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$N$-Body Problem: Minimal $N$'s for Qualitative Nontrivialities
General Relativity and Quantum Cosmology · Submitted 23 Jul 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This singles out $N = 5$ and 6 in 1-$d$ and $N = 6$ and 8 in $\geq$ 2-$d$ for the onsets of various graph-theoretical nontrivialities.
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The abstract, sentence by sentence
We review the $N$-Body Problem in arbitrary dimension $d$ at the kinematical level, with modelling Background Independence in mind. In particular, we give a structural analysis of its reduced configuration spaces, decomposing this subject matter into basic Topology, Geometry, Group Theory, Linear Algebra, Graph Theory and Order Theory. At the metric level, these configuration spaces of shapes form basic geometric series for 1- and 2-$d$: $\mathbb{S}^{N - 2}$ and $\mathbb{CP}^{N - 2}$, though there are no more such series for $d \geq 3$. $d \geq 3$ also sees an onset of stratification. Casson's diagonal, for which $N = d + 1$, plays a critical role which we explain in simple Linear Algebra terms; these are moreover topologically spheres. $N = d$ and $N = d + 2$ have further significance as well, the latter as regards a counting notion of genericity of the isotropy groups and kinematical orbits realized. These observations twin the $N$ = (3, 4, 5) progression in qualitative complexity that almost all $N$-Body Problem work for concrete $N$ concentrates on with the much better-known $N$ = (2, 3, 4) progression in 2-$d$: from intervals to triangles to quadrilaterals: a large source of intuitions and mathematical analogies. We furthermore provide an Order-Theoretic genericity criterion, which is almost always bounded by the double-slope $N = 2 d + 1$ line, though an accidental relation pushes $N$ up by 1 to 8 in 3-$d$. We finally consider rubber shapes, for which the configuration spaces are graphs: much simpler than stratified manifolds, and yet containing quite a few of metric-level shapes' qualitative features. This singles out $N = 5$ and 6 in 1-$d$ and $N = 6$ and 8 in $\geq$ 2-$d$ for the onsets of various graph-theoretical nontrivialities.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We review the $N$-Body Problem in arbitrary dimension $d$ at the kinematical level, with modelling Background Independence in mind. | contribution 0.64 | 0.78 | 0.04 | asserted 0.90 |
| s1 | In particular, we give a structural analysis of its reduced configuration spaces, decomposing this subject matter into basic Topology, Geometry, Group Theory, Linear Algebra, Graph Theory and Order Theory. | contribution 0.87 | 0.88 | 0.07 | asserted 1.00 |
| s2 | At the metric level, these configuration spaces of shapes form basic geometric series for 1- and 2-$d$: $\mathbb{S}^{N - 2}$ and $\mathbb{CP}^{N - 2}$, though there are no more such series for $d \geq 3$. | result 0.95 | 0.37 | 0.12 | asserted 1.00 |
| s3 | $d \geq 3$ also sees an onset of stratification. | result 0.90 | 0.30 | 0.05 | asserted 1.00 |
| s4 | Casson's diagonal, for which $N = d + 1$, plays a critical role which we explain in simple Linear Algebra terms; these are moreover topologically spheres. | result 0.78 | 0.34 | 0.10 | asserted 1.00 |
| s5 | $N = d$ and $N = d + 2$ have further significance as well, the latter as regards a counting notion of genericity of the isotropy groups and kinematical orbits realized. | result 0.94 | 0.62 | 0.08 | asserted 1.00 |
| s6 | These observations twin the $N$ = (3, 4, 5) progression in qualitative complexity that almost all $N$-Body Problem work for concrete $N$ concentrates on with the much better-known $N$ = (2, 3, 4) progression in 2-$d$: from intervals to triangles to quadrilaterals: a large source of intuitions and mathematical analogies. | interpretation 0.67 | 0.16 | 0.11 | asserted 0.94 |
| s7 | We furthermore provide an Order-Theoretic genericity criterion, which is almost always bounded by the double-slope $N = 2 d + 1$ line, though an accidental relation pushes $N$ up by 1 to 8 in 3-$d$. | result 0.53 | 0.82 | 0.15 | asserted 0.96 |
| s8 | We finally consider rubber shapes, for which the configuration spaces are graphs: much simpler than stratified manifolds, and yet containing quite a few of metric-level shapes' qualitative features. | contribution 0.98 | 0.73 | 0.06 | asserted 1.00 |
| s9 | This singles out $N = 5$ and 6 in 1-$d$ and $N = 6$ and 8 in $\geq$ 2-$d$ for the onsets of various graph-theoretical nontrivialities. | result 0.97 | 0.75 | 0.12 | asserted 1.00 |
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The paper
Original abstract
We review the $N$-Body Problem in arbitrary dimension $d$ at the kinematical level, with modelling Background Independence in mind. In particular, we give a structural analysis of its reduced configuration spaces, decomposing this subject matter into basic Topology, Geometry, Group Theory, Linear Algebra, Graph Theory and Order Theory. At the metric level, these configuration spaces of shapes form basic geometric series for 1- and 2-$d$: $\mathbb{S}^{N - 2}$ and $\mathbb{CP}^{N - 2}$, though there are no more such series for $d \geq 3$. $d \geq 3$ also sees an onset of stratification. Casson's diagonal, for which $N = d + 1$, plays a critical role which we explain in simple Linear Algebra terms; these are moreover topologically spheres. $N = d$ and $N = d + 2$ have further significance as well, the latter as regards a counting notion of genericity of the isotropy groups and kinematical orbits realized. These observations twin the $N$ = (3, 4, 5) progression in qualitative complexity that almost all $N$-Body Problem work for concrete $N$ concentrates on with the much better-known $N$ = (2, 3, 4) progression in 2-$d$: from intervals to triangles to quadrilaterals: a large source of intuitions and mathematical analogies. We furthermore provide an Order-Theoretic genericity criterion, which is almost always bounded by the double-slope $N = 2 d + 1$ line, though an accidental relation pushes $N$ up by 1 to 8 in 3-$d$. We finally consider rubber shapes, for which the configuration spaces are graphs: much simpler than stratified manifolds, and yet containing quite a few of metric-level shapes' qualitative features. This singles out $N = 5$ and 6 in 1-$d$ and $N = 6$ and 8 in $\geq$ 2-$d$ for the onsets of various graph-theoretical nontrivialities.
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How the literature uses it
13 arXiv papers cite this in 53 sentences
Papers citing it · 36 sentences without a confident label
Builds on it 1 paper
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This is derived in [ref] for 3-$d$ and in the current Article for 0- to 2-$d$.
Isotropy Groups and Kinematic Orbits for 1 and 2-$d$ $N$-Body Problems · Minimal-$N$ cases dimension by dimension · 0.85
Uses its method or tool 2 papers
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In particular, subsequent sections benefit from rephrasing ([ref]) by use of the particular linear combination (ρ^i) , These $ρ^i$ are some $N$-point choice of (if relevant, mass-weighted) relative Jacobi coordinates [ref] .
Specific PDEs for Preserved Quantities in Geometry. I. Similarities and Subgroups · 1-$d$ translations · 0.86
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Upon doing this, Jacobi coordinates [ref] furthermore furnish a widespread simplification of one's remaining equations [ref] .
Spaces of Observables from Solving PDEs. I. Translation-Invariant Theory · PDE reformulation · 0.98
Compares with it 1 paper
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2) Compare with Cartan's [ref] more well-known differential theory of invariants [ref] , in particular as regards the extent to which this can be interpreted in subsequently-introduced shape-theoretic terms [ref] .
Shape Derivatives · Conclusion · 1.00
Cites it as background 8 papers
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We conclude with an outline of pointers to further research directions in Sec 8; see also [ref] for further details.
Isotropy Groups and Kinematic Orbits for 1 and 2-$d$ $N$-Body Problems · Introduction · 0.80
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General Kendall-type Shape(-and-Scale) Theory [ref] is the culmination of the following four layers of structure.
Shape Theories. I. Their Diversity is Killing-Based and thus Nongeneric · Kendall's Shape Theory and its Leibnizian scaled counterpart · 0.97
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This rests on Sec 2's preliminary outline of configuration space $$ [ref] , configurations being `what is left' to build upon in primarily timeless pictures, including via building velocity, change or momentum bundles thereover.
A Local Resolution of the Problem of Time. I. Introduction and Temporal Relationalism · Outline of the rest of this Article · 0.91
What it cites · 53 sentences without a confident label
Compares with 4 papers
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A fairly high proportion of this information is new to the current article and to [ref] .
The Smallest Shape Spaces. I. Shape Theory Posed, with Example of 3 Points on the Line · Summary of results · 0.85
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A fairly high proportion of this information is new to the current article and to [ref] .
The Smallest Shape Spaces. II. 4 Points in 1-d Suffices to have a Complex Background-Independent Theory of Inhomogeneity · Summary of results · 0.85
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A fairly high proportion of this information is new to the current article and to [ref] .
The Smallest Shape Spaces. III. Triangles in 2- and 3-d · Summary of results · 0.85
Cites as support 1 paper
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$n = 2$ is the minimal dependentland, supports the first relationally nontrivial shape-and-scale theory [ref] , and is both C- and O-generic.
The Smallest Shape Spaces. I. Shape Theory Posed, with Example of 3 Points on the Line · Summary of results · 0.98
Cites as background 20 papers
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Such graphs are further studied in the recent article [ref] .
Rubber Relationalism: Smallest Graph-Theoretically Nontrivial Leibniz Spaces · Topological shape spaces · 0.81
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Remark 25 See Sec [ref] and [ref] for further instances of Graph Theory entering Shape Theory.
The Smallest Shape Spaces. I. Shape Theory Posed, with Example of 3 Points on the Line · $ℝ^d$ relative space · 0.96
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Remark 25 See Sec [ref] and [ref] for further instances of Graph Theory entering Shape Theory.
The Smallest Shape Spaces. II. 4 Points in 1-d Suffices to have a Complex Background-Independent Theory of Inhomogeneity · $ℝ^d$ relative space · 0.96
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