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Introduction to Nanotechnology

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38 METHODS OF MEASURING PROPERTIES<br />

is related <strong>to</strong> the X-ray energy E expressed in the units kiloelectronvolts (keV)<br />

through the expression<br />

1.240<br />

/I=- nm<br />

E<br />

Ordinarily the beam is fixed in direction and the crystal is rotated through a broad<br />

range of angles <strong>to</strong> record the X-ray spectrum, which is also called a diffrac<strong>to</strong>meter<br />

recording or X-ray-diffraction scan. Each detected X-ray signal corresponds <strong>to</strong> a<br />

coherent reflection, called a Bragg reflection, from successive planes of the crystal<br />

for which Bragg's law is satisfied<br />

2d sin 6' = nll (3.2)<br />

as shown in Fig. 3.1, where d is the spacing between the planes, 6' is the angle that<br />

the X-ray beam makes with respect <strong>to</strong> the plane, ll is the wavelength of the X rays,<br />

and n = 1,2,3, . . . is an integer that usually has the value n = 1.<br />

Each crystallographic plane has three indices h,k,l, and for a cubic crystal they are<br />

ratios of the points at which the planes intercept the Cartesian coordinate axes x, y, z.<br />

The distance d between parallel crystallographic planes with indices hkZ for a simple<br />

cubic lattice of lattice constant a has the particularly simple form<br />

a<br />

d=<br />

(h2 + k2 + Z2)1/2<br />

a Ak=G<br />

d sin 0<br />

(3.3)<br />

Figure 3.1. Reflection of X-ray beam incident at the angle 0 off two parallel planes separated<br />

by the distance d. The difference in pathlength 2dsinO for the two planes is indicated.<br />

(From C. P. Poole Jr., The Physics Handbook, Wiley, New York, 1998, p. 333.)

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