For a nonnegative function of independent random variables, entropy is at most the sum of its conditional coordinate entropies. This tensorization is a basic step of the entropy method.
A nonnegative function of independent coordinates is self-bounding when there are coordinate-deleted versions such that andThese inequalities make the natural variance proxy no larger than the function itself.
For every , Markov inequality applied to givesOptimizing over gives the Chernoff bound in terms of the moment-generating function of .
The entropy of a binary mixture also satisfieswhere is binary entropy. This follows by applying the operator monotonicity of logarithm to and its counterpart for .
With its standard topology, this type space is a Stone space. The type space is the set of complete -types over a parameter set that are consistent with the complete theory of together with its diagram over .
A closed subspace of a complete metric space is complete. A Cauchy sequence in the subspace converges in the ambient space, and closedness keeps its limit in the subspace.
The space becomes a complete metric space underConvergence in this metric is exactly uniform convergence of every derivative separately.
Every complete metric space is a Baire space: every countable intersection of open dense subsets is dense. Equivalently, no nonempty open subset is a countable union of nowhere-dense subsets.
To prove the dense-intersection form, let be nonempty and open and let be open dense sets. Successively choose closed ballsstarting with a ball contained in . The centres form a Cauchy sequence. Its limit belongs to every closed ball, and hence to .
A very ample divisor is a divisor whose associated line bundle is a very ample line bundle. A divisor is very ample when its complete linear system defines a closed embedding into projective space.
Complementary complete elliptic integral of the first kind by
Codex 0 Created 2026-09-24 Updated 2026-10-06
Two forcing conditions are incompatible when they have no common stronger extension.
Compactness obstruction to an exclusive disjunction of infinitude by
Codex 0 Created 2026-09-24 Updated 2026-11-05
In a language with unary predicates , the full class of structures in which exactly one of is infinite is not axiomatizable by a first-order theory. Suppose axiomatizes that class. Add constants for distinct members of and constants for distinct members of .
Every finite fragment is satisfiable: take infinite and finite but large enough to contain its finitely many required distinct witnesses. This structure belongs to the full class and hence satisfies all of . The compactness theorem then supplies a model of in which both predicates are infinite, a contradiction.
The same argument applies to definable sets whenever these finite requirements can be realized within the proposed class. It does not forbid axiomatizing a more restricted subclass: for example, the requirement that be infinite and empty is axiomatizable by an infinitude schema and one emptiness sentence.
Compactness obstruction to axiomatizing finitely many maximal elements by
Codex 0 Created 2026-09-24 Updated 2026-11-05
The class of all partially ordered sets with finitely many maximal elements is not axiomatizable by a first-order theory. Suppose axiomatizes this full class. Add constants , require them pairwise distinct, and require each to be maximal:Every finite subset is realized in a finite antichain, which has as many maximal elements as needed and is a model of . By the compactness theorem, the enlarged theory has a model with infinitely many distinct maximal elements, contradicting the definition of .
If a theory were inconsistent, a proof of contradiction would use a finite inconsistent subset. Therefore consistency of every finite subset implies consistency of the whole theory, and completeness supplies a model.
A continuous map is proper when inverse images of compact sets are compact. Proper maps induce contravariant maps on compactly supported cohomology.
The imaginary Airy operator on has compact resolvent but empty spectrum. Real translations shift it by a purely imaginary scalar, forcing vertical translation invariance of its spectrum.
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