Killing vectors in isotropic space-times

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Discussion Overview

The discussion revolves around the properties and implications of Killing vectors in isotropic space-times, particularly focusing on the conditions that must be satisfied at a point in the manifold. Participants explore the significance of the Killing vector fields vanishing at a point and the implications of the covariant derivative being non-zero.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that for an isotropic spacetime, the Killing vector fields must vanish at a point to maintain rotational symmetry, as this ensures that the point remains unchanged during transformations.
  • Others argue that the requirement for the covariant derivative of the Killing vector to be non-zero at that point is essential for generating rotations of neighboring points, as a zero derivative would imply no movement around the fixed point.
  • A later reply questions the intuition behind the condition that the Killing vector must vanish at the point, suggesting that it indicates there is no direction for transformation at that point.
  • Some participants clarify that the transformation generated by the Killing vector field can be viewed infinitesimally as a translation, reinforcing the idea that the Killing vector must be zero at the fixed point to prevent any change.

Areas of Agreement / Disagreement

Participants generally agree on the necessity of the Killing vector vanishing at a point for isotropy but express differing views on the implications and interpretations of the covariant derivative condition. The discussion remains unresolved regarding the deeper intuition behind these conditions.

Contextual Notes

Some limitations in understanding arise from the dependence on definitions of isotropy and the nature of Killing vectors, as well as the nuances of infinitesimal transformations.

"Don't panic!"
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I've been reading up on Killing vectors, and have got on to the topics of homogeneous, isotropic and maximally symmetric space-times. I've read that for an isotropic spacetime, one can construct a set of Killing vector fields ##K^{(i)}##, such that, at some point ##p\in M## (where ##M## is the space-time manifold), ##K^{(i)\mu}(p)=0## and ##\nabla_{\nu}K^{(i)\mu}(p)\neq 0##. Intuitively, I understand that we must have ##K^{(i)\mu}(p)=0##, since isotropy is a rotational symmetry, and so we don't want the Killing vectors to translate the points, we want them to rotate about them. However, I don't understand why we require ##\nabla_{\nu}K^{(i)\mu}(p)\neq 0##. Why must the covariant derivative of each Killing vector be arbitrary? I read that it has something to do with ##\nabla_{\nu}K^{(i)\mu}(p)## generating "rotations" of neighbouring points about ##p##, but this is unclear to me.
 
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"Don't panic!" said:
I understand that we must have ##K^{(i)\mu}(p)=0##, since isotropy is a rotational symmetry, and so we don't want the Killing vectors to translate the points, we want them to rotate about them.

That's not quite what the condition ##K^{(i)\mu}(p)=0## is saying. It is saying that any rotation must leave at least one point (the point ##p##) unchanged; hence, the action of the Killing vector on that point vanishes.

"Don't panic!" said:
I don't understand why we require ##\nabla_{\nu}K^{(i)\mu}(p)\neq 0##.

Because if it were zero, the action of the KVF on points neighboring ##p## would also vanish, but that's not what a rotation would do.
 
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PeterDonis said:
That's not quite what the condition K(i)μ(p)=0K(i)μ(p)=0K^{(i)\mu}(p)=0 is saying. It is saying that any rotation must leave at least one point (the point ppp) unchanged; hence, the action of the Killing vector on that point vanishes.

Ah ok. So the Killing vector will move about all other points, but will keep the point p, about which you are applying it, fixed. It must vanish because ##K^{\mu}## generates space-time translations, i.e. ##x'^{\mu}=x^{\mu}+\epsilon K^{\mu}##, right? (And so, at p, we must have ##x'^{\mu}=x^{\mu}##).

PeterDonis said:
Because if it were zero, the action of the KVF on points neighboring ppp would also vanish, but that's not what a rotation would do.

So intuitively, is this condition stating that at neighbouring points, the action of the KVF is non-zero (i.e. its components are non-zero), such that these points will move around relative to the fixed point p, i.e. a rotation?
 
"Don't panic!" said:
It must vanish because ##K^{\mu}## generates space-time translations, i.e. ##x'^{\mu}=x^{\mu}+\epsilon K^{\mu}##, right?

No. A spacetime translation would not leave any points unchanged. The Killing vector we are discussing generates rotations.

"Don't panic!" said:
is this condition stating that at neighbouring points, the action of the KVF is non-zero (i.e. its components are non-zero), such that these points will move around relative to the fixed point p, i.e. a rotation?

Yes.
 
PeterDonis said:
No. A spacetime translation would not leave any points unchanged. The Killing vector we are discussing generates rotations.

What is the intuition for why ##K^{\mu}=0## at a point p, such that it is unchanged?
 
"Don't panic!" said:
What is the intuition for why ##K^{\mu}=0## at a point p, such that it is unchanged

Heuristically, the Killing vector at any point "points" in the direction in which the transformation induced by the Killing vector field will "move" the point. So if the point is left unchanged by the transformation, it doesn't get "moved" anywhere, and the Killing vector must vanish since there is nowhere for it to "point".
 
PeterDonis said:
Heuristically, the Killing vector at any point "points" in the direction in which the transformation induced by the Killing vector field will "move" the point. So if the point is left unchanged by the transformation, it doesn't get "moved" anywhere, and the Killing vector must vanish since there is nowhere for it to "point".

But is the transformation generated by the KVF of the form ##x’^{\mu}=x^{\mu}+\epsilon K^{\mu}##? If so, it makes sense to me that ##K^{\mu}=0## at p, as then it won’t be transformed.
 
"Don't panic!" said:
is the transformation generated by the KVF of the form ##x’^{\mu}=x^{\mu}+\epsilon K^{\mu}##?

Infinitesimally, yes, you can view it that way. But only infinitesimally.
 
PeterDonis said:
Infinitesimally, yes, you can view it that way. But only infinitesimally.

Yes, sorry. I should have stated that I meant infinitesimally. So is it correct to say that, at the infinitesimal level, the reason why the KVF must vanish at the point p is because we require that it remains unchanged, i.e. ##x’^{\mu}=x^{\mu}##?
 
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"Don't panic!" said:
But is the transformation generated by the KVF of the form ##x’^{\mu}=x^{\mu}+\epsilon K^{\mu}##?
Just to interject that this is true for the flow generated by any vector field by definition.

"Don't panic!" said:
Yes, sorry. I should have stated that I meant infinitesimally. So is it correct to say that, at the infinitesimal level, the reason why the KVF must vanish at the point p is because we require that it remains unchanged, i.e. ##x’^{\mu}=x^{\mu}##?
Yes. Any point ##p## for which ##K(p) = 0## is a fixed point under the flow of ##K##. Again, this is regardless of whether ##K## is a Killing field or not.
 
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  • #11
Orodruin said:
Any point ppp for which K(p)=0K(p)=0K(p) = 0 is a fixed point under the flow of KKK. Again, this is regardless of whether KKK is a Killing field or not.

Thanks for the info. In the case where K is a killing field, is the interpretation of ##K(p)=0## at ##p##, that the point p remains fixed, i.e. its coordinates remain unchanged?
 
  • #12
Why would it change just because it is a Killing field?
 
  • #13
Orodruin said:
Why would it change just because it is a Killing field?

You’re right, I got myself mixed up there.
 

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