Tissue Engineering And Nanotheranostics

(Steven Felgate) #1
b2815 Tissue Engineering and Nanotheranostics “9.61x6.69”

156 Tissue Engineering and Nanotheranostics


a > b = c. The depolarization factors isotropically alter the values of


ε 1 and ε2 and the resulting LSPR peak frequencies. Explicitly, they are


as follows:


2
2

1 11


P ln 1


A 21


ee


ee e


−+


=−


−


1


P,


2


A
BC

P


P



==


(10)


where e is the following factor, which includes the particle aspect


ratio R:


(^11)
(^222)
2


1


11.


B


e


AR





=−=−





(11)


The resulting extinction spectrum display non­sphere nanoparti­


cles have two peaks: one result from the transverse plasmon mode


from the x and y contributions to the sum, and the other come form


the longitudinal plasmon mode from the z contribution. Equation (9)


could be used to analyze the effect of the aspect ratio on the LSPR


peak wavelength. Increase in the aspect ratio of non­sphere nanopar­


ticles could result in an increase in weighting εm [(1–Pj) /Pj ], which


is 2 for spherical particles. This leads to a red­shift of the plasmon


peak with increasing aspect ratio, as well as increased sensitivity to the


dielectric constant of the surrounding medium.


2.3. Large Particles Theory


In order to obtain quantitative results for larger particles, the logarith­


mic derivative was introduced in the context of computing scattering


coefficient for a sphere.^5


nn() ln ().


d


D


d


ρψρ


ρ


=


(12)

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