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Analysis of optical solitons propagation in the dual-mode resonant nonlinear Schrödinger dynamical equation with assorted nonlinear interactions 具有各种非线性相互作用的双模共振非线性薛定谔动力学方程中的光孤子传播分析
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924504335
Hamood Ur Rehman, Kiran Khushi, Ifrah Iqbal, El-Sayed M. Sherif, M. Umair Shahzad, Mohammad Amir Khan

This research explores the dual-mode manifestation within the nonlinear Schrödinger equation, elucidating the amplification or absorption of paired waves. This study delves into the simultaneous generation of two distinct waves associated with the dual-mode phenomenon with three crucial parameters: phase velocity, nonlinearity and dispersive factor. The resulting wave phenomena from these solutions have implications across various fields, including fluid dynamics, water wave mechanics, ocean engineering and scientific inquiry. The study employs the modified Sardar sub-equation method to obtain the optical soliton solutions, encompassing various types such as dark, bright, singular, combo dark–singular, periodic singular and dark–bright solitons. The obtained results highlight the reliability and simplicity of the modified Sardar sub-equation method. Additionally, the paper delves into the parametric conditions crucial for shaping and sustaining these solitons. The research explores the interaction of dual waves and the variation in wave speed. Furthermore, dynamic phenomena are illustrated, and the physical implications of the solutions are interpreted using 3D and 2D plots with different parameter values.

本研究探讨了非线性薛定谔方程中的双模表现,阐明了成对波的放大或吸收。本研究深入探讨了与双模现象相关的两个不同波的同时产生,以及三个关键参数:相位速度、非线性度和色散因子。这些解法产生的波现象对流体动力学、水波力学、海洋工程和科学探索等多个领域都有影响。研究采用改进的萨达尔子方程法获得光学孤子解,包括暗孤子、亮孤子、奇异孤子、组合暗-奇异孤子、周期奇异孤子和暗-亮孤子等各种类型。所获得的结果凸显了改进的萨达尔子方程法的可靠性和简便性。此外,论文还深入探讨了形成和维持这些孤子的关键参数条件。研究探讨了双波的相互作用和波速的变化。此外,论文还说明了动态现象,并利用不同参数值的三维和二维图解释了求解的物理意义。
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引用次数: 0
Design of NiO–ZnCo2O4 heterostructures for room temperature H2S sensing 设计用于室温 H2S 传感的 NiO-ZnCo2O4 异质结构
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924504098
Ali Akhtar, Rujun Zhou, Daru Chen, Shama Sadaf, Ce Fu, Jianqiao Liu

Hydrogen sulfide (H2S) detection with novel sensing properties such as higher response and minimum detection limit at room temperature is essential to ensure the safety of humans and the environment. A hydrothermal method was utilized to synthesize NiO–ZnCo2O4 heterostructures. The purpose of these materials was to fabricate gas sensors and detect different hazardous gases. The intrinsic properties of synthesized products were studied to check the microstructure and morphological properties of the heterostructures. Different gas sensors performed gas sensing properties, and the significant properties such as high response (ratio of response in gas and response in air RgRa=290) towards 20ppm H2S, short response/recovery time (32/20 s), a low detection limit (0.5 ppm), and great selectivity were detected based on the gas sensor of NZCO-5 (5% NiO–ZnCo2O4) compared with other sensors NiO, NZCO-0 (0% NiO–ZnCo2O4) and NZCO-10 (10% NiO–ZnCo2O4). The significant H2S gas sensing improvement in this study could be a potential route for saving human lives.

硫化氢(H2S)检测具有新颖的传感特性,如更高的响应和室温下的最低检测限,这对于确保人类和环境的安全至关重要。研究人员采用水热法合成了 NiO-ZnCo2O4 异质结构。这些材料的目的是制造气体传感器,检测不同的有害气体。研究人员对合成产品的内在特性进行了研究,以检查异质结构的微观结构和形态特性。不同的气体传感器具有不同的气体传感特性,其中显著的特性包括:对 20ppm H2S 的高响应(气体中的响应与空气中的响应之比 Rg∕Ra=290)、短响应/恢复时间(32/20 秒)、低检测限(0.NZCO-5 (5% NiO-ZnCo2O4) 气体传感器与其他 NiO、NZCO-0 (0% NiO-ZnCo2O4) 和 NZCO-10 (10% NiO-ZnCo2O4) 传感器相比,检测到了 5 ppm 的 H2S,并具有很高的选择性。)这项研究在 H2S 气体传感方面的重大改进可能是拯救人类生命的潜在途径。
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引用次数: 0
Astrophysical expedition: Transit search heuristics for fractional Hammerstein control autoregressive models 天体物理学考察:分数哈默斯坦控制自回归模型的过境搜索启发式方法
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924504177
Faisal Altaf, Ching-Lung Chang, Naveed Ishtiaq Chaudhary, Taimoor Ali Khan, Zeshan Aslam Khan, Chi-Min Shu, Muhammad Asif Zahoor Raja

This study presents an astrophysics-inspired transit search optimization (TSO) algorithm based on exoplanet search divided into five phases: galaxy phase, star phase, transit phase, neighbor phase and exploitation phase for effective parameter estimation of fractional Hammerstein control autoregressive (Fr-HCAR) systems. Various physical phenomena and real processes can be modeled with Fr-HCAR systems and estimating the Fr-HCAR parameters becomes a vital task. The mean-square error (MSE)-based criterion function is developed, and efficacy of the TSO for Fr-HCAR identification is deeply analyzed for different fractional orders, disturbance levels and degrees of freedom. The TSO remained accurate, convergent, robust and stable for all variations in Fr-HCAR but the accuracy level degrades a little bit for high disturbance and increased degrees of freedom. The reliability and trustworthiness of the TSO for Fr-HCAR identification are endorsed through statistical analyses conducted on sufficient autonomous executions of the scheme.

本研究提出了一种天体物理学启发的过境搜索优化(TSO)算法,该算法基于系外行星搜索,分为五个阶段:星系阶段、恒星阶段、过境阶段、邻近阶段和利用阶段,用于有效估计分数哈默斯坦控制自回归(Fr-HCAR)系统的参数。各种物理现象和真实过程都可以用 Fr-HCAR 系统建模,因此估计 Fr-HCAR 参数成为一项重要任务。本文开发了基于均方误差(MSE)的判据函数,并深入分析了 TSO 在不同分数阶数、扰动水平和自由度下对 Fr-HCAR 识别的有效性。对于 Fr-HCAR 的所有变化,TSO 都保持了准确性、收敛性、鲁棒性和稳定性,但在高干扰和自由度增加的情况下,准确性略有下降。通过对足够多的自主执行方案进行统计分析,证明了用于 Fr-HCAR 识别的 TSO 的可靠性和可信度。
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引用次数: 0
Synthesis of mulberry-like Fe nanoparticles assembly by nano-spheres and its excellent electromagnetic absorption properties 用纳米球组装合成桑葚状铁纳米粒子及其优异的电磁吸收特性
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s021798492442003x
Fuli Yang, Bo Zou, Lirui Wang

Considering the development of ultra-wideband detection technology, the effective attenuation performance of conventional electromagnetic absorbing materials prepared by component-morphology method is still affected by narrowband, which hinders its application. An effective strategy is to develop nanomagnetic metal absorbent that can effectively overcome skin effect through fine control based on nanotechnology. Mulberry-like Fe nanoparticles based on the self-assembly of spheroid blocks were synthesized in a simple chemical reduction process supplemented by a magnetic field. In view of synergistic loss of magnetic metal Fe, and unique physical properties of nanoparticles, the mulberry-like Fe nanoparticles exhibited attractive wave-absorbing properties. At a thickness of 3mm, the minimum reflection loss (RL) reaches −29.57dB, and the bandwidth less than −10dB reaches 8.38GHz, which covers the entire X-band, most of the C-band and part of the Ku-band. This will make it possible for electromagnetic protection and electromagnetic stealth. A possible growth mechanism was proposed to provide theoretical guidance for the subsequent preparation of nanomagnetic metal absorbent.

考虑到超宽带探测技术的发展,传统的分量形态法制备的电磁吸波材料的有效衰减性能仍然受到窄带的影响,阻碍了其应用。一种有效的策略是基于纳米技术,通过精细控制,开发出能有效克服皮肤效应的纳米磁性金属吸波材料。通过简单的化学还原过程并辅以磁场,合成了基于球状块自组装的桑葚状铁纳米粒子。鉴于磁性金属铁的协同损耗和纳米粒子的独特物理性质,桑椹状铁纳米粒子表现出极具吸引力的吸波特性。在厚度为 3 毫米时,最小反射损耗(RL)达到 -29.57dB,带宽小于 -10dB,达到 8.38GHz,覆盖了整个 X 波段、大部分 C 波段和部分 Ku 波段。这将使电磁防护和电磁隐身成为可能。该研究提出了一种可能的生长机制,为后续制备纳米磁性金属吸波材料提供了理论指导。
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引用次数: 0
Investigation of electrolysis corrosion on marine propellers 船用螺旋桨电解腐蚀调查
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924420119
Annie Wang, Karnika de Silva, Mark Jones, Wei Gao

Marine propellers operate under severe service conditions and experience various corrosion forms. Electrochemical, mechanical, and biological corrosion are the three main common types of corrosion that occur on marine propellers. Electrolysis (electrolytic corrosion), being one of the electrochemical corrosion forms, has been extensively observed on marine propellers. It is the forced introduction of an external current in metals when submerged in seawater. However, it has rarely been studied for marine propellers, mostly on underground pipelines. This paper investigates the effect of electrolysis on a chromium-containing coating on copper substrate by studying the surface and cross-sectional microstructure of the substrate. It is likely that cathodic disbondment caused by high alkalinity and hydrogen evolution at the defect location were the primary reasons contributing to the failure of the coating, and the silver-colored layer deposition around the delaminated area is the corrosion product of copper–chromium oxide. The purpose of this study is to understand the electrolysis corrosion mechanism on Cu substrate and to develop a highly effective anticorrosion coating for marine propellers.

船用螺旋桨在恶劣的服役条件下工作,会经历各种形式的腐蚀。电化学腐蚀、机械腐蚀和生物腐蚀是船用螺旋桨常见的三大腐蚀类型。电解(电解腐蚀)是电化学腐蚀的一种,在船用螺旋桨上已被广泛观察到。当金属浸没在海水中时,会强制引入外部电流。然而,人们很少对船用螺旋桨进行研究,主要是对地下管道进行研究。本文通过研究铜基体的表面和横截面微观结构,探讨了电解对铜基体含铬涂层的影响。高碱度引起的阴极脱粘和缺陷位置的氢演化可能是导致涂层失效的主要原因,脱粘区域周围的银色沉积层是铜铬氧化物的腐蚀产物。本研究的目的是了解铜基材的电解腐蚀机理,并开发一种用于船用螺旋桨的高效防腐涂层。
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引用次数: 0
Applications of variational integrators to couple of linear dynamical models discussing temperature distribution and wave phenomena 变分积分器在讨论温度分布和波浪现象的线性动力学耦合模型中的应用
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924504359
Syed Oan Abbas, Aly R. Seadawy, Sana Ghafoor, Syed T. R. Rizvi

Variational Integrator (VI) is a numerical technique, in which the Lagrangian of the system is used as the action integral. It is a special type of numerical solution that preserves the energy and momentum of the system. In this paper, we retrieve numerical solutions for heat and wave equation with the help of all possible combinations of finite difference scheme like forward–forward, forward–backward, forward–centered, backward–forward, backward–backward, backward–centered, centered–forward, centered–backward, centered–centered. We also use Lagrangian approach along with the projection technique to obtain approximate solutions of these linear models. This approach provides the best approximate solutions as well as preserves the energy of the system while the finite difference scheme gives only the numerical solutions. We also draw a comparison of existing exact solution with all approximate solutions for both models and provide graphical representation of these solutions.

变量积分(Variational Integrator,VI)是一种数值技术,其中系统的拉格朗日被用作作用积分。它是一种特殊的数值解法,能保留系统的能量和动量。在本文中,我们借助所有可能的有限差分方案组合,如前向前进、前向后退、前向居中、后向前进、后向后退、后向居中、居中前进、居中后退、居中居中,检索热方程和波方程的数值解。我们还使用拉格朗日方法和投影技术来获得这些线性模型的近似解。这种方法提供了最佳近似解,并保留了系统的能量,而有限差分方案只给出了数值解。我们还对这两个模型的现有精确解与所有近似解进行了比较,并提供了这些解的图示。
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引用次数: 0
Enhanced magnetoresistance properties in La0.7−xSmxCa0.3MnO3 epitaxial films 增强 La0.7-xSmxCa0.3MnO3 外延薄膜的磁阻特性
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-31 DOI: 10.1142/s0217984924504281
Rui Chen, Kin Hong Ip, Xin Huang, Junhong Li, Zhiliang Dong, Men Shao, Min Xu, Weiyi Yang, Tingting Yan, Zhidong Li, Hui Zhang, Ji Ma, Sheng’an Yang, Qingming Chen

The electrical and magnetic properties of strongly correlated manganese oxides originate from and depend on the coupling of spin, orbital, lattice and other degrees of freedom, and can also be controlled by external stimuli (such as a magnetic field). Here, the films have been prepared using spin-coating method to determine the role of Jahn–Teller (JT) distortion and double exchange (DE) interaction in electronic transport and magnetoresistance (MR) by magnetic field in La0.7xSmxCa0.3MnO3/SrTiO3(001). The Sm-induced lattice distortion suppresses the metal-insulator transition temperature and increases the films’ resistivity, which is due to the weakening of the DE interaction between Mn3+–O2–Mn4+ ions and the enhancement of the single electron bandwidth. Moreover, the MR can be increased to 96.5% and the AMR can be increased to 66.6% under 1 T magnetic field. These findings indicate the importance of JT distortion in multi-field control of hole-doped perovskite manganites.

强相关锰氧化物的电学和磁学特性源于并取决于自旋、轨道、晶格和其他自由度的耦合,也可受外部刺激(如磁场)的控制。本文采用自旋涂层法制备了薄膜,以确定在 La0.7-xSmxCa0.3MnO3/SrTiO3(001) 中,Jahn-Teller(JT)畸变和双交换(DE)相互作用在电子传输和磁阻(MR)中的作用。Sm引起的晶格畸变抑制了金属-绝缘体转变温度并提高了薄膜的电阻率,这是由于Mn3+-O2--Mn4+离子之间的DE相互作用减弱以及单电子带宽增强所致。此外,在 1 T 磁场下,MR 可提高到 96.5%,AMR 可提高到 66.6%。这些发现表明了JT畸变在空穴掺杂透晶锰酸盐多场控制中的重要性。
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引用次数: 0
Modulation instability analysis and optical solitary waves solutions of high-order dispersive parabolic Schrödinger–Hirota equation 高阶分散抛物线薛定谔-希罗塔方程的调制不稳定性分析和光孤波解
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-30 DOI: 10.1142/s0217984924504141
Aizaz Khan, Saud Fahad Aldosary, Meraj Ali Khan, Mati ur Rahman, Shabir Ahmad

The balance of nonlinearity and dispersion in optical fiber medium gives rise to a constantly propagating pulse. Such distortion less waves have attracted potential interest. The dynamics of optical solitons are governed by the nonlinear Schrödinger’s equation (NLSE). A modified form of NLSE which incorporates group velocity dispersion (GVD) and the Kerr law nonlinearity is recently adopted for the study of such waves. Here, we investigate the nonlinear Schrödinger–Hirota’s equation (NLSHE) using the Sardar subequation approach. Some novel solutions to the NLSHE corresponding to the bright, dark, kink, and cusp solitons have been reported. Additionally, the spatial and temporal dynamics of these solitons provide deep insight into the behavior of these solutions. The stability study is carried out via modulation instability (MI) concept. Our work might have benefits in the propagation of these pulses in the optical fiber for communication.

光纤介质中非线性和色散的平衡产生了不断传播的脉冲。这种不失真波引起了人们的潜在兴趣。光孤子的动力学受非线性薛定谔方程(NLSE)支配。最近,一种包含群速度色散(GVD)和克尔定律非线性的 NLSE 修正形式被用于研究此类波。在此,我们使用萨达尔子方程方法研究了非线性薛定谔-希罗塔方程(NLSHE)。报告中提到了与亮孤子、暗孤子、扭结孤子和尖顶孤子相对应的非线性薛定谔-希罗塔方程的一些新解。此外,这些孤子的空间和时间动力学也为这些解的行为提供了深刻的见解。稳定性研究是通过调制不稳定性(MI)概念进行的。我们的工作可能会对这些脉冲在光纤中的传播通信产生益处。
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引用次数: 0
Enhanced nonlinear optical responses of doped superalkali metal salts with fluorinated/non-fluorinated planar boron sheets: A theoretical study 掺杂了氟化/非氟化平面硼片的超碱金属盐的增强非线性光学响应:理论研究
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-30 DOI: 10.1142/s0217984924504153
Abrar Ul Hassan, Sajjad H. Sumrra, Wardha Zafar, Nyiang K. Nkungli, Norah Alhokbany
<p>The widespread use of nonlinear optical (NLO) materials for contemporary technologies has sparked intense interest in their production with the creation of materials with a continuous endeavor. In this theoretical study, we investigate the NLO responses of doped superalkali (SA) metal salts with planar boron sheets (PBSs). We consider four different substrates (B<span><math altimg="eq-00001.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>0</mn></mrow></msub></math></span><span></span>, B<span><math altimg="eq-00002.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>0</mn></mrow></msub></math></span><span></span>F<sub>3</sub>, B<span><math altimg="eq-00003.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>6</mn></mrow></msub></math></span><span></span>, and B<span><math altimg="eq-00004.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>6</mn></mrow></msub></math></span><span></span>F<sub>3</sub>) to create 12 new surfaces ( <b>1-12</b>) by doping SAs (Li<sub>2</sub>F, Li<sub>2</sub>OF, Li<sub>2</sub>O<sub>2</sub>) with them. We optimize the geometries of these surfaces and analyze their frontier molecular orbitals (FMOs) and natural bond orbitals (NBO) to obtain insights into their global chemical reactivity. We also examined their NLO responses ranging as 1.22–<span><math altimg="eq-00005.gif" display="inline"><mn>1</mn><mo>.</mo><mn>6</mn><mn>7</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>2</mn><mn>1</mn></mrow></msup></math></span><span></span>, 3.39–<span><math altimg="eq-00006.gif" display="inline"><mn>7</mn><mo>.</mo><mn>5</mn><mn>9</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>2</mn><mn>4</mn></mrow></msup></math></span><span></span>, and <span><math altimg="eq-00007.gif" display="inline"><mn>3</mn><mo>.</mo><mn>5</mn><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>2</mn><mn>4</mn></mrow></msup></math></span><span></span><span><math altimg="eq-00008.gif" display="inline"><mspace width=".17em"></mspace></math></span><span></span>e.s.u. Our results reveal that the doped surfaces exhibit stronger NLO responses compared to the undoped surfaces, and that the strongest NLO response is found in the B<span><math altimg="eq-00009.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>6</mn></mrow></msub></math></span><span></span>F<sub>3</sub>-doped surface. The role of various segments in FMOs is investigated using the TDOS and PDOS spectral analyses. To comprehend the relationship between the SA and the B<span><math altimg="eq-00010.gif" display="inline"><msub><mrow></mrow><mrow><mn>1</mn><mn>0</mn></mrow></msub></math></span><span></span>F<sub>3</sub> substrates molecule more effectively, non-covalent interaction (NCI) investigation is carried out. Additionally, Time-dependent DFT (TD-DFT) simulations are done for UV–Vis analysis to observe significant redshifts up to 1050<span><math altimg="eq-00011.gif" display="inli
随着非线性光学(NLO)材料在当代技术中的广泛应用,人们对其生产产生了浓厚的兴趣,并不断致力于材料的创造。在这项理论研究中,我们探讨了掺杂了平面硼片(PBS)的超碱(SA)金属盐的 NLO 响应。我们考虑了四种不同的基底(B10、B10F3、B16 和 B16F3),通过掺杂 SAs(Li2F、Li2OF、Li2O2)来创建 12 个新的表面(1-12)。我们优化了这些表面的几何结构,并分析了它们的前沿分子轨道(FMO)和天然键轨道(NBO),以深入了解它们的全局化学反应性。我们的研究结果表明,与未掺杂表面相比,掺杂表面表现出更强的 NLO 反应,其中掺杂 B16F3 的表面具有最强的 NLO 反应。我们使用 TDOS 和 PDOS 光谱分析研究了 FMO 中不同区段的作用。为了更有效地理解 SA 与 B10F3 底物分子之间的关系,还进行了非共价相互作用(NCI)研究。此外,还进行了与时间相关的 DFT(TD-DFT)模拟,以进行紫外可见光分析,从而观察到高达 1050nm 的显著红移。所有掺杂 SA 的表面都是热力学稳定的 NLO 材料,具有更好的 NLO 响应,因此建议在构建高级 NLO 响应时使用这些材料。
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We consider four different substrates (B&lt;span&gt;&lt;math altimg=\"eq-00001.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, B&lt;span&gt;&lt;math altimg=\"eq-00002.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;F&lt;sub&gt;3&lt;/sub&gt;, B&lt;span&gt;&lt;math altimg=\"eq-00003.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, and B&lt;span&gt;&lt;math altimg=\"eq-00004.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;F&lt;sub&gt;3&lt;/sub&gt;) to create 12 new surfaces ( &lt;b&gt;1-12&lt;/b&gt;) by doping SAs (Li&lt;sub&gt;2&lt;/sub&gt;F, Li&lt;sub&gt;2&lt;/sub&gt;OF, Li&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt;) with them. We optimize the geometries of these surfaces and analyze their frontier molecular orbitals (FMOs) and natural bond orbitals (NBO) to obtain insights into their global chemical reactivity. We also examined their NLO responses ranging as 1.22–&lt;span&gt;&lt;math altimg=\"eq-00005.gif\" display=\"inline\"&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, 3.39–&lt;span&gt;&lt;math altimg=\"eq-00006.gif\" display=\"inline\"&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math altimg=\"eq-00007.gif\" display=\"inline\"&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;&lt;span&gt;&lt;math altimg=\"eq-00008.gif\" display=\"inline\"&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;e.s.u. Our results reveal that the doped surfaces exhibit stronger NLO responses compared to the undoped surfaces, and that the strongest NLO response is found in the B&lt;span&gt;&lt;math altimg=\"eq-00009.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;F&lt;sub&gt;3&lt;/sub&gt;-doped surface. The role of various segments in FMOs is investigated using the TDOS and PDOS spectral analyses. To comprehend the relationship between the SA and the B&lt;span&gt;&lt;math altimg=\"eq-00010.gif\" display=\"inline\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;F&lt;sub&gt;3&lt;/sub&gt; substrates molecule more effectively, non-covalent interaction (NCI) investigation is carried out. Additionally, Time-dependent DFT (TD-DFT) simulations are done for UV–Vis analysis to observe significant redshifts up to 1050&lt;span&gt;&lt;math altimg=\"eq-00011.gif\" display=\"inli","PeriodicalId":18570,"journal":{"name":"Modern Physics Letters B","volume":"16 1","pages":""},"PeriodicalIF":1.9,"publicationDate":"2024-05-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141254257","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Mechanical normal dispersive 𝒩ℒℋ𝒮 shock waves of microfluidics in shallow model 浅层模型中微流体的机械法向色散𝒩ℒℋ𝒮冲击波
IF 1.9 4区 物理与天体物理 Q3 PHYSICS, APPLIED Pub Date : 2024-05-30 DOI: 10.1142/s0217984924503810
Fatih Şevgin, Talat Körpinar

In this paper, we obtain normal dispersive 𝒩𝒮 shock waves for ϕ(𝒥1),ϕ(𝒥2),ϕ(𝒥3) dam-break intensity by the nonlinear heat system. Then, we obtain super-fluid normal dispersive 𝒩𝒮 shock waves for ϕ(𝒥1),ϕ(𝒥2),ϕ(𝒥3) dam-break microfluidics. Finally, we illustrate thermonormal 𝒩𝒮 pressure of ϕ(𝒥1),ϕ(𝒥2),ϕ(𝒥3) wave energy with normal dam-break in shallow water.

本文通过非线性热系统得到了j(𝒩1),j(𝒥2),j(𝒥3)溃坝强度的法向色散𝒩ℒℋ𝒮冲击波。然后,我们得到了ϕ(𝒥1),ϕ(𝒥2),ϕ(𝒥3)溃坝微流体的超流体法向色散𝒩ℒℋ𝒮冲击波。最后,我们说明了在浅水中具有法向破坝作用的热法向𝒩ℒℋ𝒮压力j(𝒥1),j(𝒥2),j(𝒥3)波能。
{"title":"Mechanical normal dispersive 𝒩ℒℋ𝒮 shock waves of microfluidics in shallow model","authors":"Fatih Şevgin, Talat Körpinar","doi":"10.1142/s0217984924503810","DOIUrl":"https://doi.org/10.1142/s0217984924503810","url":null,"abstract":"<p>In this paper, we obtain normal dispersive <span><math altimg=\"eq-00003.gif\" display=\"inline\"><mi mathvariant=\"cal\">𝒩</mi><mi mathvariant=\"cal\">ℒ</mi><mi mathvariant=\"cal\">ℋ</mi><mi mathvariant=\"cal\">𝒮</mi></math></span><span></span> shock waves for <span><math altimg=\"eq-00004.gif\" display=\"inline\"><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>2</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>3</mn></mrow></msub><mo stretchy=\"false\">)</mo></math></span><span></span> dam-break intensity by the nonlinear heat system. Then, we obtain super-fluid normal dispersive <span><math altimg=\"eq-00005.gif\" display=\"inline\"><mi mathvariant=\"cal\">𝒩</mi><mi mathvariant=\"cal\">ℒ</mi><mi mathvariant=\"cal\">ℋ</mi><mi mathvariant=\"cal\">𝒮</mi></math></span><span></span> shock waves for <span><math altimg=\"eq-00006.gif\" display=\"inline\"><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>2</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>3</mn></mrow></msub><mo stretchy=\"false\">)</mo></math></span><span></span> dam-break microfluidics. Finally, we illustrate thermonormal <span><math altimg=\"eq-00007.gif\" display=\"inline\"><mi mathvariant=\"cal\">𝒩</mi><mi mathvariant=\"cal\">ℒ</mi><mi mathvariant=\"cal\">ℋ</mi><mi mathvariant=\"cal\">𝒮</mi></math></span><span></span> pressure of <span><math altimg=\"eq-00008.gif\" display=\"inline\"><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>2</mn></mrow></msub><mo stretchy=\"false\">)</mo><mo>,</mo><mi>ϕ</mi><mo stretchy=\"false\">(</mo><msub><mrow><mi mathvariant=\"cal\">𝒥</mi></mrow><mrow><mn>3</mn></mrow></msub><mo stretchy=\"false\">)</mo></math></span><span></span> wave energy with normal dam-break in shallow water.</p>","PeriodicalId":18570,"journal":{"name":"Modern Physics Letters B","volume":"66 1","pages":""},"PeriodicalIF":1.9,"publicationDate":"2024-05-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141254261","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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Modern Physics Letters B
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