Bravais lattices and lattices with a basis

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Discussion Overview

The discussion revolves around the concepts of Bravais lattices and lattices with a basis, exploring their definitions, relationships, and implications in the context of crystal structures. Participants examine whether a lattice with a basis can still possess primitive vectors and how these concepts interact in the characterization of crystals.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that a Bravais lattice is defined by the ability to reach each lattice point using integer combinations of primitive vectors, while a lattice with a basis complicates this definition.
  • Others argue that a non-Bravais lattice can be viewed as a Bravais lattice with a basis at the lattice points, suggesting that it can still have primitive vectors, as illustrated by examples like CuO2 planes in cuprate superconductors.
  • One participant asserts that primitive vectors refer specifically to the lattice and are independent of the presence of a basis.
  • Another participant clarifies that an ideal crystal consists of both a basis and a lattice, emphasizing that the lattice is merely a vector space of defined vectors and that the complete crystal structure includes the basis.
  • A later reply questions whether it is always possible to decompose a crystal into its basis and an underlying Bravais lattice, suggesting that periodicity is a necessary condition for this decomposition.
  • It is noted that all Bravais lattices have three basis vectors in three dimensions, and while some may involve centering translations for convenience, they are fundamentally primitive in the context of electron scattering.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between Bravais lattices and lattices with a basis, with no consensus reached on whether a crystal can always be decomposed into these components. The discussion remains unresolved regarding the implications of these definitions and their applications.

Contextual Notes

Participants highlight the potential confusion between the definitions of lattice and basis, and the implications of periodicity in crystal structures. There are also mentions of specific examples and conditions that may affect the understanding of these concepts.

Niles
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Hi guys

Ok, so one way to define a Bravais lattice is to say that each lattice point can be reached by R = la1+ma2+na3 for some integer m, l and n. Obviously, this cannot be the case when we have a lattice with a basis.

But does that also mean that a lattice with a basis does not have primitive vectors?
 
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A non-Bravais lattice can be viewed as some Bravais lattice with the basis sitting at the lattice points, and so it will have primitive vectors, as long as we realize our lattice points are now a collection of atoms.

For example, think of the CuO2 planes in a cuprate superconductor. We can think of a basis consisting of a copper atom with two neighbouring oxygen atoms. We can think of the primitive vectors of this lattice as those of the square lattice. A picture would explain this far more clearly, but unfortunately I don't have one to hand.
 
A lattice is a lattice and a basis is a basis. The primitive vectors refer to the lattice and are independent of whether one considers a basis or not.
 
I was quite in a hurry when I wrote the last message.
So what I wanted to say is that an ideal crystal can be thought off to be composed of a basis and a lattice, the lattice being just the collection of all vectors R you defined. So in mathematical terminology, the lattice is just a vector space (of the vectors R). Physicist often mingle this up by meaning with lattice the complete crystal structure including the basis. A crystal is never only a lattice. Even if the basis contains only one atom, the electron density within the basis is not constant and you need both the position inside the basis and a lattice vector to uniquely specify a point of the crystal.
 
DrDu said:
I was quite in a hurry when I wrote the last message.
So what I wanted to say is that an ideal crystal can be thought off to be composed of a basis and a lattice, the lattice being just the collection of all vectors R you defined. So in mathematical terminology, the lattice is just a vector space (of the vectors R). Physicist often mingle this up by meaning with lattice the complete crystal structure including the basis. A crystal is never only a lattice. Even if the basis contains only one atom, the electron density within the basis is not constant and you need both the position inside the basis and a lattice vector to uniquely specify a point of the crystal.

I see, thanks. But can I always "decompose" a crystal into its basis and the underlying lattice, which is always Bravais?Niles
 
Niles said:
I see, thanks. But can I always "decompose" a crystal into its basis and the underlying lattice, which is always Bravais?


Niles

Any bravias lattice has 3 basis vectors in 3D. There are some Bravias lattices with centering translations, for instance bcc (Im3m), but this is done for convenience to have more right angles and so on. Real Bravias lattice on which electrons are scattered are _always_ primitive. Simply if you choose a bigger direct space unit cell you get a smaller reciprocal cell, but some nodes will be extinct.
 
Niles said:
But can I always "decompose" a crystal into its basis and the underlying lattice, which is always Bravais?

Yes, as long as there is periodicity, which is implied by "crystal" (as opposed to amorphous).
 

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