``,rho), E[3] = Diff(``,theta), E[4] = Diff(``,phi)]](prod/atlas/Templates/images/schw8.gif)
Metric tensor field : Metric( g=(1-r[g]/rho+Lambda/3*rho^2)*d(t)&.d(t)-1/(1-r[g]/rho+Lambda/3*rho^2)*d(rho)&.d(rho)-rho^2*(d(theta)&.d(theta)+sin(theta)^2*d(phi)&.d(phi)) ); ![g = (1-r[g]/rho+1/3*Lambda*rho^2)*`&.`(e[1],e[1])-1/(1-r[g]/rho+1/3*Lambda*rho^2)*`&.`(e[2],e[2])-rho^2*(`&.`(e[3],e[3])+sin(theta)^2*`&.`(e[4],e[4]))](prod/atlas/Templates/images/schw9.gif)
Connection 1-forms: Connection(omega); ![omega[i,j]](prod/atlas/Templates/images/schw10.gif)
eval(omega); ![TABLE([(4, 3) = 1/sin(theta)*cos(theta)*e[4], (3, 4) = -sin(theta)*cos(theta)*e[4], (4, 4) = 1/rho*e[2]+1/sin(theta)*cos(theta)*e[3], (1, 2) = 1/2*1/rho/(3*rho-3*r[g]+Lambda*rho^3)*(3*r[g]+2*Lambda*rho...](prod/atlas/Templates/images/schw17.gif)
Curvature 2-forms: Curvature(Omega); ![Omega[i,j]](prod/atlas/Templates/images/schw18.gif)
eval(Omega); ![TABLE([(4, 3) = 1/3*(Lambda*rho^3-3*r[g])/rho*`&^`(e[3],e[4]), (3, 4) = -1/3*sin(theta)^2*(Lambda*rho^3-3*r[g])/rho*`&^`(e[3],e[4]), (4, 4) = 0, (1, 2) = -(Lambda*rho^3-3*r[g])/rho^2/(3*rho-3*r[g]+Lamb...](prod/atlas/Templates/images/schw27.gif)
Curvature tensor field: Riemann(R); ![R = -1/3*1/rho^3*(Lambda*rho^3-3*r[g])*`&.`(`&^`(e[1],e[2]),`&^`(e[1],e[2]))+1/2*1/(3*rho-3*r[g]+Lambda*rho^3)*(3*r[g]+2*Lambda*rho^3)*`&.`(`&^`(e[2],e[3]),`&^`(e[2],e[3]))-1/18*1/rho^2*(3*r[g]+2*Lambd...](prod/atlas/Templates/images/schw32.gif)
Ricci tensor field calculation: Ricci(ric); ![ric = 1/3*Lambda/rho*(3*rho-3*r[g]+Lambda*rho^3)*`&.`(e[1],e[1])-3*rho/(3*rho-3*r[g]+Lambda*rho^3)*Lambda*`&.`(e[2],e[2])-Lambda*rho^2*`&.`(e[3],e[3])-sin(theta)^2*Lambda*rho^2*`&.`(e[4],e[4])](prod/atlas/Templates/images/schw34.gif)
Verify that metric is Einstein one: 'ric'-Lambda*g=simplify(ric-Lambda*ToBasis(g)); 
Verify that and are Killing vector fields: 'L[E[1]](g)'=L[E[1]](g); ![L[E[1]](g) = 0](prod/atlas/Templates/images/schw39.gif)
'L[E[4]](g)'=L[E[4]](g); ![L[E[4]](g) = 0](prod/atlas/Templates/images/schw40.gif)
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