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befj0001
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If g_{ab},0 = 0 (g does not depend on time), then the manifold must have a timelike killing vector.
How can one prove that?
How can one prove that?
Why is this the wrong way to think of it?? It seems to me a perfectly reasonable way to think of it.WannabeNewton said:But this isn't the correct way to think about the time-like Killing field. Rather one first looks for the existence of a time-like vector field ##\xi^{\mu}## satisfying ##\nabla_{(\mu}\xi_{\nu)} = 0##. If such a vector field exists then there necessarily exists a coordinate system ##\{x^{\mu}\}## in which ##\partial_0 g_{\mu\nu} = 0## and ##\xi^{\mu} = \delta^{\mu}_0##.
befj0001 said:If g_{ab},0 = 0 (g does not depend on time), then the manifold must have a timelike killing vector.
A timelike Killing vector is a vector field in a spacetime that preserves the metric at every point along its flow. This means that the vector field is tangent to the geodesic curves of the spacetime and represents a symmetry of the metric. In other words, it describes a flow of spacetime that does not change the overall structure of the spacetime.
Proving timelike Killing vectors is important because it allows us to identify symmetries in a spacetime. This is crucial in understanding the behavior of matter and energy in the universe, as well as making predictions about the evolution of spacetime. It also plays a crucial role in the study of general relativity and the formulation of Einstein's equations.
The notation g_{ab},0 = 0 represents the derivative of the metric tensor g with respect to the time coordinate, which is set to equal zero. This is a way of expressing the requirement that the vector field must be timelike, as it ensures that the flow of spacetime is along the time coordinate and does not change the structure of the spacetime in the temporal direction.
To prove timelike Killing vectors for a given metric, one needs to show that the Lie derivative of the metric tensor along the vector field is equal to zero. This can be done by first calculating the Lie derivative and then setting it equal to zero and solving for the vector field components. This process may involve some mathematical manipulations and use of the metric tensor's symmetries.
Timelike Killing vectors have many important applications in physics and cosmology. They are used in the study of black holes, as they represent symmetries that preserve the black hole's event horizon. They are also used in the study of gravitational waves, as they help identify symmetries in the spacetime that can give rise to these ripples in the fabric of space. Additionally, timelike Killing vectors play a crucial role in the formulation of the Einstein field equations, which are the foundation of general relativity.