As noted in Fig.1.5, the frequencies of optical waves run from 1× 1012 to
3 × 1016 Hz, which corresponds to maximum and minimum wavelengths of
300 μm and 10 nm, respectively, in the optical spectrum.
The waveform also can be expressed by the following complex function
U(r;t)¼A(rÞexpfi½xtþuð Þg ¼r UðÞr expðixtÞð 2 : 2 Þ
where the time-independent factor UðÞ¼r AðÞr exp½iuðrÞis the complex ampli-
tude of the wave. The waveform u(r, t) is found by taking the real part of U(r,t)
uðÞ¼r;t Re UfgðÞr;t ¼
1
2
½ðUðÞþr;t U*ðÞr;t 2 : 3 Þ
where the symbol * denotes the complex conjugate.
Theoptical intensityI(r, t), which is defined as the optical power per unit area
(for example, in units such as W/cm^2 or mW/mm^2 ), is equal to the average of the
squared wavefunction. That is, by letting the operation xhidenote the average of a
generic function x, then
IðÞ¼r;t U^2 ðÞr;t
¼jUðÞjr^2 hi 1 þcosð 2 ½ 2 pmtþuð ÞÞr ð 2 : 4 Þ
When this average is taken over a time longer than the optical wave period T, the
average of the cosine function goes to zero so that the optical intensity of a
monochromatic wave becomes
IðÞ¼jr UðÞjr^2 ð 2 : 5 Þ
Thus the intensity of a monochromatic wave is independent of time and is the
square of the absolute value of its complex amplitude.
Example 2.1Consider a spherical wave given by
UrðÞ¼
A 0
r
expði2pr=kÞ
where A 0 = 1.5 W1/2is a constant and r is measured in cm. What is the
intensity of this wave?
Solution: From Eq. (2.5),
IðÞ¼jr UðÞjr^2 ¼ðÞA 0 =r^2 ¼ 1 :5W^1 =^2
=rincmðÞ
hi 2
¼ 2 :25 W=cm^2
28 2 Basic Principles of Light