Kronig-Penney Model in Reciprocal Space

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SUMMARY

The discussion focuses on solving part (a) of Charles Kittel's Solid State Physics problem 7.3, which involves the Kronig-Penney model with a delta-function potential. The objective is to find the energy of the lowest energy band at k=0, given that P<<1. The attempts at a solution include setting (P/Ka)=0 and using Taylor expansions for the trigonometric functions, leading to the conclusion that P≈(1/2)(Ka)². The correct approach involves recognizing that at k=0, the relationship between P, sinc(Ka), and cos(Ka) must be carefully analyzed using Taylor expansions.

PREREQUISITES
  • Understanding of the Kronig-Penney model
  • Familiarity with delta-function potentials
  • Knowledge of Taylor series expansions
  • Basic concepts of solid state physics, particularly energy bands
NEXT STEPS
  • Study the implications of delta-function potentials in quantum mechanics
  • Learn about the derivation and applications of the Kronig-Penney model
  • Explore Taylor series expansions in the context of physics problems
  • Investigate energy band structures in solid state physics
USEFUL FOR

Students and researchers in solid state physics, particularly those studying quantum mechanics and energy band theory. This discussion is beneficial for anyone tackling problems related to the Kronig-Penney model and delta-function potentials.

irishhockey
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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=\hbar2K2/(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=\hbar2(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.
 
Last edited:
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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).
 

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