{"title":"四维爱因斯坦-高斯-波内特引力下银河系晕中可穿越虫洞的可能性","authors":"Zinnat Hassan, P.K. Sahoo","doi":"10.1002/andp.202400114","DOIUrl":null,"url":null,"abstract":"<p>Recently, there has been significant interest regarding the regularization of a <span></span><math>\n <semantics>\n <mrow>\n <mi>D</mi>\n <mo>→</mo>\n <mn>4</mn>\n </mrow>\n <annotation>$D\\rightarrow 4$</annotation>\n </semantics></math> limit of Einstein–Gauss–Bonnet (EGB) gravity. This regularization involves re-scaling the Gauss–Bonnet (GB) coupling constant as <span></span><math>\n <semantics>\n <mrow>\n <mi>α</mi>\n <mo>/</mo>\n <mo>(</mo>\n <mi>D</mi>\n <mo>−</mo>\n <mn>4</mn>\n <mo>)</mo>\n </mrow>\n <annotation>$\\alpha /(D-4)$</annotation>\n </semantics></math>, which bypasses Lovelock's theorem and avoids Ostrogradsky instability. A noteworthy observation is that the maximally or spherically symmetric solutions for all the regularized gravities coincide in the <span></span><math>\n <semantics>\n <mrow>\n <mn>4</mn>\n <mi>D</mi>\n </mrow>\n <annotation>$4D$</annotation>\n </semantics></math> scenario. Considering this, the wormhole solutions in the galactic halos are investigated based on three different choices of dark matter (DM) profiles, such as Universal Rotation Curve, Navarro–Frenk–White, and Scalar Field Dark Matter with the framework of <span></span><math>\n <semantics>\n <mrow>\n <mn>4</mn>\n <mi>D</mi>\n </mrow>\n <annotation>$4D$</annotation>\n </semantics></math> EGB gravity. Also, the Karmarkar condition is used to find the exact solutions for the shape functions under different non-constant redshift functions. The energy conditions for each DM profile are discussed and the influence of GB coefficient <span></span><math>\n <semantics>\n <mi>α</mi>\n <annotation>$\\alpha$</annotation>\n </semantics></math> in violating energy conditions are noticed, especially null energy conditions. Further, some physical features of wormholes, viz. complexity factor, active gravitational mass, total gravitational energy, and embedding diagrams, have been explored.</p>","PeriodicalId":7896,"journal":{"name":"Annalen der Physik","volume":"536 8","pages":""},"PeriodicalIF":2.2000,"publicationDate":"2024-07-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Possibility of the Traversable Wormholes in the Galactic Halos within 4D Einstein–Gauss–Bonnet Gravity\",\"authors\":\"Zinnat Hassan, P.K. Sahoo\",\"doi\":\"10.1002/andp.202400114\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Recently, there has been significant interest regarding the regularization of a <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>D</mi>\\n <mo>→</mo>\\n <mn>4</mn>\\n </mrow>\\n <annotation>$D\\\\rightarrow 4$</annotation>\\n </semantics></math> limit of Einstein–Gauss–Bonnet (EGB) gravity. This regularization involves re-scaling the Gauss–Bonnet (GB) coupling constant as <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>α</mi>\\n <mo>/</mo>\\n <mo>(</mo>\\n <mi>D</mi>\\n <mo>−</mo>\\n <mn>4</mn>\\n <mo>)</mo>\\n </mrow>\\n <annotation>$\\\\alpha /(D-4)$</annotation>\\n </semantics></math>, which bypasses Lovelock's theorem and avoids Ostrogradsky instability. A noteworthy observation is that the maximally or spherically symmetric solutions for all the regularized gravities coincide in the <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>4</mn>\\n <mi>D</mi>\\n </mrow>\\n <annotation>$4D$</annotation>\\n </semantics></math> scenario. Considering this, the wormhole solutions in the galactic halos are investigated based on three different choices of dark matter (DM) profiles, such as Universal Rotation Curve, Navarro–Frenk–White, and Scalar Field Dark Matter with the framework of <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>4</mn>\\n <mi>D</mi>\\n </mrow>\\n <annotation>$4D$</annotation>\\n </semantics></math> EGB gravity. Also, the Karmarkar condition is used to find the exact solutions for the shape functions under different non-constant redshift functions. The energy conditions for each DM profile are discussed and the influence of GB coefficient <span></span><math>\\n <semantics>\\n <mi>α</mi>\\n <annotation>$\\\\alpha$</annotation>\\n </semantics></math> in violating energy conditions are noticed, especially null energy conditions. Further, some physical features of wormholes, viz. complexity factor, active gravitational mass, total gravitational energy, and embedding diagrams, have been explored.</p>\",\"PeriodicalId\":7896,\"journal\":{\"name\":\"Annalen der Physik\",\"volume\":\"536 8\",\"pages\":\"\"},\"PeriodicalIF\":2.2000,\"publicationDate\":\"2024-07-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Annalen der Physik\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/andp.202400114\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annalen der Physik","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/andp.202400114","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Possibility of the Traversable Wormholes in the Galactic Halos within 4D Einstein–Gauss–Bonnet Gravity
Recently, there has been significant interest regarding the regularization of a limit of Einstein–Gauss–Bonnet (EGB) gravity. This regularization involves re-scaling the Gauss–Bonnet (GB) coupling constant as , which bypasses Lovelock's theorem and avoids Ostrogradsky instability. A noteworthy observation is that the maximally or spherically symmetric solutions for all the regularized gravities coincide in the scenario. Considering this, the wormhole solutions in the galactic halos are investigated based on three different choices of dark matter (DM) profiles, such as Universal Rotation Curve, Navarro–Frenk–White, and Scalar Field Dark Matter with the framework of EGB gravity. Also, the Karmarkar condition is used to find the exact solutions for the shape functions under different non-constant redshift functions. The energy conditions for each DM profile are discussed and the influence of GB coefficient in violating energy conditions are noticed, especially null energy conditions. Further, some physical features of wormholes, viz. complexity factor, active gravitational mass, total gravitational energy, and embedding diagrams, have been explored.
期刊介绍:
Annalen der Physik (AdP) is one of the world''s most renowned physics journals with an over 225 years'' tradition of excellence. Based on the fame of seminal papers by Einstein, Planck and many others, the journal is now tuned towards today''s most exciting findings including the annual Nobel Lectures. AdP comprises all areas of physics, with particular emphasis on important, significant and highly relevant results. Topics range from fundamental research to forefront applications including dynamic and interdisciplinary fields. The journal covers theory, simulation and experiment, e.g., but not exclusively, in condensed matter, quantum physics, photonics, materials physics, high energy, gravitation and astrophysics. It welcomes Rapid Research Letters, Original Papers, Review and Feature Articles.