{"title":"Falsifiable analog model predictions of W mass in CDF II and ATLAS","authors":"R. N. C. Pfeifer","doi":"10.1142/s0217751x23400043","DOIUrl":null,"url":null,"abstract":"<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>9</mn><mn>1</mn><mo>.</mo><mn>1</mn><mn>9</mn><mn>2</mn><mn>2</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. The unenhanced masses are consistent with ATLAS data collected at <span><math altimg=\"eq-00014.gif\" display=\"inline\" overflow=\"scroll\"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>7</mn><mspace width=\".17em\"></mspace><mstyle><mtext mathvariant=\"normal\">TeV</mtext></mstyle></math></span><span></span>, and the enhanced masses are consistent with CDF II data collected at <span><math altimg=\"eq-00015.gif\" display=\"inline\" overflow=\"scroll\"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>1</mn><mo>.</mo><mn>9</mn><mn>6</mn><mspace width=\".17em\"></mspace><mstyle><mtext mathvariant=\"normal\">TeV</mtext></mstyle></math></span><span></span>. According to CASMIR, operation of the Large Hadron Collider (LHC) at center-of-mass energies small compared with <span><math altimg=\"eq-00016.gif\" display=\"inline\" overflow=\"scroll\"><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> but large enough for <span><math altimg=\"eq-00017.gif\" display=\"inline\" overflow=\"scroll\"><mi>W</mi></math></span><span></span> boson formation should permit ATLAS to replicate the result from CDF II.</p>","PeriodicalId":50309,"journal":{"name":"International Journal of Modern Physics a","volume":"8 1","pages":""},"PeriodicalIF":1.4000,"publicationDate":"2023-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Modern Physics a","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1142/s0217751x23400043","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
The CDF II measurement of boson mass is at significant () tension with the Standard Model, and moderate () 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 and boson masses of and , respectively. During baryon collisions satisfying , CASMIR predicts a color-mediated enhancement of and boson masses, becoming and , respectively. The unenhanced masses are consistent with ATLAS data collected at , and the enhanced masses are consistent with CDF II data collected at . According to CASMIR, operation of the Large Hadron Collider (LHC) at center-of-mass energies small compared with but large enough for boson formation should permit ATLAS to replicate the result from CDF II.
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。
期刊介绍:
Started in 1986, IJMPA has gained international repute as a high-quality scientific journal. It consists of important review articles and original papers covering the latest research developments in Particles and Fields, and selected topics intersecting with Gravitation and Cosmology. The journal also features articles of long-standing value and importance which can be vital to research into new unexplored areas.