For a T0 space , evaluation against all continuous maps is a homeomorphism onto its image under the mapinto a power of the Sierpiński space. The axiom makes it injective, and the coordinate inverse images of recover every open subset of .
Between parallel boundaries, a guided shear-horizontal mode has a discrete transverse wavenumber and dispersion relation . Its cutoff frequency is .
A sheaf of modules over the sheaf of smooth functions is fine when every locally finite open cover admits a subordinate family of sheaf endomorphisms summing to the identity. Fine sheaves on a paracompact space are acyclic, so their positive-degree sheaf cohomology vanishes.
The Chebyshev estimate isIt gives upper and lower bounds of the correct linear order without asserting the Prime number theorem asymptotic .
A scheme has characteristic when in its structure sheaf of a scheme. Equivalently, its structure morphism factors through .
If is an irreducible character of a finite group and , thenEquality holds exactly when vanishes on .
D. Higman's criterion says that an -module is relative projective module for exactly when there is satisfying
Let a finite group act on an algebra by conjugation and let . The transfer ideal from isThe notation records both the source subgroup and the ambient fixed-point algebra.
If are the complex irreducible representations of a finite group and , decomposition of the regular representation gives
Let and be set partitions of the two parts of a bipartite graph. The pair of partitions is -regular whenThus a uniformly random pair in lies in an irregular cell pair with probability at most .
For the zero-frequency dispersion relationwrite . Thenwhere is the direction of the group velocity. Maximizing the angular slope gives a downstream wake wedge of semi-angle
A finite extension of number fields is unramified everywhere when every finite prime ideal is unramified. If infinite places are included in the convention, one also requires every real place to remain real.
A quasar light curve records its measured brightness as a function of time. Intrinsic accretion variability, measurement noise, and gravitational lensing can all contribute structure.
For a full-column-rank matrix , extend the thin QR decomposition to an orthogonal matrix . Thenso maps the column space of onto the first coordinate directions. Successive Householder transformations construct the same reduction without first forming a full orthogonal basis.
Let , and let be its algebraic conjugate, the other fixed point of the Möbius transformation represented by . ThenThe identity follows by transposing the continued-fraction matrix and substituting in its fixed-point equation.
The derivative at the identity of a smooth curve in is a vector fieldAfter shifting the origin perpendicular to , it becomes rotation about the axis parallel to plus translation along that axis.
Lie-symmetry determining equation for a first-order ordinary differential equation by
Codex 0 2026-10-03
For , a point-symmetry generator must satisfyIt follows by applying the first prolongation to and restricting to its solution manifold.
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