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Symmetry, Volume 11, Issue 11 (November 2019) – 103 articles

Cover Story (view full-size image): Could a superconductor at a temperature slightly higher than the critical temperature (in the fluctuations regime) change the gravitational field where it is immersed? We try to answer this question using the time-dependent Ginzburg–Landau equations. View this paper.
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16 pages, 3611 KiB  
Article
Dynamic Behaviors Analysis of Asymmetric Stochastic Delay Differential Equations with Noise and Application to Weak Signal Detection
by Qiubao Wang, Xing Zhang and Yuejuan Yang
Symmetry 2019, 11(11), 1428; https://doi.org/10.3390/sym11111428 - 19 Nov 2019
Cited by 5 | Viewed by 2433
Abstract
This paper presents the dynamic behaviors of a second-order asymmetric stochastic delay system with a Duffing oscillator as well as through the detection of weak signals, which are analyzed theoretically and numerically. The dynamic behaviors of the asymmetric system are analyzed based on [...] Read more.
This paper presents the dynamic behaviors of a second-order asymmetric stochastic delay system with a Duffing oscillator as well as through the detection of weak signals, which are analyzed theoretically and numerically. The dynamic behaviors of the asymmetric system are analyzed based on the stochastic center manifold, together with Hopf bifurcation. Numerical analysis revealed that the time delay could enhance the noise immunity of the asymmetric system so as to enhance the asymmetric system’s ability to detect weak signals. The frequency of the weak signal under noise excitation was detected through the ‘act-and-wait’ method. The small amplitude was detected through the transition from the chaotic to the periodic state. Theoretical analysis and numerical simulation indicate that the application of the asymmetric Duffing oscillator with delay to detect weak signal is feasible. Full article
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<p>The time delay <math display="inline"><semantics> <mi>τ</mi> </semantics></math> enhances the noise immunity of chaotic state: (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>; (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>; (<b>d</b>) <math display="inline"><semantics> <mrow> <mi>τ</mi> <mo>=</mo> <mn>3</mn> </mrow> </semantics></math>.</p>
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<p>Bifurcation diagrams of the asymmetric system (1) with respect to frequency <math display="inline"><semantics> <mi>ω</mi> </semantics></math>: (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.001</mn> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.02</mn> </mrow> </semantics></math>; and (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>0.05</mn> </mrow> </semantics></math>.</p>
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<p>Phase diagrams of the asymmetric system (1): (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>ω</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>ω</mi> <mo>=</mo> <mn>1.1</mn> </mrow> </semantics></math>.</p>
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<p>Bifurcation diagram of the asymmetric system (1).</p>
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<p>Phase diagrams of the asymmetric system (1): (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>=</mo> <mn>0.3541</mn> </mrow> </semantics></math>; (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>=</mo> <mn>0.3542</mn> </mrow> </semantics></math>; and (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>=</mo> <mn>0.39</mn> </mrow> </semantics></math>.</p>
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<p>Bifurcation diagram of the asymmetric system (<a href="#FD17-symmetry-11-01428" class="html-disp-formula">17</a>).</p>
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<p>Phase diagrams of the asymmetric system (<a href="#FD17-symmetry-11-01428" class="html-disp-formula">17</a>): (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>=</mo> <mn>0.3448</mn> </mrow> </semantics></math> and (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>f</mi> <mo>=</mo> <mn>0.3449</mn> </mrow> </semantics></math>.</p>
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12 pages, 274 KiB  
Article
A Conformally Invariant Derivation of Average Electromagnetic Helicity
by Ivan Fernandez-Corbaton
Symmetry 2019, 11(11), 1427; https://doi.org/10.3390/sym11111427 - 19 Nov 2019
Cited by 5 | Viewed by 2919
Abstract
The average helicity of a given electromagnetic field measures the difference between the number of left- and right-handed photons contained in the field. Here, the average helicity is derived using the conformally invariant inner product for Maxwell fields. Several equivalent integral expressions in [...] Read more.
The average helicity of a given electromagnetic field measures the difference between the number of left- and right-handed photons contained in the field. Here, the average helicity is derived using the conformally invariant inner product for Maxwell fields. Several equivalent integral expressions in momentum space, in ( r , t ) space, and in the time-harmonic ( r , ω ) space are obtained, featuring Riemann–Silberstein-like fields and potentials. The time-harmonic expressions can be directly evaluated using the outputs of common numerical solvers of Maxwell equations. The results are shown to be equivalent to the well-known volume integral for the average helicity, featuring the electric and magnetic fields and potentials. Full article
(This article belongs to the Special Issue Duality Symmetry)
24 pages, 4183 KiB  
Article
A Decision Support System Using Text Mining Based Grey Relational Method for the Evaluation of Written Exams
by Mehmet Erkan Yuksel and Huseyin Fidan
Symmetry 2019, 11(11), 1426; https://doi.org/10.3390/sym11111426 - 19 Nov 2019
Cited by 6 | Viewed by 3723
Abstract
Grey relational analysis (GRA) is a part of the Grey system theory (GST). It is appropriate for solving problems with complicated interrelationships between multiple factors/parameters and variables. It solves multiple-criteria decision-making problems by combining the entire range of performance attribute values being considered [...] Read more.
Grey relational analysis (GRA) is a part of the Grey system theory (GST). It is appropriate for solving problems with complicated interrelationships between multiple factors/parameters and variables. It solves multiple-criteria decision-making problems by combining the entire range of performance attribute values being considered for every alternative into one single value. Thus, the main problem is reduced to a single-objective decision-making problem. In this study, we developed a decision support system for the evaluation of written exams with the help of GRA using contextual text mining techniques. The answers obtained from the written exam with the participation of 50 students in a computer laboratory and the answer key prepared by the instructor constituted the data set of the study. A symmetrical perspective allows us to perform relational analysis between the students’ answers and the instructor’s answer key in order to contribute to the measurement and evaluation. Text mining methods and GRA were applied to the data set through the decision support system employing the SQL Server database management system, C#, and Java programming languages. According to the results, we demonstrated that the exam papers are successfully ranked and graded based on the word similarities in the answer key. Full article
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<p>Text mining process.</p>
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<p>System model. GRA, Grey Relational Analysis; BoW, Bag of Words; VSM, Vector Space Model.</p>
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<p>Database tables.</p>
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<p>BoW1 and BoW2 for first question first student.</p>
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<p>Two-stage decision-making process.</p>
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12 pages, 3396 KiB  
Article
Statistic-Driven Proton Transfer Affecting Nanoscopic Organization in an Ethylammonium Nitrate Ionic Liquid and 1,4-Diaminobutane Binary Mixture: A Steamy Pizza Model
by Alessandro Mariani, Matteo Bonomo and Stefano Passerini
Symmetry 2019, 11(11), 1425; https://doi.org/10.3390/sym11111425 - 19 Nov 2019
Cited by 6 | Viewed by 3312
Abstract
Herein, we report on the theoretical and experimental investigation of the chemical equilibrium in a Ethylammonium Nitrate (EAN)/1,4-Diaminobutane (DAB) binary mixture displaying a significant excess of the latter component (namely, a 1:9 mole ratio). Both the neutral compounds, i.e., ethylamine (EtNH2) [...] Read more.
Herein, we report on the theoretical and experimental investigation of the chemical equilibrium in a Ethylammonium Nitrate (EAN)/1,4-Diaminobutane (DAB) binary mixture displaying a significant excess of the latter component (namely, a 1:9 mole ratio). Both the neutral compounds, i.e., ethylamine (EtNH2) and DAB, present very similar chemical properties, especially concerning their basic strength, resulting in a continuous jump of the proton from the ethylammonium to the diamine (and vice-versa). Due to the significant excess of DAB, the proton is (statistically) expected to be bound to one of its nitrogen atoms, leading to the formation of a new (ternary) mixture containing DAB (ca. 80%), ethylamine (ca. 10%) and 4-amino-1-butylammonium nitrate (ABAN, ca. 10%). This is probed by means of SAXS measurements, showing LqE (low q excess) that increases over time. This feature tends to stabilize after approximately one day. When the measurement is repeated after one year, the LqE feature shows an increased intensity. Based on the results of our simulations, we suggest that this phenomenon is likely due to partial ethylamine evaporation, pushing the equilibrium toward the formation of ABAN. Full article
(This article belongs to the Special Issue Materials Science and X-Ray Diffraction)
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Graphical abstract

Graphical abstract
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<p>Experimental SAXS patterns for the EAN+DAB (10%mol EAN) mixture. Data were collected at room temperature at ID02 beamline of ESRF. Five minutes after preparation (purple); 1 h (cyan); 1 day (dark green); 1 week (light green); 1 month (orange); 1 year (red).</p>
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<p>Normalized <sup>1</sup>H spectrum of the one-year old sample.</p>
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<p>Computed SAXS patterns for EAN+DAB (10% mol EAN) (purple); ABAN+DAB (10% mol ABAN) (gray); EAN+EtNH<sub>2</sub>+DAB+ABAN (0.5% mol EAN, 9.75% mol EtNH<sub>2</sub>, 9.75% mol ABAN) (black); EtNH<sub>2</sub>+DAB+ABAN (10% mol EtNH<sub>2</sub>, 10% mol ABAN) (red).</p>
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<p>Radial distribution functions for selected hydrogen bonded pairs. Anion-cation (<b>a</b>); DAB-DAB (<b>b</b>); DAB-anion (<b>c</b>); cation-cation (<b>d</b>); anion-anion (<b>e</b>). In all the panels EAN-containing system (black); ABAN-containing system (red).</p>
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<p>Radial distribution functions for selected hydrogen-bonded pairs. Amine-amine (<b>a</b>), where ethylamine-ethylamine (black); ethylamine-ABA(NH2) (red); DAB-ABA(NH2) (blue); ethylamine-DAB (purple); ABA(NH2)-ABA(NH2) (green). Amine-ammonium (<b>b</b>), where DAB-ethylammonium (black); ethylamine-ABA(NH3) (blue); DAB-ABA(NH3) (red); ABA(NH2)-ABA(NH3) (green). Amine-anion (<b>c</b>), where ethylamine-anion (black); DAB-anion in the “no transfer” model (blue); DAB-anion in the “total transfer” model (red); ABA(NH2)-anion (green).</p>
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<p>Coordination numbers and spatial distribution functions. For all the panels, the color of the diagram and the isosurface is the same for a given fragment. All the isosurfaces are plotted for a value of twice the average density. DAB in EAN-containing system (<b>a</b>); DAB in ABAN-containing system (<b>b</b>); ABA (<b>c</b>); Ethylammonium (<b>d</b>); Ethylamine (<b>e</b>).</p>
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<p>Schematics of the end-to-end bridging hydrogen bond responsible for the stabilization of the ABAN ion pair.</p>
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<p>Snapshots of the simulated systems. (<b>a</b>) EAN+DAB (10% mol EAN); (<b>b</b>) EtNH<sub>2</sub>+DAB+ABAN (10% mol EtNH<sub>2</sub>, 10% mol ABAN); (<b>c</b>) EAN+EtNH<sub>2</sub>+DAB+ABAN (0.5% mol EAN, 9.75% mol EtNH<sub>2</sub>, 9.75% mol ABAN); (<b>d</b>) ABAN+DAB (10% mol ABAN). Polar part (red); apolar part (green); DAB (transparent-orange); ethylamine (blue); for panel c ethylammonium (cyan). For all the panels, only a 20 Å thick slice is shown for clarity.</p>
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18 pages, 4227 KiB  
Article
Robust Hybrid Beamforming Scheme for Millimeter-Wave Massive-MIMO 5G Wireless Networks
by Saleem Latteef Mohammed, Mohammed H. Alsharif, Sadik Kamel Gharghan, Imran Khan and Mahmoud Albreem
Symmetry 2019, 11(11), 1424; https://doi.org/10.3390/sym11111424 - 18 Nov 2019
Cited by 47 | Viewed by 4933
Abstract
Wireless networks employing millimeter-wave (mmWave) and Massive Multiple-Input Multiple-Output (MIMO) technologies are a key approach to boost network capacity, coverage, and quality of service (QoS) for future communications. They deploy symmetric antennas on a large scale in order to enhance the system throughput [...] Read more.
Wireless networks employing millimeter-wave (mmWave) and Massive Multiple-Input Multiple-Output (MIMO) technologies are a key approach to boost network capacity, coverage, and quality of service (QoS) for future communications. They deploy symmetric antennas on a large scale in order to enhance the system throughput and data rate. However, increasing the number of antennas and Radio Frequency (RF) chains results in high computational complexity and more energy requirements. Therefore, to solve these problems, this paper proposes a low-complexity hybrid beamforming scheme for mmWave Massive-MIMO 5G wireless networks. The proposed algorithm is on the basis of alternating the minimum mean square error (Alt-MMSE) hybrid beamforming technique in which the orthogonal properties of the digital matrix were designed, and then the MSE of the transmitted and received signal was reduced. The phase of the analog matrix was obtained from the updated digital matrix. Simulation results showed that the proposed hybrid beamforming algorithm had better performance than existing state-of-the-art algorithms, and similar performance with the optimal digital precoding algorithm. Full article
(This article belongs to the Special Issue Information Technologies and Electronics)
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<p>Proposed framework for millimeter-wave (mmWave) MIMO system.</p>
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<p>System performance when number of RF links <math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">t</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">r</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <mn mathvariant="bold">8</mn> </mrow> </semantics></math>, and number of streams <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <mrow> <mo>{</mo> <mrow> <mn mathvariant="bold">2</mn> <mo>,</mo> <mn mathvariant="bold">4</mn> <mo>,</mo> <mn mathvariant="bold">8</mn> </mrow> <mo>}</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>System performance when number of RF links <math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">t</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">r</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <mn mathvariant="bold">8</mn> </mrow> </semantics></math>, and number of streams <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <mrow> <mo>{</mo> <mrow> <mn mathvariant="bold">2</mn> <mo>,</mo> <mn mathvariant="bold">4</mn> <mo>,</mo> <mn mathvariant="bold">8</mn> </mrow> <mo>}</mo> </mrow> </mrow> </semantics></math>.</p>
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<p>System performance when number of data streams equals RF links (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">t</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">r</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> </mrow> </semantics></math>).</p>
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<p>System performance when number of data streams equals RF links (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">t</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> <mo>=</mo> <msubsup> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">r</mi> <mrow> <mi mathvariant="bold-italic">R</mi> <mi mathvariant="bold-italic">F</mi> </mrow> </msubsup> </mrow> </semantics></math>).</p>
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<p>System performance when number of data streams is <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <mrow> <mo>{</mo> <mrow> <mn mathvariant="bold">2</mn> <mo>,</mo> <mn mathvariant="bold">4</mn> <mo>,</mo> <mn mathvariant="bold">8</mn> </mrow> <mo>}</mo> </mrow> </mrow> </semantics></math> and SNR <math display="inline"><semantics> <mo>=</mo> </semantics></math> 0 dB.</p>
Full article ">Figure 4 Cont.
<p>System performance when number of data streams is <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="bold-italic">N</mi> <mi mathvariant="bold-italic">s</mi> </msub> <mo>=</mo> <mrow> <mo>{</mo> <mrow> <mn mathvariant="bold">2</mn> <mo>,</mo> <mn mathvariant="bold">4</mn> <mo>,</mo> <mn mathvariant="bold">8</mn> </mrow> <mo>}</mo> </mrow> </mrow> </semantics></math> and SNR <math display="inline"><semantics> <mo>=</mo> </semantics></math> 0 dB.</p>
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<p>Comparison of spectral efficiency against number of BS antennas with 8 RF chains and SNR = 0 dB.</p>
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<p>Comparison of spectral efficiency against the number of user antennas with 8 RF chains and SNR = 0 dB.</p>
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<p>Comparison of energy efficiency against number of RF chains.</p>
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<p>Bit error rate (BER) comparison of different algorithms under various SNR levels.</p>
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<p>Complexity analysis of algorithms with increasing number of BS antennas.</p>
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16 pages, 908 KiB  
Article
Feature Selection Based on Swallow Swarm Optimization for Fuzzy Classification
by Ilya Hodashinsky, Konstantin Sarin, Alexander Shelupanov and Artem Slezkin
Symmetry 2019, 11(11), 1423; https://doi.org/10.3390/sym11111423 - 18 Nov 2019
Cited by 16 | Viewed by 3120
Abstract
This paper concerns several important topics of the Symmetry journal, namely, pattern recognition, computer-aided design, diversity and similarity. We also take advantage of the symmetric structure of a membership function. Searching for the (sub) optimal subset of features is an NP-hard problem. In [...] Read more.
This paper concerns several important topics of the Symmetry journal, namely, pattern recognition, computer-aided design, diversity and similarity. We also take advantage of the symmetric structure of a membership function. Searching for the (sub) optimal subset of features is an NP-hard problem. In this paper, a binary swallow swarm optimization (BSSO) algorithm for feature selection is proposed. To solve the classification problem, we use a fuzzy rule-based classifier. To evaluate the feature selection performance of our method, BSSO is compared to induction without feature selection and some similar algorithms on well-known benchmark datasets. Experimental results show the promising behavior of the proposed method in the optimal selection of features. Full article
(This article belongs to the Special Issue Information Technologies and Electronics)
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<p>Dataset Optdigits. Average classification rates of the competing methods versus number of selected features.</p>
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<p>Dataset Spambase. Average classification rates of the competing methods versus number of selected features.</p>
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<p>Dataset Coil2000. Average classification rates of the competing methods versus number of selected features.</p>
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15 pages, 2252 KiB  
Article
Makeup Interpolation Based on Color and Shape Parametrization
by Jieun Cho, Jun Ohya and Sang Il Park
Symmetry 2019, 11(11), 1422; https://doi.org/10.3390/sym11111422 - 18 Nov 2019
Cited by 4 | Viewed by 3406
Abstract
In this paper, we address the problem of synthesizing continuous variations with the appearance of makeup by taking a linear combination of the examples. Makeup usually shows a vague boundary and does not form a clear shape, which makes this problem unique from [...] Read more.
In this paper, we address the problem of synthesizing continuous variations with the appearance of makeup by taking a linear combination of the examples. Makeup usually shows a vague boundary and does not form a clear shape, which makes this problem unique from the existing image interpolation problems. We approach this problem as an interpolation between semi-transparent image layers and tackle this by presenting new parametrization schemes for the color and for the shape separately in order to achieve an effective interpolation. For the color parametrization, our main idea is based on the observation of the symmetric relation between the color and transparency of the makeup; we provide an optimization framework for extracting a representative palette of colors associated with the transparent values, which enables us to easily set up the color correspondence among the multiple makeup samples. For the shape parametrization, we exploit a polar coordinate system, that creates the in-between shapes effectively, without ghosting artifacts. Full article
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Figure 1
<p>We take multiple makeup images as the examples and a single no-makeup image as the target image. Courtesy of images from [<a href="#B29-symmetry-11-01422" class="html-bibr">29</a>].</p>
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<p>We align the example makeup image to the target image by using a thin plate spline-based image warping technique: (<b>a</b>) the example makeup image; (<b>b</b>) the aligned example image; (<b>c</b>) the target image. Courtesy of images from [<a href="#B29-symmetry-11-01422" class="html-bibr">29</a>].</p>
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<p>We use Shahrian et al.’s matting method [<a href="#B34-symmetry-11-01422" class="html-bibr">34</a>] to generate an initial matte for a further refinement: (<b>a</b>) input makeup image; (<b>b</b>) input trimap; and (<b>c</b>) resulting matte.</p>
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<p>In color makeup, we observe a common tendency of the foreground colors to change along with the density of the makeup.</p>
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<p>An overview of our matte refinement process.</p>
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<p>Results of the background color tone matching. The image furthest to the left in the lower row is the no-makeup target image. Its background color tone is adjusted to be matched with the corresponding makeup images in the upper row.</p>
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<p>Results of the matte refinement. The upper row shows the composited images of the no-makeup target image with the initial mattes. The refinement process adjusts the mattes to make the composited images resemble the example makeup images well as shown in the middle row. The lowest row shows the resulting color parametrization for each example, where the leftmost color of each image corresponds to <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>, and the rightmost color is for <math display="inline"><semantics> <mrow> <mi>α</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>.</p>
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<p>We build 48 B-spline approximations evenly spaced along the angular direction: (<b>a</b>) example alpha mattes; (<b>b</b>) 48 radial sampling directions, where the red lines denote the reference radial directions of zero degrees; (<b>c</b>) B-spline approximated alpha mattes.</p>
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<p>The convergence of the error in the foreground color parametrization along with the iteration. The errors are measured by the average distance in the color space of the pixels between the composited makeup images (middle) and the example makeup image on the furthest right.</p>
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<p>The synthesized makeup interpolation sequence between the two makeup examples shown in the upper row (<b>a</b>–<b>e</b>). Those are the composited results by computing the inbetween alpha mattes from the B-spline shape approximation (the second row) followed by adding details using the patch match method (the third row). The foreground makeup color lookup tables are also interpolated during the sequence (the bottom row).</p>
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<p>The synthesized makeup morphing sequence from (<b>b</b>–<b>d</b>) between the given two makeup examples (<b>a</b>,<b>e</b>) with their corresponding alpha mattes and foreground color lookup tables.</p>
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<p>Continuous blending results of the four different makeup examples.</p>
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<p>The color parametrization facilitates the user to easily edit the makeup color by changing the foreground color lookup table: (<b>a</b>) the original lookup table; (<b>b</b>–<b>d</b>) using the lookup table of other examples; (<b>e</b>) the user given lookup table.</p>
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<p>Morphing sequence comparison between our method and the simple image blending: (<b>a</b>,<b>b</b>) resulting images and their corresponding alpha mattes from our method; (<b>c</b>,<b>d</b>) those from simple image blending.</p>
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21 pages, 833 KiB  
Article
Agglomeration Economies: An Analysis of the Determinants of Employment in the Cities of Ecuador
by Tania Paola Torres-Gutiérrez, Ronny Correa-Quezada, José Álvarez-García and María de la Cruz del Río-Rama
Symmetry 2019, 11(11), 1421; https://doi.org/10.3390/sym11111421 - 16 Nov 2019
Cited by 5 | Viewed by 4338
Abstract
The objective of this investigation is to study the role of agglomeration economies (manufacturing) in urban employment growth, as a proxy for economic growth, between 1980 and 2010 in Ecuador. The three measures of agglomeration-specialization, diversity, and density-are tested to determine their effect [...] Read more.
The objective of this investigation is to study the role of agglomeration economies (manufacturing) in urban employment growth, as a proxy for economic growth, between 1980 and 2010 in Ecuador. The three measures of agglomeration-specialization, diversity, and density-are tested to determine their effect on employment growth in industries. The empirical analysis is based on firm- and city-level data from manufacturing activities. A model is proposed to estimate the effect of agglomeration economies on the growth of employment and a regression is conducted using instrumental variables. In particular, the two-stage least squares (2SLS) estimator is used. We conclude that localization economies measured by a specialization index have a positive impact on the growth of employment in the period analyzed. The results are similar to those obtained by other work carried out both in developed and developing countries. Full article
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<p>Average annual growth of employment in the cities of Ecuador: 1980–2010. Source: Based on National Institute of Statistics and Census-INEC data [<a href="#B60-symmetry-11-01421" class="html-bibr">60</a>].</p>
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<p>Relationship between size and diversity of the cities of Ecuador. Source: Own elaboration based on INEC data [<a href="#B60-symmetry-11-01421" class="html-bibr">60</a>].</p>
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12 pages, 2402 KiB  
Article
Closed Form Solutions for Nonlinear Oscillators Under Discontinuous and Impulsive Periodic Excitations
by Valery Pilipchuk
Symmetry 2019, 11(11), 1420; https://doi.org/10.3390/sym11111420 - 16 Nov 2019
Cited by 1 | Viewed by 2359
Abstract
Periodic responses of linear and nonlinear systems under discontinuous and impulsive excitations are analyzed with non-smooth temporal transformations incorporating temporal symmetries of periodic processes. The related analytical manipulations are illustrated on a strongly nonlinear oscillator whose free vibrations admit an exact description in [...] Read more.
Periodic responses of linear and nonlinear systems under discontinuous and impulsive excitations are analyzed with non-smooth temporal transformations incorporating temporal symmetries of periodic processes. The related analytical manipulations are illustrated on a strongly nonlinear oscillator whose free vibrations admit an exact description in terms of elementary functions. As a result, closed form analytical solutions for the non-autonomous strongly nonlinear case are obtained. Conditions of existence for such solutions are represented as a family of period-amplitude curves. The family is represented by different couples of solutions associated with different numbers of vibration half cycles between any two consecutive pulses. Poincaré sections showed that the oscillator can respond quite chaotically when shifting from the period-amplitude curves. Full article
(This article belongs to the Special Issue Asymptotic Methods in the Mechanics and Nonlinear Dynamics)
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<p>Non-smooth periodic basis.</p>
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<p>Geometrical interpretation of the particular case with a sine-wave temporal symmetry: observing the coordinate x does not reveal which of the two temporal variables, τ or t, is ‘in play’.</p>
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<p>(<b>a</b>) Possible smooth fitting curve (20) approximating the restoring force of combined springs including the amplitude limiters, and (<b>b</b>) moving platform periodically strikes the perfectly stiff walls creating the impulsive inertia load on the oscillator in the moving noninertial frame; it is assumed that both spatial and temporal variables are appropriately scaled.</p>
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<p>First seven amplitude-period curves (22) and (23) of the oscillator at (<b>a</b>): <math display="inline"><semantics> <mrow> <mi>F</mi> <mo>=</mo> <mn>2.0</mn> </mrow> </semantics></math>, first seven branches are shown, and (<b>b</b>): <math display="inline"><semantics> <mrow> <mi>F</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>, first 21 branches are shown.</p>
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<p>Time histories of the oscillator’ response near the minimum amplitude parameter A = 1.12: k = 1 (<b>a</b>,<b>b</b>); k = 2 (<b>c</b>,<b>d</b>); k = 3 (<b>e</b>,<b>f</b>); the left and right columns correspond to the lower and upper branches of loops shown in <a href="#symmetry-11-01420-f004" class="html-fig">Figure 4</a>.</p>
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<p>Time histories of the oscillator’ response near the minimum amplitude parameter A = 1.12: k = 1 (<b>a</b>,<b>b</b>); k = 2 (<b>c</b>,<b>d</b>); k = 3 (<b>e</b>,<b>f</b>); the left and right columns correspond to the lower and upper branches of loops shown in <a href="#symmetry-11-01420-f004" class="html-fig">Figure 4</a>.</p>
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<p>Time histories of the oscillator’ response near the minimum amplitude parameter A = 1.1708: k = 1 (<b>a</b>,<b>b</b>); k = 2 (<b>c</b>,<b>d</b>); k = 3 (<b>e</b>,<b>f</b>); the left and right columns correspond to the lower and upper branches of the loops shown in <a href="#symmetry-11-01420-f004" class="html-fig">Figure 4</a>.</p>
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<p>Time histories of the oscillator’ response near the minimum amplitude parameter A = 1.1708: k = 1 (<b>a</b>,<b>b</b>); k = 2 (<b>c</b>,<b>d</b>); k = 3 (<b>e</b>,<b>f</b>); the left and right columns correspond to the lower and upper branches of the loops shown in <a href="#symmetry-11-01420-f004" class="html-fig">Figure 4</a>.</p>
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<p>Case k = 1, larger amplitude parameter A = 1.4708: (<b>a</b>) corresponds to the lower part of the loop, and (<b>b</b>) corresponds the upper part of the loop shown in <a href="#symmetry-11-01420-f004" class="html-fig">Figure 4</a> for k = 1.</p>
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<p>Poincaré sections at (<b>a</b>): T = 0.25; F = 2.0; ζ = 0.0001, and (<b>b</b>): T = 0.5; F = 2.0; ζ = 0.0001; (<b>c</b>): T = 0.25; F = 0.6; ζ = 0.0001; (<b>d</b>): T = 0. 5; F = 0.6; ζ = 0.0001; (<b>e</b>): T = 0.25; F = 2.0; ζ = 0.05; (<b>f</b>): T = 0.5; F = 2.0; ζ = 0.05; snapshots are taken once per period at time of negative pulses.</p>
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<p>Poincaré sections at (<b>a</b>): T = 0.25; F = 2.0; ζ = 0.0001, and (<b>b</b>): T = 0.5; F = 2.0; ζ = 0.0001; (<b>c</b>): T = 0.25; F = 0.6; ζ = 0.0001; (<b>d</b>): T = 0. 5; F = 0.6; ζ = 0.0001; (<b>e</b>): T = 0.25; F = 2.0; ζ = 0.05; (<b>f</b>): T = 0.5; F = 2.0; ζ = 0.05; snapshots are taken once per period at time of negative pulses.</p>
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<p>Poincaré sections at (<b>a</b>): T = 4.5; F = 2.0; ζ = 0.01, and (<b>b</b>): T = 8.5; F = 2.0; ζ = 0.01; snapshots are taken once per period at time of negative pulses.</p>
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11 pages, 354 KiB  
Article
Lorentz Violation Footprints in the Spectrum of High-Energy Cosmic Neutrinos—Deformation of the Spectrum of Superluminal Neutrinos from Electron-Positron Pair Production in Vacuum
by José Manuel Carmona, José Luis Cortés, José Javier Relancio and Maykoll Anthonny Reyes
Symmetry 2019, 11(11), 1419; https://doi.org/10.3390/sym11111419 - 16 Nov 2019
Cited by 9 | Viewed by 2718
Abstract
The observation of cosmic neutrinos up to 2 PeV is used to put bounds on the energy scale of Lorentz invariance violation through the loss of energy due to the production of e + e pairs in the propagation of superluminal neutrinos. [...] Read more.
The observation of cosmic neutrinos up to 2 PeV is used to put bounds on the energy scale of Lorentz invariance violation through the loss of energy due to the production of e + e pairs in the propagation of superluminal neutrinos. A model to study this effect, which allows us to understand qualitatively the results of numerical simulations, is presented. Full article
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<p>Neutrino disintegration through vacuum electron-positron pair emission (VPE).</p>
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<p>Logarithmic representation of the flux of neutrinos for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>.</p>
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<p>Logarithmic representation of the flux of neutrinos for <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>.</p>
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8 pages, 328 KiB  
Article
The Grimus–Neufeld Model with FlexibleSUSY at One-Loop
by Simonas Draukšas, Vytautas Dūdėnas, Thomas Gajdosik, Andrius Juodagalvis, Paulius Juodsnukis and Darius Jurčiukonis
Symmetry 2019, 11(11), 1418; https://doi.org/10.3390/sym11111418 - 16 Nov 2019
Viewed by 2530
Abstract
The Grimus–Neufeld model can explain the smallness of measured neutrino masses by extending the Standard Model with a single heavy neutrino and a second Higgs doublet, using the seesaw mechanism and radiative mass generation. The Grimus–Lavoura approximation allows us to calculate the light [...] Read more.
The Grimus–Neufeld model can explain the smallness of measured neutrino masses by extending the Standard Model with a single heavy neutrino and a second Higgs doublet, using the seesaw mechanism and radiative mass generation. The Grimus–Lavoura approximation allows us to calculate the light neutrino masses analytically. By inverting these analytic expressions, we determine the neutrino Yukawa couplings from the measured neutrino mass differences and the neutrino mixing matrix. Short-cutting the full renormalization of the model, we implement the Grimus–Neufeld model in the spectrum calculator FlexibleSUSY and check the consistency of the implementation. These checks hint that FlexibleSUSY is able to do the job of numerical renormalization in a restricted parameter space. As a summary, we also comment on further steps of the implementation and the use of FlexibleSUSY for the model. Full article
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<p>Feynman diagrams contributing to the self-energies of the light neutrinos. For the correction to the mass, the internal fermion line has to be a Majorana propagator with a mass insertion; hence, charged particles will not contribute to <math display="inline"><semantics> <mrow> <mi>δ</mi> <msub> <mi>M</mi> <mi>L</mi> </msub> </mrow> </semantics></math> at this loop level.</p>
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8 pages, 257 KiB  
Article
On Some Sufficient Conditions for a Function to Be p-Valent Starlike
by Mamoru Nunokawa, Janusz Sokół and Edyta Trybucka
Symmetry 2019, 11(11), 1417; https://doi.org/10.3390/sym11111417 - 15 Nov 2019
Viewed by 1735
Abstract
A function f analytic in a domain D C is called p-valent in D, if for every complex number w, the equation f ( z ) = w has at most p roots in D, so that there [...] Read more.
A function f analytic in a domain D C is called p-valent in D, if for every complex number w, the equation f ( z ) = w has at most p roots in D, so that there exists a complex number w 0 such that the equation f ( z ) = w 0 has exactly p roots in D. The aim of this paper is to establish some sufficient conditions for a function analytic in the unit disc D to be p-valent starlike in D or to be at most p-valent in D . Our results are proved mainly by applying Nunokawa’s lemmas. Full article
14 pages, 5658 KiB  
Article
Study of Indoor Ventilation Based on Large-Scale DNS by a Domain Decomposition Method
by Junyang Jiang, Zichao Jiang, Trevor Hocksun Kwan, Chun-Ho Liu and Qinghe Yao
Symmetry 2019, 11(11), 1416; https://doi.org/10.3390/sym11111416 - 15 Nov 2019
Cited by 3 | Viewed by 2817
Abstract
This paper presents a large-scale Domain Decomposition Method (DDM) based Direct Numerical Simulation (DNS) for predicting the behavior of indoor airflow, where the aim is to design a comfortable and efficient indoor air environment of modern buildings. An analogy of the single-phase convection [...] Read more.
This paper presents a large-scale Domain Decomposition Method (DDM) based Direct Numerical Simulation (DNS) for predicting the behavior of indoor airflow, where the aim is to design a comfortable and efficient indoor air environment of modern buildings. An analogy of the single-phase convection problems is applied, and the pressure stabilized domain decomposition method is used to symmetrize the linear systems of Navier-Stokes equations and the convection-diffusion equation. Furthermore, a balancing preconditioned conjugate gradient method is utilized to deal with the interface problem caused by domain decomposition. The entire simulation model is validated by comparing the numerical results with that of recognized experimental and numerical data from previous literature. The transient behavior of indoor airflow and its complexity in the ventilated room are discussed; the velocity and vortex distribution of airflow are investigated, and its possible influence on particle accumulation is classified. Full article
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<p>Parallel efficiency (<b>a</b>) and speed up (<b>b</b>) of the current algorithm.</p>
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<p>An indoor ventilation model.</p>
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<p>details of meshing: front view (upper) and top view (lower).</p>
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<p>Vectors of flow velocity, the color bar number represents the velocity magnitude (m/s).</p>
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<p>Comparison of velocity along Line 1 (<b>left</b>) and Line 2 (<b>right</b>).</p>
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<p>Streamline at 30 s.</p>
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<p>Isosurface of vortex field at 30 s (<b>a</b>) vortex contour in the plane Y = 0.2285 m (<b>b</b>).</p>
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<p>Isosurface of vortex field at 30 s (<b>a</b>) vortex contour in the plane Y = 0.2285 m (<b>b</b>).</p>
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13 pages, 355 KiB  
Article
An E-Sequence Approach to the 3x + 1 Problem
by Sanmin Wang
Symmetry 2019, 11(11), 1415; https://doi.org/10.3390/sym11111415 - 15 Nov 2019
Viewed by 2067
Abstract
For any odd positive integer x, define ( x n ) n 0 and ( a n ) n 1 by setting [...] Read more.
For any odd positive integer x, define ( x n ) n 0 and ( a n ) n 1 by setting x 0 = x ,   x n = 3 x n 1 + 1 2 a n such that all x n are odd. The 3 x + 1 problem asserts that there is an x n = 1 for all x. Usually, ( x n ) n 0 is called the trajectory of x. In this paper, we concentrate on ( a n ) n 1 and call it the E-sequence of x. The idea is that we generalize E-sequences to all infinite sequences ( a n ) n 1 of positive integers and consider all these generalized E-sequences. We then define ( a n ) n 1 to be Ω -convergent to x if it is the E-sequence of x and to be Ω -divergent if it is not the E-sequence of any odd positive integer. We prove a remarkable fact that the Ω -divergence of all non-periodic E-sequences implies the periodicity of ( x n ) n 0 for all x 0 . The principal results of this paper are to prove the Ω -divergence of several classes of non-periodic E-sequences. Especially, we prove that all non-periodic E-sequences ( a n ) n 1 with lim ¯ n b n n > log 2 3 are Ω -divergent by using Wendel’s inequality and the Matthews and Watts’ formula x n = 3 n x 0 2 b n k = 0 n 1 ( 1 + 1 3 x k ) , where b n = k = 1 n a k . These results present a possible way to prove the periodicity of trajectories of all positive integers in the 3 x + 1 problem, and we call it the E-sequence approach. Full article
(This article belongs to the Special Issue Symmetry and Dynamical Systems)
16 pages, 3043 KiB  
Article
Dynamic Soft Sensor Development for Time-Varying and Multirate Data Processes Based on Discount and Weighted ARMA Models
by Longhao Li and Yongshou Dai
Symmetry 2019, 11(11), 1414; https://doi.org/10.3390/sym11111414 - 15 Nov 2019
Cited by 3 | Viewed by 2541
Abstract
To solve the soft sensor modeling (SSMI) problem in a nonlinear chemical process with dynamic time variation and multi-rate data, this paper proposes a dynamic SSMI method based on an autoregressive moving average (ARMA) model of weighted process data with discount (DSSMI-AMWPDD) and [...] Read more.
To solve the soft sensor modeling (SSMI) problem in a nonlinear chemical process with dynamic time variation and multi-rate data, this paper proposes a dynamic SSMI method based on an autoregressive moving average (ARMA) model of weighted process data with discount (DSSMI-AMWPDD) and optimization methods. For the sustained influence of auxiliary variable data on the dominant variables, the ARMA model structure is adopted. To reduce the complexity of the model, the dynamic weighting model is combined with the ARMA model. To address the weights of auxiliary variable data with different sampling frequencies, a calculation method for AMWPDD is proposed using assumptions that are suitable for most sequential chemical processes. The proposed method can obtain a discount factor value (DFV) of auxiliary variable data, realizing the dynamic fusion of chemical process data. Particle swarm optimization (PSO) is employed to optimize the soft sensor model parameters. To address the poor convergence problem of PSO, ω-dynamic PSO (ωDPSO) is used to improve the PSO convergence via the dynamic fluctuation of the inertia weight. A continuous stirred tank reactor (CSTR) simulation experiment was performed. The results show that the proposed DSSMI-AMWPDD method can effectively improve the SSM prediction accuracy for a nonlinear time-varying chemical process. The AMWPDD proposed in this paper can reflect the dynamic change of chemical process and improve the accuracy of SSM data prediction. The ω dynamic PSO method proposed in this paper has faster convergence speed and higher convergence accuracy, thus, these models correlate with the concept of symmetry. Full article
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<p>Irregular quality sample in the chemical process.</p>
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<p>Multipoint input ARMA model structure.</p>
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<p>Dynamic weighted ARMA model structure.</p>
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<p>Discount-weighted ARMA model structure.</p>
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<p>Dynamic adjustment of inertia weight <span class="html-italic">ω</span> in 100 iterations.</p>
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<p>The principle of the CSTR.</p>
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<p>Variation pattern of catalyst activity <span class="html-italic">k</span><sub>0</sub>.</p>
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<p>Modeling data training for the different SSMI methods. (<b>a</b>) The training curve based on LSSVM; (<b>b</b>) The training curve based on PSO-LSSVM; (<b>c</b>) The training curve based on <span class="html-italic">ω</span>DPSO-LSSVM.</p>
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<p>Prediction of test data by the different SSMI methods. (<b>a</b>) The prediction curve based on LSSVM; (<b>b</b>) The prediction curve based on PSO-LSSVM; (<b>c</b>) The prediction curve based on <span class="html-italic">ω</span>DPSO-LSSVM.</p>
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<p>Modeling data training for the different SSMI methods. (<b>a</b>) The training curve based on LSSVM; (<b>b</b>) The training curve based on PSO-LSSVM; (<b>c</b>) The training curve based on <span class="html-italic">ω</span>DPSO-LSSVM.</p>
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<p>Prediction of test data by the different SSMI methods. (<b>a</b>) The prediction curve based on LSSVM; (<b>b</b>) The prediction curve based on PSO-LSSVM; (<b>c</b>) The prediction curve based on <span class="html-italic">ω</span>DPSO-LSSVM.</p>
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20 pages, 431 KiB  
Article
Precanonical Structure of the Schrödinger Wave Functional of a Quantum Scalar Field in Curved Space-Time
by Igor V. Kanatchikov
Symmetry 2019, 11(11), 1413; https://doi.org/10.3390/sym11111413 - 15 Nov 2019
Cited by 5 | Viewed by 2363
Abstract
The functional Schrödinger representation of a nonlinear scalar quantum field theory in curved space-time is shown to emerge as a singular limit from the formulation based on precanonical quantization. The previously established relationship between the functional Schrödinger representation and precanonical quantization is extended [...] Read more.
The functional Schrödinger representation of a nonlinear scalar quantum field theory in curved space-time is shown to emerge as a singular limit from the formulation based on precanonical quantization. The previously established relationship between the functional Schrödinger representation and precanonical quantization is extended to arbitrary curved space-times. In the limiting case when the inverse of the ultraviolet parameter ϰ introduced by precanonical quantization is mapped to the infinitesimal invariant spatial volume element, the canonical functional derivative Schrödinger equation is derived from the manifestly covariant partial derivative precanonical Schrödinger equation. The Schrödinger wave functional is expressed as the trace of the multidimensional spatial product integral of Clifford-algebra-valued precanonical wave function or the product integral of a scalar function obtained from the precanonical wave function by a sequence of transformations. In non-static space-times, the transformations include a nonlocal transformation given by the time-ordered exponential of the zero-th component of spin-connection. Full article
21 pages, 6094 KiB  
Article
Enhanced Membrane Computing Algorithm for SAT Problems Based on the Splitting Rule
by Le Hao and Jun Liu
Symmetry 2019, 11(11), 1412; https://doi.org/10.3390/sym11111412 - 15 Nov 2019
Cited by 3 | Viewed by 2143
Abstract
Boolean propositional satisfiability (SAT) problem is one of the most widely studied NP-complete problems and plays an outstanding role in many domains. Membrane computing is a branch of natural computing which has been proven to solve NP problems in polynomial time with a [...] Read more.
Boolean propositional satisfiability (SAT) problem is one of the most widely studied NP-complete problems and plays an outstanding role in many domains. Membrane computing is a branch of natural computing which has been proven to solve NP problems in polynomial time with a parallel compute mode. This paper proposes a new algorithm for SAT problem which combines the traditional membrane computing algorithm of SAT problem with a classic simplification rule, the splitting rule, which can divide a clause set into two axisymmetric subsets, deal with them respectively and simultaneously, and obtain the solution of the original clause set with the symmetry of their solutions. The new algorithm is shown to be able to reduce the space complexity by distributing clauses with the splitting rule repeatedly, and also reduce both time and space complexity by executing one-literal rule and pure-literal rule as many times as possible. Full article
(This article belongs to the Special Issue Symmetry and Complexity 2019)
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Graphical abstract

Graphical abstract
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<p>Process diagram of the traditional membrane computing algorithm of SAT problems, of which m is the number of given clauses, n is the number of the given clause set’s atoms.</p>
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<p>Initial membrane structure of the algorithm.</p>
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<p>Flow chart of the algorithm.</p>
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<p>The initial membrane structure of the given clause set.</p>
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<p>The membrane structure during calculation (1).</p>
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<p>The membrane structure during calculation (2).</p>
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<p>The membrane structure during calculation (3).</p>
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<p>The membrane structure during calculation (4).</p>
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<p>The membrane structure during calculation (5).</p>
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<p>The membrane structure during calculation (6).</p>
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<p>The membrane structure during calculation (7).</p>
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<p>The membrane structure during calculation (8).</p>
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<p>The membrane structure during calculation (9).</p>
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<p>The membrane structure during calculation (10).</p>
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<p>The membrane structure during calculation (11).</p>
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<p>The membrane structure during calculation (12).</p>
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<p>The membrane structure during calculation (13).</p>
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<p>The membrane structure during calculation (14).</p>
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<p>The membrane structure during calculation (15).</p>
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<p>The membrane structure during calculation (16).</p>
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<p>The membrane structure during calculation (17).</p>
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<p>The membrane structure during calculation (18).</p>
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16 pages, 507 KiB  
Article
Algebraic Properties of the Block Cipher DESL
by Kenneth Matheis, Rainer Steinwandt and Adriana Suárez Corona
Symmetry 2019, 11(11), 1411; https://doi.org/10.3390/sym11111411 - 15 Nov 2019
Cited by 4 | Viewed by 2640
Abstract
The Data Encryption Standard Lightweight extension (DESL) is a lightweight block cipher which is very similar to DES, but unlike DES uses only a single S-box. This work demonstrates that this block cipher satisfies comparable algebraic properties to DES—namely, the round functions of [...] Read more.
The Data Encryption Standard Lightweight extension (DESL) is a lightweight block cipher which is very similar to DES, but unlike DES uses only a single S-box. This work demonstrates that this block cipher satisfies comparable algebraic properties to DES—namely, the round functions of DESL generate the alternating group and both ciphers resist multiple right-hand sides attacks. Full article
(This article belongs to the Special Issue Interactions between Group Theory, Symmetry and Cryptology)
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<p>Data Encryption Standard Lightweight extension (DESL) overview.</p>
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<p>Equivalent description of DESL with the permutation <span class="html-italic">P</span> being applied before the expansion function <span class="html-italic">E</span>.</p>
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<p>Agreeing1 algorithm.</p>
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<p>Definition of <math display="inline"><semantics> <mrow> <mi>I</mi> <mo>(</mo> <mi>j</mi> <mo>)</mo> </mrow> </semantics></math>.</p>
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<p>Definition of <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>(</mo> <mi>j</mi> <mo>)</mo> </mrow> </semantics></math>.</p>
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15 pages, 1117 KiB  
Article
Modified Power-Symmetric Distribution
by Emilio Gómez-Déniz, Yuri A. Iriarte, Enrique Calderín-Ojeda and Héctor W. Gómez
Symmetry 2019, 11(11), 1410; https://doi.org/10.3390/sym11111410 - 15 Nov 2019
Cited by 4 | Viewed by 3118
Abstract
In this paper, a general class of modified power-symmetric distributions is introduced. By choosing as symmetric model the normal distribution, the modified power-normal distribution is obtained. For the latter model, some of its more relevant statistical properties are examined. Parameters estimation is carried [...] Read more.
In this paper, a general class of modified power-symmetric distributions is introduced. By choosing as symmetric model the normal distribution, the modified power-normal distribution is obtained. For the latter model, some of its more relevant statistical properties are examined. Parameters estimation is carried out by using the method of moments and maximum likelihood estimation. A simulation analysis is accomplished to study the performance of the maximum likelihood estimators. Finally, we compare the efficiency of the modified power-normal distribution with other existing distributions in the literature by using a real dataset. Full article
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<p>Plot of the pdf of <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> distribution for selected values of the parameters.</p>
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<p>Plot of the first derivative of <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> distribution for selected values of the parameters.</p>
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<p>Plot of the <math display="inline"><semantics> <mrow> <mi mathvariant="double-struck">E</mi> <mo>(</mo> <mi>X</mi> <mo>)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi mathvariant="double-struck">V</mi> <mi>a</mi> <mi>r</mi> <mo>(</mo> <mi>X</mi> <mo>)</mo> </mrow> </semantics></math> of the <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> distribution.</p>
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<p>Graphs of the skewness and kurtosis coefficients for the <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> and <math display="inline"><semantics> <mi mathvariant="script">PN</mi> </semantics></math> distributions.</p>
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<p><b>Left</b> panel: Histogram of the empirical distribution and fitted densities by ML superimposed for pollen dataset. <b>Right</b> panel: Plots of the tails for the four models.</p>
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<p>QQ-plots: (<b>a</b>) <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> model; (<b>b</b>) <math display="inline"><semantics> <mi mathvariant="script">PN</mi> </semantics></math> model; (<b>c</b>) <math display="inline"><semantics> <mi mathvariant="script">SN</mi> </semantics></math> model; (<b>d</b>) <math display="inline"><semantics> <mi mathvariant="script">TS</mi> </semantics></math> model.</p>
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<p>Profile log-likelihood of <math display="inline"><semantics> <mi>μ</mi> </semantics></math>, <math display="inline"><semantics> <mi>σ</mi> </semantics></math> and <math display="inline"><semantics> <mi>α</mi> </semantics></math> for the <math display="inline"><semantics> <mi mathvariant="script">MPN</mi> </semantics></math> distribution.</p>
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22 pages, 5959 KiB  
Article
Bat Optimized Link State Routing Protocol for Energy-Aware Mobile Ad-Hoc Networks
by Mohammed Ahmed Jubair, Salama A. Mostafa, Ravie Chandren Muniyandi, Hairulnizam Mahdin, Aida Mustapha, Mustafa Hamid Hassan, Moamin A. Mahmoud, Yasir Amer Al-Jawhar, Ahmed Salih Al-Khaleefa and Ahmed Jubair Mahmood
Symmetry 2019, 11(11), 1409; https://doi.org/10.3390/sym11111409 - 15 Nov 2019
Cited by 51 | Viewed by 5868
Abstract
Mobile ad hoc network (MANET) can be described as a group of wireless mobile nodes that form a temporary dynamic and independent infrastructure network or a central administration facility. High energy consumption is one of the main problems associated with the MANET technology. [...] Read more.
Mobile ad hoc network (MANET) can be described as a group of wireless mobile nodes that form a temporary dynamic and independent infrastructure network or a central administration facility. High energy consumption is one of the main problems associated with the MANET technology. The wireless mobile nodes used in this process rely on batteries because the network does not have a steady power supply. Thus, the rapid battery drain reduces the lifespan of the network. In this paper, a new Bat Optimized Link State Routing (BOLSR) protocol is proposed to improve the energy usage of the Optimized Link State Routing (OLSR) protocol in the MANET. The symmetry between OLSR of MANET and Bat Algorithm (BA) is that both of them use the same mechanism for finding the path via sending and receiving specific signals. This symmetry resulted in the BOLSR protocol that determines the optimized path from a source node to a destination node according to the energy dynamics of the nodes. The BOLSR protocol is implemented in a MANET simulation by using MATLAB toolbox. Different scenarios are tested to compare the BOLSR protocol with the Cellular Automata African Buffalo Optimization (CAABO), Energy-Based OLSR (EBOLSR), and the standard OLSR. The performance metric consists of routing overhead ratios, energy consumption, and end-to-end delay which is applied to evaluate the performance of the routing protocols. The results of the tests reveal that the BOLSR protocol reduces the energy consumption and increases the lifespan of the network, compared with the CAABO, EBOLSR, and OLSR. Full article
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<p>An example of a mobile ad-hoc network.</p>
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<p>Flooding mechanism with/without Multipoint Relay (MPR) [<a href="#B39-symmetry-11-01409" class="html-bibr">39</a>]. (<b>a</b>) Flooding a packet in a wireless multi-hop network; (<b>b</b>) flooding a packet in a wireless multi-hop network from using MPRs (marker in black).</p>
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<p>The mechanism of the Optimized Link State Routing (OLSR) routing process.</p>
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<p>An overview of the bat algorithm.</p>
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<p>The optimization scheme of the protocol.</p>
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<p>Snapshot of the simulation.</p>
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<p>The mobile ad hoc network (MANET) simulation model.</p>
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<p>Routing overhead ratio (ROR) vs. No. of nodes.</p>
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<p>Energy Consumption (EC) vs. No. of nodes.</p>
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<p>End-To-End (E2E) delay vs. No. of nodes.</p>
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<p>ROR vs. node speed.</p>
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<p>EC vs. node speed.</p>
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<p>E2E delay vs. node speed.</p>
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<p>The ROR vs. simulation time.</p>
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<p>The EC vs. simulation time.</p>
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<p>E2E delay vs. simulation time.</p>
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11 pages, 914 KiB  
Article
Deep Recurrent Neural Network and Data Filtering for Rumor Detection on Sina Weibo
by Yichun Xu, Chen Wang, Zhiping Dan, Shuifa Sun and Fangmin Dong
Symmetry 2019, 11(11), 1408; https://doi.org/10.3390/sym11111408 - 15 Nov 2019
Cited by 18 | Viewed by 3368
Abstract
Social media makes it easy for individuals to publish and consume news, but it also facilitates the spread of rumors. This paper proposes a novel deep recurrent neural model with a symmetrical network architecture for automatic rumor detection in social media such as [...] Read more.
Social media makes it easy for individuals to publish and consume news, but it also facilitates the spread of rumors. This paper proposes a novel deep recurrent neural model with a symmetrical network architecture for automatic rumor detection in social media such as Sina Weibo, which shows better performance than the existing methods. In the data preparing phase, we filter the posts according to the followers of the user. We then use sequential encoding for the posts and multiple embedding layers to get better feature representation, and multiple recurrent neural network layers to capture the dynamic temporal signals characteristic. The experimental results on the Sina Weibo dataset show that: 1. the sequential encoding performs better than the term frequency-inverse document frequency (TF-IDF) or the doc2vec encoding scheme; 2. the model is more accurate when trained on the posts from the users with more followers; and 3. the model achieves superior improvements over the existing works on the accuracy of detection, including the early detection. Full article
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<p>Number of posts published at different times (<b>a</b>) and number of posts published by the users with different numbers of followers (<b>b</b>).</p>
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<p>Deep recurrent neural network (DRNN) architecture.</p>
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<p>The accuracy of three models on different data subsets.</p>
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<p>Performance of the proposed models and GRU-2 in [<a href="#B11-symmetry-11-01408" class="html-bibr">11</a>] for the early detection. (<b>a</b>) The accuracy of each model; and (<b>b</b>) LSTM and GRU models converge faster than SRNN.</p>
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17 pages, 799 KiB  
Article
Normal-G Class of Probability Distributions: Properties and Applications
by Fábio V. J. Silveira, Frank Gomes-Silva, Cícero C. R. Brito, Moacyr Cunha-Filho, Felipe R. S. Gusmão and Sílvio F. A. Xavier-Júnior
Symmetry 2019, 11(11), 1407; https://doi.org/10.3390/sym11111407 - 15 Nov 2019
Cited by 5 | Viewed by 2728
Abstract
In this paper, we propose a novel class of probability distributions called Normal-G. It has the advantage of demanding no additional parameters besides those of the parent distribution, thereby providing parsimonious models. Furthermore, the class enjoys the property of identifiability whenever [...] Read more.
In this paper, we propose a novel class of probability distributions called Normal-G. It has the advantage of demanding no additional parameters besides those of the parent distribution, thereby providing parsimonious models. Furthermore, the class enjoys the property of identifiability whenever the baseline is identifiable. We present special Normal-G sub-models, which can fit asymmetrical data with either positive or negative skew. Other important mathematical properties are described, such as the series expansion of the probability density function (pdf), which is used to derive expressions for the moments and the moment generating function (mgf). We bring Monte Carlo simulation studies to investigate the behavior of the maximum likelihood estimates (MLEs) of two distributions generated by the class and we also present applications to real datasets to illustrate its usefulness. Full article
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<p>Plots of pdf and hrf for the Normal-Weibull distribution.</p>
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<p>Skewness of the Normal-Weibull distribution.</p>
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<p>Plots of pdf and hrf for the Normal-log-logistic distribution.</p>
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<p>Skewness of the Normal-log-logistic distribution.</p>
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<p>Histogram of soil fertility dataset and fitted densities.</p>
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<p>Histogram of eruption dataset and fitted densities.</p>
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16 pages, 350 KiB  
Article
Ideals of Numerical Semigroups and Error-Correcting Codes
by Maria Bras-Amorós
Symmetry 2019, 11(11), 1406; https://doi.org/10.3390/sym11111406 - 14 Nov 2019
Cited by 2 | Viewed by 2559
Abstract
Several results relating additive ideals of numerical semigroups and algebraic-geometry
codes are presented. In particular, we deal with the set of non-redundant parity-checks, the code
length, the generalized Hamming weights, and the isometry-dual sequences of algebraic-geometry
codes from the perspective of the related [...] Read more.
Several results relating additive ideals of numerical semigroups and algebraic-geometry
codes are presented. In particular, we deal with the set of non-redundant parity-checks, the code
length, the generalized Hamming weights, and the isometry-dual sequences of algebraic-geometry
codes from the perspective of the related Weierstrass semigroups. These results are related to
cryptographic problems such as the wire-tap channel, t-resilient functions, list-decoding, network
coding, and ramp secret sharing schemes. Full article
(This article belongs to the Special Issue Interactions between Group Theory, Symmetry and Cryptology)
17 pages, 5231 KiB  
Article
Lattice-Boltzmann and Eulerian Hybrid for Solid Burning Simulation
by Eunchan Jo, Byungmoon Kim and Oh-Young Song
Symmetry 2019, 11(11), 1405; https://doi.org/10.3390/sym11111405 - 14 Nov 2019
Cited by 1 | Viewed by 3251
Abstract
We propose a new hybrid simulation method to model burning solid interactions. Unlike gas fuel, fire and smoke interactions that have been relatively well studied in the past, simulations of solid fuel combustion processes remain largely unaddressed. These include pyrolysis/smoldering, interactions with oxygen [...] Read more.
We propose a new hybrid simulation method to model burning solid interactions. Unlike gas fuel, fire and smoke interactions that have been relatively well studied in the past, simulations of solid fuel combustion processes remain largely unaddressed. These include pyrolysis/smoldering, interactions with oxygen and flow inside porous solid. To advance this simulation problem, we designed a new hybrid of the Lattice-Boltzmann method (LBM) and a Eulerian grid based Navier-Stokes equation (NSE). It uses the LBM, which has symmetrical directions of particle velocities in a cell, for inside the solid fuel and the NSE, which has a representative velocity in a cell, for outside the solid. At the interface where the two methods join, we develop a novel method to exchange physical quantities and show a natural transition between the two methods. Since LBM allows us to directly manage the quantity of exchanges from the microscopic perspective, that is, between lattice points, we can easily simulate the burning speed and the shape change of burning an inhomogeneous solid. Also, we derive an LBM version of the previously proposed porous Navier-Stokes equation to simulate gas flow inside the porous solid. In addition, we use the NS solver outside the solid where macroscopic behavior is much more dominant and, hence, LBM is less efficient than NS solver. Our results show us the physical stability and accuracy and visual realism. Full article
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<p>Illustration of physical quantity exchanges across LBM and NSE interface. Upper row is the LBM domain and bottom row is the NSE domain. The macroscopic value (green row) from LBM is required for evolution of the NSE grid cell <span class="html-italic">B</span>. The value of the NSE grid cell has to decompose for the streaming of the LBM grid cell <math display="inline"><semantics> <mi>β</mi> </semantics></math>.</p>
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<p>Weighting function for temperature streaming.</p>
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<p>Wood burning simulation in 3D. The wood is eroded by the collaboration of velocity fields computed in the NSE field, weighted streaming into solid domain (NSE to LBM) and solid-internal flows simulated by LBM.</p>
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<p>The leftmost image is flow obtained by the NS solver that shows strong vorticity formation. The rest of the three images was done by porous LBM with a uniform porosity of 0.9 and a permeability coefficient of 1000, 1 and 0.001, respectively.</p>
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<p>NS and LBM comparison experiment. Upper images are 3 s, 12 s and 30 s using NS solver. Lower images are 15 s, 40 s and 80 s using LBM solver.</p>
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<p>Pyrolysis experiment. Solid fuel is burned by heat underneath and produces charcoal shown in black and gas fuel shown in green. On the right image, burnt wood, on the left, charcoal. However, the temperature is low enough so that gas fuel does not start the combustion process and charcoal smoldering is minimal. Note that the LBM domain includes charcoal in black color including heated in red near the heat source.</p>
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<p>Upper row is burning with oxygen, where we can observe that the oxygen rich region burns first, while in the lower row where oxygen is not considered, burning is less natural and interesting.</p>
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<p>Upper row has low permeability, where flow inside wood is minimal. In the lower row where permeability high, flow occurs naturally across the two simulation domains. We can observe that the proposed hybrid boundary handling enables smoke exchanging flows towards inside and outside woods, and the proposed porous LBM method generates natural flow inside the wood.</p>
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<p>3D permeability test. Smoke passes through wood grain.</p>
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12 pages, 426 KiB  
Article
Volume Preserving Maps Between p-Balls
by Adrian Holhoş and Daniela Roşca
Symmetry 2019, 11(11), 1404; https://doi.org/10.3390/sym11111404 - 14 Nov 2019
Viewed by 1960
Abstract
We construct a volume preserving map U p from the p-ball B p ( r ) = x R 3 , x p r to the regular octahedron B 1 ( r ) , for arbitrary [...] Read more.
We construct a volume preserving map U p from the p-ball B p ( r ) = x R 3 , x p r to the regular octahedron B 1 ( r ) , for arbitrary p > 0 . Then we calculate the inverse U p 1 and we also deduce explicit expressions for U and U 1 . This allows us to construct volume preserving maps between arbitrary balls B p ( r ) and B p ( r ˜ ) , and also to map uniform and refinable grids between them. Finally we list some possible applications of our maps. Full article
(This article belongs to the Special Issue Symmetry in Applied Mathematics)
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<p>Some balls <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="script">B</mi> <mi>p</mi> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> for <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>0.75</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math> (<b>first line</b>) and <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>1.2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>p</mi> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math> (<b>second line</b>), respectively.</p>
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18 pages, 4161 KiB  
Article
Quasi-Periodic Oscillating Flows in a Channel with a Suddenly Expanded Section
by Takuya Masuda and Toshio Tagawa
Symmetry 2019, 11(11), 1403; https://doi.org/10.3390/sym11111403 - 13 Nov 2019
Cited by 4 | Viewed by 3899
Abstract
In this study, two-dimensional numerical simulation was carried out for an oscillatory flow between parallel flat plates having a suddenly expanded section. Governing equations were discretized with the second-order accuracy by a finite volume method on an unequal interval mesh system resolving finer [...] Read more.
In this study, two-dimensional numerical simulation was carried out for an oscillatory flow between parallel flat plates having a suddenly expanded section. Governing equations were discretized with the second-order accuracy by a finite volume method on an unequal interval mesh system resolving finer near walls and corners to obtain the characteristics of the oscillatory flow accurately. Amplitude spectrums of a velocity component were obtained to investigate the periodic characteristics of the oscillatory flow. At low Reynolds numbers, the flow is periodic because the spectrum mostly consists of harmonic components, and then at high Reynolds numbers, it transits to a quasi-periodic flow mixed with non-harmonic components. In conjunction with the periodic oscillation of a main flow, separation vortices that are not uniform in size are generated from the corner of a sudden contraction part and pass through a downstream region coming into contact with the wall. The number of the vortices decreases rapidly after they are generated, but the vortices are generated again in the downstream region. In order to specify where aperiodicity is generated, the turbulent kinetic energy is introduced, and it is decomposed into the harmonic and non-harmonic components. The peaks of the non-harmonic component are generated in the region of the expanded section. Full article
(This article belongs to the Special Issue Symmetry in Fluid Flow)
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Graphical abstract

Graphical abstract
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<p>Channel geometry and coordinates.</p>
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<p>Mesh structure of the finest mesh, Model C. This picture shows the range of 6 ≤ <span class="html-italic">x</span> ≤ 8 and 0.8 ≤ <span class="html-italic">y</span> ≤ 1.2.</p>
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<p>Time evolution of the velocity component <span class="html-italic">v</span> at (<span class="html-italic">x</span>, <span class="html-italic">y</span>) = (10, 0.5). (<b>a</b>) It was a periodic oscillating flow. At <span class="html-italic">Re</span> = 1400, as shown in (<b>b</b>), the local maximum is not constant, so it is a quasi-periodic oscillating flow with a modulated wave containing low frequency components. At <span class="html-italic">Re</span> = 1600, as shown in (<b>c</b>), in addition to having a waveform of a modulated wave, it is a quasi-periodic oscillating flow with irregular fluctuations. At <span class="html-italic">Re</span> = 2000, as shown in (<b>d</b>), the irregularity becomes even stronger.</p>
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<p>Amplitude spectrum |<span class="html-italic">V</span>(<span class="html-italic">f</span>)| of the velocity component <span class="html-italic">v</span> at (<span class="html-italic">x</span>, <span class="html-italic">y</span>) = (10, 0.5). (<b>a</b>) <span class="html-italic">Re</span> = 1200. (<b>b</b>) <span class="html-italic">Re</span> = 1400. (<b>c</b>) <span class="html-italic">Re</span> = 1600. (<b>d</b>) <span class="html-italic">Re</span> = 2000.</p>
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<p>Stream lines at <span class="html-italic">Re</span> = 2000, which represent the evolution process of a group of vortices. (<b>a</b>) <span class="html-italic">t</span> = 1531. (<b>b</b>) <span class="html-italic">t</span> = 1533. (<b>c</b>) <span class="html-italic">t</span> = 1538.</p>
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<p>Maximum of the wall shear stress <span class="html-italic">τ</span><sub>0</sub> at <span class="html-italic">y</span> = 1 during <span class="html-italic">t</span> = 1000–2000.</p>
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<p>Number of the vortices coming into contact with the wall at <span class="html-italic">y</span> = 1 during <span class="html-italic">t</span> = 1000–2000.</p>
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<p>Mesh structure of the non-matching mesh for Model E. This picture shows the range of −5 ≤ <span class="html-italic">x</span> ≤ 10 and 0 ≤ <span class="html-italic">y</span> ≤ 3.</p>
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<p>Stream lines in the channel with the sudden contraction part at <span class="html-italic">Re</span> = 4000 at a certain moment.</p>
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<p>Amplitude spectrum |<span class="html-italic">V</span>(<span class="html-italic">f</span>)| of the velocity component <span class="html-italic">v</span> in the channel with the sudden contraction part at (<span class="html-italic">x</span>, <span class="html-italic">y</span>) = (10, 0.5) at <span class="html-italic">Re</span> = 4000.</p>
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<p>The time-fluctuating velocity component <span class="html-italic">v′</span>, which was decomposed into the harmonic <span class="html-italic">v′<sub>H</sub></span> and the non-harmonic <span class="html-italic">v′<sub>N</sub></span> at (<span class="html-italic">x</span>, <span class="html-italic">y</span>) = (10, 0.5). (<b>a</b>) Fluctuation. (<b>b</b>) Harmonic. (<b>c</b>) Non-harmonic.</p>
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<p>Distributions of the turbulent kinetic energy <span class="html-italic">k</span>, which is decomposed into the harmonic component <span class="html-italic">k<sub>H</sub></span> and the non-harmonic component <span class="html-italic">k<sub>N</sub></span>.</p>
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14 pages, 262 KiB  
Article
Some Inequalities Using Generalized Convex Functions in Quantum Analysis
by Miguel J. Vivas-Cortez, Artion Kashuri, Rozana Liko and Jorge E. Hernández Hernández
Symmetry 2019, 11(11), 1402; https://doi.org/10.3390/sym11111402 - 13 Nov 2019
Cited by 22 | Viewed by 2417
Abstract
In the present work, the Hermite–Hadamard inequality is established in the setting of quantum calculus for a generalized class of convex functions depending on three parameters: a number in ( 0 , 1 ] and two arbitrary real functions defined on [...] Read more.
In the present work, the Hermite–Hadamard inequality is established in the setting of quantum calculus for a generalized class of convex functions depending on three parameters: a number in ( 0 , 1 ] and two arbitrary real functions defined on [ 0 , 1 ] . From the proven results, various inequalities of the same type are deduced for other types of generalized convex functions and the methodology used reveals, in a sense, a symmetric mathematical phenomenon. In addition, the definition of dominated convex functions with respect to the generalized class of convex functions aforementioned is introduced, and some integral inequalities are established. Full article
13 pages, 261 KiB  
Article
Spacetime and Deformations of Special Relativistic Kinematics
by José Manuel Carmona, José Luis Cortés and José Javier Relancio
Symmetry 2019, 11(11), 1401; https://doi.org/10.3390/sym11111401 - 12 Nov 2019
Cited by 14 | Viewed by 2446
Abstract
A deformation of special relativistic kinematics (possible signal of a theory of quantum gravity at low energies) leads to a modification of the notion of spacetime. At the classical level, this modification is required when one considers a model including single- or multi-interaction [...] Read more.
A deformation of special relativistic kinematics (possible signal of a theory of quantum gravity at low energies) leads to a modification of the notion of spacetime. At the classical level, this modification is required when one considers a model including single- or multi-interaction processes, for which absolute locality in terms of canonical spacetime coordinates is lost. We discuss the different alternatives for observable effects in the propagation of a particle over very large distances that emerge from the new notion of spacetime. A central ingredient in the discussion is the cluster decomposition principle, which can be used to favor some alternatives over the others. Full article
(This article belongs to the Special Issue Symmetry and Quantum Gravity)
22 pages, 2516 KiB  
Article
Novel Fuzzy Clustering Methods for Test Case Prioritization in Software Projects
by A. D. Shrivathsan, K. S. Ravichandran, R. Krishankumar, V. Sangeetha, Samarjit Kar, Pawel Ziemba and Jaroslaw Jankowski
Symmetry 2019, 11(11), 1400; https://doi.org/10.3390/sym11111400 - 12 Nov 2019
Cited by 10 | Viewed by 3704
Abstract
Systematic Regression Testing is essential for maintaining software quality, but the cost of regression testing is high. Test case prioritization (TCP) is a widely used approach to reduce this cost. Many researchers have proposed regression test case prioritization techniques, and clustering is one [...] Read more.
Systematic Regression Testing is essential for maintaining software quality, but the cost of regression testing is high. Test case prioritization (TCP) is a widely used approach to reduce this cost. Many researchers have proposed regression test case prioritization techniques, and clustering is one of the popular methods for prioritization. The task of selecting appropriate test cases and identifying faulty functions involves ambiguities and uncertainties. To alleviate the issue, in this paper, two fuzzy-based clustering techniques are proposed for TCP using newly derived similarity coefficient and dominancy measure. Proposed techniques adopt grouping technology for clustering and the Weighted Arithmetic Sum Product Assessment (WASPAS) method for ranking. Initially, test cases are clustered using similarity//dominancy measures, which are later prioritized using the WASPAS method under both inter- and intra-perspectives. The proposed algorithms are evaluated using real-time data obtained from Software-artifact Infrastructure Repository (SIR). On evaluation, it is inferred that the proposed algorithms increase the likelihood of selecting more relevant test cases when compared to the recent state-of-the-art techniques. Finally, the strengths of the proposed algorithms are discussed in comparison with state-of-the-art techniques. Full article
(This article belongs to the Special Issue Multi-Criteria Decision Aid methods in fuzzy decision problems)
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<p>The workflow of the proposed similarity-based test case prioritization (TCP).</p>
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<p>Area plot: (<b>a</b>) Average Percentage Fault Detection (APFD) measure for non-prioritization; (<b>b</b>) APFD measure for cluster-based similarity coefficient prioritization; and (<b>c</b>) APFD measure for cluster-based on prioritization.</p>
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<p>Input Gaussian Membership function.</p>
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<p>Box plot: (<b>a</b>) Performance analysis of the proposed methods and others—Pool 1; (<b>b</b>) Performance analysis of the proposed methods and others—Pool 2; (<b>c</b>) Performance analysis of the proposed methods and others—Pool 3; (<b>d</b>) Performance analysis of the proposed methods and others—Pool 4.</p>
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23 pages, 7663 KiB  
Article
A Haptic Model of Entanglement, Gauge Symmetries and Minimal Interaction Based on Knot Theory
by Stefan Heusler and Malte Ubben
Symmetry 2019, 11(11), 1399; https://doi.org/10.3390/sym11111399 - 12 Nov 2019
Cited by 4 | Viewed by 3952
Abstract
The Heegaard splitting of S U ( 2 ) is a particularly useful representation for quantum phases of spin j-representation arising in the mapping S 1 S 3, which can be related to ( 2 j , 2 ) torus [...] Read more.
The Heegaard splitting of S U ( 2 ) is a particularly useful representation for quantum phases of spin j-representation arising in the mapping S 1 S 3, which can be related to ( 2 j , 2 ) torus knots in Hilbert space. We show that transitions to homotopically equivalent knots can be associated with gauge invariance, and that the same mechanism is at the heart of quantum entanglement. In other words, (minimal) interaction causes entanglement. Particle creation is related to cuts in the knot structure. We show that inner twists can be associated with operations with the quaternions ( I , J , K ), which are crucial to understand the Hopf mapping S 3 S 2. We discuss the relationship between observables on the Bloch sphere S 2, and knots with inner twists in Hilbert space. As applications, we discuss selection rules in atomic physics, and the status of virtual particles arising in Feynman diagrams. Using a simple paper strip model revealing the knot structure of quantum phases in Hilbert space including inner twists, a h a p t i c model of entanglement and gauge symmetries is proposed, which may also be valid for physics education. Full article
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Figure 1

Figure 1
<p>Quantum tomography: For an ensemble of identical qubits, successive measurements lead to a random pattern with probabilities for ‘black’ (<math display="inline"><semantics> <mrow> <mo>+</mo> <mn>1</mn> </mrow> </semantics></math> eigenvalues) or ‘white’ (<math display="inline"><semantics> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math> eigenvalues) in the <math display="inline"><semantics> <mrow> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> </mrow> </semantics></math> direction, respectively. With <math display="inline"><semantics> <msubsup> <mi>p</mi> <mi>k</mi> <mo>+</mo> </msubsup> </semantics></math> as probability for ‘black’, and <math display="inline"><semantics> <msubsup> <mi>p</mi> <mi>k</mi> <mo>−</mo> </msubsup> </semantics></math> as probability for ‘white’, the relation <math display="inline"><semantics> <mrow> <msub> <mi>n</mi> <mi>k</mi> </msub> <mo>=</mo> <mi>tr</mi> <mrow> <mo stretchy="false">(</mo> <msub> <mi>σ</mi> <mi>k</mi> </msub> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msubsup> <mi>p</mi> <mi>k</mi> <mo>+</mo> </msubsup> <mo>−</mo> <msubsup> <mi>p</mi> <mi>k</mi> <mo>−</mo> </msubsup> </mrow> </semantics></math> holds. Here, <math display="inline"><semantics> <mrow> <mrow> <mi>ρ</mi> <mo>=</mo> <mo> </mo> <mo stretchy="false">|</mo> </mrow> <msub> <mn>0</mn> <mi>n</mi> </msub> <mrow> <mo>〉</mo> <mo>〈</mo> </mrow> <msub> <mn>0</mn> <mi>n</mi> </msub> <mrow> <mo stretchy="false">|</mo> </mrow> </mrow> </semantics></math> is the <math display="inline"><semantics> <mrow> <mn>2</mn> <mo>×</mo> <mn>2</mn> </mrow> </semantics></math> density matrix of the single qubit.</p>
Full article ">Figure 2
<p>The operation of the quaternions <math display="inline"><semantics> <mrow> <mi>I</mi> <mo>,</mo> <mi>J</mi> <mo>,</mo> <mi>K</mi> </mrow> </semantics></math> on the Dirac belt in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. Note that these operations lead to inner twists of the Dirac belt. In particular, for operation <math display="inline"><semantics> <mrow> <mi>I</mi> <mi>J</mi> <mi>K</mi> <mo>=</mo> <msup> <mi>e</mi> <mrow> <mn>2</mn> <mi>π</mi> <mo>/</mo> <mn>2</mn> </mrow> </msup> <mo>=</mo> <mo>−</mo> <mn>1</mn> </mrow> </semantics></math> leads to two inner twists.</p>
Full article ">Figure 3
<p>Left: Heegaard splitting of <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>, Right: Hopf mapping to the Bloch sphere. In <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>, a homotopic loop <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math> is considered ranging from <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>, which is mapped to a great circle <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math> traversed <math display="inline"><semantics> <mrow> <mi>t</mi> <mi>w</mi> <mi>i</mi> <mi>c</mi> <mi>e</mi> </mrow> </semantics></math> on the Bloch sphere <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>. The Dirac belt describing the quantum phase on the homotopic loop in <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math> is equivalent to a Möbius strip when the parts <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> separated in <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math> are ‘glued together’, [see also <a href="#symmetry-11-01399-f004" class="html-fig">Figure 4</a>]. Superposition of right- and left-twisted Möbius strips leads to a node on the Bloch sphere. The antipode of this node is called ‘direction of the spin’, describing the direction of maximal amplitude.</p>
Full article ">Figure 4
<p>The node on the Bloch sphere [in this case, the node at <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>2</mn> <mo>,</mo> <mi>ϕ</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math> arises due to superposition of the quantum phases <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <msqrt> <mn>2</mn> </msqrt> <mrow> <mo stretchy="false">(</mo> <msup> <mi>e</mi> <mrow> <mi>i</mi> <mi>ϕ</mi> <mo>/</mo> <mn>2</mn> </mrow> </msup> <mo>−</mo> <msup> <mi>e</mi> <mrow> <mo>−</mo> <mi>i</mi> <mi>ϕ</mi> <mo>/</mo> <mn>2</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math>]. In the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm, an infinite number of homotopically equivalent quantum phases in <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mn>1</mn> </msub> <mo stretchy="false">→</mo> <msub> <mi>S</mi> <mn>3</mn> </msub> </mrow> </semantics></math> arise which all map to the great circle <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mi>θ</mi> <mo>=</mo> <mi>π</mi> <mo>/</mo> <mn>2</mn> <mo>,</mo> <mi>ϕ</mi> <mo>∈</mo> <mo>{</mo> <mn>0</mn> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo>}</mo> <mo stretchy="false">)</mo> </mrow> </semantics></math>. The superposition on the Bloch sphere translates to a superposition of Dirac belts.</p>
Full article ">Figure 5
<p>Representation of the superposition state <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">|</mo> <mo>−</mo> <mo>〉</mo> </mrow> <mo>=</mo> <mfrac> <mn>1</mn> <msqrt> <mn>2</mn> </msqrt> </mfrac> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> </mrow> <mo>−</mo> <mrow> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math> on the Bloch sphere (<math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm). Positions × of nodes are antipodes to the direction of <math display="inline"><semantics> <mover accent="true"> <mi>n</mi> <mo stretchy="false">→</mo> </mover> </semantics></math>. The superposition of the qubits <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> <mo>,</mo> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> </mrow> </semantics></math> changes the position of the direction of the spin, which in turn changes the position × of the node. The relation between nodes on the Bloch sphere and knots in Hilbert space are shown in <a href="#symmetry-11-01399-f004" class="html-fig">Figure 4</a>.</p>
Full article ">Figure 6
<p>For spin <span class="html-italic">j</span>-states, <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>j</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> nodes arise on the Bloch sphere which may be described as a complex function <math display="inline"><semantics> <mrow> <msubsup> <mo>∏</mo> <mrow> <mi>k</mi> <mo>=</mo> <mn>1</mn> </mrow> <mrow> <mn>2</mn> <mi>j</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo>−</mo> <msub> <mi>z</mi> <mi>k</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math> in the stellar representation. The corresponding knot structure in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm is described by the Jones polynomial <math display="inline"><semantics> <mrow> <msub> <mi>J</mi> <mi>j</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math>. Additionally, the quantum phase has <math display="inline"><semantics> <mrow> <mn>4</mn> <mi>j</mi> </mrow> </semantics></math> inner twists (bosons), or <math display="inline"><semantics> <mrow> <mn>4</mn> <mi>j</mi> <mo>+</mo> <mn>2</mn> </mrow> </semantics></math> inner twists (fermions), respectively, denoted by (+).</p>
Full article ">Figure 7
<p>Left: Double copy of <math display="inline"><semantics> <mi>ν</mi> </semantics></math> inner twists, describing a boson with spin <math display="inline"><semantics> <mrow> <mn>2</mn> <mi>ν</mi> </mrow> </semantics></math>. Right: By joining the two pieces to a fermionic knot, two additional inner twists arise, leading to a knot with <math display="inline"><semantics> <mrow> <mn>4</mn> <mi mathvariant="bold">j</mi> <mo>±</mo> <mn>2</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>Due to the interaction <math display="inline"><semantics> <mrow> <mi mathvariant="bold">U</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mo form="prefix">exp</mo> <mrow> <mo>−</mo> <mo stretchy="false">(</mo> <mi>i</mi> <mi mathvariant="bold">H</mi> <mi>t</mi> <mo>/</mo> <mi>ℏ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math> with <math display="inline"><semantics> <mrow> <mi mathvariant="bold">H</mi> <mo>=</mo> <mi>ℏ</mi> <mi>ω</mi> <mo stretchy="false">(</mo> <msub> <mi>σ</mi> <mi>z</mi> </msub> <mo>×</mo> <msub> <mi>σ</mi> <mi>z</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math>, the initial state <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mo>+</mo> <mo>〉</mo> <mo stretchy="false">|</mo> <mo>+</mo> <mo>〉</mo> </mrow> </semantics></math> becomes the entangled Bell state <math display="inline"><semantics> <mrow> <mfrac> <mn>1</mn> <msqrt> <mn>2</mn> </msqrt> </mfrac> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <msub> <mn>0</mn> <mi>a</mi> </msub> <msub> <mn>1</mn> <mi>a</mi> </msub> <mo>〉</mo> </mrow> <mo>+</mo> <mrow> <mo stretchy="false">|</mo> <msub> <mn>1</mn> <mi>a</mi> </msub> <msub> <mn>0</mn> <mi>a</mi> </msub> <mo>〉</mo> </mrow> </mrow> </semantics></math>. We consider the homotopic loop perpendicular to the <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">|</mo> </mrow> <msub> <mn>0</mn> <mi>a</mi> </msub> <mrow> <mo>〉</mo> <mo>↔</mo> <mo stretchy="false">|</mo> </mrow> <msub> <mn>1</mn> <mi>a</mi> </msub> <mrow> <mo>〉</mo> </mrow> </mrow> </semantics></math>-direction.</p>
Full article ">Figure 9
<p>Using transitions to homotopically equivalent knots similar to Type-2 Reidemeister moves in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm, the constant phase can also be viewed as a combination of two qubits <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> </mrow> </semantics></math> or <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> </mrow> </semantics></math>. Since both possibilities are indistinguishable, the superposition <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> <mo>+</mo> <mo stretchy="false">|</mo> <mn>1</mn> <mo>〉</mo> <mo stretchy="false">|</mo> <mn>0</mn> <mo>〉</mo> </mrow> </semantics></math> emerges, which is an entangled state. After taking the particle trace, a mixed state arises. The latter result is basis-independent.</p>
Full article ">Figure 10
<p>Paper strip model of the interaction of two qubits: The entangled state is described by one common state with one quantum phase. By rotating the phase once and cutting into two pieces, two separate particles with left- and right twists arise. Here, we use the model of the paper strip near the boundary, where the phases <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> are glued together. The general homotopy in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm is shown in <a href="#sec6dot3-symmetry-11-01399" class="html-sec">Section 6.3</a>.</p>
Full article ">Figure 11
<p>In the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm, the constant phase in <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> can superpose constructively (symmetric wave function) <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">|</mo> </mrow> <msup> <mi mathvariant="sans-serif">Ψ</mi> <mo>+</mo> </msup> <mrow> <mo>〉</mo> </mrow> </mrow> </semantics></math> or destructively (anti symmetric wave function) <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">|</mo> </mrow> <msup> <mi mathvariant="sans-serif">Ψ</mi> <mo>−</mo> </msup> <mrow> <mo>〉</mo> </mrow> </mrow> </semantics></math> with the constant phase in <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>. The situation on the Bloch sphere in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm is shown in <a href="#symmetry-11-01399-f008" class="html-fig">Figure 8</a>.</p>
Full article ">Figure 12
<p>Paper strip model of minimal interaction: The insertion of additional twists is compensated by a gauge field. Only after a torus splitting, the gauge field with <math display="inline"><semantics> <mrow> <mo>−</mo> <mi>T</mi> </mrow> </semantics></math> twists is separated from the original particle, which then has <math display="inline"><semantics> <mrow> <mi>J</mi> <mo>+</mo> <mi>T</mi> </mrow> </semantics></math> twists due to the gauge interaction.</p>
Full article ">Figure 13
<p>The quantum phase of the state <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>3</mn> <mi>s</mi> <mo>〉</mo> </mrow> </semantics></math> is homotopically equivalent to <math display="inline"><semantics> <mrow> <mfrac> <mn>1</mn> <msqrt> <mn>2</mn> </msqrt> </mfrac> <mrow> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mn>2</mn> <mi>p</mi> <mo>,</mo> <mo>+</mo> <mn>1</mn> <mo>〉</mo> </mrow> <mo stretchy="false">|</mo> <mi>L</mi> <mo>〉</mo> <mo>+</mo> <mo stretchy="false">|</mo> <mn>2</mn> <mi>p</mi> <mo>,</mo> <mo>−</mo> <mn>1</mn> <mo>〉</mo> <mo stretchy="false">|</mo> <mi>R</mi> <mo>〉</mo> <mo stretchy="false">)</mo> </mrow> </mrow> </semantics></math>, see also <a href="#symmetry-11-01399-f009" class="html-fig">Figure 9</a>. The entangled state decays into a mixed state due to interaction of the photon with the environment.</p>
Full article ">Figure 14
<p>Paper strip model of the quantum phase of the decay <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>3</mn> <mi>s</mi> <mo>〉</mo> <mo stretchy="false">→</mo> <mo stretchy="false">|</mo> <mn>2</mn> <mi>p</mi> <mo>〉</mo> </mrow> </semantics></math> in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. If <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>R</mi> </mrow> </semantics></math> is associated with the right-circular polarized photon, the <math display="inline"><semantics> <mrow> <mi>L</mi> <mi>L</mi> </mrow> </semantics></math> described the quantum phase of the electron in the state <math display="inline"><semantics> <mrow> <mo stretchy="false">|</mo> <mn>2</mn> <mi>p</mi> <mo>,</mo> <mo>−</mo> <mn>1</mn> <mo>〉</mo> </mrow> </semantics></math>. With <math display="inline"><semantics> <mrow> <mn>50</mn> <mo>%</mo> </mrow> </semantics></math> probability, the roles of the pieces <math display="inline"><semantics> <mrow> <mi>R</mi> <mi>R</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>L</mi> <mi>L</mi> </mrow> </semantics></math> are interchanged, see <a href="#symmetry-11-01399-f013" class="html-fig">Figure 13</a>.</p>
Full article ">Figure 15
<p>Leading-order Feynman diagrams for electron-electron and electron-positron interaction. In view of entanglement, a direct interpretation of Feynman diagrams in space time is impossible. The quantum phase of the entangled state can be modeled in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm as shown in <a href="#symmetry-11-01399-f010" class="html-fig">Figure 10</a>, and in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm as shown in <a href="#symmetry-11-01399-f016" class="html-fig">Figure 16</a>.</p>
Full article ">Figure 16
<p>Haptic model of the quantum phase of an entangled pair of qubits in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. Here, we consider any homotopy in the bulk of <math display="inline"><semantics> <msub> <mi>B</mi> <mn>1</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>B</mi> <mn>2</mn> </msub> </semantics></math> in the Heegaard splitting, see <a href="#symmetry-11-01399-f003" class="html-fig">Figure 3</a>. After Hopf mapping, the pieces <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo>,</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math> from <math display="inline"><semantics> <msub> <mi>B</mi> <mn>1</mn> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>B</mi> <mn>2</mn> </msub> </semantics></math> are ‘glued together’, leading to the description in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm as shown in <a href="#symmetry-11-01399-f010" class="html-fig">Figure 10</a>. As discussed in the text, we associate with the two qubits either a pair of electrons, or an electron-positron pair. (<b>A</b>) The constant phase, see also <a href="#symmetry-11-01399-f011" class="html-fig">Figure 11</a>. (<b>B</b>) One rotation leads to a homotopically equivalent configuration, which can be seen as a pair of entangled spin <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </semantics></math> particles, see also <a href="#symmetry-11-01399-f010" class="html-fig">Figure 10</a>A. Due to the homotopic equivalences shown in <a href="#symmetry-11-01399-f009" class="html-fig">Figure 9</a>, we may view this quantum state also a combination of two spin <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </semantics></math> particles with a (virtual) gauge particle. (<b>C</b>) Encounter of the quantum phases, see also <a href="#symmetry-11-01399-f010" class="html-fig">Figure 10</a>B. (<b>D</b>) First splitting of the quantum phase in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm, see also <a href="#symmetry-11-01399-f0A1" class="html-fig">Figure A1</a> for the corresponding Jones polynomials. This configuration cannot be mapped to the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. (<b>E</b>) Second splitting of the quantum phase in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. The situation in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm, where both splitting are combined to one torus splitting is shown in <a href="#symmetry-11-01399-f010" class="html-fig">Figure 10</a>C,D. (<b>f</b>) Quantum phase of two distinguishable spin <math display="inline"><semantics> <mrow> <mn>1</mn> <mo>/</mo> <mn>2</mn> </mrow> </semantics></math> particles in the <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </semantics></math>-realm. The inner twists in the Dirac belts have opposite sign, i.e., <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>+</mo> <mo>+</mo> <mo>+</mo> <mo>+</mo> <mo stretchy="false">)</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>−</mo> <mo>−</mo> <mo>−</mo> <mo>−</mo> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p>
Full article ">Figure A1
<p>Calculation of Jones polynomials for the torus splitting described in the main text (<a href="#symmetry-11-01399-f016" class="html-fig">Figure 16</a>).</p>
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