Topological question from Ashcroft-Mermin

In summary, the boundary condition for an electron confined to a one-dimensional metal can be replaced by a circle. This is analogous to the situation in two dimensions, where two opposite sides of a square are joined. However, in three dimensions this cannot be done and the analytic form of the boundary condition must be used.
  • #1
hagopbul
357
36
TL;DR Summary
about chapter 2
Hello :

doing some reading in physics and some of it is in solid state physics , in Ashcroft- mermin book chapter 2 page 33 you read

" Thus if our metal is one dimensional we would simply replace the line from 0 to L to which the electron were confined by a circle of circumference L. In three dimensions the geometrical embodiment of the boundary condition , in which three pairs of opposite faces on the cube are joint , becomes topologically impossible to construct in three dimensional space "

the above is not very clear to me could some one provide references to above paragraph or a short explanation

Best Regards
HB
 
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  • #2
I believe they are talking about "periodic" boundary conditions. In 1D it is easy to picture in real space as described. For 3D periodic boundary conditions no such real structure should be contemplated. The construct however still works and gives the correct density of states. Just don't try to picture it in your head, you will get agita.
 
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  • #3
It is like:
two pairs of opposite sides on the square are joint , becomes topologically impossible to construct in two dimensional space
because that is topologically a torus, which can be constructed in 3D but not 2D.
 
  • #4
could you prove it is tours ? it is 3cubes why tours not hexagon or other 3d object ?
 
  • #5
hagopbul said:
could you prove it is tours
No, I can't even prove the 2D case.
 
  • #6
hagopbul said:
Summary:: about chapter 2

" Thus if our metal is one dimensional we would simply replace the line from 0 to L to which the electron were confined by a circle of circumference L. In three dimensions the geometrical embodiment of the boundary condition , in which three pairs of opposite faces on the cube are joint , becomes topologically impossible to construct in three dimensional space. Nevertheless the analytic form of the boundary condition is easily generalized "
I have added the next line from Ashcroft and Mermin. Your question is not salient to the physics of Born-von Karman boundary conditions. Not to worry.
 
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  • #7
Joining opposite faces of a cube produces a 3-torus, a perfectly well defined topology. The limitation is simply that it cannot be represented (embedded) in 3-dimensional Euclidean space. However, it is easily embedded in a higher dimensional Euclidean space. This is similar to the situation of a Klein bottle. Trying to represent it 3-space requires self intersection, which is not feature of the actual Klein bottle (which can be embedded with no problems in 4-space).

Also, note that something as simple as 3-sphere cannot be embedded in Euclidean 3-space, so there is no problem here other than that our intuitions are guided by Euclidean 3-space.
 
Last edited:

1. What is topological order?

Topological order is a concept in condensed matter physics that describes the organization of matter in a system at the quantum level. It is characterized by the presence of long-range quantum entanglement and the absence of local order parameters.

2. How is topological order different from conventional order?

Unlike conventional order, which is characterized by local order parameters and can be destroyed by thermal fluctuations, topological order is robust and can persist even at high temperatures. It also exhibits properties such as fractionalization and topological degeneracy that are not seen in conventional order.

3. What is the role of topology in topological order?

Topology plays a crucial role in topological order as it describes the global properties of a system that cannot be changed by continuous deformations. In topological order, the topology of the system determines its ground state properties and the nature of its excitations.

4. How are topological insulators and topological superconductors related to topological order?

Topological insulators and topological superconductors are examples of systems that exhibit topological order. In these systems, the presence of a band gap and time-reversal symmetry protection lead to topologically non-trivial phases with unique surface states and edge modes.

5. What is the significance of the Ashcroft-Mermin topological question?

The Ashcroft-Mermin topological question is a thought experiment that highlights the importance of topology in understanding the properties of matter. It demonstrates that the topology of a system can dictate its behavior, even in the absence of any local order parameters. This has led to the development of new theoretical frameworks and the discovery of novel phases of matter.

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