Elsevier

Chemical Physics Letters

Volume 479, Issues 1–3, 7 September 2009, Pages 100-104
Chemical Physics Letters

Plasmon tuning of nano-Au in dichroic devitrified antimony glass nanocomposites by refractive index control

https://doi.org/10.1016/j.cplett.2009.07.109Get rights and content

Abstract

Tuning of the surface plasmon resonance (SPR) band of Au0 (587–611 nm) has been demonstrated by controlling the refractive index (1.8349–2.0006) of the encapsulating matrix in a new series of nano-Au0-antimony glass (K2O–B2O3–Sb2O3) dichroic devitrified composites. They have been synthesized by a single-step melt-quench in situ thermochemical reduction technique without using any external reducing agent or additional processing step. Dichroic behavior is due to elliptical shape of Au0 nanoparticles having 13–18 nm size range and aspect ratio about 1.2 according to transmission electron microscopic image. X-ray and selected area electron diffractions manifest the growth of (1 1 1) and (2 0 0) crystallographic planes of Au.

Graphical abstract

We demonstrate the tuning of the surface plasmon resonance (SPR) band of elliptical Au0 nanoparticles (587–611 nm) by controlling the refractive index (1.8349–2.0006) of the encapsulating host matrix in a new series of nano-Au0-antimony glass (K2O–B2O3–Sb2O3) dichroic composites which are synthesized by a new single-step methodology without using any external reducing agent or additional processing step.

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Introduction

Metal–dielectric (glass) nanocomposites have captured sustained intellectual and practical interests over several years owing to their unusual optical and electrical properties and are widely used for real applications, such as fluorescence (photonic) and non-linear optical devices [1], [2], [3], [4]. Noble metal nanoparticles (Au or Ag) are associated with the unique surface plasmon resonance (SPR) phenomenon, which is the dynamic collective oscillation of the conduction electrons upon irradiation [1], [5]. SPR is intimately dependent on the nanoparticle size, shape, refractive index of the dielectric environment and other proximal nanoparticles (NPs) [6]. Precise tuning of the SPR band across a wide spectroscopic range can be accomplished by varying any of the aforesaid parameters [7], [8]. The effects of the medium refractive index on the optical properties of noble metal nanostructures have predominantly captured rising fundamental and technological interest in recent times. The SPR peaks generally experience a red-shift as the refractive index of the surrounding environment is increased [1], [7], [9]. This dependence of their SPR wavelengths on the surrounding refractive index forms the basis of localized surface plasmon resonance spectroscopy (LSPRS) [9] and is also utilized for medium sensing applications [10].

However, the fabrication of metal–glass nanocomposites is not simple. Conventional methods of their preparation involves multi-step techniques like melt-quench or sol–gel route fabrication followed by ion-implantation, ion-exchange and subsequent laser, ion or X-ray beam irradiation and heat treatment for long time at high temperatures in reducing atmosphere (e.g. hydrogen), to generate nanometal incorporated glasses [1], [2], [3], [4], [11]. Most of metal–glass composites to date have been comprised of spherical NPs inserted within silicate or phosphate matrices where it is very difficult to make wide variations of refractive indices. Hence it would be quite interesting to study the effect of matrix refractive index on the unusual optical properties of anisotropic metal NPs embedded within heavy metal oxide glass matrices, like antimony(III) oxide glass, by altering a wide variation of refractive index.

Earlier reports on preparation of high Sb2O3 containing glasses show they are yielded in tiny pieces or pulverized form [12], [13]. This is because the low field strength (0.73) of Sb3+ makes it a poor glass former [12]. Hence, the areas of nanometal-embedded Sb2O3 based glasses and nanocomposites have remained totally unexploited because of their difficulties in preparation particularly in the bulk monolithic forms which are very much essential for convenient optical applications. But, the most important advantage of using Sb2O3 based glass systems over conventional ones is that Sb2O3 is a mild reducing agent [14]. This property enables in situ reduction of Au3+ (HAuCl4·xH2O) to Au0 during the melting process, thereby providing for a straightforward, low-cost strategy for the fabrication of bulk metal–glass nanocomposites in a single-step. Besides other important applications like plasmon enhanced luminescence of rare-earth ions are also promising, taking advantage of the enhanced local field properties of anisotropic NPs [15], [16]. Sb2O3 based systems are also encouraging because they have inherent non-linear optical (NLO) properties and suggested for technological applications like optical recording media [17] due to their photosensitivity, high refractive index, non-centrosymmetric structure [13]. Plasmonic metal nanocrystals if incorporated within such Sb2O3 based glassy hosts are expected to attribute enhanced NLO properties. Consequently, such materials, if synthesized, are also expected to have prospective optoelectronic applications in optical switching and optical limiting devices.

Pondering over the above facts, in this Letter we demonstrate the synthesis of a new series of nano-Au0-embedded antimony glass dichroic nanocomposites by a simple single-step technique and establish the effect of the matrix refractive index on Au SPR band at a fixed concentration of Au. We characterize the resultant nanocomposites by UV–visible absorption spectroscopy, transmission electron microscopy (TEM), selected area electron diffraction (SAED), X-ray diffraction (XRD) and field emission scanning electron microscopy (FESEM) analyses.

Section snippets

Experimental procedure

Twenty gram of nanocomposites having the base glass (KBS) compositions (mol%) xK2O–xB2O3–(100  2x)Sb2O3, where x = 10–25 (composition details are given in Table 1) with KBO2·xH2O (15.7% H2O, Johnson Matthey), Sb2O3 (GR, 99%, Loba Chemie) and HAuCl4·xH2O (49% Au, Loba Chemie) as raw materials were melted at 900 °C in air for 10 min in a high purity silica crucible with an intermittent stirring of 0.5 min. The molten glasses were cast into a carbon plate and annealed at 260 °C for 3 h.

Optical spectra

Results and discussion

A probable mechanism of selective chemical reduction of Au3+ to Au0 by Sb3+ can be explained by considering the reduction potentials (Eo) of the respective redox systems [14]. As the standard potential values for antimony glasses at high temperature are unavailable in literature, so we have used here the room temperature standard potential for simples systems at equilibrium with air.Sb5+/Sb3+,E=0.649VAu3+/Au0,E=1.498VThe overall reaction 3Sb3+ + 2Au3+  3Sb5+ + 2Au0 is a spontaneous reduction having E

Conclusions

We have demonstrated here refractive index controlled plasmon tuning of Au nanoparticles in transparent monolithic devitrified antimony glass nanocomposites synthesized by a new single-step technique without using external reducing agent or additional processing step. UV–visible spectra as well as the physical appearance of the nanocomposites showed a systematic red-shifting of the SPR peak of Au with increasing refractive index, i.e., with increasing Sb2O3 content. TEM image showed

Acknowledgements

T.S. (NET-SRF) gratefully acknowledges the financial support of the Council of Scientific and Industrial Research (CSIR), New Delhi. The authors thank Dr. H.S. Maiti, Director of this institute for his kind permission to publish this Letter. The technical support of the X-ray Division of this institute and TEM facility of IACS, Kolkata are also thankfully acknowledged.

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