Kronig-Penney Model in Reciprocal Space

In summary, for the delta-function potential and with P<<1, at k=0 the energy of the lowest energy band is ε=0. This can be found by expanding the trigonometric functions and using the fact that P<<1 and max(sinc(Ka))=1. This leads to 1-cos(Ka)<<1, which tells us that Ka is very small.
  • #1
irishhockey
14
0

Homework Statement


(a) For the delta-function potential and with P<<1, find at k=0 the energy of the lowest energy band.
(This is part A of Charles Kittel Solid State Physics problem 7.3)

Homework Equations



(P/Ka)sin(Ka)+cos(Ka)=cos(ka) (note, K and k are different variables)

ε=[itex]\hbar [/itex]2K2/(2m)

The Attempt at a Solution



I have tried two different things.

attempt 1)

simply say (P/Ka)=0

so we get

cos(Ka)=cos(0)=1

or K=arcos(1)/a

plugging into energy equation

ε=[itex]\hbar [/itex]2(arcos(1)/a)2/(2m)=0

which is obviously wrong

second attempt is to Taylor expand the trig functions, and assume the because P<<1, Ka<<1,
(in order to keep both left hand terms) and so (P/Ka)=1

after expanding and cancelling,

2cos(0)=1

which again stumps me

I'm not sure what to do. I have the sln manual, which says to expand the first equation, to find P≈(1/2)(Ka)2

Thank you for any help.
 
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  • #2
We have P*sinc(Ka)+cos(Ka)=cos(ka)=1 at k=0, where I have used sinc(x)=sin(x)/x. Then P*sinc(Ka)=1-cos(Ka). We know P<<1, and that max(sinc(Ka))=1. This tells us that LHS=P*sinc(Ka)<=P<<1. If LHS<<1, then RHS<<1. Therefore 1-cos(Ka)<<1. What does this tell us about Ka? Recall the Taylor Expansion for cos(x) and sinc(x).
 

FAQ: Kronig-Penney Model in Reciprocal Space

1. What is the Kronig-Penney Model in Reciprocal Space?

The Kronig-Penney Model in Reciprocal Space is a quantum mechanical model used to describe the behavior of electrons in a periodic lattice structure. It is a simplified version of the more complex Bloch wave model and is often used to understand the electronic band structure of materials.

2. How does the Kronig-Penney Model in Reciprocal Space differ from the Bloch wave model?

The Kronig-Penney Model in Reciprocal Space simplifies the Bloch wave model by assuming a one-dimensional periodic potential. This allows for a more straightforward analysis of the electronic band structure and makes it easier to understand the effects of lattice periodicity on electron behavior.

3. What are the assumptions made in the Kronig-Penney Model in Reciprocal Space?

The Kronig-Penney Model in Reciprocal Space assumes a one-dimensional periodic potential, identical potential barriers between lattice sites, and no interactions between electrons. It also assumes that the potential is infinite outside the lattice sites and zero inside the lattice sites.

4. How is the Kronig-Penney Model in Reciprocal Space used in materials science?

The Kronig-Penney Model in Reciprocal Space is used to understand the electronic band structure of materials, which plays a crucial role in determining their electrical, thermal, and optical properties. It can also be used to predict the behavior of electrons in different materials, which is essential for designing new materials with specific properties.

5. What are some limitations of the Kronig-Penney Model in Reciprocal Space?

The Kronig-Penney Model in Reciprocal Space is a simplified model and does not take into account many factors that can affect the behavior of electrons in real materials. These include electron-electron interactions, defects in the lattice structure, and the effects of temperature and pressure. Therefore, it should be used with caution and in conjunction with other models to fully understand the electronic properties of materials.

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