TY - JOUR
T1 - Photoconductance and inverse photoconductance in films of functionalized metal nanoparticles
AU - Nakanishi, Hideyuki
AU - Bishop, Kyle J.M.
AU - Kowalczyk, Bartlomiej
AU - Nitzan, Abraham
AU - Weiss, Emily A.
AU - Tretiakov, Konstantin V.
AU - Apodaca, Mario M.
AU - Klajn, Rafal
AU - Stoddart, J. Fraser
AU - Grzybowski, Bartosz A.
N1 - Funding Information:
Acknowledgements We thank M. Ratner, G. C. Schatz and R. van Duyne for discussions and advice. This work was supported by the Alfred P. Sloan Fellowship and the Dreyfus Teacher-Scholar Award (to B.A.G.).
PY - 2009/7/16
Y1 - 2009/7/16
N2 - In traditional photoconductors, the impinging light generates mobile charge carriers in the valence and/or conduction bands, causing the materials conductivity to increase. Such positive photoconductance is observed in both bulk and nanostructured photoconductors. Here we describe a class of nanoparticle-based materials whose conductivity can either increase or decrease on irradiation with visible light of wavelengths close to the particles surface plasmon resonance. The remarkable feature of these plasmonic materials is that the sign of the conductivity change and the nature of the electron transport between the nanoparticles depend on the molecules comprising the self-assembled monolayers (SAMs) stabilizing the nanoparticles. For SAMs made of electrically neutral (polar and non-polar) molecules, conductivity increases on irradiation. If, however, the SAMs contain electrically charged (either negatively or positively) groups, conductivity decreases. The optical and electrical characteristics of these previously undescribed inverse photoconductors can be engineered flexibly by adjusting the material properties of the nanoparticles and of the coating SAMs. In particular, in films comprising mixtures of different nanoparticles or nanoparticles coated with mixed SAMs, the overall photoconductance is a weighted average of the changes induced by the individual components. These and other observations can be rationalized in terms of light-induced creation of mobile charge carriers whose transport through the charged SAMs is inhibited by carrier trapping in transient polaron-like states. The nanoparticle-based photoconductors we describe could have uses in chemical sensors and/or in conjunction with flexible substrates.
AB - In traditional photoconductors, the impinging light generates mobile charge carriers in the valence and/or conduction bands, causing the materials conductivity to increase. Such positive photoconductance is observed in both bulk and nanostructured photoconductors. Here we describe a class of nanoparticle-based materials whose conductivity can either increase or decrease on irradiation with visible light of wavelengths close to the particles surface plasmon resonance. The remarkable feature of these plasmonic materials is that the sign of the conductivity change and the nature of the electron transport between the nanoparticles depend on the molecules comprising the self-assembled monolayers (SAMs) stabilizing the nanoparticles. For SAMs made of electrically neutral (polar and non-polar) molecules, conductivity increases on irradiation. If, however, the SAMs contain electrically charged (either negatively or positively) groups, conductivity decreases. The optical and electrical characteristics of these previously undescribed inverse photoconductors can be engineered flexibly by adjusting the material properties of the nanoparticles and of the coating SAMs. In particular, in films comprising mixtures of different nanoparticles or nanoparticles coated with mixed SAMs, the overall photoconductance is a weighted average of the changes induced by the individual components. These and other observations can be rationalized in terms of light-induced creation of mobile charge carriers whose transport through the charged SAMs is inhibited by carrier trapping in transient polaron-like states. The nanoparticle-based photoconductors we describe could have uses in chemical sensors and/or in conjunction with flexible substrates.
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U2 - 10.1038/nature08131
DO - 10.1038/nature08131
M3 - Article
C2 - 19606145
AN - SCOPUS:67650809277
SN - 0028-0836
VL - 460
SP - 371
EP - 375
JO - Nature
JF - Nature
IS - 7253
ER -