Killing vector field => global isomorphisms?

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The discussion revolves around the relationship between Killing vector fields and global isometries on manifolds. It is established that a Killing vector field generates local flows that are isometries, but these flows may not be globally defined on non-compact manifolds. The example of the open upper half-plane illustrates that the flow can be undefined for certain points, highlighting the limitations of non-compact spaces. In contrast, compact manifolds allow for global flows due to finite coverage by open sets. The conversation concludes with the clarification that while complete vector fields can exist on non-compact manifolds, they do not necessarily yield global isometries.
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Suppose we have a vector field ##V## defined everywhere on a manifold ##M##. Consider now point ##p \in M##. As a consequence of the existence and uniqueness theorem of differential equations. this implies that ##V## gives rise to a unique local flow
$$\theta:(-\epsilon,\epsilon) \times U \to M$$
for ##(-\epsilon,\epsilon) \in \mathbb{R}## and ##p \in U## where ##U## is an open subset of M.

Now if ##\theta_t(p) = \theta(t,p)##, and if ##V## is a killing field, then ##\theta_t: U \to M## should be isometries. But do they belong to isometry group ##Isom(M)##? I.e. are they global as a consequence of ##V## being globally defined and a killing field?

Is there not a bijective correspondence between global isometries and globally defined Killing vector fields?
 
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The issue is that for a given t, no matter how small, \theta_t(p) may not be defined for all p in M. The typical example is M= open upper half plane and V = -\partial/\partial y. Given any t, you can always choose For p=(x,y) with y small enough so that the flow at time t is not defined (because following the flow would "take us out of M").

But if M is compact, you can cover it with finitely many open sets U_i on which the flow is defined on (-\epsilon_i,\epsilon_i). Then for |t|<\epsilon:=\min_i\epsilon_i, the flow is defined globally.

Also, if V is complete, then its flow is defined on all M for all t.
 
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quasar987 said:
The issue is that for a given t, no matter how small, \theta_t(p) may not be defined for all p in M. The typical example is M= open upper half plane and V = -\partial/\partial y. Given any t, you can always choose For p=(x,y) with y small enough so that the flow at time t is not defined (because following the flow would "take us out of M").

But if M is compact, you can cover it with finitely many open sets U_i on which the flow is defined on (-\epsilon_i,\epsilon_i). Then for |t|<\epsilon:=\min_i\epsilon_i, the flow is defined globally.

Also, if V is complete, then its flow is defined on all M for all t.

I see the problem here when ##M## is not compact. Does this then imply that ##\text{Isom(M)}## does not contain any globally defined one-parameter subgroups? For then it seems possible to use these to define a global action who's induced vector field would be Killing fields.
 
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Even if M is not compact there can exist complete vector fields.

For instance, let f:R-->R be a smooth "bump function" which is 0 on [0,½] and 1 on [1,oo), and let V'(x,y):=-f(y)\partial/\partial y. This is a Killing field on our open half plane whose flow is defined on all of M for all t.
 
quasar987 said:
Even if M is not compact there can exist complete vector fields.

For instance, let f:R-->R be a smooth "bump function" which is 0 on [0,½] and 1 on [1,oo), and let V'(x,y):=-f(y)\partial/\partial y. This is a Killing field on our open half plane whose flow is defined on all of M for all t.

I have to disagree there. ##V' \equiv - f(y) \, \partial_y## is not Killing on the upper-half-plane with standard Euclidean metric (which I think you have been discussing):

\mathcal{L}_{V'} \big( dx \otimes dx + dy \otimes dy \big) = - 2 \frac{\partial f}{\partial y} \, dy \otimes dy \neq 0.
Your attempt to "compress" the flow of ##V'## causes it to fail to preserve the metric between ##\frac12 < y < 1##.

The upper-half-plane with Euclidean metric is geodesically incomplete, which is why ##V \equiv \partial_y## fails to be a global isometry.
 
Oh yes of course, bad example! Thx Ben.
 
I should maybe say then that d/dx is Killing complete on the open upper half-plane.
 

After reading up on flows in John Lee's "introduction to smooth manifolds" at page 212 he states the fundamental theorem of flows which asserts that given a smooth vector field ##V## on ##M## there exists a unique smooth maximal flow ##\theta: D \to M##, where ##D## is an open subset of ##\mathbb{R} \times M##, such that ##\theta^{(p)}: (-\epsilon_p,\epsilon_p) \to M## is the unique maximal integral curve starting at ##p##.

I might have misunderstood your argument for ##-\partial_y## on the upper half plane, but does it not imply that such a maximal flow does not exist?
 
Never mind. I got it straighten out.
 

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