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Nanotechnology-Enabled Sensors

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3.5 Solid State Transducers 107<br />

When p-type and n-type semiconductors are placed next to each other to<br />

form a p-n junction, the majority carries in the p-type material (holes) diffuse<br />

a certain distance into the n-type material, and similarly at the n-type<br />

material, majority carries (electrons) diffuse into the p-type material. Once<br />

this diffusion is balanced, a depletion region forms (Fig. 3.29). A potential<br />

barrier then exists between the p- and n-doped materials, which must be<br />

exceeded for the current to conduct. Devices having one p-n junction are<br />

termed diodes, whilst those contained two, in the form of p-n-p or p-n-p<br />

junctions, are referred to as BJTs. BJT’s have the added advantage of internal<br />

current amplification as well.<br />

Fig. 3.29 A Schematic reorientation of a p-n junction.<br />

From the Shockley equation, the current flowing is given by: 20<br />

qV / nkT<br />

saturation e<br />

( ) = ( −1)<br />

I V I , (3.76)<br />

where q is the electron charge, V is the voltage, n is the ideality factor, k is<br />

Boltzmann’s constant, T is the temperature in Kelvin, and Isaturation is the<br />

saturation current of the device..<br />

Devices such as diodes and BJTs are commonly employed for monitoring<br />

charge 21 and widely used in sensing electromagnetic irradiation. The<br />

application of these devices in monitoring irradiation has already been described<br />

in Chap. 2 in the section pertaining to photoconductive and photovoltaic<br />

devices. They may also be employed, albeit less commonly, for<br />

chemical and pressure sensing applications.<br />

Diode and transistor based transducers are extensively used in irradiation<br />

spectroscopy, 22 which will be described in further detail in Chap. 5. In<br />

many such spectroscopic measurements, the amount of light to be monitored<br />

may be very low. Using a photodiode in conjunction with an amplifier<br />

may rectify such limitations. However, low irradiation intensity<br />

produces small currents which are inherently difficult to amplify externally,<br />

if electrical noise is to be avoided. In such situations, phototransistor<br />

may be used as an alternative to external signal amplification. A transistor

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