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Geometry and entanglement in the scattering matrix
A formulation of nucleon–nucleon scattering is developed in which the S-matrix, rather than an effective-field theory (EFT) action, is the fundamental object. Spacetime plays no role in this description: the S-matrix is a trajectory that moves between RG fixed points in a compact theory space define...
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Published in: | Annals of physics 2021-10, Vol.433 (C), p.168581, Article 168581 |
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description | A formulation of nucleon–nucleon scattering is developed in which the S-matrix, rather than an effective-field theory (EFT) action, is the fundamental object. Spacetime plays no role in this description: the S-matrix is a trajectory that moves between RG fixed points in a compact theory space defined by unitarity. This theory space has a natural operator definition, and a geometric embedding of the unitarity constraints in four-dimensional Euclidean space yields a flat torus, which serves as the stage on which the S-matrix propagates. Trajectories with vanishing entanglement are special geodesics between RG fixed points on the flat torus, while entanglement is driven by an external potential. The system of equations describing S-matrix trajectories is in general complicated, however the very-low-energy S-matrix –that appears at leading-order in the EFT description– possesses a UV/IR conformal invariance which renders the system of equations integrable, and completely determines the potential. In this geometric viewpoint, inelasticity is in correspondence with the radius of a three-dimensional hyperbolic space whose two-dimensional boundary is the flat torus. This space has a singularity at vanishing radius, corresponding to maximal violation of unitarity. The trajectory on the flat torus boundary can be explicitly constructed from a bulk trajectory with a quantifiable error, providing a simple example of a holographic quantum error correcting code.
•Geometrical S-matrix construction of nucleon–nucleon scattering.•Leading order in effective range expansion has UV/IR symmetry not seen in action.•Space of S-matrices maps to the flat torus.•Entanglement needed to probe full manifold of S-matrices.•Inelasticities correspond to the radius of a hyperbolic space. |
doi_str_mv | 10.1016/j.aop.2021.168581 |
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•Geometrical S-matrix construction of nucleon–nucleon scattering.•Leading order in effective range expansion has UV/IR symmetry not seen in action.•Space of S-matrices maps to the flat torus.•Entanglement needed to probe full manifold of S-matrices.•Inelasticities correspond to the radius of a hyperbolic space.</description><subject>Effective field theory</subject><subject>Nuclear theory</subject><subject>Quantum entanglement</subject><issn>0003-4916</issn><issn>1096-035X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNp9kEFLwzAYhoMoOKc_wFvx3pqvbdIETzJ0EwZeFLyFNPm6ZazpSIK4f29LPXv63sP7vHw8hNwDLYACfzwUejgVJS2hAC6YgAuyACp5Tiv2dUkWlNIqryXwa3IT44FSgJqJBSnXOPSYwjnT3mbok_a7I_ZjyJzP0h6zaHRKGJzfZb1Owf3ckqtOHyPe_d0l-Xx9-Vht8u37-m31vM1NxZuUm8Y2JQpWSV4LQLR1K3TFOt5qw6Q1stWyYqChpNa2XSeNRNQNRQNN2Y3ckjzMu0NMTkXjEpq9GbxHkxQIqAWvxxLMJROGGAN26hRcr8NZAVWTGXVQoxk1mVGzmZF5mhkcv_92GKZx9AatC9O2Hdw_9C91c2vV</recordid><startdate>202110</startdate><enddate>202110</enddate><creator>Beane, Silas R.</creator><creator>Farrell, Roland C.</creator><general>Elsevier Inc</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0001-7189-0424</orcidid><orcidid>https://orcid.org/0000000171890424</orcidid></search><sort><creationdate>202110</creationdate><title>Geometry and entanglement in the scattering matrix</title><author>Beane, Silas R. ; Farrell, Roland C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c367t-c7d72e85396481eed4b8a35f6bac59dc9ba9351a120ddbff9c9eea70ec172f853</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Effective field theory</topic><topic>Nuclear theory</topic><topic>Quantum entanglement</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Beane, Silas R.</creatorcontrib><creatorcontrib>Farrell, Roland C.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Annals of physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Beane, Silas R.</au><au>Farrell, Roland C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Geometry and entanglement in the scattering matrix</atitle><jtitle>Annals of physics</jtitle><date>2021-10</date><risdate>2021</risdate><volume>433</volume><issue>C</issue><spage>168581</spage><pages>168581-</pages><artnum>168581</artnum><issn>0003-4916</issn><eissn>1096-035X</eissn><abstract>A formulation of nucleon–nucleon scattering is developed in which the S-matrix, rather than an effective-field theory (EFT) action, is the fundamental object. Spacetime plays no role in this description: the S-matrix is a trajectory that moves between RG fixed points in a compact theory space defined by unitarity. This theory space has a natural operator definition, and a geometric embedding of the unitarity constraints in four-dimensional Euclidean space yields a flat torus, which serves as the stage on which the S-matrix propagates. Trajectories with vanishing entanglement are special geodesics between RG fixed points on the flat torus, while entanglement is driven by an external potential. The system of equations describing S-matrix trajectories is in general complicated, however the very-low-energy S-matrix –that appears at leading-order in the EFT description– possesses a UV/IR conformal invariance which renders the system of equations integrable, and completely determines the potential. In this geometric viewpoint, inelasticity is in correspondence with the radius of a three-dimensional hyperbolic space whose two-dimensional boundary is the flat torus. This space has a singularity at vanishing radius, corresponding to maximal violation of unitarity. The trajectory on the flat torus boundary can be explicitly constructed from a bulk trajectory with a quantifiable error, providing a simple example of a holographic quantum error correcting code.
•Geometrical S-matrix construction of nucleon–nucleon scattering.•Leading order in effective range expansion has UV/IR symmetry not seen in action.•Space of S-matrices maps to the flat torus.•Entanglement needed to probe full manifold of S-matrices.•Inelasticities correspond to the radius of a hyperbolic space.</abstract><cop>United States</cop><pub>Elsevier Inc</pub><doi>10.1016/j.aop.2021.168581</doi><orcidid>https://orcid.org/0000-0001-7189-0424</orcidid><orcidid>https://orcid.org/0000000171890424</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Effective field theory Nuclear theory Quantum entanglement |
title | Geometry and entanglement in the scattering matrix |
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