High-Sensitivity Biosensor-Based Enhanced SPR by ZnO/MoS<sub>2</sub> Nanowires Array Layer with Graphene Oxide Nanosheet

Guo, Shiliang; Wu, Xiaogang; Li, Zhiquan; Tong, Kai

doi:https://doi.org/10.1155/2020/7342737

International Journal of Optics

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Abstract Introduction Results and Discussion Conclusion Data Availability Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2020 | Article ID 7342737 | https://doi.org/10.1155/2020/7342737

High-Sensitivity Biosensor-Based Enhanced SPR by ZnO/MoS₂ Nanowires Array Layer with Graphene Oxide Nanosheet

Shiliang Guo,¹Xiaogang Wu,^1,2Zhiquan Li,¹and Kai Tong¹

Academic Editor: Tomasz Osuch

Received02 Aug 2019

Revised01 Feb 2020

Accepted27 May 2020

Published01 Sept 2020

Abstract

A novel SPR biosensor that can achieve a high sensitivity is proposed; therefore, a new prism coupling structure based on metal nanowires array layer is designed in this paper. The thickness of each medium layer for the structure is analyzed to obtain the optimal SPR spectrum, by the finite element method, so that the sensitivity is able to be enhanced greatly. The optimal thicknesses of each medium layer are given, and the sensitivity of the SPR biosensor can reach as high as 210.75°/RIU for the refractive index of the sensing medium, from 1.30 to 1.38.

1. Introduction

Surface plasmon resonance (SPR) is the resonance for free electrons with collective oscillations in the metal surface when excited by the incident light, and the energy of the incident light would be absorbed by free electrons during the resonance, so that the energy of the output light would be decreased to some extent [1–3]. The decreasing degree of the output light is related to the the incident light, and the SPR angle is the incident light as the output light is decreased to the minimum. SPR can be excited in a variety of ways, such as prism coupling, grating coupling, and optical fiber coupling, and SPR has been extensively used in sensing of various physical, chemical, and biochemical parameters [4–6].

The surface plasmon resonance biosensor (SPR biosensor) has a remarkable capability of real-time detection and monitoring of biomolecule [7–9]. There are various factors that significantly affect the function of the SPR biosensor, which are needed to be considered for designing a stable and highly sensitive SPR biosensor. The two features, the high detection sensitivity and the good SPR peak for better precision, are critical to the function implementation of the SPR biosensor as well as its application. The SPR biosensor has been studied during the past thirty years [8, 9]. There are many studies on the sensitivity of the SPR biosensor before, such as transition metal dichalcogenides (TMDC) materials [10], magneto-optic (MO) material layer [11], magneto-plasmonic (MP) transducers [12], graphene [13, 14], graphene-MoS₂ hybrid nanostructures [15], and graphene and silicon layers [16]. However, a new prism coupling structure with the TiO₂-ZnO layer and MoS₂-graphene oxide (GO) was present. Based on this, a novel SPR biosensor capability of achieving a higher sensitivity was proposed in this paper which can provide a further theoretical preparation for making the SPR biosensor detecting instrument in the future.

2. Design Consideration and Theoretical Model

2.1. Design Consideration

In this paper, there are various nanosheets considered to be added into the structure, in order to enhance the sensitivity of the SPR biosensor. MoS₂ has high optical absorption and there exists direct bandgap (1.8 eV) for the monolayer MoS₂ [17]. Graphene oxide (GO) has several advantages because of its extraordinary optical and structural properties, and it was studied that there was four times greater sensitivity for the SPR biosensor based on GO than that based on the conventional gold film [18–20]. Then, the GO-MoS₂ hybrid nanolayer was chosen to strengthen the SPR effect.

Zn oxide (ZnO) is a semiconductor with a wide energy band (3.37 eV), and also has the high exciton binding energy [21–23]. TiO₂ has the important characteristics that the electric field would be enhanced by local SPR, and also the form of electron and hole pairs would be increased for TiO₂, as there exists plasmon enhancement because of the light absorption [24, 25]. And therefore, TiO₂-ZnO hybrid nanolayer is able to benefit the sensitivity of the SPR biosensor and can be chosen to enhance the sensitivity.

The model of the proposed biosensor is a prism coupling structure with seven-layer, as shown in Figure 1. The structure is composed of a prism, TiO₂-ZnO, Au, MoS₂-GO, and a sensing medium layer successively. ZnO and MoS₂ nanolayer are designed to be nanowires array layers. The refractive index of the prism is 1.54. The refractive index of TiO₂, ZnO and Au is 2.5837, 2.9497 + 0.0227i, and 0.0585 + 4.2665i, respectively. The refractive index of MoS₂ is 5.9 + 0.8i, the monolayer thickness is 0.65 nm, and the multilayer thickness is L × 0.65 nm. The refractive index of GO is 2 + 0.56i, the monolayer thickness is 1.6 nm, and the multilayer thickness is L × 1.6 nm. L is the number of thicknesses for MoS₂ and GO layer. The refractive index of the sensing medium layer of the biosensor is from 1.30 to 1.38. The wavelength of incident light is 632.8 nm.

2.2. Calculation Method

The structure of the proposed SPR biosensor in this paper is shown in Figure 1. The incident light and p-polarized light falls on the metal layers through the prism by the total reflection. There exists an evanescent wave whose amplitude is decayed exponentially normal to the interface by the total reflection. When , surface plasmon, at the interface of the metal and dielectric, are excited by the evanescent wave. The relationship between them is given as follows:where is the wave number vector of the incident light across the medium, is the wave number vector of the surface plasmon wave, and (j = 0, 1, 2, …, 6) is the dielectric constants of each medium layer including the prism, TiO₂, ZnO, Au, MoS₂, GO, and the sensing medium layer, respectively. (j = 0, 1, 2, …, 6) is the refractive index correspondingly, is the speed of light in vacuum, is the frequency, and is the angle of incidence.

When the incident light is p-polarized light, the reflection coefficient R for the whole structure designed can be given, according to the Fresnel equation and the reflectivity equation, as follows [26]:where is the reflection ratio of the strength for the electric field at the interface between the two adjacent medium, and , (p = 0, 1, …, 5. q = 1, 2, …, 6. j = 0, 1, 2, …, 6).

3. Results and Discussion

3.1. Thickness of Au, MoS₂, and Graphene Oxide

The effect of the number of MoS₂ nanowires array layers on the SPR spectrum, when the refractive index of the sensing medium layer is 1.30, 1.32, 1.34, 1.36, and 1.38 is shown in Figure 2. The thickness of TiO₂, ZnO, Au, and GO layer is 20 nm, 10 nm, 40 nm, and 1 × 1.6 nm, respectively. As shown in Figures 2(a)–2(d), it is obviously found that there exist a good SPR spectrum and shift of the SPR angle for all the refractive indices of 1.30, 1.32, 1.34, 1.36, and 1.38, when MoS₂ nanowires array is monolayer. And also, the conclusion is still effective for other thicknesses of TiO₂, ZnO, Au, and GO layer, as the same case of the refractive index for the sensing medium layer.

(a)

(b)

(c)

(d)

Figure 2

SPR spectrum (a) for number of MoS₂ layer L = 0, (b) for number of MoS₂ layer L = 1, (c) for number of MoS₂ layer L = 2, (d) for number of MoS₂ layer L = 3, for different refractive indices of sensing medium layer. The curves A1, A2, A3, A4, and A5 stand for the refractive index of sensing layers n = 1.30, n = 1.32, n = 1.34, n = 1.36, and n = 1.38, respectively. The thickness is 20 nm, 10 nm, 40 nm, and 1 × 1.6 nm for TiO₂, ZnO, Au, and GO layer, respectively.

The effect of the number of GO layers on the SPR spectrum, when the refractive indices of the sensing medium layer are 1.30, 1.32, 1.34, 1.36, and 1.38, is shown in Figure 3. The thickness of TiO₂, ZnO, Au, and MoS₂ layer is 15 nm, 10 nm, 46 nm, and 1 × 0.65 nm, respectively. As shown in Figures 3(a)–3(d), it is obviously found that the shift of the SPR angle increased gradually, with the increase in the number of GO layers from L = 0 to L = 4. However, only when the number of GO layers is three (L = 3), there would exist a good SPR spectrum for all the refractive indices of the sensing medium layer from 1.30 to 1.38. It is shown from the beginning that the number of GO layers is four (L = 4), the SPR curves begin to become not obvious. As a result, it is shown by the research that the number of GO layers is three (L = 3) which is a benefit of the generation of SPR tip and the shift of SPR angle, which shows reasonable agreement with the other cases of different thicknesses of TiO₂, ZnO, Au, and MoS₂ layer.

(a)

(b)

(c)

(d)

Figure 3

SPR spectrum (a) for number of GO layer L = 0, (b) for number of GO layer L = 2, (c) for number of GO layer L = 3, (d) for number of GO layer L = 4, for different refractive indices of the sensing medium layer. The curves A1, A2, A3, A4, and A5 stand for the refractive index of sensing layer n = 1.30, n = 1.32, n = 1.34, n = 1.36, and n = 1.38, respectively. And the thickness is 15 nm, 10 nm, 46 nm, and 1 × 0.65 nm for TiO₂, ZnO, Au, and MoS₂ respectively.

The effect of thickness of Au layer on the SPR spectrum, when the refractive index of the sensing medium layer is 1.30 and 1.38, is shown in Figure 4. The thickness of TiO₂, ZnO, MoS₂, and GO layer is 15 nm, 10 nm, 1 × 0.65 nm, and 3 × 1.6 nm, respectively. As shown in Figure 4, it is found that there is an obvious SPR peak when the thickness of Au layer is between 45 nm and 60 nm for n = 1.30, and also, there is an obvious SPR peak when the thickness is between 40 nm and 50 nm for n = 1.38. Moreover, it is shown by the research that 46 nm, the thickness of Au layer, is the optimal thickness because of the good SPR peak as well as the large shift of the SPR angle, for the refractive index from 1.30 to 1.38.

Figure 4

SPR spectrum for different thicknesses of Au layer for d = 40 nm (curves A1 and A2), 45 nm (curves B1 and B2), 50 nm (curves C1 and C2), and 60 nm (curves D1 and D2), as the case of n = 1.30 and n = 1.38 for sensing medium. The curves A1, B1, C1, and D1 stand for the refractive index of sensing layer n = 1.30, the curves A2, B2, C2, and D2 stands for the refractive index of sensing layer n = 1.38. The thickness is 15 nm, 10 nm, 1 × 0.65 nm, and 3 × 1.6 nm for TiO₂, ZnO, MoS₂, and GO layer, respectively.

3.2. Thickness of TiO₂ and ZnO Layers

The sensitivity of the SPR biosensor can be defined aswhere, Δθ_SPR is the change in resonance angle, Δn is the the change in refractive index, and S_n is the sensitivity of the SPR biosensor.

The thickness of TiO₂-ZnO layers is a positive factor that enhances the sensitivity of the proposed SPR biosensor. The variation of the SPR spectrum with the thickness of TiO₂ is shown in Figure 5(a). There exists an obvious change for the SPR spectrum as the different thickness of TiO₂ for 10 nm, 15 nm, and 20 nm. The change relation between the change of SPR angle and the thickness of TiO₂ layer is shown in Figure 5(b); it is found that the change of SPR angle reaches the largest when the thickness of TiO₂ layer is 15 nm, which the largest change of SPR angle is 16.86°. The change relation between the sensitivity of the SPR biosensor and the thickness of TiO₂ layer is shown in Figure 5(b), and it is found that the sensitivity of SPR biosensor reaches the highest when the thickness of ZnO nanowires array layer is 40 nm as a result of the largest change of SPR angle, for which the sensitivity can reach 210.75°/RIU.

(a)

(b)

The variation of the SPR spectrum with the thickness of ZnO nanowires array layer is shown in Figure 6(a). There exists an obvious change for the SPR spectrum as the different thicknesses of ZnO nanowires array layer are 10 nm, 15 nm, and 20 nm. The change relation between the change of SPR angle and the thickness of ZnO nanowires array layer is shown in Figure 6(b), and it is found that the change of SPR angle reaches the largest when the thickness of TiO₂ layer is 40 nm and the largest change of SPR angle is 16.86°. The change relation between the sensitivity of the SPR biosensor and the thickness of ZnO nanowires array layer is shown in Figure 6(b), and it is found that the sensitivity of the SPR biosensor reaches the highest when the thickness of ZnO nanowires array layer is 40 nm as a result of the largest change of SPR angle, for which the sensitivity is 210.75°/RIU.

(a)

(b)

Therefore, keeping all the results above into consideration, the optimized thickness is found to be 46 nm for Au, 15 nm for TiO₂, and 40 nm for ZnO, and the optimized layer number is found to be 1 for MoS₂ and 3 for GO, where the thickness is 1 × 0.65 nm for MoS₂ and 3 × 1.6 nm for TiO₂. The proposed SPR biosensor has a big shift of 16.86° and high sensitivity of 210.75°/RIU for the refractive index of the sensing medium from 1.30 to 1.38. The relationship between the SPR angle and the refractive index of the sensing medium is shown in Figure 7.

4. Conclusion

A novel SPR biosensor that can achieve a high sensitivity is proposed in this paper. The SPR biosensor with two nanowires array layers of ZnO and MoS₂ has TiO₂ nanolayer based on graphene oxide nanosheet; therefore, there is a great enhancement of sensitivity. The thickness of each medium for the structure designed is given. The sensitivity of the SPR biosensor is obtained, which can reach as high as 210.75°/RIU. Also, the sensitivity is greatly improved compared with the traditional SPR biosensor.

Data Availability

The data used to support the findings of this study in the manuscript are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

This work was supported by the Local Science and Technology Development Fund Projects guided by the Central Government, China (no. 206Z1703G).

References

H. Raether, Surface Plasmons on Smooth and Rough Surfaces and on Grating, Springer, Berlin, Germany, 1988.
J. Homola, S. S. Yee, and G. Gauglitz, “Surface plasmon resonance sensors: review,” Sensors and Actuators B: Chemical, vol. 54, no. 1-2, pp. 3–15, 1999.
View at: Publisher Site | Google Scholar
E. Kretschmann and H. Raether, “Notizen: radiative decay of non radiative surface plasmons excited by light,” Zeitschrift für Naturforschung A, vol. 23, no. 12, pp. 2135-2136, 1968.
View at: Publisher Site | Google Scholar
S. Shukla, M. Rani, N. K. Sharma, and V. Sajal, “Sensitivity enhancement of a surface plasmon resonance based fiber optic sensor utilizing platinum layer,” Optik, vol. 126, no. 23, pp. 4636–4639, 2015.
View at: Publisher Site | Google Scholar
P. T. Arasu, A. S. M. Noor, A. A. Shabaneh, M. H. Yaacob, H. N. Lim, and M. A. Mahdi, “Fiber Bragg grating assisted surface plasmon resonance sensor with graphene oxide sensing layer,” Optics Communications, vol. 380, pp. 260–266, 2016.
View at: Publisher Site | Google Scholar
V. P. Devanarayanan, V. Manjuladevi, and R. K. Gupta, “Surface plasmon resonance sensor based on a new opto-mechanical scanning mechanism,” Sensors and Actuators B: Chemical, vol. 227, pp. 643–648, 2016.
View at: Publisher Site | Google Scholar
J. Homola, “Surface plasmon resonance sensors for detection of chemical and biological species,” Chemical Reviews, vol. 108, no. 2, pp. 462–493, 2008.
View at: Publisher Site | Google Scholar
R. Karlsson, “SPR for molecular interaction analysis: a review of emerging application areas,” Journal of Molecular Recognition, vol. 17, no. 3, pp. 151–161, 2004.
View at: Publisher Site | Google Scholar
B. Liu, X. Liu, S. Shi et al., “Design and mechanisms of antifouling materials for surface plasmon resonance sensors,” Acta Biomaterialia, vol. 40, pp. 100–118, 2016.
View at: Publisher Site | Google Scholar
M. H. H. Hasib, J. N. Nur, C. Rizal, and K. N. Shushama, “Improved transition metal dichalcogenides-based surface plasmon resonance biosensors,” Condensed Matter, vol. 4, no. 2, p. 49, 2019.
View at: Publisher Site | Google Scholar
C. Rizal, S. Pisana, and I. Hrvoic, “Improved magneto-optic surface plasmon resonance biosensors,” Photonics, vol. 5, no. 3, p. 15, 2018.
View at: Publisher Site | Google Scholar
D. Regatos, B. Sepúlveda, D. Fariña, L. G. Carrascosa, and L. M. Lechuga, “Suitable combination of noble/ferromagnetic metal multilayers for enhanced magneto-plasmonic biosensing,” Optics Express, vol. 19, no. 9, pp. 8336–8346, 2011.
View at: Publisher Site | Google Scholar
A. Verma, A. Prakash, and R. Tripathi, “Sensitivity improvement of graphene based surface plasmon resonance biosensors with chaclogenide prism,” Optik, vol. 127, no. 4, pp. 1787–1791, 2016.
View at: Publisher Site | Google Scholar
L. Wu, H. S. Chu, W. S. Koh, and E. P. Li, “Highly sensitive graphene biosensors based on surface plasmon resonance,” Optics Express, vol. 18, no. 14, pp. 14395–14400, 2010.
View at: Publisher Site | Google Scholar
S. Zeng, S. Hu, J. Xia et al., “Graphene-MoS₂ hybrid nanostructures enhanced surface plasmon resonance biosensors,” Sensors and Actuators B: Chemical, vol. 207, pp. 801–810, 2015.
View at: Publisher Site | Google Scholar
R. Verma, B. D. Gupta, and R. Jha, “Sensitivity enhancement of a surface plasmon resonance based biomolecules sensor using graphene and silicon layers,” Sensors and Actuators B: Chemical, vol. 160, no. 1, pp. 623–631, 2011.
View at: Publisher Site | Google Scholar
Q. Ouyang, S. Zeng, X.-Q. Dinh, P. Coquet, and K.-T. Yong, “Sensitivity enhancement of MoS₂ nanosheet based surface plasmon resonance biosensor,” Procedia Engineering, vol. 140, pp. 134–139, 2016.
View at: Publisher Site | Google Scholar
B. Meshginqalam, M. T. Ahmadi, R. Ismail, and A. Sabatyan, “Graphene/graphene oxide-based ultrasensitive surface plasmon resonance biosensor,” Plasmonics, vol. 12, no. 6, pp. 1991–1997, 2017.
View at: Publisher Site | Google Scholar
J. Liu, “Adsorption of DNA onto gold nanoparticles and graphene oxide: surface science and applications,” Physical Chemistry Chemical Physics, vol. 14, no. 30, pp. 10485–10496, 2012.
View at: Publisher Site | Google Scholar
J. B. Maurya, Y. K. Prajapati, V. Singh, J. P. Saini, and R. Tripathi, “Performance of graphene-MoS₂ based surface plasmon resonance sensor using Silicon layer,” Optical and Quantum Electronics, vol. 47, no. 11, pp. 3599–3611, 2015.
View at: Publisher Site | Google Scholar
M. Mahanti and D. Basak, “Highly enhanced UV emission due to surface plasmon resonance in Ag-ZnO nanorods,” Chemical Physics Letters, vol. 542, pp. 110–116, 2012.
View at: Publisher Site | Google Scholar
S. Shukla, N. K. Sharma, and V. Sajal, “Sensitivity enhancement of a surface plasmon resonance based fiber optic sensor using ZnO thin film: a theoretical study,” Sensors and Actuators B: Chemical, vol. 206, pp. 463–470, 2015.
View at: Publisher Site | Google Scholar
R. Khan, P. Uthirakumar, K.-B. Bae, S.-J. Leem, and I.-H. Lee, “Localized surface plasmon enhanced photoluminescence of ZnO nanosheets by Au nanoparticles,” Materials Letters, vol. 163, pp. 8–11, 2016.
View at: Publisher Site | Google Scholar
J. H. Park, S. Kim, and A. J. Bard, “Novel carbon-doped TiO₂ nanotube arrays with high aspect ratios for efficient solar water splitting,” Nano Letters, vol. 6, no. 1, pp. 24–28, 2006.
View at: Publisher Site | Google Scholar
B.-H. Wu, W.-T. Liu, T.-Y. Chen, T.-P. Perng, J.-H. Huang, and L.-J. Chen, “Plasmon-enhanced photocatalytic hydrogen production on Au/TiO₂ hybrid nanocrystal arrays,” Nano Energy, vol. 27, pp. 412–419, 2016.
View at: Publisher Site | Google Scholar
A. Verma, A. Prakash, and R. Tripathi, “Performance analysis of graphene based surface plasmon resonance biosensors for detection of pseudomonas-like bacteria,” Optical and Quantum Electronics, vol. 47, no. 5, pp. 1197–1205, 2015.
View at: Publisher Site | Google Scholar

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Copyright © 2020 Shiliang Guo et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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International Journal of Optics

High-Sensitivity Biosensor-Based Enhanced SPR by ZnO/MoS2 Nanowires Array Layer with Graphene Oxide Nanosheet

Abstract

1. Introduction

2. Design Consideration and Theoretical Model

2.1. Design Consideration

2.2. Calculation Method

3. Results and Discussion

3.1. Thickness of Au, MoS2, and Graphene Oxide

3.2. Thickness of TiO2 and ZnO Layers

4. Conclusion

Data Availability

Conflicts of Interest

Acknowledgments

References

Copyright

High-Sensitivity Biosensor-Based Enhanced SPR by ZnO/MoS₂ Nanowires Array Layer with Graphene Oxide Nanosheet

3.1. Thickness of Au, MoS₂, and Graphene Oxide

3.2. Thickness of TiO₂ and ZnO Layers