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\newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{Randall-Sundrum model} \hypertarget{context}{}\subsubsection*{{Context}}\label{context} \hypertarget{gravity}{}\paragraph*{{Gravity}}\label{gravity} [[!include gravity contents]] \hypertarget{string_theory}{}\paragraph*{{String theory}}\label{string_theory} [[!include string theory - contents]] \hypertarget{contents}{}\section*{{Contents}}\label{contents} \noindent\hyperlink{idea}{Idea}\dotfill \pageref*{idea} \linebreak \noindent\hyperlink{related_concepts}{Related concepts}\dotfill \pageref*{related_concepts} \linebreak \noindent\hyperlink{references}{References}\dotfill \pageref*{references} \linebreak \noindent\hyperlink{general}{General}\dotfill \pageref*{general} \linebreak \noindent\hyperlink{as_intersecting_brane_models_in_string_theory}{As intersecting brane models in string theory}\dotfill \pageref*{as_intersecting_brane_models_in_string_theory} \linebreak \noindent\hyperlink{cosmology}{Cosmology}\dotfill \pageref*{cosmology} \linebreak \noindent\hyperlink{in_gaugehiggs_grand_unification}{In gauge-Higgs grand unification}\dotfill \pageref*{in_gaugehiggs_grand_unification} \linebreak \noindent\hyperlink{observation}{Observation}\dotfill \pageref*{observation} \linebreak \hypertarget{idea}{}\subsection*{{Idea}}\label{idea} The \emph{Randall-Sumdrum model} (\hyperlink{RandallSundrum99a}{Randall-Sundrum 99a}, \hyperlink{RandallSundrum99b}{99b}) is a class of [[string theory inspired model|string theory inspired]] [[model (physics)|models]] in combined [[cosmology]] and [[particle physics]], which assume that the [[observable universe]] constitutes the [[asymptotic boundary]] of an ambient [[anti de Sitter spacetime]]: the [[force]] of [[gravity]] would pertain to the full [[anti de Sitter spacetime|anti de sitter]] ``[[bulk]]'' [[spacetime]], but the [[gauge fields]] and [[fermion field|fermion]] [[matter fields]] would be constrained to reside on that boundary, as would hence be all observations made via [[electromagnetic radiation]] by [[observers]] inside this cosmology. Hence the extra [[bulk]] [[dimensions]] in these models need not be small (technically: the [[fiber]] spaces need not be [[compact topological spaces]] with tiny [[Riemannian geometry|Riemannian]] [[volume]]) in order to be unobservable for [[observers]]. This is in contrast to the (historically much older) [[Kaluza-Klein compactification]] models for [[physics]] with extra [[dimensions]]. Therefore Randall-Sumdrum-like models are also referred to as \emph{large extra dimension models}. One original motivation for the RS-models was the idea that this setup could address the [[hierarchy problem]]. Something at least close to Randall-Sundrum models naturally appears in [[string phenomenology]]: In [[intersecting D-brane models]] the [[standard model of particle physics]] is part of the [[worldvolume]] [[quantum field theory]] of [[D6-branes]] [[intersection|intersected]] to a 3+1-dimensional subspace. By the general lore of [[black holes in string theory]], [[non-perturbative effect|non-perturbatively]] these [[D6-branes]] are [[black branes]] with [[anti de Sitter spacetime|anti de Sitter]] [[near horizon geometry]]. Hence the [[cosmology]] of [[intersecting D-brane models]] is qualitatively of Randall-Sundrum form, even if details may differ. For the quick idea see \hyperlink{Teraguchi07}{Teraguchi 07, around slide 21}, for review and further pointers see \hyperlink{Uranga02}{Uranga 02, section 18}. For more on this see at \emph{[[intersecting D-brane models]]} the section \emph{\href{intersecting+D-brane+model#Cosmology}{Cosmology and Holography}}. \hypertarget{related_concepts}{}\subsection*{{Related concepts}}\label{related_concepts} \begin{itemize}% \item [[anti de Sitter gravity]] \item [[AdS-CFT duality]] \item [[intersecting D-brane model]] \item [[ekpyrotic cosmology]] \item [[standard model of cosmology]] \end{itemize} \hypertarget{references}{}\subsection*{{References}}\label{references} \hypertarget{general}{}\subsubsection*{{General}}\label{general} The model was introduced in \begin{itemize}% \item Lisa Randall, Raman Sundrum, \emph{A Large Mass Hierarchy from a Small Extra Dimension}, Phys.Rev.Lett.83:3370-3373, 1999 (\href{https://arxiv.org/abs/hep-ph/9905221}{arXiv:hep-ph/9905221}) \item Lisa Randall, Raman Sundrum, \emph{An Alternative to Compactification}, Phys.Rev.Lett.83:4690-4693,1999 (\href{https://arxiv.org/abs/hep-th/9906064}{arXiv:hep-th/9906064}) \end{itemize} Different but similar approaches are \begin{itemize}% \item Nima Arkani-Hamed, Savas Dimopoulos, Gia Dvali, \emph{The Hierarchy Problem and New Dimensions at a Millimeter}, Phys.Lett.B429:263-272,1998 (\href{https://arxiv.org/abs/hep-ph/9803315}{arXiv:hep-ph/9803315}) \end{itemize} and the GRS model, due to \begin{itemize}% \item Ruth Gregory, Valery A. Rubakov, Sergei M. Sibiryakov, \emph{Opening up extra dimensions at ultra-large scales}, Phys.Rev.Lett. 84 (2000) 5928-5931 (\href{https://arxiv.org/abs/hep-th/0002072}{arXiv:hep-th/0002072}) \item Csaba Csaki, Joshua Erlich, Timothy J. Hollowood, \emph{Quasi-Localization of Gravity by Resonant Modes}, Phys. Rev. Lett.84:5932-5935, 2000 (\href{https://arxiv.org/abs/hep-th/0002161}{arXiv:hep-th/0002161}) \end{itemize} a well as [[intersecting D-brane models]]. Review includes \begin{itemize}% \item Yoonbai Kim, Chong Oh Lee, Ilbong Lee, JungJai Lee, \emph{Brane World of Warp Geometry: An Introductory Review}, J. Kor. Astron. Soc. 37 (2004) 1-14 (\href{https://arxiv.org/abs/hep-th/0307023}{arXiv:hep-th/0307023}) \end{itemize} Possible relation to [[flavour anomalies]] via potential [[leptoquarks]]: \begin{itemize}% \item [[Andreas Crivellin]], \emph{Explaining the Flavour Anomalies with the Pati-Salam Vector Leptoquark}, PoS LHCP2018 (2018) 269 (\href{http://inspirehep.net/record/1713260}{spire:1713260}, \href{https://doi.org/10.22323/1.321.0269}{doi:10.22323/1.321.0269}) \item Monika Blanke, [[Andreas Crivellin]], \emph{$B$ Meson Anomalies in a Pati-Salam Model within the Randall-Sundrum Background}, Phys. Rev. Lett. 121, 011801 (2018) (\href{https://arxiv.org/abs/1801.07256}{arXiv:1801.07256}) \end{itemize} \hypertarget{as_intersecting_brane_models_in_string_theory}{}\subsubsection*{{As intersecting brane models in string theory}}\label{as_intersecting_brane_models_in_string_theory} Discussion of relation to [[string theory]] originates around \begin{itemize}% \item [[Edward Witten]], from p. 8 on in \emph{The Cosmological Constant From The Viewpoint Of String Theory}, in \emph{Sources and detection of dark matter and dark energy in the universe}, Springer 2001. 27-36. (\href{https://arxiv.org/abs/hep-ph/0002297}{arXiv:hep-ph/0002297}) \item [[Steven Giddings]], [[Shamit Kachru]], [[Joseph Polchinski]], \emph{Hierarchies from Fluxes in String Compactifications}, Phys. Rev. D66:106006, 2002 (\href{https://arxiv.org/abs/hep-th/0105097}{arXiv:hep-th/0105097}) \end{itemize} Review of the relation to [[string theory]]/[[intersecting D-brane models]] includes \begin{itemize}% \item [[Angel Uranga]], section 18 of \emph{TASI lectures on String Compactification, Model Building, and Fluxes} (\href{https://arxiv.org/abs/hep-th/0201209}{arXiv:hep-th/0201209}) \item Shunsuke Teraguchi, around slide 21 \emph{String theory and its relation to particle physics}, 2007 (\href{http://phys.cts.ntu.edu.tw/ppp7/talks/PPP7_Shunsuke_Teraguchi.pdf}{pdf}) \end{itemize} based on \begin{itemize}% \item [[Igor Klebanov]], [[Matthew Strassler]], \emph{Supergravity and a Confining Gauge Theory: Duality Cascades and $\chi^{SB}$-Resolution of Naked Singularities}, JHEP 0008:052, 2000 (\href{https://arxiv.org/abs/hep-th/0007191}{arXiv:hep-th/0007191}) \item [[Igor Klebanov]], [[Edward Witten]], \emph{Superconformal Field Theory on Threebranes at a Calabi-Yau Singularity}, Nucl.Phys.B536:199-218, 1998 (\href{https://arxiv.org/abs/hep-th/9807080}{arXiv:hep-th/9807080}) \end{itemize} with further developments including \begin{itemize}% \item Nemanja Kaloper, \emph{Origami World}, JHEP 0405 (2004) 061 (\href{https://arxiv.org/abs/hep-th/0403208}{arXiv:hep-th/0403208}) \item Antonino Flachi, Masato Minamitsuji, \emph{Field localization on a brane intersection in anti-de Sitter spacetime}, Phys.Rev.D79:104021, 2009 (\href{https://arxiv.org/abs/0903.0133}{arXiv:0903.0133}) \end{itemize} Relation to [[AdS-CFT duality]]: \begin{itemize}% \item Jiro Soda, \emph{AdS/CFT on the brane}, Lect.Notes Phys.828:235-270, 2011 (\href{https://arxiv.org/abs/1001.1011}{arXiv:1001.1011}) \end{itemize} \hypertarget{cosmology}{}\subsubsection*{{Cosmology}}\label{cosmology} Discussion of [[cosmology]] on branes in $\sim$ [[anti de Sitter spacetime|anti de Sitter]]-[[near horizon geometry|throat]] geometries: \begin{itemize}% \item Tetsuya Shiromizu, Daisuke Ida, \emph{Anti-de Sitter no-hair, AdS/CFT and the brane-world}, Phys. Rev. D64 (2001) 044015 (\href{https://arxiv.org/abs/hep-th/0102035}{arXiv:hep-th/0102035}) \item Antonio Padilla, \emph{Braneworld Cosmology and Holography} (\href{https://arxiv.org/abs/hep-th/0210217}{arxiv:hep-th/0210217}) \end{itemize} On [[de Sitter spacetime]] [[cosmology]] realized in [[brane world models]] in ambient $\sim$[[anti de Sitter spacetime|AdS]]-[[bulk]] [[spacetime]]: \begin{itemize}% \item Souvik Banerjee, [[Ulf Danielsson]], Giuseppe Dibitetto, Suvendu Giri, Marjorie Schillo, \emph{Emergent de Sitter cosmology from decaying AdS} (\href{https://arxiv.org/abs/1807.01570}{arXiv:1807.01570}) \item Souvik Banerjee, [[Ulf Danielsson]], Giuseppe Dibitetto, Suvendu Giri, Marjorie Schillo, \emph{de Sitter Cosmology on an expanding bubble} (\href{https://arxiv.org/abs/1907.04268}{arXiv:1907.04268}) \end{itemize} \hypertarget{in_gaugehiggs_grand_unification}{}\subsubsection*{{In gauge-Higgs grand unification}}\label{in_gaugehiggs_grand_unification} RS-like models for [[gauge-Higgs unification|gauge-Higgs]] [[grand unified theories]]: with [[Spin(11)]] (``[[SO(11)]]'') [[gauge group]]: \begin{itemize}% \item [[Yutaka Hosotani]], Naoki Yamatsu, \emph{Gauge–Higgs grand unification}, Progress of Theoretical and Experimental Physics, Volume 2015, Issue 11, November 2015 (\href{https://doi.org/10.1093/ptep/ptv153}{doi:10.1093/ptep/ptv153}, \href{https://doi.org/10.1093/ptep/ptw116}{doi:10.1093/ptep/ptw116}) \item Atsushi Furui, [[Yutaka Hosotani]], Naoki Yamatsu, \emph{Toward Realistic Gauge-Higgs Grand Unification}, Progress of Theoretical and Experimental Physics, Volume 2016, Issue 9, September 2016, 093B01 (\href{https://arxiv.org/abs/1606.07222}{arXiv:1606.07222}) \item [[Yutaka Hosotani]], \emph{New dimensions from gauge-Higgs unification} (\href{https://arxiv.org/abs/1702.08161}{arXiv:1702.08161}) \item [[Yutaka Hosotani]], Naoki Yamatsu, \emph{Electroweak Symmetry Breaking and Mass Spectra in Six-Dimensional Gauge-Higgs Grand Unification} (\href{https://arxiv.org/abs/1710.04811}{arXiv:1710.04811}) \end{itemize} with [[Spin(12)]] (``[[SO(12)]]'') [[gauge group]]: \begin{itemize}% \item S. Rajpoot and P. Sithikong, \emph{Implications of the $SO(12)$ gauge symmetry for grand unification}, Phys. Rev. D 23, 1649 (1981) (\href{https://doi.org/10.1103/PhysRevD.23.1649}{doi:10.1103/PhysRevD.23.1649}) \item Takaaki Nomura and Joe Sato, \emph{Standard(-like) Model from an $SO(12)$ Grand Unified Theory in six-dimensions with $S^2$ extra-space}, Nucl.Phys.B811:109-122, 2009 (\href{https://arxiv.org/abs/0810.0898}{arXiv:0810.0898}) \item Takaaki Nomura, \emph{Physics beyond the standard model with $S^2$ extra-space}, 2009 (\href{http://krishna.th.phy.saitama-u.ac.jp/joe/doctor/nomura-doctor.pdf}{pdf}, [[NomuraSO12GUT.pdf:file]]) \item Cheng-Wei Chiang, Takaaki Nomura, Joe Sato, \emph{Gauge-Higgs unification models in six dimensions with $S^2/\mathbb{Z}_2$ extra space and GUT gauge symmetry} (\href{https://arxiv.org/abs/1109.5835}{arXiv:1109.5835}) \end{itemize} \hypertarget{observation}{}\subsubsection*{{Observation}}\label{observation} \begin{itemize}% \item Indrani Banerjee, Sumanta Chakraborty, Soumitra SenGupta, \emph{Silhouette of M87${}^*$: A new window to peek into the world of hidden dimensions} (\href{https://arxiv.org/abs/1909.09385}{arXiv:1909.09385}) \end{itemize} [[!redirects Randall-Sundrum models]] [[!redirects RS model]] [[!redirects RS models]] [[!redirects RS-model]] [[!redirects RS-models]] [[!redirects GRS model]] [[!redirects GRS models]] [[!redirects GRS-model]] [[!redirects GRS-models]] \end{document}