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For a bounded sequence $(u_n)$ in a Hilbert space, put $c_h={\mathrm{limsup}}_{N\to \infty }|N^{-1}{\sum }_{n=0}^{N-h-1}⟨u_{n+h},u_n⟩|$. If $H^{-1}{\sum }_{h=1}^H{c}_h\to 0$, then $N^{-1}{\sum }_{n=0}^{N-1}{u}_n\to 0$ in norm. Since the $c_h$ are bounded, it suffices that $(c_h)$ has convergence in density of a sequence to zero. The proof applies the Cauchy-Schwarz inequality to an average of shifted sums.

A continuous self-map of a compact metric space is uniquely ergodic when it has exactly one invariant Borel probability measure. An irrational rotation of the circle is uniquely ergodic: invariance multiplies its nonzero-index Fourier coefficients by nontrivial phases, forcing those coefficients to vanish. The Stone-Weierstrass theorem then identifies the invariant measure as normalized Lebesgue measure.

Cutting and stacking constructs measure-preserving transformations from towers of equal-measure levels. Cut a tower into equal-width subcolumns, add new spacer levels, and stack the resulting columns. Map each level to the one above by a measure-preserving identification; subsequent stages extend the partial map. When uncovered and top-level measures tend to zero, the limiting map is defined modulo null sets.

For a measurable transformation $T$, a measure is invariant if the pushforward measure equals the original measure, or equivalently $\mu (T^{-1}A)=\mu (A)$ for every measurable $A$. This is the measure used in a measure-preserving system.

For fixed positive integers $r,t$, a graph $G$ on $n$ vertices with $e(G)=(1-1/r+o(1))n^2/2$ and no balanced complete multipartite blow-up $K_{r+1}(t)$ contains an $r$-partite subgraph $H$ with $n-o(n)$ vertices, balanced classes of size $n/r+o(n)$, and minimum degree of a graph $\delta (H)=(1-1/r+o(1))n$.

One proof first removes a vanishing fraction of vertices of low degree of a vertex, finds a slowly growing $K_r(L)$ by the Erdős-Stone theorem, and assigns almost every remaining vertex to a root class in which it has fewer than $t$ neighbours of a vertex. After discarding a further vanishing fraction, a $K_{t,t}$ inside an assigned class would extend to $K_{r+1}(t)$ using the root classes. Thus internal edges and missing cross-class edges both number $o(n^2)$. Removing the vertices with unusually many missing cross-class edges gives the stated minimum degree of a graph.

An equivalence class collects all the set elements indistinguishable from a specified set element under an equivalence relation. For an equivalence relation $R$ on a set $X$, the precise definition isThe ambient set matters: a finite class for integer congruence restricted to $\{0,\dots ,8\}$ differs from the infinite residue class for the same integer congruence on all integers. We write $[x]$ when the equivalence relation and ambient set are clear.

In the finite modulo-three example,There are nine names $[x]$ but only three distinct equivalence classes. In particular, $3\in [0]$, whereas $[3]=[0]$: the first statement is membership of a set element; the second is equality of two sets.

For any equivalence relation on $X$, the essential rule isReflexivity puts $x$ in $[x{]}_R$, so the equivalence classes are nonempty and cover $X$. If two equivalence classes share $z$, the symmetric relation property and transitivity relate their defining elements through $z$; transitivity then makes their members coincide. Thus distinct equivalence classes are disjoint, giving a partition of a set. Conversely, declare two set elements equivalent when they belong to the same block of a partition of a set. The three relation properties follow immediately and its equivalence classes recover the blocks. ^[ref]

Two functions $f:A\to X$ and $g:B\to X$, whose domains lie in one ambient set, are equivalent modulo finite changes when $A△B$ is a finite set and the functions disagree at only finitely many points of $A\cap B$. The symmetric difference inclusion $A△C\subseteq (A△B)\cup (B△C)$ handles domains in a transitive chain. An exceptional set for values must also include points of $A\cap C$ absent from the middle domain $B$; these lie in the finite difference $A\setminus B$.

For fixed positive frequency and $n\ge 1$, the equatorial shallow-water dispersion relation has real zonal wavenumbers only ifBetween these values the zonal roots are complex, giving an evanescent response rather than freely propagating modes.

For epicyclic motion in a Keplerian shearing sheet, write $x-x_0=\mathrm{Re}(A{e}^{-i\Omega t})$. The energy of the radial harmonic oscillator per unit mass is $E_{\mathrm{epi}}={\Omega }^2|A{|}^2/2$. The full horizontal Jacobi energy in a shearing sheet also includes the negative guiding-center term $-3{\Omega }^2{x}_0^2/8$.

The epicyclic guiding center is the circular-orbit location about which a particle performs epicyclic motion. In a Keplerian shearing sheet, the conserved canonical momentum is $p_y=\dot{y}+2\Omega x=\Omega x_0/2$. The guiding center therefore labels the particle's first-order specific angular momentum offset, even while its instantaneous radial coordinate oscillates.

An entanglement-breaking channel admits a Kraus representation with rank-one Kraus operators $K_j=|a_j⟩⟨b_j|$. Its Choi state is a sum of positive tensor-product operators, hence separable. Conversely, spectral decompositions of each prepared state and each POVM effect in a measure-and-prepare channel produce rank-one Kraus operators. Trace preservation imposes ${\sum }_j\Vert a_j{\Vert }^2|b_j⟩⟨b_j|=I$.

A quantum channel is entanglement breaking exactly when its Choi state is a separable quantum state. If $C_{\Lambda }={\sum }_a{p}_a{\sigma }_a\otimes {\tau }_a$, the Choi reconstruction formula gives a measure-and-prepare channel with POVM $E_a=d{p}_a{\tau }_a^T$. Conversely, applying an entanglement-breaking channel to a maximally entangled state produces a separable Choi state. Horodecki, Shor and Ruskai's entanglement-breaking channel paper develops the equivalences.

For a strictly positive Dirichlet realization of an elliptic operator with smooth coefficients and smooth boundary, put $X_0=L^2(U)$. For each integer $k\ge 1$,These are the domains $D(A_D^{k/2})$, with norms equivalent to the indicated Sobolev space norms. The bilinear forms $((u,v){)}_{2l}=(L^{l}u,L^{l}v{)}_{L^2}$ and $((u,v){)}_{2l+1}=B[L^{l}u,L^{l}v]$ are inner products on $X_{2l}$ and $X_{2l+1}$. The higher boundary conditions are essential: for $L=-d^2/d{x}^2$ and $u=x(\pi -x)$, $u$ is smooth and zero at the boundary but $L^{2}u=0$, so $\Vert L^{2}u{\Vert }_2$ is not a norm on all of $H^4\cap H_0^1$. Repeated elliptic regularity proves $A_D:X_{k+2}\to X_k$ is an isomorphism, which gives the norm equivalence inductively from $X_0$ and $X_1=H_0^1$.

Let $(w_m)$ be the orthonormal basis of Dirichlet eigenfunctions for a strictly positive Dirichlet realization of an elliptic operator, with eigenvalues ${\lambda }_m$. ThenFor integers $k$, these domains are the Sobolev domains of powers of an elliptic Dirichlet operator. At $k=0$ the condition is just Parseval identity and imposes no boundary condition. At $k=1,2$ it describes $H_0^1$ and $H^2\cap H_0^1$, respectively. Higher $k$ impose traces of powers of $L$, not only the trace of $u$. For $L=-d^2/d{x}^2$ on $(0,\pi )$, the smooth Dirichlet function $u=x(\pi -x)$ has sine coefficients proportional to $m^{-3}$ for odd $m$, so the weighted sum diverges at $k=3$ despite its ordinary $H^3$ regularity.

For a constant-coefficient elliptic differential operator $P(D)$ of order $N\ge 1$, localizing the equation gives $P(D)(\chi u)=\chi P(D)u+[P(D),\chi ]u$. The commutator has order at most $N-1$, so a global Fourier transform estimate raises the known Local Sobolev space index by one until the forcing index plus $N$ is reached.

The number $m_n$ of monomials in $n$ variables with each exponent at most two and total polynomial degree at most $\lfloor 2n/3\rfloor$ satisfiesFor each exponent vector $a$ counted on the left, $1\le 2^{2n/3-{\sum }_i{a}_i}$. Summing and then allowing all $a\in \{0,1,2{\}}^n$ gives $m_n\le 2^{2n/3}(1+1/2+1/4{)}^n$. The base has cube $343/16<27$, so it is strictly less than three. This elementary weighted count gives the exponential saving in the polynomial method in combinatorics without an unstated probability estimate.

Steady conservative small-amplitude waves have divergence-free Eliassen–Palm flux by wave activity conservation. In a balanced mean state with homogeneous impermeable boundaries and no independently forced residual mean circulation, this gives zero residual circulation and zero mean acceleration. The Eulerian mean circulation can nevertheless be nonzero because the residual circulation includes an eddy-induced correction. Wave dissipation, time-dependent wave activity or boundary forcing can invalidate the conclusion.

A directed system of first-order structures and coherent elementary embeddings has a direct limit into which every member embeds elementarily. Represent an element by a pair consisting of a stage and an element at that stage; identify two representatives when their images agree at a common later stage. Interpret functions and relations at a common stage. Mathematical induction on first-order formulas proves elementarity: for an existential first-order formula true at the limit, its witness and parameters occur at a common stage, and elementarity pulls truth back to the stage containing the original parameters. This generalizes the elementary chain theorem beyond linearly ordered diagrams.

Because the electromagnetic field tensor is the exterior derivative $F=dA$ of a potential, $dF=d^{2}A=0$. For a torsion-free connection this iswhich is the covariant form of the two homogeneous Maxwell equations.

The source-free electromagnetic Lagrangian density is quadratic in the electromagnetic field tensor. Its Euler-Lagrange field equation is ${\partial }_{\mu }{F}^{\mu \nu }=0$. Antisymmetry of $F$ makes the density invariant under gauge transformations, and contraction of its indices makes it a Lorentz scalar.