{"title":"论广义勒梅特-托尔曼-邦迪公设:经典敏感性与量子爱因斯坦-瓦兹壳","authors":"Mohammadreza Molaei, Christian Corda","doi":"10.1002/prop.202300195","DOIUrl":null,"url":null,"abstract":"<p>In this paper, in the classical framework, the lower bounds for the sensitivities of the generalized Lemaitre Tolman Bondi metric are evaluated. The calculated lower bounds via the linear dynamical systems <span></span><math>\n <semantics>\n <msub>\n <mi>L</mi>\n <mfrac>\n <mi>∂</mi>\n <mrow>\n <mi>∂</mi>\n <mi>θ</mi>\n </mrow>\n </mfrac>\n </msub>\n <annotation>$L_{\\frac{\\partial }{\\partial \\theta }}$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <msub>\n <mi>L</mi>\n <mfrac>\n <mi>∂</mi>\n <mrow>\n <mi>∂</mi>\n <mi>r</mi>\n </mrow>\n </mfrac>\n </msub>\n <annotation>$L_{\\frac{\\partial }{\\partial r}}$</annotation>\n </semantics></math>, and <span></span><math>\n <semantics>\n <msub>\n <mi>L</mi>\n <mfrac>\n <mi>∂</mi>\n <mrow>\n <mi>∂</mi>\n <mi>ϕ</mi>\n </mrow>\n </mfrac>\n </msub>\n <annotation>$L_{\\frac{\\partial }{\\partial \\phi }}$</annotation>\n </semantics></math> are <span></span><math>\n <semantics>\n <mrow>\n <mrow>\n <mo>−</mo>\n <mi>ln</mi>\n <mn>2</mn>\n <mo>+</mo>\n <mi>ln</mi>\n <mo>|</mo>\n </mrow>\n <msup>\n <mrow>\n <mo>(</mo>\n <mover>\n <mi>R</mi>\n <mo>̇</mo>\n </mover>\n <mi>B</mi>\n <mo>)</mo>\n </mrow>\n <mn>2</mn>\n </msup>\n <mo>−</mo>\n <msup>\n <mrow>\n <mo>(</mo>\n <msup>\n <mi>R</mi>\n <mo>′</mo>\n </msup>\n <mo>)</mo>\n </mrow>\n <mn>2</mn>\n </msup>\n <mrow>\n <mo>|</mo>\n <mo>−</mo>\n <mn>2</mn>\n <mi>ln</mi>\n <mo>|</mo>\n <mi>B</mi>\n <mo>|</mo>\n </mrow>\n </mrow>\n <annotation>$-\\ln 2+\\ln|{(\\dot{R}B)}^{2}-{(R^{\\prime })}^{2}|-2\\ln|B|$</annotation>\n </semantics></math>, <span></span><math>\n <semantics>\n <mrow>\n <mrow>\n <mn>2</mn>\n <mi>ln</mi>\n <mo>|</mo>\n </mrow>\n <mover>\n <mi>B</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mo>|</mo>\n <mo>−</mo>\n <mi>ln</mi>\n <mn>2</mn>\n </mrow>\n </mrow>\n <annotation>$2\\ln|\\dot{B}|-\\ln 2$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mrow>\n <mrow>\n <mo>−</mo>\n <mi>ln</mi>\n <mn>2</mn>\n <mo>−</mo>\n <mn>2</mn>\n <mi>ln</mi>\n <mo>|</mo>\n <mi>B</mi>\n <mo>|</mo>\n <mo>+</mo>\n <mi>ln</mi>\n <mo>|</mo>\n </mrow>\n <mrow>\n <mo>(</mo>\n <msup>\n <mover>\n <mi>R</mi>\n <mo>̇</mo>\n </mover>\n <mn>2</mn>\n </msup>\n <msup>\n <mi>B</mi>\n <mn>2</mn>\n </msup>\n <mo>−</mo>\n <msup>\n <mi>R</mi>\n <mrow>\n <mo>′</mo>\n <mn>2</mn>\n </mrow>\n </msup>\n <mo>)</mo>\n </mrow>\n <msup>\n <mi>sin</mi>\n <mn>2</mn>\n </msup>\n <mi>θ</mi>\n <mo>−</mo>\n <msup>\n <mi>B</mi>\n <mn>2</mn>\n </msup>\n <msup>\n <mi>cos</mi>\n <mn>2</mn>\n </msup>\n <mrow>\n <mi>θ</mi>\n <mo>|</mo>\n </mrow>\n </mrow>\n <annotation>$-\\ln 2-2\\ln|B|+ \\ln |(\\dot{R}^{2}B^{2}-R^{\\prime 2})\\sin ^{2}\\theta -B^{2}\\cos ^{2}\\theta|$</annotation>\n </semantics></math> respectively. The sensitivities and the lower sensitivities via <span></span><math>\n <semantics>\n <msub>\n <mi>L</mi>\n <mfrac>\n <mi>∂</mi>\n <mrow>\n <mi>∂</mi>\n <mi>t</mi>\n </mrow>\n </mfrac>\n </msub>\n <annotation>$L_{\\frac{\\partial }{\\partial t}}$</annotation>\n </semantics></math> are zero are also shown. In the quantum framework, the properties of the Einstein-Vaz shells which are the final result of the quantum gravitational collapse arising from the Lemaitre Tolman Bondi discussed by Vaz in 2014 are analyzed. In fact, Vaz showed that continued collapse to a singularity can only be obtained if one combines two independent and entire solutions of the Wheeler-DeWitt equation. Forbidding such a combination leads naturally to matter condensing on the Schwarzschild surface during quantum collapse. In that way, an entirely new framework for black holes (BHs) has emerged. The approach of Vaz was also consistent with Einstein's idea in 1939 of the localization of the collapsing particles within a thin spherical shell. Here, following an approach of oned of us (CC), we derive the BH mass and energy spectra via a Schrodinger-like approach, by further supporting Vaz's conclusions that instead of a spacetime singularity covered by an event horizon, the final result of the gravitational collapse is an essentially quantum object, an extremely compact “dark star”. This “gravitational atom” is held up not by any degeneracy pressure but by quantum gravity in the same way that ordinary atoms are sustained by quantum mechanics. Finally, the time evolution of the Einstein-Vaz shells is discussed.</p>","PeriodicalId":55150,"journal":{"name":"Fortschritte Der Physik-Progress of Physics","volume":"72 4","pages":""},"PeriodicalIF":7.8000,"publicationDate":"2024-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"On the Generalized Lemaitre Tolman Bondi Metric: Classical Sensitivities and Quantum Einstein-Vaz Shells\",\"authors\":\"Mohammadreza Molaei, Christian Corda\",\"doi\":\"10.1002/prop.202300195\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>In this paper, in the classical framework, the lower bounds for the sensitivities of the generalized Lemaitre Tolman Bondi metric are evaluated. The calculated lower bounds via the linear dynamical systems <span></span><math>\\n <semantics>\\n <msub>\\n <mi>L</mi>\\n <mfrac>\\n <mi>∂</mi>\\n <mrow>\\n <mi>∂</mi>\\n <mi>θ</mi>\\n </mrow>\\n </mfrac>\\n </msub>\\n <annotation>$L_{\\\\frac{\\\\partial }{\\\\partial \\\\theta }}$</annotation>\\n </semantics></math>, <span></span><math>\\n <semantics>\\n <msub>\\n <mi>L</mi>\\n <mfrac>\\n <mi>∂</mi>\\n <mrow>\\n <mi>∂</mi>\\n <mi>r</mi>\\n </mrow>\\n </mfrac>\\n </msub>\\n <annotation>$L_{\\\\frac{\\\\partial }{\\\\partial r}}$</annotation>\\n </semantics></math>, and <span></span><math>\\n <semantics>\\n <msub>\\n <mi>L</mi>\\n <mfrac>\\n <mi>∂</mi>\\n <mrow>\\n <mi>∂</mi>\\n <mi>ϕ</mi>\\n </mrow>\\n </mfrac>\\n </msub>\\n <annotation>$L_{\\\\frac{\\\\partial }{\\\\partial \\\\phi }}$</annotation>\\n </semantics></math> are <span></span><math>\\n <semantics>\\n <mrow>\\n <mrow>\\n <mo>−</mo>\\n <mi>ln</mi>\\n <mn>2</mn>\\n <mo>+</mo>\\n <mi>ln</mi>\\n <mo>|</mo>\\n </mrow>\\n <msup>\\n <mrow>\\n <mo>(</mo>\\n <mover>\\n <mi>R</mi>\\n <mo>̇</mo>\\n </mover>\\n <mi>B</mi>\\n <mo>)</mo>\\n </mrow>\\n <mn>2</mn>\\n </msup>\\n <mo>−</mo>\\n <msup>\\n <mrow>\\n <mo>(</mo>\\n <msup>\\n <mi>R</mi>\\n <mo>′</mo>\\n </msup>\\n <mo>)</mo>\\n </mrow>\\n <mn>2</mn>\\n </msup>\\n <mrow>\\n <mo>|</mo>\\n <mo>−</mo>\\n <mn>2</mn>\\n <mi>ln</mi>\\n <mo>|</mo>\\n <mi>B</mi>\\n <mo>|</mo>\\n </mrow>\\n </mrow>\\n <annotation>$-\\\\ln 2+\\\\ln|{(\\\\dot{R}B)}^{2}-{(R^{\\\\prime })}^{2}|-2\\\\ln|B|$</annotation>\\n </semantics></math>, <span></span><math>\\n <semantics>\\n <mrow>\\n <mrow>\\n <mn>2</mn>\\n <mi>ln</mi>\\n <mo>|</mo>\\n </mrow>\\n <mover>\\n <mi>B</mi>\\n <mo>̇</mo>\\n </mover>\\n <mrow>\\n <mo>|</mo>\\n <mo>−</mo>\\n <mi>ln</mi>\\n <mn>2</mn>\\n </mrow>\\n </mrow>\\n <annotation>$2\\\\ln|\\\\dot{B}|-\\\\ln 2$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mrow>\\n <mrow>\\n <mo>−</mo>\\n <mi>ln</mi>\\n <mn>2</mn>\\n <mo>−</mo>\\n <mn>2</mn>\\n <mi>ln</mi>\\n <mo>|</mo>\\n <mi>B</mi>\\n <mo>|</mo>\\n <mo>+</mo>\\n <mi>ln</mi>\\n <mo>|</mo>\\n </mrow>\\n <mrow>\\n <mo>(</mo>\\n <msup>\\n <mover>\\n <mi>R</mi>\\n <mo>̇</mo>\\n </mover>\\n <mn>2</mn>\\n </msup>\\n <msup>\\n <mi>B</mi>\\n <mn>2</mn>\\n </msup>\\n <mo>−</mo>\\n <msup>\\n <mi>R</mi>\\n <mrow>\\n <mo>′</mo>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n <mo>)</mo>\\n </mrow>\\n <msup>\\n <mi>sin</mi>\\n <mn>2</mn>\\n </msup>\\n <mi>θ</mi>\\n <mo>−</mo>\\n <msup>\\n <mi>B</mi>\\n <mn>2</mn>\\n </msup>\\n <msup>\\n <mi>cos</mi>\\n <mn>2</mn>\\n </msup>\\n <mrow>\\n <mi>θ</mi>\\n <mo>|</mo>\\n </mrow>\\n </mrow>\\n <annotation>$-\\\\ln 2-2\\\\ln|B|+ \\\\ln |(\\\\dot{R}^{2}B^{2}-R^{\\\\prime 2})\\\\sin ^{2}\\\\theta -B^{2}\\\\cos ^{2}\\\\theta|$</annotation>\\n </semantics></math> respectively. The sensitivities and the lower sensitivities via <span></span><math>\\n <semantics>\\n <msub>\\n <mi>L</mi>\\n <mfrac>\\n <mi>∂</mi>\\n <mrow>\\n <mi>∂</mi>\\n <mi>t</mi>\\n </mrow>\\n </mfrac>\\n </msub>\\n <annotation>$L_{\\\\frac{\\\\partial }{\\\\partial t}}$</annotation>\\n </semantics></math> are zero are also shown. In the quantum framework, the properties of the Einstein-Vaz shells which are the final result of the quantum gravitational collapse arising from the Lemaitre Tolman Bondi discussed by Vaz in 2014 are analyzed. In fact, Vaz showed that continued collapse to a singularity can only be obtained if one combines two independent and entire solutions of the Wheeler-DeWitt equation. Forbidding such a combination leads naturally to matter condensing on the Schwarzschild surface during quantum collapse. In that way, an entirely new framework for black holes (BHs) has emerged. The approach of Vaz was also consistent with Einstein's idea in 1939 of the localization of the collapsing particles within a thin spherical shell. Here, following an approach of oned of us (CC), we derive the BH mass and energy spectra via a Schrodinger-like approach, by further supporting Vaz's conclusions that instead of a spacetime singularity covered by an event horizon, the final result of the gravitational collapse is an essentially quantum object, an extremely compact “dark star”. This “gravitational atom” is held up not by any degeneracy pressure but by quantum gravity in the same way that ordinary atoms are sustained by quantum mechanics. Finally, the time evolution of the Einstein-Vaz shells is discussed.</p>\",\"PeriodicalId\":55150,\"journal\":{\"name\":\"Fortschritte Der Physik-Progress of Physics\",\"volume\":\"72 4\",\"pages\":\"\"},\"PeriodicalIF\":7.8000,\"publicationDate\":\"2024-02-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Fortschritte Der Physik-Progress of Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/prop.202300195\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Fortschritte Der Physik-Progress of Physics","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/prop.202300195","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
On the Generalized Lemaitre Tolman Bondi Metric: Classical Sensitivities and Quantum Einstein-Vaz Shells
In this paper, in the classical framework, the lower bounds for the sensitivities of the generalized Lemaitre Tolman Bondi metric are evaluated. The calculated lower bounds via the linear dynamical systems , , and are , and respectively. The sensitivities and the lower sensitivities via are zero are also shown. In the quantum framework, the properties of the Einstein-Vaz shells which are the final result of the quantum gravitational collapse arising from the Lemaitre Tolman Bondi discussed by Vaz in 2014 are analyzed. In fact, Vaz showed that continued collapse to a singularity can only be obtained if one combines two independent and entire solutions of the Wheeler-DeWitt equation. Forbidding such a combination leads naturally to matter condensing on the Schwarzschild surface during quantum collapse. In that way, an entirely new framework for black holes (BHs) has emerged. The approach of Vaz was also consistent with Einstein's idea in 1939 of the localization of the collapsing particles within a thin spherical shell. Here, following an approach of oned of us (CC), we derive the BH mass and energy spectra via a Schrodinger-like approach, by further supporting Vaz's conclusions that instead of a spacetime singularity covered by an event horizon, the final result of the gravitational collapse is an essentially quantum object, an extremely compact “dark star”. This “gravitational atom” is held up not by any degeneracy pressure but by quantum gravity in the same way that ordinary atoms are sustained by quantum mechanics. Finally, the time evolution of the Einstein-Vaz shells is discussed.
期刊介绍:
The journal Fortschritte der Physik - Progress of Physics is a pure online Journal (since 2013).
Fortschritte der Physik - Progress of Physics is devoted to the theoretical and experimental studies of fundamental constituents of matter and their interactions e. g. elementary particle physics, classical and quantum field theory, the theory of gravitation and cosmology, quantum information, thermodynamics and statistics, laser physics and nonlinear dynamics, including chaos and quantum chaos. Generally the papers are review articles with a detailed survey on relevant publications, but original papers of general interest are also published.