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Auto-generated module
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Functions§
- adiabatic_
qc_ equivalence_ ty AdiabaticQCEquivalence : PropAdiabatic quantum computation is polynomially equivalent to the standard gate model of quantum computation.- adiabatic_
theorem_ ty AdiabaticTheorem : ∀ (gap : Real), PropThe adiabatic theorem: if a Hamiltonian is evolved slowly enough (relative to the inverse square of the spectral gap), the system remains in its instantaneous ground state.- amplitude_
amplification_ ty AmplitudeAmplification : ∀ n : Nat, ∀ k : Nat, PropGeneral amplitude amplification: if a state has success probability p, then after O(1/√p) oracle calls the success probability is amplified to nearly 1.- anyon_
ty Anyon : TypeAn anyon: a quasi-particle in (2+1)D that obeys fractional (non-Abelian) statistics under exchange.- app
- app2
- app3
- arrow
- bb84_
key_ rate_ ty BB84KeyRate : ∀ e : Real, PropThe BB84 asymptotic key rate r(e) = 1 − 2H(e), where H is the binary entropy function and e is the quantum bit-error rate.- bb84_
security_ ty BB84Security : PropInformation-theoretic security of the BB84 protocol: any eavesdropper introduces detectable disturbance, and the secret key rate is positive below the QBER threshold ≈ 11%.- bool_ty
- boson_
sampling_ hardness_ ty BosonSamplingHardness : PropBoson sampling is classically hard to simulate (under plausible complexity theoretic conjectures): efficient classical simulation would imply P^#P = BPP^NP.- boson_
sampling_ ty BosonSampling : Nat → TypeThe boson sampling problem on n photons: sample from the output distribution of a linear optical network acting on Fock states.- bqp_
contains_ bpp_ ty BQPContainsBPP : PropThe complexity class BQP (bounded-error quantum polynomial time) contains BPP (bounded-error probabilistic polynomial time): BPP ⊆ BQP.- bqp_
in_ psharp_ p_ ty BQPInPSHARPP : PropBQP is contained in P^#P (and hence in PSPACE): BQP ⊆ P^#P.- braiding_
operator_ ty BraidingOperator : Anyon → Anyon → TypeThe unitary braiding operator R_{ij} arising from exchanging two anyons.- build_
quantum_ computing_ env - cst
- dense_
coding_ protocol_ ty DenseCodingProtocol : PropSuper-dense coding: using one shared Bell pair, Alice can send 2 classical bits to Bob using only a single qubit transmission.- entanglement_
ty Entanglement : Type— entangled quantum state (e.g., Bell state).- fault_
tolerant_ threshold_ ty FaultTolerantThreshold : PropThe threshold theorem: if the physical error rate p is below a constant threshold p_th ≈ 10⁻², arbitrarily long quantum computations can be performed with exponentially suppressed logical error rates.- fibonacci_
anyon_ ty FibonacciAnyon : PropFibonacci anyons are universal for topological quantum computation: any unitary can be approximated by braiding Fibonacci anyons.- gate_
set_ ty GateSet : Type— a finite set of quantum gates.- grover_
iterations - Optimal number of Grover iterations for
n_qubitsqubits. - grover_
optimality_ ty GroverOptimality : PropGrover’s algorithm is optimal: any quantum algorithm requires Ω(√N) oracle queries for unstructured search.- grover_
speedup_ ty - Grover’s Quadratic Speedup: Grover’s algorithm solves unstructured search on N items in O(√N) queries, a quadratic speedup over classical O(N).
- grover_
success_ prob - Probability of success after
iterationsGrover iterations onn_qubitsqubits. - hamiltonian_
simulation_ ty HamiltonianSimulation : ∀ (t : Real), PropFor any local Hamiltonian H, the time-evolution operator e^{−iHt} can be approximated to precision ε in poly(n, t, 1/ε) gate complexity.- ht_
clifford_ universal_ ty HTCliffordUniversal : PropThe gate set {H, T, CNOT} is universal for quantum computation.- local_
hamiltonian_ qma_ complete_ ty LocalHamiltonianQMAComplete : PropThe k-local Hamiltonian problem is QMA-complete for k ≥ 2.- measurement_
ty Measurement : Type— quantum measurement (observable).- nat_ty
- no_
cloning_ ty - No-Cloning Theorem: it is impossible to create an identical copy of an arbitrary unknown quantum state.
- no_
deleting_ ty - No-Deleting Theorem: it is impossible to delete a copy of an arbitrary unknown quantum state given two identical copies.
- non_
abelian_ statistics_ ty NonAbelianStatistics : PropNon-Abelian anyons: the braiding operators do not commute in general, enabling topologically protected quantum gates.- period_
finding_ ty PeriodFinding : ∀ (N a : Nat), PropShor’s period-finding subroutine: for coprime a, N, the quantum period finding algorithm finds the order r of a mod N in polynomial time.- phase_
estimation_ precision_ ty PhaseEstimationPrecision : ∀ n : Nat, PhaseError n ≤ Real.pow 2 nThe phase estimation error is bounded by 2^{-n}.- phase_
estimation_ ty PhaseEstimation : ∀ (n : Nat), PropQuantum phase estimation approximates the eigenvalue e^{2πiφ} of a unitary U to n bits of precision using n ancilla qubits and O(2^n) controlled-U applications.- pi
- prop
- qaoa_
approximation_ ty QAOAApproximation : ∀ p : Nat, PropAs the QAOA depth p → ∞, the algorithm converges to the exact solution of the combinatorial optimization problem.- qaoa_
state_ ty QAOAState : Nat → TypeThe variational state produced by the Quantum Approximate Optimization Algorithm (QAOA) at depth p.- qft_
complexity_ ty QFTComplexity : ∀ n : Nat, QFTGateCount n ≤ Nat.pow n 2The QFT on n qubits requires O(n²) gates.- qft_
correctness_ ty QFTCorrectness : ∀ n : Nat, PropThe quantum Fourier transform on n qubits correctly computes the DFT of the amplitude vector.- qft_
state_ ty QFTState : Nat → TypeThe state produced by the quantum Fourier transform on n qubits.- qma_
definition_ ty QMADefinition : PropQMA (Quantum Merlin-Arthur) is the quantum analogue of NP: a problem is in QMA if there exists a polynomial-time quantum verifier and a quantum witness state.- quantum_
circuit_ ty QuantumCircuit : Type— sequence of quantum gates applied to a register.- quantum_
gate_ ty QuantumGate : Nat → Type— unitary operator on n qubits.- quantum_
hamming_ bound_ ty QuantumHammingBound : ∀ (n k t : Nat), PropThe quantum Hamming (Singleton) bound: n − k ≥ 4t for a code correcting t errors.- quantum_
teleportation_ ty - Quantum Teleportation Theorem: the quantum teleportation protocol faithfully transmits an arbitrary unknown qubit state using one shared Bell pair and two classical bits.
- quantum_
volume_ monotone_ ty QuantumVolumeMonotone : ∀ (n m : Nat), PropQuantum volume is monotone: improvements in gate fidelity and connectivity cannot decrease the quantum volume.- quantum_
volume_ ty QuantumVolume : Nat → NatThe quantum volume V_Q = 2^n where n is the largest square quantum circuit that a device can implement with at-least-2/3 probability of success.- qubit_
ty Qubit : Type— qubit state α|0⟩ + β|1⟩ in ℂ².- real_ty
- shor_
exponential_ ty - Shor’s Exponential Speedup: Shor’s algorithm factors an n-bit integer in polynomial time O(n³), an exponential speedup over the best classical algorithm.
- shor_
factoring_ ty ShorFactoring : ∀ N : Nat, PropGiven access to the period-finding subroutine, Shor’s algorithm factors N in O(log³ N) quantum gate operations with high probability.- solovay_
kitaev_ ty SolovayKitaev : ∀ (g : GateSet), UniversalGateSet g → PropThe Solovay-Kitaev theorem: any universal gate set can approximate any single-qubit unitary to precision ε in O(log^c(1/ε)) gates.- stabilizer_
code_ corrects_ errors_ ty StabilizerCodeCorrectsErrors : ∀ (n k d : Nat), PropAn [[n, k, d]] stabilizer code can correct ⌊(d−1)/2⌋ arbitrary qubit errors.- stabilizer_
code_ ty StabilizerCode : Nat → Nat → TypeAn [[n, k]] stabilizer code encodes k logical qubits into n physical qubits.- standard_
quantum_ algorithms - Standard quantum algorithms summary.
- surface_
code_ distance_ ty SurfaceCodeDistance : ∀ d : Nat, PropThe surface code with parameter d has code distance d, i.e., the minimum weight of any undetectable logical error is d.- surface_
code_ ty SurfaceCode : Nat → TypeA surface code of linear size d (code distance d, n ≈ 2d² physical qubits, 1 logical qubit).- topological_
protection_ ty TopologicalProtection : PropTopological quantum computation is inherently fault-tolerant: logical operations correspond to global topological properties immune to local perturbations.- trotter_
suzuki_ error_ ty TrotterSuzukiError : ∀ (t : Real) (r : Nat), PropThe first-order Trotter-Suzuki product formula has error O(t²/r) for r time steps.- type0
- universal_
gate_ set_ ty UniversalGateSet : GateSet → PropA gate set G is universal if any unitary can be approximated arbitrarily well by a circuit from G.- vqe_
state_ ty VQEState : TypeThe parameterized ansatz state used in the variational quantum eigensolver.- vqe_
variational_ principle_ ty VQEVariationalPrinciple : PropThe variational principle underlying VQE: the expectation value of any Hamiltonian H with any normalized state |ψ⟩ satisfies ⟨ψ|H|ψ⟩ ≥ E_0, where E_0 is the ground-state energy.