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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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% of Peak<br />

100<br />

80<br />

60<br />

40<br />

20<br />

NONIONIZING RADIATION SAFETY 757<br />

0<br />

200 400 600 800 1000<br />

0<br />

800 1000 1200 1400 1600 1800<br />

A Wavelength (nm)<br />

B<br />

Wavelength (nm)<br />

Figure 14-10. Calibration curve for a pho<strong>to</strong>electric detec<strong>to</strong>r. A. Silicon diode B. In GaAs detec<strong>to</strong>r.<br />

(Courtesy of Coherent, Inc, Santa Clara, CA.)<br />

and peak power. Like most quantum electronic devices, pho<strong>to</strong>electric detec<strong>to</strong>rs are<br />

highly energy-dependent and each instrument must be calibrated. A typical calibration<br />

curve, as supplied by the manufacturer, is shown in Figure 14-10.<br />

W Example 14.16<br />

The output from a 60-Hz pulsed ruby laser, λ = 694.3 nm, is measured with a<br />

pho<strong>to</strong>diode-type meter. With the aid of an oscilloscope, we find rectangular pulses<br />

as shown below:<br />

The meter reading, which is proportional <strong>to</strong> the average power, is 35 μA. Calculate<br />

the<br />

% of Peak<br />

100<br />

(a) duty cycle (fraction of time that lasing actions occurs),<br />

(b) average power, P , μW,<br />

(c) peak power, P0, μW, and<br />

(d) energy per pulse, J.<br />

80<br />

60<br />

40<br />

20

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