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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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12<br />

correction factor in small nanocrystal. This interacting electron hole pair is now called an<br />

exciton. When a semiconductor radius decreases from infinite to confined solid where mean<br />

free path is close to radius, coulomb interaction has a significant role to play. Theoretically<br />

this interplay between confinement energy and coulomb interaction leads to three different<br />

confinement regimes. Before going into effects of degree of confinement we define the mean<br />

free path of the exciton ( a<br />

B<br />

, also called Bohr Radius of the exciton) as<br />

a B<br />

2<br />

<br />

(1.17)<br />

2<br />

e<br />

Based on a B<br />

and attractive coulomb interaction we can define three kinds of weak (r> a B<br />

),<br />

intermediate confinement (r~ a B<br />

) and strong confinement (r< a B<br />

) [1.16]<br />

Weak Confinement Regime: In this regime confinement energy is less than coulomb<br />

interaction or Exciton binding energy. The band gap in this case can be given as<br />

2 2<br />

<br />

EQD EB Ec<br />

<br />

2( m m ) a<br />

e<br />

h<br />

2<br />

(1.18)<br />

Intermediate Confinement Regime: In this size regime confinement will be set in the<br />

carrier with smaller effective mass. Very often electrons have a low<br />

er effective mass; therefore in such a size regime electron levels will exhibit discreteness<br />

while the hole levels will be continuous. Therefore the system may be approximated as a<br />

donor type exciton with electron governing quantization behavior.<br />

Strong Confinement Regime: In this size regime, exciton as a whole experiences<br />

confinement leading to quantization of exciton levels.

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