In bcc lattice why XRD 100 peak is not observed ?

In summary, the absence of the XRD 100 peak in BCC lattice can be explained by the destructive interference between the planes passing through the base atoms and the planes defined by the atoms on the edge of the cell. This is due to the equal scattering power of these planes, resulting in a phase difference of pi and cancelling out their contribution. The diffraction pattern for the BCC lattice does not contain planes with odd integer values for h+k+l, but does show reflections from planes with even integer values. The presence of an intervening plane with equal composition also contributes to the cancellation of the (100) reflection.
  • #1
hkazmi25
1
0
Can someone tell me that in bcc lattice why xrd 100 peak does not appear?
 
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  • #2
The planes passing through the base atoms are a/2 away from the planes passing through the planes defined by the atoms on the edge of the cell. And is only a shifted copy of the latter. Hence it will reflect x rays exactly as does one of the edge planes and you get destructive interference.
 
  • #3
If you calculate the structure factor of the BCC lattice using:
$$S(hkl)=f{1+exp[-i\pi(h+k+l)]}$$, where f= form factor. The value o f S is zero when the exponential has the value -1, which is whenever the argument is: -i*pi* (odd integer).
So we have:
S=0 when h+k+l= odd integer
S=2f when h+k+l= even integer
So therefore the diffraction pattern does not contain these planes: (100), (300), (111), (221)
But it occurs for fx.: (200), (110), (222)

The (100) reflection occurs when reflections from the planes that bound the cubic cell differ in phase by 2*pi. In BCC there is an intervening plane of atoms, which is equal to in scattering power to the other planes. Situated between them it gives a reflection retarded in phase by pi w.r.t. the first plane, thereby cancelling the contribution from that plane. So the cancellation occurs since the planes are identical in composition.
 

1. Why is the XRD 100 peak not observed in a bcc lattice?

The XRD 100 peak is not observed in a bcc (body-centered cubic) lattice because the atoms in a bcc structure are arranged in a way that causes the X-rays to diffract in such a way that the intensity of the 100 peak is very low, making it difficult to detect.

2. Can the XRD 100 peak be observed in other types of lattices?

Yes, the XRD 100 peak can be observed in other types of lattices such as fcc (face-centered cubic) and hcp (hexagonal close-packed) structures. These lattices have a different arrangement of atoms which causes the X-rays to diffract in a way that the 100 peak is more prominent.

3. Are there any other factors that can affect the intensity of the XRD 100 peak?

Yes, the intensity of the XRD 100 peak can also be affected by the size of the unit cell, the presence of impurities or defects in the lattice, and the orientation of the crystal with respect to the X-ray beam.

4. Is there a way to enhance the intensity of the XRD 100 peak in a bcc lattice?

Yes, there are several techniques that can be used to enhance the intensity of the XRD 100 peak in a bcc lattice. These include using high-energy X-rays, increasing the thickness of the sample, and using a glancing angle of incidence for the X-rays.

5. Why is the XRD 100 peak important in materials science?

The XRD 100 peak is important in materials science because it provides valuable information about the crystal structure of a material. By analyzing the intensity and position of this peak, scientists can determine the type of lattice present and the arrangement of atoms in a crystal, which is crucial for understanding the physical and mechanical properties of materials.

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