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Self-Assembly of Synthetic and Biological Polymeric Systems of ...

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typical AFM is shown. Cantilevers commonly are either V-shaped or a rectangular “diving<br />

board” shaped. The cantilever posses a sharp tip at its free end, which acts as the interaction<br />

probe. This probe has most commonly the form <strong>of</strong> a square-based pyramid or cylindrical cone.<br />

The probe is brought into <strong>and</strong> out <strong>of</strong> contact with the sample surface by the use <strong>of</strong> a piezo-<br />

crystal where the cantilever or the surface itself is mounted, depending on the particular<br />

equipment used. The movement in this direction is conventionally referred to as the Z-axis. A<br />

laser light beam is reflected from the reverse side <strong>of</strong> the cantilever onto a position-sensitive<br />

photodetector. The configuration <strong>of</strong> the photodetector consisted <strong>of</strong> a quadrant photodiode<br />

divide into four parts with a horizontal <strong>and</strong> vertical dividing line. If each section <strong>of</strong> the detector<br />

is labelled from A to D, as shown in Figure 2.12, then the deflection signal is calculated by the<br />

signal difference detected in each part <strong>of</strong> the detector (38).<br />

2.6.- Fluorescence spectroscopy<br />

Once a molecule is excited by the absorption <strong>of</strong> a photon, this can return its ground state<br />

through either fluorescence emission, internal energy conversion (i.e. direct return to the<br />

ground state without fluorescence emission for example, by heat radiation), intersystem<br />

crossing (possibly followed by phosphorescence emission), intramolecular charge transfer<br />

<strong>and</strong>/or conformational change. All these processes can be visualized in the Perrin-Jablonski<br />

diagram (Figure 2.13). The singlet electronic states are denoted as S0 (fundamental electronic<br />

state), S1, S2, ... <strong>and</strong> the triplet states as, T1, T2, ..., with different vibrational levels associated<br />

with each electronic state. It is important to note that energy absorption is very fast (≈10 -15 s)<br />

with respect to all other processes (so that there is no concomitant displacement <strong>of</strong> the nuclei<br />

according to the Franck-Codon principle) (39)(40). The vertical arrows corresponding to the<br />

energy absorption process start from the 0 vibrational energy level, S0, since most <strong>of</strong> molecules<br />

are in this state at room temperature. Absorption <strong>of</strong> a photon, hence, can bring a molecule to<br />

one <strong>of</strong> the vibrational levels <strong>of</strong> S1, S2, ...<br />

Emission <strong>of</strong> photons accompanying the S1 S0 relaxation is called fluorescence. It should be<br />

emphasized that, apart from a few exception, fluorescence emission occurs from S1 <strong>and</strong>,<br />

therefore, its characteristics (except polarization) do not depend on the excitation wavelength<br />

(<strong>of</strong> course only one species exists in the ground state). The transition between the ground<br />

state <strong>and</strong> the excited stated (0-transition) is usually the same for absorption <strong>and</strong> fluorescence.<br />

However, the fluorescence spectrum is located at higher wavelengths than the absorption one<br />

48

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