/**
 * Quantum Hamiltonian Implementation
 *
 * This module provides a comprehensive implementation of quantum Hamiltonians,
 * which are the fundamental operators representing the total energy of quantum
 * systems. The Hamiltonian determines:
 * - System energy levels (eigenvalues)
 * - Stationary states (eigenvectors)
 * - Time evolution (through Schrödinger equation)
 *
 * Key features:
 * - Custom and predefined Hamiltonian types
 * - Time evolution generation
 * - Energy expectation calculation
 * - Support for common physical systems:
 *   * Spin-1/2 in magnetic field
 *   * Heisenberg spin chains
 *   * Harmonic oscillators
 *   * Custom interactions
 *
 * Mathematical form:
 * H = Σᵢ cᵢOᵢ where:
 * - cᵢ are complex coefficients
 * - Oᵢ are quantum operators
 *
 * @module quantum/hamiltonian
 */
import { Complex, IOperator } from '../core/types';
import { StateVector } from '../states/stateVector';
import { MatrixOperator } from './operator';
/**
 * Classifies different types of quantum Hamiltonians
 *
 * Each type represents a specific physical system:
 *
 * @property 'free' - Free particle Hamiltonian
 *    H = p²/2m (kinetic energy only)
 *
 * @property 'harmonic' - Harmonic oscillator
 *    H = p²/2m + mω²x²/2 (kinetic + potential)
 *
 * @property 'spin' - Spin system in magnetic field
 *    H = -μ·B (magnetic coupling)
 *
 * @property 'interaction' - Interaction between systems
 *    H = Σᵢⱼ Jᵢⱼ(Sᵢ·Sⱼ) (spin-spin coupling)
 *
 * @property 'custom' - User-defined Hamiltonian
 *    H = Σᵢ cᵢOᵢ (general form)
 */
export type HamiltonianType = 'free' | 'harmonic' | 'spin' | 'interaction' | 'custom' | 'non-hermitian';
/**
 * Represents a single term in a Hamiltonian expansion
 *
 * A Hamiltonian is typically expressed as a sum of terms:
 * H = Σᵢ cᵢOᵢ
 * where each term consists of:
 * - A complex coefficient cᵢ (coupling strength, energy scale)
 * - A quantum operator Oᵢ (physical observable)
 *
 * Examples:
 * - Zeeman term: H = μB·σ (coefficient = magnetic field strength)
 * - Coupling term: H = JSᵢ·Sⱼ (coefficient = exchange coupling)
 * - External field: H = εσz (coefficient = field strength)
 *
 * @property coefficient - Complex coupling strength (energy units)
 * @property operator - Quantum operator representing physical observable
 */
export interface IHamiltonianTerm {
    coefficient: Complex;
    operator: IOperator;
}
/**
 * Core Hamiltonian class representing quantum system energy operators
 *
 * The Hamiltonian is the fundamental operator in quantum mechanics that:
 * 1. Determines the total energy of the system
 * 2. Generates time evolution through Schrödinger's equation
 * 3. Defines the system's energy eigenstates
 *
 * Features:
 * - Constructs Hamiltonians from operator terms
 * - Validates Hermiticity (optional)
 * - Generates time evolution operators
 * - Computes energy expectations
 * - Supports both time-dependent and time-independent cases
 *
 * Physical Significance:
 * - Eigenvalues represent possible energy measurements
 * - Eigenvectors represent stationary states
 * - Expectation values give average energy
 * - Time evolution U(t) = exp(-iHt/ħ) describes dynamics
 *
 * @extends MatrixOperator
 */
export declare class Hamiltonian extends MatrixOperator {
    readonly hamiltonianType: HamiltonianType;
    readonly terms: IHamiltonianTerm[];
    private _timeDependent;
    constructor(dimension: number, terms: IHamiltonianTerm[], hamiltonianType?: HamiltonianType, timeDependent?: boolean, requireHermitian?: boolean);
    /**
     * Generates the quantum time evolution operator U(t) = exp(-iHt/ħ)
     *
     * The time evolution operator is fundamental in quantum mechanics:
     * - Transforms states from time t₀ to t: |ψ(t)⟩ = U(t-t₀)|ψ(t₀)⟩
     * - Preserves probability (unitary)
     * - Satisfies group properties (U(t₁)U(t₂) = U(t₁+t₂))
     *
     * Implementation:
     * 1. Validates time-independence
     * 2. Computes -iHt (using ħ = 1 units)
     * 3. Calculates matrix exponential
     * 4. Ensures unitarity
     *
     * @param time - Evolution time (in natural units)
     * @returns Unitary evolution operator U(t)
     * @throws Error for time-dependent Hamiltonians
     * @throws Error for invalid matrix structure
     */
    getEvolutionOperator(time: number): IOperator;
    /**
     * Evolves a quantum state under this Hamiltonian for time t
     *
     * Implements Schrödinger equation evolution:
     * |ψ(t)⟩ = exp(-iHt/ħ)|ψ(0)⟩
     *
     * Process:
     * 1. Validates state dimension
     * 2. Computes evolution operator U(t)
     * 3. Applies U(t) to initial state
     * 4. Ensures normalization (corrects numerical errors)
     *
     * Physical meaning:
     * - Describes how quantum state changes with time
     * - Preserves total probability (norm = 1)
     * - Maintains quantum superposition
     *
     * @param state - Initial quantum state |ψ(0)⟩
     * @param time - Evolution time t
     * @returns Evolved state |ψ(t)⟩
     * @throws Error if dimensions don't match
     */
    evolveState(state: StateVector, time: number): StateVector;
    /**
     * Computes the expectation value of energy for a given state
     *
     * The energy expectation value is:
     * ⟨E⟩ = ⟨ψ|H|ψ⟩
     *
     * Physical significance:
     * - Average energy in state |ψ⟩
     * - Real for physical (Hermitian) Hamiltonians
     * - Bounded by energy eigenvalues
     * - Constant for energy eigenstates
     *
     * @param state - Quantum state |ψ⟩
     * @returns Complex energy expectation value
     * @throws Error if dimensions don't match
     */
    expectationValue(state: StateVector): Complex;
    /**
     * Creates a spin-1/2 Hamiltonian in a magnetic field
     *
     * Implements the Zeeman Hamiltonian:
     * H = B·σ = Bxσx + Byσy + Bzσz
     * where:
     * - B = (Bx, By, Bz) is the magnetic field vector
     * - σ = (σx, σy, σz) are the Pauli matrices
     *
     * Physical significance:
     * - Describes magnetic dipole in field
     * - Energy splitting ΔE = 2|B|
     * - Precession frequency ω = 2|B|
     * - Eigenstates align/anti-align with B
     *
     * @param magneticField - [Bx, By, Bz] field components
     * @returns Spin Hamiltonian operator
     *
     * @example
     * // Create Hamiltonian for field along z-axis
     * const H = Hamiltonian.createSpinHamiltonian([0, 0, 1]);
     */
    static createSpinHamiltonian(magneticField: [number, number, number]): Hamiltonian;
    /**
     * Creates a Heisenberg interaction Hamiltonian for a spin chain
     *
     * Implements the Heisenberg model:
     * H = J Σᵢ Sᵢ·Sᵢ₊₁
     * where:
     * - J is the exchange coupling constant
     * - Sᵢ are spin operators at site i
     * - Sum runs over nearest neighbors
     *
     * The interaction term Sᵢ·Sᵢ₊₁ expands as:
     * Sᵢ·Sᵢ₊₁ = SxᵢSxᵢ₊₁ + SyᵢSyᵢ₊₁ + SzᵢSzᵢ₊₁
     *
     * Physical significance:
     * - Models magnetic interactions in materials
     * - J > 0: Ferromagnetic coupling (parallel spins favored)
     * - J < 0: Antiferromagnetic coupling (anti-parallel spins favored)
     * - Conserves total spin
     * - Supports quantum entanglement
     *
     * @param numSpins - Number of spins in the chain
     * @param coupling - Exchange coupling strength J
     * @returns Heisenberg Hamiltonian operator
     * @throws Error if numSpins < 2
     *
     * @example
     * // Create antiferromagnetic chain of 3 spins
     * const H = Hamiltonian.createHeisenbergHamiltonian(3, -1.0);
     */
    static createHeisenbergHamiltonian(numSpins: number, coupling: number): Hamiltonian;
}