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W. Richard Bowen and Nidal Hilal 4

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Y Range: 1.21 μm<br />

(a)<br />

0.205<br />

–1.00 –0.399<br />

8.5 STAR-SHAPEd POLyMERS AdSORBEd ON SURFACES 239<br />

Height range: 2.234 nm<br />

1.03 1.63 2.24<br />

X Range: 1.21 μm<br />

Y Range: 1.21 μm<br />

(c)<br />

–1.71 –1.11<br />

–2.32<br />

2<br />

1.6<br />

1.2<br />

0.8<br />

0.4<br />

Height range: 5.050 nm<br />

–1.26 –0.652 –0.0473<br />

X Range: 1.21 μm<br />

adsorbed amounts, no interpenetration <strong>and</strong> fusion were observed. The star<br />

polymers continued to keep their individuality <strong>and</strong> they formed isolated<br />

globules upon the evaporation of the solvent.<br />

In Figure 8.14, we compare the overall monolayer organisation for<br />

long incubation times. Such incubation times are long enough to achieve<br />

the maximum adsorbed amount (within our adsorption protocol using<br />

dilute polymer solutions). The 18-arm star polymers organised in discontinuous<br />

asymmetric isl<strong>and</strong>s, which consist of several individual polymer<br />

chains; it is clear that the star polymers penetrated each other when in<br />

good solvent <strong>and</strong> they collapsed in groups upon drying. The 32-arm star<br />

polymers also penetrated each other <strong>and</strong> they self-assembled in a continuous<br />

dense network. On the other h<strong>and</strong>, the 59-arm star polymers did<br />

Y Range: 1.21 μm<br />

(b)<br />

–0.56 0.0452 0.65<br />

Height range: 10.03 nm<br />

–2.59 –1.98 –1.38<br />

X Range: 1.21 μm<br />

FIgurE 8.12 AFM topography images of star polymers adsorbed on mica: (a) 18 arms,<br />

incubation time of 5 min; (b) 32 arms, incubation time of 10 min <strong>and</strong> (c) 59 arms, incubation<br />

time of 180 min.<br />

10<br />

7.5<br />

5<br />

2.5<br />

5<br />

4<br />

3<br />

2<br />

1

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