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Showing 541–570 of 1709 reference entries
In a metric space, K is compact exactly when every sequence in K has a subsequence converging to a point in K.
Mathematical statementMathematics & logicUniform continuity on compact domainsUniform continuity requires one δ>0 for each ε>0 to control d_Y(f(p),f(q))<ε whenever d_X(p,q)<δ, for all p,q.
Mathematical statementMathematics & logicFourier mean-square convergence and ParsevalFor a complex 2π-periodic Riemann-integrable f, cₙ=(2π)⁻¹∫₋π^πf(x)e⁻ⁱⁿˣdx and s_N=Σ|n|≤N cₙeⁱⁿˣ satisfy ∫|f−s_N|²→0.
Mathematical statementMathematics & logicUpper and lower sequence limitsFor a real sequence, lim sup xₙ=lim_N sup{k≥N}xₖ and lim inf xₙ=lim_N inf{k≥N}xₖ.
DefinitionMathematics & logicLoops and simple connectednessA space X is simply connected when it is path connected and every continuous loop based at a∈X deforms to the constant loop while keeping its endpoints at a.
DefinitionInformationLogarithmic and polynomial space classesDSPACE(s(n)) and NSPACE(s(n)) contain decision languages solvable with O(s(n)) workspace by deterministic and nondeterministic Turing machines.
DefinitionInformationConstructible resource boundsA time bound t(n)≥n is time constructible here when a Turing machine on unary input 1ⁿ can write 1ᵗ⁽ⁿ⁾ in O(t(n)) time.
DefinitionInformationSavitch deterministic space simulationFor a space-constructible s(n)≥log n, NSPACE(s(n))⊆DSPACE(s(n)²).
Mathematical statementInformationLogspace reductions and directed reachabilityA logspace many-one reduction computes f with x∈A exactly when f(x)∈B, using a read-only input, O(log n) work tape and write-only output.
Mathematical statementInformationNL complement closureNL=coNL: complements of nondeterministic logspace decision languages also lie in NL.
Mathematical statementInformationDeterministic time hierarchyFor time-constructible f,g≥n with f(n)log f(n)=o(g(n)), DTIME(f(n)) is a proper subset of DTIME(g(n)).
Mathematical statementInformationDeterministic space hierarchyIf S is space constructible, S(n)≥n, and s(n)=o(S(n)), then DSPACE(s(n))⊊DSPACE(S(n)).
Mathematical statementInformationTime–space inclusions and exponential timeL⊆NL⊆P⊆NP⊆PSPACE=NPSPACE⊆EXP, where EXP=⋃ₖ≥₁DTIME(2ⁿᵏ).
Mathematical statementInformationCook–Levin satisfiability theoremBoolean satisfiability SAT is NP-complete under polynomial-time many-one reductions.
Mathematical statementInformationEquisatisfiable reduction from SAT to 3SATIntroduce variables for Boolean subformula gates, constrain each gate to agree with its inputs using clauses of at most three literals, and require the output gate true.
MethodInformationQuantified Boolean truth and PSPACE completenessTQBF asks whether a fully quantified finite Boolean formula is true.
Mathematical statementInformationComputable self-reference and recursion theoremFor any Turing machine T taking a machine description and ordinary input, a machine R can behave on input x as T does on (⟨R⟩,x).
Mathematical statementInformationContext-free pumping lemmaFor every context-free language L, some p≥1 makes every w∈L with |w|≥p decomposable as w=uvxyz with |vxy|≤p, |vy|≥1 and uvⁱxyⁱz∈L for every integer i≥0.
Mathematical statementInformationA non-context-free equal-block witnessThe language {0ⁿ1ⁿ2ⁿ:n≥0} is not context free.
Mathematical statementInformationContext-sensitive grammars and linear bounded automataContext-sensitive productions replace αAβ by αγβ with γ nonempty; equivalently, their nonempty-word languages admit noncontracting productions u→v with |u|≤|v| and a nonterminal in u.
Mathematical statementMathematics & logicDiagonalization and eigenspace multiplicitiesA real n×n matrix A is diagonalizable over ℝ exactly when it has n linearly independent real eigenvectors.
Mathematical statementMathematics & logicCayley–Hamilton matrix identityFor a finite square matrix A over a field, its characteristic polynomial p(t)=det(tI−A)=tⁿ+cₙ₋₁tⁿ⁻¹+⋯+c₀ satisfies p(A)=Aⁿ+cₙ₋₁Aⁿ⁻¹+⋯+c₀I=0.
Mathematical statementMathematics & logicNilpotent and Jordan-block exponentialsIf Nʳ=0 and A=λI+N, then eᵗᴬ=e^(λt)Σₖ₌₀ʳ⁻¹tᵏNᵏ/k!.
MethodPhysicsHamiltonian and unitary quantum evolutionA closed quantum system evolves by iħ d|ψ⟩/dt=H(t)|ψ⟩.
ModelPhysicsStationary states and spectral superpositionFor a time-independent Hamiltonian, an energy eigenstate evolves by a phase exp(−iEt/ħ).
ModelPhysicsInfinite one-dimensional potential wellWith zero potential inside 0<x<L and impenetrable walls, normalized eigenfunctions are √(2/L) sin(nπx/L) and energies are n²π²ħ²/(2mL²), n=1,2,… .
ModelPhysicsProbability flux and rectangular-barrier tunnellingA real one-dimensional potential conserves probability current.
ModelPhysicsQuantum harmonic-oscillator spectrumFor H=p²/(2m)+mω²x²/2 on the real line, normalizable states have E_n=ħω(n+½), n=0,1,… .
ModelPhysics · ChemistryOscillator creation and annihilation operatorsFor the canonical oscillator, a=√(mω/(2ħ))x+ip/√(2mħω) and its adjoint satisfy [a,a†]=1.
ModelPhysicsHeisenberg evolution and conserved observablesThe Heisenberg observable A_H=U†A_SU obeys dA_H/dt=(i/ħ)[H_H,A_H]+(∂A_S/∂t)_H.
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