Elsevier

Vacuum

Volume 180, October 2020, 109497
Vacuum

Design of silver nanoparticles with graphene coatings layers used for LSPR biosensor applications

https://doi.org/10.1016/j.vacuum.2020.109497Get rights and content

Highlights

  • We proposed a hetero-structured glass/Ag-nanoparticles/graphene as high sensitive biosensor applications.

  • Performance enhancement of graphene coated LSPR biosensor.

  • The sensitivity is optimized by selecting the suitable graphene layers.

  • The sensitivity improved by 304.60% when the pure AgNPs conventional biosensor was coated with graphene layer of the 9 nm.

Abstract

A new hybrid graphene nanoplasmonic structure, using silver nanoparticles (AgNPs) coated with a graphene film and deposited on a substrate is proposed in this paper. The aim is to obtain a plasmonic response with high sensitivity for plasmonic biosensors. We show, through the calculation of absorption spectra, that the localized surface plasmon resonance (LSPR) obtained in the SiOx/AgNPs/Graphene nanostructure is very sensitive to variations in the thickness of the graphene and those of the refractive index of the detection medium. The study reveals a shift in plasmon resonance peaks resulting from the coupling between the AgNPs networks and the covering graphene layer. We obtained the red-shift of LSPR modes from 412 nm to 548 nm when the thickness of the graphene layer increases from 0.34 nm to 9 nm. We have shown that the increase in graphene thickness significantly affects the sensitivity of the device under study. An optimal sensitivity value is obtained for a graphene thickness of 9 nm, with a 304.60% gain in sensitivity value compared to the structure without graphene. These properties should enhance these nano-device and make them a preferred choice for biosensors applications, over other current biosensors.

Introduction

Surface plasmon resonance is an electromagnetic mode formed in a region of metal/dielectric surface and results from the interaction between free electrons and the excitation light [1]. Optical properties of metal nanoparticles (Ag or Au) and their contributions in several fields thanks to their multiple advantages that have brought to the forefront broad fields of fundamental and applied research. We would like to mention in particular from wave guiding to biosensor designs based on the nanoparticles array [[2], [3], [4]]. Localized surface plasmonic resonance biosensors (LSPR) are the most advantageous biosensors by virtue of their ability to providing biomolecular detection with higher sensitivity, mainly by removing the time-consuming marking process that reduces molecular bonding perturbations [[5], [6], [7]]. The plasmonic response of metal nanoparticles has been intensively studied and has shown a strong dependence on their sizes, shapes and constituent material [[8], [9], [10]]. It is evident from previous available studied literature (on metallic nanoparticles) that a number of parameters definitely govern their performance [11,12].

Spectacular progress on the control of optical properties of the graphene material sheets stimulated the search for new types of two-dimensional materials. Graphene is actually a two-dimensional crystal, composed of carbon atoms arranged in a hexagonal pattern, and whose stack constitutes graphite. In the visible field, it is an absorbent and dispersive material. It has many potential applications thanks to its unique electrical, mechanical, chemical and optical properties [[13], [14], [15], [16]]. Graphene may outperform existing transparent conductive materials, and a graphene based flexible touch screen was demonstrated by Bae et al. [17]. Multilayer graphene is a graphene of thin film with weak van der Waals interaction between the layers, and its electronic and optical properties are sensitive to the number of the layers as well as the stacking sequence [14].

Graphene is being considered a very interesting new kind of material that can be applied in various fields (including bio-plasmonics). It's well proven that AgNPs extensively absorb within restricted frequency bands in the visible spectrum when their LSPR are excited. Besides, the influence of the dielectric medium has been extensively studied [[18], [19], [20], [21]]. Some of this work concentrates on the effect of the graphene layers (whose refractive index is ng [22,23]) on AgNPs optical properties. Graphene has received significant interest in late years due to its outstanding properties [2,14,24], an extremely sensitive plasmonic biosensor that uses the graphene layers to amplify the sensitivity induced by light absorbed in the graphene [18,25].

This is performed in the case when the graphene layers are deposited on the nanoparticles array. More precisely, we will analyze the effect by gradually varying the thickness of the graphene multilayers from 0.34 nm to 9 nm. Different dielectric coatings of the index n2 are embedded above AgNPs/graphene, which in turn rest in direct or indirect contact with a SiOx substrate (n1). We study how the graphene layers are deposited; those are SiOx/AgNPs/graphene. The associated work geometry is illustrated in Fig. 1(a) and (b). The incident-light wave (along the Oy-axis) whose electric field is TM polarized along Ox-axis.

The LSPR structures used throughout this work consist of a random assembly of silver nanostructures (AgNPs) supported on glass. The SEM image in Fig. 2(a) shows the distribution size as well as the overall shape of the resulting Ag nanoparticles. To validate the numerical model, we studied the response of a sample manufactured by our collaborators at the Lille University [12], the SEM image in the surface characterization Fig. 2 shows the sample in question which consists of Ag nanoparticles aletorically deposited on a glass substrate. We made an image analysis and extracted the relevant geometrical parameters. The nonoparticles were modelled by nanoribbons, the gometrical parameters considered are: l, h and a Fig. 1(a) and (b).

Throughout the document, the structural geometrical parameters will be defined such that l = 25 nm is the nanoparticles length, a = 70 nm is the network parameter (along x-axis), and h = 20 nm is the nanoparticles height.

Due to the important properties of the graphene as an effective solution to the sulfidation problem of Ag nanoparticles and the binding of biological elements [2,26], the AgNPs nanostructure was coated with a graphene layer on top, as shown in Fig. 1(b). The numerical results show that, compared to graphene is an LSPR substrate based biosensor/AgNPs, graphene in an LSPR substrate based biosensor/AgNPs/graphene offers a 304.60% higher sensitivity for nine graphene layers.

This work is structured as follow: Section 2 briefly introduces the theoretical model of numerical calculation and the method used to calculate the biosensor sensitivity. Section 3, demonstrates the corresponding results when AgNPs are covered with graphene multilayers, and when the trainers are applied on to a SiOx substrate. Finally, section 4 will summarize the sensitivity results.

Section snippets

Simulation model

The optical properties of silver nanoparticles (AgNPs) are determined numerically within a wavelength domain ranging from UV to near IR, specifically, [300 nm–800 nm]. Simulations are performed using Finite Element Method (FEM) [27]. Actually, the simulation method has already been well documented in Refs [[28], [29], [30]]; it focuses on solving Maxwell's equations in the frequency domain by discretizing space in small finite elements (having various possible shapes such as triangular,

Results and discussion

The plasmonic characteristics of the nanoparticles (AgNPs) are defined by the interaction between incident electromagnetic wave and free electrons on the surface. In order to have an understanding of the plasmonic behavior of the AgNPs arrays system depicted in Fig. 1, we have first calculated the absorption of the array when immersed in a non-absorbent dielectric (n2). The AgNPs array has an aspect ratio (defined as the ratio of length(l)/height(h)) of 1.25. The interaction between AgNPs is

Conclusion

The refractive index sensitivities S (in nm/RIU) of multilayered localized plasmonic interfaces, glass/AgNPs/graphene/dielectric were determined by using the Lorentz-Drude model. Our study showed that the plasmonic response of the nanostructure is very sensitive to variations in the thickness of the graphene film and/or the refractive index of the detection medium. The increase in graphene thickness from 0.34 nm to 9 nm causes a red shift of the localized surface plasmon resonance (LSPR). The

Acknowledgements

A. Akjouj gratefully acknowledges the hospitality of the department of Physics, Faculty of Science, University of Moulay Ismail of Meknes. This work was partially supported by the program FINCOME “Centre National pour la Recherche Scientifique et Technique, Morocco”.

References (57)

  • R. Verma et al.

    Sensitivity enhancement of a surface plasmon resonance based biomolecules sensor using graphene and silicon layers

    Sensor. Actuator. B Chem.

    (2011)
  • J. Homola et al.

    Surface plasmon resonance sensors: review

    Sensor. Actuator. B Chem.

    (1999)
  • H. Mu et al.

    Localized surface plasmon resonance properties of Ag nanorod arrays on graphene-coated Au substrate

    Optic Commun.

    (2017)
  • S. Zeng et al.

    Graphene-MoS2 hybrid nanostructures enhanced surface plasmon resonance biosensors

    Sensor. Actuator. B Chem.

    (2015)
  • N.-C. Chen et al.

    Self-corrected sensing based on a metal-dielectric-metal surface plasmon resonance structure for disturbance-free detection

    Vcuum

    (2015)
  • W. Wei et al.

    Single-layer graphene-coated gold chip for enhanced SPR imaging immunoassay

    Sensor. Actuator. B Chem.

    (2018)
  • M. El Barghouti et al.

    MoS2-graphene hybrid nanostructures enhanced localized surface plasmon resonance biosensors

    Optic Laser. Technol.

    (2020)
  • J.C. Reed et al.

    Graphene-enabled silver nanoantenna sensors

    Nano Lett.

    (2012)
  • A. Hessel et al.

    A new theory of woods anomalies on optical gratings

    Appl. Optic.

    (1965)
  • M. El Barghouti et al.

    Effect of MoS2 layer on the LSPR in periodic nanostructures

    Optik

    (2018)
  • J. Homola et al.

    Surface plasmon resonance based sensors

    Spring

    (2006)
  • A.L. Spetz

    Vacuum technology applied to solid state chemical sensors, processing, characterization and applications

    Vacuum

    (2012)
  • A.G. Nikitin et al.

    “Narrow plasmon resonances in diffractive arrays of gold nanoparticles in asymmetric environment: experimental studies,” Appl

    Phys. Lett.

    (2013)
  • A. Otto

    Excitation of nonradiative surface plasma waves in silver by method of frustrated total reflection

    Z. Phys.

    (1968)
  • E. Kretschmann et al.

    Radiative decay of nonradiative surface plasmons excited by light

    Z. Naturforsch.

    (1968)
  • L. Touahir et al.

    Plasmonic properties of silver nanostructures coated with an amorphoussilicon-carbon alloy and their applications for sensitive sensing of DNA hybridization

    J. Phys.: Analyst

    (2011)
  • S.-E. Zhu et al.

    Optical transmittance of multilayer graphene

    EPL (Europhys Lett)

    (2014)
  • Neto A.H. Castro et al.

    The electronic properties of graphene

    Rev. Mod. Phys.

    (2009)
  • Cited by (41)

    • Polarization-independent multifunction applications based on perfect absorption in a simple graphene metasurface

      2022, Vacuum
      Citation Excerpt :

      During the past ten years, research on SPR has mostly focused on metal materials to study various optical properties in metamaterials or waveguide systems at visible and near-infrared wavelengths. Especially, their respective excitation conditions, propagation distances, loss coefficients, modulation methods, and potential applications [16–21]. Although, these structures can overcome the diffraction limit associated with classical physics, and can initially achieve photonic circuits in the subwavelength range.

    • Figure of merit and sensitivity enhancement of biosensor LSPR in investigated for visible and near infrared

      2022, Photonics and Nanostructures - Fundamentals and Applications
      Citation Excerpt :

      On the other hand, a substantial decrease in absorption intensity is observed as the dAu increases. This supports the claim that, although the characteristics of the LSPR can be improved by the insertion of a gold film [4,64,65], the selection of a gold film with a thickness greater than 30 nm would be appropriate: (i) for the accurate detection of interaction processes and (ii) for the thinner gold film to be easily cased. As can be seen in Fig. 7(c), the resonance wavelength increases significantly with increasing incidence angle.

    • Nanophotonic biosensors for disease diagnosis

      2022, Nanomaterials for Sensing and Optoelectronic Applications
    View all citing articles on Scopus
    View full text