Understanding Inversion Symmetry and Space Symmetry Breaking

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    Inversion Symmetry
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Discussion Overview

The discussion revolves around the concepts of inversion symmetry and space symmetry breaking, particularly in the context of two-dimensional lattices, ferroelectricity, and induced magnetism and superconductivity. Participants explore definitions, implications, and examples related to these symmetry concepts in physics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants note that while two-dimensional oblique lattices may not exhibit special symmetry, they still possess inversion symmetry, raising questions about the implications of the transformation r → -r.
  • It is mentioned that atomic displacements can break space symmetry, which is linked to the emergence of ferroelectricity, though the mechanism of how this occurs is questioned.
  • A participant provides a definition of the inversion symmetry operator and states that all "naked" Bravais lattices have inversion symmetry, emphasizing that electric polarization must be zero in such crystals to prevent ferroelectricity.
  • Another participant introduces the concept of time reversal symmetry, explaining its effects on linear momentum, angular momentum, and magnetic moments in ordered materials, particularly in ferromagnets.
  • There is a request for clarification on the relationship between gauge symmetry breaking and phenomena such as superconductivity and superfluidity, with a reference to an external article for further reading.

Areas of Agreement / Disagreement

Participants express differing views on the implications of inversion symmetry and the mechanisms behind space symmetry breaking. The discussion remains unresolved regarding the specific conditions under which these symmetries influence physical properties.

Contextual Notes

Some statements rely on specific definitions of symmetry and may depend on the context of the materials being discussed. The relationship between symmetry breaking and physical phenomena like ferroelectricity, magnetism, and superconductivity is complex and not fully resolved in the discussion.

fyw
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1. P. Marder ever said that there is no special symmetry results in two dimensional oblique lattice. But it still possesses inversion symmetry. r-r
How to understand r-r?

2. Many book ever states that space symmetry broken by atomic displacement can bring ferroelectricity. But why this kind of displacement breaks the space symmetry?
 
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The definition of the inversion symmetry operator I that it transforms a vector into a different vector of same magnitude but antiparallel orentation. This can be written in many ways, e.g. I(r) = -r, or r --> -r, where r is a vector. All "naked" Bravais lattices have inversion symmetry (=they are invariant under inversion symmetry).

Special symmetry elements in 2D are mirror axes and 60, 90 or 180deg rotation symmetry.

http://en.wikipedia.org/wiki/Bravais_lattice

Electric polarization is a vector. Therefore I(P) = -P. If the crystal is invariant under inversion symmetry, then P=0 and the crystal cannot be ferroelectric.
 
M Quack said:
The definition of the inversion symmetry operator I that it transforms a vector into a different vector of same magnitude but antiparallel orentation. This can be written in many ways, e.g. I(r) = -r, or r --> -r, where r is a vector. All "naked" Bravais lattices have inversion symmetry (=they are invariant under inversion symmetry).

Special symmetry elements in 2D are mirror axes and 60, 90 or 180deg rotation symmetry.

http://en.wikipedia.org/wiki/Bravais_lattice

Electric polarization is a vector. Therefore I(P) = -P. If the crystal is invariant under inversion symmetry, then P=0 and the crystal cannot be ferroelectric.

Dear Quack,

Thank you for your answer. I've got it.
Additionally, can you explain the time symmetry broken induced magnetism and gauge symmetry broken induced superconductor or superliquid?
 
Time reversal inverts linear momentum (p) and therefore angular momentum, L. It also inverts the spin, S and therefore the magnetic moment.

In a magnetically ordered material, there are well-defined expectation values of the magnetic moment. For example, in a ferromagnet there is a macroscopically observable magnetic moment. Time reversal inverts that.

One approach to systematically investigate the possible arrangements of magnetic moments is the classification into 1651 Shubnikov groups (black-and-white space groups) that are an extension of the 230 crystallographic space groups. Here one moment direction is represented by the color white, and the opposite by black. Time reversal exchanges black and white. Depending on the moment direction, this may also happen for some "normal" space group operations, e.g. a 180-deg rotation about an axis that is perpendicular to the moment direction.
 

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