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Introduction to Nanotechnology

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7.7. FECIROFLUIDS 189<br />

Figure 7.25. Optical microsoope picture of Ihe ends of chains of magnetic namparticles in a<br />

ferrolluid film when the OC magnettc field IS perpendicular lo !he surface of the film. The fieH<br />

strength is high enough <strong>to</strong> form Ihe hexagonal lattice configuration. [With permission from<br />

H. E. Hornig et a!., J. Phys. Chem. Solids 62, 1749 (2001).]<br />

in Fig. 7-25, which is also a picture taken through an optical microscope. Initially at<br />

IOW fields the ends of the chains are randomly distrihutcd in the plane ofthe fluid. As<br />

the field increases a critical field is reached whcrc the chain ends become ordered in<br />

a two-dimensional hexagonal amy as shown in Fig. 7-25. This behavior is analogous<br />

<strong>to</strong> the formation of the yoflex lattice in ygc II superconduc<strong>to</strong>rs.<br />

The formation of the chains in the ferrofluid film when a DC magnetic field is<br />

applied makes the fluid optically anisotropic. Light, or more generally electrornagnetic<br />

waves, have oscilla<strong>to</strong>ry magnetic and clt'ctric fields perpendicular <strong>to</strong> the<br />

direction of propagation of the beam. Light is lincarly polarized when these<br />

vibrations nre confined <strong>to</strong> one plane perpendicular <strong>to</strong> the direction of propagation.<br />

rather thnn having random transverse directions. When linearly polarized light is<br />

incidcnt on a magne<strong>to</strong>fluid film <strong>to</strong> which a DC magnetic field is applied, the light<br />

cmcrging from the other side of the film is elliptically polarized. Elliptically<br />

polarized light occurs when the E and H vibrations around the direction of<br />

propagation are confined <strong>to</strong> two mnutllally perpendicular planes, and the vibrations<br />

in each plane are oat of phase. This is called thc Co!fon-Mim?on eflec/. The<br />

expcrimcntal arrangement <strong>to</strong> investigate this eWect is shown in Fig. 7.26. A He-Ne<br />

law hcam linearly polarized by a polarizer is incident QFI the magne<strong>to</strong>fluid film.<br />

A DC magnetic field is applied parallel <strong>to</strong> the plane of thc film. To examine the<br />

polarization of the light emerging From the film, another polarizcr called an anahzer<br />

is placcd between the film and the light detec<strong>to</strong>r, which is a ~h~~<strong>to</strong>~ni~l~iplie~~.<br />

The<br />

intcnsity of thc tmnsrnittcd light is measured as a function of thc oricntation of the

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