03.01.2015 Views

handbook of modern sensors

handbook of modern sensors

handbook of modern sensors

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

422 14 Light Detectors<br />

<strong>of</strong> generated carriers per second per unit <strong>of</strong> volume. For a CdS cell, µ n τ n ≫ µ p τ p ;<br />

hence, conductance by free holes can be ignored. Then, the sensor becomes an n-type<br />

semiconductor. Thus,<br />

σ = ef µ n τ n . (14.18)<br />

We can define the sensitivity b <strong>of</strong> the photoresistor through a number <strong>of</strong> electrons<br />

generated by one photon (until the carrier life span ends):<br />

b = τ n<br />

t t<br />

, (14.19)<br />

where t t = l 2 /Vµ n is the transit time for the electron between the sensor’s electrodes,<br />

l is the distance between the electrodes, and V is the applied voltage. Then, we arrive<br />

at<br />

b = µ n τ nV<br />

l 2 . (14.20)<br />

For example, if µ n = 300 cm 2 /V s, τ n = 10 −3 s, l = 0.2 mm, and V = 1.2 V, then<br />

the sensitivity is 900, which means that a single photon releases 900 electrons for<br />

conduction, making a photoresistor work as a photomultiplier. Indeed, a photoresistor<br />

is a very sensitive device.<br />

It can be shown that for better sensitivity and lower cell resistance, the distance<br />

l between the electrodes should be reduced, and the width d <strong>of</strong> the sensor should<br />

be increased. This suggests that the sensor should be very short and very wide. For<br />

practical purposes, this is accomplished by fabricating a sensor in a serpentine shape<br />

(Fig. 14.14B) where the electrodes are connected to the leads.<br />

Depending on the manufacturing process, the photoresistive cells can be divided<br />

into the sintered type, single-crystal type, and evaporated type. Of these, the sintered<br />

type <strong>of</strong>fers high sensitivity and easier fabrication <strong>of</strong> large sensitive areas, which<br />

eventually translate into lower-cost devices. The fabrication <strong>of</strong> CdS cells consists <strong>of</strong><br />

the following steps.<br />

1. Highly pure CdS powder is mixed with appropriate impurities and a fusing agent.<br />

2. The mixture is dissolved in water.<br />

3. The solution in a form <strong>of</strong> paste is applied on the surface <strong>of</strong> a ceramic substrate<br />

and allowed to dry.<br />

4. The ceramic subassemblies are sintered in a high-temperature oven to form a<br />

multicrystal structure. At this stage, a photoconductive layer is formed.<br />

5. Electrode layers and leads (terminals) are attached.<br />

6. The sensor is packaged into a plastic or metal housing with or without a window.<br />

To tailor a spectral response <strong>of</strong> a photoresistor, the powder <strong>of</strong> step 1 can contain some<br />

variations; for instance, the addition <strong>of</strong> selenide or even the replacement <strong>of</strong> CdS for<br />

CdSe shifts the spectral response toward longer wavelengths (orange and red).<br />

To illustrate, how photoresistors can be used, Fig. 14.15 shows two circuits. Circuit<br />

A shows an automatic light switch which turns lights on when illumination drops (the<br />

turn-<strong>of</strong>f part <strong>of</strong> the circuit is not shown). Circuit B shows a beacon with a free-running<br />

multivibrator, which is enabled at darkness, when the resistance <strong>of</strong> a photoresistor<br />

becomes high.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!