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Modified f(Q,C) gravity dark energy models with observational constraints 具有观测约束的修正 f(Q,C) 引力暗能量模型
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-26 DOI: 10.1142/s0217732324500342
Dinesh Chandra Maurya

We investigate an isotropic and homogeneous flat dark energy model in f(Q,C) gravity theory that is linear in non-metricity Q and quadratic in boundary term C as f(Q,C)=Q+αC2, where α is a model parameter. We have solved the field equations in flat Friedmann–Lemaitre–Robertson–Walker (FLRW) spacetime geometry and considered a relation in the form of Hubble function in total energy density parameters Ωm0, Ω0(Q,C), and Hubble constant H0. We have compared our results with two observational datasets H(z) and Pantheon SNe Ia datasets by using MCMC analysis and have obtained the best fit present values of parameters. We have used these best fit values throughout in result analysis and discussion. We have found the equation of state (EoS) parameter as 1ω0.2 over 1z3. We have also investigated the Om diagnostic function and present age of the universe for these two datasets.

我们研究了f(Q,C)引力理论中的各向同性均匀平面暗能量模型,该模型与非度量Q是线性关系,与边界项C是二次关系,即f(Q,C)=Q+αC2,其中α是模型参数。我们在平坦的弗里德曼-勒梅特尔-罗伯逊-沃克(FLRW)时空几何中求解了场方程,并考虑了总能量密度参数Ωm0、Ω0(Q,C) 和哈勃常数 H0 的哈勃函数关系。我们利用 MCMC 分析方法将我们的结果与两个观测数据集 H(z) 和 Pantheon SNe Ia 数据集进行了比较,并得到了参数的最佳拟合现值。我们在结果分析和讨论中一直使用这些最佳拟合值。我们发现在-1≤z≤3的范围内,状态方程(EoS)参数为-1≤ω≤0.2。我们还研究了这两个数据集的奥姆诊断函数和宇宙的现年龄。
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引用次数: 0
Generalized ghost dark energy model in Brans–Dicke theory with logarithmic scalar field 具有对数标量场的布兰斯-迪克理论中的广义幽灵暗能量模型
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-26 DOI: 10.1142/s0217732324500469
Pinki, Pankaj Kumar, C. P. Singh

We study generalized ghost dark energy model in Brans–Dicke theory within the framework of flat Friedmann–Lemaitre–Robertson–Walker Universe. We assume the well-motivated logarithmic form of Brans–Dicke scalar field in terms of the scale factor to find the observational parameters such as equation of state parameter wg and deceleration parameter q. It is observed that the equation of state parameter crosses the phantom divide line (wg=1) for a suitable range of model parameters. We observe that the deceleration parameter is time-dependent which shows the recent phase transition from decelerated to accelerated expansion of the Universe. Moreover, the model shows that the Universe will go through two future phase transitions, recent accelerated expansion to decelerated expansion and again decelerated expansion to accelerated expansion. We have also plotted the trajectories of the model in the wgwg plane for different values of parameters and explored the freezing and thawing regions. Further, we apply the sound squared speed method to check the stability of the model and found that the model is stable for suitable range of parameters.

我们在平坦的弗里德曼-勒梅特尔-罗伯逊-沃克宇宙框架内研究布兰斯-迪克理论中的广义幽灵暗能量模型。我们假定布兰-迪克标量场的对数形式在尺度因子方面具有良好的激励性,从而找到状态方程参数wg和减速参数q等观测参数。我们观察到减速参数与时间有关,这表明宇宙最近正处于从减速膨胀到加速膨胀的阶段性转变。此外,模型还显示宇宙未来将经历两次阶段转换,即近期加速膨胀到减速膨胀,以及再次减速膨胀到加速膨胀。我们还在 wg-wg′ 平面上绘制了模型在不同参数值下的运行轨迹,并探索了冻结和解冻区域。此外,我们还采用声平方速度法检验了模型的稳定性,发现在适当的参数范围内模型是稳定的。
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引用次数: 0
Searching for lepton flavor violation with the CMS experiment 用 CMS 实验寻找轻子味道违反现象
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-26 DOI: 10.1142/s0217732324300015
Jian Wang

Searches for Lepton Flavor Violation (LFV) stand at the forefront of experimental particle physics research, offering a sensitive probe to many scenarios of physics beyond the Standard Model. The high proton–proton collision energy and luminosity provided by the CERN Large Hadron Collider (LHC) and the excellent CMS detector performance allow for an extensive program of LFV searches. This paper reviews a broad range of LFV searches conducted at the CMS experiment using data collected in LHC Run 2, including τ3μ decays, Higgs boson decays, and top quark production and decays. In each analysis, the online and offline event selections, signal modeling, background suppression and estimation, and statistical interpretation are elucidated. These searches involve various final state particles in a large transverse momentum range, showcasing the capability of the CMS experiment in exploring fundamental questions in particle physics.

对质子味道违反(LFV)的搜索处于粒子物理实验研究的前沿,为标准模型之外的许多物理场景提供了灵敏的探测手段。欧洲核子研究中心大型强子对撞机(LHC)提供的高质子-质子对撞能量和光度,以及 CMS 探测器的卓越性能,使得 LFV 搜寻项目得以广泛开展。本文回顾了 CMS 实验利用大型强子对撞机运行 2 收集的数据进行的广泛低频变构搜索,包括τ→3μ 衰变、希格斯玻色子衰变以及顶夸克产生和衰变。每项分析都阐明了在线和离线事件选择、信号建模、背景抑制和估计以及统计解释。这些搜索涉及大横向动量范围内的各种终态粒子,展示了CMS实验在探索粒子物理基本问题方面的能力。
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引用次数: 0
Ground state spectra, decay properties of B and D mesons in a relativistic square root potential 相对平方根势中 B 和 D 介子的基态光谱和衰变特性
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-26 DOI: 10.1142/s021773232450038x
S. Behera, S. Panda
<p>We look at the mass spectra of the <span><math altimg="eq-00001.gif" display="inline" overflow="scroll"><msup><mrow><mi>D</mi></mrow><mrow><mo>±</mo></mrow></msup></math></span><span></span>, <span><math altimg="eq-00002.gif" display="inline" overflow="scroll"><msup><mrow><mi>D</mi></mrow><mrow><mo>±</mo><mo>∗</mo></mrow></msup></math></span><span></span>, <span><math altimg="eq-00003.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>D</mi></mrow><mrow><mi>s</mi></mrow><mrow><mo>±</mo><mo>∗</mo></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00004.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>D</mi></mrow><mrow><mi>s</mi></mrow><mrow><mo>±</mo></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00005.gif" display="inline" overflow="scroll"><msup><mrow><mi>B</mi></mrow><mrow><mo>±</mo></mrow></msup></math></span><span></span>, <span><math altimg="eq-00006.gif" display="inline" overflow="scroll"><msup><mrow><mi>B</mi></mrow><mrow><mo>±</mo><mo>∗</mo></mrow></msup></math></span><span></span>, <span><math altimg="eq-00007.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>0</mn><mo>∗</mo></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00008.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>0</mn></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00009.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>B</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>±</mo><mo>∗</mo></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00010.gif" display="inline" overflow="scroll"><msubsup><mrow><mi>B</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>±</mo></mrow></msubsup></math></span><span></span>, <span><math altimg="eq-00011.gif" display="inline" overflow="scroll"><mi>ρ</mi></math></span><span></span>, <span><math altimg="eq-00012.gif" display="inline" overflow="scroll"><mi>π</mi></math></span><span></span>, and <span><math altimg="eq-00013.gif" display="inline" overflow="scroll"><mi>ω</mi></math></span><span></span> mesons using a relativistic square root potential. Before looking at the mass spectra, we have to figure out the model parameters, which are <span><math altimg="eq-00014.gif" display="inline" overflow="scroll"><msub><mrow><mi>U</mi></mrow><mrow><mn>0</mn></mrow></msub><mo>=</mo><mo>−</mo><mn>1</mn><mo>.</mo><mn>1</mn><mn>1</mn><mn>5</mn></math></span><span></span><span><math altimg="eq-00015.gif" display="inline" overflow="scroll"><mspace width=".17em"></mspace></math></span><span></span>GeV and <span><math altimg="eq-00016.gif" display="inline" overflow="scroll"><mi>a</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>8</mn><mn>8</mn><mn>5</mn></math></span><span></span><span><math altimg="eq-00017.gif" display="inline" overflow="scroll"><mspace width=".17em"></mspace></math></span><span></span>GeV. The calculated result of <span><math altim
我们使用相对论平方根势来研究 D±、D±∗、Ds±∗、Ds±、B±、B±∗、Bs0∗、Bs0、Bc±∗、Bc±、ρ、π 和 ω 介子的质谱。在研究质量谱之前,我们必须计算出模型参数,即 U0=-1.115GeV 和 a=0.885GeV。计算结果为 D±(1.861GeV)、D±∗(2.010GeV)、Ds±(1.903GeV)、Ds∗±(2.112GeV)、B±(5.264GeV)、B±∗(5.327GeV)、Bs0(5.345GeV)、Bs0∗(5.423GeV)、BC±(5.956GeV)、BC±∗(6.277GeV),这些研究结果与实验观测和相关理论预测都有显著的一致性。在保持模型参数不变的情况下,我们估算了伪高子和矢量介子(特别是 B 介子和 D 介子)的衰变常数、轻子衰变宽度、半轻子衰变宽度和分支分数。B介子和D介子 "的伪谱衰变常数和部分衰变宽度与理论预言、晶格量子色动力学(LQCD)计算和实验数据相当吻合。此外,我们还有效地找到了这些介子的轻子衰变宽度和分支分数,使实验结果和理论预测相吻合。半轻子衰变的计算值分别为:D0→π-e+νe(2.892×10-3)、D+→π0e+νe(3.669×10-3)、D+→ρ0e+νe(1.659×10-3)和D+→η′e+νe(3.17×10-4)、DS+→φe+νe(2.599×10-2)、DS+→ηe+νe(2.303×10-2),观测结果与实验和某些理论模型的接近是显而易见的。
{"title":"Ground state spectra, decay properties of B and D mesons in a relativistic square root potential","authors":"S. Behera, S. Panda","doi":"10.1142/s021773232450038x","DOIUrl":"https://doi.org/10.1142/s021773232450038x","url":null,"abstract":"&lt;p&gt;We look at the mass spectra of the &lt;span&gt;&lt;math altimg=\"eq-00001.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&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-00002.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mo&gt;∗&lt;/mo&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-00003.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00004.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&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-00006.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mo&gt;∗&lt;/mo&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-00007.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00008.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;ρ&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, &lt;span&gt;&lt;math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;π&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, and &lt;span&gt;&lt;math altimg=\"eq-00013.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;ω&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; mesons using a relativistic square root potential. Before looking at the mass spectra, we have to figure out the model parameters, which are &lt;span&gt;&lt;math altimg=\"eq-00014.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;&lt;span&gt;&lt;math altimg=\"eq-00015.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;GeV and &lt;span&gt;&lt;math altimg=\"eq-00016.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;&lt;span&gt;&lt;math altimg=\"eq-00017.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;GeV. The calculated result of &lt;span&gt;&lt;math altim","PeriodicalId":18752,"journal":{"name":"Modern Physics Letters A","volume":"32 1","pages":""},"PeriodicalIF":1.4,"publicationDate":"2024-04-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140798335","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
Formation of supermassive black holes from N self-gravitating small black holes: A thermodynamic study 由 N 个自重力小黑洞形成超大质量黑洞:热力学研究
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-26 DOI: 10.1142/s0217732324500512
Baljeet Kaur Lotte, Prasanta Kumar Mahapatra, Subodha Mishra

Both statistical and thermodynamic aspects are used to analyze the collapse of N self-gravitating black holes that result in the formation of supermassive black holes. The change in energy and entropy of the system in relation to the masses of the constituent black holes and their numbers are obtained. The transition temperature for the change from the high-temperature interacting gas (or particles) to the low-temperature condensed state of black holes in forming supermassive black hole is determined.

从统计和热力学两方面分析了 N 个自引力黑洞坍缩形成超大质量黑洞的过程。得出了系统能量和熵的变化与组成黑洞的质量及其数量的关系。确定了形成超大质量黑洞时黑洞从高温相互作用气体(或粒子)向低温凝聚态变化的过渡温度。
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引用次数: 0
Atmospheric Neutrino octant from flavor symmetry 从味道对称性看大气中微子八分仪
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-19 DOI: 10.1142/s0217732324500287
Paul H. Frampton, Claudio Corianò, Pietro Santorelli

The binary tetrahedral group (T) has provided the most successful flavor symmetry in understanding simultaneously the three mixing angles both for quarks in the CKM matrix and for neutrinos in the PMNS matrix. One prediction, invariant under leptonic CP violation, relates the atmospheric and reactor neutrino mixings θ32 and θ13, respectively. We study sedulously this relation using the latest neutrino data. It is natural to focus on the frustrating experimental octant ambiguity of θ32. We conclude that the flavor symmetry requires that θ32 is in the second octant θ32>45, not in the first one θ32<45, and eagerly await experimental confirmation of this prediction.

二元四面体群(T′)提供了最成功的味道对称性,可以同时理解CKM矩阵中的夸克和PMNS矩阵中的中微子的三个混合角。在轻子CP违反下不变的一个预言,分别与大气中微子混合和反应堆中微子混合θ32和θ13有关。我们利用最新的中微子数据对这一关系进行了深入研究。我们很自然地把重点放在θ32令人沮丧的实验八度模糊性上。我们得出结论:味道对称性要求θ32位于第二个八度角θ32>45∘,而不是第一个八度角θ32<45∘,并热切期待这一预言得到实验证实。
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引用次数: 0
Comments on oscillations in elastic scattering of hadrons 关于强子弹性散射振荡的评论
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-19 DOI: 10.1142/s0217732324750014
S. M. Troshin, N. E. Tyurin

The observed absence of the small-t oscillations in differential cross-section of the elastic scattering is considered as a consequence of the reflective scattering mode appearance at the highest energy of the LHC s=13TeV.

在弹性散射的差分截面上观察到的小t振荡的缺失,被认为是在大型强子对撞机的最高能量s=13TeV时出现反射散射模式的结果。
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引用次数: 0
Einstein–Podolsky–Rosen steering paradox “2=1” for N qubits N 个量子比特的爱因斯坦-波多尔斯基-罗森转向悖论 "2=1"
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-19 DOI: 10.1142/s0217732324500305
Zhi-Jie Liu, Jie Zhou, Hui-Xian Meng, Xing-Yan Fan, Mi Xie, Fu-Lin Zhang, Jing-Ling Chen

Einstein–Podolsky–Rosen (EPR) paradox highlights the absence of a local realistic explanation for quantum mechanics, and shows the incompatibility of the local-hidden-state models with quantum theory. For N-qubit states, or more importantly, the N-qubit mixed states, we present the EPR steering paradox in the form of the contradictory equality “2=1”. We show that the contradiction holds for any N-qubit state as long as both “the pure state requirement” and “the measurement requirement” are satisfied. This also indicates that the EPR steering paradox exists in more general cases. Finally, we give specific examples to demonstrate and analyze our arguments.

爱因斯坦-波多尔斯基-罗森(EPR)悖论凸显了量子力学缺乏局部现实的解释,并表明局部隐态模型与量子理论不相容。对于 N 量子位态,或更重要的 N 量子位混合态,我们以矛盾相等 "2=1 "的形式提出了 EPR 转向悖论。我们证明,只要同时满足 "纯态要求 "和 "测量要求",这个矛盾对于任何 N 量子比特态都成立。这也表明,EPR转向悖论存在于更普遍的情况中。最后,我们给出了具体的例子来证明和分析我们的论点。
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引用次数: 0
Tripartite quantum teleportation in de Sitter spacetime 德西特时空中的三方量子传送
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-19 DOI: 10.1142/s0217732324500330
Zhiming Huang, Xiangfu Zou, Haozhen Situ, Zhimin He, Lianghui Zhao, Yiyong Ye, Zhenbang Rong

In this paper, a tripartite quantum teleportation scheme in de Sitter vacuum is constructed. Then we investigate the influence of vacuum fluctuation, temperature and two-atom distance on performance of the tripartite quantum teleportation. It is found that fidelity drops fast with temperature and evolution time increasing. While temperature is low relatively, the influence of two-atom distance cannot be negligible, the change of fidelity is different with two-atom separation and time varying. The results may be helpful for dealing with quantum information tasks in curve spacetime and exploring the properties of curve spacetime through quantum information means.

本文构建了德西特真空中的三方量子远传方案。然后,我们研究了真空波动、温度和两原子距离对三方量子远传性能的影响。研究发现,随着温度和演化时间的增加,保真度会快速下降。虽然温度相对较低,但双原子间距的影响不容忽视,保真度随双原子间距和时间的变化而变化。这些结果可能有助于处理曲线时空中的量子信息任务,并通过量子信息手段探索曲线时空的特性。
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引用次数: 0
Effects of the new type of extended uncertainty principle on Van der Waals black hole thermodynamics: A theoretical and deep learning approach 新型扩展不确定性原理对范德华黑洞热力学的影响:理论与深度学习方法
IF 1.4 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Pub Date : 2024-04-09 DOI: 10.1142/s021773232450041x
Abdelhakim Benkrane, Djamel Eddine Zenkhri, Abderrahmane Benhadjira

In this paper, we study the Van der Waals black holes (the case b=0) in the anti-de Sitter space under the effect of the linear extended uncertainty principle (EUP). The analysis was undertaken using deep learning by employing physics-informed neural networks in addition to the semi-classical approach, we have calculated the thermal quantities, including mass, volume, temperature, entropy, and Gibbs free energy. Additionally, we visually depict the effects of the EUP-term on the thermodynamic properties of the studied black holes.

本文研究了线性扩展不确定性原理(EUP)作用下的反德西特空间范德华黑洞(b=0 的情况)。除了半经典方法外,我们还利用物理信息神经网络进行了深度学习分析,并计算了热量,包括质量、体积、温度、熵和吉布斯自由能。此外,我们还直观地描述了EUP项对所研究黑洞热力学性质的影响。
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Modern Physics Letters A
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