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Tellurite And Fluorotellurite Glasses For Active And Passive

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6. Optical properties; MDO 178<br />

energy of transitions from the ground state (υ = 0), to higher levels is given by equation<br />

(6.17) [2].<br />

∆E = E − E = ω υ − ω x υ(<br />

υ + 1)<br />

(6.17)<br />

υ 0 e e e<br />

The transition between levels υ = 0 to υ = 1 for a molecule is known as the fundamental<br />

transition, and is seen on vibrational spectra as the fundamental frequency. Higher<br />

transitions, which are approximate multiples of the fundamental frequency, are known as<br />

the first overtone (υ = 0 to υ = 2), second overtone (υ = 0 to υ = 3) etc. [2].<br />

The harmonic model predicts equally spaced overtones, when in fact this spacing<br />

decreases slightly with increasing energy level [2]. The disassociation energy of the<br />

molecule, e D , is not equal to E d , but shown by equation (6.18) [2].<br />

1 1<br />

De = Ed<br />

− E0<br />

= Ed<br />

− ωe<br />

+ ωe<br />

xe<br />

(6.18)<br />

2 4<br />

ω e is related to ke, the anharmonic force constant and is a better representation of bond<br />

strength than k obtained from the harmonic model [2].<br />

Selection rules<br />

The general selection rule for infrared vibration of a molecule is that the dipole of the<br />

molecule must change with the atomic displacement. This process can occur as the

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