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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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2. Literature review; MDO 44<br />

originates from charge separation, or orientation, however, experimental evidence<br />

indicates the former [45].<br />

Electric field poling of glasses at elevated temperatures has induced non-zero χ2 in a<br />

number of systems such as silicates and tellurites. Similar effects have been observed<br />

using corona poling, electron bombardment, and UV laser exposure. This is though to be<br />

due to space charge left behind after mobile species, such as alkali or hydrogen ions, have<br />

moved out of the poled region [45].<br />

If the incident beam is non-resonant, i.e. detuned from any fundamental frequency of<br />

components in the glass, third-order non-linear effects will dominate. Equation (2.12)<br />

shows the relation between the non-linear refractive index, n2, to the real part of χ3 [45].<br />

12π<br />

n 2 = Re χ 3 ( 1111)(<br />

−ϖ<br />

, ϖ , ϖ , −ϖ<br />

)<br />

(2.12)<br />

n<br />

where n is the linear refractive index. This phenomena results in intensity dependent self-<br />

focusing. These non-linearities are electronic in origin, and due to fluctuations in electron<br />

cloud density, with sub-ps (10 -12 s) response times [45]. The non-linear refractive index<br />

can be approximated by equation (2.13).<br />

n<br />

2<br />

2 ⎛ n + 2 ⎞ 2 2<br />

⎜ ( n −1)<br />

d n<br />

3 ⎟<br />

=<br />

⎝ ⎠<br />

(2.13)<br />

nE<br />

2<br />

s

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