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Galilean invariance in 2+1 dimensions
High Energy Physics - Theory · Submitted 8 Mar 1995
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It appears that the Galilei group in 2+1 dimensions posses a three-parameter family of projective representations.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
The Galilean invariance in three dimensional space-time is considered. It appears that the Galilei group in 2+1 dimensions posses a three-parameter family of projective representations. Their physical interpretation is discussed in some detail.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The Galilean invariance in three dimensional space-time is considered. | background 0.85 | 0.43 | 0.05 | asserted 0.88 |
| s1 | It appears that the Galilei group in 2+1 dimensions posses a three-parameter family of projective representations. | result 0.98 | 0.57 | 0.65 | hedged possibility 0.94 |
| s2 | Their physical interpretation is discussed in some detail. | interpretation 0.73 | 0.76 | 0.08 | asserted 0.81 |
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The paper
Original abstract
The Galilean invariance in three dimensional space-time is considered. It appears that the Galilei group in 2+1 dimensions posses a three-parameter family of projective representations. Their physical interpretation is discussed in some detail.
Human review
References
How the literature uses it
14 arXiv papers cite this in 25 sentences
Papers citing it · 17 sentences without a confident label
Compares with it 1 paper
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En la presencia del tercer generador central $Ž$, los �nicos Casimires de la �lgebra son los tres elementos centrales, y entonces, $H$ y $J$ no pueden ser presentados en t�rminos de los generadores de traslaciones y boosts, ver [ref] .
Exotic Newton-Hooke group, noncommutative plane and superconformal symmetry · Cohomolog�a de Eilenberg-Chevalley de $NH_-$ · 0.92
Cites it as background 6 papers
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In comparison with the Galilei algebra, described by the generators $J_ij$ (nonrelativistic rotation), $P_i$ (space translations), $K_i$ (nonrelativistic boots) and $H$ (time translations) in NH algebra one relation is deformed for the finite value $R$ of nonrelativistic $(A)dS$ radius [equation] In arbitrary dimension $D$ one can introduce one central charge described by the mass parameter $m$ [equation] If $D=2+1$ one can add second “exotic" central charge $θ$ [ref] [equation] Recently the NH symmetries were enlarged by adding the constant accelerations, described by the generator $F_i$ [ref] .
Enlarged NH symmetries: Particle Dynamics and Gauge Symmetries · Introduction · 0.94
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In the case of $2+1$ dimensions, the Galilei group admits two central extensions [ref] , one associated to the exotic non-commuting boost and other appearing in the commutator of the ordinary boost and spatial translations.
Symmetries of the Free Schr\"odinger Equation in the Non-Commutative Plane · Introduction and results · 0.83
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In a special non-relativistic limit, that is an Inönü-Wigner contraction, (2+1)D Poincaré symmetry of a free anyon theory is reduced to an exotic Galilei symmetry with two central charges [ref] .
Anisotropic harmonic oscillator, non-commutative Landau problem and exotic Newton-Hooke symmetry · Introduction · 0.85
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