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. Author manuscript; available in PMC: 2010 May 27.
Published in final edited form as: J Phys Chem C Nanomater Interfaces. 2009 May 28;113(21):9023–9028. doi: 10.1021/jp903343p

Table 1.

Comparison of the optical cross-sections of Au-based nanostructures obtained experimentally by photoacoustic imaging and theoretical calculation, respectively.a

Cross-section (10-15 m2)
Extinction (σe) Absorption (σa) σa / σe
Nanocages (45.0 nm) Experimental 7.26 ± 0.06 5.96 ± 0.25 0.82 ± 0.04
Calculated 19.88 16.26 0.82
Nanocages (32.0 nm) Experimental 2.99 ± 0.04 3.05 ± 0.12 1 ± 0.04
Calculated 6.39 6.02 0.94
Nanorods (44.0 × 19.8 nm2) Experimental 2.16 ± 0.02 1.87 ± 0.23 0.87 ± 0.11
Calculated 2.15 1.83 0.85
Nanospheres (150 nm) Experimental 145 ± 14.76 -b -
Calculated 99.96 5.73 0.056
a

All the values were obtained at 638 nm.

b

Not detected with photoacoustic imaging.