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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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9<br />

Substituting this in Schrödinger’s equation we get,<br />

() r u () r e<br />

ikr<br />

(1.5)<br />

k<br />

k<br />

2 2 2<br />

p ( k. p)<br />

k <br />

V u<br />

E u<br />

2m m 2m<br />

<br />

nk nk nk<br />

(1.6)<br />

At regions close to the zone center we can write the energies using parabolic approximation<br />

as follows<br />

E<br />

nk<br />

2 2<br />

k<br />

En0<br />

(1.7)<br />

2<br />

m <br />

Effective mass can be written as<br />

1 1 2 | un | k. p| un<br />

|<br />

<br />

<br />

m m m k E E<br />

2<br />

0 0<br />

2 2 (1.8)<br />

nn n0 <br />

n0<br />

It is clear from the above relationship that the effective mass is a combined effect of mass<br />

and potentials experienced by the electron. Effective mass is tensor due to different<br />

dispersions along different symmetry axes.<br />

E<br />

2<br />

1 1<br />

ko<br />

<br />

2<br />

ij<br />

kikj<br />

m<br />

<br />

(1.9)<br />

1.2.3 Effect of 3-Dimensional Confinement on Electronic<br />

Structure<br />

From the previous sections of this chapter it was assumed that wave function is only<br />

dependent on the periodicity and the potentials experienced by charge carriers. Therefore it is<br />

necessary to ask, how does dimensionality influence wave function?

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