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Growth Rates<br />

Pure sorbitol<br />

2.5 hours at 40°C<br />

17 hours at RT<br />

2 hours at 35°C<br />

Linear Birefringence<br />

Figure 4a. Figure 4c.<br />

CV<br />

CV<br />

Figure 4b. Figure 4d.<br />

Figure 3a. Figure 3b.<br />

Linear Dichroism Image<br />

Distorted Growth<br />

At Elevated Temperature<br />

CV<br />

Figure 4b.<br />

Diameter (Millimeters<br />

0.5<br />

0.45<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

Figure 3c. Linear<br />

Birefringence Magnitude<br />

Growth rates are influenced by temperature,<br />

molecular structure, and thickness <strong>of</strong> sample.<br />

With increased temperature there is loss <strong>of</strong> order<br />

in the assembly process as indicated by Figure<br />

4b above; additionally the optical properties are<br />

changed indicated by 3b, a linear dichroism<br />

image. In the case <strong>of</strong> D-sorbitol spherulites, the<br />

birefringence is strongly dependent on the<br />

growth temperature. The bright section in Figure<br />

3a has higher birefringence, quantified by the<br />

corresponding Metripol image in Figure 3c.<br />

Growth rates <strong>of</strong> MGO and CV are plotted in<br />

Figure 3d which shows significant variance<br />

based not only on temperature, but also dye<br />

inclusion. Nucleation could not be initiated<br />

above 50° C, though slides that were previously<br />

nucleated showed even faster growth at 50° and<br />

above. Ongoing studies are being conducted to<br />

quantify these growth rates.<br />

Spherulite Growth (µm/hr) at 45°C<br />

Malachite<br />

Green<br />

Oxalate<br />

Malachite<br />

Green<br />

Oxalate<br />

Crystal<br />

Violet<br />

Crystal<br />

Violet<br />

m1y = 0.0014x + 0.0629<br />

R 2 = 0.9603<br />

m2y = 0.0019x + 0.0418<br />

R 2 = 0.9956<br />

c1y= 0.0022x + 0.2124<br />

R 2 = 0.9962<br />

c2y = 0.0024x + 0.0237<br />

R 2 = 0.9473<br />

84 µm/hr<br />

132 µm/hr<br />

144 µm/hr<br />

114 µm/hr<br />

MGO<br />

Metripol has elucidated the slow direction<br />

for light propagation through the spherulites as<br />

indicated in Figures 4a and 4b above. The<br />

magnitude <strong>of</strong> birefringence can also be measured<br />

as seen in Figures 4c and 4d and Table 2. The<br />

direction with the highest refractive index is<br />

oriented radially in the polycrystalline mass<br />

illustrated by the green line in the images 4a<br />

and4b. Work is ongoing to correlate the<br />

refractive index anisotropy to the molecular<br />

structure <strong>of</strong> the material.<br />

Conclusions<br />

Using the self assembly <strong>of</strong> crystal growth<br />

we have demonstrated an anisotropic<br />

chromophore alignment without the use <strong>of</strong><br />

poling techniques. Two orthogonal orientations<br />

are possible with differing chromophores.<br />

Birefringence can also be manipulated based on<br />

the chromophore structure. Growth rates are<br />

easily altered with changes in temperature and<br />

dye structure. Further studies will investigate the<br />

extent to which dyes are aligned in a polar<br />

manner, as well as testing these materials for<br />

their potential as EO devices.<br />

References<br />

Yu, L. 2003 Cryst. Growth Des. 3, 967-971<br />

Wood, E.A. 1977 Crystals and Light, Dover<br />

Publications, New York<br />

Kaminsky, W. 1996 JSTOR 452, 195<br />

Kaminsky, W. 2000 J. Microscopy 198, 1-9<br />

0.05<br />

0<br />

0 20 40 60 80 100 120<br />

Time (Minutes)<br />

Figure 3d. Pure sorbitol spherulites grow at<br />

69.4+ 2.8 µm/hr at 40.5° C.<br />

48 <strong>CMDITR</strong> <strong>Review</strong> <strong>of</strong> <strong>Undergraduate</strong> <strong>Research</strong> Vol. 1 No. 1 Summer 2004

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