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Fluorescence; Fluorescence resonance energy transfer (FRET); Metal-ion sensing; Molecular wire effect

https://doi.org/10.1016/J.TRAC.2011.04.017
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behera, pradipta. Fluorescence; Fluorescence Resonance Energy Transfer (FRET); Metal-Ion Sensing; Molecular Wire Effect.

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behera, pradipta. Fluorescence; Fluorescence resonance energy transfer (FRET); Metal-ion sensing; Molecular wire effect. https://doi.org/10.1016/J.TRAC.2011.04.017

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behera, pradipta. “Fluorescence; Fluorescence Resonance Energy Transfer (FRET); Metal-Ion Sensing; Molecular Wire Effect,” n.d. doi:10.1016/J.TRAC.2011.04.017.

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behera pradipta. Fluorescence; Fluorescence resonance energy transfer (FRET); Metal-ion sensing; Molecular wire effect. doi:10.1016/J.TRAC.2011.04.017

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behera, pradipta (no date) “Fluorescence; Fluorescence resonance energy transfer (FRET); Metal-ion sensing; Molecular wire effect.” doi: 10.1016/J.TRAC.2011.04.017.

Abstract

This review deals with the emerging field of fluorescent conjugated polymers for the development of chemical and/or biochemical sensors. As a result of their amplified physical properties due to a ''molecular wire effect'', these materials offer excellent characteristics to develop different sensing schemes (e.g., employing direct superquenching or relying on development of fluorescence-resonance-energy-transfer formats). The versatility of their synthesis procedures allows us to introduce the desired functional groups to achieve analytically useful interactions with analytes [e.g., from transition-metal ions to explosives, or even, in recent years, relevant biomolecules (e.g., proteins or DNA, where conformational changes play a decisive role in detection)].

Fluorescent conjugated polymers for chemical and biochemical sensing Adrian Alvarez, Alfonso Salinas-Castillo, Jose ´ M. Costa-Ferna ´ndez, Rosario Pereiro, Alfredo Sanz-Medel This review deals with the emerging field of fluorescent conjugated polymers for the development of chemical and/or bio- chemical sensors. As a result of their amplified physical properties due to a ‘‘molecular wire effect’’, these materials offer excellent characteristics to develop different sensing schemes (e.g., employing direct superquenching or relying on development of fluor- escence-resonance-energy-transfer formats). The versatility of their synthesis procedures allows us to introduce the desired functional groups to achieve analytically useful interactions with analytes [e.g., from transition-metal ions to explosives, or even, in recent years, relevant biomolecules (e.g., proteins or DNA, where conformational changes play a decisive role in detection)]. ª 2011 Elsevier Ltd. All rights reserved. Keywords: Biochemical sensing; Chemical sensing; Conjugated polymer; Conjugated polyelectrolyte; DNA sensing; Explosives sensing; Fluorescence; Fluorescence resonance energy transfer (FRET); Metal-ion sensing; Molecular wire effect 1. Introduction Synthetic polymeric materials are widely used today in a great variety of applica- tions, including packaging, adhesives and lubricants, electrical insulators for micro- electronics, and implantable devices in biomedical applications. A particular type of polymer of emerging potential in ana- lytical chemistry is the so-called conju- gated polymer (CP). CPs, which are conducting polymers, are polyunsaturated compounds with alternating single and double bonds along the polymer chain, in which all backbone atoms are sp or sp 2 hybridized. The resulting interaction be- tween orbitals creates a semiconductor- band structure having a valence band (filled with electrons) and a conduction band (devoid of electrons). The electronic conjugation between each repeating unit creates a semicon- ductive ‘‘molecular wire’’, providing very useful optical and electronic properties. It is the presence of such a conjugated elec- tronic structure that gives CPs their name, and Fig. 1 shows some of the most common basic structures. Also, CPs incorporating pendant ionic functional groups in the polymeric back- bones (Fig. 2) are named ‘‘conjugated polyelectrolytes’’ (CPEs). The discovery in 1977 of the first con- ducting polymer, a halogenated derivative of poly(acetylene), by Shirakawa et al. [1], opened a growing field of exciting new applications. The delocalized (conjugated) electronic structure of poly(acetylene) is responsible of the good mobility of the charge carriers (which can be created through doping) and of the strong light absorption in the UV–visible region. Unfortunately, poly(acetylene) is difficult to process and is unstable in the presence of oxygen or water, making it useless for many applications. Nevertheless, further research led chemists to develop much more stable aromatic CPs. Such polymeric materials today offer a combination of the best fea- tures of metals and typical semiconductors with those of synthetic polymers. They have been successfully employed (e.g., as transparent antistatic coatings, transis- tors, light-emitting diodes, photovoltaic cells, modified electrodes, and biosensors). A general characteristic of neutral CPs is that they are wide band-gap semicon- ductors usually showing efficient UV-Vis- ible absorption or emission at the band Adrian Alvarez, Jose ´ M. Costa-Ferna ´ndez, Rosario Pereiro, Alfredo Sanz-Medel* Department of Physical and Analytical Chemistry, University of Oviedo, Avda. Julian Claveria 8, E-33006 Oviedo, Spain Alfonso Salinas-Castillo* Department of Analytical Chemistry, Faculty of Sciences, University of Granada, Granada, Spain * Corresponding author. Tel./Fax: +34 985 103 474; E-mail: asm@uniovi.es Trends in Analytical Chemistry, Vol. 30, No. 9, 2011 Trends 0165-9936/$ - see front matter ª 2011 Elsevier Ltd. All rights reserved. doi:10.1016/j.trac.2011.04.017 1513
edge. Moreover, they can emit strong luminescence, but its efficiency is affected by delocalization and polarization of the electronic structure. Although CPs generally exhibit low conductivities, these can be significantly increased by means of doping. (When talking about doping in a CP, we are not referring to the replacement of atoms in its structure, as happens in a common semiconducting material, but to the oxi- dation or the reduction of the conjugated electronic system: p-doping and n-doping, respectively). This can be carried out chemically or electrochemically, and a counterion is needed to keep electroneutrality. The intrinsic physico-chemical properties of CPs make them highly attractive for the development of novel chemical and biochemical sensors [2]. One of their most remarkable advantages for sensing applications, compared to devices based on conventional organic molecules, is the ability of CPs to exhibit enhanced col- lective properties, resulting in amplified sensitivity to very small perturbations or interactions, (particularly as a result of their enhanced transport properties, electrical conductivity or rate of energy migration). Moreover, another function of polymers when used in sensory devices is to act as structural materials to ensure stability. Such CP-based sensors can provide analyte recognition as a result of an appropriate covalent or physical inte- gration of the appropriate receptor, imprinting, and/or due to the intrinsic electrostatic and chemical charac- Figure 1. Basic repeating units of some of the most common conjugated polymers. Figure 2. Common functionalizations leading to conjugated polyelectrolytes. (MPS-PPV): [poly (2-methoxy-5-propyloxy sulfonate phenylene vinylene] (Reproduced from [58] with permission). Trends Trends in Analytical Chemistry, Vol. 30, No. 9, 2011 1514 http://www.elsevier.com/locate/trac
teristics of the CP. As usual, such recognition results in a measurable change (analytical signal). As a consequence of their advantageous properties of CPs, CP-based sensors have been developed with a variety of transducing schemes, those employing changes in electrochemical or optical properties being particularly relevant. Although CPs have been used for the construction of very diverse chemical-sensing platforms, growing interest has been focused in recent years on biomolecular recognition, with DNA molecules being remarkable targets, both for electrochemical and optical CP-based sensors. CP-based electrochemical sensors mainly rely on conductometric and potentiometric measurements. At a fixed potential, CP conductivity can change by several orders of magnitude even with a small amount of charge injection. CPs have also been employed in the development of potentiometric sensors, just by immobilizing the CP on a single electrode. The reversible nature of the redox pro- cesses taking place in CPs, as well as their sensitivity to conformation and electrostatics in the medium, is the basis for potentiometric measurements with CPs. As alternatives, optical sensors can also be developed by taking advantage of the excellent optical properties of CPs. Many colorimetric sensing systems have been successful, based on changes in the absorption properties of CPs. However, in this review, we review and discuss the exploitation of the intrinsic fluorescence of CPs, of increasing analytical importance. Fluorescent CPs have the structure of a conjugated molecular wire, for which a minor disturbance caused by the analyte can be ampli- fied in not only the molecular chains of the system but also the entire polymer system. This determines the ability of CPs to detect analytes at ultra-low content, due to their improved sensitivity, typically better than that of conventional, small molecule-based fluorescent sensors. After reviewing the sensing mechanisms of fluorescent CPs, we review their use as optical sensors for ions and small molecules, as well as biosensing of proteins. Finally, we discuss future prospects for the use of fluor- escent CPs in bioanalysis. 2. Optical properties of conjugated polymers As mentioned above, due to electronic delocalization, CPs exhibit interesting optical properties, especially related to the absorption of radiation and the relaxation of their electronic excited states via fluorescent emission. Development of fluorescence sensors with CPs is partic- ularly interesting because of the expected enhanced sensitivity, as discussed above, as a consequence of the delocalization of the charge carriers in the polymeric structure. As a result, they have been referred to as ‘‘amplifying fluorescent polymers’’. Fluorescence-quenching processes can also be observed (called ‘‘superquenching’’). Direct superquen- ching of CP fluorescence can be described by the well- known Stern-Volmer relationships, and it has allowed the development of very sensitive sensors for some molecules or ions (although the selectivity observed was not usually very satisfactory). Selectivity can be in- creased by means of so-called quencher-tether-ligand complexes, resulting from the conjugation of a quencher group to a ligand of biological relevance, selectivity being achieved by means of the specific interaction between the resulting complex and the analyte (e.g., a protein). A special application of fluorescence in CPs is to develop systems based on the deactivation of their intrinsic fluo- rescent emission (so-called ‘‘turn off’’ optosensing sys- tems) and those based on an increase of the intensity of that emission previously quenched (so-called ‘‘turn off- turn on’’ systems). When comparing both approaches, probably the greatest advantage of the fluorescence ‘‘turn-on’’ sensors over ‘‘turn-off’’ systems is the higher sensitivity typically achieved by ‘‘turn-on’’ sensors be- cause of the low fluorescence background. Moreover, ‘‘turn-on’’ systems reduce the likelihood of false-positive signals as fluorescence-enhancement processes are typi- cally more selective than fluorescence quenching. The semiconductive nature of CPs makes such mate- rials a highly efficient electron-transport medium. The collective optical and conducting properties of CPs lead to ultra-highly-sensitive optical-sensing systems. Thus, CPs are extremely sensitive to minor external structural per- turbations or electron-density changes within the poly- mer, as they self-amplify their fluorescence-quenching response to perturbation of the electronic network upon binding of the analyte. Appropriate CPs can exhibit strong luminescence, and delocalization and/or polarization of their electronic structure may change such luminescence dramatically, so such polymers are good candidates as transducers for very sensitive fluorescence sensing. Fig. 3 shows how CPs amplify the molecular recogni- tion signal via migration of electrons along the polymer chain. Whereas complete fluorescence quenching would be observed with the CP upon interaction with an analyte, with non-conjugated sites exposed to the same analyte concentration, only a small quenching effect would be observed. Each analyte is confined to its particular mole- cule and can sample only one binding site, so the emission is observed from those molecules that did not bind the analyte. In the CP approach, one single interaction can quench a large number of fluorophores and the signal obtained in the presence of the analyte is amplified. The highly amplified quenching effect in CPs can be explained as a consequence of the electronic mobility and the transport of excitons (electron-hole pairs gener- ated through photoexcitation) along the polymer back- bone (‘‘molecular wire effect’’). Analyte binding produces a trapping site whereby the excitation is effectively deac- tivated by electron-transfer quenching. This energy migration should be considered a collective property of the Trends in Analytical Chemistry, Vol. 30, No. 9, 2011 Trends http://www.elsevier.com/locate/trac 1515

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