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Showing 541–570 of 1709 reference entries

Mathematics & logicSequential compactness and Euclidean Heine–Borel

In a metric space, K is compact exactly when every sequence in K has a subsequence converging to a point in K.

Mathematical statement
Mathematics & logicUniform continuity on compact domains

Uniform 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 statement
Mathematics & logicFourier mean-square convergence and Parseval

For 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 statement
Mathematics & logicUpper and lower sequence limits

For a real sequence, lim sup xₙ=lim_N sup{k≥N}xₖ and lim inf xₙ=lim_N inf{k≥N}xₖ.

Definition
Mathematics & logicLoops and simple connectedness

A 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.

Definition
InformationLogarithmic and polynomial space classes

DSPACE(s(n)) and NSPACE(s(n)) contain decision languages solvable with O(s(n)) workspace by deterministic and nondeterministic Turing machines.

Definition
InformationConstructible resource bounds

A 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.

Definition
InformationSavitch deterministic space simulation

For a space-constructible s(n)≥log n, NSPACE(s(n))⊆DSPACE(s(n)²).

Mathematical statement
InformationLogspace reductions and directed reachability

A 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 statement
InformationNL complement closure

NL=coNL: complements of nondeterministic logspace decision languages also lie in NL.

Mathematical statement
InformationDeterministic time hierarchy

For 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 statement
InformationDeterministic space hierarchy

If S is space constructible, S(n)≥n, and s(n)=o(S(n)), then DSPACE(s(n))⊊DSPACE(S(n)).

Mathematical statement
InformationTime–space inclusions and exponential time

L⊆NL⊆P⊆NP⊆PSPACE=NPSPACE⊆EXP, where EXP=⋃ₖ≥₁DTIME(2ⁿᵏ).

Mathematical statement
InformationCook–Levin satisfiability theorem

Boolean satisfiability SAT is NP-complete under polynomial-time many-one reductions.

Mathematical statement
InformationEquisatisfiable reduction from SAT to 3SAT

Introduce 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.

Method
InformationQuantified Boolean truth and PSPACE completeness

TQBF asks whether a fully quantified finite Boolean formula is true.

Mathematical statement
InformationComputable self-reference and recursion theorem

For 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 statement
InformationContext-free pumping lemma

For 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 statement
InformationA non-context-free equal-block witness

The language {0ⁿ1ⁿ2ⁿ:n≥0} is not context free.

Mathematical statement
InformationContext-sensitive grammars and linear bounded automata

Context-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 statement
Mathematics & logicDiagonalization and eigenspace multiplicities

A real n×n matrix A is diagonalizable over ℝ exactly when it has n linearly independent real eigenvectors.

Mathematical statement
Mathematics & logicCayley–Hamilton matrix identity

For 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 statement
Mathematics & logicNilpotent and Jordan-block exponentials

If Nʳ=0 and A=λI+N, then eᵗᴬ=e^(λt)Σₖ₌₀ʳ⁻¹tᵏNᵏ/k!.

Method
PhysicsHamiltonian and unitary quantum evolution

A closed quantum system evolves by iħ d|ψ⟩/dt=H(t)|ψ⟩.

Model
PhysicsStationary states and spectral superposition

For a time-independent Hamiltonian, an energy eigenstate evolves by a phase exp(−iEt/ħ).

Model
PhysicsInfinite one-dimensional potential well

With 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,… .

Model
PhysicsProbability flux and rectangular-barrier tunnelling

A real one-dimensional potential conserves probability current.

Model
PhysicsQuantum harmonic-oscillator spectrum

For H=p²/(2m)+mω²x²/2 on the real line, normalizable states have E_n=ħω(n+½), n=0,1,… .

Model
Physics · ChemistryOscillator creation and annihilation operators

For the canonical oscillator, a=√(mω/(2ħ))x+ip/√(2mħω) and its adjoint satisfy [a,a†]=1.

Model
PhysicsHeisenberg evolution and conserved observables

The Heisenberg observable A_H=U†A_SU obeys dA_H/dt=(i/ħ)[H_H,A_H]+(∂A_S/∂t)_H.

Model
ModelSource checked

Probability flux and rectangular-barrier tunnelling

Physics

A real one-dimensional potential conserves probability current.

Key knowledge

A real one-dimensional potential conserves probability current. For a rectangular barrier of height V₀ and width a with equal zero-potential exterior regions and 0<E<V₀, the transmitted flux fraction is [1+V₀² sinh²(κa)/(4E(V₀−E))]⁻¹, κ=√[2m(V₀−E)]/ħ; reflection and transmission fractions sum to one.

Values and equations

j=(ħ/m)Im(ψ*∂ψ/∂x); T=[1+V₀²sinh²(κa)/(4E(V₀−E))]⁻¹; R+T=1

j
Probability flux for a normalized 1D state s⁻¹
ψ
Position amplitude m⁻¹ᐟ²
ħ
Reduced Planck constant J s
m
Particle mass kg
x,a
Position and barrier width m
E,V₀
Incident energy and barrier height J
κ
Evanescent wavenumber m⁻¹
T,R
Transmission and reflection flux fractions

Conditions and scope

  • Stationary elastic scattering, constant m>0, a>0, no absorption, and an incoming wave from one side.
  • Match ψ and its first derivative at finite potential steps; unequal exterior velocities require a flux ratio, not just squared amplitude.
Sources · 1

References

Sources retain their recorded scope. A source link alone does not establish verification of every statement.

  1. Quantum Mechanics (2010): Square potential barrierRichard Fitzpatrick / University of Texas at AustinCourse notesfarside.ph.utexas.eduRead source

Evidence and review

Quantum Mechanics (2010): Square potential barrier: Equations 316–319, 330–336; the equal-speed flux normalization and sub-barrier continuation.

2026-10-10 · Independent AI editorial review: All 136 unique authored Physics compact statements, all hypotheses and displayed equations/variable/units tables, all 192 Physics-origin semantic links, exact 165 author inspection matrix and mapped retained conceptual claims have been independently read. Three Physics-tagged Measurement realization records are delegated to root Measurement review. Scientific source verification combines exact author section inspection with independent whole compact-content/semantic review and targeted primary rechecks recorded below; it does not claim each full source body was independently reread. Independent AI editorial review is not human specialist certification or experimental replication. Field inventory is approved after independently reviewing the two added source-inspected band-construction methods. Receipt: physics-independent-content-inventory-review.1.

Entry detailsPermanent link to this entry ↗
Record identity
physics-barrier-tunnelling
Revision
university-core.1
Structured reference record
University core expansion