FireEcho / quantum /algorithms.py
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"""
FireEcho Quantum Gold - Standard Quantum Algorithms
Implements common quantum algorithms and state preparations:
- Bell states (maximally entangled 2-qubit states)
- GHZ states (n-qubit entangled states)
- Quantum Fourier Transform (QFT)
- Grover's search algorithm primitives
These serve as both utilities and benchmarks for the simulator.
"""
import torch
import math
from typing import Optional, List
from .circuit import QuantumCircuit
from .simulator import QuantumSimulator, StateVector
def bell_state(variant: int = 0, device: str = 'cuda:0') -> StateVector:
"""
Create one of the four Bell states.
Bell states are maximally entangled 2-qubit states:
- Φ⁺ = (|00⟩ + |11⟩)/√2 (variant=0)
- Φ⁻ = (|00⟩ - |11⟩)/√2 (variant=1)
- Ψ⁺ = (|01⟩ + |10⟩)/√2 (variant=2)
- Ψ⁻ = (|01⟩ - |10⟩)/√2 (variant=3)
Args:
variant: Which Bell state (0-3)
device: CUDA device
Returns:
Bell state vector
Example:
state = bell_state(0) # (|00⟩ + |11⟩)/√2
# Verify entanglement
from .measurement import entanglement_entropy
S = entanglement_entropy(state, [0]) # Should be 1.0
"""
qc = QuantumCircuit(2, f"bell_{variant}")
# Start with |00⟩
# Apply H to qubit 0: (|0⟩ + |1⟩)/√2 ⊗ |0⟩
qc.h(0)
# CNOT creates entanglement: (|00⟩ + |11⟩)/√2
qc.cx(0, 1)
# Variants modify the state
if variant == 1:
# Φ⁻: Apply Z to add relative phase
qc.z(0)
elif variant == 2:
# Ψ⁺: Apply X to flip second qubit
qc.x(1)
elif variant == 3:
# Ψ⁻: Apply both
qc.z(0)
qc.x(1)
sim = QuantumSimulator(device)
return sim.run(qc)
def ghz_state(num_qubits: int, device: str = 'cuda:0') -> StateVector:
"""
Create a GHZ (Greenberger-Horne-Zeilinger) state.
GHZ state: (|00...0⟩ + |11...1⟩)/√2
This is the maximally entangled n-qubit state, generalizing
the Bell state to n qubits.
Args:
num_qubits: Number of qubits (≥2)
device: CUDA device
Returns:
GHZ state vector
Example:
state = ghz_state(3) # (|000⟩ + |111⟩)/√2
# Sample measurements - only "000" or "111"
counts = sample(state, shots=1000)
"""
if num_qubits < 2:
raise ValueError("GHZ state requires at least 2 qubits")
qc = QuantumCircuit(num_qubits, f"ghz_{num_qubits}")
# Hadamard on first qubit
qc.h(0)
# CNOT cascade
for i in range(1, num_qubits):
qc.cx(0, i)
sim = QuantumSimulator(device)
return sim.run(qc)
def w_state(num_qubits: int, device: str = 'cuda:0') -> StateVector:
"""
Create a W state.
W state: (|100...0⟩ + |010...0⟩ + ... + |000...1⟩)/√n
W states are entangled but more robust to qubit loss than GHZ.
Args:
num_qubits: Number of qubits (≥2)
device: CUDA device
Returns:
W state vector
"""
if num_qubits < 2:
raise ValueError("W state requires at least 2 qubits")
# Direct construction
state = StateVector.zeros(num_qubits, device)
norm = 1.0 / math.sqrt(num_qubits)
for i in range(num_qubits):
idx = 1 << i # Single 1 in position i
state.amplitudes[idx] = norm
state.amplitudes[0] = 0 # Clear |000...0⟩
return state
def qft(num_qubits: int) -> QuantumCircuit:
"""
Create Quantum Fourier Transform circuit.
QFT transforms computational basis states to Fourier basis:
|j⟩ → (1/√N) Σₖ e^(2πijk/N) |k⟩
QFT is a key subroutine in Shor's algorithm and quantum
phase estimation.
Args:
num_qubits: Number of qubits
Returns:
QFT circuit
Example:
qc = qft(4)
sim = QuantumSimulator()
state = sim.run(qc)
"""
qc = QuantumCircuit(num_qubits, f"qft_{num_qubits}")
for i in range(num_qubits):
# Hadamard on qubit i
qc.h(i)
# Controlled rotations
for j in range(i + 1, num_qubits):
angle = math.pi / (2 ** (j - i))
qc.cp(angle, j, i)
# Swap qubits to reverse order (standard QFT convention)
for i in range(num_qubits // 2):
qc.swap(i, num_qubits - 1 - i)
return qc
def inverse_qft(num_qubits: int) -> QuantumCircuit:
"""
Create inverse Quantum Fourier Transform circuit.
QFT† is the adjoint (inverse) of QFT:
QFT† · QFT = I
Args:
num_qubits: Number of qubits
Returns:
Inverse QFT circuit
"""
return qft(num_qubits).inverse()
def grover_diffusion(num_qubits: int) -> QuantumCircuit:
"""
Create Grover diffusion operator circuit.
D = 2|s⟩⟨s| - I where |s⟩ is uniform superposition.
Also known as the "inversion about the mean" operator.
Args:
num_qubits: Number of qubits
Returns:
Diffusion operator circuit
"""
qc = QuantumCircuit(num_qubits, "grover_diffusion")
# H⊗n
for i in range(num_qubits):
qc.h(i)
# X⊗n
for i in range(num_qubits):
qc.x(i)
# Multi-controlled Z (via decomposition)
if num_qubits == 2:
qc.cz(0, 1)
elif num_qubits == 3:
# CCZ = H-CCX-H on target
qc.h(2)
qc.ccx(0, 1, 2)
qc.h(2)
else:
# General multi-controlled Z
# Use H on last qubit, multi-controlled X, H again
qc.h(num_qubits - 1)
# Decompose multi-controlled X (simplified)
for i in range(num_qubits - 2):
qc.ccx(i, i + 1, num_qubits - 1)
qc.h(num_qubits - 1)
# X⊗n
for i in range(num_qubits):
qc.x(i)
# H⊗n
for i in range(num_qubits):
qc.h(i)
return qc
def quantum_phase_estimation(num_counting_qubits: int, unitary_circuit: QuantumCircuit) -> QuantumCircuit:
"""
Create Quantum Phase Estimation circuit.
QPE estimates the phase φ in U|ψ⟩ = e^(2πiφ)|ψ⟩.
Args:
num_counting_qubits: Precision qubits for phase estimate
unitary_circuit: Circuit implementing unitary U
Returns:
QPE circuit
Note: The unitary eigenstate should be prepared separately.
"""
total_qubits = num_counting_qubits + unitary_circuit.num_qubits
qc = QuantumCircuit(total_qubits, "qpe")
# Hadamard on counting qubits
for i in range(num_counting_qubits):
qc.h(i)
# Controlled-U^(2^k) operations
for k in range(num_counting_qubits):
# Apply U^(2^k) controlled by qubit k
repetitions = 2 ** k
for _ in range(repetitions):
# Add controlled version of unitary
# (simplified - actual implementation needs controlled gates)
for gate in unitary_circuit.gates:
if gate.name == "RZ":
qc.crz(gate.params[0], k, num_counting_qubits + gate.targets[0])
# Inverse QFT on counting qubits
inv_qft = inverse_qft(num_counting_qubits)
qc.compose(inv_qft, list(range(num_counting_qubits)))
return qc
def random_circuit(num_qubits: int, depth: int, seed: Optional[int] = None) -> QuantumCircuit:
"""
Create a random quantum circuit.
Useful for benchmarking and testing.
Args:
num_qubits: Number of qubits
depth: Circuit depth
seed: Random seed
Returns:
Random circuit
"""
import random
if seed is not None:
random.seed(seed)
qc = QuantumCircuit(num_qubits, f"random_{num_qubits}x{depth}")
single_gates = ['h', 'x', 'y', 'z', 's', 't']
rotation_gates = ['rx', 'ry', 'rz']
for _ in range(depth):
# Single-qubit layer
for q in range(num_qubits):
gate_type = random.choice(single_gates + rotation_gates)
if gate_type in single_gates:
getattr(qc, gate_type)(q)
else:
angle = random.uniform(0, 2 * math.pi)
getattr(qc, gate_type)(angle, q)
# Two-qubit layer (CNOTs on adjacent pairs)
for q in range(0, num_qubits - 1, 2):
if random.random() > 0.5:
qc.cx(q, q + 1)
return qc
# =============================================================================
# Variational Circuits (for VQE/QAOA)
# =============================================================================
def variational_ansatz(num_qubits: int, num_layers: int, params: List[float]) -> QuantumCircuit:
"""
Create a variational ansatz circuit for VQE.
Hardware-efficient ansatz with Ry-CNOT structure.
Args:
num_qubits: Number of qubits
num_layers: Number of variational layers
params: Rotation parameters (length = num_qubits * num_layers * 2)
Returns:
Parameterized circuit
"""
expected_params = num_qubits * num_layers * 2
if len(params) != expected_params:
raise ValueError(f"Expected {expected_params} parameters, got {len(params)}")
qc = QuantumCircuit(num_qubits, f"vqe_ansatz_{num_layers}L")
param_idx = 0
for layer in range(num_layers):
# Rotation layer
for q in range(num_qubits):
qc.ry(params[param_idx], q)
param_idx += 1
qc.rz(params[param_idx], q)
param_idx += 1
# Entangling layer (linear connectivity)
for q in range(num_qubits - 1):
qc.cx(q, q + 1)
return qc
def qaoa_circuit(num_qubits: int, p: int, gamma: List[float], beta: List[float]) -> QuantumCircuit:
"""
Create QAOA (Quantum Approximate Optimization Algorithm) circuit.
Standard QAOA ansatz for combinatorial optimization.
Args:
num_qubits: Number of qubits
p: Number of QAOA layers
gamma: Cost unitary parameters
beta: Mixer unitary parameters
Returns:
QAOA circuit
"""
if len(gamma) != p or len(beta) != p:
raise ValueError(f"Expected {p} gamma and beta values each")
qc = QuantumCircuit(num_qubits, f"qaoa_p{p}")
# Initial superposition
for q in range(num_qubits):
qc.h(q)
for layer in range(p):
# Cost unitary (problem-dependent ZZ interactions)
for i in range(num_qubits - 1):
qc.cx(i, i + 1)
qc.rz(gamma[layer], i + 1)
qc.cx(i, i + 1)
# Mixer unitary (X rotations)
for q in range(num_qubits):
qc.rx(2 * beta[layer], q)
return qc
# =============================================================================
# VQE (Variational Quantum Eigensolver)
# =============================================================================
class VQE:
"""
Variational Quantum Eigensolver for finding ground state energies.
VQE is a hybrid quantum-classical algorithm that uses:
1. Quantum circuit to prepare trial wavefunctions
2. Classical optimizer to minimize energy expectation value
Example:
from quantum.algorithms import VQE
# Define Hamiltonian (e.g., H2 molecule)
hamiltonian = [
(0.5, 'ZZ', [0, 1]),
(-0.5, 'X', [0]),
(-0.5, 'X', [1]),
]
vqe = VQE(num_qubits=2, num_layers=2)
energy, params = vqe.run(hamiltonian)
"""
def __init__(
self,
num_qubits: int,
num_layers: int = 2,
ansatz_type: str = 'hardware_efficient',
device: str = 'cuda:0'
):
"""
Args:
num_qubits: Number of qubits
num_layers: Depth of variational ansatz
ansatz_type: 'hardware_efficient', 'uccsd', or 'hea'
device: CUDA device
"""
self.num_qubits = num_qubits
self.num_layers = num_layers
self.ansatz_type = ansatz_type
self.device = device
self.sim = QuantumSimulator(device)
# Parameter count depends on ansatz
if ansatz_type == 'hardware_efficient':
self.num_params = num_qubits * num_layers * 2
elif ansatz_type == 'uccsd':
self.num_params = num_qubits * (num_qubits - 1)
else:
self.num_params = num_qubits * num_layers * 3
def build_circuit(self, params: List[float]) -> QuantumCircuit:
"""Build variational circuit with given parameters."""
if self.ansatz_type == 'hardware_efficient':
return variational_ansatz(self.num_qubits, self.num_layers, params)
elif self.ansatz_type == 'uccsd':
return self._build_uccsd_ansatz(params)
else:
return self._build_hea_ansatz(params)
def _build_uccsd_ansatz(self, params: List[float]) -> QuantumCircuit:
"""Build UCCSD (Unitary Coupled Cluster) ansatz."""
qc = QuantumCircuit(self.num_qubits, "uccsd")
# Hartree-Fock initial state (alternating |1⟩|0⟩)
for i in range(0, self.num_qubits, 2):
qc.x(i)
# Single excitations
param_idx = 0
for p in range(0, self.num_qubits, 2):
for q in range(1, self.num_qubits, 2):
if param_idx < len(params):
# Givens rotation for single excitation
theta = params[param_idx]
qc.cx(p, q)
qc.ry(theta, p)
qc.cx(p, q)
param_idx += 1
return qc
def _build_hea_ansatz(self, params: List[float]) -> QuantumCircuit:
"""Build Hardware-Efficient Ansatz with Ry-Rz-CNOT."""
qc = QuantumCircuit(self.num_qubits, "hea")
param_idx = 0
for layer in range(self.num_layers):
# Ry layer
for q in range(self.num_qubits):
qc.ry(params[param_idx], q)
param_idx += 1
# Rz layer
for q in range(self.num_qubits):
qc.rz(params[param_idx], q)
param_idx += 1
# Rx layer
for q in range(self.num_qubits):
qc.rx(params[param_idx], q)
param_idx += 1
# Entangling layer
for q in range(self.num_qubits - 1):
qc.cx(q, q + 1)
if self.num_qubits > 2:
qc.cx(self.num_qubits - 1, 0) # Ring topology
return qc
def compute_expectation(
self,
params: List[float],
hamiltonian: List[tuple]
) -> float:
"""
Compute expectation value ⟨ψ|H|ψ⟩.
Args:
params: Variational parameters
hamiltonian: List of (coeff, pauli_string, qubits) tuples
e.g., [(0.5, 'ZZ', [0,1]), (-0.3, 'X', [0])]
Returns:
Energy expectation value
"""
qc = self.build_circuit(params)
state = self.sim.run(qc)
total_energy = 0.0
for coeff, pauli_string, qubits in hamiltonian:
# Measure in appropriate basis
exp_val = self._measure_pauli_string(state, pauli_string, qubits)
total_energy += coeff * exp_val
return total_energy
def _measure_pauli_string(
self,
state: StateVector,
pauli_string: str,
qubits: List[int]
) -> float:
"""
Measure expectation of Pauli string on specified qubits.
For multi-qubit states, we need to properly handle the tensor structure.
"""
import torch
if len(pauli_string) != len(qubits):
raise ValueError("Pauli string length must match qubit count")
# Define Pauli matrices
I = torch.eye(2, dtype=torch.complex64, device=state.amplitudes.device)
X = torch.tensor([[0, 1], [1, 0]], dtype=torch.complex64, device=state.amplitudes.device)
Y = torch.tensor([[0, -1j], [1j, 0]], dtype=torch.complex64, device=state.amplitudes.device)
Z = torch.tensor([[1, 0], [0, -1]], dtype=torch.complex64, device=state.amplitudes.device)
paulis = {'I': I, 'X': X, 'Y': Y, 'Z': Z}
# Build full observable by tensor product
num_qubits = state.num_qubits
# Start with identity on all qubits
ops = [I.clone() for _ in range(num_qubits)]
# Place Paulis on specified qubits
for pauli, qubit in zip(pauli_string, qubits):
ops[qubit] = paulis[pauli]
# Compute tensor product
full_obs = ops[0]
for op in ops[1:]:
full_obs = torch.kron(full_obs, op)
# Compute expectation: ⟨ψ|O|ψ⟩
psi = state.amplitudes
o_psi = torch.mv(full_obs, psi)
expectation = torch.vdot(psi, o_psi).real
return expectation.item()
def run(
self,
hamiltonian: List[tuple],
max_iters: int = 100,
learning_rate: float = 0.1,
callback: Optional[callable] = None
) -> tuple:
"""
Run VQE optimization.
Args:
hamiltonian: List of (coeff, pauli_string, qubits)
max_iters: Maximum optimization iterations
learning_rate: Gradient descent step size
callback: Optional callback(iter, energy, params)
Returns:
(final_energy, optimal_params)
"""
import random
# Initialize random parameters
params = [random.uniform(-math.pi, math.pi) for _ in range(self.num_params)]
best_energy = float('inf')
best_params = params.copy()
for iteration in range(max_iters):
# Compute energy
energy = self.compute_expectation(params, hamiltonian)
if energy < best_energy:
best_energy = energy
best_params = params.copy()
if callback:
callback(iteration, energy, params)
# Parameter shift gradient
gradients = []
for i in range(len(params)):
params_plus = params.copy()
params_minus = params.copy()
params_plus[i] += math.pi / 2
params_minus[i] -= math.pi / 2
e_plus = self.compute_expectation(params_plus, hamiltonian)
e_minus = self.compute_expectation(params_minus, hamiltonian)
grad = (e_plus - e_minus) / 2
gradients.append(grad)
# Update parameters
for i in range(len(params)):
params[i] -= learning_rate * gradients[i]
return best_energy, best_params
# =============================================================================
# QSVM (Quantum Support Vector Machine)
# =============================================================================
class QSVM:
"""
Quantum Support Vector Machine for classification.
Uses quantum feature maps to encode classical data into quantum states,
enabling kernel-based classification in exponentially large Hilbert space.
Example:
from quantum.algorithms import QSVM
# Binary classification
qsvm = QSVM(num_features=4, num_qubits=4)
# Train
X_train = [[0.1, 0.2, 0.3, 0.4], ...]
y_train = [0, 1, 0, 1, ...]
qsvm.fit(X_train, y_train)
# Predict
predictions = qsvm.predict(X_test)
"""
def __init__(
self,
num_features: int,
num_qubits: Optional[int] = None,
feature_map: str = 'zz',
num_layers: int = 2,
device: str = 'cuda:0'
):
"""
Args:
num_features: Dimension of input data
num_qubits: Number of qubits (defaults to num_features)
feature_map: 'zz', 'pauli', or 'iqp'
num_layers: Feature map depth
device: CUDA device
"""
self.num_features = num_features
self.num_qubits = num_qubits or num_features
self.feature_map_type = feature_map
self.num_layers = num_layers
self.device = device
self.sim = QuantumSimulator(device)
# Storage for training data (for kernel computation)
self.X_train = None
self.y_train = None
self.alpha = None # SVM dual coefficients
def _build_feature_map(self, x: List[float]) -> QuantumCircuit:
"""Build quantum feature map circuit for data point x."""
if len(x) < self.num_qubits:
x = list(x) + [0.0] * (self.num_qubits - len(x))
qc = QuantumCircuit(self.num_qubits, "feature_map")
if self.feature_map_type == 'zz':
return self._zz_feature_map(qc, x)
elif self.feature_map_type == 'pauli':
return self._pauli_feature_map(qc, x)
else:
return self._iqp_feature_map(qc, x)
def _zz_feature_map(self, qc: QuantumCircuit, x: List[float]) -> QuantumCircuit:
"""ZZ Feature Map - encodes data through ZZ interactions."""
for layer in range(self.num_layers):
# Hadamard layer
for q in range(self.num_qubits):
qc.h(q)
# Feature encoding layer
for q in range(self.num_qubits):
qc.rz(2 * x[q], q)
# Entangling layer with product features
for i in range(self.num_qubits - 1):
qc.cx(i, i + 1)
qc.rz(2 * (math.pi - x[i]) * (math.pi - x[i + 1]), i + 1)
qc.cx(i, i + 1)
return qc
def _pauli_feature_map(self, qc: QuantumCircuit, x: List[float]) -> QuantumCircuit:
"""Pauli Feature Map - encodes through Pauli rotations."""
for layer in range(self.num_layers):
# Hadamard layer
for q in range(self.num_qubits):
qc.h(q)
# Z rotations
for q in range(self.num_qubits):
qc.rz(x[q], q)
# ZZ interactions
for i in range(self.num_qubits - 1):
qc.cx(i, i + 1)
qc.rz(x[i] * x[i + 1], i + 1)
qc.cx(i, i + 1)
return qc
def _iqp_feature_map(self, qc: QuantumCircuit, x: List[float]) -> QuantumCircuit:
"""IQP (Instantaneous Quantum Polynomial) Feature Map."""
for layer in range(self.num_layers):
# Hadamard layer
for q in range(self.num_qubits):
qc.h(q)
# Diagonal gates encoding
for q in range(self.num_qubits):
qc.rz(x[q], q)
# Cross terms
for i in range(self.num_qubits):
for j in range(i + 1, self.num_qubits):
qc.cx(i, j)
qc.rz(x[i] * x[j], j)
qc.cx(i, j)
return qc
def compute_kernel(self, x1: List[float], x2: List[float]) -> float:
"""
Compute quantum kernel K(x1, x2) = |⟨φ(x1)|φ(x2)⟩|².
This is the probability of measuring |0...0⟩ after preparing
the state U†(x2)U(x1)|0⟩.
"""
# Build circuits
qc1 = self._build_feature_map(x1)
qc2 = self._build_feature_map(x2)
# Combined circuit: U(x1) followed by U†(x2)
combined = QuantumCircuit(self.num_qubits, "kernel")
combined.compose(qc1, list(range(self.num_qubits)))
combined.compose(qc2.inverse(), list(range(self.num_qubits)))
# Run and get probability of |0...0⟩
state = self.sim.run(combined)
p_zero = (state.amplitudes[0].abs() ** 2).item()
return p_zero
def compute_kernel_matrix(self, X: List[List[float]]) -> torch.Tensor:
"""Compute full kernel matrix for dataset."""
n = len(X)
K = torch.zeros(n, n, device=self.device)
for i in range(n):
for j in range(i, n):
k_ij = self.compute_kernel(X[i], X[j])
K[i, j] = k_ij
K[j, i] = k_ij
return K
def fit(self, X: List[List[float]], y: List[int], C: float = 1.0):
"""
Fit QSVM to training data.
Args:
X: Training features, shape [n_samples, n_features]
y: Training labels, {0, 1} or {-1, 1}
C: Regularization parameter
"""
self.X_train = X
self.y_train = [1 if label > 0 else -1 for label in y]
n = len(X)
# Compute kernel matrix
K = self.compute_kernel_matrix(X)
# Convert to numpy for SVM solver
K_np = K.cpu().numpy()
y_np = torch.tensor(self.y_train, dtype=torch.float32).numpy()
# Simple gradient descent for dual SVM
self.alpha = torch.zeros(n, device=self.device)
for iteration in range(100):
for i in range(n):
# Compute gradient for alpha[i]
grad = 1.0
for j in range(n):
grad -= self.alpha[j].item() * self.y_train[j] * self.y_train[i] * K[i, j].item()
# Update
self.alpha[i] = max(0, min(C, self.alpha[i] + 0.01 * grad))
def predict(self, X: List[List[float]]) -> List[int]:
"""Predict labels for new data."""
if self.X_train is None:
raise ValueError("Model not fitted. Call fit() first.")
predictions = []
for x in X:
# Compute kernel with all training points
decision = 0.0
for i, x_train in enumerate(self.X_train):
k = self.compute_kernel(x, x_train)
decision += self.alpha[i].item() * self.y_train[i] * k
predictions.append(1 if decision > 0 else 0)
return predictions
def score(self, X: List[List[float]], y: List[int]) -> float:
"""Compute classification accuracy."""
predictions = self.predict(X)
correct = sum(1 for p, t in zip(predictions, y) if p == t)
return correct / len(y)
# =============================================================================
# Quantum Autoencoder
# =============================================================================
def quantum_autoencoder_circuit(
num_qubits: int,
latent_qubits: int,
params: List[float]
) -> QuantumCircuit:
"""
Create a quantum autoencoder circuit.
Compresses num_qubits down to latent_qubits through a trash-latent separation.
Args:
num_qubits: Input dimension
latent_qubits: Compressed dimension
params: Variational parameters
Returns:
Autoencoder circuit
"""
if latent_qubits >= num_qubits:
raise ValueError("latent_qubits must be < num_qubits")
trash_qubits = num_qubits - latent_qubits
qc = QuantumCircuit(num_qubits, f"qae_{num_qubits}to{latent_qubits}")
# Encoder - variational layers
param_idx = 0
num_layers = min(2, len(params) // num_qubits)
for layer in range(num_layers):
for q in range(num_qubits):
if param_idx < len(params):
qc.ry(params[param_idx], q)
param_idx += 1
for q in range(num_qubits - 1):
qc.cx(q, q + 1)
# Compression: SWAP latent qubits to the beginning
# This moves qubits [0..latent-1] to the front
for i in range(trash_qubits):
for j in range(trash_qubits - i):
if j < num_qubits - 1:
qc.swap(j, j + 1)
return qc
# =============================================================================
# Quantum Principal Component Analysis
# =============================================================================
def quantum_pca_circuit(num_qubits: int, num_components: int) -> QuantumCircuit:
"""
Create a quantum PCA circuit using quantum phase estimation.
Args:
num_qubits: Data dimension
num_components: Number of principal components to extract
Returns:
QPCA circuit
"""
total_qubits = num_qubits + num_components
qc = QuantumCircuit(total_qubits, f"qpca_{num_components}")
# Prepare superposition on counting qubits
for i in range(num_components):
qc.h(i)
# Controlled rotations encoding covariance structure
for k in range(num_components):
for q in range(num_qubits):
angle = math.pi / (2 ** (k + 1))
qc.crz(angle, k, num_components + q)
# Inverse QFT on counting qubits
for i in range(num_components // 2):
qc.swap(i, num_components - 1 - i)
for i in range(num_components):
qc.h(i)
for j in range(i + 1, num_components):
angle = -math.pi / (2 ** (j - i))
qc.cp(angle, j, i)
return qc