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| In [[Kaluza–Klein theory]], a unification of [[general relativity]] and [[electromagnetism]], the five-fimensional Kaluza–Klein–Riemann curvature tensor (or Kaluza–Klein–Riemann–Christoffel curvature tensor) is the generalization of the four-dimensional [[Riemann curvature tensor]] (or Riemann–Christoffel curvature tensor).
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| The [[Ising model]] is a prototypical model in [[statistical physics]]. The model consists of discrete variables that represent magnetic dipole moments of atomic "spins" that can be in one of two states (+1 or −1). The spins are arranged in a graph, usually a lattice (where the local structure repeats periodically in all directions), allowing each spin to interact with its neighbors.
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| In [[differential geometry]] and in particular [[Yang–Mills theory]], Uhlenbeck's singularity theorem is a result allowing the removal of a [[Singularity (mathematics)|singularity]] of a [[Four-dimensional Yang–Mills theory|four-dimensional Yang–Mills]] field with finite energy using gauge. It states as a consequence that Yang–Mills fields with finite energy on flat [[euclidean space]] arise from Yang–Mills fields on the curved [[sphere]], its [[one-point compactification]].
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| data-sort-value=1252 | [[Special:Contribs/FrankBierFarmer|FrankBierFarmer]] (1252)
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<span style="font-style: italic; font-size: 85%;">Last updated by [[User:SDZeroBot|SDZeroBot]] <sup>''[[User:SD0001|operator]] / [[User talk:SD0001|talk]]''</sup> at
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