Compact support of matter fields

In summary, the conversation discusses the relationship between compact support and asymptotic behaviour of matter fields and the Riemann tensor in a certain spacetime. It is noted that saying the matter fields have compact support means they vanish outside of some finite spatial region, while asymptotic behaviour refers to their fall-off rate near infinity. It is also stated that the Ricci tensor will have compact support if the matter fields do, but this is not necessarily true for the Riemann tensor. However, in three dimensions, compactly supported matter fields do imply that the Riemann tensor also has compact support.
  • #1
haushofer
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Hi,

I have a question concerning the asymptotic boundary conditions on matter fields and the Riemann tensor. What is the precise relation between saying that "the matter fields go to zero at spatial infinity" and "the matter fields have compact support"? And how natural is it to state that the Riemann tensor has "compact support" on a certain spacetime? I would say that if the matter fields have compact support, the Riemann tensor also has, right?

Thanks!
 
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  • #2
It seems to me that people often abuse the concept of "having compact support" whenever they actually mean a certain asymptotic behaviour. Can anyone comment on this?
 
  • #3
To say that the matter fields have compact support means that their intersection with a Cauchy surface has compact support in the mathematical sense. This is usually used loosely to mean that all matter fields (exactly) vanish outside of some finite spatial region. Saying that the matter fields fall off at some rate near infinity is therefore a weaker condition.

Einstein's equation implies that the Ricci tensor will have compact support if the matter fields do. The same is not true of the Riemann tensor. It will usually fall off at some rate as one moves away from the matter, but there is no radius beyond which it will vanish.
 
  • #4
Ok, thanks! But in three dimensions compactly supported matter fields then do imply that the Riemann tensor has compact support, right?
 
  • #5
Yes, that's right.
 

1. What is the definition of compact support of matter fields?

The compact support of matter fields refers to the region in space where the matter fields have non-zero values. It is a mathematical concept used in theoretical physics to describe the extent of the influence of matter fields in a given space.

2. How is compact support related to the size of particles?

The compact support of matter fields is directly related to the size of particles. The smaller the compact support, the smaller the size of the particles. This is because a smaller compact support means that the matter fields have a smaller influence and are more localized in space.

3. Can compact support of matter fields change over time?

Yes, the compact support of matter fields can change over time. In some physical theories, the compact support is fixed and does not change, but in other theories, it can vary depending on the dynamics of the system. For example, in quantum field theory, the compact support of matter fields can change due to interactions between particles.

4. What are the implications of a compact support in quantum mechanics?

In quantum mechanics, a compact support of matter fields has important implications. It allows for the localization of particles in space and explains the discrete energy levels of atoms and molecules. It also plays a crucial role in the uncertainty principle, as the more localized a particle is in space, the less certain we are about its momentum.

5. How is compact support related to the conservation of energy and momentum?

The compact support of matter fields is related to the conservation of energy and momentum in the sense that it determines the extent of the influence of matter fields in a given space. This, in turn, affects the exchange of energy and momentum between particles. In other words, the compact support helps to define the boundaries within which the conservation laws of energy and momentum hold.

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