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Tellurite And Fluorotellurite Glasses For Active And Passive

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6. Optical properties; MDO 167<br />

sample for near monochromatic radiation over a range of wavelengths. The energy, E, of<br />

the incident radiation is given by equation (6.1) [3].<br />

E = hf<br />

(6.1)<br />

where h = Planck’s constant = 6.62608×10 -34 J.s and f = frequency of the incident<br />

radiation. The wavelength, λ, of the radiation is given by equation (6.2) [3].<br />

c<br />

λ =<br />

(6.2)<br />

f<br />

where c = the speed of light in a vacuum = 2.99792458×10 8 m.s -1 . Spectroscopists often<br />

express the x-axis of spectra in wavenumbers, f ~ , which are usually measured in<br />

reciprocal centimetres (cm -1 ). This is convenient, as wavenumbers are directly<br />

proportional to energy. Equation (6.3) shows the relation between wavenumbers and<br />

equation (6.1) and (6.2) [3].<br />

~ f 1<br />

f = = =<br />

c λ<br />

E<br />

hc<br />

Fig. (6.1) shows the setup of a typical dual beam absorption spectrometer [3].<br />

(6.3)

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