Symmetries of Higher Dimensions & Extra Spacetimes

In summary: Yes, any isometry corresponds to the existence of a Killing vector field. From the Killing vector, we can define a conjugate coordinate, at least locally, for which the isometry corresponds to a translation.
  • #1
latentcorpse
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Is it true to say that most higher dimensional spacetimes have symmetries amongst their n extra dimensions?

Thanks.
 
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  • #2
latentcorpse said:
Is it true to say that most higher dimensional spacetimes have symmetries amongst their n extra dimensions?

Thanks.

Most manifolds have no isometries at all, so no. If you are talking about some Kaluza-Klein or string theory model that would try to reproduce standard model physics, then there are additional constraints on the allowed manifolds that require certain symmetries.
 
  • #3
fzero said:
Most manifolds have no isometries at all, so no. If you are talking about some Kaluza-Klein or string theory model that would try to reproduce standard model physics, then there are additional constraints on the allowed manifolds that require certain symmetries.

Yeah. Thanks.

Just to clear up what an isometry actually is though:

I know it is a symmetry transformation of the metric tensor field.
i.e. a map [itex]\phi: M \rightarrow M[/itex] such that [itex](\phi)_*g=g[/itex]

However, what does this actually mean?

Suppose the metric is invariant of t. We can see from Killing's equation that [itex]\frac{\partial}{\partial t}[/itex] will be a Killing vector field easily enough but what does this actually mean the isometry is?
Would the isometry be the map [itex]\phi: M \rightarrow M ; t \mapsto t+c[/itex] i.e. time translations?

Thanks.
 
  • #4
latentcorpse said:
Yeah. Thanks.

Just to clear up what an isometry actually is though:

I know it is a symmetry transformation of the metric tensor field.
i.e. a map [itex]\phi: M \rightarrow M[/itex] such that [itex](\phi)_*g=g[/itex]

However, what does this actually mean?

Suppose the metric is invariant of t. We can see from Killing's equation that [itex]\frac{\partial}{\partial t}[/itex] will be a Killing vector field easily enough but what does this actually mean the isometry is?
Would the isometry be the map [itex]\phi: M \rightarrow M ; t \mapsto t+c[/itex] i.e. time translations?

Thanks.

Yes, any isometry corresponds to the existence of a Killing vector field. From the Killing vector, we can define a conjugate coordinate, at least locally, for which the isometry corresponds to a translation.
 
  • #5


I can say that while it is true that many higher dimensional spacetimes have symmetries among their extra dimensions, it is not necessarily a universal truth. The existence of symmetries in higher dimensions is dependent on the specific model or theory being studied.

Some theories, such as string theory, propose the existence of extra dimensions that are compactified and have symmetries among them. This is because these symmetries play a crucial role in the mathematical framework of string theory, known as supersymmetry.

However, other theories, such as brane cosmology, do not require the existence of extra dimensions with symmetries. In fact, the brane world model proposes that our observable universe is a 3-dimensional brane embedded in a higher dimensional spacetime, where the extra dimensions are not necessarily symmetric.

Therefore, it is important to note that while symmetries among extra dimensions may be present in some models, it is not a universal feature of all higher dimensional spacetimes. Further research and experimentation are needed to fully understand the nature of these extra dimensions and their potential symmetries.
 

1. What are symmetries of higher dimensions?

Symmetries of higher dimensions refer to the ways in which objects or systems behave and appear the same when rotated, translated, or reflected in higher dimensional spaces. These symmetries play a crucial role in understanding the underlying structure and dynamics of the universe.

2. How are symmetries of higher dimensions related to extra spacetimes?

Extra spacetimes are additional dimensions beyond the three dimensions of space and one dimension of time that we are familiar with. Symmetries of higher dimensions are closely related to extra spacetimes because they describe the behavior of objects and systems in these additional dimensions.

3. Why are symmetries of higher dimensions important in physics?

Symmetries of higher dimensions are important in physics because they help us understand the fundamental laws and principles that govern the behavior of matter and energy in our universe. They also provide insights into the nature of space and time and can lead to new theories and discoveries.

4. Can symmetries of higher dimensions be observed or measured?

While we cannot directly observe or measure symmetries of higher dimensions, their effects can be seen and measured in the behavior of physical systems and particles. The study of these effects, such as particle interactions and the behavior of light, can provide evidence for the existence of higher dimensions and their symmetries.

5. How do symmetries of higher dimensions relate to theories like string theory and M-theory?

Symmetries of higher dimensions play a crucial role in theories like string theory and M-theory, which aim to unify all the fundamental forces and particles in the universe. These theories posit the existence of extra dimensions and use symmetries to describe the behavior of particles and interactions in these dimensions.

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