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matlab-based transfer matrix code  (MathWorks Inc)


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    MathWorks Inc matlab-based transfer matrix code
    Matlab Based Transfer Matrix Code, 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/pm38768370__jz4c01120_si_001-27-10-10
    Average 90 stars, based on 1 article reviews
    matlab-based transfer matrix code - by Bioz Stars, 2026-10
    90/100 stars

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    Related Articles

    Transmission Assay:

    Article Title: Dynamic Color Generation with Electrically Tunable Thin Film Optical Coatings.
    Article Snippet: .. Reflection, transmission, and absorption spectra were simulated using transfer matrix method code written in MATLAB. ..

    other:

    Article Title: Photovoltaic devices and methods
    Article Snippet: The active layer thickness was estimated by using the MATLAB™ code (Burkhard, G. F.; Hoke, E. T. Transfer Matrix Optical Modeling.

    Article Title: Assessing the Determinants of Cavity Polariton Relaxation Using Angle-Resolved Photoluminescence Excitation Spectroscopy.
    Article Snippet: The thickness of the active layer was determined using a MATLAB-based transfer matrix code to achieve a 50 meV red detuning from the Soret resonances, crucial for resolving the anti-crossing behavior of cavity polaritons.

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

    Article Title: Wide-Angle Tunable Critical Coupling in Nanophotonic Optical Coatings with Low-Loss Phase Change Material.
    Article Snippet: K. V. Sreekanth, J. Teng Institute of Materials Research and Engineering Agency for Science, Technology and Research (A*STAR) 2 Fusionopolis Way, Singapore 138634, Singapore E-mail: sreekanth@imre.a-star.edu.sg; jh-teng@imre.a-star.edu.sg P. Prabhathan, Y. Lekina, S. Zexiang, R. Singh Division of Physics and Applied Physics School of Physical and Mathematical Sciences Nanyang Technological University Singapore 637371, Singapore E-mail: ranjans@ntu.edu.sg P. Prabhathan, Y. Lekina, S. Zexiang, R. Singh Centre for Disruptive Photonic Technologies The Photonics Institute Nanyang Technological University Singapore 637371, Singapore A. Chaturvedi, E. H. Tong Teo School of Materials Science and Engineering Nanyang Technological University Singapore 639798, Singapore S. Han ZJU-Hangzhou Global Science and Technology Innovation Center Key Laboratory of Advanced Micro/Nano Electronic Devices & Smart Systems of Zhejiang Zhejiang University Hangzhou 311200, China E. H. Tong Teo School of Electrical and Electronics Engineering Nanyang Technological University 50, Nanyang Avenue, Singapore 639798, Singapore

    Derivative Assay:

    Article Title: High-Performance Planar Thin Film Thermochromic Window via Dynamic Optical Impedance Matching
    Article Snippet: .. Simulations of multilayer transmittance and reflectance were performed using a transfer matrix code written in MATLAB, with material properties for each material derived from ellipsometry. ..



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