I What is a Space-Time Crystal?

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A space-time crystal is a theoretical structure that oscillates in its ground state, raising questions about the nature of such oscillation without external thermodynamic input. The discussion highlights the complexity of broken symmetry states, where the Hamiltonian cannot be represented as an operator in Hilbert space, complicating the understanding of energy states. Recent experimental evidence supporting the existence of space-time crystals has been published in Nature, indicating that these concepts may have practical implications. The conversation underscores the challenges in reconciling theoretical frameworks with observable phenomena. Overall, the existence and implications of space-time crystals remain a significant topic in contemporary physics.
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I know what the definition is, but the concept it's conjuring for me seems in my experience of learning about these things, to indicate that I'm missing the point completely. What does it mean for something to be oscillating when it's in a ground state? I was under the impression that such a thing is impossible unless there's some external thermodynamic input. Is this a hypothetical structure that is believed *not* to exist, but is interesting as a thought experiment?

Naively it sounds like a PPM, which is why I assume that I must be missing quite a bit.
 
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I just read the presentation by Wilczek cited in Wikipedia:
http://www.ctc.cam.ac.uk/stephen70/talks/swh70_wilczek.pdf

A general feature of broken symmetry states (which Wilczek doens't mention) is that the generator of the broken symmetry - i.e. the Hamiltonian in our case -
can't be represented as an operator in the Hilbert space any more. For infinite systems, whether time translation symmetry is broken or not, this is the generic case. E.g. a gas of atoms of which a given fraction is in an excited state has infinite energy relative to the ground state. Hence the hamiltonian is not a well defined operator.
So we can't rely on any proof that the hamiltonian has only non-degenerate ground states simply because the Hamiltonian does not exist.

Edit: I just found this article which elaborates on the comment I made:
https://arxiv.org/pdf/1605.04188v1.pdf
 
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DrDu said:
I just read the presentation by Wilczek cited in Wikipedia:
http://www.ctc.cam.ac.uk/stephen70/talks/swh70_wilczek.pdf

A general feature of broken symmetry states (which Wilczek doens't mention) is that the generator of the broken symmetry - i.e. the Hamiltonian in our case -
can't be represented as an operator in the Hilbert space any more. For infinite systems, whether time translation symmetry is broken or not, this is the generic case. E.g. a gas of atoms of which a given fraction is in an excited state has infinite energy relative to the ground state. Hence the hamiltonian is not a well defined operator.
So we can't rely on any proof that the hamiltonian has only non-degenerate ground states simply because the Hamiltonian does not exist.

Edit: I just found this article which elaborates on the comment I made:
https://arxiv.org/pdf/1605.04188v1.pdf

Thanks for the explanation, and the links!
 
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