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Introduction to Nanotechnology

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1 meV<br />

10 meV<br />

100 meV<br />

FJ<br />

E<br />

W<br />

1 eV<br />

10 eV<br />

Positronium<br />

Hydrogen<br />

n=5<br />

n=5 - n=4<br />

n=4 - n=3<br />

n=3<br />

n=2<br />

n=2<br />

n=l<br />

n=l<br />

2.3. LOCALIZED PARTICLES 33<br />

n=4<br />

n=3<br />

n=2<br />

n=l<br />

Exci<strong>to</strong>n<br />

Figure 2.20. First few energy levels in the Rydberg series of a hydrogen a<strong>to</strong>m (left), positronium<br />

(center), and a typical exci<strong>to</strong>n (right).<br />

Table B.ll that the relative dielectric constant &/EO has the range of values<br />

7.2 < &/eO < 17.7 for these materials, where c0 is the dielectric constant of free<br />

space. Both of these fac<strong>to</strong>rs have the effect of decreasing the exci<strong>to</strong>n energy E,, from<br />

that of positronium, and as a result this energy is given by<br />

1 3.6m*/mo<br />

E,, = - m*/mo e’ - eV<br />

(&/Eo)’ 4n&oaon2 - (&/&o)’n’<br />

(2.18)<br />

as shown plotted in Fig. 2.20. These same two fac<strong>to</strong>rs also increase the effective<br />

Bohr radius of the electron orbit, and it becomes<br />

(2.19)

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