Open unit ball Created 2026-10-03 Updated 2026-10-06
Loomis--Whitney inequality Created 2026-10-03 Updated 2026-10-14
For in the strip , the travel-time coordinate is . The characteristic curves areequivalently . Outside the strip the same separated ordinary differential equation gives hyperbolic cotangent branches, and the equilibrium curves are also characteristic.
Poisson-sampled continuous-time Markov chain 2026-10-03
Sample a finite-state continuous-time Markov chain with generator at the independent arrival times of a rate- Poisson process. The sampled states form a discrete-time Markov chain with transition matrixIts invariant distributions are exactly those of the continuous-time chain.
Representable presheaves are the tiny objects of an idempotent-complete finite-product category Created 2026-10-03 Updated 2026-10-05
If a small finite-product category splits idempotents, the tiny objects of its presheaf topos are exactly the representable presheaves. Exponentiation by is precomposition with and therefore has a right adjoint given by Right Kan extension. Conversely, if is tiny, then preserves all colimits; idempotent completeness makes every such presheaf representable.
Tensor square 2026-10-03
The tensor square is the second tensor power . Over a field of characteristic different from two it decomposes as the direct sum of the symmetric square and exterior square.
Symmetric power 2026-10-03
The nth symmetric power is the quotient of that identifies tensors differing by a permutation of their factors. Equivalently, over characteristic zero it is the subspace of symmetric tensors.
Logistic stochastic block model Created 2026-10-03 Updated 2026-10-06
Dirac operator 2026-10-03
The Dirac operator is the first-order elliptic operator obtained by composing the spin connection with Clifford multiplication. On an even-dimensional compact spin manifold it exchanges positive and negative chirality spinors.
If , every continuous map is null-homotopic. After simplicial approximation, its image lies in the -skeleton of a triangulation of , hence omits a point. The punctured sphere is homeomorphic to and is therefore contractible.
Nonabsoluteness of singular cardinalhood 2026-10-03
The statement that is a cardinal number with is generally neither upward nor downward absolute. Upward absoluteness can fail when a larger model collapses the cardinal; downward absoluteness can fail when a larger model adds a short cofinal sequence to a cardinal that the smaller model regards as regular.
Upward absoluteness of countability 2026-10-03
If a smaller transitive model has a function witnessing that is a countable set, the same witness exists in every larger transitive model. Downward absoluteness can fail because a larger model may contain a new enumeration of .
Downward absoluteness of cardinalhood 2026-10-03
If a larger transitive model regards an ordinal as a cardinal number, then a smaller transitive model does too: any bijection in the smaller model witnessing otherwise would remain in the larger one. The converse can fail when the larger model contains a new bijection between and a smaller ordinal.
Transitive models of ZFC have the same natural numbers and agree on whether a shared set is a finite set. Consequently they also agree on whether it is an infinite set.
Bounded formula in set theory Created 2026-10-03 Updated 2026-10-05
A bounded formula in set theory has every quantifier in one of the forms or . Such formulas are absolute between transitive models containing their parameters.
Selberg sieve weights Created 2026-10-03 Updated 2026-10-06
For , , and , direct application of their third prolongations givesThus the Schwarzian is invariant under translation and has weight minus two under dilation; the third identity is its infinitesimal projective transformation law.
For , the th prolongations of the translation, dilation, and special projective generators acting on the independent variable are
Gliding hump argument 2026-10-03
A gliding hump argument selects a subsequence and successive finite coordinate blocks so that each selected vector has little mass before and after its assigned block. A bounded dual vector can then align its signs independently on those disjoint blocks.
Over a perfect field of characteristic , the scheme-theoretic fiber of the Absolute Frobenius morphism of over a rational point isIts underlying space is one point, but its coordinate ring has a nonzero nilpotent element, so the fibre is a length- nonreduced scheme.
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