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Falsifiable analog model predictions of W mass in CDF II and ATLAS CDF II 和 ATLAS 对 W 质量的可证伪模拟模型预测
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-30 DOI: 10.1142/s0217751x23400043
R. N. C. Pfeifer
<p>The CDF II measurement of <span><math altimg="eq-00002.gif" display="inline" overflow="scroll"><mi>W</mi></math></span><span></span> boson mass is at significant (<span><math altimg="eq-00003.gif" display="inline" overflow="scroll"><mn>6</mn><mo>.</mo><mn>9</mn><mspace width=".17em"></mspace><mi>σ</mi></math></span><span></span>) tension with the Standard Model, and moderate (<span><math altimg="eq-00004.gif" display="inline" overflow="scroll"><mn>4</mn><mo>.</mo><mn>0</mn><mspace width=".17em"></mspace><mi>σ</mi></math></span><span></span>) tension with recent results from ATLAS. Any attempt to interpret this as a signature of new physics requires high-precision, robust, falsifiable predictions. The Classical Analogue to the Standard Model In pseudo-Riemannian space–time (CASMIR) is an analogue model predicting <span><math altimg="eq-00005.gif" display="inline" overflow="scroll"><mi>W</mi></math></span><span></span> and <span><math altimg="eq-00006.gif" display="inline" overflow="scroll"><mi>Z</mi></math></span><span></span> boson masses of <span><math altimg="eq-00007.gif" display="inline" overflow="scroll"><mn>8</mn><mn>0</mn><mo>.</mo><mn>3</mn><mn>5</mn><mn>8</mn><mn>7</mn><mo stretchy="false">(</mo><mn>2</mn><mn>2</mn><mo stretchy="false">)</mo><mspace width=".17em"></mspace><mstyle><mtext mathvariant="normal">GeV</mtext></mstyle><mo stretchy="false">/</mo><msup><mrow><mi>c</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span><span></span> and <span><math altimg="eq-00008.gif" display="inline" overflow="scroll"><mn>9</mn><mn>1</mn><mo>.</mo><mn>1</mn><mn>8</mn><mn>7</mn><mn>7</mn><mo stretchy="false">(</mo><mn>3</mn><mn>5</mn><mo stretchy="false">)</mo><mspace width=".17em"></mspace><mstyle><mtext mathvariant="normal">GeV</mtext></mstyle><mo stretchy="false">/</mo><msup><mrow><mi>c</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span><span></span>, respectively. During baryon collisions satisfying <span><math altimg="eq-00009.gif" display="inline" overflow="scroll"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo><</mo><mn>3</mn><mo>.</mo><mn>0</mn><mn>9</mn><mspace width=".17em"></mspace><mstyle><mtext mathvariant="normal">TeV</mtext></mstyle></math></span><span></span>, CASMIR predicts a color-mediated enhancement of <span><math altimg="eq-00010.gif" display="inline" overflow="scroll"><mi>W</mi></math></span><span></span> and <span><math altimg="eq-00011.gif" display="inline" overflow="scroll"><mi>Z</mi></math></span><span></span> boson masses, becoming <span><math altimg="eq-00012.gif" display="inline" overflow="scroll"><mn>8</mn><mn>0</mn><mo>.</mo><mn>4</mn><mn>3</mn><mn>4</mn><mn>0</mn><mo stretchy="false">(</mo><mn>2</mn><mn>2</mn><mo stretchy="false">)</mo><mspace width=".17em"></mspace><mstyle><mtext mathvariant="normal">GeV</mtext></mstyle><mo stretchy="false">/</mo><msup><mrow><mi>c</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span><span></span> and <span><math altimg="eq-00013.gif" display="inline" overflow="scroll"><mn>
W 玻色子质量的 CDF II 测量结果与标准模型存在显著(6.9σ)紧张关系,与 ATLAS 的最新结果存在中等(4.0σ)紧张关系。任何将此解释为新物理学特征的尝试都需要高精度、稳健、可证伪的预测。标准模型在伪黎曼时空的经典模拟(CASMIR)是一个模拟模型,预测 W 和 Z 玻色子的质量分别为 80.3587(22)GeV/c2 和 91.1877(35)GeV/c2 。在满足 s<3.09TeV 的重子对撞中,CASMIR 预测 W 和 Z 玻色子的质量会在颜色介导下增强,分别变为 80.4340(22)GeV/c2 和 91.1922(35)GeV/c2。未增强的质量与在 s=7TeV 收集的 ATLAS 数据一致,增强的质量与在 s=1.96TeV 收集的 CDF II 数据一致。根据CASMIR,大型强子对撞机(LHC)在质量中心能量小于3.09TeV但足够大的情况下运行时,W玻色子的形成应该允许ATLAS复制CDF II的结果。
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Any attempt to interpret this as a signature of new physics requires high-precision, robust, falsifiable predictions. The Classical Analogue to the Standard Model In pseudo-Riemannian space–time (CASMIR) is an analogue model predicting &lt;span&gt;&lt;math altimg=\"eq-00005.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;W&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; and &lt;span&gt;&lt;math altimg=\"eq-00006.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; boson masses of &lt;span&gt;&lt;math altimg=\"eq-00007.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;(&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;)&lt;/mo&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;mstyle&gt;&lt;mtext mathvariant=\"normal\"&gt;GeV&lt;/mtext&gt;&lt;/mstyle&gt;&lt;mo stretchy=\"false\"&gt;/&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&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-00008.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;(&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;)&lt;/mo&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;mstyle&gt;&lt;mtext mathvariant=\"normal\"&gt;GeV&lt;/mtext&gt;&lt;/mstyle&gt;&lt;mo stretchy=\"false\"&gt;/&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, respectively. During baryon collisions satisfying &lt;span&gt;&lt;math altimg=\"eq-00009.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;msqrt&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;/msqrt&gt;&lt;mo&gt;&lt;&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;mstyle&gt;&lt;mtext mathvariant=\"normal\"&gt;TeV&lt;/mtext&gt;&lt;/mstyle&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt;, CASMIR predicts a color-mediated enhancement of &lt;span&gt;&lt;math altimg=\"eq-00010.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;W&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; and &lt;span&gt;&lt;math altimg=\"eq-00011.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mi&gt;Z&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;&lt;span&gt;&lt;/span&gt; boson masses, becoming &lt;span&gt;&lt;math altimg=\"eq-00012.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;8&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;(&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo stretchy=\"false\"&gt;)&lt;/mo&gt;&lt;mspace width=\".17em\"&gt;&lt;/mspace&gt;&lt;mstyle&gt;&lt;mtext mathvariant=\"normal\"&gt;GeV&lt;/mtext&gt;&lt;/mstyle&gt;&lt;mo stretchy=\"false\"&gt;/&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;c&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&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-00013.gif\" display=\"inline\" overflow=\"scroll\"&gt;&lt;mn&gt;","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"8 1","pages":""},"PeriodicalIF":1.6,"publicationDate":"2023-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140129196","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
Topological defects on relativistic quantum oscillator in wormhole space-time background 虫洞时空背景下相对论量子振荡器的拓扑缺陷
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-15 DOI: 10.1142/s0217751x23501786
Faizuddin Ahmed
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引用次数: 0
Relativistic quantum oscillator under rainbow gravity's effects in traversable wormhole with disclination 带偏差的可穿越虫洞中彩虹引力效应下的相对论量子振荡器
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-15 DOI: 10.1142/s0217751x23501798
A. Guvendi, Faizuddin Ahmed
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引用次数: 0
Thermal leptogenesis in anisotropic cosmology 各向异性宇宙学中的热轻生现象
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-15 DOI: 10.1142/s0217751x23501816
Mehran Dehpour
There is no evidence that the universe must have been homogeneous and isotropic before the big bang nucleosynthesis. The Bianchi type-I cosmology is the simplest homogeneous but anisotropic cosmology. In this work, we investigate thermal leptogenesis, as a baryogenesis scenario, in the Bianchi type-I cosmology. Our results show that for specific values of the anisotropy, the modified thermal leptogenesis generated more baryon asymmetry than the standard one. In this way, anisotropy can help to achieve low-scale leptogenesis.
没有证据表明宇宙在大爆炸核合成之前一定是均质和各向同性的。比安奇 I 型宇宙学是最简单的均质但各向异性的宇宙学。在这项工作中,我们研究了比安奇 I 型宇宙学中作为重生成情景的热轻生成。我们的研究结果表明,对于各向异性的特定值,修正的热跃迁发生比标准的热跃迁发生产生了更多的重子不对称。因此,各向异性有助于实现低尺度的跃迁发生。
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引用次数: 0
Joule-Thomson Expansion of Black Holes in STU Supergravity STU 超引力中黑洞的焦耳-汤姆森膨胀
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-08 DOI: 10.1142/s0217751x23501762
Y. Sekhmani, R. Myrzakulov, Riasat Ali
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引用次数: 0
Michelson-Morley Experiments: at the crossroads of Relativity, Cosmology and Quantum Physics 迈克尔逊-莫利实验:相对论、宇宙学和量子物理学的交叉点
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-08 DOI: 10.1142/s0217751x2330017x
M. Consoli, Alessandro Pluchino
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引用次数: 0
Three-body strong decays of the Y(4230) via the light-cone QCD sum rules 通过光锥 QCD 和则的 Y(4230)三体强衰变
IF 1.6 4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-12-01 DOI: 10.1142/s0217751x23501750
Zhi-Gang Wang
We tentatively assign the Y (4230) as the vector tetraquark state with a relative P-wave be-tween the scalar diquark pair, and explore the three-body strong decays Y (4230) → ¯ D ∗− D ∗ 0 π + , ¯ D ∗− D 0 π + , J/ψπ + π − and J/ψK + K − with the light-cone QCD sum rules by assuming contact four-meson coupling constants. The resulting partial decay widths are too small to account for the experimental data, and we expect those decays take place through an intermediate meson. We can search for the intermediate states and precisely measure the branching fractions to diagnose the nature of the Y states.
我们暂定Y(4230)为矢量四夸克态,在标量双夸克对之间存在相对p波,并通过假设接触四介子耦合常数,用光锥QCD和规则探索了Y(4230)→¯D∗−D∗0 π +,¯D∗−D 0 π +, J/ψπ + π−和J/ψK + K−的三体强衰变。由此产生的部分衰变宽度太小,无法解释实验数据,我们预计这些衰变是通过中间介子发生的。我们可以搜索中间状态并精确测量分支分数来诊断Y状态的性质。
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引用次数: 0
Pairwise Helicity in Higher Dimensions 高维中的成对螺旋度
4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-11-04 DOI: 10.1142/s0217751x2350149x
Yale Fan
Studies of scattering amplitudes for electric and magnetic charges have identified previously overlooked multiparticle representations of the Poincaré group in four dimensions. Such representations associate nontrivial quantum numbers (known as pairwise helicities) with asymptotically separated pairs of particles, and thus cannot be described as tensor products of one-particle states. We extend this construction to sources and spacetimes of higher dimension. We first establish the dynamical origin of pairwise helicity in [Formula: see text]-form electrodynamics coupled to mutually nonlocal branes. We then interpret this pairwise helicity as a quantum number under an SO(2) pairwise little group associated with pairs of distinct branes. We further characterize the “higher” little groups that could in principle be used to induce multiparticle or multi-brane representations of the Lorentz group.
对电荷和磁荷散射振幅的研究已经确定了以前被忽视的四维庞卡洛群的多粒子表示。这样的表示将非平凡量子数(称为成对螺旋)与渐近分离的粒子对联系起来,因此不能被描述为单粒子态的张量积。我们将这种构造扩展到更高维度的源和时空。我们首先在[公式:见文本]中建立了耦合到相互非局部膜的双螺旋度的动力学起源。然后,我们将这种对螺旋度解释为与不同膜对相关的SO(2)对小群下的量子数。我们进一步描述了“更高”的小群,这些小群原则上可以用来诱导洛伦兹群的多粒子或多膜表示。
{"title":"Pairwise Helicity in Higher Dimensions","authors":"Yale Fan","doi":"10.1142/s0217751x2350149x","DOIUrl":"https://doi.org/10.1142/s0217751x2350149x","url":null,"abstract":"Studies of scattering amplitudes for electric and magnetic charges have identified previously overlooked multiparticle representations of the Poincaré group in four dimensions. Such representations associate nontrivial quantum numbers (known as pairwise helicities) with asymptotically separated pairs of particles, and thus cannot be described as tensor products of one-particle states. We extend this construction to sources and spacetimes of higher dimension. We first establish the dynamical origin of pairwise helicity in [Formula: see text]-form electrodynamics coupled to mutually nonlocal branes. We then interpret this pairwise helicity as a quantum number under an SO(2) pairwise little group associated with pairs of distinct branes. We further characterize the “higher” little groups that could in principle be used to induce multiparticle or multi-brane representations of the Lorentz group.","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"14 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-11-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135728310","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
Adiabatic expansion, Local equilibrium and Extended Maxwell distribution for Fire-ball to Describe Multiple particle production 描述多粒子产生的火球绝热膨胀、局部平衡和扩展麦克斯韦分布
4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-11-03 DOI: 10.1142/s0217751x2350166x
Akinori Ohsawa
{"title":"Adiabatic expansion, Local equilibrium and Extended Maxwell distribution for Fire-ball to Describe Multiple particle production","authors":"Akinori Ohsawa","doi":"10.1142/s0217751x2350166x","DOIUrl":"https://doi.org/10.1142/s0217751x2350166x","url":null,"abstract":"","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"89 9","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-11-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135868967","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
P - v Criticality and Joule-Thomson expansion in corrected thermodynamics of conformally dressed (2 + 1)D AdS black hole 共形修饰(2 + 1)dads黑洞的P - v临界和焦耳-汤姆逊展开的修正热力学
4区 物理与天体物理 Q3 PHYSICS, NUCLEAR Pub Date : 2023-11-01 DOI: 10.1142/s0217751x23501658
Himanshu Kumar Sudhanshu, Dharm Veer Singh, Sabit Bekov, Kairat Myrzakulov, Sudhaker Upadhyay
{"title":"<i>P - v</i> Criticality and Joule-Thomson expansion in corrected thermodynamics of conformally dressed (2 + 1)<i>D</i> AdS black hole","authors":"Himanshu Kumar Sudhanshu, Dharm Veer Singh, Sabit Bekov, Kairat Myrzakulov, Sudhaker Upadhyay","doi":"10.1142/s0217751x23501658","DOIUrl":"https://doi.org/10.1142/s0217751x23501658","url":null,"abstract":"","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"132 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"135320932","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
期刊
International Journal of Modern Physics a
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