Euclidean Killing Field Question

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The discussion centers on the properties of Killing fields in the context of the Euclidean 2-metric, specifically the translations represented by K_1 = ∂/∂x and K_2 = ∂/∂y, along with the rotational Killing field K_3. The components of K_3 must satisfy the differential equation ∂K^y/∂x + ∂K^x/∂y = 0, leading to two solutions: (K^x, K^y) = (-y, x) and (K^x, K^y) = (y, -x). These solutions represent rotations in opposite directions, raising the question of whether the orientation of the field matters or if the general flow is sufficient for equivalence.

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Kreizhn
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Hey,

This may seem like a simple question, but hopefully someone can answer it quickly.

Consider the Euclidean 2-metric ds^2 = dx^2 + dy^2. There are three killing fields, two translations
K_1 = \frac{\partial}{\partial x}, \qquad K_2 = \frac{\partial}{\partial y}
and a rotation. Now my issue is this, if K_3 is the rotational Killing field, with coordinate decomposition
K_3 = K_3^x \frac{\partial}{\partial x} + K_3^y \frac{\partial}{\partial y}
We can show that K_3's components must satisfy the differential question
\frac{\partial K^y}{\partial x} + \frac{\partial K^x}{\partial y} = 0
Hence we can have two solutions (K^x,K^y) = (-y,x) and (K^x,K^y) = (y, -x). Clearly these are just a multiple of -1 different. But if one were to plot these, they would give rotations in opposite directions. One would move clockwise, the other counter-clockwise.

Do we care about the orientation of the field? Or just it's general flow? Do these both represent the same field all the same?
 
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Is it because the flow (as a one parameter semi-group) can move in both directions? Hence the flow generated by each is equivalent, and just corresponds to taking a negative "time?"
 

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