Abstract:In this paper, a variety of 2D materials on the surface plasmon resonance sensor based on Al–Ni bimetallic layer are compared. Simulation results indicate that lateral position shift, which is calculated according to the real and imaginary parts of the refractive index of material, can be used as an effective parameter to optimize the sensitivity. By using the parameters for optimizing the SPR structures, the results show that the multiple layer models of Al(40 nm)–Ni(22 nm)–black phosphorus (BP)(1 L) and Al(4… Show more
“…The monolayer BP plane features two non-equivalent directions: armchair (ac) and zigzag (zz), as illustrated in Figure 1b,c. Drawing from prior experimental studies and the Cauchy absorption model [40][41][42][43][44][45], FLBP exhibits refractive indexes of n zz = 3.56 + 0.126i in the zz direction and n ac = 3.29 + 0.428i in the ac direction, which indicates significantly lower imaginary parts of the refractive index compared to bulk BP. Compared to typical metal oxides, e.g., TiO 2 (n TiO 2 = 1.977 + 0.05i) and ZnO (n ZnO = 1.71749 + 0.066i), though, the imaginary part of the refractive index of BP is not relatively small: the real part is larger.…”
Lossy mode resonance (LMR) sensors offer a promising avenue to surpass the constraints of conventional surface plasmon resonance (SPR) sensors by delivering enhanced label-free detection capabilities. A notable edge of LMR over SPR is its excitation potential by both transverse electric (TE) and transverse magnetic (TM) polarized light. Yet this merit remains underexplored due to challenges to achieving high sensing performance under both TM and TE polarization within a singular LMR model. This study introduces a theoretical model for an LMR prism refractive index sensor based on a MgF2-few layer black phosphorus-MgF2 configuration, which can achieve angular sensitivity nearing 90∘ refractive index unit−1 (RIU−1) for both polarizations. Leveraging the distinct anisotropic nature of black phosphorus, the figure of merit (FOM) values along its two principal crystal axes (zigzag and armchair) show great difference, achieving an impressive FOM of 1.178 × 106 RIU−1 along the zigzag direction under TE polarized light and 1.231 × 104 RIU−1 along the armchair direction under TM polarized light. We also provide an analysis of the electric field distribution for each configuration at its respective resonant conditions. The proposed structure paves the way for innovative applications of anisotropic-material-based LMR sensors in various applications.
“…The monolayer BP plane features two non-equivalent directions: armchair (ac) and zigzag (zz), as illustrated in Figure 1b,c. Drawing from prior experimental studies and the Cauchy absorption model [40][41][42][43][44][45], FLBP exhibits refractive indexes of n zz = 3.56 + 0.126i in the zz direction and n ac = 3.29 + 0.428i in the ac direction, which indicates significantly lower imaginary parts of the refractive index compared to bulk BP. Compared to typical metal oxides, e.g., TiO 2 (n TiO 2 = 1.977 + 0.05i) and ZnO (n ZnO = 1.71749 + 0.066i), though, the imaginary part of the refractive index of BP is not relatively small: the real part is larger.…”
Lossy mode resonance (LMR) sensors offer a promising avenue to surpass the constraints of conventional surface plasmon resonance (SPR) sensors by delivering enhanced label-free detection capabilities. A notable edge of LMR over SPR is its excitation potential by both transverse electric (TE) and transverse magnetic (TM) polarized light. Yet this merit remains underexplored due to challenges to achieving high sensing performance under both TM and TE polarization within a singular LMR model. This study introduces a theoretical model for an LMR prism refractive index sensor based on a MgF2-few layer black phosphorus-MgF2 configuration, which can achieve angular sensitivity nearing 90∘ refractive index unit−1 (RIU−1) for both polarizations. Leveraging the distinct anisotropic nature of black phosphorus, the figure of merit (FOM) values along its two principal crystal axes (zigzag and armchair) show great difference, achieving an impressive FOM of 1.178 × 106 RIU−1 along the zigzag direction under TE polarized light and 1.231 × 104 RIU−1 along the armchair direction under TM polarized light. We also provide an analysis of the electric field distribution for each configuration at its respective resonant conditions. The proposed structure paves the way for innovative applications of anisotropic-material-based LMR sensors in various applications.
“…Therefore, SPR sensing technology has been widely used in biochemical analysis [ 22 ], food safety [ 23 ], medical diagnosis [ 24 ] and other fields with remarkable effects, such as the detection of staphylococcal enterotoxin in milk [ 25 ], drug residue detection [ 26 , 27 ], real-time disease diagnosis [ 28 ], gas detection [ 29 ], etc. However, the traditional SPR structure usually uses Otto structure or Kretschmann–Raether (KR) structure based on noble metals (such as Au [ 30 ], Ag [ 31 ], Al [ 32 ], etc.) to excite SPR.…”
In this paper, we study the sensitivity-tunable terahertz (THz) liquid/gas biosensor in a coupling prism–three-dimensional Dirac semimetal (3D DSM) multilayer structure. The high sensitivity of the biosensor originates from the sharp reflected peak caused by surface plasmon resonance (SPR) mode. This structure achieves the tunability of sensitivity due to the fact that the reflectance could be modulated by the Fermi energy of 3D DSM. Besides, it is found that the sensitivity curve depends heavily on the structural parameters of 3D DSM. After parameter optimization, we obtained sensitivity over 100°/RIU for liquid biosensor. We believe this simple structure provides a reference idea for realizing high sensitivity and a tunable biosensor device.
“…Recently, two-dimensional nanomaterials have received much attention due to their unique properties. The presence of these materials improves the incident light energy transferring to SPP and leads to an increase in the sensitivity of the sensor [19,20]. Also, the stable chemical properties of these materials protect the internal chemical unstable structure of the SPR sensor [19].…”
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confidence: 99%
“…The presence of these materials improves the incident light energy transferring to SPP and leads to an increase in the sensitivity of the sensor [19,20]. Also, the stable chemical properties of these materials protect the internal chemical unstable structure of the SPR sensor [19]. In the present work, we investigate the performance of the sensor using black phosphorus (BP) and Tungsten Disulfide (WS 2 ).…”
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confidence: 99%
“…These also protect the metal layer from oxidation because oxygen atoms cannot pass through these materials. So far, many works using these two-dimensional nanomaterials have been reported [19,28,29,33]. In this paper, we try to design a biosensor with a simple design and suitable performance characteristics by using two-dimensional materials, which can be easily and cheaply manufactured.…”
The authors theoretically designed a highly sensitive SPR biosensor with a hybrid structure using two‐dimensional nanomaterials (BP‐WS2). Using the transfer matrix method (TMM), the performance of the sensor in terms of reflection, sensitivity, detection accuracy, and quality factor is investigated, and by changing the structural parameters of the sensor, the obtained results are further analysed so that an optimal structure with optimal performance can be achieved. The sensor was optimised with four layers of BP and a single layer of WS2. This composite structure is placed on a 50 nm thick gold layer and concluded with a maximum sensitivity of 234 deg/RIU with a FOM of 26.53 RIU−1. This biosensor is designed by considering the advantages and characteristics of biosensors in their resistance and high electrical properties, as well as the ability to detect diseases quickly.
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