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transfer matrix method coded in a commercial software  (MathWorks Inc)


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    MathWorks Inc transfer matrix method coded in a commercial software
    Transfer Matrix Method Coded In A Commercial Software, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/transfer-matrix+code/pm31144506-106-11-19
    Average 90 stars, based on 1 article reviews
    transfer matrix method coded in a commercial software - by Bioz Stars, 2026-09
    90/100 stars

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    Article Title: High Sensitivity One-Dimensional Photonic Crystal Sensor Design for Waterborne Bacteria Detection
    Article Snippet: This paper introduces an advanced optical biosensor designed for the highly sensitive detection of waterborne bacteria.. The proposed biosensor relies on a Ge/LiF multilayer photonic crystal with a central defect layer, showcasing an innovative approach to improve sensitivity.. The introduction of different water samples into the defect layer disrupts the photonic crystal’s symmetry, resulting in a unique resonant peak within the photonic band gap.

    Article Title: Effect of BaTiO3 and Chitosan Composite Material on the Enhancement of the Sensitivity and Limit of Detection of the Surface Plasmon Resonance Sensor-Divergent Beam Based
    Article Snippet: The results were realized by using transfer matrix method with help of MATLAB software [2].

    Article Title: Spectral tuning of Bloch Surface Wave resonances by light-controlled optical anisotropy
    Article Snippet: The angular-dependent spectral reflectivity map of the planar 1DPC is calculated by means of a MATLAB implementation of the transfer matrix method.

    Article Title: Tunable GH shift based on hyperbolic metamaterials composed of graphene and dielectric.
    Article Snippet: In Fig. 6b, the electric field distribution in the structure is simulated by the transfer matrix method with the MATLAB software.

    Article Title: Differential Evolution Particle Swarm Optimization for Phase-Sensitivity Enhancement of Surface Plasmon Resonance Gas Sensor Based on MXene and Blue Phosphorene/Transition Metal Dichalcogenide Hybrid Structure.
    Article Snippet: In this work, a high-phase-sensitivity SPR sensor based on a Ag-BlueP/TMDCs-AgMXene hybrid structure is designed and numerically investigated using MATLAB software (R2021a), based on differential evolution particle swarm optimization and the transfer matrix method with the Fresnel equation for the detection of various gases.

    Article Title: Semitransparent Organic Solar Cells with Homogeneous Transmission and Colorful Reflection Enabled by an ITO-Free Microcavity Architecture.
    Article Snippet: Semitransparent organic photovoltaics (ST-OPVs), owing to the merits of high power generation, thermal insulation, and aesthetic features, have become a promising candidate for intellectual buildingintegrated photovoltaic windows.. However, the traditional optical evaluation only focuses on the transmission properties and ignores the reflection behaviors.. And the lack of quantitative descriptions for array appearance hinders implementation of ST-OPV based large-area modules.

    Refractive Index:

    Article Title: Tunable Exciton-Driven Photoelasticity in 2D Material Acoustic Cavities
    Article Snippet: .. To calculate the strain-induced, probe-wavelength-dependent modulation of reflectivity based on equation (3) a transfer matrix method was used (Matlab jreftran).5 The initial (“unperturbed”) values of the refractive index for TMD layers were obtained for both the real n(λ) and imaginary κ(λ) parts of the refractive index from Munkbhat et al.6 To account for thermal effects the n, κ values assigned to a heated film were calculated as an interpolation of the “unperturbed” dispersion curves taken at wavelength probe+BGR. ..

    Dispersion:

    Article Title: Tunable Exciton-Driven Photoelasticity in 2D Material Acoustic Cavities
    Article Snippet: .. To calculate the strain-induced, probe-wavelength-dependent modulation of reflectivity based on equation (3) a transfer matrix method was used (Matlab jreftran).5 The initial (“unperturbed”) values of the refractive index for TMD layers were obtained for both the real n(λ) and imaginary κ(λ) parts of the refractive index from Munkbhat et al.6 To account for thermal effects the n, κ values assigned to a heated film were calculated as an interpolation of the “unperturbed” dispersion curves taken at wavelength probe+BGR. ..



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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method <t>(TMM)</t> calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.
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    (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method (TMM) calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.

    Journal: ACS Applied Materials & Interfaces

    Article Title: Low-Temperature Stability and Sensing Performance of Mid-Infrared Bloch Surface Waves on a One-Dimensional Photonic Crystal

    doi: 10.1021/acsami.2c07894

    Figure Lengend Snippet: (a) Sketch of the Kretschmann–Raether configuration. The prism is quoted and the radiation wavevector k has been decomposed in its parallel, β , and perpendicular, k x , components. (b) Scanning electron microscopy (SEM) image of the focused ion beam (FIB) milled cross-section of the deposited 1D-PC and a sketch of the transverse geometry with measured layer thicknesses. (c) R (θ,λ) reflectance map according to the transfer-matrix method (TMM) calculation for σ polarization. The black and red lines are the photonic band edges (BEs), calculated for the infinitely extended 1D-PC. The surface waves (SWs) and the band-edge (BE) modes appear as dark reflectance lines. In the insets, we plot the square modulus of the electric fields of the modes, superimposed on the 1D-PC refractive index distribution. The external medium is vacuum.

    Article Snippet: Based on the real 1D-PC geometry and materials’ optical properties, the room temperature numerical simulation of the reflectance R (θ,λ) was carried out by a proprietary transfer-matrix method (TMM) MATLAB code.

    Techniques: Electron Microscopy, Refractive Index