For every continuous linear operator A: H \rightarrow H from a Hilbert space H to itself, there is a unique continuous linear operator A^* called its Hermitian adjoint such that
\langle Ax, y \rangle = \langle x, A^* y \rangle
for all x,y \in H.
Given that \mathcal{L}_X: \Omega^0(M)...
I'm working thru Thirring's Classical Mathematical Physics. The lie derivative is defined and used on a vector field. I.e. L(x)f where x is a vector field. () = subscript
However, later on, he uses the lie derivative of the hamiltonian, which is a scalar function. I.e. L(H)f () =...
Homework Statement
Hi,
it's the first time I post here, so apologies if this is not the right place.
I'm trying to self-study GR, but I'm stuck with Lie Derivatives. The book I'm using (Ludvigsen - General Relativity. A geometric approach) starts with the usual definitions and then gives...
Homework Statement
Calculate the lie derivative of the metric tensor, given the metric,
g_{ab}=diag(-(1-\frac{2M}{r}),1-\frac{2M}{r},r^2,R^2sin^2\theta)
and coordinates (t,r,theta,phi)
given the vector
E^i=\delta^t_0
Homework Equations...
Can somone remind me how to see that the Lie derivative of a vector field, defined as
(L_XY)_p=\lim_{t\rightarrow 0}\frac{\phi_{-t}_*Y_{\phi_t(p)}-Y_p}{t}
is actually equal to [X,Y]_p?
I'm trying to use an example to make sense out of the equation
\mathcal{L}_X = d\circ i_X + i_X\circ d.
Some simple equations:
\omega = \omega^1 dx_1 + \omega^2 dx_2
i_X\omega = X_1\omega^1 + X_2\omega^2
(d\omega)^{11} = (d\omega)^{22} = 0,\quad (d\omega)^{12} =...
Suppose you have a spacetime with an observer at rest at the origin, and the surface at t = 0 going through the origin, and passing through the surface there are geodesics along increasing time. Then as you get a small ways away from the surface, the geodesics start to deviate from each other...
Suppose we define the Lie derivative on a tensor T at a point p in a manifold by
\mathcal{L}_V (T) = \lim_{\epsilon \to 0}\frac{\varphi_{-\epsilon \ast}T(\varphi_\epsilon(p))- T(p)}{\epsilon}
where V is the vector field which generates the family of diffeomorphisms \varphi_t.
If T is just an...
Loosely speaking or Intuitively how should one understand the difference between Lie Derivative and Covariant derivative? Definitions for both sounds awfully similar...
Let M be a diff. manifold, X a complete vectorfield on M generating the 1-parameter group of diffeomorphisms \phi_t. If I now define the Lie Derivative of a real-valued function f on M by
\mathscr{L}_Xf=\lim_{t\rightarrow 0}\left(\frac{\phi_t^*f-f}{t}\right)=\frac{d}{dt}\phi_{t}^{*}f |_{t=0}...
I'd like an example of calculating the Lie derivative of a one-form with respect to a vector field, for example, the one-form
\omega = 3 dx_1 + 4x dx_2
with the vector field
X = 7x \frac{\partial }{\partial x_1} + 2 \frac{\partial }{\partial x_2}
Any input would be...