What are the properties of reciprocal lattice vectors?

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SUMMARY

The reciprocal lattice vector represents the change in wavevector of radiation incident upon a real lattice, specifically correlating to allowed k-values for waves that can be Bragg-diffracted. Reciprocal vectors are defined as perpendicular to two of the three lattice vectors, with a length inversely proportional to the third vector's length. The first Brillouin zone (1BZ) contains these allowed k-values, establishing a direct relationship between reciprocal space and the physical properties of the lattice. Understanding this concept is crucial for interpreting diffraction patterns and wave interactions in crystallography.

PREREQUISITES
  • Understanding of reciprocal lattice and its geometric properties
  • Familiarity with Bragg's law and diffraction principles
  • Knowledge of Miller indices and their relation to crystal planes
  • Basic concepts of vector spaces and dual spaces in physics
NEXT STEPS
  • Study the mathematical formulation of reciprocal lattice vectors in crystallography
  • Learn about the Brillouin zone and its significance in solid-state physics
  • Explore the relationship between reciprocal space and diffraction patterns
  • Investigate the physical implications of wave-vector changes in materials science
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Students and researchers in physics, materials science, and crystallography who seek to deepen their understanding of reciprocal lattice vectors and their applications in wave diffraction and solid-state phenomena.

malawi_glenn
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Homework Statement



"What does a reciprocal lattice vector represent in the real lattice?"


The Attempt at a Solution



The answer to that one is that the reciprocal lattice represent all possible k-values for the incoming radiation to be contained in the real lattice. Hence a reciprocal vector represent one of these possible k-values.

Am I right?
 
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Here are some discussion of the reciprocal lattice and vectors.

http://www.matter.org.uk/diffraction/geometry/lattice_vectors.htm

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

http://www.chembio.uoguelph.ca/educmat/chm729/recip/6reci.htm

http://ocw.mit.edu/NR/rdonlyres/Earth--Atmospheric--and-Planetary-Sciences/12-108Fall-2004/7160155B-B411-4346-ADF3-C89439D43852/0/lec8.pdf

See pages 6,7 in the last one.

Reciprocal vectors are defined to be perpendicular to two of the three lattice
vectors and with length equal to 1/length of the third vector.

Linear combinations formed from these reciprocal vectors and the
Miller indices are vectors that are in the same direction as the poles to
the corresponding planes. The vector length of this vector is the
reciprocal of the plane spacing.
 
Last edited by a moderator:
If you're familiar with vector spaces and their duals, let \mathbf{e}_\mu be the basis vectors for V, and \mathbf{\theta}^\mu be the (co-)basis for V*, such that \mathbf{e}_\mu \mathbf{\theta}^\nu = \delta_\mu^\nu. Let there be a metric, g_{\mu\nu}. The reciprocal vectors are basis covectors \mathbf{\theta}^\mu turned into vectors by the inverse metric.
 
Thanx, I already checked them out. And also I have two good books.

The things is that the last one, p 6,7 has the Crystallographical definition of reciprocal space; Hence the connection between planes, distance of planes and points in reciprocal space. But the definition in my course is the physics one: i.e you have multiplied with 2pi.

So I wonder if the points in reciprocal space represent allowed k-values for waves that can be Bragg-difracted in the real-lattice. And if the reciprocal lattice vector represent a certain k-value.
 
genneth said:
If you're familiar with vector spaces and their duals, let \mathbf{e}_\mu be the basis vectors for V, and \mathbf{\theta}^\mu be the (co-)basis for V*, such that \mathbf{e}_\mu \mathbf{\theta}^\nu = \delta_\mu^\nu. Let there be a metric, g_{\mu\nu}. The reciprocal vectors are basis covectors \mathbf{\theta}^\mu turned into vectors by the inverse metric.

Thanx , but not what I looked for ;)
 
malawi_glenn said:
Thanx , but not what I looked for ;)

I know it sounds a bit esoteric, but it's really just geometry. I certainly didn't understand reciprocal lattice vectors until I made that connection -- but maybe I'm just a mathmo trying to pretend to be a physicist ;-)
 
genneth said:
I know it sounds a bit esoteric, but it's really just geometry. I certainly didn't understand reciprocal lattice vectors until I made that connection -- but maybe I'm just a mathmo trying to pretend to be a physicist ;-)

The geometrical connetion I am fine with, but I am after the physical intepretation of the reciprocal lattice vector.

I know that the answer to this: "So I wonder if the points in reciprocal space represent allowed k-values for waves that can be Bragg-difracted in the real-lattice. And if the reciprocal lattice vector represent a certain k-value."

Is that the allowed k-vales are contained in the 1BZ, so I now wonder what points in reciporcal lattice space and reciprocal lattice vectors represents. If there are any physical inteprenation of those, or just geometrical.
 
malawi_glenn said:
The geometrical connetion I am fine with, but I am after the physical intepretation of the reciprocal lattice vector.

I know that the answer to this: "So I wonder if the points in reciprocal space represent allowed k-values for waves that can be Bragg-difracted in the real-lattice. And if the reciprocal lattice vector represent a certain k-value."

Is that the allowed k-vales are contained in the 1BZ, so I now wonder what points in reciporcal lattice space and reciprocal lattice vectors represents. If there are any physical inteprenation of those, or just geometrical.

If we know that reciprocal vectors are just covectors turned into vectors, then they can represent anything from the covector space. As you've noted, the wave-vector is one such thing, as is momentum (same thing as wave-vector really).
 
malawi_glenn said:

Homework Statement



"What does a reciprocal lattice vector represent in the real lattice?"

Think about the change in wavevector of radiation incident upon a lattice.
 
  • #10
Kurdt said:
Think about the change in wavevector of incident radiation upon a lattice.

You are talking about Bragg condition right?
 
  • #11
malawi_glenn said:
You are talking about Bragg condition right?

I am indeed. Now to help you a little more, consider a 1D lattice with an incident wavevector k and a reflected wavevector k'. Take the difference of the wavevectors and see if they look familiar.
 
  • #12
Kurdt said:
I am indeed. Now to help you a little more, consider a 1D lattice with an incident wavevector k and a reflected wavevector k'. Take the difference of the wavevectors and see if they look familiar.

I know that delta k is equal to reciprocal lattice vector.


I could write an essay about reciprocal space, diffraction and so on, but I still don't know what to answer to the original question.. =(
 
  • #13
If delta k is equal to the reciprocal lattice vector then I would think you would have your answer. The reciprocal lattice of the periodic system is equal to the change in wavevector of the radiation. Or in other words it represents the change in wavevector of the radiation.
 
  • #14
okay, I go with that answer =) thanx
 
  • #15
It is a bit of a vague question but to me I couldn't imagine what else it would be. If its for a homework assignment you could always approach the tutor and ask if that's what they are looking for before the deadline and I'm sure they will be helpful.
 
  • #16
yes, we have many of those questions. Hate this course=P

Will ask the guy tomorrow. Thanx
 

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