What is a Space-Time Crystal?

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SUMMARY

The discussion centers on the concept of Space-Time Crystals, specifically addressing the oscillation of systems in a ground state without external thermodynamic input. Participants reference the work of Frank Wilczek and highlight the implications of broken symmetry states, particularly regarding the Hamiltonian's representation in Hilbert space. The conversation also notes recent experimental evidence published in Nature, confirming the existence of Space-Time Crystals, which challenges traditional understandings of energy states in infinite systems.

PREREQUISITES
  • Understanding of quantum mechanics and Hamiltonian operators
  • Familiarity with broken symmetry states in physics
  • Knowledge of Hilbert space concepts
  • Awareness of recent advancements in condensed matter physics
NEXT STEPS
  • Read Frank Wilczek's presentation on Space-Time Crystals
  • Study the implications of broken symmetry in quantum systems
  • Examine the recent articles published in Nature regarding experimental evidence of Space-Time Crystals
  • Explore the concept of Hamiltonians in infinite systems and their implications
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Physicists, researchers in condensed matter physics, and students interested in advanced quantum mechanics and the implications of Space-Time Crystals.

dvdt
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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
 
Last edited:
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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