Undergrad Understanding Admit & Adapt: Timelike Killing Vector Field

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A space-time is stationary if it has a timelike Killing vector field, which indicates a symmetry in time. The term "admit" means that the space-time possesses such a vector field, while "adapted" refers to a coordinate system that aligns with this vector field. It is possible to choose a coordinate system where the Killing vector field takes a specific form, such as ##X^a=\delta^a_0##, but this is not mandatory. Different coordinate systems, like Kruskal-Szekeres, can represent the same physical situation without adhering to this form. Ultimately, the choice of coordinates is flexible and can be tailored to the problem at hand.
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"A space-time is said to be stationary if and only if it admits a timelike Killing vector field"
"...given a a timelike Killing vector field,then there always exists a coordinate system which is adapted to the Killing vector field##X^a##,that is,in which##X^a=\delta^a_0##holds..."
How to understand "admit"and"adapt"?Does it mean that ##X^a=\delta^a_0## may not hold even if there exists a timelike Killing vector field?Thanks!
 
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Admits, in this context, is a fancy way of saying "has". Stationary spacetimes are those that have a timelike Killing vector field.

"Adapted to" means "well matched to". You can always pick a coordinate system with a timelike basis parallel to the Killing field. It's often a good idea because then your definition of space can be independent of time, and Schwarzschild coordinates are an example of this. But as always with coordinates you are free to make any choice you like. In Kruskal-Szekeres coordinates, for example, the integral curves of the Killing vector field form hyperbolas. You don't even have to have a timelike basis vector if you don't want to.
 
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MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

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