Scattering of Neutrons from 2d Crystal Lattice

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Homework Help Overview

The discussion revolves around the scattering of neutrons from a two-dimensional rectangular crystal lattice. The original poster examines whether specific reflections (11), (20), and (02) can be observed using the Laue condition for diffraction or Bragg's Law, given the dimensions of the unit cell and the wavelength of the neutrons.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to apply both the Laue conditions and Bragg's Law to determine the allowed reflections, expressing uncertainty about their conclusions.
  • Some participants question the application of the Laue condition and suggest exploring the relationship between the wave vectors involved in the scattering process.
  • Others discuss the implications of the maximum wavelength for reflections and how it relates to the orientation of the crystal lattice.

Discussion Status

Participants are actively engaging with the problem, offering hints and clarifications regarding the application of the Laue condition and Bragg's Law. There is a productive exchange of ideas, with some participants confirming the original poster's reasoning while others raise additional questions about the generality of the conclusions drawn.

Contextual Notes

There is an ongoing exploration of the assumptions regarding the wavelength of the incoming neutrons and the conditions under which reflections can occur. The original poster expresses confusion about the validity of their approach, indicating a need for further clarification on the principles involved.

1Kris
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Homework Statement



A two-dimensional rectangular crystal has a unit cell with sides a 6.28Å and
b 3.14Å. A beam of monochromatic neutrons of wavelength 5.0 Å is used to
examine the crystal.

Using either the Laue condition for diffraction or Bragg's Law, determine
whether it would be possible to observe the following reflections: (11), (20)
and (02).

Homework Equations



Laue conditions: K\cdota=2πh
K\cdotb=2πk
K\cdotc=2πl

for wavevector K, lattice vectors a,b,c and integers h,k,l.

Bragg's law: 2dsinθ=nλ

for lattice plane spacing d, Bragg angle θ, scattering order n and wavelength λ.

The Attempt at a Solution



Reciprocal space lattice is rectangular with lengths a* = 2π/a, b*=2π/b. Incoming wavevector k has magnitude 2π/5 = 1.26Å-1.

Laue conditions:
Direction (11) → K=a*+b*
K\cdota=a*\cdota=2π
K\cdotb=b*\cdotb=2π

both are integer multiples of 2π and so (11) reflections are allowed.

Direction (20) → K=2a*
K\cdota=4π
K\cdotb=0

allowed again for same reasons.

Direction (02) → K=2b*
K\cdota=0
K\cdotb=4π

allowed.

Bragg's law:

(11) → d = ((h/a)2+(k/b)2)-1/2
= ((1/6.28)2+(1/3.14)2)-1/2
≈ 2π/√5 (assuming a = 2π and b = π)

(11) reflection has highest common factor 1 so it is an n=1 reflection:
Bragg's law gives

1*5=2*(2π/√5)sinθ

rearrangement gives sinθ = 0.88970... which is certainly an allowed value for sinθ so I conclude that it is an allowed reflection.

(20) is an n=2 reflection, d = a/h = a/2 ≈ π
Bragg's law gives sinθ = 5/π > 1 which is not valid so the reflection cannot happen.

(02) is also n=2, d = b/k ≈ π/2
Bragg's law gives sinθ=3.18 and so it is not an allowed reflection.

I'm not too confident in the way I've gone about solving this problem by either method and the contradictory conclusions definitely show that at least one of them is wrong. Could anyone give some hints as to where I'm going wrong? Thanks!
 
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If k is the wave-vector of the incoming wave and k’ for the diffracted wave, then the Laue condition is that k’- k = K where K is a reciprocal lattice vector.

The dot product of a reciprocal lattice vector K with a direct lattice vector (a or b) will always yield an integer multiple of 2##\pi##. So, all you did was verify that fact for the particular reciprocal lattice vectors corresponding to (1,1), (2, 0) and (0,2).

Since |k| = |k’|, see if you can use the condition k’- k = K to find the minimum possible value of |k| for a given |K|. That will tell you the maximum wavelength that the incident waves can have and still satisfy the Laue condition.
 
Thanks for the reply.

The vectors k, k' and K make a triangle because of the vector addition relating them. To minimise k, surely the triangle would be flattened such that k and k' run parallel to K.

This gives k=k'=K/2.
and we know
λ=2\pi/k

(11): K=((\frac{2\pi}{a})2+(\frac{2\pi}{b})2)\frac{1}{2}
= \sqrt{5}Å-1

corresponding to a maximum λ of 4\pi/\sqrt{5}Å

Similarly I get

(20): λ = 2\piÅ (maximum)
(02): λ = \piÅ (maximum)

As it is given that the incoming beam has wavelength 5Å then (11), (20) are allowed and (02) is excluded.

Is this reasoning correct? Is it generally true that all wavelengths below a maximum are reflected by a crystal?
 
1Kris said:
As it is given that the incoming beam has wavelength 5Å then (11), (20) are allowed and (02) is excluded. Is this reasoning correct?
Yes, that all looks right to me.

Is it generally true that all wavelengths below a maximum are reflected by a crystal?

If λ is below the maximum for a set of lattice planes, then you will get reflection if the crystal is oriented such that the lattice planes make the proper angle with respect to the direction of the the incident wavevector. If you change λ then you would need to adjust the orientation. If you use a powder of little crystals oriented in all directions, then there will always be some crystals oriented to give reflection as long as λ is below the maximum.
 
Thanks very much. You've pulled me out of that horrible mess of confusion! I had briefly thought of the condition you gave but I dismissed them before I figured out the consequences because I didn't think it was either the Laue condition or Bragg's law. Thanks again.
 

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