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Symmetry, Volume 15, Issue 3 (March 2023) – 214 articles

Cover Story (view full-size image): The intriguing strange metal behavior, characterized by a linear dependence of the electrical resistivity on the temperature, is observed in a variety of systems and remains an unsolved mystery. In the last years, we were led to attribute this behavior to the scattering of electrons on slow bosons. Recent resonant x-ray scattering experiments on cuprates unambiguously detected a good candidate for the slow boson in the form of dynamical short-ranged charge density fluctuations. To extend the strange metal behavior down to very low temperature, the characteristic relaxation time of these fluctuations must grow large, and in this work we propose a possible mechanism that triggers this growth, due to the interplay of charge density fluctuations and long-wavelength diffusive charge collective modes. View this paper
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18 pages, 1527 KiB  
Article
Multiple-Attribute Decision Making Based on Intuitionistic Hesitant Fuzzy Connection Set Environment
by Wajid Ali, Tanzeela Shaheen, Iftikhar Ul Haq, Hamza Ghazanfar Toor, Faraz Akram, Saeid Jafari, Md. Zia Uddin and Mohammad Mehedi Hassan
Symmetry 2023, 15(3), 778; https://doi.org/10.3390/sym15030778 - 22 Mar 2023
Cited by 17 | Viewed by 2639
Abstract
The intuitionistic hesitant fuzzy set (IHFS) is an enriched version of hesitant fuzzy sets (HFSs) that can cover both fuzzy sets (FSs) and intuitionistic fuzzy sets (IFSs). By assigning membership and non-membership grades as subsets of [0, 1], the IHFS can model and [...] Read more.
The intuitionistic hesitant fuzzy set (IHFS) is an enriched version of hesitant fuzzy sets (HFSs) that can cover both fuzzy sets (FSs) and intuitionistic fuzzy sets (IFSs). By assigning membership and non-membership grades as subsets of [0, 1], the IHFS can model and handle situations more proficiently. Another related theory is the theory of set pair analysis (SPA), which considers both certainties and uncertainties as a cohesive system and represents them from three aspects: identity, discrepancy, and contrary. In this article, we explore the suitability of combining the IHFS and SPA theories in multi-attribute decision making (MADM) and present the hybrid model named intuitionistic hesitant fuzzy connection number set (IHCS). To facilitate the design of a novel MADM algorithm, we first develop several averaging and geometric aggregation operators on IHCS. Finally, we highlight the benefits of our proposed work, including a comparative examination of the recommended models with a few current models to demonstrate the practicality of an ideal decision in practice. Additionally, we provide a graphical interpretation of the devised attempt to exhibit the consistency and efficiency of our approach. Full article
(This article belongs to the Special Issue Research on Fuzzy Logic and Mathematics with Applications II)
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<p>Flow chart of the manuscript.</p>
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<p>Graphical illustration of the developed and existing operator. Tahir et al. [<a href="#B35-symmetry-15-00778" class="html-bibr">35</a>].</p>
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22 pages, 377 KiB  
Article
Behavior as t → ∞ of Solutions of a Mixed Problem for a Hyperbolic Equation with Periodic Coefficients on the Semi-Axis
by Hovik A. Matevossian and Vladimir Yu. Smirnov
Symmetry 2023, 15(3), 777; https://doi.org/10.3390/sym15030777 - 22 Mar 2023
Cited by 5 | Viewed by 1351
Abstract
In this paper, we consider the asymptotic behavior (as t) of solutions as an initial boundary value problem for a second-order hyperbolic equation with periodic coefficients on the semi-axis (x>0). The main approach to studying the [...] Read more.
In this paper, we consider the asymptotic behavior (as t) of solutions as an initial boundary value problem for a second-order hyperbolic equation with periodic coefficients on the semi-axis (x>0). The main approach to studying the problem under consideration is based on the spectral theory of differential operators, as well as on the properties of the spectrum (σ(H0)) of the one-dimensional Schrödinger operator H0 with periodic coefficients p(x) and q(x). Full article
(This article belongs to the Section Physics)
26 pages, 1417 KiB  
Article
Topology and Emergent Symmetries in Dense Compact Star Matter
by Yong-Liang Ma and Wen-Cong Yang
Symmetry 2023, 15(3), 776; https://doi.org/10.3390/sym15030776 - 22 Mar 2023
Cited by 6 | Viewed by 1916
Abstract
It has been found that the topology effect and the possible emergent hidden scale and hidden local flavor symmetries at high density reveal a novel structure of compact star matter. When Nf2, baryons can be described by skyrmions when [...] Read more.
It has been found that the topology effect and the possible emergent hidden scale and hidden local flavor symmetries at high density reveal a novel structure of compact star matter. When Nf2, baryons can be described by skyrmions when the number of color Nc is regarded as a large parameter and there is a robust topology change—the transition from skyrmion to half-skyrmion—in the skyrmion matter approach to dense nuclear matter. The hidden scale and local flavor symmetries, which are sources introducing the scalar meson and vector mesons, are significant elements for understanding the nuclear force in nonlinear chiral effective theories. We review in this paper how the robust conclusions from the topology approach to dense matter and emergent hidden scale and hidden local flavor symmetries figure in generalized nuclear effective field theory (GnEFT), which is applicable to nuclear matter from low density to compact star density. The topology change encoded in the parameters of the effective field theory is interpreted as the hadron-quark continuity in the sense of the Cheshire Cat Principle. A novel feature predicted in this theory that has not been found before is the precocious appearance of the conformal sound velocity in the cores of massive stars, although the trace of the energy-momentum tensor of the system is not zero. That is, there is a pseudoconformal structure in the compact star matter and, in contrast to the usual picture, the matter is made of colorless quasiparticles of fractional baryon charges. A possible resolution of the longstanding gA quench problem in nuclei transition and the compatibility of the predictions of the GnEFT with the global properties of neutron star and the data from gravitational wave detections are also discussed. Full article
(This article belongs to the Special Issue Symmetries and Ultra Dense Matter of Compact Stars)
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<p>The distribution of the baryon number density (the blue areas) in the skyrmion (<b>left panel</b>) matter and half-skyrmion matter (<b>right panel</b>). The crystal size 2 <span class="html-italic">L</span> is denoted by the blue quare.</p>
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<p>Typical results of the medium modified <math display="inline"><semantics> <msubsup> <mi>f</mi> <mi>π</mi> <mo>*</mo> </msubsup> </semantics></math> and <math display="inline"><semantics> <msubsup> <mi>m</mi> <mi>N</mi> <mo>*</mo> </msubsup> </semantics></math> vs. lattice size <span class="html-italic">L</span> calculated from the FCC crystal by using the HLS up to the next leading order including the Wess–Zumino terms [<a href="#B84-symmetry-15-00776" class="html-bibr">84</a>]. The vertical line denotes the location of the normal nuclear matter density in the FCC crystal.</p>
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<p>Chiral bag (annulus) in <math display="inline"><semantics> <mrow> <mo>(</mo> <mn>1</mn> <mo>+</mo> <mn>2</mn> <mo>)</mo> </mrow> </semantics></math>-dimension surrounding a QH droplet (green sheet) [<a href="#B96-symmetry-15-00776" class="html-bibr">96</a>].</p>
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<p>Sound velocity for <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mi>VM</mi> </msub> <mo>=</mo> <mn>6.75</mn> <mspace width="3.33333pt"/> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> (<b>upper panel</b>) and <math display="inline"><semantics> <mrow> <mn>20</mn> <mspace width="3.33333pt"/> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> (<b>lower panel</b>) for neutron matter (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>) and symmetric matter (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>), both computed in <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>l</mi> <mi>o</mi> <mi>w</mi> <mi>k</mi> </mrow> </msub> </semantics></math> RG with <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </msub> <mo>=</mo> <mn>2.5</mn> <mspace width="3.33333pt"/> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> [<a href="#B77-symmetry-15-00776" class="html-bibr">77</a>].</p>
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<p>The density dependence of <math display="inline"><semantics> <mrow> <mo>〈</mo> <msubsup> <mi>θ</mi> <mi>μ</mi> <mi>μ</mi> </msubsup> <mo>〉</mo> </mrow> </semantics></math> (<b>upper panel</b>) and <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> (<b>lower panel</b>) for <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> (nuclear matter) and <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> (neutron matter) in <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>l</mi> <mi>o</mi> <mi>w</mi> <mi>k</mi> </mrow> </msub> </semantics></math> RG for <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </msub> <mo>=</mo> <mn>2</mn> <mspace width="3.33333pt"/> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mi>VM</mi> </msub> <mo>=</mo> <mn>25</mn> <mspace width="3.33333pt"/> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> [<a href="#B5-symmetry-15-00776" class="html-bibr">5</a>].</p>
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<p>The polytropic index <math display="inline"><semantics> <mrow> <mi>γ</mi> <mo>=</mo> <mrow> <mi>d</mi> <mo form="prefix">ln</mo> <mi>P</mi> </mrow> <mo>/</mo> <mrow> <mi>d</mi> <mo form="prefix">ln</mo> <mi>ϵ</mi> </mrow> </mrow> </semantics></math> as a function of density in neutron matter from the pseudo-conformal model with typical value <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </msub> <mo>=</mo> <mn>2.5</mn> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> [<a href="#B14-symmetry-15-00776" class="html-bibr">14</a>].</p>
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<p>Comparison of <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>P</mi> <mo>/</mo> <mi>ϵ</mi> <mo>)</mo> </mrow> </semantics></math> between the PCM velocity (red line) and the band generated with the sound velocity interpolation method used in [<a href="#B116-symmetry-15-00776" class="html-bibr">116</a>]. The location of the topology change is denoted by the dash-dotted line.</p>
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<p>Density dependence of the sound velocity in neutron matter with different <math display="inline"><semantics> <msub> <mi>n</mi> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </msub> </semantics></math> [<a href="#B5-symmetry-15-00776" class="html-bibr">5</a>].</p>
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<p>Comparision of the density dependence of the pressure for neutron matter (<math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>) with the available experimental bound (shaded) given in [<a href="#B122-symmetry-15-00776" class="html-bibr">122</a>]. The bound at <math display="inline"><semantics> <mrow> <mn>6</mn> <msub> <mi>n</mi> <mn>0</mn> </msub> </mrow> </semantics></math> is indicated by the blue band.</p>
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<p>M-R relation from PCM with observed mass of pulsar J0348 + 0432 [<a href="#B124-symmetry-15-00776" class="html-bibr">124</a>] and radius constraints [<a href="#B126-symmetry-15-00776" class="html-bibr">126</a>,<a href="#B127-symmetry-15-00776" class="html-bibr">127</a>] from NICER [<a href="#B77-symmetry-15-00776" class="html-bibr">77</a>].</p>
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<p>Tidal deformabilities <math display="inline"><semantics> <msub> <mo>Λ</mo> <mn>1</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mo>Λ</mo> <mn>2</mn> </msub> </semantics></math> of the components of the binary neutron star system GW170817 with chirp mass <math display="inline"><semantics> <mrow> <mn>1.188</mn> <msub> <mi>M</mi> <mo>⊙</mo> </msub> </mrow> </semantics></math> [<a href="#B5-symmetry-15-00776" class="html-bibr">5</a>]. The constraint from GW170817 at the 90% probability contour and the result from “FSUGarnet (0.16)” [<a href="#B128-symmetry-15-00776" class="html-bibr">128</a>] are also quoted for reference.</p>
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16 pages, 3196 KiB  
Article
Influence of Asymmetric Agglomerations Effects over the Photothermal Release of Liposome-Encapsulated Nanodiamonds Assisted by Opto-Mechanical Changes
by Samuel Morales-Bonilla, Isaac I. Mota-Díaz, Janna Douda, Ariel Fuerte-Hernández, Juan Pablo Campos-López and Carlos Torres-Torres
Symmetry 2023, 15(3), 775; https://doi.org/10.3390/sym15030775 - 22 Mar 2023
Cited by 2 | Viewed by 1513
Abstract
An analysis of optical effects exhibited by blood plasma under healthy/unhealthy conditions, and of the penetrating evolution of nanovehicles conformed by nanodiamonds (NDs) encapsulating liposomes (L) within these biofluids, is presented. Optical ablation of liposome clusters was actuated and controlled by a standard [...] Read more.
An analysis of optical effects exhibited by blood plasma under healthy/unhealthy conditions, and of the penetrating evolution of nanovehicles conformed by nanodiamonds (NDs) encapsulating liposomes (L) within these biofluids, is presented. Optical ablation of liposome clusters was actuated and controlled by a standard two-wave mixing (λ = 532 nm, τp = 4 ns) laser light method. Radiant time exposure effects (30 min) and threshold laser energy parameters (250 mJ/cm2 numerical; 181 mJ/cm2 experimental) necessary to release NDs were identified and confirmed with similar experiments in the literature. Interactions during the sedimentation process between nanovehicles and the laser beams barrier were considered as the principal thermal damage process to achieve the release and transportation of drugs within these static fluids. The mechanical response during the release of NDs focuses on the temperature propagation, dynamic effects of nanovehicles associated with the diffusion coefficient, and some agglomeration effects. The principal findings of this research concern the threshold temperature (51.85 °C) of liposomes for the release of NDs with respect to that typically quoted in the literature (40–70 °C) for pure liposomes. The assessment of the release of NDs focuses on the numerical magnitude of Quantum Yield. Furthermore, the optical contrast enhancement was associated with NDs size agglomerations and the healthy/unhealthy conditions of fluids. This research aims to be a first proof approximation for delivery and transportation approaches to guide and interpret outcomes when combined with the vectorial nature basis of laser light and further effects once the cargo is retained in the fluids. Full article
(This article belongs to the Special Issue Asymmetric and Symmetric Studies on Applied Physics)
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<p>Experimental setup utilized for performing the laser light propagation by a TWM configuration in the samples studied.</p>
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<p>Representative TEM images: (<b>a</b>) agglomerated NDs encapsulated in liposomes; (<b>b</b>) typical view of pure liposomes; (<b>c</b>) typical evolution of liposomes with a trend of agglomeration.</p>
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<p>(<b>a</b>) Absorption coefficient in Samples A, B, and C; (<b>b</b>) transmittance properties; (<b>c</b>) integrated fluence as function of laser beam diameter and maximum pulse energy; (<b>d</b>) integrated fluence as function of wavelength (<span class="html-italic">λ</span>) and time exposure (<span class="html-italic">t</span>).</p>
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<p>(<b>a</b>) Amount of nanovehicles accumulated; (<b>b</b>) diffusion coefficient upon irradiation as a function of viscosity of the samples for different temperatures; (<b>c</b>) temperature distribution at <span class="html-italic">t</span> = 30 min; (<b>d</b>) ablation threshold as a function of cluster size.</p>
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26 pages, 534 KiB  
Review
Sensitivity of Quantum-Enhanced Interferometers
by Dariya Salykina and Farid Khalili
Symmetry 2023, 15(3), 774; https://doi.org/10.3390/sym15030774 - 22 Mar 2023
Cited by 3 | Viewed by 2059
Abstract
We review various schemes of quantum-enhanced optical interferometers, both linear (SU(2)) and non-linear (SU(1,1)) ones, as well as hybrid SU(2)/SU(1,1) options, using the unified modular approach based on the Quantum Cramèr–Rao bound (QCRB), and taking into account the practical limitations pertinent to all [...] Read more.
We review various schemes of quantum-enhanced optical interferometers, both linear (SU(2)) and non-linear (SU(1,1)) ones, as well as hybrid SU(2)/SU(1,1) options, using the unified modular approach based on the Quantum Cramèr–Rao bound (QCRB), and taking into account the practical limitations pertinent to all real-world highly-sensitive interferometers. We focus on three important cases defined by the interferometer symmetry: (i) the asymmetric single-arm interferometer; (ii) the symmetric two-arm interferometer with the antisymmetric phase shifts in the arms; and (iii) the symmetric two-arm interferometer with the symmetric phase shifts in the arms. We show that while the optimal regimes for these cases differ significantly, their QCRBs asymptotically correspond to the same squeezing-enhanced shot noise limit (2), which first appeared in the pioneering work by C. Caves in 1981.We show also that in all considered cases the QCRB can be asymptotically saturated by the standard (direct or homodyne) detection schemes. Full article
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<p>Michelson (<b>a</b>) and Mach–Zehnder (<b>b</b>) interferometers.</p>
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<p>Single-arm (<b>a</b>) and two-arm (<b>b</b>) SU(1,1) interferometers. DOPA 1,2: degenerate optical parametric amplifiers; NOPA: nondegenerate optical parametric amplifiers.</p>
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<p>Conceptual schemes of the single-arm (<b>a</b>) and two-arm (<b>b</b>) interferometers. <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mi>ψ</mi> <mo stretchy="false">〉</mo> </mrow> </semantics></math>: single- or two-mode quantum state of the probing light.</p>
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<p>Single-arm SU(2) (<b>a</b>) and SU(1,1) (<b>b</b>) interferometers. BS: beamsplitters; DOPA: degenerate optical parametric amplifiers; Det: detectors. The part, common for both schemes, is enclosed into the dashed rectangle and labeled as “QCRB”.</p>
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<p>Preparation options for the two-arm interferometer shown in <a href="#symmetry-15-00774-f003" class="html-fig">Figure 3</a>b. (<b>a</b>): SU(2) interferometer; (<b>b</b>): SU(1,1) interferometer. BS 1: beamsplitters; DOPA 1,2: degenerate optical parametric amplifiers; NOPA: non-degenerate optical parametric amplifier.</p>
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<p>Measurement options for the two-arm interferometer shown in <a href="#symmetry-15-00774-f003" class="html-fig">Figure 3</a>b. (<b>a</b>): Double homodyne detection; (<b>b</b>): double direct detection; (<b>c</b>): SU(1,1) type measurement. BS 2: beamsplitter; NOPA 2: non-degenerate optical parametric amplifier; HD 1,2: homodyne detectors; Det 1,2: detectors; “opt” means the optimally weighted sum of the two outputs.</p>
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12 pages, 304 KiB  
Article
Application of Fixed-Point Results to Integral Equation through F-Khan Contraction
by Arul Joseph Gnanaprakasam, Gunaseelan Mani, Rajagopalan Ramaswamy, Ola A. Ashour Abdelnaby, Khizar Hyatt Khan and Stojan Radenović
Symmetry 2023, 15(3), 773; https://doi.org/10.3390/sym15030773 - 22 Mar 2023
Cited by 1 | Viewed by 1516
Abstract
In this article, we establish fixed point results by defining the concept of F-Khan contraction of an orthogonal set by modifying the symmetry of usual contractive conditions. We also provide illustrative examples to support our results. The derived results have been applied [...] Read more.
In this article, we establish fixed point results by defining the concept of F-Khan contraction of an orthogonal set by modifying the symmetry of usual contractive conditions. We also provide illustrative examples to support our results. The derived results have been applied to find analytical solutions to integral equations. The analytical solutions are verified with numerical simulation. Full article
(This article belongs to the Special Issue Symmetries in Differential Equation and Application)
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<p>Graph of approximation (m = 64) compared to exact solution (h = 0.1).</p>
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<p>Graph of approximation (m = 128) compared to exact solution with h = 0.1.</p>
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<p>Comparison of approximation and exact solution with h = 0.1.</p>
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13 pages, 3526 KiB  
Article
Numerical Simulation of the Effects of Reduced Gravity, Radiation and Magnetic Field on Heat Transfer Past a Solid Sphere Using Finite Difference Method
by Amir Abbas, Muhammad Ashraf, Ioannis E. Sarris, Kaouther Ghachem, Taher Labidi, Lioua Kolsi and Hafeez Ahmad
Symmetry 2023, 15(3), 772; https://doi.org/10.3390/sym15030772 - 22 Mar 2023
Cited by 14 | Viewed by 1618
Abstract
The current study deals with the reduced gravity and radiation effects on the magnetohydrodynamic natural convection past a solid sphere. The studied configuration is modeled using coupled and nonlinear partial differential equations. The obtained model is transformed to dimensionless form using suitable scaling [...] Read more.
The current study deals with the reduced gravity and radiation effects on the magnetohydrodynamic natural convection past a solid sphere. The studied configuration is modeled using coupled and nonlinear partial differential equations. The obtained model is transformed to dimensionless form using suitable scaling variables. The finite difference method is adopted to solve the governing equation and determine the velocity and temperature profiles in addition to the skin friction coefficient and Nusselt number. Furthermore, graphic and tabular presentations of the results are made. The verification of the numerical model is performed by comparing with results presented in the literature and a good concordance is encountered. The main objective of this investigation is to study the effect of the buoyancy force caused by the density variation on natural convective heat transfer past a solid sphere. The results show that the velocity increases with the reduced gravity parameter and solar radiation but decreases with Prandtl number and magnetic field parameter. It is also found that the temperature increases the with solar radiation and magnetic field but decreases with the reduced gravity parameter and Prandtl number. Full article
(This article belongs to the Special Issue Advances in Heat and Mass Transfer with Symmetry)
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<p>Flow Geometry and Coordinate System.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>θ</mi> </semantics></math> for <span class="html-italic">Pr</span> = 7.0,<math display="inline"><semantics> <mrow> <mo> </mo> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>U</mi> </semantics></math> for <span class="html-italic">Pr</span> = 7.0, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>U</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> = 10.0, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>θ</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> = 10.0, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>U</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> <mo>=</mo> </mrow> </semantics></math> 10.0, <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> <mo>=</mo> <mn>7.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> </mrow> </semantics></math> on <math display="inline"><semantics> <mi>θ</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> = 10.0, <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> <mo>=</mo> <mn>7.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mi>M</mi> </semantics></math> on <math display="inline"><semantics> <mi>U</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> = 5.0, <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> <mo>=</mo> <mn>7.0</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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<p>Effect of <math display="inline"><semantics> <mi>M</mi> </semantics></math> on <math display="inline"><semantics> <mi>θ</mi> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>g</mi> </mrow> </semantics></math> = 5.0, <math display="inline"><semantics> <mrow> <mi>P</mi> <mi>r</mi> <mo>=</mo> <mn>7.0</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>d</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <mi>M</mi> <mo>=</mo> <mn>1.0</mn> </mrow> </semantics></math>.</p>
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15 pages, 7820 KiB  
Article
Cross-Correlation Fusion Graph Convolution-Based Object Tracking
by Liuyi Fan, Wei Chen and Xiaoyan Jiang
Symmetry 2023, 15(3), 771; https://doi.org/10.3390/sym15030771 - 21 Mar 2023
Cited by 1 | Viewed by 2014
Abstract
Most popular graph attention networks treat pixels of a feature map as individual nodes, which makes the feature embedding extracted by the graph convolution lack the integrity of the object. Moreover, matching between a template graph and a search graph using only part-level [...] Read more.
Most popular graph attention networks treat pixels of a feature map as individual nodes, which makes the feature embedding extracted by the graph convolution lack the integrity of the object. Moreover, matching between a template graph and a search graph using only part-level information usually causes tracking errors, especially in occlusion and similarity situations. To address these problems, we propose a novel end-to-end graph attention tracking framework that has high symmetry, combining traditional cross-correlation operations directly. By utilizing cross-correlation operations, we effectively compensate for the dispersion of graph nodes and enhance the representation of features. Additionally, our graph attention fusion model performs both part-to-part matching and global matching, allowing for more accurate information embedding in the template and search regions. Furthermore, we optimize the information embedding between the template and search branches to achieve better single-object tracking results, particularly in occlusion and similarity scenarios. The flexibility of graph nodes and the comprehensiveness of information embedding have brought significant performance improvements in our framework. Extensive experiments on three challenging public datasets (LaSOT, GOT-10k, and VOT2016) show that our tracker outperforms other state-of-the-art trackers. Full article
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<p>Of our CFGC with SiamGAT on the challenging sequences from LaSOT. The baseline SiamGAT (in blue) only uses local information, while our CFGC (in red) has both local and global information in nodes. Based on the same template image and search image, our CFGC obtains a more accurate response map and tracking results. Please zoom in for a better view.</p>
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<p>Overview of our proposed method. The architecture of the proposed CFGC, which consists of three core modules: a Siamese network, a cross-correlation layer, and a graph attention fusion model.</p>
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<p>(<b>a</b>) is graph attention part. (<b>b</b>) is an attention by node 1 on its neighborhood. The aggregated features are <math display="inline"><semantics> <msubsup> <mover accent="true"> <mi>h</mi> <mo stretchy="false">→</mo> </mover> <mrow> <mn>1</mn> </mrow> <msup> <mrow/> <mo>′</mo> </msup> </msubsup> </semantics></math>.</p>
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<p>The architecture of GAF model, which combines graph attention network with cross-correlation feature. The representation of each search node is reconstructed by template target nodes with attention mechanism. Then, it fuses the cross-correlation similarity map. The final new node is fed into the tracking head for target location prediction.</p>
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<p>Comparison with the state-of-the-art trackers on the LaSOT dataset in terms of the normalized precision and precision plots of OPE.</p>
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<p>Comparison with the state-of-the-art trackers on the LaSOT dataset in terms of success plot of OPE including all attributes and three individual attributes.</p>
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<p>Comparison of our CFGC with state-of-the-art trackers on the four challenging sequences from LaSOT. (<b>a</b>): Motorcycle-3, (<b>b</b>): Pool-7, (<b>c</b>): Elephant-12, (<b>d</b>): Volleyball-18. Our tracker is able to handle occlusion, similar interference, and deformation due to the embedding of part-level and global information. As shown in the graph, our tracker (in red) significantly outperforms the baseline SiamGAT (in blue), SiamRPN++ (in yellow), ClNet (in purple), SiamRPN++-RBO (in orange), and GroundTruth (in green). Please zoom in for a better view.</p>
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<p>Expected averaged overlap performance on VOT2016.</p>
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14 pages, 1363 KiB  
Article
Algebraic Morphology of DNA–RNA Transcription and Regulation
by Michel Planat, Marcelo M. Amaral and Klee Irwin
Symmetry 2023, 15(3), 770; https://doi.org/10.3390/sym15030770 - 21 Mar 2023
Cited by 3 | Viewed by 2297
Abstract
Transcription factors (TFs) and microRNAs (miRNAs) are co-actors in genome-scale decoding and regulatory networks, often targeting common genes. To discover the symmetries and invariants of the transcription and regulation at the scale of the genome, in this paper, we introduce tools of infinite [...] Read more.
Transcription factors (TFs) and microRNAs (miRNAs) are co-actors in genome-scale decoding and regulatory networks, often targeting common genes. To discover the symmetries and invariants of the transcription and regulation at the scale of the genome, in this paper, we introduce tools of infinite group theory and of algebraic geometry to describe both TFs and miRNAs. In TFs, the generator of the group is a DNA-binding domain while, in miRNAs, the generator is the seed of the sequence. For such a generated (infinite) group π, we compute the SL(2,C) character variety, where SL(2,C) is simultaneously a ‘space-time’ (a Lorentz group) and a ‘quantum’ (a spin) group. A noteworthy result of our approach is to recognize that optimal regulation occurs when π looks similar to a free group Fr (r=1 to 3) in the cardinality sequence of its subgroups, a result obtained in our previous papers. A non-free group structure features a potential disease. A second noteworthy result is about the structure of the Groebner basis G of the variety. A surface with simple singularities (such as the well known Cayley cubic) within G is a signature of a potential disease even when π looks similar to a free group Fr in its structure of subgroups. Our methods apply to groups with a generating sequence made of two to four distinct DNA/RNA bases in {A,T/U,G,C}. We produce a few tables of human TFs and miRNAs showing that a disease may occur when either π is away from a free group or G contains surfaces with isolated singularities. Full article
(This article belongs to the Special Issue Symmetry: Feature Papers 2023)
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<p><b>Left</b>: the Nanog transcription factor (PDB 9ANT). <b>Right</b>: the pre-miR-155 secondary structure [<a href="#B16-symmetry-15-00770" class="html-bibr">16</a>].</p>
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<p>(<b>Up</b>): Complementary base-pairing between miR-155-3p and the human Irak3 (interleukin-1 receptor-associated kinase 3) mRNA ([<a href="#B16-symmetry-15-00770" class="html-bibr">16</a>], Figure 5). The requisite‘seed sequence’ base-pairing is denoted by the bold dashes. (<b>Down</b>): the surface <math display="inline"><semantics> <mrow> <msubsup> <mi>f</mi> <mi>b</mi> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> <mo>=</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>y</mi> <mn>2</mn> </msup> <mo>−</mo> <mn>6</mn> <msup> <mi>z</mi> <mn>2</mn> </msup> <mo>+</mo> <mn>4</mn> <mi>x</mi> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math>.</p>
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<p>(<b>Left</b>): the Cayley cubic <math display="inline"><semantics> <mrow> <msub> <mi>κ</mi> <mn>4</mn> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>. (<b>Right</b>): the surface <math display="inline"><semantics> <mrow> <msubsup> <mi>f</mi> <mi>a</mi> <mrow> <mo>(</mo> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>The Fricke surface <math display="inline"><semantics> <mrow> <msub> <mi>V</mi> <mrow> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> <mo>=</mo> <msubsup> <mi>f</mi> <mi>a</mi> <mrow> <mo>(</mo> <mn>3</mn> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> (with three simple singularities of type <math display="inline"><semantics> <msub> <mi>A</mi> <mn>1</mn> </msub> </semantics></math>).</p>
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<p>(<b>Up</b>): Complementary base-pairing between miR-155-5p and the human Spi1 (spleen focus forming virus proviral integration oncogene) ([<a href="#B16-symmetry-15-00770" class="html-bibr">16</a>], Figure 4). The requisite ‘seed sequence’ base-pairing is denoted by the bold dashes. (<b>Down (from left to right)</b>): the surfaces <math display="inline"><semantics> <mrow> <msubsup> <mi>f</mi> <mi>H</mi> <mrow> <mo>(</mo> <mn>4</mn> <mo>)</mo> </mrow> </msubsup> <mo>=</mo> <msub> <mi>κ</mi> <mn>4</mn> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msup> <mi>f</mi> <mrow> <mo>(</mo> <mn>3</mn> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>κ</mi> <mn>3</mn> </msub> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>, four copies of them are contained within the Groebner basis for the character variety.</p>
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<p>A diagram with the main results discussed in the main text.</p>
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<p>(<b>Left</b>): the cubic surface <math display="inline"><semantics> <mrow> <msubsup> <mi>f</mi> <mrow> <mn>4</mn> <mo>,</mo> <mo>{</mo> <mo>}</mo> </mrow> <mrow> <mo>(</mo> <mn>2</mn> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>. (<b>Right</b>): the cubic surface <math display="inline"><semantics> <mrow> <msubsup> <mi>f</mi> <mi>b</mi> <mrow> <mo>(</mo> <mn>3</mn> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>)</mo> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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16 pages, 4390 KiB  
Article
A Novel Heteromorphic Ensemble Algorithm for Hand Pose Recognition
by Shiruo Liu, Xiaoguang Yuan, Wei Feng, Aifeng Ren, Zhenyong Hu, Zuheng Ming, Adnan Zahid, Qammer H. Abbasi and Shuo Wang
Symmetry 2023, 15(3), 769; https://doi.org/10.3390/sym15030769 - 21 Mar 2023
Cited by 3 | Viewed by 1660
Abstract
Imagining recognition of behaviors from video sequences for a machine is full of challenges but meaningful. This work aims to predict students’ behavior in an experimental class, which relies on the symmetry idea from reality to annotated reality centered on the feature space. [...] Read more.
Imagining recognition of behaviors from video sequences for a machine is full of challenges but meaningful. This work aims to predict students’ behavior in an experimental class, which relies on the symmetry idea from reality to annotated reality centered on the feature space. A heteromorphic ensemble algorithm is proposed to make the obtained features more aggregated and reduce the computational burden. Namely, the deep learning models are improved to obtain feature vectors representing gestures from video frames and the classification algorithm is optimized for behavior recognition. So, the symmetric idea is realized by decomposing the task into three schemas including hand detection and cropping, hand joints feature extraction, and gesture classification. Firstly, a new detector method named YOLOv4-specific tiny detection (STD) is proposed by reconstituting the YOLOv4-tiny model, which could produce two outputs with some attention mechanism leveraging context information. Secondly, the efficient pyramid squeeze attention (EPSA) net is integrated into EvoNorm-S0 and the spatial pyramid pool (SPP) layer to obtain the hand joint position information. Lastly, the D–S theory is used to fuse two classifiers, support vector machine (SVM) and random forest (RF), to produce a mixed classifier named S–R. Eventually, the synergetic effects of our algorithm are shown by experiments on self-created datasets with a high average recognition accuracy of 89.6%. Full article
(This article belongs to the Section Computer)
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<p>The overall method for hand pose recognition.</p>
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<p>The improved YOLOv4-STD model.</p>
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<p>Some components have been added to improve the backbone EPSAnet. The blue dotted box is the original pipeline and the green one is the improved one.</p>
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<p>Hand joint nodes are calibrated, and the wrist is the first point. Then, starting from the thumb, a key point is assigned to each bone node of the palm positions to visualize hand key point numbering. Specifically, the red points represent the joint position, and the numbers are the count of the red points.</p>
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<p>Plots of precision and recall for the original and improved models.</p>
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34 pages, 15543 KiB  
Article
A Novel Row Index Mathematical Procedure for the Mitigation of PV Output Power Losses during Partial Shading Conditions
by Muhammad Zeeshan, Naeem Ul Islam, Faiz Faizullah, Ihsan Ullah Khalil and Jaebyung Park
Symmetry 2023, 15(3), 768; https://doi.org/10.3390/sym15030768 - 21 Mar 2023
Cited by 3 | Viewed by 1787
Abstract
Energy demand forecasted for the next several years has been bench marked due to the massive need for electrical energy. Solar power plants have earned a great marketplace position in recent years, but also face challenges in terms of power dissipation due to [...] Read more.
Energy demand forecasted for the next several years has been bench marked due to the massive need for electrical energy. Solar power plants have earned a great marketplace position in recent years, but also face challenges in terms of power dissipation due to the frequent occurrence of shade. As a result, the per unit solar electricity price increases drastically. There is an immense need to ensure the maximum dependable power conversion efficiency of Photovoltaic (PV) systems by mitigating power output losses during partial shading conditions. The reconfiguration of PV arrays is a useful, effective, and promising approach in this context. Though several reconfiguration techniques have been developed in recent years, their applicability to real-time power plants is debatable due to the requirement of many physical relocations, long interconnecting ties, and complexity. This research work proposes a novel row index mathematical procedure followed by a technique in which the reconfiguration matrix indexes are filled with a unique number so that no row number repeats in the same row and column. Additionally, the proposed approach uses small number of switches that reduce the cost as well as the computational complexity. To strengthen the analysis, very recent techniques such as Sudoku, Total Cross Tied (TCT), Chess-Knight, and Particle Swarm Optimization (PSO) based reconfiguration are compared against five different shading patterns. It has been observed that approximately 68% power loss is mitigated in TCT configuration. It is worth noting that it results in higher PV output power than the existing latest reconfiguration techniques such as PSO, Chess-Knight, Sudoku, and others. Full article
(This article belongs to the Section Engineering and Materials)
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<p>Different interconnections schemes of PV array: (<b>a</b>) SP arrangement; (<b>b</b>) TCT arrangement; (<b>c</b>) BL arrangement; (<b>d</b>) Honeycomb arrangement.</p>
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<p>Overview of PV structure and equivalent circuit of PV cells, as in [<a href="#B4-symmetry-15-00768" class="html-bibr">4</a>].</p>
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<p>Characteristics curves with multiple peaks and an overview of mitigation methods.</p>
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<p>Characteristics curves with multiple peaks and an overview of mitigation methods.</p>
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<p>Characteristics curves with multiple peaks and an overview of mitigation methods.</p>
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<p>Classification of mismatch faults in PV arrays.</p>
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<p>PV array reconfiguration via a physical relocation procedure and the partial shade effect on TCT, and the proposed technique with the P–V characteristics curve.</p>
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<p>Reconfiguration of 9 × 9 PV array using the row index method.</p>
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<p>Reconfiguration of 9 × 9 PV array using the row index method.</p>
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<p>Reconfiguration of 9 × 9 PV array using the row index method.</p>
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<p>Flow chart of proposed row index based reconfiguration procedure.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for Case 1.</p>
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<p>Simulated I–V and P–V curves for Case 1.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for Case 2.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for Case 2.</p>
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<p>Simulated I–V and P–V characteristics for Case 2.</p>
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<p>Simulated I–V and P–V characteristics for Case 2.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for Case 3.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for Case 3.</p>
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<p>Simulated I–V and P–V characteristics for Case 3.</p>
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<p>Simulated I–V and P–V characteristics for Case 3.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for test Case 4.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for test Case 4.</p>
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<p>Simulated I–V and P–V characteristics for Case 4.</p>
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<p>Simulated I–V and P–V characteristics for Case 4.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for test Case 5.</p>
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<p>Shade dispersion in TCT, Chess-Knight, Sudoku, PSO and the proposed scheme for test Case 5.</p>
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<p>Simulated I–V and P–V characteristics for Case 5.</p>
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<p>Simulated I–V and P–V characteristics for Case 5.</p>
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16 pages, 7890 KiB  
Article
A Numerical Solution of Symmetric Angle Ply Plates Using Higher-Order Shear Deformation Theory
by Saira Javed
Symmetry 2023, 15(3), 767; https://doi.org/10.3390/sym15030767 - 21 Mar 2023
Viewed by 1459
Abstract
This research aims to provide the numerical analysis solution of symmetric angle ply plates using higher-order shear deformation theory (HSDT). The vibration of symmetric angle ply composite plates is analyzed using differential equations consisting of supplanting and turning functions. These supplanting and turning [...] Read more.
This research aims to provide the numerical analysis solution of symmetric angle ply plates using higher-order shear deformation theory (HSDT). The vibration of symmetric angle ply composite plates is analyzed using differential equations consisting of supplanting and turning functions. These supplanting and turning functions are numerically approximated through spline approximation. The obtained global eigenvalue problem is solved numerically to find the eigenfrequency parameter and a related eigenvector of spline coefficients. The plates of different constituent components are used to study the parametric effects of the plate’s aspect ratio, side-to-thickness ratio, assembling sequence, number of composite layers, and alignment of each layer on the frequency of the plate. The obtained results are validated by existing literature. Full article
(This article belongs to the Special Issue Symmetry and Approximation Methods II)
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<p>Composite plate geometry.</p>
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<p>Variation of the aspect ratio vs. frequency parameter of 6-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of the aspect ratio vs. frequency parameter of 6-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of the aspect ratio vs. frequency parameter of 6-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of the side-to-thickness ratio vs. frequency parameter of 5-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of side-to-thickness ratio vs. frequency parameter of 6-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>30</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of side-to-thickness ratio vs. frequency parameter of 6-layered plates <math display="inline"><semantics> <mrow> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mn>0</mn> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>45</mn> </mrow> <mo>°</mo> </msup> <mo>/</mo> <msup> <mrow> <mn>60</mn> </mrow> <mo>°</mo> </msup> </mrow> </semantics></math>.</p>
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<p>Variation of the theta vs. frequency parameter of 6-layered plates.</p>
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<p>Variation of the theta vs. frequency parameter of 5-layered plates.</p>
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<p>Variation of the theta vs. frequency parameter of 3-layered plates.</p>
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16 pages, 1153 KiB  
Article
The Reliability of Stored Water behind Dams Using the Multi-Component Stress-Strength System
by Hanan Haj Ahmad, Dina A. Ramadan, Mahmoud M. M. Mansour and Mohamed S. Aboshady
Symmetry 2023, 15(3), 766; https://doi.org/10.3390/sym15030766 - 21 Mar 2023
Cited by 4 | Viewed by 1560
Abstract
Dams are essential infrastructure for managing water resources and providing entry to clean water for human needs. However, the construction and maintenance of dams require careful consideration of their reliability and safety, specifically in the event of extreme weather conditions such as heavy [...] Read more.
Dams are essential infrastructure for managing water resources and providing entry to clean water for human needs. However, the construction and maintenance of dams require careful consideration of their reliability and safety, specifically in the event of extreme weather conditions such as heavy rainfall or flooding. In this study, the stress-strength model provides a useful framework for evaluating the reliability of dams and their ability to cope with external stresses such as water pressure, earthquake activity, and erosion. The Shasta reservoir in the United States is a prime example of a dam that requires regular assessment of its reliability to guarantee the safety of communities and infrastructure. The Gumbel Type II distribution has been suggested as a suitable model for fitting the collected data on the stress and strength of the reservoir behind the Shasta dam. Both classical and Bayesian approaches have been used to estimate the reliability function under the multi-component stress-strength model, and Monte Carlo simulation has been employed for parameter estimation. In addition, some measures of goodness-of-fit are employed to examine the suitability of the suggested model. Full article
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<p>A flowchart indicating the research process.</p>
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<p>View of Shasta Lake during the season of floods and a plan view for the dam.</p>
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<p>Empirical and fitted survival functions for the two datasets <span class="html-italic">X</span> and <span class="html-italic">Y</span>.</p>
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<p>Convergence for the estimated parameters <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>β</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>α</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>β</mi> <mn>2</mn> </msub> </semantics></math> and <span class="html-italic">R</span>.</p>
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23 pages, 1842 KiB  
Article
Enhancing Interval-Valued Pythagorean Fuzzy Decision-Making through Dombi-Based Aggregation Operators
by Ghaliah Alhamzi, Saman Javaid, Umer Shuaib, Abdul Razaq, Harish Garg and Asima Razzaque
Symmetry 2023, 15(3), 765; https://doi.org/10.3390/sym15030765 - 20 Mar 2023
Cited by 17 | Viewed by 1803
Abstract
The success of any endeavor or process is heavily contingent on the ability to reconcile and satisfy balance requirements, which are often characterized by symmetry considerations. In practical applications, the primary goal of decision-making processes is to efficiently manage the symmetry or asymmetry [...] Read more.
The success of any endeavor or process is heavily contingent on the ability to reconcile and satisfy balance requirements, which are often characterized by symmetry considerations. In practical applications, the primary goal of decision-making processes is to efficiently manage the symmetry or asymmetry that exists within different sources of information. In order to address this challenge, the primary aim of this study is to introduce novel Dombi operation concepts that are formulated within the framework of interval-valued Pythagorean fuzzy aggregation operators. In this study, an updated score function is presented to resolve the deficiency of the current score function in an interval-valued Pythagorean fuzzy environment. The concept of Dombi operations is used to introduce some interval-valued Pythagorean fuzzy aggregation operators, including the interval-valued Pythagorean fuzzy Dombi weighted arithmetic (IVPFDWA) operator, the interval-valued Pythagorean fuzzy Dombi ordered weighted arithmetic (IVPFDOWA) operator, the interval-valued Pythagorean fuzzy Dombi weighted geometric (IVPFDWG) operator, and the interval-valued Pythagorean fuzzy Dombi ordered weighted geometric (IVPFDOWG) operator. Moreover, the study investigates many important properties of these operators that provide new semantic meaning to the evaluation. In addition, the suggested score function and newly derived interval-valued Pythagorean fuzzy Dombi aggregation (IVPFDA) operators are successfully employed to select a subject expert in a certain institution. The proposed approach is demonstrated to be successful through empirical validation. Lastly, a comparative study is conducted to demonstrate the validity and applicability of the suggested approaches in comparison with current techniques. This research contributes to the ongoing efforts to advance the field of evaluation and decision-making by providing novel and effective tools and techniques. Full article
(This article belongs to the Special Issue Recent Developments on Fuzzy Sets Extensions)
16 pages, 2995 KiB  
Article
Bio-Inspired Machine Learning Approach to Type 2 Diabetes Detection
by Marwan Al-Tawil, Basel A. Mahafzah, Arar Al Tawil and Ibrahim Aljarah
Symmetry 2023, 15(3), 764; https://doi.org/10.3390/sym15030764 - 20 Mar 2023
Cited by 15 | Viewed by 2573
Abstract
Type 2 diabetes is a common life-changing disease that has been growing rapidly in recent years. According to the World Health Organization, approximately 90% of patients with diabetes worldwide have type 2 diabetes. Although there is no permanent cure for type 2 diabetes, [...] Read more.
Type 2 diabetes is a common life-changing disease that has been growing rapidly in recent years. According to the World Health Organization, approximately 90% of patients with diabetes worldwide have type 2 diabetes. Although there is no permanent cure for type 2 diabetes, this disease needs to be detected at an early stage to provide prognostic support to allied health professionals and develop an effective prevention plan. This can be accomplished by analyzing medical datasets using data mining and machine-learning techniques. Due to their efficiency, metaheuristic algorithms are now utilized in medical datasets for detecting chronic diseases, with better results than traditional methods. The main goal is to improve the performance of the existing approaches for the detection of type 2 diabetes. A bio-inspired metaheuristic algorithm called cuttlefish was used to select the essential features in the medical data preprocessing stage. The performance of the proposed approach was compared to that of a well-known bio-inspired metaheuristic feature selection algorithm called the genetic algorithm. The features selected from the cuttlefish and genetic algorithms were used with different classifiers. The implementation was applied to two datasets: the Pima Indian diabetes dataset and the hospital Frankfurt diabetes dataset; generally, these datasets are asymmetry, but some of the features in these datasets are close to symmetry. The results show that the cuttlefish algorithm has better accuracy rates, particularly when the number of instances in the dataset increases. Full article
(This article belongs to the Special Issue Machine Learning and Data Analysis)
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<p>Diagram of cuttlefish skin detailing the three main skin structures [<a href="#B24-symmetry-15-00764" class="html-bibr">24</a>].</p>
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<p>Reorder of the six cases in <a href="#symmetry-15-00764-f001" class="html-fig">Figure 1</a> [<a href="#B24-symmetry-15-00764" class="html-bibr">24</a>].</p>
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<p>Steps for predicting type 2 diabetes.</p>
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<p>Kappa values on the PID dataset at different levels of the training set.</p>
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<p>Kappa values on the HFD dataset at different levels of the training set.</p>
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<p>MAE values on the PID dataset at different levels of the training set.</p>
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<p>MAE values on the HFD dataset at different levels of the training set.</p>
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18 pages, 319 KiB  
Article
Sharp Coefficient Bounds for a New Subclass of q-Starlike Functions Associated with q-Analogue of the Hyperbolic Tangent Function
by Chetan Swarup
Symmetry 2023, 15(3), 763; https://doi.org/10.3390/sym15030763 - 20 Mar 2023
Cited by 6 | Viewed by 1544
Abstract
In this study, by making the use of q-analogous of the hyperbolic tangent function and a Sălăgean q-differential operator, a new class of q-starlike functions is introduced. The prime contribution of this study covers the derivation of sharp coefficient bounds [...] Read more.
In this study, by making the use of q-analogous of the hyperbolic tangent function and a Sălăgean q-differential operator, a new class of q-starlike functions is introduced. The prime contribution of this study covers the derivation of sharp coefficient bounds in open unit disk U, especially the first three coefficient bounds, Fekete–Szego type functional, and upper bounds of second- and third-order Hankel determinant for the functions to this class. We also use Zalcman and generalized Zalcman conjectures to investigate the coefficient bounds of a newly defined class of functions. Furthermore, some known corollaries are highlighted based on the unique choices of the involved parameters l and q. Full article
(This article belongs to the Special Issue Symmetry in Geometric Functions and Mathematical Analysis II)
26 pages, 7620 KiB  
Article
A New Technique to Uniquely Identify the Edges of a Graph
by Hafiz Muhammad Ikhlaq, Rashad Ismail, Hafiz Muhammad Afzal Siddiqui and Muhammad Faisal Nadeem
Symmetry 2023, 15(3), 762; https://doi.org/10.3390/sym15030762 - 20 Mar 2023
Cited by 4 | Viewed by 1973
Abstract
Graphs are useful for analysing the structure models in computer science, operations research, and sociology. The word metric dimension is the basis of the distance function, which has a symmetric property. Moreover, finding the resolving set of a graph is NP-complete, and the [...] Read more.
Graphs are useful for analysing the structure models in computer science, operations research, and sociology. The word metric dimension is the basis of the distance function, which has a symmetric property. Moreover, finding the resolving set of a graph is NP-complete, and the possibilities of finding the resolving set are reduced due to the symmetric behaviour of the graph. In this paper, we introduce the idea of the edge-multiset dimension of graphs. A representation of an edge is defined as the multiset of distances between it and the vertices of a set, BV(Γ). If the representation of two different edges is unequal, then B is an edge-multiset resolving a set of Γ. The least possible cardinality of the edge-multiset resolving a set is referred to as the edge-multiset dimension of Γ. This article presents preliminary results, special conditions, and bounds on the edge-multiset dimension of certain graphs. This research provides new insights into structure models in computer science, operations research, and sociology. They could have implications for developing computer algorithms, aircraft scheduling, and species movement between regions. Full article
(This article belongs to the Special Issue Theoretical Computer Science and Discrete Mathematics II)
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<p>A graph with the <math display="inline"><semantics> <mrow> <mi>m</mi> <mi>d</mi> <mo>(</mo> <mi>G</mi> <mo>)</mo> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>.</p>
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<p>Diagram for the multiset and edge-multiset dimension.</p>
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<p>The kayak paddle graph <math display="inline"><semantics> <mrow> <mi>K</mi> <mi>P</mi> <mo>(</mo> <mn>12</mn> <mo>,</mo> <mn>8</mn> <mo>,</mo> <mn>5</mn> <mo>)</mo> </mrow> </semantics></math>.</p>
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<p>The dragon graph <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mrow> <mn>8</mn> <mo>,</mo> <mn>5</mn> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>The comb product of <math display="inline"><semantics> <msub> <mi>P</mi> <mn>5</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>P</mi> <mn>4</mn> </msub> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mn>5</mn> </msub> <msub> <mo>⊳</mo> <mo>∘</mo> </msub> <msub> <mi>P</mi> <mn>4</mn> </msub> </mrow> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mi mathvariant="sans-serif">Γ</mi> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mi mathvariant="sans-serif">Γ</mi> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>(</mo> <msub> <mi>T</mi> <mrow> <mn>7</mn> <mo>,</mo> <mn>3</mn> </mrow> </msub> <mo>)</mo> </mrow> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mi mathvariant="sans-serif">Γ</mi> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mi mathvariant="sans-serif">Γ</mi> </semantics></math>.</p>
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<p>Caterpillar graph <math display="inline"><semantics> <mrow> <mi>C</mi> <msub> <mi>T</mi> <mn>7</mn> </msub> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>{</mo> <mn>2</mn> <mo>,</mo> <mn>4</mn> <mo>,</mo> <mn>6</mn> <mo>}</mo> </mrow> </semantics></math>.</p>
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<p>Lobster graph <math display="inline"><semantics> <msub> <mi>L</mi> <mn>7</mn> </msub> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>{</mo> <mn>3</mn> <mo>,</mo> <mn>4</mn> <mo>,</mo> <mn>5</mn> <mo>}</mo> </mrow> </semantics></math>.</p>
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<p>Three cases of graph <math display="inline"><semantics> <msub> <mi>T</mi> <mi>n</mi> </msub> </semantics></math> with diameter 3.</p>
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<p>Caterpillar graph <math display="inline"><semantics> <mrow> <mi>C</mi> <msub> <mi>T</mi> <mn>6</mn> </msub> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>{</mo> <mn>3</mn> <mo>,</mo> <mn>4</mn> <mo>}</mo> </mrow> </semantics></math>.</p>
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<p>Lobster graph <math display="inline"><semantics> <msub> <mi>L</mi> <mn>6</mn> </msub> </semantics></math> with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>{</mo> <mn>3</mn> <mo>,</mo> <mn>4</mn> <mo>}</mo> </mrow> </semantics></math>.</p>
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<p>Complete 2-ary tree graph with <math display="inline"><semantics> <mrow> <mi>h</mi> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">Γ</mi> </mrow> </semantics></math>.</p>
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<p>The graph <math display="inline"><semantics> <mrow> <mi mathvariant="sans-serif">Γ</mi> </mrow> </semantics></math>.</p>
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18 pages, 716 KiB  
Article
Complexity Analysis of Benes Network and Its Derived Classes via Information Functional Based Entropies
by Jun Yang, Asfand Fahad, Muzammil Mukhtar, Muhammad Anees, Amir Shahzad and Zahid Iqbal
Symmetry 2023, 15(3), 761; https://doi.org/10.3390/sym15030761 - 20 Mar 2023
Cited by 6 | Viewed by 2314
Abstract
The use of information–theoretical methodologies to assess graph-based systems has received a significant amount of attention. Evaluating a graph’s structural information content is a classic issue in fields such as cybernetics, pattern recognition, mathematical chemistry, and computational physics. Therefore, conventional methods for determining [...] Read more.
The use of information–theoretical methodologies to assess graph-based systems has received a significant amount of attention. Evaluating a graph’s structural information content is a classic issue in fields such as cybernetics, pattern recognition, mathematical chemistry, and computational physics. Therefore, conventional methods for determining a graph’s structural information content rely heavily on determining a specific partitioning of the vertex set to obtain a probability distribution. A network’s entropy based on such a probability distribution is obtained from vertex partitioning. These entropies produce the numeric information about complexity and information processing which, as a consequence, increases the understanding of the network. In this paper, we study the Benes network and its novel-derived classes via different entropy measures, which are based on information functionals. We construct different partitions of vertices of the Benes network and its novel-derived classes to compute information functional dependent entropies. Further, we present the numerical applications of our findings in understanding network complexity. We also classify information functionals which describe the networks more appropriately and may be applied to other networks. Full article
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<p>Normal representation of B(3).</p>
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<p>Normal representation of <math display="inline"><semantics> <mrow> <mi>H</mi> <mi>C</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p>
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<p>Normal representation of <math display="inline"><semantics> <mrow> <mi>V</mi> <mi>C</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p>
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<p>The patterns of Entropies of <math display="inline"><semantics> <mrow> <mi>B</mi> <mo stretchy="false">(</mo> <mi>η</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> from information functionals based on eccentricity-dependent TIs.</p>
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<p>The patterns of Entropies of <math display="inline"><semantics> <mrow> <mi>H</mi> <mi>C</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mi>η</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> from information functionals based on eccentricity-dependent TIs.</p>
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<p>The patterns of Entropies of <math display="inline"><semantics> <mrow> <mi>V</mi> <mi>C</mi> <mi>B</mi> <mo stretchy="false">(</mo> <mi>η</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> from information functionals based on eccentricity-dependent TIs.</p>
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11 pages, 449 KiB  
Article
New Features in the Differential Cross Sections Measured at the LHC
by Oleg Selyugin
Symmetry 2023, 15(3), 760; https://doi.org/10.3390/sym15030760 - 20 Mar 2023
Cited by 6 | Viewed by 1075
Abstract
The critical analysis of the new experimental data obtained by the ATLAS Collaboration group at 13 TeV is presented and the problem of the tension between data of the ATLAS and TOTEM Collaborations is considered. The analysis of new effects discovered on the [...] Read more.
The critical analysis of the new experimental data obtained by the ATLAS Collaboration group at 13 TeV is presented and the problem of the tension between data of the ATLAS and TOTEM Collaborations is considered. The analysis of new effects discovered on the basis of experimental data at 13 TeV MDPI: ref is not allowed in abstract, please correct. and associated with the specific properties of the hadron potential at large distances is carried out taking account of all sets of experimental data on elastic proton-proton scattering obtained by the TOTEM and ATLAS Collaborations in a wide momentum transfer region. It also gives quantitative descriptions of all examined experimental data with a minimum of fitting parameters. It is shown that the new features determined at a high statistical level give an important contribution to the differential cross sections and allow the research analytic properties and symmetries into hadron interactions at large distances. Full article
(This article belongs to the Section Physics)
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<p><math display="inline"><semantics> <mrow> <msub> <mo>Δ</mo> <mrow> <mi>C</mi> <mi>N</mi> <mi>I</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> extracted from experimental data: open squares and full squares—with different magnitudes of <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mrow> <mi>t</mi> <mi>o</mi> <mi>t</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>s</mi> <mo>)</mo> </mrow> <mo>=</mo> <mn>104</mn> </mrow> </semantics></math> mb and <math display="inline"><semantics> <mrow> <msub> <mi>σ</mi> <mrow> <mi>t</mi> <mi>o</mi> <mi>t</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>s</mi> <mo>)</mo> </mrow> <mo>=</mo> <mn>110</mn> </mrow> </semantics></math> mb with ATLAS form of <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mi>h</mi> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>; circles—extracted from the model representation of TOTEM data; hard line—representation of the CNI-term in the form <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mrow> <mi>C</mi> <mi>h</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <mo>=</mo> <mn>8</mn> <msub> <mi>α</mi> <mrow> <mi>e</mi> <mi>m</mi> </mrow> </msub> <mo>/</mo> <mi>t</mi> </mrow> </semantics></math>; long dashed line—HEGS model calculations of the CNI term; short, dashed line—model calculations with ATLAS phenomenological fit of <math display="inline"><semantics> <mrow> <msub> <mi>F</mi> <mi>h</mi> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>Comparison of experimental data on the differential cross sections at small momentum transfer of the TOTEM and ATLAS Collaboration only with statistical errors. (Full circles—ATLAS data, crosses—TOTEM data).</p>
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<p>(<b>left side</b>) The effect of the oscillation term in the even and odd parts of the intervals of momentum transfer of ATLAS data at 13 TeV (hard and dotes lines) The same but with shifted intervals by half the period—(short, dashed lines); (<b>right side</b>) <math display="inline"><semantics> <mrow> <mi>R</mi> <msub> <mo>Δ</mo> <mrow> <mi>t</mi> <mi>h</mi> </mrow> </msub> </mrow> </semantics></math> of Equation (<a href="#FD5-symmetry-15-00760" class="html-disp-formula">5</a>) (the hard line) and <math display="inline"><semantics> <mrow> <mi>R</mi> <msub> <mo>Δ</mo> <mrow> <mi>e</mi> <mi>x</mi> <mo>.</mo> </mrow> </msub> </mrow> </semantics></math> Equation (<a href="#FD6-symmetry-15-00760" class="html-disp-formula">6</a>) (the tiny line) of ATLAS data at 13 TeV.</p>
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<p>The <math display="inline"><semantics> <mrow> <mi>d</mi> <msub> <mi>σ</mi> <mrow> <mi>e</mi> <mi>l</mi> </mrow> </msub> <mo>/</mo> <mi>d</mi> <mi>t</mi> </mrow> </semantics></math> are calculatedin the framework of the HEGS model at 2–13 TeV (the experimental points with only statistical errors). (<b>right</b>) the full region of <span class="html-italic">t</span>; (<b>left</b>) the magnification of the region of the small momentum transfer; (the data of ATLAS (<math display="inline"><semantics> <mrow> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </mrow> </semantics></math> TeV) are drawn without an additional coefficient of the normalization.</p>
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<p>The <span class="html-italic">s</span> and <span class="html-italic">t</span> dependence of the imaginary (<b>left</b>) and real (<b>right</b>) parts of the elastic scattering amplitude (lines at small <span class="html-italic">t</span> correspond top down to 13, 7, 2.96 TeV).</p>
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3 pages, 180 KiB  
Editorial
Asymmetry of Movement and Postural Balance and Underlying Functions in Humans
by Thierry Paillard
Symmetry 2023, 15(3), 759; https://doi.org/10.3390/sym15030759 - 20 Mar 2023
Cited by 1 | Viewed by 3116
Abstract
Human movements and posture often show lateral asymmetries. Although symmetry [...] Full article
(This article belongs to the Special Issue Neuroscience, Neurophysiology and Symmetry)
19 pages, 3716 KiB  
Article
A Malware Detection Approach Based on Deep Learning and Memory Forensics
by Shuhui Zhang, Changdong Hu, Lianhai Wang, Miodrag J. Mihaljevic, Shujiang Xu and Tian Lan
Symmetry 2023, 15(3), 758; https://doi.org/10.3390/sym15030758 - 19 Mar 2023
Cited by 11 | Viewed by 6427
Abstract
As cyber attacks grow more complex and sophisticated, new types of malware become more dangerous and challenging to detect. In particular, fileless malware injects malicious code into the physical memory directly without leaving attack traces on disk files. This type of attack is [...] Read more.
As cyber attacks grow more complex and sophisticated, new types of malware become more dangerous and challenging to detect. In particular, fileless malware injects malicious code into the physical memory directly without leaving attack traces on disk files. This type of attack is well concealed, and it is difficult to find the malicious code in the static files. For malicious processes in memory, signature-based detection methods are becoming increasingly ineffective. Facing these challenges, this paper proposes a malware detection approach based on convolutional neural network and memory forensics. As the malware has many symmetric features, the saved training model can detect malicious code with symmetric features. The method includes collecting executable static malicious and benign samples, running the collected samples in a sandbox, and building a dataset of portable executables in memory through memory forensics. When a process is running, not all the program content is loaded into memory, so binary fragments are utilized for malware analysis instead of the entire portable executable (PE) files. PE file fragments are selected with different lengths and locations. We conducted several experiments on the produced dataset to test our model. The PE file with 4096 bytes of header fragment has the highest accuracy. We achieved a prediction accuracy of up to 97.48%. Moreover, an example of fileless attack is illustrated at the end of the paper. The results show that the proposed method can detect malicious codes effectively, especially the fileless attack. Its accuracy is better than that of common machine learning methods. Full article
(This article belongs to the Section Computer)
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<p>Process information analysis.</p>
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<p>The overall workflow of the proposed approach.</p>
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<p>Data type conversion.</p>
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<p>Select head segment.</p>
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<p>Select tail segment.</p>
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<p>Select a random segment.</p>
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<p>Our model.</p>
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<p>Sample fragments of different lengths.</p>
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<p>Sample fragments from different locations.</p>
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<p>Comparison of different models.</p>
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<p>Comparison of different models.</p>
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<p>Encrypted file.</p>
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<p>Detect file.</p>
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<p>Detect result.</p>
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37 pages, 8111 KiB  
Review
Green IoT: A Review and Future Research Directions
by Mohammed H. Alsharif, Abu Jahid, Anabi Hilary Kelechi and Raju Kannadasan
Symmetry 2023, 15(3), 757; https://doi.org/10.3390/sym15030757 - 19 Mar 2023
Cited by 57 | Viewed by 11122
Abstract
The internet of things (IoT) has a significant economic and environmental impact owing to the billions or trillions of interconnected devices that use various types of sensors to communicate through the internet. It is well recognized that each sensor requires a small amount [...] Read more.
The internet of things (IoT) has a significant economic and environmental impact owing to the billions or trillions of interconnected devices that use various types of sensors to communicate through the internet. It is well recognized that each sensor requires a small amount of energy to function; but, with billions of sensors, energy consumption can be significant. Therefore, it is crucial to focus on developing energy-efficient IoT technology and sustainable solutions. The contribution of this article is to support the implementation of eco-friendly IoT solutions by presenting a thorough examination of energy-efficient practices and strategies for IoT to assist in the advancement of sustainable and energy-efficient IoT technologies in the future. Four framework principles for achieving this are discussed, including (i) energy-efficient machine-to-machine (M2M) communications, (ii) energy-efficient and eco-sustainable wireless sensor networks (WSN), (iii) energy-efficient radio-frequency identification (RFID), and (iv) energy-efficient microcontroller units and integrated circuits (IC). This review aims to contribute to the next-generation implementation of eco-sustainable and energy-efficient IoT technologies. Full article
(This article belongs to the Special Issue Next-Generation Green Wireless Networks and Industrial IoT)
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<p>Top 10 IoT application areas in 2020.</p>
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<p>Research methodology of the article.</p>
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<p>The proposed framework and energy-efficient technologies for IoT in this study.</p>
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<p>Classification of energy-efficient techniques for M2M communications.</p>
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<p>Architecture of computing layers.</p>
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<p>Classification of energy-efficient techniques for WSNs.</p>
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<p>A selection of battery types commonly used in IoT/sensor devices.</p>
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<p>The operating concept of wireless charging by both magnetic inductive and magnetic resonance coupling.</p>
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<p>Cluster network architecture.</p>
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<p>Operating principle of RFID system.</p>
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<p>Classifications of RFID tags.</p>
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<p>Passive RFID system.</p>
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<p>Active RFID system.</p>
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<p>Comparison of energy storage options: batteries versus capacitors.</p>
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<p>Demonstration of typical power consumption scenario of a microcontroller for generic IoT applications.</p>
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<p>A summary of the key characteristics of MCUs commonly employed in ultra-low power applications.</p>
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<p>Comparison of the power efficiency of single-core vs. multi-core processors.</p>
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<p>Potential future directions for green IoT.</p>
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26 pages, 1303 KiB  
Article
Comparing the Min–Max–Median/IQR Approach with the Min–Max Approach, Logistic Regression and XGBoost, Maximising the Youden Index
by Rocío Aznar-Gimeno, Luis M. Esteban, Gerardo Sanz and Rafael del-Hoyo-Alonso
Symmetry 2023, 15(3), 756; https://doi.org/10.3390/sym15030756 - 19 Mar 2023
Cited by 2 | Viewed by 2280
Abstract
Although linearly combining multiple variables can provide adequate diagnostic performance, certain algorithms have the limitation of being computationally demanding when the number of variables is sufficiently high. Liu et al. proposed the min–max approach that linearly combines the minimum and maximum values of [...] Read more.
Although linearly combining multiple variables can provide adequate diagnostic performance, certain algorithms have the limitation of being computationally demanding when the number of variables is sufficiently high. Liu et al. proposed the min–max approach that linearly combines the minimum and maximum values of biomarkers, which is computationally tractable and has been shown to be optimal in certain scenarios. We developed the Min–Max–Median/IQR algorithm under Youden index optimisation which, although more computationally intensive, is still approachable and includes more information. The aim of this work is to compare the performance of these algorithms with well-known Machine Learning algorithms, namely logistic regression and XGBoost, which have proven to be efficient in various fields of applications, particularly in the health sector. This comparison is performed on a wide range of different scenarios of simulated symmetric or asymmetric data, as well as on real clinical diagnosis data sets. The results provide useful information for binary classification problems of better algorithms in terms of performance depending on the scenario. Full article
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<p>Normal distributions. Difference in the average Youden index achieved by our approach (MMM/MMIQR) and the other algorithms (MMM-LR, MMM-XG, MMM-MM). <b>1</b>: Independents. <b>2</b>: High correlations. <b>3</b>: Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.3</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.7</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>0.7</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.3</mn> <mo>·</mo> <mi>J</mi> </mrow> </semantics></math>). <b>4</b>: Negative correlations. <b>5</b>: Low correlation. <b>6</b>: Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.3</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.7</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>0.7</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.3</mn> <mo>·</mo> <mi>J</mi> </mrow> </semantics></math>). <b>7</b>: Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.5</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mi>I</mi> </mrow> </semantics></math>).</p>
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<p>Non-normal distributions. Difference in the average Youden index achieved by our approach (MMM/MMIQR) and the other algorithms (MMM-LR, MMM-XG, MMM-MM). <b>1</b>: Log-normal. Independents. <b>2</b>: Log-normal. High correlations. <b>3</b>: Log-normal. Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.3</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.7</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>0.7</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.3</mn> <mo>·</mo> <mi>J</mi> </mrow> </semantics></math>). <b>4</b>: Log-normal. Negative correlations. <b>5</b>: Log-normal. Low correlation. <b>6</b>: Log-normal. Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.3</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.7</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mn>0.7</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.3</mn> <mo>·</mo> <mi>J</mi> </mrow> </semantics></math>). <b>7</b>: Log-normal. Different correlations (<math display="inline"><semantics> <mrow> <msub> <mo>Σ</mo> <mn>1</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mo>·</mo> <mi>I</mi> <mo>+</mo> <mn>0.5</mn> <mo>·</mo> <mi>J</mi> <mo>,</mo> <msub> <mo>Σ</mo> <mn>2</mn> </msub> <mo>=</mo> <mi>I</mi> </mrow> </semantics></math>).</p>
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<p>Marginal distributions of biomarkers. DMD dataset.</p>
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<p>Marginal distributions of biomarkers. Maternal Health dataset. High–Medium vs. Low Risk.</p>
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<p>Marginal distributions of biomarkers. Maternal Health dataset. High vs. Medium–Low Risk.</p>
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25 pages, 3854 KiB  
Article
Omnidimensional Convex Polytopes
by Szymon Łukaszyk and Andrzej Tomski
Symmetry 2023, 15(3), 755; https://doi.org/10.3390/sym15030755 - 19 Mar 2023
Cited by 2 | Viewed by 2217
Abstract
The study shows that the volumes and surfaces of n-balls, n-simplices, and n-orthoplices are holomorphic functions of n, which makes those objects omnidimensional, that is well defined in any complex dimension. Applications of these formulas to the omnidimensional polytopes [...] Read more.
The study shows that the volumes and surfaces of n-balls, n-simplices, and n-orthoplices are holomorphic functions of n, which makes those objects omnidimensional, that is well defined in any complex dimension. Applications of these formulas to the omnidimensional polytopes inscribed in and circumscribed about n-balls reveal previously unknown properties of these geometric objects. In particular, for 0<n<1, the volumes of the omnidimensional polytopes are larger than those of circumscribing n-balls, and both their volumes and surfaces are smaller than those of inscribed n-balls. The surface of an n-simplex circumscribing a unit diameter n-ball is spirally convergent to zero with real n approaching negative infinity but first has a local maximum at n=3.5. The surface of an n-orthoplex circumscribing a unit diameter n-ball is spirally divergent with real n approaching negative infinity but first has a local minimum at n=1.5, where its real and imaginary parts are equal to each other; similarly, is its volume, where the similar local minimum occurs at n=3.5. Reflection functions for volumes and surfaces of these polytopes inscribed in and circumscribed about n-balls are proposed. Symmetries of products and quotients of the volumes in complex dimensions n and n and of the surfaces in complex dimensions n and 2n are shown to be independent of the metric factor and the gamma function. Specific symmetries also hold between the volumes and surfaces in dimensions n=1/2 and n=1/2. Full article
(This article belongs to the Special Issue Mathematical Modelling of Physical Systems 2021)
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<p>Graphs of volumes (<span class="html-italic">V</span>) and surfaces (<span class="html-italic">S</span>) of unit edge length regular <span class="html-italic">n</span>-simplices (red), <span class="html-italic">n</span>-orthoplices (green), <span class="html-italic">n</span>-cubes (pink), and unit diameter <span class="html-italic">n</span>-balls (blue), along with the integer recurrence relations (dashed lines) for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>4</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of volumes (<span class="html-italic">V</span>) and surfaces (<span class="html-italic">S</span>) of unit edge length regular <span class="html-italic">n</span>-simplices (red), <span class="html-italic">n</span>-orthoplices (green), and unit diameter <span class="html-italic">n</span>-balls (blue) for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>:</mo> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>4</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (red) and <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue) for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (red) and <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue) for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (red), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>V</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark red), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mspace width="3.33333pt"/> <mo>∈</mo> <mspace width="3.33333pt"/> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (red), <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>S</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark red), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mspace width="3.33333pt"/> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (green) and <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (green) and <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (green), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>V</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark green), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (green), <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>S</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark green), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>C</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (pink), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>V</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>C</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark pink), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Graphs of <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>C</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (pink), <math display="inline"><semantics> <mrow> <mi>S</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), and <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>S</mi> <mo>˜</mo> </mover> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>C</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark pink), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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<p>Volume metric and gamma function independent relations. <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>B</mi> </msub> </mrow> </semantics></math> (blue), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>S</mi> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>S</mi> </msub> </mrow> </semantics></math> (red), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (dark red), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>S</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (orange-red), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>O</mi> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mi>O</mi> </msub> <mo>=</mo> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>I</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (lime green), <math display="inline"><semantics> <mrow> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> <mi>V</mi> <msub> <mrow> <mo>(</mo> <mo>−</mo> <mi>n</mi> <mo>)</mo> </mrow> <mrow> <mi>O</mi> <mi>C</mi> <mi>B</mi> </mrow> </msub> </mrow> </semantics></math> (yellow-green), for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>:</mo> <mi>n</mi> <mo>∈</mo> <mfenced separators="" open="[" close="]"> <mo>−</mo> <mn>6</mn> <mo>,</mo> <mn>6</mn> </mfenced> </mrow> </semantics></math>.</p>
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18 pages, 324 KiB  
Article
Expansion-Free Dissipative Fluid Spheres: Analytical Solutions
by Luis Herrera, Alicia Di Prisco and Justo Ospino
Symmetry 2023, 15(3), 754; https://doi.org/10.3390/sym15030754 - 19 Mar 2023
Cited by 10 | Viewed by 1488
Abstract
We search for exact analytical solutions of spherically symmetric dissipative fluid distributions satisfying the vanishing expansion condition (vanishing expansion scalar Θ). To accomplish this, we shall impose additional restrictions allowing integration of the field equations. The solutions are analyzed, and possible applications [...] Read more.
We search for exact analytical solutions of spherically symmetric dissipative fluid distributions satisfying the vanishing expansion condition (vanishing expansion scalar Θ). To accomplish this, we shall impose additional restrictions allowing integration of the field equations. The solutions are analyzed, and possible applications to astrophysical scenarios as well as alternative approaches to obtaining new solutions are discussed. Full article
(This article belongs to the Special Issue Symmetry in Cosmology and Gravity: Topic and Advance)
11 pages, 277 KiB  
Article
Tangent Bundles of P-Sasakian Manifolds Endowed with a Quarter-Symmetric Metric Connection
by Mohammad Nazrul Islam Khan, Fatemah Mofarreh and Abdul Haseeb
Symmetry 2023, 15(3), 753; https://doi.org/10.3390/sym15030753 - 19 Mar 2023
Cited by 13 | Viewed by 1588
Abstract
The purpose of this study is to evaluate the curvature tensor and the Ricci tensor of a P-Sasakian manifold with respect to the quarter-symmetric metric connection on the tangent bundle TM. Certain results on a semisymmetric P-Sasakian manifold, generalized [...] Read more.
The purpose of this study is to evaluate the curvature tensor and the Ricci tensor of a P-Sasakian manifold with respect to the quarter-symmetric metric connection on the tangent bundle TM. Certain results on a semisymmetric P-Sasakian manifold, generalized recurrent P-Sasakian manifolds, and pseudo-symmetric P-Sasakian manifolds on TM are proved. Full article
17 pages, 7780 KiB  
Article
Electrochemistry of Rhodanine Derivatives as Model for New Colorimetric and Electrochemical Azulene Sensors for the Detection of Heavy Metal Ions
by Ovidiu-Teodor Matica, Cornelia Musina (Borsaru), Alina Giorgiana Brotea, Eleonora-Mihaela Ungureanu, Mihaela Cristea, Raluca Isopescu, George-Octavian Buica and Alexandru C. Razus
Symmetry 2023, 15(3), 752; https://doi.org/10.3390/sym15030752 - 18 Mar 2023
Cited by 3 | Viewed by 1596
Abstract
Rhodanine (R) is a heterocycle having complexing properties for heavy metal (HM) ions. Considering the similar electron-donating character of diethylaminobenzene and azulene, electrochemical characterization of (Z)-5-(azulen-1-ylmethylene)-2-thioxo-thiazolidin-4-one (R1) and 5-(4 diethylamino-benzylidene)-2-thioxo-thiazolidin-4-one (R2) was performed to establish [...] Read more.
Rhodanine (R) is a heterocycle having complexing properties for heavy metal (HM) ions. Considering the similar electron-donating character of diethylaminobenzene and azulene, electrochemical characterization of (Z)-5-(azulen-1-ylmethylene)-2-thioxo-thiazolidin-4-one (R1) and 5-(4 diethylamino-benzylidene)-2-thioxo-thiazolidin-4-one (R2) was performed to establish their common features. Chemically modified electrodes based on R1 and R2 were compared for HM recognition. Evidence for the formation of films was provided by scanning and controlled potential electrolysis, and HM recognition experiments were performed using their films. Parallel studies for analysis of HMs by complexation in solution were performed by UV-Vis. The analogy between R1 and R2 created the premise for easier selection of compounds for certain applications. The performance of the chemically modified electrodes was evaluated as detection limits for HMs. The azulene monomer (R1) proved to be the best candidate for Pb(II) detection, being about eight times more sensitive than R2. However, in solution, R2 proved to be a good choice for optical measurements, having a higher absorption coefficient. These results support the two ligands having different behaviors in homogeneous and heterogeneous systems. Full article
(This article belongs to the Section Chemistry: Symmetry/Asymmetry)
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<p>Structures of (<span class="html-italic">Z</span>)-5-(azulen-1-ylmethylene)-2-thioxo-thiazolidin-4-one (<b>R1</b>), 2-thioxo-thiazolidin-4-one (<b>R</b>), and 5-(4 diethylamino-benzylidene)-2-thioxo-thiazolidin-4-one (<b>R2</b>).</p>
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<p>CV (0.1 Vs<sup>−1</sup>) anodic and cathodic curves (with currents in absolute values) on GC for <b>R1</b> and <b>R2</b> in 0.1 M TBAP/CH<sub>3</sub>CN at different concentrations; a1–a5 and c1–c5 are the anodic and cathodic peaks, respectively.</p>
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<p>CV curves for 1 mM solution of <b>R2</b> in 0.1 M TBAP/CH<sub>3</sub>CN at different scan rates (<b>a</b>); a1 and c1 current peak variations with the square root of the scan rate (<b>b</b>).</p>
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<p>CV curves (0.1 V s<sup>−1</sup>) on GC at different potential domains for 1 mM solutions in 0.1 M TBAP/CH<sub>3</sub>CN for <b>R2</b>; a1–a5 and c1–c3 are the anodic and cathodic peaks, respectively.</p>
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<p>DPV curves (with anodic and cathodic currents in absolute values) for <b>R1</b> and <b>R2</b> solutions in 0.1 M TBAP/CH<sub>3</sub>CN at different concentrations; a1–a5 and c1–c5 are the anodic and cathodic peaks, respectively.</p>
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<p>RDE curves on GC for [<b>R1</b>] and [<b>R2</b>] solutions in 0.1 M TBAP/CH<sub>3</sub>CN; the cathodic currents are plotted in absolute values.</p>
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<p>RDE curves on GC at 1000 rpm for [<b>R1</b>] and [<b>R2</b>] solutions at different concentrations in 0.1 M TBAP/CH<sub>3</sub>CN; the cathodic currents are in absolute values.</p>
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<p>Successive CV cycles (0.1 V/s) in <b>R2</b> solution (2 mM) in 0.1 M TBAP/CH<sub>3</sub>CN carried out during the synthesis of CMEs by scanning at different anodic limit potentials (V) increasing in the order: (<b>A</b>) &lt; (<b>B</b>) &lt; (<b>C</b>) &lt; (<b>D</b>) &lt; (<b>E</b>) &lt; (<b>F</b>) &lt; (<b>G</b>) &lt; (<b>H</b>) (<b>left</b> side), and the curves in 1 mM Fc solution in 0.1 M TBAP/CH<sub>3</sub>CN of the corresponding <span class="html-italic">CMEs</span> vs. bare electrode (dashed lines) (<b>right</b> side).</p>
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<p>Analysis of <b>R2</b>-CME film formation by scanning: cumulated CV curves (0.1 V/s) after the transfer of <b>R2</b>-CMEs in 1 mM Fc solution in 0.1 M TBAP/CH<sub>3</sub>CN vs. bare electrode (<b>A</b>), variations of Epa (blue), Epc (red), Δep (olive), and Ef (wine) (<b>B</b>), and of ipa (blue) and ipc (red) vs. anodic limit for scanning potential (<b>C</b>).</p>
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<p>Analysis of <b>R2</b>-CME film formation by CPE: cumulated CV curves (0.1 V/s) on <b>R2</b>-CMEs after the transfer in 1 mM Fc solution in 0.1 M TBAP/CH3CN vs. bare electrode (<b>A</b>); plots of Epa (blue), Epc (red), Δep (olive), and Ef (wine) vs. CPE potential (<b>B</b>), and of ipa (blue) and ipc (red) vs. CPE potential (<b>C</b>).</p>
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<p>DPV curves recorded on <b>R2</b>-CMEs (obtained by CPE at 1.3 V and 2 mC) for different concentrations of mixed metals in the accumulation solutions at 10 min accumulation times.</p>
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<p>Dependence of DPV stripping peak area on the metallic ion’s concentration for each ion (<b>A</b>), and on Pb ion concentration in the linear dependence range (<b>B</b>).</p>
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<p>DPV curves (0.01 V s<sup>−1</sup>) for CMEs obtained by CPE (at 1.3 V, 2 mC for <b>R2</b> and 1.2 V, 0.7 mC for <b>R1</b>) after 10 min accumulation times in solution concentrations of 10<sup>−6</sup> M mixed metals for <b>R2</b> and 10<sup>−6</sup> M Pb(II) for <b>R1</b>.</p>
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<p>UV-Vis spectra (recorded after 1 min) for various [Pb]/[<b>R1</b>] ratios; insets: variation of the absorbance for the peak at 457 nm vs. [Pb]/[<b>R1</b>] (<b>I1</b> inset) and vs. [Pb]/([Pb] + [<b>R1</b>]) (<b>I2</b> inset).</p>
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<p>UV-Vis spectra after 1 min for different [Pb]/[<b>R2</b>] ratios; insets: variation of the absorbance for the peak at 457 nm vs. [Pb]/[<b>R2</b>] (<b>I1</b> inset) and vs. [Pb]/([Pb] + [<b>R2</b>]) (<b>I2</b> inset).</p>
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17 pages, 356 KiB  
Article
Five Generalized Rough Approximation Spaces Produced by Maximal Rough Neighborhoods
by A. A. Azzam and Tareq M. Al-shami
Symmetry 2023, 15(3), 751; https://doi.org/10.3390/sym15030751 - 18 Mar 2023
Cited by 4 | Viewed by 1317
Abstract
In rough set theory, the multiplicity of methods of calculating neighborhood systems is very useful to calculate the measures of accuracy and roughness. In line with this research direction, in this article we present novel kinds of rough neighborhood systems inspired by the [...] Read more.
In rough set theory, the multiplicity of methods of calculating neighborhood systems is very useful to calculate the measures of accuracy and roughness. In line with this research direction, in this article we present novel kinds of rough neighborhood systems inspired by the system of maximal neighborhood systems. We benefit from the symmetry between rough approximations (lower and upper) and topological operators (interior and closure) to structure the current generalized rough approximation spaces. First, we display two novel types of rough set models produced by maximal neighborhoods, namely, type 2 mξ-neighborhood and type 3 mξ-neighborhood rough models. We investigate their master properties and show the relationships between them as well as their relationship with some foregoing ones. Then, we apply the idea of adhesion neighborhoods to introduce three additional rough set models, namely, type 4 mξ-adhesion, type 5 mξ-adhesion and type 6 mξ-adhesion neighborhood rough models. We establish the fundamental characteristics of approximation operators inspired by these models and discuss how the properties of various relationships relate to one another. We prove that adhesion neighborhood rough models increase the value of the accuracy measure of subsets, which can improve decision making. Finally, we provide a comparison between Yao’s technique and current types of adhesion neighborhood rough models. Full article
22 pages, 4003 KiB  
Article
A Robust-Reliable Decision-Making Methodology Based on a Combination of Stakeholders’ Preferences Simulation and KDD Techniques for Selecting Automotive Platform Benchmark
by Asad Saghari, Ivana Budinská, Masoud Hosseinimehr and Shima Rahmani
Symmetry 2023, 15(3), 750; https://doi.org/10.3390/sym15030750 - 18 Mar 2023
Cited by 8 | Viewed by 1683
Abstract
The automotive family design is known as one of the most complex engineering design problems with multiple groups of stakeholders involved from different domains of interest and contradictory attributes. Taking into account all stakeholders’ preferences, which are generally symmetrical, non-deterministic distributions around a [...] Read more.
The automotive family design is known as one of the most complex engineering design problems with multiple groups of stakeholders involved from different domains of interest and contradictory attributes. Taking into account all stakeholders’ preferences, which are generally symmetrical, non-deterministic distributions around a mean value, and determining the right value of attributes for each alternative are two basic challenges for these types of decision-making problems. In this research, the possibility to achieve a robust-reliable decision by focusing on the two aforementioned challenges is explored. In the proposed methodology, a random simulation technique is used to elicit stakeholders’ preferences and determine the relative importance of attributes. The decision space and values of attributes are determined using the Knowledge Discovery in Databases (KDD) technique, and to achieve a robust-reliable decision, statistical and sensitivity analyses are performed. By implementing this methodology, the decision-maker is assured that the preferences of all stakeholders are taken into account and the determined values for attributes are reliable with the least degree of uncertainty. The proposed methodology aims to select benchmark platforms for the development of an automotive family. The decision space includes 546 automobiles in 11 different segments based on 34 platforms. There are 6223 unique possible states of stakeholders’ preferences. As a result, five platforms with the highest degree of desirability and robustness to diversity and uncertainty in the stakeholders’ preferences are selected. The presented methodology can be implemented in complex decision-making problems, including a large and diverse number of stakeholders and multiple attributes. In addition, this methodology is compatible with many Multi-Attribute Decision-Making (MADM) techniques, including SAW, AHP, SWARA, and TOPSIS. Full article
(This article belongs to the Special Issue Algorithms for Multi-Criteria Decision-Making under Uncertainty)
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<p>Flowchart of the proposed method.</p>
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<p>Hierarchical system for the MADM problem.</p>
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<p>The normalized values of the simulated weights of importance.</p>
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<p>Each alternative’s position in ranking after solving the decision-making problem 6223 times.</p>
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<p>Variation in the order of alternatives in the first five positions of ranking order.</p>
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<p>Box diagram of the positions occupied by the alternatives in 6223 solutions of the decision problem.</p>
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<p>The most robust-reliable ranking order in the first five positions.</p>
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<p>Statistical comparison of (<b>a</b>) alternative P6 and (<b>b</b>) alternative P31.</p>
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14 pages, 2787 KiB  
Article
Energy Transfer Processes in NASICON-Type Phosphates under Synchrotron Radiation Excitation
by Nataliya Krutyak, Vitali Nagirnyi, Ivo Romet, Dina Deyneko and Dmitry Spassky
Symmetry 2023, 15(3), 749; https://doi.org/10.3390/sym15030749 - 18 Mar 2023
Cited by 1 | Viewed by 1563
Abstract
The luminescence properties of NASICON-type Na3.6M1.8(PO4)3 (M = Y, Lu) and Na3Sc2(PO4)3 phosphates, undoped and rare earth-doped (RE = Tb3+, Dy3+, Eu3+, Ce [...] Read more.
The luminescence properties of NASICON-type Na3.6M1.8(PO4)3 (M = Y, Lu) and Na3Sc2(PO4)3 phosphates, undoped and rare earth-doped (RE = Tb3+, Dy3+, Eu3+, Ce3+), were studied using synchrotron radiation in a wide energy region of 4.5–45 eV. Intrinsic emission originating from self-trapped excitons with electron component localized at the 3d Sc states was detected in both doped and undoped Na3Sc2(PO4)3 while only defect-related emission was registered in Na3.6M1.8(PO4)3. Emission of RE ions substituting three-valent cations in low-symmetry sites was detected in all doped phosphates. The efficiency and pass ways of energy transfer from the host to emission centres were analysed based on luminescence excitation spectra. It is shown that the most efficient energy transfer is realized in Tb3+-doped phosphors, while it was poor for other RE ions. The differences in energy transfer efficiencies are explained by different position of RE f states in the crystal electronic band structure influencing the efficiency of charge carrier trapping in the substance. Based on excitation spectra analysis, the bandgap values were estimated to ~8 eV for all studied phosphates. Full article
(This article belongs to the Special Issue Advances in Synchrotron and Undulator Radiation Studies Ⅱ)
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<p>XRD patterns for undoped and RE-doped Na<sub>3</sub>Sc<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub>, as well as for undoped Na<sub>3.6</sub>Lu<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub> and Na<sub>3.6</sub>Y<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub>.</p>
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<p>Normalized luminescence spectra of undoped NASICON phosphates ((<b>a</b>)—Na<sub>3</sub>Sc<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub>, (<b>b</b>)—Na<sub>3.6</sub>Lu<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub>, (<b>c</b>)—Na<sub>3.6</sub>Y<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub>) at different excitation energies, T = 7 K.</p>
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<p>Luminescence excitation spectra of undoped NASICON phosphates ((<b>a</b>)—Na<sub>3</sub>Sc<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub>, (<b>b</b>)—Na<sub>3.6</sub>Lu<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub>, (<b>c</b>)—Na<sub>3.6</sub>Y<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub>) at T = 7 K.</p>
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<p>Luminescence spectra of Na<sub>3.6</sub>Y<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub> (<b>a</b>) and Na<sub>3.6</sub>Lu<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub> (<b>b</b>), doped with Eu<sup>3+</sup> (1), Tb<sup>3+</sup> (2) and Dy<sup>3+</sup> (3) at E<sub>ex</sub> = 45 eV, T = 7 K.</p>
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<p>Luminescence excitation spectra of Na<sub>3.6</sub>Y<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub> (<b>a</b>) and Na<sub>3.6</sub>Lu<sub>1.8</sub>(PO<sub>4</sub>)<sub>3</sub> (<b>b</b>), doped with Eu<sup>3+</sup> (1), Tb<sup>3+</sup> (2) and Dy<sup>3+</sup> (3) at T = 7 K; λ<sub>em</sub> = 620 nm (1), 545 nm (2) and 580 nm (3). Arrows indicate exciton peak position in undoped samples.</p>
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<p>Luminescence spectra of Na<sub>3</sub>Sc<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub>, doped with 0.02 Ce<sup>3+</sup> (<b>a</b>) at E<sub>ex</sub> = 45 eV (1), 7.8 eV (2) and 6.0 eV (3) and 0.01 Eu<sup>3+</sup> (<b>b</b>) at E<sub>ex</sub> = 7.7 eV (1), 6.4 eV (2) and 5.3 eV (3), T = 7 K.</p>
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<p>Luminescence excitation spectra of Na<sub>3</sub>Sc<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub>, doped with 0.02 Ce<sup>3+</sup> (<b>a</b>) at λ<sub>em</sub> = 240 (1), 340 (2) and 400 (3) nm and 0.01 Eu<sup>3+</sup> (<b>b</b>) at λ<sub>em</sub> = 600 (1) and 450 (2) nm, T = 7 K.</p>
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