Undergrad Uniform Translation of a Lattice

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SUMMARY

The discussion centers on the concept of translational symmetry in crystal lattices, specifically addressing the implications of uniform displacement and its energy cost. The author clarifies that while a crystal lattice breaks continuous translational symmetry, uniform translations do not incur energy costs due to the presence of long wavelength modes, as articulated in Goldstone's theorem. This relationship highlights the nuances of symmetry breaking and its effects on atomic interactions within the lattice.

PREREQUISITES
  • Understanding of translational symmetry in physics
  • Familiarity with Goldstone's theorem
  • Knowledge of crystal lattice structures
  • Basic principles of energy interactions in solid-state physics
NEXT STEPS
  • Study the implications of Goldstone's theorem in condensed matter physics
  • Explore the concept of long wavelength modes in crystal lattices
  • Investigate the role of symmetry breaking in physical systems
  • Learn about the mathematical formulation of translational symmetry in solid-state physics
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Physicists, materials scientists, and students studying condensed matter physics who are interested in the principles of symmetry and energy interactions in crystal structures.

thatboi
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I'm currently reading through this brief review on symmetries, and on page 5, the following statement is made: "Why is there no energy cost for a uniform displacement? Well, there is a translational symmetry: moving all the atoms the same amount doesn’t change their interactions. But haven’t we broken that symmetry? That is precisely the point." Perhaps I just misunderstood the punchline, but what exactly did the author mean by the last sentence, "that is precisely the point"? The crystal lattice has broken continuous translational symmetry, but what does that have to do with uniform translations of the lattice and the action costing 0 energy?
 
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This is just a cryptic way of stating Goldstone's theorem. Associated with the spontaneous breaking of a continuous symmetry is the introduction of long wavelength modes. The uniform translation of the lattice is the long wavelength mode.
 

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