{"title":"Thick Branes in Horndeski Gravity","authors":"Fabiano F. Santos, F. A. Brito","doi":"10.1155/2024/5402411","DOIUrl":"https://doi.org/10.1155/2024/5402411","url":null,"abstract":"We investigate thick brane solutions in the Horndeski gravity. In this setup, we found analytical solutions, applying the first-order formalism to two scalar fields where the first field comes from the nonminimal scalar-tensor coupling and the second is due to the matter contribution sector. With these analytical solutions, we evaluate the symmetric thick brane solutions in Horndeski gravity with four-dimensional geometry. In such a setup, we evaluate the gravity fluctuations to find “almost massless modes,” for any values of the Horndeski parameters. These modes were used to compute the corrections to the Newtonian potential and evaluate the limit four-dimensional gravity.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":"37 1","pages":""},"PeriodicalIF":1.7,"publicationDate":"2024-02-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139664788","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}
Kh. Helensana Devi, K. Sashikanta Singh, N. Nimai Singh
{"title":"Stability of the Next-to-Tribimaximal Mixings under Radiative Corrections with the Variation of the SUSY Breaking Scale in MSSM","authors":"Kh. Helensana Devi, K. Sashikanta Singh, N. Nimai Singh","doi":"10.1155/2023/2365316","DOIUrl":"https://doi.org/10.1155/2023/2365316","url":null,"abstract":"We analyze the radiative stability of the next-to-tribimaximal mixings (NTBM) with the variation of the SUSY breaking scale (<span><svg height=\"9.25202pt\" style=\"vertical-align:-3.29111pt\" version=\"1.1\" viewbox=\"-0.0498162 -5.96091 15.1941 9.25202\" width=\"15.1941pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,10.192,3.132)\"></path></g></svg>)</span> in MSSM, for both normal ordering (NO) and inverted ordering (IO) at the fixed input value of the seesaw scale <span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"-0.0498162 -11.5914 29.79 14.8825\" width=\"29.79pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,12.22,3.132)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,22.159,0)\"></path></g></svg><span></span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"33.372183799999995 -11.5914 22.096 14.8825\" width=\"22.096pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,33.422,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,39.662,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,45.902,-5.741)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,50.334,-5.741)\"></path></g></svg></span> GeV and two different values of <span><svg height=\"12.7178pt\" style=\"vertical-align:-3.42947pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.28833 26.6668 12.7178\" width=\"26.6668pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,4.043,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,9.633,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,18.986,0)\"></path></g></svg>.</span> All the neutrino oscillation parameters receive varying radiative corrections irrespective of the <svg height=\"9.25202pt\" style=\"vertical-align:-3.29111pt\" version=\"1.1\" viewbox=\"-0.0498162 -5.96091 15.1941 9.25202\" width=\"15.1941pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-110\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,10.192,3.132)\"><use xlink:href=\"#g50-84\"></use></g></svg> values at the electroweak scale, which are all within the <svg height=\"8.55521pt\" style=\"vertical-align:-0.2063904pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.34882 13.7356 8.55521\" width=\"13.7356pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,6.24,0)\"></path></g></svg> range of the latest global fit data at a low value of <span><svg height=\"12.7178pt\" style=\"vertical-align:-3.42947pt\" version=\"1.1\" viewbo","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" 24","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138514431","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}
{"title":"Reformulating the Quantum Uncertainty Relation through Geometric Illustrations","authors":"Hao Xu, Mengjie Shi, Shuijing Li","doi":"10.1155/2023/6703001","DOIUrl":"https://doi.org/10.1155/2023/6703001","url":null,"abstract":"The uncertainty principle stands as a fundamental tenet within the realm of quantum theory. In this study, we embark on a reexamination of an emerging variant of the uncertainty relation within both pure and mixed quantum systems, leveraging a geometric elucidation. Subsequently, an enhancement to this relation is achieved by the incorporation of a surface angle denoted as <span><svg height=\"9.49473pt\" style=\"vertical-align:-0.2063999pt\" version=\"1.1\" viewbox=\"-0.0498162 -9.28833 6.59789 9.49473\" width=\"6.59789pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g></svg>,</span> thereby transforming it from an inequality into an equation. Notably, this surface angle encapsulates the dynamics inherent in quantum state transitions. Complementing our analysis, a series of calculations are conducted, yielding results that offer an intuitive elucidation of the uncertainty relation across distinct quantum states. Consequently, this method bears significance as a pivotal visual insight within the domain of quantum information and measurement.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" 10","pages":""},"PeriodicalIF":1.7,"publicationDate":"2023-11-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138514427","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}
{"title":"Theoretical and Experimental Challenges in the Measurement of Neutrino Mass","authors":"Jyotsna Singh, M. Ibrahim Mirza","doi":"10.1155/2023/8897375","DOIUrl":"https://doi.org/10.1155/2023/8897375","url":null,"abstract":"Neutrino masses are yet unknown. We discuss the present state of effective electron antineutrino mass from <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M1\"> <mi>β</mi> </math> decay experiments; effective Majorana neutrino mass from neutrinoless double-beta decay experiments; neutrino mass squared differences from neutrino oscillation: solar, atmospheric, reactor, and accelerator-based experiments; sum of neutrino masses from cosmological observations. Current experimental challenges in the determination of neutrino masses are briefly discussed. The main focus is devoted to contemporary experiments.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":"50 7","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136234242","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}
{"title":"Note on the Corrected Hawking Temperature of a Parametric Deformed Black Hole with Influence of Quantum Gravity","authors":"Zhonghua Li","doi":"10.1155/2023/9702181","DOIUrl":"https://doi.org/10.1155/2023/9702181","url":null,"abstract":"In this paper, using the Hamilton-Jacobi method, we discuss the tunnelling of fermions when the dual influence of quantum gravity and the deformation of a parameterized black hole are taken into account. With the influence of the generalized uncertainty principle, there exists an offset around the standard Hawking temperature. We investigate a parametric deformed black hole and find that the corrected temperature is lower than the standard one, so there exists a remnant of the black hole, and the correction is not only determined by the mass and the energy of the emitted fermion but also determined by the mass of the black hole and the deformation parameter. Under the dual influence of quantum gravity and deformation, the correction effect of quantum gravity is the main influencing factor, while the correction effect of the deformation parameter is secondary. For both the massive and massless cases, the quantum gravity correction factor is only determined by the energy of the emitted fermion, while the deformation correction factor is only determined by the mass of the black hole.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":"152 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2023-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136264452","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}