Topological classification of defects

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SUMMARY

The discussion focuses on the topological classification of defects in ordered media, specifically addressing the characterization of 2D defects such as domain walls in crystal lattices. Participants clarify that defects can be classified into three dimensions: 0D (vacancies, interstitials), 1D (dislocations), and 2D (grain/phase boundaries). The classification relies on the fundamental group of the order parameter space, which is essential for understanding the topology of defects. A key reference mentioned is Mermin's review, which provides foundational insights into this classification scheme.

PREREQUISITES
  • Understanding of algebraic topology as it relates to order parameter spaces
  • Familiarity with crystal lattice structures and defect types
  • Knowledge of 0D, 1D, and 2D defect classifications
  • Basic comprehension of the concept of fundamental groups in topology
NEXT STEPS
  • Research Mermin's review on topological defects in ordered media
  • Explore the algebraic topology of order parameter spaces
  • Investigate the classification of 2D defects in various ordered structures
  • Study the implications of grain and phase boundaries in solid crystals
USEFUL FOR

Researchers, physicists, and materials scientists interested in the topological aspects of defects in ordered media, particularly those studying crystal lattices and their properties.

ayan849
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Please help somebody on this problem...

When we topologically classify the defects in ordered media, we consider the character of the fundamental group of the associated order parameter space. To construct those groups, we circumscribe the line defects by circles and the point defects by spheres.
My question is what is done for a surface (possibly infinite) defect, say domain walls. My query primary concerns crystal lattices. I want to characterize the essential defects in solid crystals--for dislocation and interstitial/vacancy, it is straightforward. But what to be done in case of grain/phase boundary?
 
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ayan849 said:
When we topologically classify the defects in ordered media, we consider the character of the fundamental group of the associated order parameter space.
That is the most sciency statement I've ever heard in connection to defects. But seriously: What exactly are you trying to do? I always was of the impression that the classification goes like this:

0D defects: vacancies, interstitial. 0D since there is sizable spatial extend in zero directions.

1D: dislocations and so on. Basically given by a line--spatial extend only in one direction (from local topologic perspective, of course the actual dislocation lines can have complex 3D shapes)

2D: grain/phase boundaries and so on. Spatial extend in two directions (locally, idealized).

Of course, in practice grain and phase boundaries are not sharp. For example, a grain bounday will usually consist of at least 10-100 atomic layers; however, in relation to the spatial extension of the other two dimensions (which usually would me measured in µm to mm, and not nm), they can still be considered as essentially flat.

So are you looking for some hard mathematical definition of the defect dimension? I think that "circle around a dislocation" argument is just intended as a tool for the definition; if you just accept that a point is a 0-dimensional obeject, a line is a 1-dimensional object, and a sheet is a 2-dimensional object, you don't need such definitions.
 
@ cgk
I think you are not aware of the topological classification of defects in ordered media. An ordered media is the generalization of crystalline materials. It can include liquid crystals to superfluids, ferromagnets and so on. There is a general classification scheme of defects occurring in those ordered structures, which revolves around algebraic topology of the order parameter space of that media. I want to know how 2D defects are classified in that scheme, because there are ample works done on 1D and 0D defects.
 
How to understand the "domain walls"
 
@ayan849
The most popular reference for this topic is Mermin's review http://rmp.aps.org/abstract/RMP/v51/i3/p591_1" . Sorry I cannot provide you with a direct answer, Its some time ago I studied these topics.
 
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I think you need to look for how many disconnected pieces there are in the order parameter space.
 

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